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<article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="1.3" xml:lang="en" article-type="research-article"><?properties manuscript?><processing-meta base-tagset="archiving" mathml-version="3.0" table-model="xhtml" tagset-family="jats"><restricted-by>pmc</restricted-by></processing-meta><front><journal-meta><journal-id journal-id-type="nlm-journal-id">0266262</journal-id><journal-id journal-id-type="pubmed-jr-id">5187</journal-id><journal-id journal-id-type="nlm-ta">J Physiol</journal-id><journal-id journal-id-type="iso-abbrev">J Physiol</journal-id><journal-title-group><journal-title>The Journal of physiology</journal-title></journal-title-group><issn pub-type="ppub">0022-3751</issn><issn pub-type="epub">1469-7793</issn></journal-meta><article-meta><article-id pub-id-type="pmid">39722577</article-id><article-id pub-id-type="pmc">11955869</article-id><article-id pub-id-type="doi">10.1113/JP287596</article-id><article-id pub-id-type="manuscript">NIHMS2039207</article-id><article-categories><subj-group subj-group-type="heading"><subject>Article</subject></subj-group></article-categories><title-group><article-title>Computational modelling of cardiac control following myocardial infarction using an <italic toggle="yes">in silico</italic> patient cohort</article-title></title-group><contrib-group><contrib contrib-type="author"><name><surname>Gee</surname><given-names>Michelle M.</given-names></name><xref rid="A1" ref-type="aff">1</xref><xref rid="A2" ref-type="aff">2</xref></contrib><contrib contrib-type="author"><name><surname>Lenhoff</surname><given-names>Abraham M.</given-names></name><xref rid="A1" ref-type="aff">1</xref></contrib><contrib contrib-type="author"><name><surname>Schwaber</surname><given-names>James S.</given-names></name><xref rid="A2" ref-type="aff">2</xref></contrib><contrib contrib-type="author"><contrib-id contrib-id-type="orcid" authenticated="false">http://orcid.org/0000-0002-8405-1037</contrib-id><name><surname>Vadigepalli</surname><given-names>Rajanikanth</given-names></name><xref rid="A2" ref-type="aff">2</xref><xref rid="CR1" ref-type="corresp">*</xref></contrib></contrib-group><aff id="A1"><label>1</label>Department of Chemical and Biomolecular Engineering, University of Delaware, Newark, DE 19716 USA</aff><aff id="A2"><label>2</label>Daniel Baugh Institute for Functional Genomics and Computational Biology, Department of Pathology and Genomic Medicine, Thomas Jefferson University, Philadelphia, PA 19107 USA</aff><author-notes><fn fn-type="con" id="FN1"><label>C.</label><p id="P1">Author contributions</p><p id="P2">M.G. collected and analysed the data and drafted the manuscript. A.L. and J.S. assisted in interpreting the results and critically revised the manuscript. R.V. conceived the study and critically revised the manuscript. All authors have read and approved the final version of the manuscript submitted for publication and agree to be accountable for all aspects of the work, ensuring that questions related to the accuracy or integrity of any part of the work are appropriately investigated and resolved. All persons designated as authors qualify for authorship and all those who qualify for authorship are listed.</p></fn><corresp id="CR1"><label>*</label><bold>Corresponding author:</bold> Rajanikanth Vadigepalli, <email>Rajanikanth.Vadigepalli@jefferson.edu</email></corresp></author-notes><pub-date pub-type="nihms-submitted"><day>24</day><month>12</month><year>2024</year></pub-date><pub-date pub-type="ppub"><month>3</month><year>2025</year></pub-date><pub-date pub-type="epub"><day>25</day><month>12</month><year>2024</year></pub-date><pub-date pub-type="pmc-release"><day>01</day><month>3</month><year>2026</year></pub-date><volume>603</volume><issue>7</issue><fpage>2021</fpage><lpage>2042</lpage><abstract id="ABS1"><p id="P3">Loss of cardiac physiological function following myocardial infarction (MI) is accompanied by neural adaptations in the baroreflex that are compensatory in the short term but then become associated with long-term disease progression. One marker of these adaptations is decreased baroreflex sensitivity, a strong predictor of post-MI mortality. The relative contributions of cardiac remodelling and neural adaptation in the sensory, central brainstem, and peripheral ganglionic loci to baroreflex sensitivity changes remain underexplored. We used a computational model-based approach that accounts for the short-term dynamics of closed-loop human cardiac control to integrate disparate experimental studies on neural adaptation following MI into a unified quantitative framework. We developed an ensemble of 59 distinct model parameterizations that account for the clinically observed heterogeneity of cardiac control in healthy individuals. We simulated an <italic toggle="yes">in silico</italic> cohort of 35,400 patients with MI, corresponding to six scenarios of one or more loci of neural adaptation coupled with cardiac remodelling. We evaluated the range of MI-induced shifts in arterial pressure, heart rate and baroreflex curve responses. Our results show that adaptation in any single neural locus coupled with cardiac remodelling is sufficient to account for the MI-induced hemodynamic and autonomic changes observed experimentally. Of the adaptation pathways, we found that individuals with central or peripheral vagal efferent adaptation and preserved baroreceptor gain could maintain high baroreflex sensitivity after ischemic injury. These results suggest that there are a multitude of adaptive pathways for tuning the baroreflex circuit to shift cardiac control physiology, potentially explaining patient heterogeneity post-MI.</p></abstract><abstract id="ABS2" abstract-type="graphical"><title>Abstract figure.</title><p id="P4">The baroreflex adapts to compensate for the decrease in cardiac function after myocardial infarction. We used <italic toggle="yes">in silico</italic> patient cohorts representing afferent and efferent loci of neural adaptation to explore neural remodelling that allowed individuals to maintain higher baroreflex sensitivity after cardiac injury. The model suggests that adaptation along the vagal efferent pathway can help maintain higher baroreflex sensitivity after cardiac injury. Figure created with <ext-link xlink:href="https://BioRender.com" ext-link-type="uri">BioRender.com</ext-link>.</p></abstract><kwd-group><kwd>Cardiovascular control</kwd><kwd>vagus nerve</kwd><kwd>cardiac remodelling</kwd><kwd>computational modelling</kwd><kwd>autonomic regulation</kwd><kwd>myocardial infarction</kwd></kwd-group></article-meta></front><body><sec id="S2"><label>I.</label><title>INTRODUCTION</title><p id="P5">Myocardial ischemia and the subsequent injury to the cardiac tissue trigger a multitude of changes to heart physiology, including ventricular stiffening and loss of contractility. Reperfusion leads to an inflammatory response that further exacerbates the injury around the infarct. These changes can result in a variety of hemodynamic states ranging from hypotension to hypertension in different individuals (<xref rid="R26" ref-type="bibr">Ma et al., 2015</xref>). In addition to alterations in cardiac physiology, adaptation of closed-loop neuronal regulation occurs simultaneously in an attempt to maintain cardiovascular homeostasis. While the majority of the investigational focus and therapeutic attention has been on the cardiac remodelling aspect, there is mounting evidence that neural adaptation may also play a role in the aberrant physiological response following MI (<xref rid="R39" ref-type="bibr">Sabbah, 2012</xref>). Neuronal adaptations to compensate for decreased cardiac function after MI deliver short-term gains that are believed to result in long-term cardiovascular disease progression (<xref rid="R10" ref-type="bibr">Floras, 2009</xref>; <xref rid="R14" ref-type="bibr">Herring et al., 2024</xref>). Several questions regarding neural adaptation following myocardial infarction have been posed in the recent white paper by <xref rid="R14" ref-type="bibr">Herring et al., 2024</xref>. We aim to address one such neural adaptation, the observed decrease in baroreflex sensitivity after cardiac injury, which is correlated with increased cardiac mortality in patients with recent myocardial infarction (<xref rid="R22" ref-type="bibr">La Rovere et al., 1998</xref>).</p><p id="P6">The baroreflex is a complex control system that regulates cardiac function on a beat-to-beat basis via several neural loci. Adaptation contributing to decreased baroreflex function could originate from the periphery via the baroreceptors, the intrinsic cardiac nervous system (ICN), dorsal root ganglia, and the stellate ganglia, or centrally in multiple autonomic nuclei, including the nucleus tractus solitarius (NTS), nucleus ambiguus (NA), dorsal motor nucleus of the vagus (DMV), rostral ventral lateral medulla, and caudal ventrolateral medulla. There is a variety of evidence to supporting neuronal adaptation in response to ischemic injury in these neural groups including neuropeptide and morphological changes in the stellate ganglia (<xref rid="R2" ref-type="bibr">Ajijola et al., 2015</xref>), transcriptomic changes in the DMV (<xref rid="R12" ref-type="bibr">Gorky et al., 2021</xref>), as well as structural and functional remodelling in the ICN (<xref rid="R38" ref-type="bibr">Rajendran et al., 2016</xref>). It is reasonable to expect that different loci of neural adaptation could adapt, depending on the individual, contributing to the heterogeneity observed clinically. We propose that differential balance of nuclei across the baroreflex arc may be partially responsible for the diversity in baroreflex function observed clinically.</p><p id="P7">We approach this hypothesis using a computational modelling and simulation strategy to overcome the challenges in unpacking the experimental complexity to discern the contributions of each neural locus to baroreflex adaptation in health and disease. Experimental interventions are likely to induce new adaptations in other parts of the closed-loop cardiovascular control system, making it difficult to tease apart the cause and effect relationships. Closed-loop computational models of the baroreflex are established predictive tools for describing the heart rate response to blood pressure changes (<xref rid="R45" ref-type="bibr">Ursino, 1998</xref>). These models have been used to predict changes under a variety of conditions and gain insights on physiological phenomena including exercise (<xref rid="R36" ref-type="bibr">Park et al., 2020</xref>), hypoxia (<xref rid="R46" ref-type="bibr">Ursino &#x00026; Magosso, 2000</xref>), and respiratory sinus arrhythmia (<xref rid="R4" ref-type="bibr">Ben-Tal et al., 2012</xref>). To date, many models of the baroreflex have been proposed, but only a few have considered baroreflex changes following myocardial infarction (<xref rid="R18" ref-type="bibr">Kember et al., 2017</xref>), and only in ways that do not explicitly include cardiac damage. On the other hand, computational approaches that explicitly model the cardiac physiology are usually computationally expensive finite-element models or are focused on the immune response following MI, and do not include baroreflex regulation in the quantitative scheme (<xref rid="R5" ref-type="bibr">Berberoglu &#x00026; G&#x000f6;ktepe, 2015</xref>; <xref rid="R40" ref-type="bibr">S&#x000e1;ez &#x00026; Kuhl, 2016</xref>). Furthermore, computational models that account for individual heterogeneity of cardiac physiology have been explored to a limited extent and are actively emerging in recent studies (<xref rid="R33" ref-type="bibr">Niederer et al., 2020</xref>; <xref rid="R3" ref-type="bibr">Argus et al., 2022</xref>; <xref rid="R49" ref-type="bibr">Yang et al., 2023</xref>). These computational models tend to address the cardiac, respiratory, or drug response level, but limited work has been done on variability of the baroreflex.</p><p id="P8">In the present study, we aim to address a question on adaptations in cardiac control with cardiovascular disease posed in the recent white paper on translational advancements and potential in neurocardiology (<xref rid="R14" ref-type="bibr">Herring et al., 2024</xref>). The white paper brings forward the question &#x0201c;How does localized pathology in specific regions of the neural hierarchy influence the behaviour of the system as a whole?&#x0201d; We aim to address this question more specifically by exploring the question of how localized pathology in the heart influences the system as a whole and how specific regions of the neural hierarchy can compensate for that pathology. We hypothesise that adaptation in a subset of neural loci is sufficient for maintenance of baroreflex sensitivity after ischemic insult. We generate and simulate an <italic toggle="yes">in silico</italic> patient cohort that accounts for inter-individual heterogeneity, and is consistent with the range of hemodynamic behaviour observed clinically, to capture closed-loop cardiac autonomic control aspects with high fidelity. Our overall strategy is to compare pre- versus post-ischemia/reperfusion models over the range of neural loci of adaptation and identify characteristics of virtual patients with higher baroreflex sensitivity after myocardial injury.</p></sec><sec id="S3"><label>II.</label><title>METHODS</title><p id="P9">The present model extends our previously published work on baroreflex control of the cardiovascular system (<xref rid="R11" ref-type="bibr">Gee et al., 2023</xref>). Briefly, the cardiovascular control model consists of two main parts: (1) the cardiovascular system, represented by ordinary differential equations derived from mass balances of blood flow through body compartments, and (2) the neural control system, represented by sigmoidal functions representing the saturating firing behaviour of neurons (<xref rid="F1" ref-type="fig">Fig. 1</xref>). The cardiovascular system model includes representations of the pulmonary and systemic circulatory systems and a pulsatile model of the heart. The neural portion of the model includes representations of sensory neuronal groups as well as brainstem and ICN neuronal groups. This model is used to simulated pre-ischemia and post-ischemia <italic toggle="yes">in silico</italic> patient cohorts to examine adaptation following cardiac injury and the role of inter-individual variability.</p><sec id="S4"><label>A.</label><title>Pre-ischemia model ensemble</title><p id="P10">The plausible range of baroreflex curves in healthy individuals was quantified using data from five individuals and measured using neck chamber pressure (<xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>). To quantify the characteristics of these baroreflex curves, these individual data were fit to the sigmoidal function
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which was previously used by (<xref rid="R9" ref-type="bibr">Fadel et al., 2003</xref>; <xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>). In this case, we have fit the RR interval response to estimated carotid sinus pressure, which is the pre-stimulus mean arterial pressure minus the neck chamber pressure. The parameter <inline-formula><mml:math id="M2" display="inline"><mml:mi>A</mml:mi><mml:mn>1</mml:mn></mml:math></inline-formula> represents the response range (maximum - minimum), <inline-formula><mml:math id="M3" display="inline"><mml:mi>A</mml:mi><mml:mn>2</mml:mn></mml:math></inline-formula> represents the gain coefficient, i.e. the slope of the sigmoid, <inline-formula><mml:math id="M4" display="inline"><mml:mi>A</mml:mi><mml:mn>3</mml:mn></mml:math></inline-formula> represents the centering point for the horizontal shift of the sigmoid, and <inline-formula><mml:math id="M5" display="inline"><mml:mi>A</mml:mi><mml:mn>4</mml:mn></mml:math></inline-formula> represents the minimum response. <xref rid="FD1" ref-type="disp-formula">Eq. 1</xref> is used to quantitatively compare the model predictions of overall baroreflex function with experimentally measured baroreflex curves and filter out plausible models.</p><p id="P11">To develop an averaged cardiovascular control model capturing this pre-I/R RR interval response to carotid sinus pressure changes, we re-estimated a minimal set of parameters from our previously published model (<xref rid="R11" ref-type="bibr">Gee et al., 2023</xref>). The two parameters represent the minimum and maximum firing rate of the population of ICN neurons that regulate heart rate were re-fit to match the average baroreflex curve response of the data from (<xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>). All other parameter values were the same as in the previous model and the new parameter values are provided in <xref rid="T1" ref-type="table">Table 1</xref>.</p><p id="P12">The sensory neuronal groups include baroreceptors that convert arterial pressure changes into electrical signals. Based on prior models (<xref rid="R45" ref-type="bibr">Ursino, 1998</xref>; <xref rid="R36" ref-type="bibr">Park et al., 2020</xref>; <xref rid="R11" ref-type="bibr">Gee et al., 2023</xref>), the baroreceptors are represented by a linear derivative first-order dynamic function and a sigmoidal static function in series as indicated by experimental results (<xref rid="R6" ref-type="bibr">Chapleau &#x00026; Abboud, 1987</xref>):
<disp-formula id="FD2">
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<mml:math id="M6" display="block"><mml:msub><mml:mrow><mml:mi>&#x003c4;</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mfrac><mml:mrow><mml:mi>d</mml:mi><mml:mi mathvariant="normal">&#x01e54;</mml:mi></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>&#x003c4;</mml:mi></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msub><mml:mfrac><mml:mrow><mml:mi>d</mml:mi><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac><mml:mo>-</mml:mo><mml:mi mathvariant="normal">&#x01e54;</mml:mi></mml:math>
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<disp-formula id="FD3">
<label>(3)</label>
<mml:math id="M7" display="block"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:mi mathvariant="normal">*</mml:mi><mml:mi mathvariant="normal">e</mml:mi><mml:mi mathvariant="normal">x</mml:mi><mml:mi mathvariant="normal">p</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mfrac><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mo>&#x000b4;</mml:mo></mml:mover><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mo>+</mml:mo><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mfrac><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mo>&#x000b4;</mml:mo></mml:mover><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mfrac></mml:math>
</disp-formula></p><p id="P13"><xref rid="FD2" ref-type="disp-formula">Eq. 2</xref> converts the measured arterial pressure <inline-formula><mml:math id="M8" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> to the output variable of the dynamic function <inline-formula><mml:math id="M9" display="inline"><mml:mover accent="true"><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mo>&#x000b4;</mml:mo></mml:mover></mml:math></inline-formula> (with dimensions of pressure). The time constants <inline-formula><mml:math id="M10" display="inline"><mml:msub><mml:mrow><mml:mi>&#x003c4;</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> and <inline-formula><mml:math id="M11" display="inline"><mml:msub><mml:mrow><mml:mi>&#x003c4;</mml:mi></mml:mrow><mml:mrow><mml:mi>z</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> are for the real pole and real zero in the linear dynamic block. <inline-formula><mml:math id="M12" display="inline"><mml:mover accent="true"><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mo>&#x000b4;</mml:mo></mml:mover></mml:math></inline-formula> is converted to the baroreceptor firing rate (<inline-formula><mml:math id="M13" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>) in <xref rid="FD3" ref-type="disp-formula">Eq. 3</xref>, with the minimal and maximal output firing rate given by <inline-formula><mml:math id="M14" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> and <inline-formula><mml:math id="M15" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>, respectively. <inline-formula><mml:math id="M16" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is the intrasinus pressure at the central point of the sigmoidal curve and <inline-formula><mml:math id="M17" display="inline"><mml:msub><mml:mrow><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is the gain constant describing the magnitude of the response of the firing rate to pressure changes. Larger values of <inline-formula><mml:math id="M18" display="inline"><mml:msub><mml:mrow><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> mean the baroreceptors are less sensitive to pressure changes.</p><p id="P14">Sensory signals from the baroreceptors are sent to the brainstem where neuronal groups are represented by sigmoidal functions of the form:
<disp-formula id="FD4">
<label>(4)</label>
<mml:math id="M19" display="block"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>o</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mo>+</mml:mo><mml:msup><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>p</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>d</mml:mi><mml:mi>p</mml:mi><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:mi>k</mml:mi></mml:mrow></mml:msup></mml:mrow></mml:mfrac><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:math>
</disp-formula></p><p id="P15"><xref rid="FD4" ref-type="disp-formula">Eq. 4</xref> describes the input-output behaviour of the <italic toggle="yes">j</italic><sup><italic toggle="yes">th</italic></sup> neuronal group, where <inline-formula><mml:math id="M20" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> and <inline-formula><mml:math id="M21" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> are the minimal and the maximal output firing rates. Changes in the value of the parameter <inline-formula><mml:math id="M22" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>d</mml:mi><mml:mi>p</mml:mi><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> shift the range of input firing rates to which the neuronal group is sensitive and the sigmoidal gain, <inline-formula><mml:math id="M23" display="inline"><mml:msub><mml:mrow><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>, represents the magnitude of the output firing rate change in response to a change in input firing rate.</p><p id="P16">These sigmoidal functions are used to describe brainstem neuronal subtypes in the NTS, NA, and DMV as well as peripheral neuronal subtypes in the ICN. The NTS includes separate representations for neuronal subtypes based on previous single-neuron transcriptomic analysis, which indicated that neuronal subtypes in the NTS are distinct based on the inputs they receive (<xref rid="R35" ref-type="bibr">Park et al., 2014</xref>). Therefore, the model incorporates NTS neuronal subtypes that receive different types of sensory input (baroreceptor inputs with information on arterial pressure, cardiopulmonary receptor inputs with information on pressure in the heart chambers, and lung stretch receptor with information on lung inflation). NTS neurons project to the NA and DMV, which transmit signals through the vagus nerve to the ICN. Neuronal tracing studies have shown that the NA and DMV project to separate populations of principal neurons (PN) in the ICN, so we have included representations of those neuronal groups in the model (PN<sub>NA</sub> and PN<sub>DMV</sub>). These separate populations interact via local circuit neurons (LCN) that also incorporate sensory information, forming an inner feedback loop.</p><p id="P17">Effector functions based on mathematical relationships derived from experimental measurements then translate firing rates from the ICN into changes in HR and ventricular elastance (<xref rid="R45" ref-type="bibr">Ursino, 1998</xref>). Experiments on the effects of sympathetic activity and the time delays observed were used to inform a logarithmic relationship between elastance and sympathetic firing rate.</p><disp-formula id="FD5">
<label>(5)</label>
<mml:math id="M24" display="block"><mml:msub><mml:mrow><mml:mi>&#x003c3;</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mfenced open="{" close="" separators="|"><mml:mrow><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>l</mml:mi><mml:mi>n</mml:mi><mml:mfenced open="[" close="]" separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:mfenced></mml:mtd><mml:mtd><mml:mi>i</mml:mi><mml:mi>f</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi></mml:mrow></mml:msub><mml:mo>&#x02265;</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mn>0</mml:mn></mml:mtd><mml:mtd><mml:mi>i</mml:mi><mml:mi>f</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0003c;</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:mfenced></mml:math>
</disp-formula><p id="P18">Where <inline-formula><mml:math id="M25" display="inline"><mml:msub><mml:mrow><mml:mi>&#x003c3;</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>, is the effect of sympathetic activity on elastance, <inline-formula><mml:math id="M26" display="inline"><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is a gain value, <inline-formula><mml:math id="M27" display="inline"><mml:msub><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is a time delay, <inline-formula><mml:math id="M28" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> a sympathetic activity constant. based on experiments on the effects of sympathetic activity and the time delays observed (<xref rid="R45" ref-type="bibr">Ursino, 1998</xref>). A first-order filter with time constant <inline-formula><mml:math id="M29" display="inline"><mml:msub><mml:mrow><mml:mi>&#x003c4;</mml:mi></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>
<disp-formula id="FD6">
<label>(6)</label>
<mml:math id="M30" display="block"><mml:mfrac><mml:mrow><mml:mi>d</mml:mi><mml:mi mathvariant="normal">&#x00394;</mml:mi><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>E</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo stretchy="false">(</mml:mo><mml:mi>t</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x003c4;</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>[</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="normal">&#x00394;</mml:mi><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>E</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>&#x003c3;</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo>]</mml:mo></mml:math>
</disp-formula>
further blunts the effects on elastance. The parasympathetic contribution to ventricular elastance has a linear relationship between the vagal firing rate <inline-formula><mml:math id="M31" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>v</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> multiplied by gain <inline-formula><mml:math id="M32" display="inline"><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> with time delay <inline-formula><mml:math id="M33" display="inline"><mml:msub><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>,
<disp-formula id="FD7">
<label>(7)</label>
<mml:math id="M34" display="block"><mml:msub><mml:mrow><mml:mi>&#x003c3;</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>v</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:math>
</disp-formula>
also blunted by a first-order filter.
<disp-formula id="FD8">
<label>(8)</label>
<mml:math id="M35" display="block"><mml:mfrac><mml:mrow><mml:mi>d</mml:mi><mml:mi mathvariant="normal">&#x00394;</mml:mi><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>E</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow><mml:mrow><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo stretchy="false">(</mml:mo><mml:mi>t</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x003c4;</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo stretchy="false">[</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="normal">&#x00394;</mml:mi><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>E</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow><mml:mrow><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>&#x003c3;</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo stretchy="false">]</mml:mo></mml:math>
</disp-formula></p><p id="P19">The change in elastance due to sympathetic activity <inline-formula><mml:math id="M36" display="inline"><mml:mo stretchy="false">(</mml:mo><mml:mi mathvariant="normal">&#x00394;</mml:mi><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>E</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo stretchy="false">)</mml:mo></mml:math></inline-formula> and the change due to parasympathetic activity <inline-formula><mml:math id="M37" display="inline"><mml:mo stretchy="false">(</mml:mo><mml:mi mathvariant="normal">&#x00394;</mml:mi><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>E</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow><mml:mrow><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo stretchy="false">)</mml:mo></mml:math></inline-formula> are summed to produce the effect of neural activity on left ventricular elastance:
<disp-formula id="FD9">
<label>(9)</label>
<mml:math id="M38" display="block"><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>E</mml:mi><mml:mi>&#x02032;</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mi mathvariant="normal">&#x00394;</mml:mi><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>E</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>+</mml:mo><mml:mi mathvariant="normal">&#x00394;</mml:mi><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>E</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow><mml:mrow><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:math>
</disp-formula></p><p id="P20">The effect of neural activity is added to the baseline elastance, obtained from a denervated heart (<xref rid="R45" ref-type="bibr">Ursino, 1998</xref>; <xref rid="R46" ref-type="bibr">Ursino &#x00026; Magosso, 2000</xref>; <xref rid="R36" ref-type="bibr">Park et al., 2020</xref>) with the baseline elastance (<inline-formula><mml:math id="M39" display="inline"><mml:msub><mml:mrow><mml:mi>E</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi><mml:mo>,</mml:mo><mml:mn>0</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula>) to calculate the ventricular elastance:
<disp-formula id="FD10">
<label>(10)</label>
<mml:math id="M40" display="block"><mml:msub><mml:mrow><mml:mi>E</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:msup><mml:mi>E</mml:mi><mml:mi>&#x02032;</mml:mi></mml:msup><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>E</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi><mml:mo>,</mml:mo><mml:mn>0</mml:mn></mml:mrow></mml:msub></mml:math>
</disp-formula></p><p id="P21">Equations representing the effects of sympathetic activity on arterial resistances and venous unstressed volumes have the same form as <xref rid="FD5" ref-type="disp-formula">Eqs. 5</xref> and <xref rid="FD6" ref-type="disp-formula">6</xref>. Parameters were likewise adapted from previous models, which were measured or deduced from empirical observations of relationships between physiological variables (<xref rid="R45" ref-type="bibr">Ursino, 1998</xref>; <xref rid="R46" ref-type="bibr">Ursino &#x00026; Magosso, 2000</xref>; <xref rid="R36" ref-type="bibr">Park et al., 2020</xref>).</p></sec><sec id="S5"><label>B.</label><title>Summary of experimental data used to filter accepted models</title><p id="P22">Data from three studies were used to filter the accepted models. The data used to constrain the pre-I/R baroreflex curves were from (<xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>). These baroreflex curve data were collected in healthy subjects using a neck chamber pressure device to control carotid sinus pressure while RR interval was measured. Because paired pre- and post-I/R data were not available in humans, experimental data from rats were used (<xref rid="R30" ref-type="bibr">Mastitskaya et al., 2012</xref>). HR and MAP were measured prior to myocardial ischemia caused by a left anterior descending artery ligation. After 30 minutes of cardiac ischemia, the heart was reperfused and HR and MAP were measured again 120 minutes later (<xref rid="F4" ref-type="fig">Fig. 4B</xref>). There were other HR and MAP measurement timepoints included in the study, but the 120 minute post-ischemia timepoint was selected because it was the closest in time to what could be measured clinically post-I/R. In addition, this study included other experimental groups with selective silencing and activation of the dorsal motor nucleus of the vagus. However, because of the limited data points, large number of parameters estimated in this model, and low likelihood of finding appropriate baroreflex curve data to help constrain the model, the other experimental group data points were not used. The available post-I/R baroreflex curve data were from MI patients 30&#x02013;72 hours after the first occurrence of chest pain. The patients had no evidence of a previous MI, no history of hypertension, diabetes, or other major cardiovascular diseases. Baroreflex curve data were measured using neck chamber pressure.</p></sec><sec id="S6"><label>C.</label><title>Parametric sensitivity analysis</title><p id="P23">To decrease the number of cardiac parameters to estimate to represent the pre- and post-I/R models, we performed a global sensitivity analysis to determine which parameters significantly affected HR and MAP. A density-based sensitivity analysis known as PAWN (<xref rid="R37" ref-type="bibr">Pianosi &#x00026; Wagener, 2018</xref>) was selected because the underlying distribution of the outputs was unknown and because this method has been used successfully in other cardiovascular system models (<xref rid="R36" ref-type="bibr">Park et al., 2020</xref>; <xref rid="R11" ref-type="bibr">Gee et al., 2023</xref>). To determine the underlying distribution, PAWN uses cumulative density functions (CDF) to characterise the model output of interest (<inline-formula><mml:math id="M41" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula>) and determine the output sensitivity to the parameter of interest (<inline-formula><mml:math id="M42" display="inline"><mml:mi>&#x003b8;</mml:mi></mml:math></inline-formula>). Two sets of simulations were performed. The first set varied all parameters simultaneously to produce unconditional CDFs (<inline-formula><mml:math id="M43" display="inline"><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>y</mml:mi></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>y</mml:mi></mml:mrow></mml:mfenced></mml:math></inline-formula>). The second set varied all inputs except the parameter of interest to produce conditional CDFs (<inline-formula><mml:math id="M44" display="inline"><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>y</mml:mi><mml:mo>|</mml:mo><mml:msub><mml:mrow><mml:mi>&#x003b8;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mi>y</mml:mi><mml:mo>|</mml:mo><mml:msub><mml:mrow><mml:mi>&#x003b8;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo></mml:math></inline-formula>). To determine the sensitivity of the output to changes in the parameter of interest, the distance between the unconditional and conditional CDFs was quantified using the Kolmogorov-Smirnoff (KS) statistic. The sensitivity index for the <italic toggle="yes">i</italic><sup><italic toggle="yes">th</italic></sup> input factor is
<disp-formula id="FD11">
<label>(11)</label>
<mml:math id="M45" display="block"><mml:msub><mml:mrow><mml:mi>S</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">statmax</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x003b8;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi>y</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mfenced open="|" close="|" separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>y</mml:mi></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>y</mml:mi></mml:mrow></mml:mfenced><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>y</mml:mi><mml:mo>|</mml:mo><mml:msub><mml:mrow><mml:mi>&#x003b8;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>y</mml:mi><mml:mo>|</mml:mo><mml:msub><mml:mrow><mml:mi>&#x003b8;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced></mml:mrow></mml:mrow></mml:math>
</disp-formula>
where stat is a statistic chosen by the user (e.g., median). If the conditional and unconditional CDFs are close together, the output is sensitive to that parameter because varying other parameters did not cause a significant change in the output. If they are far apart, the output is not sensitive to the input parameter of interest. Because the KS statistic depends upon the value of the constant parameter, the PAWN method determines the KS statistic across many values. To combine these KS statistics, we use a summary statistic (e.g., median) to characterise the distribution of the KS statistic. This summary statistic varies from 0 to 1, with a value closer to 1 indicating a greater parametric influence on the output. To determine a threshold value for significant summary statistics, the PAWN method introduces a dummy parameter, which is known to have no effect on the output. If the summary statistic of a parameter is greater than the summary statistic of the dummy parameter, it is likely that the output is sensitive to that parameter. In this analysis, we performed 40,000 simulations with six conditioning intervals and checked for convergence by performing additional simulations and confirming that the results remained the same. The PAWN method also includes bootstrapping to determine 95 percent confidence intervals for each sensitivity index.</p></sec><sec id="S7"><label>D.</label><title>Peripheral versus central contributions to heart rate regulation</title><p id="P24">The peripheral versus central contributions to heart rate regulation were quantified using the Shapley value, which is a metric from game theory used to estimate the contributions of each player in a coalition game (<xref rid="R25" ref-type="bibr">Loh et al., 2022</xref>). To obtain the Shapley values, accepted parameter sets were used as the inputs to a support vector machine regression model with a polynomial kernel function that predicts heart rate. The regression model was validated using the mean square error between the predicted and actual heart rates. Because the relationship between each parameter and heart rate could be nonlinear, the Shapley value was calculated for each parameter set. The average over each of these sampled points was calculated for each individual model for central (NTS, NA, DMV) and peripheral (ICN, baroreceptors) parameters. The ratio of peripheral to central contributions was then taken for each parameter set.</p></sec><sec id="S8"><label>E.</label><title>Clustering analysis</title><p id="P25">Post-I/R models were clustered based on average afferent vagal activity, average efferent vagal activity, and baroreceptor responsivity. The analysis was performed using MATLAB R2023b&#x02019;s tsne function using the Barneshut algorithm (<xref rid="R27" ref-type="bibr">van der Maaten, 2013</xref>), which was selected for its computational efficiency (Mathworks, Natick, MA). The &#x02018;cityblock&#x02019; distance metric was used because the input metrics are in different units. Twenty was used for the perplexity value, which quantifies the weighting of the local versus global aspects of the data in running the analysis.</p></sec><sec id="S9"><label>F.</label><title>Model equations</title><p id="P26">All model equations are adapted from (<xref rid="R45" ref-type="bibr">Ursino, 1998</xref>; <xref rid="R46" ref-type="bibr">Ursino &#x00026; Magosso, 2000</xref>; <xref rid="R36" ref-type="bibr">Park et al., 2020</xref>; <xref rid="R11" ref-type="bibr">Gee et al., 2023</xref>). The full set of nominal model parameters can be found at <ext-link xlink:href="https://github.com/Daniel-Baugh-Institute/CardiovascularControl/tree/main/Virtual_patient_cohorts" ext-link-type="uri">https://github.com/Daniel-Baugh-Institute/CardiovascularControl/tree/main/Virtual_patient_cohorts</ext-link>.</p><p id="P27">The vascular system is composed of mass and force balances. These equations from first-order principles are derived for the pulmonary and systemic circulatory system. The body compartments included in the model are the systemic, splanchnic, extrasplanchnic, skeletal muscle, thoracic and pulmonary arteries, and veins. In the pulmonary arteries we have the mass balance for flow out of the right ventricle and into the pulmonary arteries:
<disp-formula id="FD12">
<label>(12)</label>
<mml:math id="M46" display="block"><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>d</mml:mi><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>o</mml:mi><mml:mo>,</mml:mo><mml:mi>r</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p><p id="P28">The corresponding force balance at the pulmonary arteries is:
<disp-formula id="FD13">
<label>(13)</label>
<mml:math id="M47" display="block"><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>d</mml:mi><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>L</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p><p id="P29">The conservation of mass at pulmonary peripheral circulation <inline-formula><mml:math id="M48" display="inline"><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mi>p</mml:mi><mml:mo>)</mml:mo></mml:math></inline-formula> is modeled as:
<disp-formula id="FD14">
<label>(14)</label>
<mml:math id="M49" display="block"><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>d</mml:mi><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p><p id="P30">The conservation of mass at pulmonary veins <inline-formula><mml:math id="M50" display="inline"><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mi>v</mml:mi><mml:mo>)</mml:mo></mml:math></inline-formula> is modeled as:
<disp-formula id="FD15">
<label>(15)</label>
<mml:math id="M51" display="block"><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>d</mml:mi><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mfenced separators="|"><mml:mrow><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>-</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p><p id="P31">The mass balance at systemic arteries <inline-formula><mml:math id="M52" display="inline"><mml:mo>(</mml:mo><mml:mi>s</mml:mi><mml:mi>a</mml:mi><mml:mo>)</mml:mo></mml:math></inline-formula> is:
<disp-formula id="FD16">
<label>(16)</label>
<mml:math id="M53" display="block"><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>d</mml:mi><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>o</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p><p id="P32">The force balance at systemic arteries is:
<disp-formula id="FD17">
<label>(17)</label>
<mml:math id="M54" display="block"><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>d</mml:mi><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>L</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p><p id="P33">Conservation of mass at peripheral systemic circulation &#x02013; splanchnic, extrasplanchnic, and lower body compartments <inline-formula><mml:math id="M55" display="inline"><mml:mo>(</mml:mo><mml:mi>s</mml:mi><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.5em"/><mml:mi>e</mml:mi><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.5em"/><mml:mi>m</mml:mi><mml:mi>p</mml:mi><mml:mo>)</mml:mo></mml:math></inline-formula> is:
<disp-formula id="FD18">
<label>(18)</label>
<mml:math id="M56" display="block"><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>d</mml:mi><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mo>+</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mo>+</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>-</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>-</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>b</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p><p id="P34">Where
<disp-formula id="FD19">
<label>(19)</label>
<mml:math id="M57" display="block"><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>b</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mspace width="0.5em"/><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>+</mml:mo><mml:mspace width="0.5em"/><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>d</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:math>
</disp-formula></p><p id="P35">To incorporate the effects of varying abdominal pressure <inline-formula><mml:math id="M58" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>b</mml:mi><mml:mi>d</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> due to respiration, transmural pressure is calculated by subtracting <inline-formula><mml:math id="M59" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>b</mml:mi><mml:mi>d</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> from <inline-formula><mml:math id="M60" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>. Equations for <inline-formula><mml:math id="M61" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>b</mml:mi><mml:mi>d</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> are provided in later equations.</p><disp-formula id="FD20">
<label>(20)</label>
<mml:math id="M62" display="block"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>p</mml:mi><mml:mo>-</mml:mo><mml:mi>t</mml:mi><mml:mi>r</mml:mi><mml:mi>a</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>b</mml:mi><mml:mi>d</mml:mi></mml:mrow></mml:msub></mml:math>
</disp-formula><p id="P36">This transmural pressure is subsequently used to determine downstream pressures.</p><p id="P37">The conservation of mass at extrasplanchnic venous circulation <inline-formula><mml:math id="M63" display="inline"><mml:mo>(</mml:mo><mml:mi>e</mml:mi><mml:mi>v</mml:mi><mml:mo>)</mml:mo></mml:math></inline-formula> is:
<disp-formula id="FD21">
<label>(21)</label>
<mml:math id="M64" display="block"><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>d</mml:mi><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mfenced separators="|"><mml:mrow><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>-</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>-</mml:mo><mml:mfrac><mml:mrow><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>d</mml:mi><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi><mml:mo>,</mml:mo><mml:mi>e</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p><p id="P38">The mass balance at skeletal muscle, part of the lower body <inline-formula><mml:math id="M65" display="inline"><mml:mo>(</mml:mo><mml:mi>m</mml:mi><mml:mi>v</mml:mi><mml:mo>)</mml:mo></mml:math></inline-formula> is:
<disp-formula id="FD22">
<label>(22)</label>
<mml:math id="M66" display="block"><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>d</mml:mi><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mfenced separators="|"><mml:mrow><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>b</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>-</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>-</mml:mo><mml:mfrac><mml:mrow><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>d</mml:mi><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p><p id="P39">The conservation of mass at thoracic vein <inline-formula><mml:math id="M67" display="inline"><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mi>v</mml:mi><mml:mo>)</mml:mo></mml:math></inline-formula> is:
<disp-formula id="FD23">
<label>(23)</label>
<mml:math id="M68" display="block"><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>d</mml:mi><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mfenced separators="|"><mml:mrow><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>+</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>+</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>-</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p><p id="P40">To incorporate the effects of varying thoracic pressure <inline-formula><mml:math id="M69" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> due to respiration, transmural pressure is calculated by subtracting <inline-formula><mml:math id="M70" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> from <inline-formula><mml:math id="M71" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>. Equations for <inline-formula><mml:math id="M72" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> are provided in later equations.</p><disp-formula id="FD24">
<label>(24)</label>
<mml:math id="M73" display="block"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>v</mml:mi><mml:mo>-</mml:mo><mml:mi>t</mml:mi><mml:mi>r</mml:mi><mml:mi>a</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub></mml:math>
</disp-formula><p id="P41">The conservation of mass determines splanchnic venous circulation, which assumes total blood volume <italic toggle="yes">(<inline-formula><mml:math id="M74" display="inline"><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>)</italic> is known.</p><disp-formula id="FD25">
<label>(25)</label>
<mml:math id="M75" display="block"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mspace linebreak="newline"/><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:math>
</disp-formula><p id="P42">Here, <inline-formula><mml:math id="M76" display="inline"><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> and <inline-formula><mml:math id="M77" display="inline"><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> are the volumes of the right and left ventricles. <inline-formula><mml:math id="M78" display="inline"><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is the total unstressed volume, defined by:
<disp-formula id="FD26">
<label>(26)</label>
<mml:math id="M79" display="block"><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi><mml:mo>,</mml:mo><mml:mi>e</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi><mml:mo>,</mml:mo><mml:mi>r</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mo>+</mml:mo><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math>
</disp-formula></p><p id="P43">The model includes a pulsatile model of the heart, again based on conservation of mass and force. Conservation of mass at the left atrium:
<disp-formula id="FD27">
<label>(27)</label>
<mml:math id="M80" display="block"><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>d</mml:mi><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mfenced separators="|"><mml:mrow><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:math>
</disp-formula>
where <inline-formula><mml:math id="M81" display="inline"><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> refers to flow into the left ventricle, determined by the mass balance:
<disp-formula id="FD28">
<label>(28)</label>
<mml:math id="M82" display="block"><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfenced open="{" close="" separators="|"><mml:mrow><mml:mtable columnalign="right"><mml:mtr><mml:mtd><mml:mn>0</mml:mn><mml:mo>,</mml:mo></mml:mtd><mml:mtd><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0003c;</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>,</mml:mo></mml:mtd><mml:mtd><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mo>&#x02265;</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p><p id="P44">Ventricular volume is calculated as:
<disp-formula id="FD29">
<label>(29)</label>
<mml:math id="M83" display="block"><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>d</mml:mi><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>o</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi></mml:mrow></mml:msub></mml:math>
</disp-formula>
where flow out of the left ventricle (<inline-formula><mml:math id="M84" display="inline"><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>o</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>) is calculated from:
<disp-formula id="FD30">
<label>(30)</label>
<mml:math id="M85" display="block"><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>o</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfenced open="{" close="" separators="|"><mml:mrow><mml:mtable columnalign="right"><mml:mtr><mml:mtd><mml:mn>0</mml:mn><mml:mo>,</mml:mo></mml:mtd><mml:mtd><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0003c;</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>,</mml:mo></mml:mtd><mml:mtd><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>&#x02265;</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p><p id="P45"><inline-formula><mml:math id="M86" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> represents the isometric pressure in the left ventricle, which is used to determine ventricular pressure during the cardiac cycle. It is used to determine <inline-formula><mml:math id="M87" display="inline"><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>, the viscous resistance of the left ventricle:
<disp-formula id="FD31">
<label>(31)</label>
<mml:math id="M88" display="block"><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math>
</disp-formula>
where <inline-formula><mml:math id="M89" display="inline"><mml:msub><mml:mrow><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is a constant parameter. Instantaneous pressure in the left ventricle represents the difference between the isometric pressure (<inline-formula><mml:math id="M90" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>) and viscous losses, therefore:
<disp-formula id="FD32">
<label>(32)</label>
<mml:math id="M91" display="block"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>F</mml:mi></mml:mrow><mml:mrow><mml:mi>o</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi></mml:mrow></mml:msub></mml:math>
</disp-formula></p><p id="P46">Isometric pressure is time-dependent and varies throughout the cardiac cycle. The base model by (<xref rid="R45" ref-type="bibr">Ursino, 1998</xref>) assumes that isometric pressure/volume can be characterised by an exponential function during diastole, when the ventricle is relaxed, and by a linear function at the end of systole, when the ventricle is contracted maximally. Thus, isometric pressure transitions between an exponential and linear function over the course of the cardiac cycle.
<disp-formula id="FD33">
<label>(33)</label>
<mml:math id="M92" display="block"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mi>&#x003c6;</mml:mi><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>E</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:mfenced open="[" close="]" separators="|"><mml:mrow><mml:mn>1</mml:mn><mml:mo>-</mml:mo><mml:mi>&#x003c6;</mml:mi><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mo>(</mml:mo><mml:mrow><mml:mrow><mml:mi mathvariant="normal">exp</mml:mi></mml:mrow><mml:mrow><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mrow><mml:mo>-</mml:mo><mml:mn>1</mml:mn></mml:math>
</disp-formula>
with <inline-formula><mml:math id="M93" display="inline"><mml:mn>0</mml:mn><mml:mspace width="0.5em"/><mml:mo>&#x02264;</mml:mo><mml:mspace width="0.5em"/><mml:mi>&#x003d5;</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>t</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mspace width="0.5em"/><mml:mo>&#x02264;</mml:mo><mml:mspace width="0.5em"/><mml:mn>1</mml:mn></mml:math></inline-formula>.</p><p id="P47"><inline-formula><mml:math id="M94" display="inline"><mml:msub><mml:mrow><mml:mi>E</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is the ventricular elastance at the maximal contraction of the ventricle. <inline-formula><mml:math id="M95" display="inline"><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>u</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is the corresponding unstressed volume of the ventricle and is the x-axis intercept of the end-systolic pressure/volume function. <inline-formula><mml:math id="M96" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> and <inline-formula><mml:math id="M97" display="inline"><mml:msub><mml:mrow><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>E</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> are constant parameters that describe the monoexponential pressure/volume function at diastole. The term <inline-formula><mml:math id="M98" display="inline"><mml:mi>&#x003d5;</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>t</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math></inline-formula> represents the &#x0201c;activation function&#x0201d; of the ventricle. When <inline-formula><mml:math id="M99" display="inline"><mml:mi>&#x003d5;</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>t</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mspace width="0.5em"/><mml:mo>=</mml:mo><mml:mspace width="0.5em"/><mml:mn>1</mml:mn></mml:math></inline-formula>, the ventricle is at maximum contraction, when <inline-formula><mml:math id="M100" display="inline"><mml:mi>&#x003d5;</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>t</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mspace width="0.5em"/><mml:mo>=</mml:mo><mml:mspace width="0.5em"/><mml:mn>0</mml:mn></mml:math></inline-formula>, it is at complete relaxation. This activation function is defined as:
<disp-formula id="FD34">
<label>(34)</label>
<mml:math id="M101" display="block"><mml:mi>&#x003c6;</mml:mi><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mfenced open="{" close="" separators="|"><mml:mrow><mml:mtable columnalign="center"><mml:mtr><mml:mtd><mml:mrow><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">sin</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mrow><mml:mfenced open="[" close="]" separators="|"><mml:mrow><mml:mfrac><mml:mrow><mml:mi>&#x003c0;</mml:mi><mml:mi mathvariant="normal">*</mml:mi><mml:mi>T</mml:mi><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>y</mml:mi><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced></mml:mrow></mml:mfrac><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>u</mml:mi></mml:mrow></mml:mfenced></mml:mrow></mml:mrow><mml:mo>,</mml:mo></mml:mtd><mml:mtd><mml:mn>0</mml:mn><mml:mo>&#x02264;</mml:mo><mml:mi>u</mml:mi><mml:mo>&#x02264;</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>y</mml:mi><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:mfrac></mml:mtd></mml:mtr><mml:mtr><mml:mtd columnalign="left"><mml:mn>0</mml:mn><mml:mo>,</mml:mo></mml:mtd><mml:mtd><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>y</mml:mi><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:mfrac><mml:mo>&#x02264;</mml:mo><mml:mi>u</mml:mi><mml:mo>&#x02264;</mml:mo><mml:mn>1</mml:mn></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p><p id="P48"><inline-formula><mml:math id="M102" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> represents the heart period (i.e., inverse of heart rate). <inline-formula><mml:math id="M103" display="inline"><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>y</mml:mi><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is the duration of systole and <inline-formula><mml:math id="M104" display="inline"><mml:mi>u</mml:mi></mml:math></inline-formula> is a dimensionless variable ranging between 0 and 1 and represents the fraction of the cardiac cycle. A value of <inline-formula><mml:math id="M105" display="inline"><mml:mi>u</mml:mi><mml:mo>=</mml:mo><mml:mn>0</mml:mn></mml:math></inline-formula> corresponds to the beginning of systole. This variable has been modeled as an integral pulse frequency modulation function.</p><disp-formula id="FD35">
<label>(35)</label>
<mml:math id="M106" display="block"><mml:mi>u</mml:mi><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mi>f</mml:mi><mml:mi>r</mml:mi><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mfenced open="[" close="]" separators="|"><mml:mrow><mml:mrow><mml:msubsup><mml:mo stretchy="false">&#x0222b;</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mi>t</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:msubsup><mml:mrow><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced></mml:mrow></mml:mfrac></mml:mrow></mml:mrow><mml:mi>d</mml:mi><mml:mi>&#x003c4;</mml:mi><mml:mo>+</mml:mo><mml:mi>u</mml:mi><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>t</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced></mml:math>
</disp-formula><p id="P49">The fractional part of this equation, frac[ ], indicates that the variable <inline-formula><mml:math id="M107" display="inline"><mml:mi>u</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>t</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math></inline-formula> is reset to zero as soon as the value reaches a value of 1.</p><p id="P50">The duration of systole is determined by the following equation:
<disp-formula id="FD36">
<label>(36)</label>
<mml:math id="M108" display="block"><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>y</mml:mi><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>y</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>y</mml:mi><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:mfrac></mml:math>
</disp-formula>
where <inline-formula><mml:math id="M109" display="inline"><mml:msub><mml:mrow><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>y</mml:mi><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> and <inline-formula><mml:math id="M110" display="inline"><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi><mml:mi>y</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mn>0</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> are constant parameters. A separate set of equations analogous to those above are used to describe the right heart as well.</p><sec id="S10"><title>Afferent input types</title><p id="P51">Like the baroreceptors, a first-order low-pass filter in series with a sigmoidal static characteristic function is used to model the cardiopulmonary receptors. Because cardiopulmonary receptors depend on transmural pressure at the pulmonary veins, this pressure difference is used as an input to first-order low-pass filter:
<disp-formula id="FD37">
<label>(37)</label>
<mml:math id="M111" display="block"><mml:msub><mml:mrow><mml:mi>&#x003c4;</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mfrac><mml:mrow><mml:mi>d</mml:mi><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mo>-</mml:mo><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:math>
</disp-formula>
<disp-formula id="FD38">
<label>(38)</label>
<mml:math id="M112" display="block"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mo>+</mml:mo><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi><mml:mfenced separators="|"><mml:mrow><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mrow></mml:mfenced></mml:mrow></mml:mfrac></mml:math>
</disp-formula></p><p id="P52">Here <inline-formula><mml:math id="M113" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>p</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is the transmural pressure at the pulmonary vein or input value to the low-pass filter function. <inline-formula><mml:math id="M114" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is the output variable of the low-pass filter. <inline-formula><mml:math id="M115" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is the spike frequency of the afferent fibers from the cardiopulmonary receptors and <inline-formula><mml:math id="M116" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>l</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is the upper saturation limit of the frequency discharge of these receptors, the lower limit being zero. <inline-formula><mml:math id="M117" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> represents the pulmonary venous pressure at the central point of the sigmoid curve. <inline-formula><mml:math id="M118" display="inline"><mml:msub><mml:mrow><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is another constant that determines the slope of the sigmoid curve, or sensitivity of the cardiopulmonary receptors.</p><p id="P53">Lung stretch receptors are modeled using a first-order lowpass filter:
<disp-formula id="FD39">
<label>(39)</label>
<mml:math id="M119" display="block"><mml:mfrac><mml:mrow><mml:mi>d</mml:mi><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>&#x003c4;</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>u</mml:mi><mml:mi>n</mml:mi><mml:mi>g</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mfenced separators="|"><mml:mrow><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>l</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>u</mml:mi><mml:mi>n</mml:mi><mml:mi>g</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p></sec><sec id="S11"><title>Sympathetic efferent outflow</title><p id="P54">Sympathetic efferent outflow is modeled to be dependent on the afferent input signals sent by the baroreceptor, cardiopulmonary, and lung stretch receptors. Moreover, the combined effects of these input signals affect sympathetic efferent outflow to different effector functions differently. Therefore, a series of calculations are included to determine i) the afferent firing frequency input that is then used to determine ii) the distinct sympathetic efferent outflow signals to the respective effector functions associated with the heart (<inline-formula><mml:math id="M120" display="inline"><mml:mi>h</mml:mi></mml:math></inline-formula>), peripheral circulation (<inline-formula><mml:math id="M121" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>), and unstressed volumes (<inline-formula><mml:math id="M122" display="inline"><mml:mi>v</mml:mi></mml:math></inline-formula>)
<disp-formula id="FD40">
<label>(40)</label>
<mml:math id="M123" display="block"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>b</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>l</mml:mi><mml:mi>h</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:math>
</disp-formula>
<disp-formula id="FD41">
<label>(41)</label>
<mml:math id="M124" display="block"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>b</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>l</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:math>
</disp-formula>
<disp-formula id="FD42">
<label>(42)</label>
<mml:math id="M125" display="block"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.5em"/><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>b</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>l</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:math>
</disp-formula></p><p id="P55"><inline-formula><mml:math id="M126" display="inline"><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>b</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>, where <inline-formula><mml:math id="M127" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula> is a general index for the heart, peripheral circulation, or unstressed volume, represents a constant gain factor indicating how much influence each afferent input has on determining sympathetic efferent outflow. A factor of &#x02212;1 is used for <inline-formula><mml:math id="M128" display="inline"><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>l</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> as this provided the best fits for the model. The resulting <inline-formula><mml:math id="M129" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.5em"/><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> values are then used to determine sympathetic efferent outflow to the respective effector functions using a negative monotonic function to relate afferent activity to efferent neural pathways,
<disp-formula id="FD43">
<label>(43)</label>
<mml:math id="M130" display="block"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">&#x0221e;</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">&#x0221e;</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mo>-</mml:mo><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:math>
</disp-formula>
<disp-formula id="FD44">
<label>(44)</label>
<mml:math id="M131" display="block"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">&#x0221e;</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">&#x0221e;</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mo>-</mml:mo><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:math>
</disp-formula>
<disp-formula id="FD45">
<label>(45)</label>
<mml:math id="M132" display="block"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">&#x0221e;</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">&#x0221e;</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mo>-</mml:mo><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p><p id="P56">Lung volume, thoracic, and abdominal pressures A linear relationship between lung volume and thoracic pressure is used to model lung volume measured by the lung stretch receptors:
<disp-formula id="FD46">
<label>(46)</label>
<mml:math id="M133" display="block"><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>u</mml:mi><mml:mi>n</mml:mi><mml:mi>g</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>l</mml:mi><mml:mi>u</mml:mi><mml:mi>n</mml:mi><mml:mi>g</mml:mi><mml:mo>,</mml:mo><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mn>0.1</mml:mn><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub></mml:math>
</disp-formula></p><p id="P57">Thoracic pressure varies with time due to the effects of the respiratory cycle, which is modeled independently from any autonomic regulation. Parameters were chosen based on experimental work by (<xref rid="R31" ref-type="bibr">Moreno et al., 1969</xref>). Thoracic pressure varies linearly during respiration between a minimum of &#x02212;9 mm Hg and a maximum of &#x02212;4 mm Hg, which represents steady-state thoracic pressure during the respiratory pause, as modeled by the following equations:
<disp-formula id="FD47">
<label>(47)</label>
<mml:math id="M134" display="block"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfenced open="{" close="" separators="|"><mml:mrow><mml:mtable><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.5em"/><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>s</mml:mi><mml:mspace width="0.5em"/><mml:mspace width="0.5em"/><mml:mspace width="0.5em"/><mml:mspace width="0.5em"/><mml:mspace width="0.5em"/><mml:mspace width="0.5em"/><mml:mspace width="0.5em"/><mml:mspace width="0.5em"/><mml:mspace width="0.5em"/><mml:mn>0</mml:mn><mml:mspace width="0.5em"/><mml:mo>&#x02264;</mml:mo><mml:mi>s</mml:mi><mml:mo>&#x02264;</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mfrac><mml:mrow><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mi>s</mml:mi><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced><mml:mo>,</mml:mo><mml:mspace width="0.5em"/><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mspace width="0.5em"/><mml:mo>&#x02264;</mml:mo><mml:mi>s</mml:mi><mml:mo>&#x02264;</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:mspace width="8em"/><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>&#x02264;</mml:mo><mml:mi>s</mml:mi><mml:mo>&#x02264;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p><p id="P58">Where <inline-formula><mml:math id="M135" display="inline"><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is the period of respiration. <inline-formula><mml:math id="M136" display="inline"><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is the inspiration time, <inline-formula><mml:math id="M137" display="inline"><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is the expiration time. <inline-formula><mml:math id="M138" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.5em"/><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is the value of the intrathoracic pressure at the end of inspiration while <inline-formula><mml:math id="M139" display="inline"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mi>h</mml:mi><mml:mi>o</mml:mi><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mspace width="0.5em"/><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> is the max value of intrathoracic pressure at the end of expiration and throughout the respiratory pause, which takes place in between each respiration period. The parameter <inline-formula><mml:math id="M140" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula> is dimensionless, varying between 0 and 1, and represents the fraction of the respiratory cycle. A value of 0 represents the beginning of the respiration cycle. Similar to other parameters representing a fraction of cycle completion, an expression for <inline-formula><mml:math id="M141" display="inline"><mml:mi>s</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>t</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math></inline-formula> has been developed by introducing yet another state variable <inline-formula><mml:math id="M142" display="inline"><mml:mi>&#x003f5;</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>t</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math></inline-formula>, which is determined by the following equation:
<disp-formula id="FD48">
<label>(48)</label>
<mml:math id="M143" display="block"><mml:mfrac><mml:mrow><mml:mi>d</mml:mi><mml:mi>&#x003b5;</mml:mi></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:math>
</disp-formula>
with <inline-formula><mml:math id="M144" display="inline"><mml:mi>s</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>t</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mspace width="0.5em"/><mml:mo>=</mml:mo><mml:mspace width="0.5em"/><mml:mi>f</mml:mi><mml:mi>r</mml:mi><mml:mi>a</mml:mi><mml:mi>c</mml:mi><mml:mo>(</mml:mo><mml:mi>&#x003f5;</mml:mi><mml:mo>)</mml:mo></mml:math></inline-formula>.</p><p id="P59">Abdominal pressure is modeled similarly:
<disp-formula id="FD49">
<label>(49)</label>
<mml:math id="M145" display="block"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi><mml:mi>b</mml:mi><mml:mi>d</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfenced open="{" close="" separators="|"><mml:mrow><mml:mtable columnalign="center"><mml:mtr><mml:mtd><mml:mo>-</mml:mo><mml:mn>2.5</mml:mn><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>s</mml:mi><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo>/</mml:mo><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:mrow></mml:mrow></mml:mfrac><mml:mo>-</mml:mo><mml:mn>4</mml:mn></mml:mtd><mml:mtd><mml:mn>0</mml:mn><mml:mo>&#x0003c;</mml:mo><mml:mi>s</mml:mi><mml:mo>&#x0003c;</mml:mo><mml:mfrac><mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo>/</mml:mo><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:mrow></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr><mml:mtr><mml:mtd columnalign="left"><mml:mo>-</mml:mo><mml:mn>2.5</mml:mn></mml:mtd><mml:mtd><mml:mfrac><mml:mrow><mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo>/</mml:mo><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:mrow></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>&#x0003c;</mml:mo><mml:mi>s</mml:mi><mml:mo>&#x0003c;</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr><mml:mtr><mml:mtd columnalign="left"><mml:mo>-</mml:mo><mml:mn>2.5</mml:mn><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mi>s</mml:mi><mml:mi mathvariant="normal">*</mml:mi><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd><mml:mtd columnalign="left"><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>&#x0003c;</mml:mo><mml:mi>s</mml:mi><mml:mo>&#x0003c;</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mo>-</mml:mo><mml:mn>5</mml:mn><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:mi>s</mml:mi><mml:mi mathvariant="normal">*</mml:mi><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>-</mml:mo><mml:mn>4</mml:mn></mml:mtd><mml:mtd columnalign="left"><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>&#x0003c;</mml:mo><mml:mi>s</mml:mi><mml:mo>&#x0003c;</mml:mo><mml:mn>1</mml:mn></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:mfenced></mml:math>
</disp-formula></p><p id="P60">Where <inline-formula><mml:math id="M146" display="inline"><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> represents the respiratory period, <inline-formula><mml:math id="M147" display="inline"><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> represents the duration of inspiration and <inline-formula><mml:math id="M148" display="inline"><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>x</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> represents the duration of expiration. <inline-formula><mml:math id="M149" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula> is a dimensionless variable, which is the same as <xref rid="FD47" ref-type="disp-formula">Eq. 47</xref>.</p></sec><sec id="S12"><title>Respiratory sinus arrhythmia</title><p id="P61">A gating function to modulate the outputs of the NTS that go to the NA (<inline-formula><mml:math id="M150" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>N</mml:mi><mml:mi>A</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>p</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>) based on the phase of the respiratory cycle was added to the extended model to capture RSA. The respiratory phase, <inline-formula><mml:math id="M151" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula>, varies between zero and one and resets to zero at the end of each respiratory cycle. The inspiration and post-inhalation phases of s are defined using the inhalation time (<inline-formula><mml:math id="M152" display="inline"><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>) divided by the total respiratory cycle time (<inline-formula><mml:math id="M153" display="inline"><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>). During inspiration, outputs from the NTS (<inline-formula><mml:math id="M154" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>N</mml:mi><mml:mi>T</mml:mi><mml:mi>S</mml:mi><mml:mo>,</mml:mo><mml:mi>o</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi><mml:mi>p</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>) are decreased by the gain value (<inline-formula><mml:math id="M155" display="inline"><mml:msub><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>S</mml:mi><mml:mi>A</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>), and during exhalation, outputs from the NTS are unaffected to mimic the observed NA input gating behaviour.</p><disp-formula id="FD50">
<label>(50)</label>
<mml:math id="M156" display="block"><mml:msub><mml:mrow><mml:mi>f</mml:mi><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>N</mml:mi><mml:mi>A</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>p</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mfenced open="{" close="" separators="|"><mml:mrow><mml:mtable columnalign="right"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>S</mml:mi><mml:mi>A</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>f</mml:mi><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>N</mml:mi><mml:mi>T</mml:mi><mml:mi>S</mml:mi><mml:mo>,</mml:mo><mml:mi>o</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi><mml:mi>p</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo></mml:mtd><mml:mtd><mml:mi>s</mml:mi><mml:mo>&#x0003c;</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>f</mml:mi><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>N</mml:mi><mml:mi>T</mml:mi><mml:mi>S</mml:mi><mml:mo>,</mml:mo><mml:mi>o</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi><mml:mi>p</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo></mml:mtd><mml:mtd><mml:mi>s</mml:mi><mml:mo>&#x02265;</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:mfenced></mml:math>
</disp-formula></sec><sec id="S13"><title>Intrinsic cardiac nervous system</title><p id="P62">We included in the model a first-order filter on the output of principal neurons that receive direct inputs from the dorsal motor nucleus. This filter is added to represent the slower dynamics of signal transmission due to the muscarinic receptor type that this population of neurons uses. The output, filtered (<inline-formula><mml:math id="M157" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>f</mml:mi><mml:mi>i</mml:mi><mml:mi>l</mml:mi><mml:mi>t</mml:mi><mml:mi>e</mml:mi><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>d</mml:mi><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mi>N</mml:mi></mml:mrow><mml:mrow><mml:mi>D</mml:mi><mml:mi>M</mml:mi><mml:mi>V</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:math></inline-formula>) is delayed by <inline-formula><mml:math id="M158" display="inline"><mml:msub><mml:mrow><mml:mi>&#x003c4;</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi><mml:mi>N</mml:mi></mml:mrow><mml:mrow><mml:mi>D</mml:mi><mml:mi>M</mml:mi><mml:mi>V</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:math></inline-formula> compared to the input (<inline-formula><mml:math id="M159" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>o</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mi>N</mml:mi></mml:mrow><mml:mrow><mml:mi>D</mml:mi><mml:mi>M</mml:mi><mml:mi>V</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:math></inline-formula>).</p><disp-formula id="FD51">
<label>(51)</label>
<mml:math id="M160" display="block"><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>d</mml:mi><mml:mi>f</mml:mi><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>f</mml:mi><mml:mi>i</mml:mi><mml:mi>l</mml:mi><mml:mi>t</mml:mi><mml:mi>e</mml:mi><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>d</mml:mi><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mi>N</mml:mi></mml:mrow><mml:mrow><mml:mi>D</mml:mi><mml:mi>M</mml:mi><mml:mi>V</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>&#x003c4;</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi><mml:mi>N</mml:mi></mml:mrow><mml:mrow><mml:mi>D</mml:mi><mml:mi>M</mml:mi><mml:mi>V</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>f</mml:mi><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>o</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi><mml:mi>N</mml:mi></mml:mrow><mml:mrow><mml:mi>D</mml:mi><mml:mi>M</mml:mi><mml:mi>V</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>f</mml:mi><mml:mi>i</mml:mi><mml:mi>l</mml:mi><mml:mi>t</mml:mi><mml:mi>e</mml:mi><mml:mi>r</mml:mi><mml:mi>e</mml:mi><mml:mi>d</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mrow><mml:mi>P</mml:mi><mml:mi>N</mml:mi></mml:mrow><mml:mrow><mml:mi>D</mml:mi><mml:mi>M</mml:mi><mml:mi>V</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:math>
</disp-formula><p id="P63">Inputs to the local circuit neurons are a linear combination of firing frequencies from the baroreceptors (<inline-formula><mml:math id="M161" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>B</mml:mi><mml:mi>R</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>), cardiopulmonary receptors (<inline-formula><mml:math id="M162" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>C</mml:mi><mml:mi>P</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>), sympathetic efferent firing frequency (<inline-formula><mml:math id="M163" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>f</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>h</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>), and vagal efferent firing frequency (<inline-formula><mml:math id="M164" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>f</mml:mi><mml:mi>e</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>) multiplied by their respective gain values.</p><disp-formula id="FD52">
<label>(52)</label>
<mml:math id="M165" display="block"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>p</mml:mi><mml:mi>u</mml:mi><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>L</mml:mi><mml:mi>C</mml:mi><mml:mi>N</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>L</mml:mi><mml:mi>C</mml:mi><mml:mi>N</mml:mi></mml:mrow><mml:mrow><mml:mi>B</mml:mi><mml:mi>R</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>L</mml:mi><mml:mi>C</mml:mi><mml:mi>N</mml:mi></mml:mrow><mml:mrow><mml:mi>C</mml:mi><mml:mi>P</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>L</mml:mi><mml:mi>C</mml:mi><mml:mi>N</mml:mi></mml:mrow><mml:mrow><mml:mi>f</mml:mi><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>h</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mi>h</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>L</mml:mi><mml:mi>C</mml:mi><mml:mi>N</mml:mi></mml:mrow><mml:mrow><mml:mi>f</mml:mi><mml:mi>e</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math>
</disp-formula></sec><sec id="S14"><title>Heart period</title><p id="P64">We have modified the original model developed by (<xref rid="R45" ref-type="bibr">Ursino, 1998</xref>) and its subsequent iterations (<xref rid="R46" ref-type="bibr">Ursino &#x00026; Magosso, 2000</xref>; <xref rid="R28" ref-type="bibr">Magosso et al., 2002</xref>; <xref rid="R29" ref-type="bibr">Magosso &#x00026; Ursino, 2002</xref>), to account for the differences in the effect vagal activity has depending on when in the cardiac cycle it occurs. The same functions as Ursino (<xref rid="FD53" ref-type="disp-formula">Eqs. 53</xref>&#x02013;<xref rid="FD56" ref-type="disp-formula">56</xref>) are used to calculate the change in heart period from baseline due to vagal activity (<inline-formula><mml:math id="M166" display="inline"><mml:mi mathvariant="normal">&#x00394;</mml:mi><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>).</p><disp-formula id="FD53">
<label>(53)</label>
<mml:math id="M167" display="block"><mml:msub><mml:mrow><mml:mi>&#x003c3;</mml:mi></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mfenced open="{" close="" separators="|"><mml:mrow><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mi>l</mml:mi><mml:mi>n</mml:mi><mml:mfenced open="[" close="]" separators="|"><mml:mrow><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003b8;</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mtd><mml:mtd><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi></mml:mrow></mml:msub><mml:mo>&#x02265;</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mn>0</mml:mn><mml:mo>,</mml:mo></mml:mtd><mml:mtd><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi></mml:mrow></mml:msub><mml:mo>&#x0003c;</mml:mo><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:mfenced></mml:math>
</disp-formula><disp-formula id="FD54">
<label>(54)</label>
<mml:math id="M168" display="block"><mml:mfrac><mml:mrow><mml:mi>d</mml:mi><mml:mi mathvariant="normal">&#x00394;</mml:mi><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x003c4;</mml:mi></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mfenced separators="|"><mml:mrow><mml:mo>-</mml:mo><mml:mi mathvariant="normal">&#x00394;</mml:mi><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>&#x003c3;</mml:mi></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced></mml:math>
</disp-formula><disp-formula id="FD55">
<label>(55)</label>
<mml:math id="M169" display="block"><mml:msub><mml:mrow><mml:mi>&#x003c3;</mml:mi></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>G</mml:mi></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi><mml:mi>v</mml:mi><mml:mo>,</mml:mo><mml:mi>h</mml:mi></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfenced></mml:math>
</disp-formula><disp-formula id="FD56">
<label>(56)</label>
<mml:math id="M170" display="block"><mml:mfrac><mml:mrow><mml:mi>d</mml:mi><mml:mi mathvariant="normal">&#x00394;</mml:mi><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mi>d</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.5em"/></mml:mrow></mml:mfrac><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x003c4;</mml:mi></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mspace width="0.5em"/><mml:mi mathvariant="normal">*</mml:mi><mml:mspace width="0.5em"/><mml:mfenced separators="|"><mml:mrow><mml:mo>-</mml:mo><mml:mi mathvariant="normal">&#x00394;</mml:mi><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo>+</mml:mo><mml:msub><mml:mrow><mml:mi>&#x003c3;</mml:mi></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>v</mml:mi></mml:mrow></mml:msub><mml:mfenced separators="|"><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced></mml:math>
</disp-formula><p id="P65">The change in heart period due to vagal activity is then modified using a gain value calculated from data on the change in heart period as a function of the timing of vagal activity in the cardiac cycle in dogs by (<xref rid="R24" ref-type="bibr">Levy et al., 1972</xref>; <xref rid="R15" ref-type="bibr">Iano et al., 1973</xref>).</p><p id="P66">In equation S.6, the timing of the stimulus (<inline-formula><mml:math id="M171" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>) was measured as the time which had elapsed between the application of the stimulus (<inline-formula><mml:math id="M172" display="inline"><mml:msub><mml:mrow><mml:mi>t</mml:mi></mml:mrow><mml:mrow><mml:mi>f</mml:mi><mml:mi>e</mml:mi><mml:mi>v</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>) and the midpoint, in time (<inline-formula><mml:math id="M173" display="inline"><mml:msub><mml:mrow><mml:mi>t</mml:mi></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>R</mml:mi><mml:mo>,</mml:mo><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>d</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula>), of that cardiac cycle (<xref rid="R15" ref-type="bibr">Iano et al., 1973</xref>). The gain value to be multiplied by the change in heart period was determined using <xref rid="FD60" ref-type="disp-formula">Eq. 60</xref>, which is a function fit to data from (<xref rid="R15" ref-type="bibr">Iano et al., 1973</xref>). The constants in <xref rid="FD60" ref-type="disp-formula">Eq. 60</xref> were selected to fit the experimental data curve for the relationship between the heart period change and the timing of the stimulus relative to the midpoint of the cardiac cycle as found by (<xref rid="R15" ref-type="bibr">Iano et al., 1973</xref>). Because vagal activity affects the subsequent cardiac cycle in addition to the current one, the gain values were split into <inline-formula><mml:math id="M174" display="inline"><mml:msub><mml:mrow><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>R</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:math></inline-formula> and <inline-formula><mml:math id="M175" display="inline"><mml:msub><mml:mrow><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>R</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> to modify the effect of vagal activity on heart period for the current and subsequent cardiac cycles. For example, if <xref rid="R15" ref-type="bibr">Iano et al., 1973</xref> found that heart period increased by 10 percent for vagal activity that occurred at a given point in the cardiac cycle, then the gain value would be 1.1. If the next cardiac cycle started within a time range such that the stimulus still had an effect on it, that gain value was determined from <xref rid="FD60" ref-type="disp-formula">Eq. 60</xref> to obtain the gain value <inline-formula><mml:math id="M176" display="inline"><mml:msub><mml:mrow><mml:mi>k</mml:mi></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>R</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula>.</p><disp-formula id="FD57">
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</disp-formula></sec></sec><sec id="S15"><label>G.</label><title>Credible practice in modelling</title><p id="P67">This work followed the Ten Simple Rules of Credible Modelling and Simulation in Healthcare (<xref rid="R8" ref-type="bibr">Erdemir et al., 2020</xref>) and the associated rubric is included on GitHub (<ext-link xlink:href="https://github.com/Daniel-Baugh-Institute/CardiovascularControl/tree/main/Virtual_patient_cohorts" ext-link-type="uri">https://github.com/Daniel-Baugh-Institute/CardiovascularControl/tree/main/Virtual_patient_cohorts</ext-link>). The Ten Simple Rules are a conceptual framework for modelling and simulation design, implementation, evaluation, dissemination, and usage in healthcare. The rules cover best practices on model documentation, purpose, limitations, and independent reviews. We evaluated our model with the Ten Simple Rules and found that the model complies with each rule adequately to extensively.</p></sec></sec><sec id="S16"><label>III.</label><title>RESULTS</title><sec id="S17"><label>A.</label><title>Generation of an in silico patient cohort</title><p id="P68">To account for the inter-individual variability, we generated a cohort of 59 individual models that produced baroreflex curves within the range of behaviour observed experimentally (<xref rid="F2" ref-type="fig">Fig. 2</xref>) (<xref rid="R30" ref-type="bibr">Mastitskaya et al., 2012</xref>; <xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>). To generate the cohort, we started with a model based on that of (<xref rid="R11" ref-type="bibr">Gee et al., 2023</xref>) that fit the average of the baroreflex curve data from five individuals (<xref rid="F3" ref-type="fig">Fig. 3B</xref>) (<xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>). The model includes 51 parameters that represent the neuronal groups in the baroreflex arc as well as left ventricular function. To select parameters that affect HR and MAP, we used a parametric sensitivity analysis known as PAWN. Of the 51 parameters, 28 significantly affected HR and/or MAP (<xref rid="F3" ref-type="fig">Fig. 3A</xref>). These 28 parameter values were then varied simultaneously over a &#x000b1;2.5 fold range from the nominal parameter values to generate 500 potential individual models. Given that a large number of parameters were selected (28) and the possibility of degenerate models, we considered the possibility of over-fitting. Thus, the criteria for accepted models were based on neck chamber pressure responses over a range of perturbation pressures. Each individual model prediction of the baroreflex curve was fit to <xref rid="FD1" ref-type="disp-formula">Eq. 1</xref> to quantitatively describe each model using parameters representing (1) the response range (maximum-minimum), (2) slope of the sigmoid, (3) centering point of the sigmoid, and (4) minimum response were within the range observed experimentally (<xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>). The models were filtered so that the parameter values for the sigmoid fit are within the 95% confidence intervals based on the data from the five individuals reported in <xref rid="R42" ref-type="bibr"><italic toggle="yes">Seredynski et al</italic>, 2021</xref>. Additionally, the minimum and maximum RR interval values were required to be within the pre-I/R 95% confidence interval observed for HR and MAP (<xref rid="R30" ref-type="bibr">Mastitskaya et al., 2012</xref>) and the maximum RR interval was required to be not greater than 1.2 seconds (<xref rid="F3" ref-type="fig">Fig. 3C</xref>). While the range of the values for accepted parameter sets for any individual criterion usually overlaps with the range of the values for the rejected parameter sets, only 59 of the 500 individual patient models generated satisfied these criteria simultaneously (<xref rid="F3" ref-type="fig">Fig. 3D</xref>). Rather than try to fit models any one individual, this method generates a cohort of plausible individuals that cover the range of baroreflex characteristics observed clinically.</p></sec><sec id="S18"><label>B.</label><title>Cardiac remodelling alone partly accounts for post-MI baroreflex control</title><p id="P69">The cardiac parameters identified via sensitivity analysis were used to develop post-I/R models from each of the 59 pre-I/R models (<xref rid="F4" ref-type="fig">Fig. 4A</xref>). Post-I/R RR interval and MAP were modeled to represent the time point following 30 minutes of myocardial ischemia and 120 minutes of reperfusion (<xref rid="F4" ref-type="fig">Fig. 4B</xref>). One hundred post-I/R models were generated for each pre-I/R model using Sobol sampling in a &#x000b1;1.5 fold range from the respective pre-I/R parameter values, for a total of 5,900 post-I/R models. The post-I/R models were filtered based on the following criteria calculated from the 95% confidence interval of clinical data: (1) heart rate between 58 and 116 bpm, (2) systolic pressure between 96 and 142 mm Hg, and (3) RR interval response to neck chamber pressures of 8, 13.2, 18.5, 23.7, 30, and 37.5 mm Hg (<xref rid="R34" ref-type="bibr">Osculati et al., 1990</xref>). If multiple plausible post-I/R models were found for a single pre-I/R model, they were all included in the analysis. Of the 5,900 parameter sets sampled, 85 post-I/R parameter sets met the criteria.</p></sec><sec id="S19"><label>C.</label><title>Adaptation in neural loci after ischemia</title><p id="P70">Because autonomic changes accompany myocardial remodelling in acute MI, we developed alternative computational models (<xref rid="F1" ref-type="fig">Fig. 1</xref>) to represent cardiac changes coupled with autonomic changes at different loci in the baroreflex arc (baroreceptors, NTS, NA/DMV, ICN). We start peripherally at the baroreceptors (<xref rid="F5" ref-type="fig">Fig. 5A</xref>) and proceed through the baroreflex arc to the brainstem nuclei, then back down to the ICN. Baroreceptor adaptation coupled with cardiac changes yielded 88 out of 5,900 post-IR models that matched the criteria involving baseline MAP (<xref rid="F5" ref-type="fig">Fig. 5B</xref>) and RR interval (<xref rid="F5" ref-type="fig">Fig. 5C</xref>) ranges as well as the baroreflex curve (<xref rid="F5" ref-type="fig">Fig. 5D</xref>). The final number of accepted models for cardiac remodelling combined with baroreceptor adaptation is similar to the number of accepted models for only cardiac remodelling. These results suggest there are many degenerate ways in which the baroreflex can adapt. There is a significant amount of diversity in baroreflex behaviour that still remains within the bounded space for baroreflex function and there are several loci that can adapt to account for the hemodynamics observed post-I/R.</p><p id="P71">Comparison of the baroreceptor adaptation coupled with cardiac remodelling pre- and post-I/R baroreflex response curves reveals significant overlap (<xref rid="F5" ref-type="fig">Fig. 5E</xref>). The baroreceptor response curves vary in the gain value representing the incremental increase in firing rate for a given arterial pressure increase. While there is a decrease in the baroreceptor gain from pre- to post-I/R due to the parametric constraints enforced during model development, the range of pre- and post-I/R baroreceptor responses overlaps. These results suggest that decreases in baroreceptor sensitivity post-I/R can be responsible for heart rate and blood pressure changes in some individuals, but in others the afferent pathway is intact and the defect is in cardiac dysfunction.</p></sec><sec id="S20"><label>D.</label><title>Central versus peripheral adaptation post-MI</title><p id="P72">The post-I/R cohort of models representing central adaptation in the NTS and NA/DMV coupled with cardiac remodelling yield similar numbers of accepted models (<xref rid="F6" ref-type="fig">Fig. 6A</xref>). Of the 5,900 post-I/R models screened for each model alternative, 75 NTS adaptation models and 86 NA/DMV adaptation models met the screening criteria for MAP (<xref rid="F6" ref-type="fig">Fig. 6C</xref>), RR interval (<xref rid="F6" ref-type="fig">Fig. 6D</xref>), and baroreflex curve (<xref rid="F6" ref-type="fig">Fig. 6B</xref>). The number of accepted models is comparable to that for other loci of adaptation, suggesting that adaptation in any of these loci are plausible or that there are many degenerate ways in which the baroreflex can adapt post-I/R. These <italic toggle="yes">in silico</italic> patients are within the clinically observed baroreflex behaviour, but it is apparent that the individuals that adapted via the NTS neuronal group pathway have a more limited range of baroreflex curves. NTS adaptation may not be as suitable for maintenance of baroreflex function as a result.</p><p id="P73">Cardiac remodelling coupled with peripheral ganglionic adaptations in the ICN could also account for the hemodynamic changes observed post-I/R (<xref rid="F7" ref-type="fig">Fig. 7A</xref>). Of the 5,900 post-I/R models sampled, 93 models recapitulated the experimentally observed MAP decrease (<xref rid="F7" ref-type="fig">Fig. 7B</xref>) and RR interval changes (<xref rid="F7" ref-type="fig">Fig. 7C</xref>) in addition to the baroreflex curve (<xref rid="F7" ref-type="fig">Fig. 7D</xref>). Because the central versus peripheral contributions to neural adaptation post-I/R have been of interest, we investigated the shift in balance between central and peripheral neural loci before and after cardiac injury in all post-I/R models. To quantify the contribution of central and peripheral model parameters, we use Shapley values, which are used in game theory to calculate the contribution of each player in a coalition game. The average pre-I/R Shapley values are higher for parameters representing peripheral loci compared to central loci. This balance shifts post-I/R so that the contributions of central loci to heart rate regulation are greater.</p></sec><sec id="S21"><label>E.</label><title>Combinatorial adaptation in all neural loci</title><p id="P74">While we had hypothesised that adaptation in a subset of neural loci was sufficient to maintain baroreflex function post-I/R, it is also possible that cardiac remodelling is coupled with simultaneous adaptation in all neural loci (<xref rid="F8" ref-type="fig">Fig. 8A</xref>). Of the 5,900 post-I/R models considered, 72 of the models met the criteria (<xref rid="F8" ref-type="fig">Fig. 8 B</xref> and <xref rid="F8" ref-type="fig">C</xref>) in addition to the baroreflex curve requirements (<xref rid="F8" ref-type="fig">Fig. 8D</xref>). These results suggest that simultaneous adaptation in these neural loci coupled with cardiac changes are sufficient to match the experimentally observed hemodynamic and autonomic changes. The possibility of a baroreflex-wide response to ischemic injury could not be ruled out.</p></sec><sec id="S22"><label>F.</label><title>Adaptation along vagal efferent pathway can compensate for cardiac injury</title><p id="P75">A t-distributed stochastic neighbor embedding (t-SNE) was performed to visualize the output characteristics of each post-I/R model (<xref rid="F9" ref-type="fig">Fig. 9</xref>). These characteristics include vagal afferent activity, vagal efferent activity, and baroreceptor responsivity. The clustering analysis revealed a sub-group of post-I/R individuals in the virtual cohort with high baroreflex sensitivity (<xref rid="F9" ref-type="fig">Fig. 9A</xref>). These individuals tended to adapt via the ICN, NA, and DMV&#x02014; peripheral and central vagal efferent pathways (<xref rid="F9" ref-type="fig">Fig. 9B</xref>). The individuals in the virtual cohort with high baroreflex sensitivity also stemmed from a subgroup of pre-I/R individuals with high baroreceptor responsivity (<xref rid="F9" ref-type="fig">Fig. 9C</xref>). Taken together, these results suggest that central or peripheral vagal efferent adaptation and preserved baroreceptor gain may be sufficient to maintain high baroreflex sensitivity (BRS) post MI. No trends between baroreflex sensitivity and the ratio of central versus peripheral contributions to heart rate were identified, reinforcing the idea that vagal efferent dysfunction contributes to poor baroreflex sensitivity post-I/R rather than central versus peripheral imbalance.</p></sec></sec><sec id="S23"><label>IV.</label><title>DISCUSSION</title><p id="P76">We developed an ensemble of <italic toggle="yes">in silico</italic> patient models of the baroreflex capturing cardiac and autonomic physiology pre- and post-I/R to address the question posed in the white paper by <xref rid="R14" ref-type="bibr">Herring et al., 2024</xref> of how localized pathology in the heart affects adaptation in specific regions of the neural hierarchy and the influence on the behaviour of the system as a whole. Because autonomic adaptation is known to occur to compensate for lost cardiac function, we tested alternative models representing adaptation in sensory afferent, central, and peripheral ganglionic loci coupled with cardiac remodelling. The virtual patient cohort was filtered using observed hemodynamic behaviour with baseline MAP, RR interval, and baroreflex curves within the 95% confidence intervals (<xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>) and trends in MAP and RR interval changes before and after (<xref rid="R30" ref-type="bibr">Mastitskaya et al., 2012</xref>). We found a subgroup of <italic toggle="yes">in silico</italic> patients that maintained higher baroreflex sensitivity post-I/R. These individuals adapted via central or peripheral vagal efferent neural loci and had preserved baroreceptor gain. There were also individuals with preserved baroreceptor gain that did not adapt along the vagal efferent pathway who had lower baroreflex sensitivity, highlighting the role of adaptation in parasympathetic efferent nuclei in maintaining cardiac health post-I/R. These model predictions lead to the experimentally testable hypothesis that correlations between post-I/R baroreflex sensitivity and electrophysiological or transcriptomic measurements of neural adaptation may exist.</p><p id="P77">The model suggests that preserved baroreceptor responsivity after cardiac injury is necessary for maintaining baroreflex sensitivity. These results are in agreement with several experiments in animal models showing that there is both denervation around the infarcted area and functional transmission changes (<xref rid="R41" ref-type="bibr">Salavatian et al., 2022</xref>; <xref rid="R17" ref-type="bibr">Kazci et al., 2022</xref>). Paradoxically, the number of neurons in the nodose ganglia was increased, but functional transmission decreased in a porcine model of cardiac injury. Impaired afferent transmission is also associated with decreased vagal tone, which increases the risk of ventricular arrhythmias and heart failure (<xref rid="R41" ref-type="bibr">Salavatian et al., 2022</xref>). When performed prior to myocardial infarction, sinoaortic denervation has been found to induce additional impairment of vagal activity in rats (<xref rid="R32" ref-type="bibr">Mostarda et al., 2014</xref>). In a porcine model of cardiac ischemic injury, decreased functional afferent transmission is thought to contribute to vagal withdrawal, further impairing baroreflex function (<xref rid="R47" ref-type="bibr">Vaseghi et al., 2017</xref>; <xref rid="R48" ref-type="bibr">van Weperen &#x00026; Vaseghi, 2023</xref>). Likewise, the computational model results suggest that impaired baroreceptor function blunts overall baroreflex sensitivity, which is correlated with vagal tone (<xref rid="R19" ref-type="bibr">Kollai et al., 1994</xref>).</p><p id="P78">Resetting of the baroreceptor firing rate is a well-studied mechanism in baroreflex adaptation (<xref rid="R20" ref-type="bibr">Kosinski et al., 2018</xref>; <xref rid="R16" ref-type="bibr">Jezek et al., 2022</xref>). Baroreceptors can adapt to a new steady-state blood pressure that shifts the entire curve to the left or right if the arterial pressure is elevated for longer than 3&#x02013;5 minutes (<xref rid="R21" ref-type="bibr">Kunze, 1985</xref>). This mechanism is likely a major driver of changes in baroreflex control post-I/R. While this baroreceptor resetting was not explicitly included in the model, it is implicitly included when the parameters are resampled between pre- and post-I/R. The post-I/R baroreceptor parameters reflect the reset baroreceptors. Furthermore, a central component to baroreflex resetting has been suggested (<xref rid="R21" ref-type="bibr">Kunze, 1985</xref>; <xref rid="R7" ref-type="bibr">DiCarlo &#x00026; Bishop, 2001</xref>). The resampling of parameters representing central brainstem nuclei post-I/R also implicitly represent baroreflex resetting.</p><p id="P79">Adaptation in parasympathetic efferent nuclei post-I/R was necessary to maintain baroreflex function in most individuals. While neural adaptation is difficult to regulate, vagus nerve stimulation (VNS) can restore afferent and efferent vagal tone after myocardial infarction and during the subsequent development of heart failure (<xref rid="R13" ref-type="bibr">Hadaya et al., 2023</xref>). Increasing parasympathetic drive with vagus nerve stimulation following myocardial infarction in a chronic porcine infarct model decreased ventricular arrhythmia inducibility (<xref rid="R47" ref-type="bibr">Vaseghi et al., 2017</xref>). These results support the idea that augmenting vagal efferent tone after infarction can improve autonomic regulation of cardiovascular function. During pacing-induced heart failure development, cervical VNS was found to improve baroreflex sensitivity, heart rate variability, and ejection fraction in a canine model (<xref rid="R50" ref-type="bibr">Zhang et al., 2009</xref>). While cervical VNS stimulates both afferent and efferent vagal fibers, auricular VNS stimulates predominantly afferent fascicles. In a meta-analysis of six auricular VNS studies in humans, only one found a significant effect on BRS, supporting the idea that augmented vagal efferent tone improves BRS (<xref rid="R43" ref-type="bibr">Soltani et al., 2023</xref>). However, all six studies were in healthy subjects, who tend to experience less of an effect compared to those with poor autonomic function according to some studies (<xref rid="R43" ref-type="bibr">Soltani et al., 2023</xref>). It is also difficult to make a direct comparison between transcutaneous auricular VNS and cervical VNS due to necessary differences in stimulation level to produce similar physiological effects. Due to limitations in the current literature available, the model prediction that vagal efferent adaptation may be necessary to maintain BRS post-I/R is testable with a dataset that includes post-I/R stimulation of the cervical and auricular vagus normalized based on heart rate changes to see if afferent versus efferent stimulation improves BRS.</p><p id="P80">This model captures the progression of cardiovascular physiology from pre-I/R to the acute phase of post-I/R but has several limitations. Due to mismatch of the experimental data used to parameterize the pre- and post-I/R models, the average baroreflex sensitivity, characterised by the slope of the baroreflex curve, is higher post-I/R. It is well known that baroreflex sensitivity decreases post-I/R and that lower baroreflex sensitivity is associated with the progression of cardiovascular disease (<xref rid="R22" ref-type="bibr">La Rovere et al., 1998</xref>, <xref rid="R23" ref-type="bibr">2013</xref>; <xref rid="R47" ref-type="bibr">Vaseghi et al., 2017</xref>). A large mammal model of myocardial ischemia and reperfusion with baroreflex response curves, continuous heart rate and blood pressure, electrophysiology recordings, and responses to VNS would be useful to further validate and extend this virtual population model. There is also the opportunity to extend this computational model to include a higher-fidelity representation of sympathetic contributions to sympathovagal balance. This model extension could expand our understanding of VNS alternatives including dorsal root ganglion stimulation, which has been shown to reduce sympathetic outflow and long-term blood pressure (<xref rid="R44" ref-type="bibr">Sverrisdottir et al., 2020</xref>). Our cohort of models is primed for investigating the effects of heterogeneity in the underlying closed-loop physiology on therapeutic responses following MI.</p></sec><sec sec-type="supplementary-material" id="SM1"><title>Supplementary Material</title><supplementary-material id="SD1" position="float" content-type="local-data"><label>Supinfo</label><caption><p id="P81"><xref rid="SD1" ref-type="supplementary-material">Fig. S1</xref>. Twenty eight of 51 parameters representing baroreflex and left ventricular function had significant effects on heart rate and/or MAP. A PAWN global sensitivity analysis was used to quantify which parameters have a significant effect on hemodynamics. Heart rate was measured as the average over a 15 s period and MAP was measured as the average of a 30 s period. Sensitivity indices range between 0 and 1, with 0 indicating that the model parameter has no impact on the output, and 1 indicating that the parameter of interest has a major influence on the output. Parameters with a sensitivity index greater than the red line are significant based on the use of a dummy parameter known to have no influence on the output. Parameters were varied over a &#x000b1;2 fold range from the nominal value and six conditioning intervals were used. Each error bar represents the 95% confidence interval of the sensitivity index based on bootstrapping tests that involved 40,000 iterations of a random sampling of the simulated output. PN<sub>NA,fmid</sub>, midpoint firing rate for principal neurons that receive inputs from the nucleus ambiguus (PN<sub>NA</sub>); PN<sub>NA,fmin</sub>, minimum firing rate of PNNA; NA<sub>fmin</sub>, minimum firing rate of nucleus ambiguus neurons; PN<sub>DMV,fmin</sub>, minimum firing rate of principal neurons that receive inputs from the dorsal motor nucleus of the vagus; <italic toggle="yes">P</italic><sub>0<italic toggle="yes">lv</italic></sub>, left ventricular pressure at diastole; <italic toggle="yes">k</italic><sub><italic toggle="yes">Elv</italic></sub>, gain for volume effects on pressure changes in left ventricle; <italic toggle="yes">fes</italic><sub><italic toggle="yes">inf</italic></sub>, constant describing sympathetic efferent tone.</p></caption><media xlink:href="NIHMS2039207-supplement-Supinfo.docx" id="d67e9691" position="anchor"/></supplementary-material></sec></body><back><ack id="S24"><label>E.</label><title>Funding</title><p id="P82">National Heart, Lung, and Blood Institute U01 HL133360 and R01 HL161696 (RV and JSS), NIH Common Fund SPARC program OT2 OD030534 (RV), and National Science Foundation 1940700 (MMG). Computational resources from the DARWIN project at the University of Delaware are made possible by National Science Foundation OAC-1919839.</p></ack><fn-group><fn fn-type="COI-statement" id="FN2"><label>B.</label><p id="P84">Competing interests</p><p id="P85">The authors declare that they have no conflicts of interest to disclose.</p></fn><fn id="FN3"><label>D.</label><p id="P86">Artificial intelligence generated content disclosure</p><p id="P87">ChatGPT-4 was used to generate plotting functions and improve commenting in code. All code generated was verified by reading the code and checking that the plotted output was reasonable.</p></fn><fn id="FN4"><p id="P88"><bold>Research Governance contact:</bold> Theodore F. Taraschi (<email>Theodore.Taraschi@jefferson.edu</email>)</p></fn><fn id="FN5"><p id="P89"><bold>Institutional Ethics Committee Approval number:</bold> NA, computational modelling study</p></fn><fn id="FN6"><p id="P90"><bold>Compliance with statistics policy:</bold> The authors have read and complied with the statistics policy</p></fn><fn id="FN7"><p id="P91"><bold>Compliance with human and/or animal ethics policy:</bold> NA, computational modelling study</p></fn><fn id="FN8"><p id="P92"><bold>Table of Contents category:</bold> Computational Physiology and Modelling</p></fn></fn-group><sec sec-type="data-availability" id="S28"><label>A.</label><title>Data availability</title><p id="P83">All model equations can be found in the <xref rid="S3" ref-type="sec">Methods</xref> and in our prior work (<xref rid="R11" ref-type="bibr">Gee et al., 2023</xref>). All model files and nominal parameter values are available on GitHub (<ext-link xlink:href="https://github.com/Daniel-Baugh-Institute/CardiovascularControl/tree/main/Virtual_patient_cohorts" ext-link-type="uri">https://github.com/Daniel-Baugh-Institute/CardiovascularControl/tree/main/Virtual_patient_cohorts</ext-link>) and through the NIH CommonFund SPARC Program Portal (<ext-link xlink:href="10.26275/wabs-qul8" ext-link-type="doi">https://doi.org/10.26275/wabs-qul8</ext-link>). Simulations can be performed online through the o<sup>2</sup>S<sup>2</sup>PARC platform (<ext-link xlink:href="https://osparc.io/study/65a52908-1b13-11ee9cd1-02420a0b1bed" ext-link-type="uri">https://osparc.io/study/65a52908-1b13-11ee9cd1-02420a0b1bed</ext-link>). All data used for model development and validation were publicly available. 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</mixed-citation></ref></ref-list></back><floats-group><fig position="float" id="F1"><label>Fig. 1.</label><caption><title>Baroreflex anatomy and physiology mapped onto alternative computational models representing adaptation in different loci of neural regulation.</title><p id="P93">(A) Anatomical representation of neuronal controllers involved in closed-loop regulation of cardiovascular function. (B) Schematic of closed-loop baroreflex model. Parameters representing cardiac muscle property changes that occur after myocardial ischemia and reperfusion are adapted in alternative model 1. Alternative models 2&#x02013;5 represent cardiac parameter adaptation to represent myocardial injury along with neural adaptation in: (2) the baroreceptors, (3) the nucleus tractus solitarius (NTS), (4) the nucleus ambiguus (NA) and the dorsal motor nucleus of the vagus (DMV), and (5) the intrinsic cardiac nervous system (ICN). The lines in blue represent the forms of the functions (e.g., sigmoidal for the neuronal groups). Image of the heart used with permission from (<xref rid="R1" ref-type="bibr">Achanta et al., 2020</xref>). NA-ctr, nucleus ambiguus contribution to cardiac contractility; BR, baroreceptor neuronal subtype; LS, lung stretch receptor neuronal subtype; CP, cardiopulmonary receptor neuronal subtype; LSR, lung stretch receptor; BR, baroreceptor; CPR, cardiopulmonary receptor; PN<sub>DMV</sub>, principal neuron with inputs from the DMV; PN<sub>NA</sub>, principal neuron with inputs from the NA; LCN, local circuit neuron; SA, sinoatrial; resp., respiration; symp., sympathetic. Figure created with <ext-link xlink:href="https://BioRender.com" ext-link-type="uri">BioRender.com</ext-link>.</p></caption><graphic xlink:href="nihms-2039207-f0001" position="float"/></fig><fig position="float" id="F2"><label>Fig. 2.</label><caption><title>Creation of <italic toggle="yes">in silico</italic> patient cohort to explore inter-individual heterogeneity and neural loci of adaptation coupled with cardiac injury.</title><p id="P94">1. An <italic toggle="yes">in silico</italic> patient cohort was generated from a previously published baroreflex model (<xref rid="R11" ref-type="bibr">Gee et al., 2023</xref>). Fifty-one parameters representing neural loci of adaptation along the baroreflex arc and characterizing left ventricular function were identified. Of the 51 parameters, 28 have a significant effect on heart rate (HR) and/or mean arterial pressure (MAP) based on sensitivity analysis. The significant parameters were Sobol sampled over a 1.5-fold range to generate parameter sets representing different individuals. Simulations were performed using these parameter sets, then selected based on experimental observations of the baroreflex curve response and baseline HR and MAP. 2. Post-ischemia/reperfusion (post-I/R) models were generated from the pre-ischemia/reperfusion (pre-I/R) models for each locus of neural adaptation coupled with cardiac injury. Four neural loci were identified: baroreceptors, nucleus tractus solitarius (NTS), nucleus ambiguus (NA) and dorsal motor nucleus of the vagus (DMV), and intrinsic cardiac nervous system (ICN). A model with only cardiac injury and a model with all neural loci coupled with cardiac injury results in a total of six model alternatives. Post-I/R models were generated from each pre-I/R model for each model alternative, then screened based on experimental bounds on the HR and MAP change from pre- to post-I/R (<xref rid="R30" ref-type="bibr">Mastitskaya et al., 2012</xref>) and the post-I/R baroreflex curve (<xref rid="R34" ref-type="bibr">Osculati et al., 1990</xref>). 3. Model analyses and predictive simulations were performed to identify neural adaptation constraints based on the neural locus, inter-individual heterogeneity, and post-I/R therapeutic response diversity. NA-ctr, nucleus ambiguus contribution to cardiac contractility; BR, baroreceptor neuronal subtype; LS, lung stretch receptor neuronal subtype; CP, cardiopulmonary receptor neuronal subtype; LSR, lung stretch receptor; BR, baroreceptor; CPR, cardiopulmonary receptor; PN<sub>DMV</sub>, principal neuron with inputs from the DMV; PN<sub>NA</sub>, principal neuron with inputs from the NA; LCN, local circuit neuron; SA, sinoatrial; resp., respiration; symp., sympathetic. Figure created with <ext-link xlink:href="https://BioRender.com" ext-link-type="uri">BioRender.com</ext-link>.</p></caption><graphic xlink:href="nihms-2039207-f0002" position="float"/></fig><fig position="float" id="F3"><label>Fig. 3.</label><caption><title>Generation of pre-I/R patient cohort models.</title><p id="P95">(A) Twenty eight of 51 parameters representing baroreflex and left ventricular function had significant effects on heart rate and/or MAP. A PAWN global sensitivity analysis was used to quantify which parameters have a significant effect on hemodynamics. Heart rate was measured as the average over a 15 s period and MAP was measured as the average of a 30 s period. Sensitivity indices range between 0 and 1, with 0 indicating that the model parameter has no impact on the output, and 1 indicating that the parameter of interest has a major influence on the output. Parameters with a sensitivity index greater than the red line are significant based on the use of a dummy parameter known to have no influence on the output. Parameters were varied over a &#x000b1;2 fold range from the nominal value and six conditioning intervals were used. Each error bar represents the 95% confidence interval of the sensitivity index based on bootstrapping tests that involved 40,000 iterations of a random sampling of the simulated output. (B) Baroreflex curves of individuals from (<xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>). Dotted lines representing baroreflex curves for each patient were fit to these data using the sigmoidal function: <inline-formula><mml:math id="M182" display="inline"><mml:mi>R</mml:mi><mml:mi>R</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi><mml:mi>t</mml:mi><mml:mi>e</mml:mi><mml:mi>r</mml:mi><mml:mi>v</mml:mi><mml:mi>a</mml:mi><mml:mi>l</mml:mi><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mi>A</mml:mi><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mo>+</mml:mo><mml:mi mathvariant="normal">e</mml:mi><mml:mi mathvariant="normal">x</mml:mi><mml:mi mathvariant="normal">p</mml:mi><mml:mo>[</mml:mo><mml:mi>A</mml:mi><mml:mn>2</mml:mn><mml:mo stretchy="false">(</mml:mo><mml:mi>E</mml:mi><mml:mi>C</mml:mi><mml:mi>S</mml:mi><mml:mi>P</mml:mi><mml:mo>-</mml:mo><mml:mi>A</mml:mi><mml:mn>3</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mfrac><mml:mo>+</mml:mo><mml:mi>A</mml:mi><mml:mn>4</mml:mn></mml:math></inline-formula>. The parameter <inline-formula><mml:math id="M183" display="inline"><mml:mi>A</mml:mi><mml:mn>1</mml:mn></mml:math></inline-formula> represents the response range (maximum - minimum). <inline-formula><mml:math id="M184" display="inline"><mml:mi>A</mml:mi><mml:mn>2</mml:mn></mml:math></inline-formula> represents the gain coefficient of the slope of the sigmoid. <inline-formula><mml:math id="M185" display="inline"><mml:mi>A</mml:mi><mml:mn>3</mml:mn></mml:math></inline-formula> represents the centering point for the horizontal shift of the sigmoid. <inline-formula><mml:math id="M186" display="inline"><mml:mi>A</mml:mi><mml:mn>4</mml:mn></mml:math></inline-formula> represents the minimum response. (C) Accepted patient cohort models that were generated by simultaneously varying the parameters over a &#x000b1;2.5-fold range using Sobol sampling. The criteria for model acceptance into the patient cohort were: (1) coefficients <inline-formula><mml:math id="M187" display="inline"><mml:mi>A</mml:mi><mml:mn>1</mml:mn></mml:math></inline-formula>, <inline-formula><mml:math id="M188" display="inline"><mml:mi>A</mml:mi><mml:mn>2</mml:mn></mml:math></inline-formula>, <inline-formula><mml:math id="M189" display="inline"><mml:mi>A</mml:mi><mml:mn>3</mml:mn></mml:math></inline-formula>, <inline-formula><mml:math id="M190" display="inline"><mml:mi>A</mml:mi><mml:mn>4</mml:mn></mml:math></inline-formula> within the 95% confidence interval observed in individuals in (<xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>), (2) RR interval and MAP within the converted 95% confidence interval observed in (<xref rid="R30" ref-type="bibr">Mastitskaya et al., 2012</xref>). Conversion between rat and human RR interval and MAP was done by assuming a mean model RR interval of 0.87 s and a MAP of 91 mm Hg. All values were then converted using percentage changes. (D) Distribution of sigmoidal parameters <inline-formula><mml:math id="M191" display="inline"><mml:mi>A</mml:mi><mml:mn>1</mml:mn></mml:math></inline-formula>, <inline-formula><mml:math id="M192" display="inline"><mml:mi>A</mml:mi><mml:mn>2</mml:mn></mml:math></inline-formula>, <inline-formula><mml:math id="M193" display="inline"><mml:mi>A</mml:mi><mml:mn>3</mml:mn></mml:math></inline-formula>, and <inline-formula><mml:math id="M194" display="inline"><mml:mi>A</mml:mi><mml:mn>4</mml:mn></mml:math></inline-formula> and baseline heart rate and MAP for accepted (blue) and rejected (green) models compared to individual data in the absolute value of the slope parameter (<inline-formula><mml:math id="M195" display="inline"><mml:mi>A</mml:mi><mml:mn>2</mml:mn></mml:math></inline-formula>) of the sigmoidal function fit to the baroreflex curve. Black bars represent the 95% confidence interval of the experimental data that were used to filter the models. Of the 6,000 pre-I/R candidate models generated, 59 models met the criteria. PN<sub>NA,fmid</sub>, midpoint firing rate for principal neurons that receive inputs from the nucleus ambiguus (PN<sub>NA</sub>); PN<sub>NA,fmin</sub>, minimum firing rate of PNNA; NA<sub>fmin</sub>, minimum firing rate of nucleus ambiguus neurons; PN<sub>DMV,fmin</sub>, minimum firing rate of principal neurons that receive inputs from the dorsal motor nucleus of the vagus; <italic toggle="yes">P</italic><sub>0<italic toggle="yes">lv</italic></sub>, left ventricular pressure at diastole; <italic toggle="yes">k</italic><sub><italic toggle="yes">Elv</italic></sub>, gain for volume effects on pressure changes in left ventricle; <italic toggle="yes">fes</italic><sub><italic toggle="yes">inf</italic></sub>, constant describing sympathetic efferent tone.</p></caption><graphic xlink:href="nihms-2039207-f0003" position="float"/></fig><fig position="float" id="F4"><label>Fig. 4.</label><caption><title>Adaptation of cardiac parameters produces physiological post-I/R models.</title><p id="P96">Starting from 59 pre-I/R models that yielded 5,900 post-I/R models, we filtered to obtain 85 models within the acceptable range of physiological behaviour. The criteria for filtering the post-I/R models were (1) heart rate between 58 and 116 bpm, (2) systolic pressure between 96 and 142 mm Hg, and (3) RR interval response to neck chamber pressures of 8, 13.2, 18.5, 23.7, 30, and 37.5 mm Hg (<xref rid="R34" ref-type="bibr">Osculati et al., 1990</xref>). (A) Model schematic highlighting modified heart parameters: <italic toggle="yes">C</italic><sub><italic toggle="yes">la</italic></sub>, left atrial compliance; <italic toggle="yes">P</italic><sub>0<italic toggle="yes">lv</italic></sub>, left ventricular pressure at diastole; <italic toggle="yes">k</italic><sub><italic toggle="yes">Elv</italic></sub>, gain for volume effects on pressure changes in left ventricle; <italic toggle="yes">V</italic><sub><italic toggle="yes">ulv</italic></sub>, left ventricular unstressed volume; <italic toggle="yes">fes</italic><sub><italic toggle="yes">inf</italic></sub>, constant describing sympathetic efferent tone. (B) Experimental procedure with pre-ischemia/reperfusion (pre-I/R) and post-ischemia/reperfusion (post-I/R) time points. (C) Comparison of experimental and model mean arterial pressure (MAP). Error bars represent the standard deviation. Experimental data were collected in rats and converted to human HR and arterial pressure by assuming that the pre-ischemia rat and baseline human cardiovascular metrics were analogous (<xref rid="R30" ref-type="bibr">Mastitskaya et al., 2012</xref>; <xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>). Experimental values for post-I/R HR and MAP were converted using the percent change from pre-ischemia. Paired pre- and post-I/R models are connected by a line. (D) RR interval experimental data and models corresponding to MAP data. (E) Baroreflex curve predictions for post-I/R models with cardiac parameter adaptations filtered based on the criteria that the RR interval response be within the 95% confidence interval of the experimental data (<xref rid="R34" ref-type="bibr">Osculati et al., 1990</xref>). Each purple line represents one model that met the criteria. The experimental mean and 95% confidence interval are plotted in red. Panels A and B created with <ext-link xlink:href="https://BioRender.com" ext-link-type="uri">BioRender.com</ext-link>.</p></caption><graphic xlink:href="nihms-2039207-f0004" position="float"/></fig><fig position="float" id="F5"><label>Fig. 5.</label><caption><title>Baroreceptor adaptation coupled with cardiac produced models that match experimental observations.</title><p id="P97">Starting from 59 pre-I/R models that yielded 5,900 post-I/R models, we filtered to obtain 88 models within the acceptable range of physiological behaviour. The filtering criteria were the same as what were used for the cardiac adaptation model. (A) Model schematic highlighting the neuronal group adapted to represent the baroreceptor remodelling coupled with cardiac changes (see <xref rid="FD2" ref-type="disp-formula">Eq. 2</xref> and <xref rid="FD3" ref-type="disp-formula">Eq. 3</xref> for equations represented by this block). (B) Comparison of experimental and model mean arterial pressure (MAP). Error bars represent one standard deviation. Experimental data were collected in rats and converted to human HR and arterial pressure by assuming that the pre-ischemia rat and baseline human cardiovascular metrics were analogous (<xref rid="R30" ref-type="bibr">Mastitskaya et al., 2012</xref>; <xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>). Experimental values for end-ischemia HR and MAP were converted using the percent change from pre-ischemia. (C) RR interval experimental data and models corresponding to MAP data. (D) Baroreflex curve predictions for post-I/R models with cardiac parameter adaptations filtered based on the criteria that the RR interval response be within the 95% confidence interval of the experimental data (<xref rid="R34" ref-type="bibr">Osculati et al., 1990</xref>). Each yellow line represents one model that met the criteria. The experimental mean and 95% confidence interval are plotted in red. (E) Comparison of pre- (blue) and post-I/R (yellow) baroreceptor response curves. Shaded regions represent one standard deviation from the average for both model ensembles. Panel A created with <ext-link xlink:href="https://BioRender.com" ext-link-type="uri">BioRender.com</ext-link>.</p></caption><graphic xlink:href="nihms-2039207-f0005" position="float"/></fig><fig position="float" id="F6"><label>Fig. 6.</label><caption><title>Adaptation in brainstem (NTS or NA and DMV) neural loci coupled with cardiac remodelling models has a limited set of models that match experimentally observed hemodynamic and autonomic changes.</title><p id="P98">Starting from 59 pre-I/R models that yielded 5,900 post-I/R models per neural locus of adaptation, we filtered to obtain 75 NTS models and 86 NA/DMV models within the acceptable range of physiological behaviour. The filtering criteria were the same as what were used for the previous alternative models. (A) Model schematic highlighting the two brainstem models: NTS adaptation coupled with cardiac changes and NA+DMV remodelling coupled with cardiac alterations. (B) Baroreflex curve predictions for post-I/R models with cardiac parameter adaptations filtered based on the criteria that the RR interval response be within the 95% confidence interval of the experimental data (<xref rid="R34" ref-type="bibr">Osculati et al., 1990</xref>). Each green line represents one NTS model and each pink line represents one NA/DMV model that met the criteria. The experimental mean and 95% confidence interval are plotted in red. Pre- and post-I/R MAP and HR changes for each parameter set for NTS models coupled with cardiac remodelling (C) and (D) and for NA/DMV models coupled with cardiac remodelling (E) and (F). Error bars represent the standard deviation. Experimental data were collected in rats and converted to human HR and arterial pressure by assuming that the pre-ischemia rat and baseline human cardiovascular metrics were analogous (<xref rid="R30" ref-type="bibr">Mastitskaya et al., 2012</xref>; <xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>). Experimental values for end-ischemia HR and MAP were converted using the percent change from pre-ischemia. Panel A created with <ext-link xlink:href="https://BioRender.com" ext-link-type="uri">BioRender.com</ext-link>.</p></caption><graphic xlink:href="nihms-2039207-f0006" position="float"/></fig><fig position="float" id="F7"><label>Fig. 7.</label><caption><title>ICN adaptation combined with cardiac remodelling predicts limited models that match experimentally observed hemodynamic and autonomic changes.</title><p id="P99">Starting from 59 pre-I/R models which yielded 5,900 post-I/R models, we filtered to obtain 93 models within the acceptable range of physiological behaviour. The filtering criteria were the same as what were used for the previous alternative models. (A) Model schematic highlighting ICN remodelling coupled with cardiac changes. (B) Comparison of experimental and model MAP. Error bars represent the standard deviation. Experimental data were collected in rats and converted to human HR and arterial pressure by assuming that the pre-ischemia rat and baseline human cardiovascular metrics were analogous (<xref rid="R30" ref-type="bibr">Mastitskaya et al., 2012</xref>; <xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>). Experimental values for post-I/R HR and MAP were converted using the percent change from pre-I/R. (C) RR interval data corresponding to MAP data. (D) Baroreflex curve predictions for post-I/R models with ICN adaptation coupled with cardiac parameter adaptations filtered based on the criteria that the RR interval response be within the 95% confidence interval of the experimental data (<xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>). Each blue line represents one model. The experimental data and 95% confidence interval are plotted in red. (E) Ratio of peripheral to central contributions to heart rate regulation for all accepted pre- and post-I/R models as calculated using Shapley values that quantify parametric contributions to an output. A ratio above one indicates that peripheral parameters (baroreceptors, ICN) play a larger role in heart rate regulation compared with central (brainstem) parameters. The distribution of the averaged contribution for central and peripheral parameters, quantified using Shapley values averaged over many points, is shown for pre- versus post-I/R (<inline-formula><mml:math id="M196" display="inline"><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn>0.00160</mml:mn></mml:math></inline-formula>). Five outliers were not shown in the plot for ease of viewing but are included in the analysis. Panel A created with <ext-link xlink:href="https://BioRender.com" ext-link-type="uri">BioRender.com</ext-link>.</p></caption><graphic xlink:href="nihms-2039207-f0007" position="float"/></fig><fig position="float" id="F8"><label>Fig. 8.</label><caption><title>Simultaneous adaptation in all neural loci combined with cardiac remodelling predicts models that match experimentally observed hemodynamic and autonomic changes.</title><p id="P100">Starting from 59 pre-I/R models that yielded 5,900 post-I/R models, we filtered to obtain 47 models within the acceptable range of physiological behaviour. The filtering criteria were the same as what were used for the previous alternative models. (A) Model schematic highlighting ICN remodelling coupled with cardiac changes. (B) Comparison of experimental and model MAP. Error bars represent the standard deviation. Experimental data were collected in rats and converted to human HR and arterial pressure by assuming that the pre-ischemia rat and baseline human cardiovascular metrics were analogous (<xref rid="R30" ref-type="bibr">Mastitskaya et al., 2012</xref>; <xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>). Experimental values for post-I/R HR and MAP were converted using the percent change from pre-I/R. (C) RR interval data corresponding to MAP data. (D) Baroreflex curve predictions for post-I/R models with ICN adaptation coupled with cardiac parameter adaptations filtered based on the criterion that the RR interval response be within the 95% confidence interval of the experimental data (<xref rid="R42" ref-type="bibr">Seredy&#x00144;ski et al., 2021</xref>). Each blue line represents one model. The experimental data and 95% confidence interval are plotted in red. Panel A created with <ext-link xlink:href="https://BioRender.com" ext-link-type="uri">BioRender.com</ext-link>.</p></caption><graphic xlink:href="nihms-2039207-f0008" position="float"/></fig><fig position="float" id="F9"><label>Fig. 9.</label><caption><title>Individuals that maintain afferent function and adapt along the vagal efferent pathway are able to compensate post-I/R.</title><p id="P101">(A) T-distributed stochastic neighbor embedding (t-SNE) plot of accepted post-I/R models colored by baroreflex sensitivity. Each point represents an individual. Each model was characterised by vagal efferent activity, vagal afferent activity, and baroreceptor responsivity. Points that are closer together are more similar to each other based on these characteristics. (B) The same t-SNE plot colored by the post-IR locus of adaptation. (C) t-SNE of post-I/R models colored by pre-I/R patient number. Text boxes below the plots created with <ext-link xlink:href="https://BioRender.com" ext-link-type="uri">BioRender.com</ext-link>.</p></caption><graphic xlink:href="nihms-2039207-f0009" position="float"/></fig><table-wrap position="float" id="T1"><label>Table 1.</label><caption><p id="P102">Updated parameter values for nominal model that differ from (<xref rid="R11" ref-type="bibr">Gee et al., 2023</xref>).</p></caption><table frame="box" rules="all"><colgroup span="1"><col align="left" valign="middle" span="1"/><col align="left" valign="middle" span="1"/><col align="left" valign="middle" span="1"/></colgroup><thead><tr><th align="left" valign="top" rowspan="1" colspan="1">Parameter</th><th align="left" valign="top" rowspan="1" colspan="1">Value</th><th align="left" valign="top" rowspan="1" colspan="1">Units</th></tr></thead><tbody><tr><td align="left" valign="top" rowspan="1" colspan="1">
<inline-formula>
<mml:math id="M197" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>m</mml:mi><mml:mi>i</mml:mi><mml:mi>n</mml:mi></mml:mrow><mml:mrow><mml:mi>P</mml:mi><mml:mi>N</mml:mi><mml:mi>N</mml:mi><mml:mi>A</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:math>
</inline-formula>
</td><td align="left" valign="top" rowspan="1" colspan="1">1.69</td><td align="left" valign="top" rowspan="1" colspan="1">Hz</td></tr><tr><td align="left" valign="top" rowspan="1" colspan="1">
<inline-formula>
<mml:math id="M198" display="inline"><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>P</mml:mi><mml:mi>N</mml:mi><mml:mi>N</mml:mi><mml:mi>A</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:math>
</inline-formula>
</td><td align="left" valign="top" rowspan="1" colspan="1">7.33</td><td align="left" valign="top" rowspan="1" colspan="1">Hz</td></tr></tbody></table></table-wrap><boxed-text id="BX1" position="float"><caption><title>Key points:</title></caption><list list-type="bullet" id="L1"><list-item><p id="P103">Baroreflex sensitivity is a strong indicator of post-myocardial ischemia survival and is variable among individuals</p></list-item><list-item><p id="P104">We fine-tuned a computational model ensemble based on physiological observations to develop an <italic toggle="yes">in silico</italic> patient cohort consistent with the range of baroreflex responses observed experimentally</p></list-item><list-item><p id="P105">Simulation and analysis of the <italic toggle="yes">in silico</italic> cohort show that individuals with a functional afferent pathway and the ability to adapt along the vagal efferent pathway can maintain baroreflex sensitivity post-cardiac ischemia</p></list-item></list></boxed-text></floats-group></article>