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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Physiol.</journal-id>
<journal-title>Frontiers in Physiology</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Physiol.</abbrev-journal-title>
<issn pub-type="epub">1664-042X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">1230654</article-id>
<article-id pub-id-type="doi">10.3389/fphys.2023.1230654</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Physiology</subject>
<subj-group>
<subject>Hypothesis and Theory</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>A framework for heart-lung interaction and its application to prone position in the acute respiratory distress syndrome</article-title>
<alt-title alt-title-type="left-running-head">Kenny</alt-title>
<alt-title alt-title-type="right-running-head">
<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.3389/fphys.2023.1230654">10.3389/fphys.2023.1230654</ext-link>
</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Kenny</surname>
<given-names>Jon-Emile S.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1256494/overview"/>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>Health Sciences North Research Institute</institution>, <addr-line>Sudbury</addr-line>, <addr-line>ON</addr-line>, <country>Canada</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Flosonics Medical</institution>, <addr-line>Toronto</addr-line>, <addr-line>ON</addr-line>, <country>Canada</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1398278/overview">Antoine Vieillard-Baron</ext-link>, Assistance Publique Hopitaux De Paris, France</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/251725/overview">Arnoldo Santos</ext-link>, University Hospital Fundaci&#xf3;n Jim&#xe9;nez D&#xed;az, Spain</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1682669/overview">Per Werner M&#xf6;ller</ext-link>, University of Gothenburg, Sweden</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Jon-Emile S. Kenny, <email>jon-emile@heart-lung.org</email>
</corresp>
</author-notes>
<pub-date pub-type="epub">
<day>07</day>
<month>08</month>
<year>2023</year>
</pub-date>
<pub-date pub-type="collection">
<year>2023</year>
</pub-date>
<volume>14</volume>
<elocation-id>1230654</elocation-id>
<history>
<date date-type="received">
<day>29</day>
<month>05</month>
<year>2023</year>
</date>
<date date-type="accepted">
<day>24</day>
<month>07</month>
<year>2023</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2023 Kenny.</copyright-statement>
<copyright-year>2023</copyright-year>
<copyright-holder>Kenny</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>While both cardiac output (Q<sub>circulatory</sub>) and right atrial pressure (P<sub>RA</sub>) are important measures in the intensive care unit (ICU), they are outputs of the system and not determinants. That is to say, in a model of the circulation wherein venous return and cardiac function find equilibrium at an &#x2018;operating point&#x2019; (OP, defined by the P<sub>RA</sub> on the x-axis and Q<sub>circulatory</sub> on the y-axis) <italic>both</italic> the P<sub>RA</sub> and Q<sub>circulatory</sub> are, necessarily, <italic>dependent</italic> variables. A simplified geometrical approximation of Guyton&#x2019;s model is put forth to illustrate that the <italic>independent</italic> variables of the system are: 1) the mean systemic filling pressure (P<sub>MSF</sub>), 2) the pressure within the pericardium (P<sub>PC</sub>), 3) cardiac function and 4) the resistance to venous return. Classifying independent and dependent variables is clinically-important for therapeutic control of the circulation. Recent investigations in patients with acute respiratory distress syndrome (ARDS) have illuminated how P<sub>MSF</sub>, cardiac function and the resistance to venous return change when placing a patient in prone. Moreover, the location of the OP at baseline and the intimate physiological link between the heart and the lungs also mediate how the P<sub>RA</sub> and Q<sub>circulatory</sub> respond to prone position. Whereas turning a patient from supine to prone is the focus of this discussion, the principles described within the framework apply equally-well to other more common ICU interventions including, but not limited to, ventilator management, initiating vasoactive medications and providing intravenous fluids.</p>
</abstract>
<kwd-group>
<kwd>heart-lung interactions</kwd>
<kwd>hemodynamics</kwd>
<kwd>prone position</kwd>
<kwd>acute respiratory distress syndrome</kwd>
<kwd>venous return</kwd>
<kwd>fluid responsiveness</kwd>
</kwd-group>
<custom-meta-wrap>
<custom-meta>
<meta-name>section-at-acceptance</meta-name>
<meta-value>Clinical and Translational Physiology</meta-value>
</custom-meta>
</custom-meta-wrap>
</article-meta>
</front>
<body>
<sec id="s1">
<title>Introduction</title>
<p>Though evidence of benefit has existed for placing patients with moderate-to-severe acute respiratory distress syndrome (ARDS) in the prone position for some time, the coronavirus pandemic raised clinical awareness of this maneuver (<xref ref-type="bibr" rid="B32">Gu&#xe9;rin et al., 2020</xref>). Guidelines currently recommend prone position for patients with ARDS and a partial pressure-to-fraction of inspired oxygen (P<sub>a</sub>O<sub>2</sub>/F<sub>i</sub>O<sub>2</sub>) ratio of not more than 150&#xa0;mmHg (<xref ref-type="bibr" rid="B65">Papazian et al., 2019</xref>). Furthermore, with this ARDS severity, patients should maintain the prone position for at least 12&#xa0;h per day for optimal benefit (<xref ref-type="bibr" rid="B34">Gu&#xe9;rin et al., 2013</xref>).</p>
<p>Turning a patient from the supine to prone position has salutary benefits on gas exchange as oxygenation and carbon dioxide elimination are both enhanced (<xref ref-type="bibr" rid="B32">Gu&#xe9;rin et al., 2020</xref>). The mechanisms by which the prone position exerts its salubrious effects are manifold. When the dorsal, de-gassed &#x2018;sponge lung&#x2019; (<xref ref-type="bibr" rid="B8">Bone, 1993</xref>) is no longer gravity-dependent, it is recruited and the surface area for gas exchange increased. Critically, the newly-enlisted alveoli see no significant change in pulmonary blood flow (<xref ref-type="bibr" rid="B39">Henderson et al., 2013</xref>); as a consequence, the burden of low ventilation-to-perfusion (V/Q) lung units is reduced. In addition to alveolar recruitment, shifting to the prone position improves &#x2018;shape matching&#x2019; between the pulmonary parenchyma and the chest wall (<xref ref-type="bibr" rid="B29">Gattinoni et al., 2013</xref>). In total, the result is that there is less pulmonary inhomogeneity (<xref ref-type="bibr" rid="B18">Cressoni et al., 2014</xref>; <xref ref-type="bibr" rid="B19">Cressoni et al., 2015</xref>) and, therefore, fewer &#x2018;stress-raisers&#x2019; (<xref ref-type="bibr" rid="B60">Mead et al., 1970</xref>) that amplify radial traction forces upon the lungs <italic>and</italic> pulmonary vasculature (<xref ref-type="bibr" rid="B14">Broccard et al., 1998</xref>; <xref ref-type="bibr" rid="B58">Marini et al., 2003</xref>; <xref ref-type="bibr" rid="B72">Repess&#xe9; et al., 2016</xref>). Furthermore, stiffening the chest wall with improved pulmonary compliance diminishes trans-pulmonary pressure (P<sub>TP</sub>) as the pleural pressure is raised for any given airway pressure (<xref ref-type="bibr" rid="B57">Marini and Gattinoni, 2021</xref>). This reduces the mechanical power applied to the pulmonary parenchyma and mitigates West zone 1 and 2 conditions (<xref ref-type="bibr" rid="B28">Gattinoni and Quintel, 2016</xref>). All of the aforementioned changes in pulmonary physiology (i.e., improved oxygenation and carbon dioxide elimination, optimized perivascular pulmonary mechanics, diminished P<sub>TP</sub>) minimize the afterload experienced by the right ventricle (RV), giving weight to the motto: &#x2018;what&#x2019;s good for the lung is good for the RV (<xref ref-type="bibr" rid="B72">Repess&#xe9; et al., 2016</xref>).&#x2019;</p>
<p>While the literature is replete with elegant investigations into the mechanical pulmonary pathophysiology of ARDS in both supine and prone positions, comparatively little is known about the hemodynamic effects. With a recent investigation exploring the determinants of venous return in the prone position (<xref ref-type="bibr" rid="B48">Lai et al., 2021</xref>) and an excellent related review (<xref ref-type="bibr" rid="B49">Lai et al., 2023</xref>), this overview will expand upon relevant concepts in clinical hemodynamics, propose a simplified geometrical model clarifying the determinants of cardiac output and right atrial pressure and then relate this to what is currently known about prone position in the ARDS patient (<xref ref-type="table" rid="T1">Table 1</xref>).</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Key messages by section.</p>
</caption>
<table>
<tbody valign="top">
<tr>
<td align="left">Introduction</td>
<td align="left">A cursory overview of the mechanical effects of prone position (PP) on the injured lung. PP recruits both airspace and pulmonary vasculature. This improves pulmonary mechanics, gas exchange and reduces right ventricular outflow impedance</td>
</tr>
<tr>
<td rowspan="2" align="left">Guyton primer</td>
<td align="left">The <italic>venous return</italic> (VR) subsection describes the: 1.) pressure gradient for VR (i.e., P<sub>MSF</sub>&#x2014;P<sub>RA</sub>), 2.) resistance to VR (R<sub>VR</sub>) and 3.) how both (P<sub>MSF</sub>&#x2014;P<sub>RA</sub>) and R<sub>VR</sub> together describe VR.</td>
</tr>
<tr>
<td align="left">The <italic>Guyton diagram</italic> subsection describes how VR and cardiac function form an equilibrium&#x2014;the operating point (OP)&#x2014;which is <italic>the dependent variable</italic> in the Guyton model. As the OP is a dependent variable, so too are its two coordinates (i.e., P<sub>RA</sub> and Q<sub>circulatory</sub>). Thus, contrary to what is commonly taught, P<sub>RA</sub> is not an independent determinant of Q<sub>circulatory</sub> (i.e., total circulatory blood flow &#x3d; venous return &#x3d; cardiac output)</td>
</tr>
<tr>
<td rowspan="2" align="left">Geometrical model</td>
<td align="left">To illustrate how P<sub>RA</sub> is not a determinant of Q<sub>circulatory</sub>, a simplified geometrical model is derived; the independent variables of the circulation are shown to be: 1.) P<sub>MSF,</sub> 2.) the pericardial pressure (P<sub>PC</sub>), 3.) R<sub>VR</sub> and 4.) &#x2018;cardiac resistance&#x2019; (R<sub>cardiac</sub>)</td>
</tr>
<tr>
<td align="left">The circulation can be &#x2018;cardiac-&#x2019; or &#x2018;venous-limited.&#x2019; The former is synonymous with preload unresponsiveness. When the circulation is &#x2018;cardiac-limited&#x2019;, changing P<sub>MSF</sub> or R<sub>VR</sub> only alters P<sub>RA</sub> with no effect on Q<sub>circulatory</sub>. When &#x2018;venous-limited&#x2019;, changing cardiac function (R<sub>cardiac</sub>) or P<sub>PC</sub> only alters P<sub>RA</sub> with no effect on Q<sub>circulatory</sub>
</td>
</tr>
<tr>
<td rowspan="3" align="left">Implications for prone position</td>
<td align="left">Recent investigations in ARDS patients report how PP alters P<sub>MSF</sub>, R<sub>VR</sub>, and R<sub>cardiac</sub>; little data exist on how PP alters the circulation via the P<sub>PC</sub> (which is a key nexus for heart-lung interaction)</td>
</tr>
<tr>
<td align="left">Determining a &#x2018;cardiac-limited&#x2019; circulation helps predict the hemodynamic response to PP.</td>
</tr>
<tr>
<td align="left">In response to PP, P<sub>RA</sub> does not determine Q<sub>circulatory</sub>, the system (as described by the geometrical model) determines the OP which decides both Q<sub>circulatory</sub> <italic>and</italic> P<sub>RA</sub>.</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s1-1">
<title>Guyton primer</title>
<p>Many excellent reviews connecting Guyton&#x2019;s model of the circulatory system to critical-illness are available (<xref ref-type="bibr" rid="B78">Sylvester et al., 1983</xref>; <xref ref-type="bibr" rid="B11">Bressack and Raffin, 1987</xref>; <xref ref-type="bibr" rid="B26">Fessler, 1997</xref>; <xref ref-type="bibr" rid="B43">Jacobsohn et al., 1997</xref>; <xref ref-type="bibr" rid="B54">Magder, 2004</xref>; <xref ref-type="bibr" rid="B30">Gelman, 2008</xref>; <xref ref-type="bibr" rid="B66">Parkin and Leaning, 2008</xref>; <xref ref-type="bibr" rid="B22">Feihl and Broccard, 2009a</xref>; <xref ref-type="bibr" rid="B23">Feihl and Broccard, 2009b</xref>; <xref ref-type="bibr" rid="B53">Magder, 2012</xref>; <xref ref-type="bibr" rid="B5">Berlin and Bakker, 2015</xref>; <xref ref-type="bibr" rid="B4">Berger and Takala, 2018</xref>; <xref ref-type="bibr" rid="B69">Persichini et al., 2022</xref>). Though this model has been criticized and debated (<xref ref-type="bibr" rid="B9">Brengelmann, 2003</xref>; <xref ref-type="bibr" rid="B1">Beard and Feigl, 2011</xref>; <xref ref-type="bibr" rid="B64">Moller et al., 2017</xref>; <xref ref-type="bibr" rid="B2">Berger et al., 2019</xref>; <xref ref-type="bibr" rid="B10">Brengelmann, 2019</xref>; <xref ref-type="bibr" rid="B83">Werner-Moller et al., 2020</xref>; <xref ref-type="bibr" rid="B47">Kenny, 2021</xref>), these controversies are beyond the scope of this review. Guyton&#x2019;s contributions to hemodynamics are many and may be parsed into: 1.) the explication of venous return (<xref ref-type="bibr" rid="B37">Guyton et al., 1955</xref>) and 2.) the graphical superposition of the venous return and Starling-Sarnoff curves (<xref ref-type="bibr" rid="B35">Guyton, 1955</xref>).</p>
<sec id="s1-2">
<title>Venous return</title>
<p>The determinants of venous return from the peripheral circulation are, from Guyton&#x2019;s experiments: 1.) the mean circulatory filling pressure (P<sub>MCF</sub>), 2.) right atrial pressure (P<sub>RA</sub>) and 3.) the resistance to venous return (R<sub>VR</sub>) (<xref ref-type="bibr" rid="B35">Guyton, 1955</xref>; <xref ref-type="bibr" rid="B78">Sylvester et al., 1983</xref>; <xref ref-type="bibr" rid="B43">Jacobsohn et al., 1997</xref>; <xref ref-type="bibr" rid="B22">Feihl and Broccard, 2009a</xref>). Together the P<sub>MCF</sub> and the P<sub>RA</sub> define the pressure gradient for venous return.</p>
<sec id="s1-3">
<title>The pressure gradient for venous return</title>
<p>If blood flow were ceased, arterial pressure would fall and venous pressure would rise to a weighted recoil pressure reflecting the portion of the circulation with greatest blood volume (<xref ref-type="bibr" rid="B78">Sylvester et al., 1983</xref>; <xref ref-type="bibr" rid="B43">Jacobsohn et al., 1997</xref>). As the small veins and venules comprise this circulatory segment, the P<sub>MCF</sub> is a &#x2018;pivot pressure&#x2019; found downstream of the capillary beds but upstream from the larger veins (<xref ref-type="bibr" rid="B53">Magder, 2012</xref>). The &#x2018;pivot pressure&#x2019; description arises from the sense that when the heart recommences circulatory flow, pressure in the arteries rise up from the P<sub>MCF</sub> while the pressure in the downstream veins fall below it; thus, the P<sub>MCF</sub> acts as a quasi-static &#x2018;pivot&#x2019; around which pressures upstream and downstream rise and fall, respectively (<xref ref-type="bibr" rid="B13">Broccard, 2012</xref>). As discussed below, the P<sub>MCF</sub> is similar, but not equivalent to, the mean <italic>systemic</italic> filling pressure (P<sub>MSF</sub>). The P<sub>MSF</sub> excludes the contributions of intrathoracic blood volume and compliance.</p>
<p>The P<sub>MCF</sub> (or P<sub>MSF</sub>) is determined by two related&#x2013;and often confused&#x2013;biophysical properties: capacitance and compliance (<xref ref-type="bibr" rid="B74">Rothe, 1986</xref>; <xref ref-type="bibr" rid="B73">Rothe, 1993</xref>; <xref ref-type="bibr" rid="B81">Tyberg, 2002</xref>). To understand <italic>capacitance</italic>, the reader must appreciate that the total circulatory volume is comprised of two distinct (though dynamic) &#x2018;types&#x2019; of volume&#x2013;the unstressed (V<sub>US</sub>) and stressed (V<sub>S</sub>) volumes (<xref ref-type="bibr" rid="B30">Gelman, 2008</xref>; <xref ref-type="bibr" rid="B53">Magder, 2012</xref>). The V<sub>US</sub> does not create a vascular elastic recoil pressure while the V<sub>S</sub> does. As an analogy, filling a waterbed requires water volume before the walls are stretched (i.e., the V<sub>US</sub>); further volume generates a recoil pressure from the elastic walls (i.e., the V<sub>S</sub>). As compared to a water balloon, a waterbed has a much larger capacitance because its V<sub>US</sub> is greater than the V<sub>US</sub> of the balloon. <italic>Compliance</italic> and its inverse, <italic>elastance</italic>, describe the relationship between changing vascular volume and changing recoil pressure (<xref ref-type="bibr" rid="B73">Rothe, 1993</xref>). It follows that compliance (or elastance) pertain to the V<sub>S</sub>; the V<sub>US</sub>, by definition, generates no change in pressure (i.e., the V<sub>US</sub> has infinite compliance or zero elastance). Continuing with the analogy above, were the waterbed made from a poorly elastic (i.e., stiff) material, it would have a large capacitance, but low compliance (or high elastance). If the water balloon was made of a highly elastic material, it would have a low capacitance, but high compliance (or low elastance). Mathematically, the P<sub>MCF</sub> is determined by the volume of blood generating a recoil pressure (i.e., the V<sub>S</sub>, which is determined by total vascular volume and capacitance) divided by the vascular compliance (<xref ref-type="bibr" rid="B81">Tyberg, 2002</xref>; <xref ref-type="bibr" rid="B53">Magder, 2012</xref>) (<xref ref-type="fig" rid="F1">Figure 1</xref>).</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Illustration of capacitance and compliance. Vessel A has a relatively small capacitance because its unstressed volume (V<sub>US<sub>A</sub>
</sub>) is small. The compliance of the vessel (C<sub>A</sub>) is the inverse of elastance on this graph; by rearrangement, the recoil pressure generated in this vessel (P<sub>A</sub>) is equal to its stressed volume (V<sub>S<sub>A</sub>
</sub>) divided by its compliance. Vessel B shows a larger capacitance, but an increased elastance (i.e., reduced compliance, C<sub>B</sub>) relative to vessel A. Vessel A and B are analogous to the &#x2018;water balloon&#x2019; and &#x2018;waterbed,&#x2019; respectively, described within the text. V<sub>S<sub>B</sub>
</sub> is the stressed volume, V<sub>US<sub>B</sub>
</sub> is the unstressed volume and P<sub>B</sub> is the recoil pressure of vessel B.</p>
</caption>
<graphic xlink:href="fphys-14-1230654-g001.tif"/>
</fig>
<p>As noted above, the P<sub>MCF</sub> includes the cardiac and pulmonary vascular volumes and compliances (i.e., the total circulation) while the P<sub>MSF</sub> measures only the extra-thoracic, systemic, circulation (<xref ref-type="bibr" rid="B73">Rothe, 1993</xref>); they are very similar in value and often used interchangeably. In clinical practice, the methods for estimating this static, &#x2018;pivot pressure&#x2019; reflect the <italic>systemic</italic> pressure (i.e., P<sub>MSF</sub>) and this measure will be used throughout this review (<xref ref-type="bibr" rid="B3">Berger et al., 2016</xref>). For patients, there are three methods to estimate the P<sub>MSF</sub>: 1.) extrapolation to zero flow of the P<sub>RA</sub>&#x2013;cardiac output relationship altered by ventilator-hold maneuvers (<xref ref-type="bibr" rid="B71">Pinsky, 1984</xref>; <xref ref-type="bibr" rid="B51">Maas et al., 2009</xref>), 2.) extremely rapid cuff insufflation on the arm with an ipsilateral arterial line (<xref ref-type="bibr" rid="B52">Maas et al., 2012</xref>) and 3.) mathematical modelling by the method of Parkin and Leaning (<xref ref-type="bibr" rid="B66">Parkin and Leaning, 2008</xref>). Though beyond the scope of this discussion, the ventilator-hold and arm-occlusion methods over-estimate P<sub>MSF</sub> (<xref ref-type="bibr" rid="B52">Maas et al., 2012</xref>; <xref ref-type="bibr" rid="B3">Berger et al., 2016</xref>) for a variety of reasons (<xref ref-type="bibr" rid="B62">Moller and Berger, 2023</xref>) whereas the mean systemic filling pressure analogue (P<sub>MSA</sub>) (i.e., the method of Parkin and Leaning) accurately estimated absolute and changing values of P<sub>MSF</sub> in a porcine model (<xref ref-type="bibr" rid="B84">Werner-Moller et al., 2022</xref>). Because it is simply calculated from P<sub>RA</sub>, cardiac output and mean arterial pressure (<xref ref-type="bibr" rid="B66">Parkin and Leaning, 2008</xref>; <xref ref-type="bibr" rid="B63">Moller and Parkin, 2022</xref>), the P<sub>MSA</sub> is an attractive tool for guiding both prospective and retrospective research as well as clinical therapy (<xref ref-type="bibr" rid="B63">Moller and Parkin, 2022</xref>; <xref ref-type="bibr" rid="B62">Moller and Berger, 2023</xref>). Given the above, the importance of understanding and, arguably, measuring the P<sub>MSF</sub> is that it is a hemodynamic variable the clinician can target therapeutically. For example, a low P<sub>MSF</sub> intimates low V<sub>S</sub> which could be due to diminished total blood volume (e.g., hypovolemia, hemorrhage) and/or high venous capacitance (e.g., venodilation, sepsis). The clinician might rectify these pathological states by giving volume and/or administering alpha-agonists, respectively (<xref ref-type="bibr" rid="B66">Parkin and Leaning, 2008</xref>). Thus, the P<sub>MSF</sub> and its determinants are independent variables that can be adjusted for therapeutic control of the circulation; increasing P<sub>MSF</sub> raises venous return for any given right atrial pressure (P<sub>RA</sub>) (<xref ref-type="fig" rid="F2">Figure 2</xref>).</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Pressure gradient for venous return. The effect of changing mean systemic filling pressure (in millimeters of mercury, mmHg) from a low (P<sub>MSF1</sub>) to a higher value (P<sub>MSF2</sub>) (e.g., volume infusion, decreased capacitance). The slope of the venous return curve is constant between the two curves meaning that the resistance to venous return is constant (see below). For a given right atrial pressure (P<sub>RA</sub>), the lower P<sub>MSF1</sub> (i.e., reduced pressure gradient for venous return, <inline-formula id="inf1">
<mml:math id="m1">
<mml:mrow>
<mml:mo>&#x2206;</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula> P<sub>VR1</sub>) causes a diminished venous return on the y-axis (liters per minute, L/min). The same P<sub>RA</sub> in a system with P<sub>MSF2</sub> (i.e., increased pressure gradient for venous return, <inline-formula id="inf2">
<mml:math id="m2">
<mml:mrow>
<mml:mo>&#x2206;</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula> P<sub>VR2</sub>) results in a higher venous return on the y-axis. The P<sub>MSF</sub> is the pressure in the right atrium at zero flow (i.e., the x-intercept). V<sub>S</sub> and C are the stressed volume and average compliance, respectively, of the systemic vasculature. The flattening of the venous return curve is where the great veins collapse; this creates a maximal venous return in each state.</p>
</caption>
<graphic xlink:href="fphys-14-1230654-g002.tif"/>
</fig>
<p>Downstream from the P<sub>MSF</sub> is the P<sub>RA</sub>. In Guyton&#x2019;s original experimental set-up, P<sub>RA</sub> was studied as an independent variable, altered via the height of a collapsible tube (<xref ref-type="bibr" rid="B36">Guyton et al., 1957</xref>). Guyton observed that the P<sub>RA</sub> was inversely related to venous return; in other words, decreasing P<sub>RA</sub> increased venous return, linearly (<xref ref-type="fig" rid="F2">Figure 2</xref>). Consequently, the difference between P<sub>MSF</sub> and P<sub>RA</sub> is the pressure gradient for venous return (<inline-formula id="inf3">
<mml:math id="m3">
<mml:mrow>
<mml:mo>&#x2206;</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula> P<sub>VR</sub>); the value of this gradient is directly proportional to blood return to the right heart (Equation <xref ref-type="disp-formula" rid="e1">1</xref>). More concretely, an increase in P<sub>MSF</sub> and/or decrease in P<sub>RA</sub> will augment venous return and <italic>vice versa</italic> (<xref ref-type="bibr" rid="B53">Magder, 2012</xref>).</p>
</sec>
<sec id="s1-3-1">
<title>The resistance to venous return</title>
<p>Guyton began with a mathematical approximation of the circulation, modeled after a system of distensible tubes (<xref ref-type="bibr" rid="B43">Jacobsohn et al., 1997</xref>). In this representation, the forces that resist total blood flow back to the heart are termed the &#x2018;resistance to venous return&#x2019; (R<sub>VR</sub>). While the R<sub>VR</sub> is often considered to be a purely Poiseuillean description of the venous circulation, this is not correct. The R<sub>VR</sub>, like the P<sub>MSF</sub>, is a weighted average of the system (i.e., including arterial components) (<xref ref-type="bibr" rid="B43">Jacobsohn et al., 1997</xref>). Each vascular bed faces a downstream resistance and has a unique compliance; the R<sub>VR</sub> is a summation of the downstream resistance encountered by each vascular bed, multiplied by its individual compliance relative to the total compliance of the system (<xref ref-type="fig" rid="F3">Figure 3</xref>).</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>The resistance to venous return (R<sub>VR</sub>). R<sub>VR</sub> is composed of resistances (R<sub>x</sub>) and compliances (C<sub>x</sub>) for the entire circulation. This simplified model shows 3 vascular segments in series. The R<sub>VR</sub> is the sum of the resistance and compliance for each segment divided by the total compliance of the circulatory system (C<sub>TOT</sub>). Resistance multiplied by compliance is the time constant (<inline-formula id="inf4">
<mml:math id="m4">
<mml:mrow>
<mml:mi>&#x3c4;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>).</p>
</caption>
<graphic xlink:href="fphys-14-1230654-g003.tif"/>
</fig>
<p>In this way the R<sub>VR</sub> can also be described by the time constant (i.e., the resistance multiplied by the compliance) of each vascular segment (<xref ref-type="bibr" rid="B55">Magder, 2016</xref>). This is clinically-important because diverting blood volume towards or away from a vascular bed with a long time constant (e.g., the splanchnic circulation) will increase or decrease the R<sub>VR</sub>, respectively (<xref ref-type="bibr" rid="B16">Caldini et al., 1974</xref>). The converse is true for vascular beds with a short time constant (e.g., kidneys, muscle) (<xref ref-type="bibr" rid="B55">Magder, 2016</xref>) (<xref ref-type="fig" rid="F4">Figure 4</xref>). Accordingly, should an intervention in the ICU (e.g., prone position) alter the fraction of flow to vascular beds of differing time constants, R<sub>VR</sub> will be affected.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>The resistance to venous return with high and low time-constant segments in parallel. This is an expansion of <xref ref-type="fig" rid="F3">Figure 3</xref> with two representative segments in parallel&#x2013;the non-splanchnic (NS) (i.e., low time constant, <inline-formula id="inf5">
<mml:math id="m5">
<mml:mrow>
<mml:mfenced open="" close=")" separators="|">
<mml:mrow>
<mml:mi>&#x3c4;</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:math>
</inline-formula> and splanchnic (S) (i.e., high <inline-formula id="inf6">
<mml:math id="m6">
<mml:mrow>
<mml:mfenced open="" close=")" separators="|">
<mml:mrow>
<mml:mi>&#x3c4;</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:math>
</inline-formula> segments. Here the fraction of total circulatory flow (Q<sub>circulatory</sub>) to the splanchnic (i.e., Q<sub>S</sub>/Q<sub>circulatory</sub>) <italic>versus</italic> non-splanchnic (i.e., Q<sub>NS</sub>/Q<sub>circulatory</sub>) segments determines the R<sub>VR</sub>. If all blood diverted to the splanchnic segment (i.e., Q<sub>S</sub>/Q<sub>circulatory</sub> &#x3d; 1.0; Q<sub>NS</sub>/Q<sub>circulatory</sub> &#x3d; 0.0), its higher compliance (C<sub>S</sub>) increases R<sub>VR</sub>. If all blood diverted to the non-splanchnic segment (i.e., Q<sub>S</sub>/Q<sub>circulatory</sub> &#x3d; 0.0; Q<sub>NS</sub>/Q<sub>circulatory</sub> &#x3d; 1.0), its lower compliance (C<sub>NS</sub>) decreases R<sub>VR</sub> (assuming all other resistances remain equal). C<sub>TOT</sub> is the total compliance of the system.</p>
</caption>
<graphic xlink:href="fphys-14-1230654-g004.tif"/>
</fig>
<p>On the venous return curve, change in the R<sub>VR</sub> alters the slope for a given pressure gradient (<xref ref-type="fig" rid="F5">Figure 5</xref>). An increase in R<sub>VR</sub> reduces the slope, while a decrease in R<sub>VR</sub> steepens the slope.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>The R<sub>VR</sub> and the venous return curve. P<sub>MSF</sub> is constant, but the resistance to venous return changes. The shallow curve is a higher resistance (<inline-formula id="inf7">
<mml:math id="m7">
<mml:mrow>
<mml:mo>&#x2191;</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula> R<sub>VR</sub>) the steeper curve is a lower resistance (<inline-formula id="inf8">
<mml:math id="m8">
<mml:mrow>
<mml:mo>&#x2193;</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula> R<sub>VR</sub>). At the same P<sub>RA</sub>, lower resistance and higher resistance generate increased and decreased flow (L/min), respectively. V<sub>S</sub> and C are the stressed volume and average compliance, respectively, of the systemic vasculature. The flattening of the venous return curve is where the great veins collapse; this creates a maximal venous return in each state.</p>
</caption>
<graphic xlink:href="fphys-14-1230654-g005.tif"/>
</fig>
<p>In summary, venous return is directly proportional to the P<sub>MSF</sub> less the P<sub>RA</sub> and indirectly proportional to the R<sub>VR</sub>. If the P<sub>MSF</sub> increases and/or P<sub>RA</sub> falls, then venous return rises (<xref ref-type="fig" rid="F2">Figure 2</xref>). Similarly, decreased R<sub>VR</sub> facilitates blood return to the heart and <italic>vice versa</italic> (<xref ref-type="fig" rid="F5">Figure 5</xref>). The Ohmic representation of this relationship is as follows (<xref ref-type="bibr" rid="B4">Berger and Takala, 2018</xref>):<disp-formula id="e1">
<mml:math id="m9">
<mml:mrow>
<mml:mi>v</mml:mi>
<mml:mi>e</mml:mi>
<mml:mi>n</mml:mi>
<mml:mi>o</mml:mi>
<mml:mi>u</mml:mi>
<mml:mi>s</mml:mi>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mi>r</mml:mi>
<mml:mi>e</mml:mi>
<mml:mi>t</mml:mi>
<mml:mi>u</mml:mi>
<mml:mi>r</mml:mi>
<mml:mi>n</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mrow>
<mml:mi>M</mml:mi>
<mml:mi>S</mml:mi>
<mml:mi>F</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mrow>
<mml:mi>R</mml:mi>
<mml:mi>A</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
<mml:msub>
<mml:mi>R</mml:mi>
<mml:mrow>
<mml:mi>V</mml:mi>
<mml:mi>R</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mfrac>
</mml:mrow>
</mml:math>
<label>(1)</label>
</disp-formula>
</p>
</sec>
</sec>
<sec id="s1-3-2">
<title>Venous return and cardiac function: the Guyton diagram</title>
<p>In addition to detailing the peripheral vascular determinants of blood returning <italic>to</italic> the heart, Guyton expanded our understanding of hemodynamics by adding to his analysis the cardiac determinants of blood flow <italic>from</italic> the heart. He did so by superimposing the venous return and Starling-Sarnoff curves (<xref ref-type="bibr" rid="B35">Guyton, 1955</xref>); this depiction is commonly referred to as the &#x2018;Guyton diagram.&#x2019; These curves can be placed over each other because they both have P<sub>RA</sub> on the x-axis and blood flow on the y-axis (<xref ref-type="fig" rid="F6">Figure 6</xref>). Though it will be developed in more detail below, the Guyton diagram introduces an important distinction between intravascular and transmural pressures. The P<sub>RA</sub> and P<sub>MSF</sub> measured on the Guyton diagram are intravascular pressures. Thus, the pressure gradient for venous return is directly related to the difference between the <italic>intravascular</italic> P<sub>MSF</sub> and P<sub>RA</sub> (Equation <xref ref-type="disp-formula" rid="e1">1</xref>). The Starling mechanism, however, is related to right atrial <italic>transmural</italic> pressure which is the pressure within the right atrium less its ambient pressure (i.e., the pericardial pressure). The transmural right atrial pressure is a static pressure that determines cardiac myocyte stretch which servo-controls the ejected stroke volume to match the venous return inflow.</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>The Guyton diagram. <bold>(A)</bold> The circulation in its resting state; as in <xref ref-type="fig" rid="F2">Figure 2</xref>, the x-axis is right atrial pressure in millimeters of mercury (mmHg) and y-axis is total blood flow in liters per minute (L/min). The P<sub>MSF</sub> is approximately 8&#xa0;mmHg at the x-intercept of the venous return curve (in blue). The Starling-Sarnoff (or cardiac function) curve is in red in a normal, upright position; its x-intercept is the pressure around the right atrium, the pericardial pressure (P<sub>PC</sub>). In this model, the dependent variable is the operating point, at the intersection of the venous return and cardiac function curves at equilibrium. Accordingly, both the x- (i.e., P<sub>RA</sub>) and y- (i.e., Q<sub>circulatory</sub>) coordinates defined by the operating point are also dependent variables. <bold>(B)</bold> How the P<sub>RA</sub> and Q<sub>circulatory</sub> are determined by the system. Normal cardiac function but diminished P<sub>MSF1</sub> (e.g., volume loss, venodilation) results in operating point 1 (OP<sub>1</sub>), diminished P<sub>RA</sub> and Q<sub>circulatory</sub>. Normal cardiac function with increased P<sub>MSF2</sub> (e.g., volume expansion, decreased venous capacitance from adrenergic agents) causes OP<sub>2</sub> (i.e., increased P<sub>RA</sub> and Q<sub>circulatory</sub>). Reduced P<sub>MSF</sub> and diminished cardiac function (e.g., acute cor pulmonale with tricuspid regurgitation) leads to OP<sub>3</sub>. Elevated P<sub>MSF</sub> with reduced cardiac function leads to OP<sub>4</sub>. Both Q<sub>circulatory</sub> and P<sub>RA</sub> are dependent variables in this system. The independent variables are reflected in the position and slopes of the venous return and cardiac function curves.</p>
</caption>
<graphic xlink:href="fphys-14-1230654-g006.tif"/>
</fig>
<p>Like any model, the value of the Guyton diagram is that it makes explicit the system&#x2019;s independent and dependent variables. Independent variables are those things the clinician can change or control (e.g., vascular volume and capacitance, airway pressure), whereas dependent variables are what the clinician wants to predict or study (e.g., cardiac output) by manipulating the independent variables. These distinctions are critical when considering the effects of any intervention in the ICU (e.g., prone position).</p>
<p>Nestled within the venous return curve are some of the independent variables of the circulatory system touched upon above: 1.) vascular capacitance, 2.) total vascular volume and 3.) the R<sub>VR</sub>. Thus, increasing total vascular volume via intravenous fluids and/or decreasing vascular capacitance via alpha-agonists both augment the V<sub>S</sub> and, therefore, P<sub>MSF</sub>. On the Guyton diagram, raising P<sub>MSF</sub> right-shifts the venous return curve such that there is increased blood flow to the heart for any given P<sub>RA</sub>. Similarly, beta-agonists (<xref ref-type="bibr" rid="B31">Green, 1977</xref>) and/or shunting blood from long to short time-constant vascular beds decreases the R<sub>VR</sub> (<xref ref-type="bibr" rid="B16">Caldini et al., 1974</xref>); this also enhances venous return for any given P<sub>RA</sub>. On the Guyton diagram, diminished R<sub>VR</sub> is manifested by an increased slope of the venous return curve (<xref ref-type="fig" rid="F6">Figure 6</xref>). The converse also holds, diminished blood volume, increased capacitance and/or increased R<sub>VR</sub> all reduce venous return for any given P<sub>RA</sub>. One clinically-important scenario wherein vascular capacitance rises (i.e., which decreases P<sub>MSF</sub>) is reduced adrenergic tone (e.g., sedation, anesthesia, relief of hypoxemia) (<xref ref-type="bibr" rid="B11">Bressack and Raffin, 1987</xref>).</p>
<p>Found within the cardiac function curve are additional independent variables: heart rate, rhythm, valve function, afterload, inotropic and lusitropic states (<xref ref-type="bibr" rid="B22">Feihl and Broccard, 2009a</xref>; <xref ref-type="bibr" rid="B23">Feihl and Broccard, 2009b</xref>). Consequently, rate and rhythm control (e.g., cardioversion), afterload reduction (e.g., vasodilator therapy, pulmonary vascular recruitment), enhanced contractility and improved relaxation (e.g., epinephrine infusion) all increase the slope of the Starling-Sarnoff curve. With this, blood flow from the heart is enhanced for any given P<sub>RA</sub>. The converse also holds, for example, rapid atrial dysrhythmia coupled with torrential tricuspid regurgitation and severe pulmonary arterial hypertension decreases the slope of the cardiac function curve, that is to say, reduce cardiac output for any given P<sub>RA</sub> (<xref ref-type="fig" rid="F6">Figure 6</xref>).</p>
<p>But what about the P<sub>RA</sub> itself? Is it an independent variable? In Guyton&#x2019;s experimental work on venous return, P<sub>RA</sub> was studied as an independent variable. However, on the Guyton diagram, which considers both venous return and cardiac function simultaneously, P<sub>RA</sub> is <italic>not</italic> independent. This was clearly stated by Guyton in his initial proposal: &#x201c;<italic>right atrial pressure is not one of the primary determinants of cardiac output but, instead, is itself determined simultaneously with cardiac output</italic>&#x201d; (<xref ref-type="bibr" rid="B35">Guyton, 1955</xref>). Later, Fiehl and Broccard expanded upon P<sub>RA</sub> as a dependent variable in their excellent review (<xref ref-type="bibr" rid="B22">Feihl and Broccard, 2009a</xref>). Accordingly, when analyzing venous return and cardiac function <italic>simultaneously</italic>, the dependent variable is the equilibrium formed at their intersection&#x2013;the operating point. Thus, both the x- (i.e., P<sub>RA</sub>) and y- (i.e., cardiac output) Cartesian coordinates are equally dependent upon the system. This may be counterintuitive given the convention of placing the independent variable on the x-axis, however, with the Guyton diagram this is a vestige of his initial work on venous return. When it is understood that the operating point is the dependent variable, the circular and specious reasoning that the concept of venous return is incorrect because &#x2018;raising P<sub>RA</sub> reduces venous return per Guyton but augments cardiac output by Starling&#x2019; becomes moot. Rather, at any given time (or in response to an intervention, such as the prone position) there are characteristics of the peripheral circulation and heart that, in tandem, produce a unique cardiac output <italic>and</italic> P<sub>RA</sub> (<xref ref-type="bibr" rid="B35">Guyton, 1955</xref>). To clarify this, a modified Guyton model is proposed below to disclose the clinically-relevant independent variables.</p>
</sec>
</sec>
<sec id="s1-4">
<title>A geometrical model</title>
<p>This is a simplified geometric approximation of the principles discussed above. If we consider the intersection of cardiac function and venous return as two directly-opposed right triangles, then we can solve for the height of their shared apex at equilibrium (i.e., cardiac output or venous return presently identified as Q<sub>circulatory</sub>) as a function of their bases and hypotenuse slopes (<xref ref-type="fig" rid="F7">Figure 7</xref>). Q<sub>circulatory</sub> is numerically equivalent to cardiac output and/or venous return. It is used in the geometrical model to emphasize that total blood flow (i.e., Q<sub>circulatory</sub>) is determined by the operating point&#x2013;the intersection of both peripheral venous <italic>and</italic> cardiac function. This avoids the confusion that sometimes arises when &#x2018;cardiac output&#x2019; is thought to be determined only by cardiac factors or when &#x2018;venous return&#x2019; is thought entirely due to peripheral factors; &#x2018;Q<sub>circulatory</sub>&#x2019; circumvents this ambiguity.</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>Simplified geometrical model. This model borrows from the Guyton diagram where the red line represents cardiac function and the blue line venous return. Two right triangles are formed as described in the text; the operating point is the apex of the two right triangles. Note that the slope (change in flow per unit pressure) is conductance, G. The inverse of conductance is resistance. As in previous figures, P<sub>PC</sub> is pericardial pressure, P<sub>MSF</sub> is mean systemic filling pressure, R<sub>cardiac</sub> and R<sub>VR</sub> are cardiac and venous resistance, respectively. Q<sub>circulatory</sub> is blood flow of the system with right atrial pressure (P<sub>RA</sub>) in millimeters of mercury (mmHg) on the x-axis and blood flow in liters per minute (L/min) on the y-axis.</p>
</caption>
<graphic xlink:href="fphys-14-1230654-g007.tif"/>
</fig>
<p>The base of the left triangle rests on the x-axis and is defined by the pressure immediately surrounding the heart, within the pericardium (i.e., the P<sub>PC</sub>) and the P<sub>RA</sub>; this is the transmural pressure of the right atrium. The slope (i.e., hypotenuse) of this triangle is the change in cardiac output per mmHg of transmural right atrial pressure, or cardiac conductance (G<sub>cardiac</sub>). This value is estimated to be 35&#xa0;mL/min/kg per 1&#xa0;mmHg (<xref ref-type="bibr" rid="B73">Rothe, 1993</xref>). Multiplying the base of this triangle (i.e., P<sub>RA</sub>&#x2013;P<sub>PC</sub>) by the slope of the hypotenuse (G<sub>cardiac</sub>) gives the height of this triangle (i.e., total circulatory flow, Q<sub>circulatory</sub>).<disp-formula id="e2">
<mml:math id="m10">
<mml:mrow>
<mml:msub>
<mml:mi>Q</mml:mi>
<mml:mrow>
<mml:mi>c</mml:mi>
<mml:mi>i</mml:mi>
<mml:mi>r</mml:mi>
<mml:mi>c</mml:mi>
<mml:mi>u</mml:mi>
<mml:mi>l</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>t</mml:mi>
<mml:mi>o</mml:mi>
<mml:mi>r</mml:mi>
<mml:mi>y</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:msub>
<mml:mi mathvariant="normal">G</mml:mi>
<mml:mrow>
<mml:mi>c</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>r</mml:mi>
<mml:mi>d</mml:mi>
<mml:mi>i</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>c</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mi>x</mml:mi>
<mml:mtext>&#x2009;</mml:mtext>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mrow>
<mml:mi>R</mml:mi>
<mml:mi>A</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>C</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(2)</label>
</disp-formula>
</p>
<p>Equation <xref ref-type="disp-formula" rid="e2">2</xref> is solved for P<sub>RA</sub>
<disp-formula id="e3">
<mml:math id="m11">
<mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mrow>
<mml:mi>R</mml:mi>
<mml:mi>A</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>Q</mml:mi>
<mml:mrow>
<mml:mi>c</mml:mi>
<mml:mi>i</mml:mi>
<mml:mi>r</mml:mi>
<mml:mi>c</mml:mi>
<mml:mi>u</mml:mi>
<mml:mi>l</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>t</mml:mi>
<mml:mi>o</mml:mi>
<mml:mi>r</mml:mi>
<mml:mi>y</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">G</mml:mi>
<mml:mrow>
<mml:mi>c</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>r</mml:mi>
<mml:mi>d</mml:mi>
<mml:mi>i</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>c</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x2b;</mml:mo>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mrow>
<mml:mi>P</mml:mi>
<mml:mi>C</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
<label>(3)</label>
</disp-formula>
</p>
<p>Similarly, the base of the rightmost triangle is defined by the P<sub>MSF</sub> and the P<sub>RA</sub>; this is the pressure gradient for venous return (the difference between two intravascular pressures along a hypothetical length of vessel), as above. The slope of this triangle is the change in cardiac output per the gradient for venous return, or venous conductance (G<sub>VR</sub>). Based on a P<sub>MSF</sub> of 8&#xa0;mmHg, this value is estimated to be 10&#xa0;mL/kg/min per 1&#xa0;mmHg. Multiplying the base of this triangle (i.e., P<sub>MSF</sub>&#x2013;P<sub>RA</sub>) by the slope of its hypotenuse (G<sub>VR</sub>) gives the height of this triangle, which is also total circulatory flow, Q<sub>circulatory</sub>.<disp-formula id="e4">
<mml:math id="m12">
<mml:mrow>
<mml:msub>
<mml:mi>Q</mml:mi>
<mml:mrow>
<mml:mi>c</mml:mi>
<mml:mi>i</mml:mi>
<mml:mi>r</mml:mi>
<mml:mi>c</mml:mi>
<mml:mi>u</mml:mi>
<mml:mi>l</mml:mi>
<mml:mi>a</mml:mi>
<mml:mi>t</mml:mi>
<mml:mi>o</mml:mi>
<mml:mi>r</mml:mi>
<mml:mi>y</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:msub>
<mml:mi mathvariant="normal">G</mml:mi>
<mml:mrow>
<mml:mi>V</mml:mi>
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<label>(4)</label>
</disp-formula>
</p>
<p>Equation <xref ref-type="disp-formula" rid="e4">4</xref> is solved for P<sub>RA</sub>
<disp-formula id="e5">
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<label>(5)</label>
</disp-formula>
</p>
<p>Setting equation <xref ref-type="disp-formula" rid="e3">3</xref> equal to equation <xref ref-type="disp-formula" rid="e5">5</xref>, we can reduce the equation to Q<sub>circulatory</sub> as follows:<disp-formula id="e6">
<mml:math id="m14">
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<label>(6)</label>
</disp-formula>
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<label>(7)</label>
</disp-formula>
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<label>(8)</label>
</disp-formula>
<disp-formula id="e9">
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<label>(9)</label>
</disp-formula>
</p>
<p>Because the inverse of conductance, G, is resistance, this equation can be written as:<disp-formula id="e10">
<mml:math id="m18">
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<label>(10)</label>
</disp-formula>
</p>
<p>Accordingly, in this model the shared apex of the two triangles (i.e., the operating point, which defines Q<sub>circulatory</sub>) is a function of the total base of the two triangles (i.e., P<sub>MSF</sub> less P<sub>PC</sub>) and the inverse of the slopes of their respective hypotenuses (i.e., R<sub>VR</sub> and R<sub>cardiac</sub>). More concretely, if R<sub>VR</sub> and R<sub>cardiac</sub> remain constant, increased P<sub>MSF</sub> and/or decreased pressure surrounding the heart (P<sub>PC</sub>) raise the height of their shared apex (<xref ref-type="fig" rid="F8">Figure 8</xref>). A concomitant decrease in R<sub>cardiac</sub> (i.e., increased slope of the Starling-Sarnoff curve) or R<sub>VR</sub> (i.e., increased slope of the venous return curve) would further elevate their shared apex (<xref ref-type="fig" rid="F8">Figure 8</xref>).</p>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>The independent and dependent variables of the geometric model. <bold>(A)</bold> The effect of changing the independent variables, P<sub>PC</sub> and P<sub>MSF</sub> on the dependent variable (operating point, OP). OP<sub>1</sub> depicts baseline conditions, its x- (P<sub>RA</sub>) and y-(Q<sub>circulatory</sub>) coordinates are shown. A solitary increase in P<sub>MSF</sub> (e.g., volume infusion) results in OP<sub>2</sub>, that is, increased P<sub>RA</sub> and Q<sub>circulatory</sub>. A selective decrease in P<sub>PC</sub> (e.g., spontaneous inspiration) leads to OP<sub>3</sub> which increases Q<sub>circulatory</sub>, but decreases P<sub>RA</sub>. If P<sub>MSF</sub> rises and P<sub>PC</sub> falls, the result is OP<sub>4</sub>, increased Q<sub>circulatory</sub> at a slightly reduced P<sub>RA</sub> relative to baseline. <bold>(B)</bold> The effect of changing the independent variables, R<sub>VR</sub> and R<sub>cardiac</sub> on the dependent variable (operating point, OP). A selective decrease in venous resistance (e.g., shunting blood away from the splanchnic circulation) leads to OP<sub>2</sub> (i.e., both P<sub>RA</sub> and Q<sub>circulatory</sub> rise). A selective decrease in cardiac resistance (i.e., improving cardiac function by, for example, reducing pulmonary vascular resistance) leads to OP<sub>3</sub> (i.e., P<sub>RA</sub> falls, while Q<sub>circulatory</sub> rises). Reducing venous and cardiac resistance together leads to OP<sub>4</sub> (i.e., little P<sub>RA</sub> change with large Q<sub>circulatory</sub> augmentation).</p>
</caption>
<graphic xlink:href="fphys-14-1230654-g008.tif"/>
</fig>
<p>In this model, P<sub>RA</sub> plays no role in cardiac output because the operating point (i.e., the shared apex) is the dependent variable; Q<sub>circulatory</sub> and P<sub>RA</sub> <italic>both</italic> fall out from this equilibrium (<xref ref-type="bibr" rid="B22">Feihl and Broccard, 2009a</xref>). The equations above could have equally been solved for P<sub>RA</sub> instead of Q<sub>circulatory</sub>; P<sub>RA</sub>, nevertheless, would still be dependent upon P<sub>MSF</sub>, P<sub>PC</sub>, R<sub>cardiac</sub> and R<sub>VR</sub>.</p>
<p>To further develop this model with an emphasis on heart-lung interaction, the determinants of P<sub>PC</sub> are included. Doing so reveals additional, clinically-relevant independent variables when placing an ARDS patient in the prone position. The P<sub>PC</sub> is the x-intercept of the hypotenuse defined by R<sub>cardiac</sub> (i.e., the cardiac function curve) (<xref ref-type="bibr" rid="B54">Magder, 2004</xref>; <xref ref-type="bibr" rid="B22">Feihl and Broccard, 2009a</xref>). As originally hypothesized by Guyton (<xref ref-type="bibr" rid="B22">Feihl and Broccard, 2009a</xref>) and demonstrated by Marini and colleagues (<xref ref-type="bibr" rid="B56">Marini et al., 1981</xref>), increasing P<sub>PC</sub> initiates a parallel, right-shift of the cardiac function curve. Consequently, increased P<sub>PC</sub> decreases the shared apex (i.e., the operating point) and Q<sub>circulatory</sub> is diminished but only if there is no simultaneous change in P<sub>MSF</sub>, R<sub>cardiac</sub> or R<sub>VR</sub>.</p>
<p>Given that the P<sub>PC</sub> is a summation of: 1.) pleural pressure (P<sub>PL</sub>), 2.) pressure added by mechanical ventilation (i.e., estimated as the mean airway pressure, P<sub>AW</sub>, multiplied by the ratio of the chest wall to respiratory system elastances, E<sub>CW</sub>/E<sub>RS</sub>) (<xref ref-type="bibr" rid="B27">Gattinoni et al., 2004</xref>) and 3.) the elastic recoil pressure of the pericardium (P<sub>PC<sub>EL</sub>
</sub>) (<xref ref-type="bibr" rid="B15">Cabrera et al., 1989</xref>), we can expand equation <xref ref-type="disp-formula" rid="e10">10</xref> above.<disp-formula id="e11">
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<label>(11)</label>
</disp-formula>
</p>
<p>Accordingly, increased pleural (e.g., thoracic supports) and/or elastic recoil pressure from the pericardium (e.g., right ventricular dilatation in acute cor pulmonale), raise the pressure surrounding the heart, P<sub>PC</sub>. Furthermore, elevated P<sub>AW</sub> (e.g., increasing positive end-expiratory pressure, PEEP) or a stiffened chest wall (e.g., prone position increases the E<sub>CW</sub>/E<sub>RS</sub> ratio) both amplify P<sub>PC</sub>; from equation <xref ref-type="disp-formula" rid="e11">11</xref>, we see that increasing P<sub>PC</sub> reduces Q<sub>circulatory</sub> but only if P<sub>MSF</sub>, R<sub>cardiac</sub> and R<sub>VR</sub> are constant. It should not escape the reader&#x2019;s attention that including P<sub>PC</sub> in this model is a crucial link between cardiac and respiratory physiologies.</p>
<sec id="s1-4-1">
<title>Cardiac limitation</title>
<p>While the proposed model is meant to illuminate the clinically-relevant independent variables determining Q<sub>circulatory</sub>, equation <xref ref-type="disp-formula" rid="e11">11</xref> has important caveats (<xref ref-type="bibr" rid="B53">Magder, 2012</xref>). The most important is that it is predicated upon the intersection of two hypotenuses; <italic>in vivo</italic>, both the venous return and cardiac function curves have portions that flatten out. When the operating point falls upon the flat portion of the cardiac function curve, Q<sub>circulatory</sub> depends only upon the independent variables of cardiac function: P<sub>PC</sub>, the right atrial pressure at which the cardiac function curve begins to plateau, P<sub>RAplat</sub> and the R<sub>cardiac</sub> (<xref ref-type="fig" rid="F9">Figure 9</xref>).<disp-formula id="e12">
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<label>(12)</label>
</disp-formula>
</p>
<fig id="F9" position="float">
<label>FIGURE 9</label>
<caption>
<p>Operating point positions in the geometrical model. <bold>(A)</bold> reveals cardiac limitation where the operating point (OP) is on the flat portion of the cardiac function curve. Change in P<sub>MSF</sub> or R<sub>VR</sub> change only P<sub>RA</sub> and not Q<sub>circulatory</sub> (OP<sub>1</sub> <italic>versus</italic> OP<sub>2</sub>). <bold>(B)</bold> is when the system is neither venous nor cardiac limited. Q<sub>circulatory</sub> is changed by P<sub>MSF</sub>, P<sub>PC</sub>, R<sub>cardiac</sub> and R<sub>VR</sub> (see <xref ref-type="fig" rid="F5">Figure 5</xref>). <bold>(C)</bold> shows venous limitation or &#x2018;waterfall&#x2019; physiology. Changes in cardiac function alter only P<sub>RA</sub> and not Q<sub>circulatory</sub> (OP<sub>1</sub> <italic>versus</italic> OP<sub>2</sub>).</p>
</caption>
<graphic xlink:href="fphys-14-1230654-g009.tif"/>
</fig>
<p>Fundamentally, this equation relays that Q<sub>circulatory</sub> is no longer determined by peripheral factors when the operating point is above the P<sub>RAplat</sub>. Changing P<sub>MSF</sub> or R<sub>VR</sub> only alter P<sub>RA</sub> with fixed Q<sub>circulatory</sub>.</p>
</sec>
<sec id="s1-4-2">
<title>Venous limitation</title>
<p>In a manner similar to cardiac function, the venous return curve also flattens when the P<sub>RA</sub> falls below venous collapse pressure, P<sub>CRIT</sub> (<xref ref-type="bibr" rid="B53">Magder, 2012</xref>). This is the formation of a Starling resistor when the great veins enter the thorax and is observed with ultrasound as collapse of the great veins. This phenomenon is also termed &#x2018;waterfall&#x2019; physiology because the pressure below P<sub>CRIT</sub> has no bearing on flow, just as the height of a waterfall does not mediate its flow (<xref ref-type="bibr" rid="B68">Permutt and Riley, 1963</xref>). Consequently, when the operating point lies to the left of P<sub>CRIT</sub> (i.e., on the &#x201c;flat portion&#x201d; of the venous return curve) Q<sub>circulatory</sub> becomes independent of cardiac function or P<sub>PC</sub>; the independent variables are P<sub>CRIT</sub>, P<sub>MSF</sub> and R<sub>VR</sub> (<xref ref-type="fig" rid="F9">Figure 9</xref>).<disp-formula id="e13">
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<label>(13)</label>
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</p>
<p>In other words, when venous limited, reducing R<sub>cardiac</sub> (i.e., improving cardiac function) or changing P<sub>PC</sub> has no bearing on Q<sub>circulatory</sub>; only changing P<sub>MSF</sub>, R<sub>VR</sub> or P<sub>CRIT</sub> might alter total flow.</p>
</sec>
</sec>
<sec id="s2">
<title>Implications for the prone position</title>
<p>With a Guyton-based circulatory model proposed above, anticipating the change in Q<sub>circulatory</sub> follows the independent variables of the system: P<sub>MSF</sub>, P<sub>PC</sub>, R<sub>cardiac</sub> and R<sub>VR</sub>. At present there are three key studies that have elucidated interactions between the circulation and prone position in ARDS (<xref ref-type="bibr" rid="B82">Vieillard-Baron et al., 2007</xref>; <xref ref-type="bibr" rid="B46">Jozwiak et al., 2013</xref>; <xref ref-type="bibr" rid="B48">Lai et al., 2021</xref>). Much of the discussion below is taken from these investigations.</p>
<sec id="s2-1">
<title>Mean systemic filling pressure</title>
<p>Recently, Lai and colleagues studied the effect of prone position on the determinants of venous return (<xref ref-type="bibr" rid="B48">Lai et al., 2021</xref>). They measured P<sub>MSF</sub> by extrapolating to zero flow a series of P<sub>RA</sub>&#x2013;cardiac output pairings in response to increasing airway pressure. Though this method overestimated P<sub>MSF</sub> in a porcine model (<xref ref-type="bibr" rid="B3">Berger et al., 2016</xref>), this observation was restricted to euvolemic conditions which are less likely in ARDS patients in the ICU. Nevertheless, considering the discussion on P<sub>MSF</sub> measurement above, a retrospective calculation of P<sub>MSA</sub> would be of great interest given that the average P<sub>MSF</sub> measured by Lai et al. was clinically quite high, especially in the prone position. Irrespective of absolute values, Lai and colleagues observed that P<sub>MSF</sub> increased significantly from the semi-recumbent to prone position; they hypothesized that this was due to increased intra-abdominal pressure (IAP). However, the baseline value and change in IAP had no bearing on P<sub>MSF</sub> behavior. This is unsurprising given what is known about the mechanisms by which PEEP increase P<sub>MSF</sub>. Initially, it was also hypothesized that IAP mediated P<sub>MSF</sub> augmentation with PEEP application and/or stiffening of the chest wall (i.e., akin to prone position) in early canine models (<xref ref-type="bibr" rid="B76">Scharf et al., 1977</xref>). However, IAP had no role in raising P<sub>MSF</sub>, instead, adrenergic reflexes (i.e., changing vascular capacitance) and redistribution of blood volume from the central to peripheral circulation were the main drivers of P<sub>MSF</sub> rise (<xref ref-type="bibr" rid="B77">Scharf and Ingram, 1977</xref>; <xref ref-type="bibr" rid="B25">Fessler, 1995</xref>; <xref ref-type="bibr" rid="B26">Fessler, 1997</xref>). Accordingly, central blood volume, adrenergic reserve and exogenous vasoactive agents all undoubtedly mediate the change in P<sub>MSF</sub> upon pronation, rather than IAP. Parenthetically, this could also explain hemodynamic differences noted between elective surgical and critically-ill ARDS patients when prone position is employed (<xref ref-type="bibr" rid="B21">Edgcombe et al., 2008</xref>). The latter are more likely to be on vasoactive agents and volume-loaded, while the former more likely euvolemic; as well, anesthetic agents may blunt reflexive changes in vascular capacitance which would limit P<sub>MSF</sub> rise in the operating room. As described above, P<sub>MSF</sub> is directly related to Q<sub>circulatory</sub> when the patient is not cardiac limited and without concurrent changes in P<sub>PC</sub>, R<sub>cardiac</sub> or R<sub>VR</sub>.</p>
</sec>
<sec id="s2-1-1">
<title>Pericardial pressure</title>
<p>There are no known direct measurements of P<sub>PC</sub> in humans with ARDS placed in the prone position. Yet, inferences can be made given the mathematical approximation of P<sub>PC</sub> presented above. The prone position increases the elastance (i.e., stiffness) of the chest wall (E<sub>CW</sub>) (<xref ref-type="bibr" rid="B67">Pelosi et al., 1998</xref>). To the extent that pronation also decreases the elastance (i.e., improves compliance) of the lungs by alveolar recruitment, the E<sub>CW</sub> relative to the elastance of the respiratory system (i.e., the lungs and the chest wall together, E<sub>RS</sub>) rises. Multiplying the mean airway pressure generated by mechanical ventilation by the E<sub>CW</sub>/E<sub>RS</sub> ratio approximates P<sub>PC</sub> augmentation when a patient is passive with the ventilator. For example, if the mean airway pressure is 10&#xa0;mmHg with an E<sub>CW</sub>/E<sub>RS</sub> ratio of 0.3 in the supine position, then 3&#xa0;mmHg is added to the P<sub>PC</sub>. If mean airway pressure remains constant and prone position increases the E<sub>CW</sub>/E<sub>RS</sub> ratio to 0.5, then 5&#xa0;mmHg is added to the P<sub>PC</sub>.</p>
<p>Additionally, pericardial restraint could play an important role determining P<sub>PC</sub>, especially if there is comorbid acute cor pulmonale (ACP). Typically, when right atrial volume is low (i.e., estimated by a transmural pressure below 5&#xa0;mmHg (<xref ref-type="bibr" rid="B38">Hamilton et al., 1994</xref>)), there is little recoil pressure generated by the pericardium around it. As atrial volume increases beyond this, the pericardial sac is engaged and moves up its volume-pressure relationship. This leads to an increasingly large elastic recoil pressure from the pericardium, which raises the P<sub>PC</sub>. Elevated P<sub>PC</sub>, therefore, restricts right ventricular filling and &#x2018;protects&#x2019; from overdistention; however, this blunts Q<sub>circulatory</sub> by narrowing the P<sub>MSF</sub>&#x2013;P<sub>PC</sub> gradient.</p>
<p>In the setting of ACP, often seen in moderate-to-severe ARDS (<xref ref-type="bibr" rid="B33">Gu&#xe9;rin and Matthay, 2016</xref>; <xref ref-type="bibr" rid="B61">Mekontso Dessap et al., 2016</xref>), pericardial recoil may play an important role upon prone position. With ACP, co-existent right atrial distension elevates P<sub>PC</sub> by pericardial recoil; this is especially true with P<sub>RA</sub> above 10&#x2013;12&#xa0;mmHg (<xref ref-type="bibr" rid="B38">Hamilton et al., 1994</xref>). While prone position is expected to further increase P<sub>PC</sub> (i.e., by increasing P<sub>PL</sub>), to the extent that the elevated P<sub>PL</sub> shrinks cardiac volume, P<sub>PC</sub> may remain constant, or even fall, as the elastic recoil pressure imparted by the pericardium is reduced. More simply, the rising P<sub>PL</sub> experienced by the pericardial space is offset by falling recoil pressure of the pericardium. This was originally observed in models of continuous positive airway pressure in heart failure (<xref ref-type="bibr" rid="B42">Huberfeld et al., 1995</xref>). Were this to occur upon prone position in a patient with ACP, P<sub>PC</sub> would remain constant or fall. Taken with the effect of prone position on P<sub>MSF</sub> noted above, the P<sub>MSF</sub>&#x2013;P<sub>PC</sub> gradient would be maintained (or enhanced) and so too would Q<sub>circulatory</sub> if R<sub>cardiac</sub> and R<sub>VR</sub> remain constant.</p>
<p>Finally, some have argued for the execution of prone position with thoracoabdominal supports that allow the abdomen to hang freely (<xref ref-type="bibr" rid="B17">Chiumello et al., 2006</xref>). These supports are typically placed mid-sternum and below the pelvis. Chiumello and colleagues compared these supports to the abdomen flush with the bed in prone ARDS patients (<xref ref-type="bibr" rid="B17">Chiumello et al., 2006</xref>). They found that the supports accentuated local pressure without any benefit to gas exchange while diminishing stroke volume. Given support placement directly at the sternum, it is possible that P<sub>PC</sub> is accentuated, reducing the P<sub>MSF</sub>&#x2013;P<sub>PC</sub> gradient and Q<sub>circulatory</sub> barring a concomitant decrease in R<sub>cardiac</sub> or R<sub>VR</sub>.</p>
</sec>
<sec id="s2-1-2">
<title>Cardiac resistance</title>
<p>While not a commonly-employed term within the sphere of clinical hemodynamics, &#x2018;cardiac resistance&#x2019; (R<sub>cardiac</sub>) is analogous to R<sub>VR</sub>. Graphically and mathematically, R<sub>cardiac</sub> is simply the inverse slope of the cardiac function curve. A decrease in R<sub>cardiac</sub> (i.e., a steeper slope of the cardiac function curve) represents improved cardiac function and raises the operating point (i.e., Q<sub>circulatory</sub>) unless the system is venous limited. In an elegant ultrasonographic study, Vieillard-Baron and colleagues illuminated the salubrious effects on the RV prompted by prone position (<xref ref-type="bibr" rid="B82">Vieillard-Baron et al., 2007</xref>). In 21 patients with P<sub>a</sub>O<sub>2</sub>/F<sub>i</sub>O<sub>2</sub> ratio of less than 100&#xa0;mmHg and ACP defined as RV enlargement and septal dyskinesia, 18&#xa0;h of prone position led to a significant reduction in heart rate and increase in cardiac output. Furthermore, RV end-diastolic area fell while LV end-diastolic area increased and tricuspid regurgitation was reduced. Taken together, the rise in cardiac output with diminished RV size strongly implies reduced R<sub>cardiac</sub> as a mechanism of improved Q<sub>circulatory</sub>, at least in patients with ACP. The mechanism for this improvement (detailed at the outset of this review and by others (<xref ref-type="bibr" rid="B72">Repess&#xe9; et al., 2016</xref>)) was reduced pulmonary vascular impedance to flow facilitating RV ejection (<xref ref-type="bibr" rid="B44">Jardin and Vieillard-Baron, 2003</xref>; <xref ref-type="bibr" rid="B82">Vieillard-Baron et al., 2007</xref>) which improves stroke volume and cardiac output for any given P<sub>RA</sub>.</p>
<p>Recent studies also imply reduced R<sub>cardiac</sub>. Ruste and colleagues investigated the hemodynamic effects of prone position in over 100 patients (<xref ref-type="bibr" rid="B75">Ruste et al., 2018</xref>). 25% of prone sessions led to significantly increased cardiac output, while 23% had a significant decrease; the remainder showed no change. Importantly, of those sessions where cardiac output rose, 56% had no change or a decrease in global end-diastolic volume (GEDV) measured by transpulmonary thermodilution. Rising cardiac output without an increase in end-diastolic volume infers reduced R<sub>cardiac</sub>. Importantly, static GEDV with prone position could signify a shrinking RV end diastolic volume with enlarging LV end diastolic volume consistent with the reduced RV-to-LV end-diastolic area ratio observed with echocardiography by Vieillard-Baron et al. (<xref ref-type="bibr" rid="B82">Vieillard-Baron et al., 2007</xref>). Finally, Boesing and colleagues recently published on different PEEP titration strategies and their interaction with prone position (<xref ref-type="bibr" rid="B7">Boesing et al., 2022</xref>). In this study, esophageal pressure (P<sub>ES</sub>) was used as a surrogate for P<sub>PL</sub>. Curiously, the PEEP titration strategy that led to the greatest increase in cardiac output from supine to prone was associated with the smallest rise in transmural P<sub>RA</sub> (i.e., P<sub>RA</sub> less P<sub>ES</sub>), in other words, the least preload augmentation. Similar to the observations by Ruste and colleagues, this finding suggests, but does not prove, enhanced cardiac function (i.e., reduced R<sub>cardiac</sub>).</p>
</sec>
<sec id="s2-1-3">
<title>Resistance to venous return</title>
<p>In the study of Lai and colleagues (<xref ref-type="bibr" rid="B48">Lai et al., 2021</xref>), the R<sub>VR</sub> was calculated from semi-recumbent to prone position in ARDS patients. In total, R<sub>VR</sub> increased in the vast majority, though there were a few with stable or slightly diminished R<sub>VR</sub>. Like P<sub>MSF</sub>, the change in R<sub>VR</sub> was not related to IAP and like P<sub>MSF</sub>, this is unsurprising given the foundational work of Takata and Robotham (<xref ref-type="bibr" rid="B80">Takata et al., 1990</xref>). In their original model, Takata and Robotham proposed that the relationship between great vein pressure and IAP would behave analogously to West zones in the lung. That is, if the IAP is much greater than inferior vena cava (IVC) pressure (i.e., zone 2), then venous return is impaired when the abdomen is pressurized by diaphragmatic descent and, in theory, prone position. However, if IAP is much less than IVC pressure (i.e., zone 3), then increased IAP generated by diaphragmatic descent (or prone position) enhances venous return. Their initial work confirmed this model, however, they later found that the model held even with an open abdomen and evisceration, that is, constant IAP (<xref ref-type="bibr" rid="B79">Takata and Robotham, 1992</xref>). Thus, the ambient pressure of import was more likely focal subcostal, crural, or intra-hepatic pressure, rather than general IAP. This was observed by Decramer and colleagues (<xref ref-type="bibr" rid="B20">Decramer et al., 1984</xref>) and explored further by Brienza et al. in a porcine model (<xref ref-type="bibr" rid="B12">Brienza et al., 1995</xref>) and Jellinek et al. in humans (<xref ref-type="bibr" rid="B45">Jellinek et al., 2000</xref>). Accordingly, diaphragmatic shape-matching between the liver and upper abdomen, active <italic>versus</italic> passive diaphragm displacement, intra-hepatic compliance (e.g., intrinsic liver disease) and the use of focal thoracoabdominal supports, among other factors might affect hepatic pressure (P<sub>hepatic</sub>) upon pronation. Diminished venous pressure (e.g., hypovolemia, venodilation) relative to P<sub>hepatic</sub> might increase R<sub>VR</sub>. By contrast, elevated venous pressure (e.g., high blood volume, low venous capacitance) relative to P<sub>hepatic</sub> might blunt a rise in R<sub>VR</sub> with prone positioning.</p>
<p>Another possible mechanism for increased R<sub>VR</sub> with prone position follows that of P<sub>MSF</sub>. As described above, reflex sympathetic tone is a key mediator of increased P<sub>MSF</sub>. However, when alpha agonists act upon veins to increase the V<sub>S</sub>, resistance necessarily rises. This is because change in volume is proportional to the second power of vessel diameter but resistance is related to the fourth power. More concretely, if the diameter of a vein falls by 20% from its baseline, its volume is diminished by 36% (i.e., this reduces its capacitance, increases P<sub>MSF</sub>) but its resistance rises by 244% (<xref ref-type="bibr" rid="B73">Rothe, 1993</xref>). Because the splanchnic circulation is a crucial reservoir for venous blood, the rise in resistance in response to V<sub>S</sub> recruitment can be offset by beta-agonism (<xref ref-type="bibr" rid="B31">Green, 1977</xref>) in the hepatic veins, or redistribution of blood flow to short time constant vascular beds, as noted above (<xref ref-type="bibr" rid="B55">Magder, 2016</xref>) (<xref ref-type="fig" rid="F4">Figure 4</xref>). Nevertheless, hepatosplanchnic blood flow during prone position in ARDS changes little (<xref ref-type="bibr" rid="B40">Hering et al., 2002</xref>; <xref ref-type="bibr" rid="B59">Matejovic et al., 2002</xref>). Interestingly, one study found decreased renal blood flow (<xref ref-type="bibr" rid="B41">Hering et al., 2001</xref>)&#x2014;a fast time-constant bed; diversion of blood in this manner contributes to increased R<sub>VR</sub>. A final, potential mechanism for R<sub>VR</sub> augmentation with prone position lies in the superior vena cava (SVC). Fessler found that the rise in total R<sub>VR</sub> following PEEP application was predominantly due to the veins draining into the SVC rather than the IVC (<xref ref-type="bibr" rid="B24">Fessler et al., 1992</xref>). Because P<sub>PL</sub> is the pressure that surrounds SVC and prone tends to raise P<sub>PL</sub> for any given P<sub>AW</sub> (see equation <xref ref-type="disp-formula" rid="e11">11</xref> above), it is possible that mechanical compression of the SVC contributes to R<sub>VR</sub> (<xref ref-type="bibr" rid="B50">Lansdorp et al., 2014</xref>; <xref ref-type="bibr" rid="B3">Berger et al., 2016</xref>). Regardless of the mechanism, R<sub>VR</sub> is a critical determinant of Q<sub>circulatory</sub> (<xref ref-type="bibr" rid="B70">Pinsky, 2021</xref>).</p>
</sec>
<sec id="s2-1-4">
<title>Knowing the limits</title>
<p>Taking the above into consideration, a key factor when predicting the hemodynamic response to prone position is the location of the operating point whilst semi-recumbent; is the operating point &#x2018;cardiac limited&#x2019;, &#x2018;venous limited&#x2019; or &#x2018;unlimited&#x2019; (<xref ref-type="fig" rid="F6">Figure 6</xref>) (<xref ref-type="bibr" rid="B53">Magder, 2012</xref>)? Knowing this focuses the clinician on the independent variables most likely affecting Q<sub>circulatory</sub>. For instance, if the operating point is cardiac limited (<xref ref-type="fig" rid="F6">Figure 6</xref>) we see that changes in P<sub>MSF</sub> and R<sub>VR</sub> play no role, while changes in cardiac characteristics (e.g., R<sub>cardiac</sub>) mediate Q<sub>circulatory</sub>. Of course, this depends on how close the operating point is to the P<sub>RA</sub> at which the cardiac function curve flattens out, but this is, nevertheless, a reasonable clinical heuristic. Jozwiak and colleagues studied 18 ARDS patients with elevated right ventricular-to-left ventricular end-diastolic areas (RVEDA/LVEDA), but without ACP (<xref ref-type="bibr" rid="B46">Jozwiak et al., 2013</xref>). Prior to prone position, the change in cardiac output in response to a passive leg raise was evaluated. By the model above, &#x2018;cardiac limitation&#x2019; is detected when a patient is preload unresponsive. In this state, only improved cardiac function during pronation (i.e., reduced R<sub>cardiac</sub>) increases Q<sub>circulatory</sub>; changes in P<sub>MSF</sub> and R<sub>VR</sub> shift the operating point along the x-axis, but not the y-axis. In other words, P<sub>RA</sub> changes but not blood flow. Jozwiak and colleagues found that in &#x2018;cardiac limited&#x2019; patients, prone position significantly reduced pulmonary vascular resistance and the RVEDA/LVEDA which should diminish R<sub>cardiac</sub> and improve Q<sub>circulatory</sub>. However, these patients were also found to have depressed left ventricular ejection fraction. Furthermore, in the face of prone position, systemic afterload increased; total R<sub>cardiac</sub>, therefore, did not improve.</p>
<p>When patients are not &#x2018;cardiac limited,&#x2019; the operating point may be either &#x2018;unlimited&#x2019; or &#x2018;venous limited.&#x2019; In the study of Jozwiak and colleagues, imaging of the great veins was not reported, but those patients who were preload responsive were unlikely to have great vein collapse (i.e., venous &#x2018;waterfall&#x2019;) given that their average, baseline P<sub>RA</sub> was relatively high (i.e., 15&#xa0;mmHg) with increased RVEDA/LVEDA ratios. Thus, based on equation <xref ref-type="disp-formula" rid="e11">11</xref> above, the change in Q<sub>circulatory</sub> was probably subject to all of: P<sub>MSF</sub>, P<sub>PC</sub>, R<sub>cardiac</sub> and R<sub>VR</sub>. Given what we know from Lai and colleagues, prone position likely increased P<sub>MSF</sub>; P<sub>PC</sub> may have increased less than the rise in P<sub>PL</sub> because of reduced pericardial restraint and R<sub>cardiac</sub> fell due to diminished pulmonary vascular resistance. Each of these effects raise Q<sub>circulatory</sub>, presumably offsetting heightened R<sub>VR</sub> with prone (<xref ref-type="fig" rid="F10">Figure 10</xref>).</p>
<fig id="F10" position="float">
<label>FIGURE 10</label>
<caption>
<p>The geometrical model applied to representative data from Lai et al. <bold>(A)</bold> The effect of prone position on a preload responsive patient. At baseline, P<sub>PC</sub> is estimated by assuming a mean airway pressure of 15&#xa0;mmHg, an E<sub>CW</sub>/E<sub>RS</sub> ratio of 0.2 and a pleural pressure (P<sub>PL</sub>) at functional residual capacity of&#x2014;2.5&#xa0;mmHg. With prone position, the P<sub>MSF</sub> rises much more than P<sub>PC</sub>. There is an increase in R<sub>VR</sub> and an assumed decrease in R<sub>cardiac</sub> due to reduced pulmonary vascular resistance. The operating point with prone position (OP<sub>prone</sub>) leads to an increase in total blood flow (Q<sub>CIRC</sub>) and increased right atrial pressure (P<sub>RA</sub>). By this model, P<sub>RA</sub> does not determine Q<sub>CIRC</sub>; both P<sub>RA</sub> and Q<sub>CIRC</sub> are determined by P<sub>MSF</sub>, P<sub>PC</sub>, R<sub>cardiac</sub> and R<sub>VR</sub>. <bold>(B)</bold> Prone position in a preload unresponsive patient at baseline. P<sub>PC</sub> in prone is estimated by assuming a mean airway pressure of 15&#xa0;mmHg, and E<sub>CW</sub>/E<sub>RS</sub> ratio of 0.5 and a P<sub>PL</sub> at functional residual capacity of&#x2014;2.5&#xa0;mmHg. With cardiac limitation, only a significant change in R<sub>cardiac</sub> would increase Q<sub>CIRC</sub>.</p>
</caption>
<graphic xlink:href="fphys-14-1230654-g010.tif"/>
</fig>
<p>It is also possible for preload responsive patients to be &#x2018;venous limited&#x2019; as described by equation <xref ref-type="disp-formula" rid="e13">13</xref> above. When the operating point lies on the flat portion of the venous return curve (i.e., below P<sub>CRIT</sub>) then R<sub>cardiac</sub> ceases to affect Q<sub>circulatory</sub>. Said another way, blood flow is determined solely by peripheral venous factors. When &#x2018;venous limited&#x2019;, volume status is likely a crucial determinant of the hemodynamic response to prone position based on the model of Takata and Robotham described above (<xref ref-type="bibr" rid="B80">Takata et al., 1990</xref>). A zone 3 abdomen might have a stable or enhanced P<sub>MSF</sub> relative to P<sub>CRIT</sub> and blunt any increase in R<sub>VR</sub> (i.e., stable or increased Q<sub>circulatory</sub>), while a zone 2 abdomen would diminish P<sub>MSF</sub> relative to P<sub>CRIT</sub> and favour elevated R<sub>VR</sub> (i.e., stable or reduced Q<sub>circulatory</sub>). There is little data on &#x2018;venous limited&#x2019; ARDS patients being placed in prone. In the study by Lai and colleagues, there were four &#x2018;preload responsive&#x2019; patients who had no change (n &#x3d; 3) or a decrease (n &#x3d; 1) in Q<sub>ciculatory</sub> when placed in prone position. These patients may have been venous limited, but this data was not collected. Given that at low trans-mural pressure, the great veins are very compliant (<xref ref-type="bibr" rid="B6">Bodson and Vieillard-Baron, 2012</xref>), generation of a hemodynamically-significant Starling resistor, i.e., &#x2018;venous limitation,&#x2019; should lead to great vein collapse throughout most of the respiratory cycle. In a patient passive with the ventilator, collapse is an inspiratory event for the SVC and expiatory event for the IVC. Collecting this data with ultrasound before and after pronation could help delineate this hemodynamic phenotype.</p>
<p>Finally, it is possible to be both venous and cardiac limited simultaneously, in other words, the operating point is on both the flat portion of the venous return and cardiac function curves concurrently. This might happen in states of high P<sub>CRIT</sub> (e.g., high PEEP, high subdiaphragmatic pressure) coupled with depressed cardiac function. In the setting of ARDS, this could be a syndrome of alveolar over-distension (<xref ref-type="bibr" rid="B44">Jardin and Vieillard-Baron, 2003</xref>). Prone position in such a patient might reduce Q<sub>circulatory</sub>, especially if the patient is hypovolemic. Managing this hemodynamic phenotype might involve PEEP titration to reduce P<sub>CRIT</sub> and enhance cardiac function as this could move the operating point onto steep portions of the venous return and cardiac function curves.</p>
</sec>
</sec>
<sec sec-type="conclusion" id="s3">
<title>Conclusion</title>
<p>At equilibrium, the intersection of venous return and cardiac function generates the hemodynamic operating point. The operating point and both of its coordinates (i.e., P<sub>RA</sub> and Q<sub>circulatory</sub>) are dependent variables. The independent variables of the system are the P<sub>MSF</sub>, resistance to venous return, cardiac function and the pressure surrounding the right atrium. These are not new principles; however, clinical physiology can be muddied in terms of how dependent and independent variables are discussed. A simplified geometrical model was presented to clarify the mechanisms of blood flow at equilibrium founded on Guyton&#x2019;s model of the circulation; this focuses the clinician on how interventions in the ICU (e.g., prone position) might affect hemodynamics. Recent mechanistic investigations into the circulatory consequences of prone position have been reported. These findings were incorporated into the simplified geometrical model with emphasis on the link between cardiac and respiratory physiologies. The pericardial pressure is one nexus binding the heart and the lungs; so too are changes in cardiac function from pulmonary vascular recruitment. Measuring &#x2018;preload responsiveness&#x2019; locates the system&#x2019;s operating point; this helps predict the hemodynamic response to any intervention in the ICU, including the decision to prone a patient with ARDS.</p>
</sec>
</body>
<back>
<sec sec-type="data-availability" id="s4">
<title>Data availability statement</title>
<p>The original contributions presented in the study are included in the article/supplementary material, further inquiries can be directed to the corresponding author.</p>
</sec>
<sec id="s5">
<title>Author contributions</title>
<p>The author confirms being the sole contributor of this work and has approved it for publication.</p>
</sec>
<ack>
<p>Pietro Verrecchia for review of <xref ref-type="fig" rid="F3">Figures 3</xref> and <xref ref-type="fig" rid="F4">4</xref>.</p>
</ack>
<sec sec-type="COI-statement" id="s6">
<title>Conflict of interest</title>
<p>J-ESK is the cofounder and Chief Medical Officer of Flosonics Medical.</p>
</sec>
<sec sec-type="disclaimer" id="s7">
<title>Publisher&#x2019;s note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
<ref-list>
<title>References</title>
<ref id="B1">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Beard</surname>
<given-names>D. A.</given-names>
</name>
<name>
<surname>Feigl</surname>
<given-names>E. O.</given-names>
</name>
</person-group> (<year>2011</year>). <article-title>Understanding Guyton&#x27;s venous return curves</article-title>. <source>Am. J. Physiol. Heart Circ. Physiol.</source> <volume>301</volume> (<issue>3</issue>), <fpage>H629</fpage>&#x2013;<lpage>H633</lpage>. <pub-id pub-id-type="doi">10.1152/ajpheart.00228.2011</pub-id>
</citation>
</ref>
<ref id="B2">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Berger</surname>
<given-names>D.</given-names>
</name>
<name>
<surname>Moller</surname>
<given-names>P. W.</given-names>
</name>
<name>
<surname>Takala</surname>
<given-names>J.</given-names>
</name>
</person-group> (<year>2019</year>). <article-title>Reply to "Is the Guytonian framework justified in explaining heart lung interactions?" and "Venous return, mean systemic pressure and getting the right answer for the wrong reason</article-title>. <source>Ann. Transl. Med.</source> <volume>7</volume> (<issue>8</issue>), <fpage>186</fpage>. <pub-id pub-id-type="doi">10.21037/atm.2019.04.50</pub-id>
</citation>
</ref>
<ref id="B3">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Berger</surname>
<given-names>D.</given-names>
</name>
<name>
<surname>Moller</surname>
<given-names>P. W.</given-names>
</name>
<name>
<surname>Weber</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Bloch</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Bloechlinger</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Haenggi</surname>
<given-names>M.</given-names>
</name>
<etal/>
</person-group> (<year>2016</year>). <article-title>Effect of PEEP, blood volume, and inspiratory hold maneuvers on venous return</article-title>. <source>Am. J. physiology-heart circulatory physiology</source> <volume>311</volume> (<issue>3</issue>), <fpage>H794</fpage>&#x2013;<lpage>H806</lpage>. <pub-id pub-id-type="doi">10.1152/ajpheart.00931.2015</pub-id>
</citation>
</ref>
<ref id="B4">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Berger</surname>
<given-names>D.</given-names>
</name>
<name>
<surname>Takala</surname>
<given-names>J.</given-names>
</name>
</person-group> (<year>2018</year>). <article-title>Determinants of systemic venous return and the impact of positive pressure ventilation</article-title>. <source>Ann. Transl. Med.</source> <volume>6</volume> (<issue>18</issue>), <fpage>350</fpage>. <pub-id pub-id-type="doi">10.21037/atm.2018.05.27</pub-id>
</citation>
</ref>
<ref id="B5">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Berlin</surname>
<given-names>D. A.</given-names>
</name>
<name>
<surname>Bakker</surname>
<given-names>J.</given-names>
</name>
</person-group> (<year>2015</year>). <article-title>Starling curves and central venous pressure</article-title>. <source>Crit. Care</source> <volume>19</volume> (<issue>1</issue>), <fpage>55</fpage>. <pub-id pub-id-type="doi">10.1186/s13054-015-0776-1</pub-id>
</citation>
</ref>
<ref id="B6">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Bodson</surname>
<given-names>L.</given-names>
</name>
<name>
<surname>Vieillard-Baron</surname>
<given-names>A.</given-names>
</name>
</person-group> (<year>2012</year>). <article-title>Respiratory variation in inferior vena cava diameter: Surrogate of central venous pressure or parameter of fluid responsiveness? Let the physiology reply</article-title>. <source>Crit. Care</source> <volume>16</volume> (<issue>6</issue>), <fpage>181</fpage>. <pub-id pub-id-type="doi">10.1186/cc11824</pub-id>
</citation>
</ref>
<ref id="B7">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Boesing</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Graf</surname>
<given-names>P. T.</given-names>
</name>
<name>
<surname>Schmitt</surname>
<given-names>F.</given-names>
</name>
<name>
<surname>Thiel</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Pelosi</surname>
<given-names>P.</given-names>
</name>
<name>
<surname>Rocco</surname>
<given-names>P. R. M.</given-names>
</name>
<etal/>
</person-group> (<year>2022</year>). <article-title>Effects of different positive end-expiratory pressure titration strategies during prone positioning in patients with acute respiratory distress syndrome: A prospective interventional study</article-title>. <source>Crit. Care</source> <volume>26</volume> (<issue>1</issue>), <fpage>82</fpage>. <pub-id pub-id-type="doi">10.1186/s13054-022-03956-8</pub-id>
</citation>
</ref>
<ref id="B8">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Bone</surname>
<given-names>R. C.</given-names>
</name>
</person-group> (<year>1993</year>). <article-title>The ARDS lung. New insights from computed tomography</article-title>. <source>Jama</source> <volume>269</volume> (<issue>16</issue>), <fpage>2134</fpage>&#x2013;<lpage>2135</lpage>. <pub-id pub-id-type="doi">10.1001/jama.269.16.2134</pub-id>
</citation>
</ref>
<ref id="B9">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Brengelmann</surname>
<given-names>G. L.</given-names>
</name>
</person-group> (<year>2003</year>). <article-title>A critical analysis of the view that right atrial pressure determines venous return</article-title>. <source>J. Appl. Physiol. (1985)</source> <volume>94</volume> (<issue>3</issue>), <fpage>849</fpage>&#x2013;<lpage>859</lpage>. <pub-id pub-id-type="doi">10.1152/japplphysiol.00868.2002</pub-id>
</citation>
</ref>
<ref id="B10">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Brengelmann</surname>
<given-names>G. L.</given-names>
</name>
</person-group> (<year>2019</year>). <article-title>Venous return and the physical connection between distribution of segmental pressures and volumes</article-title>. <source>Am. J. Physiol. Heart Circ. Physiol.</source> <volume>317</volume> (<issue>5</issue>), <fpage>H939</fpage>&#x2013;<lpage>h953</lpage>. <pub-id pub-id-type="doi">10.1152/ajpheart.00381.2019</pub-id>
</citation>
</ref>
<ref id="B11">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Bressack</surname>
<given-names>M. A.</given-names>
</name>
<name>
<surname>Raffin</surname>
<given-names>T. A.</given-names>
</name>
</person-group> (<year>1987</year>). <article-title>Importance of venous return, venous resistance, and mean circulatory pressure in the physiology and management of shock</article-title>. <source>Chest</source> <volume>92</volume> (<issue>5</issue>), <fpage>906</fpage>&#x2013;<lpage>912</lpage>. <pub-id pub-id-type="doi">10.1378/chest.92.5.906</pub-id>
</citation>
</ref>
<ref id="B12">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Brienza</surname>
<given-names>N.</given-names>
</name>
<name>
<surname>Ayuse</surname>
<given-names>T.</given-names>
</name>
<name>
<surname>O&#x27;Donnell</surname>
<given-names>C. P.</given-names>
</name>
<name>
<surname>Permutt</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Robotham</surname>
<given-names>J. L.</given-names>
</name>
</person-group> (<year>1995</year>). <article-title>Regional control of venous return: Liver blood flow</article-title>. <source>Am. J. Respir. Crit. care Med.</source> <volume>152</volume> (<issue>2</issue>), <fpage>511</fpage>&#x2013;<lpage>518</lpage>. <pub-id pub-id-type="doi">10.1164/ajrccm.152.2.7633700</pub-id>
</citation>
</ref>
<ref id="B13">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Broccard</surname>
<given-names>A. F.</given-names>
</name>
</person-group> (<year>2012</year>). <article-title>Cardiopulmonary interactions and volume status assessment</article-title>. <source>J. Clin. Monit. Comput.</source> <volume>26</volume> (<issue>5</issue>), <fpage>383</fpage>&#x2013;<lpage>391</lpage>. <pub-id pub-id-type="doi">10.1007/s10877-012-9387-4</pub-id>
</citation>
</ref>
<ref id="B14">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Broccard</surname>
<given-names>A. F.</given-names>
</name>
<name>
<surname>Hotchkiss</surname>
<given-names>J. R.</given-names>
</name>
<name>
<surname>Kuwayama</surname>
<given-names>N.</given-names>
</name>
<name>
<surname>Olson</surname>
<given-names>D. A.</given-names>
</name>
<name>
<surname>Jamal</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Wangensteen</surname>
<given-names>D. O.</given-names>
</name>
<etal/>
</person-group> (<year>1998</year>). <article-title>Consequences of vascular flow on lung injury induced by mechanical ventilation</article-title>. <source>Am. J. Respir. Crit. care Med.</source> <volume>157</volume> (<issue>6</issue>), <fpage>1935</fpage>&#x2013;<lpage>1942</lpage>. <pub-id pub-id-type="doi">10.1164/ajrccm.157.6.9612006</pub-id>
</citation>
</ref>
<ref id="B15">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Cabrera</surname>
<given-names>M. R.</given-names>
</name>
<name>
<surname>Nakamura</surname>
<given-names>G. E.</given-names>
</name>
<name>
<surname>Montague</surname>
<given-names>D. A.</given-names>
</name>
<name>
<surname>Cole</surname>
<given-names>R. P.</given-names>
</name>
</person-group> (<year>1989</year>). <article-title>Effect of airway pressure on pericardial pressure</article-title>. <source>Am. Rev. Respir. Dis.</source> <volume>140</volume> (<issue>3</issue>), <fpage>659</fpage>&#x2013;<lpage>667</lpage>. <pub-id pub-id-type="doi">10.1164/ajrccm/140.3.659</pub-id>
</citation>
</ref>
<ref id="B16">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Caldini</surname>
<given-names>P.</given-names>
</name>
<name>
<surname>Permutt</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Waddell</surname>
<given-names>J. A.</given-names>
</name>
<name>
<surname>Riley</surname>
<given-names>R. L.</given-names>
</name>
</person-group> (<year>1974</year>). <article-title>Effect of epinephrine on pressure, flow, and volume relationships in the systemic circulation of dogs</article-title>. <source>Circulation Res.</source> <volume>34</volume> (<issue>5</issue>), <fpage>606</fpage>&#x2013;<lpage>623</lpage>. <pub-id pub-id-type="doi">10.1161/01.res.34.5.606</pub-id>
</citation>
</ref>
<ref id="B17">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Chiumello</surname>
<given-names>D.</given-names>
</name>
<name>
<surname>Cressoni</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Racagni</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Landi</surname>
<given-names>L.</given-names>
</name>
<name>
<surname>Li Bassi</surname>
<given-names>G.</given-names>
</name>
<name>
<surname>Polli</surname>
<given-names>F.</given-names>
</name>
<etal/>
</person-group> (<year>2006</year>). <article-title>Effects of thoraco-pelvic supports during prone position in patients with acute lung injury/acute respiratory distress syndrome: A physiological study</article-title>. <source>Crit. Care</source> <volume>10</volume> (<issue>3</issue>), <fpage>R87</fpage>. <pub-id pub-id-type="doi">10.1186/cc4933</pub-id>
</citation>
</ref>
<ref id="B18">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Cressoni</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Cadringher</surname>
<given-names>P.</given-names>
</name>
<name>
<surname>Chiurazzi</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Amini</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Gallazzi</surname>
<given-names>E.</given-names>
</name>
<name>
<surname>Marino</surname>
<given-names>A.</given-names>
</name>
<etal/>
</person-group> (<year>2014</year>). <article-title>Lung inhomogeneity in patients with acute respiratory distress syndrome</article-title>. <source>Am. J. Respir. Crit. care Med.</source> <volume>189</volume> (<issue>2</issue>), <fpage>149</fpage>&#x2013;<lpage>158</lpage>. <pub-id pub-id-type="doi">10.1164/rccm.201308-1567OC</pub-id>
</citation>
</ref>
<ref id="B19">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Cressoni</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Chiurazzi</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Gotti</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Amini</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Brioni</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Algieri</surname>
<given-names>I.</given-names>
</name>
<etal/>
</person-group> (<year>2015</year>). <article-title>Lung inhomogeneities and time course of ventilator-induced mechanical injuries</article-title>. <source>Anesthesiology</source> <volume>123</volume> (<issue>3</issue>), <fpage>618</fpage>&#x2013;<lpage>627</lpage>. <pub-id pub-id-type="doi">10.1097/ALN.0000000000000727</pub-id>
</citation>
</ref>
<ref id="B20">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Decramer</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>De Troyer</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Kelly</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Zocchi</surname>
<given-names>L.</given-names>
</name>
<name>
<surname>Macklem</surname>
<given-names>P. T.</given-names>
</name>
</person-group> (<year>1984</year>). <article-title>Regional differences in abdominal pressure swings in dogs</article-title>. <source>J. Appl. Physiol. Respir. Environ. Exerc Physiol.</source> <volume>57</volume> (<issue>6</issue>), <fpage>1682</fpage>&#x2013;<lpage>1687</lpage>. <pub-id pub-id-type="doi">10.1152/jappl.1984.57.6.1682</pub-id>
</citation>
</ref>
<ref id="B21">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Edgcombe</surname>
<given-names>H.</given-names>
</name>
<name>
<surname>Carter</surname>
<given-names>K.</given-names>
</name>
<name>
<surname>Yarrow</surname>
<given-names>S.</given-names>
</name>
</person-group> (<year>2008</year>). <article-title>Anaesthesia in the prone position</article-title>. <source>Br. J. Anaesth.</source> <volume>100</volume> (<issue>2</issue>), <fpage>165</fpage>&#x2013;<lpage>183</lpage>. <pub-id pub-id-type="doi">10.1093/bja/aem380</pub-id>
</citation>
</ref>
<ref id="B22">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Feihl</surname>
<given-names>F.</given-names>
</name>
<name>
<surname>Broccard</surname>
<given-names>A. F.</given-names>
</name>
</person-group> (<year>2009a</year>). <article-title>Interactions between respiration and systemic hemodynamics. Part I: Basic concepts</article-title>. <source>Intensive Care Med.</source> <volume>35</volume> (<issue>1</issue>), <fpage>45</fpage>&#x2013;<lpage>54</lpage>. <pub-id pub-id-type="doi">10.1007/s00134-008-1297-z</pub-id>
</citation>
</ref>
<ref id="B23">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Feihl</surname>
<given-names>F.</given-names>
</name>
<name>
<surname>Broccard</surname>
<given-names>A. F.</given-names>
</name>
</person-group> (<year>2009b</year>). <article-title>Interactions between respiration and systemic hemodynamics. Part II: Practical implications in critical care</article-title>. <source>Intensive Care Med.</source> <volume>35</volume> (<issue>2</issue>), <fpage>198</fpage>&#x2013;<lpage>205</lpage>. <pub-id pub-id-type="doi">10.1007/s00134-008-1298-y</pub-id>
</citation>
</ref>
<ref id="B24">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Fessler</surname>
<given-names>H. E.</given-names>
</name>
<name>
<surname>Brower</surname>
<given-names>R. G.</given-names>
</name>
<name>
<surname>Wise</surname>
<given-names>R. A.</given-names>
</name>
<name>
<surname>Permutt</surname>
<given-names>S.</given-names>
</name>
</person-group> (<year>1992</year>). <article-title>Effects of positive end-expiratory pressure on the canine venous return curve</article-title>. <source>Am. Rev. Respir. Dis.</source> <volume>146</volume> (<issue>1</issue>), <fpage>4</fpage>&#x2013;<lpage>10</lpage>. <pub-id pub-id-type="doi">10.1164/ajrccm/146.1.4</pub-id>
</citation>
</ref>
<ref id="B25">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Fessler</surname>
<given-names>H. E.</given-names>
</name>
</person-group> (<year>1995</year>). <article-title>Effects of CPAP on venous return</article-title>. <source>J. Sleep. Res.</source> <volume>4</volume> (<issue>S1</issue>), <fpage>44</fpage>&#x2013;<lpage>49</lpage>. <pub-id pub-id-type="doi">10.1111/j.1365-2869.1995.tb00185.x</pub-id>
</citation>
</ref>
<ref id="B26">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Fessler</surname>
<given-names>H. E.</given-names>
</name>
</person-group> (<year>1997</year>). <article-title>Heart-lung interactions: Applications in the critically ill</article-title>. <source>Eur. Respir. J.</source> <volume>10</volume> (<issue>1</issue>), <fpage>226</fpage>&#x2013;<lpage>237</lpage>. <pub-id pub-id-type="doi">10.1183/09031936.97.10010226</pub-id>
</citation>
</ref>
<ref id="B27">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Gattinoni</surname>
<given-names>L.</given-names>
</name>
<name>
<surname>Chiumello</surname>
<given-names>D.</given-names>
</name>
<name>
<surname>Carlesso</surname>
<given-names>E.</given-names>
</name>
<name>
<surname>Valenza</surname>
<given-names>F.</given-names>
</name>
</person-group> (<year>2004</year>). <article-title>Bench-to-bedside review: Chest wall elastance in acute lung injury/acute respiratory distress syndrome patients</article-title>. <source>Crit. Care</source> <volume>8</volume> (<issue>5</issue>), <fpage>350</fpage>&#x2013;<lpage>355</lpage>. <pub-id pub-id-type="doi">10.1186/cc2854</pub-id>
</citation>
</ref>
<ref id="B28">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Gattinoni</surname>
<given-names>L.</given-names>
</name>
<name>
<surname>Quintel</surname>
<given-names>M.</given-names>
</name>
</person-group> (<year>2016</year>). <article-title>How ARDS should be treated</article-title>. <source>Crit. Care</source> <volume>20</volume>, <fpage>86</fpage>. <pub-id pub-id-type="doi">10.1186/s13054-016-1268-7</pub-id>
</citation>
</ref>
<ref id="B29">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Gattinoni</surname>
<given-names>L.</given-names>
</name>
<name>
<surname>Taccone</surname>
<given-names>P.</given-names>
</name>
<name>
<surname>Carlesso</surname>
<given-names>E.</given-names>
</name>
<name>
<surname>Marini</surname>
<given-names>J. J.</given-names>
</name>
</person-group> (<year>2013</year>). <article-title>Prone position in acute respiratory distress syndrome. Rationale, indications, and limits</article-title>. <source>Am. J. Respir. Crit. care Med.</source> <volume>188</volume> (<issue>11</issue>), <fpage>1286</fpage>&#x2013;<lpage>1293</lpage>. <pub-id pub-id-type="doi">10.1164/rccm.201308-1532CI</pub-id>
</citation>
</ref>
<ref id="B30">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Gelman</surname>
<given-names>S.</given-names>
</name>
</person-group> (<year>2008</year>). <article-title>Venous function and central venous pressure: A physiologic story</article-title>. <source>Anesthesiology</source> <volume>108</volume> (<issue>4</issue>), <fpage>735</fpage>&#x2013;<lpage>748</lpage>. <pub-id pub-id-type="doi">10.1097/ALN.0b013e3181672607</pub-id>
</citation>
</ref>
<ref id="B31">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Green</surname>
<given-names>J. F.</given-names>
</name>
</person-group> (<year>1977</year>). <article-title>Mechanism of action of isoproterenol on venous return</article-title>. <source>Am. J. Physiol.</source> <volume>232</volume> (<issue>2</issue>), <fpage>H152</fpage>&#x2013;<lpage>H156</lpage>. <pub-id pub-id-type="doi">10.1152/ajpheart.1977.232.2.H152</pub-id>
</citation>
</ref>
<ref id="B32">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Gu&#xe9;rin</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Albert</surname>
<given-names>R. K.</given-names>
</name>
<name>
<surname>Beitler</surname>
<given-names>J.</given-names>
</name>
<name>
<surname>Gattinoni</surname>
<given-names>L.</given-names>
</name>
<name>
<surname>Jaber</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Marini</surname>
<given-names>J. J.</given-names>
</name>
<etal/>
</person-group> (<year>2020</year>). <article-title>Prone position in ARDS patients: Why, when, how and for whom</article-title>. <source>Intensive Care Med.</source> <volume>46</volume> (<issue>12</issue>), <fpage>2385</fpage>&#x2013;<lpage>2396</lpage>. <pub-id pub-id-type="doi">10.1007/s00134-020-06306-w</pub-id>
</citation>
</ref>
<ref id="B33">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Gu&#xe9;rin</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Matthay</surname>
<given-names>M. A.</given-names>
</name>
</person-group> (<year>2016</year>). <article-title>Acute cor pulmonale and the acute respiratory distress syndrome</article-title>. <source>Intensive Care Med.</source> <volume>42</volume> (<issue>5</issue>), <fpage>934</fpage>&#x2013;<lpage>936</lpage>. <pub-id pub-id-type="doi">10.1007/s00134-015-4197-z</pub-id>
</citation>
</ref>
<ref id="B34">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Gu&#xe9;rin</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Reignier</surname>
<given-names>J.</given-names>
</name>
<name>
<surname>Richard</surname>
<given-names>J. C.</given-names>
</name>
<name>
<surname>Beuret</surname>
<given-names>P.</given-names>
</name>
<name>
<surname>Gacouin</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Boulain</surname>
<given-names>T.</given-names>
</name>
<etal/>
</person-group> (<year>2013</year>). <article-title>Prone positioning in severe acute respiratory distress syndrome</article-title>. <source>N. Engl. J. Med.</source> <volume>368</volume> (<issue>23</issue>), <fpage>2159</fpage>&#x2013;<lpage>2168</lpage>. <pub-id pub-id-type="doi">10.1056/NEJMoa1214103</pub-id>
</citation>
</ref>
<ref id="B35">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Guyton</surname>
<given-names>A. C.</given-names>
</name>
</person-group> (<year>1955</year>). <article-title>Determination of cardiac output by equating venous return curves with cardiac response curves</article-title>. <source>Physiol. Rev.</source> <volume>35</volume> (<issue>1</issue>), <fpage>123</fpage>&#x2013;<lpage>129</lpage>. <pub-id pub-id-type="doi">10.1152/physrev.1955.35.1.123</pub-id>
</citation>
</ref>
<ref id="B36">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Guyton</surname>
<given-names>A. C.</given-names>
</name>
<name>
<surname>Lindsey</surname>
<given-names>A. W.</given-names>
</name>
<name>
<surname>Abernathy</surname>
<given-names>B.</given-names>
</name>
<name>
<surname>Richardson</surname>
<given-names>T.</given-names>
</name>
</person-group> (<year>1957</year>). <article-title>Venous return at various right atrial pressures and the normal venous return curve</article-title>. <source>Am. J. Physiol.</source> <volume>189</volume> (<issue>3</issue>), <fpage>609</fpage>&#x2013;<lpage>615</lpage>. <pub-id pub-id-type="doi">10.1152/ajplegacy.1957.189.3.609</pub-id>
</citation>
</ref>
<ref id="B37">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Guyton</surname>
<given-names>A. C.</given-names>
</name>
<name>
<surname>Lindsey</surname>
<given-names>A. W.</given-names>
</name>
<name>
<surname>Kaufmann</surname>
<given-names>B. N.</given-names>
</name>
</person-group> (<year>1955</year>). <article-title>Effect of mean circulatory filling pressure and other peripheral circulatory factors on cardiac output</article-title>. <source>Am. J. Physiol.</source> <volume>180</volume> (<issue>3</issue>), <fpage>463</fpage>&#x2013;<lpage>468</lpage>. <pub-id pub-id-type="doi">10.1152/ajplegacy.1955.180.3.463</pub-id>
</citation>
</ref>
<ref id="B38">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Hamilton</surname>
<given-names>D. R.</given-names>
</name>
<name>
<surname>Dani</surname>
<given-names>R. S.</given-names>
</name>
<name>
<surname>Semlacher</surname>
<given-names>R. A.</given-names>
</name>
<name>
<surname>Smith</surname>
<given-names>E. R.</given-names>
</name>
<name>
<surname>Kieser</surname>
<given-names>T. M.</given-names>
</name>
<name>
<surname>Tyberg</surname>
<given-names>J. V.</given-names>
</name>
</person-group> (<year>1994</year>). <article-title>Right atrial and right ventricular transmural pressures in dogs and humans. Effects of the pericardium</article-title>. <source>Circulation</source> <volume>90</volume> (<issue>5</issue>), <fpage>2492</fpage>&#x2013;<lpage>2500</lpage>. <pub-id pub-id-type="doi">10.1161/01.cir.90.5.2492</pub-id>
</citation>
</ref>
<ref id="B39">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Henderson</surname>
<given-names>A. C.</given-names>
</name>
<name>
<surname>S&#xe1;</surname>
<given-names>R. C.</given-names>
</name>
<name>
<surname>Theilmann</surname>
<given-names>R. J.</given-names>
</name>
<name>
<surname>Buxton</surname>
<given-names>R. B.</given-names>
</name>
<name>
<surname>Prisk</surname>
<given-names>G. K.</given-names>
</name>
<name>
<surname>Hopkins</surname>
<given-names>S. R.</given-names>
</name>
</person-group> (<year>2013</year>). <article-title>The gravitational distribution of ventilation-perfusion ratio is more uniform in prone than supine posture in the normal human lung</article-title>. <source>J. Appl. Physiol. (1985)</source> <volume>115</volume> (<issue>3</issue>), <fpage>313</fpage>&#x2013;<lpage>324</lpage>. <pub-id pub-id-type="doi">10.1152/japplphysiol.01531.2012</pub-id>
</citation>
</ref>
<ref id="B40">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Hering</surname>
<given-names>R.</given-names>
</name>
<name>
<surname>Vorwerk</surname>
<given-names>R.</given-names>
</name>
<name>
<surname>Wrigge</surname>
<given-names>H.</given-names>
</name>
<name>
<surname>Zinserling</surname>
<given-names>J.</given-names>
</name>
<name>
<surname>Schr&#xf6;der</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>von Spiegel</surname>
<given-names>T.</given-names>
</name>
<etal/>
</person-group> (<year>2002</year>). <article-title>Prone positioning, systemic hemodynamics, hepatic indocyanine green kinetics, and gastric intramucosal energy balance in patients with acute lung injury</article-title>. <source>Intensive Care Med.</source> <volume>28</volume> (<issue>1</issue>), <fpage>53</fpage>&#x2013;<lpage>58</lpage>. <pub-id pub-id-type="doi">10.1007/s00134-001-1166-5</pub-id>
</citation>
</ref>
<ref id="B41">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Hering</surname>
<given-names>R.</given-names>
</name>
<name>
<surname>Wrigge</surname>
<given-names>H.</given-names>
</name>
<name>
<surname>Vorwerk</surname>
<given-names>R.</given-names>
</name>
<name>
<surname>Brensing</surname>
<given-names>K. A.</given-names>
</name>
<name>
<surname>Schr&#xf6;der</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Zinserling</surname>
<given-names>J.</given-names>
</name>
<etal/>
</person-group> (<year>2001</year>). <article-title>The effects of prone positioning on intraabdominal pressure and cardiovascular and renal function in patients with acute lung injury</article-title>. <source>Anesth. analgesia</source> <volume>92</volume> (<issue>5</issue>), <fpage>1226</fpage>&#x2013;<lpage>1231</lpage>. <pub-id pub-id-type="doi">10.1097/00000539-200105000-00027</pub-id>
</citation>
</ref>
<ref id="B42">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Huberfeld</surname>
<given-names>S. I.</given-names>
</name>
<name>
<surname>Genovese</surname>
<given-names>J.</given-names>
</name>
<name>
<surname>Tarasiuk</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Scharf</surname>
<given-names>S. M.</given-names>
</name>
</person-group> (<year>1995</year>). <article-title>Effect of CPAP on pericardial pressure and respiratory system mechanics in pigs</article-title>. <source>Am. J. Respir. Crit. care Med.</source> <volume>152</volume> (<issue>1</issue>), <fpage>142</fpage>&#x2013;<lpage>147</lpage>. <pub-id pub-id-type="doi">10.1164/ajrccm.152.1.7599813</pub-id>
</citation>
</ref>
<ref id="B43">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Jacobsohn</surname>
<given-names>E.</given-names>
</name>
<name>
<surname>Chorn</surname>
<given-names>R.</given-names>
</name>
<name>
<surname>O&#x27;Connor</surname>
<given-names>M.</given-names>
</name>
</person-group> (<year>1997</year>). <article-title>The role of the vasculature in regulating venous return and cardiac output: Historical and graphical approach</article-title>. <source>Can. J. Anaesth.</source> <volume>44</volume> (<issue>8</issue>), <fpage>849</fpage>&#x2013;<lpage>867</lpage>. <pub-id pub-id-type="doi">10.1007/BF03013162</pub-id>
</citation>
</ref>
<ref id="B44">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Jardin</surname>
<given-names>F.</given-names>
</name>
<name>
<surname>Vieillard-Baron</surname>
<given-names>A.</given-names>
</name>
</person-group> (<year>2003</year>). <article-title>Right ventricular function and positive pressure ventilation in clinical practice: From hemodynamic subsets to respirator settings</article-title>. <source>Intensive Care Med.</source> <volume>29</volume> (<issue>9</issue>), <fpage>1426</fpage>&#x2013;<lpage>1434</lpage>. <pub-id pub-id-type="doi">10.1007/s00134-003-1873-1</pub-id>
</citation>
</ref>
<ref id="B45">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Jellinek</surname>
<given-names>H.</given-names>
</name>
<name>
<surname>Krenn</surname>
<given-names>H.</given-names>
</name>
<name>
<surname>Oczenski</surname>
<given-names>W.</given-names>
</name>
<name>
<surname>Veit</surname>
<given-names>F.</given-names>
</name>
<name>
<surname>Schwarz</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Fitzgerald</surname>
<given-names>R. D.</given-names>
</name>
</person-group> (<year>2000</year>). <article-title>Influence of positive airway pressure on the pressure gradient for venous return in humans</article-title>. <source>J. Appl. Physiol. (1985)</source> <volume>88</volume> (<issue>3</issue>), <fpage>926</fpage>&#x2013;<lpage>932</lpage>. <pub-id pub-id-type="doi">10.1152/jappl.2000.88.3.926</pub-id>
</citation>
</ref>
<ref id="B46">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Jozwiak</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Teboul</surname>
<given-names>J. L.</given-names>
</name>
<name>
<surname>Anguel</surname>
<given-names>N.</given-names>
</name>
<name>
<surname>Persichini</surname>
<given-names>R.</given-names>
</name>
<name>
<surname>Silva</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Chemla</surname>
<given-names>D.</given-names>
</name>
<etal/>
</person-group> (<year>2013</year>). <article-title>Beneficial hemodynamic effects of prone positioning in patients with acute respiratory distress syndrome</article-title>. <source>Am. J. Respir. Crit. care Med.</source> <volume>188</volume> (<issue>12</issue>), <fpage>1428</fpage>&#x2013;<lpage>1433</lpage>. <pub-id pub-id-type="doi">10.1164/rccm.201303-0593OC</pub-id>
</citation>
</ref>
<ref id="B47">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Kenny</surname>
<given-names>J. S.</given-names>
</name>
</person-group> (<year>2021</year>). <article-title>Letter to the editor: The venous circulation actively alters flow: A brief evolutionary perspective</article-title>. <source>Am. J. Physiol. Heart Circ. Physiol.</source> <volume>320</volume> (<issue>1</issue>), <fpage>H469</fpage>&#x2013;<lpage>h470</lpage>. <pub-id pub-id-type="doi">10.1152/ajpheart.00862.2020</pub-id>
</citation>
</ref>
<ref id="B48">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Lai</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Adda</surname>
<given-names>I.</given-names>
</name>
<name>
<surname>Teboul</surname>
<given-names>J. L.</given-names>
</name>
<name>
<surname>Persichini</surname>
<given-names>R.</given-names>
</name>
<name>
<surname>Gavelli</surname>
<given-names>F.</given-names>
</name>
<name>
<surname>Gu&#xe9;rin</surname>
<given-names>L.</given-names>
</name>
<etal/>
</person-group> (<year>2021</year>). <article-title>Effects of prone positioning on venous return in patients with acute respiratory distress syndrome</article-title>. <source>Crit. Care Med.</source> <volume>49</volume> (<issue>5</issue>), <fpage>781</fpage>&#x2013;<lpage>789</lpage>. <pub-id pub-id-type="doi">10.1097/CCM.0000000000004849</pub-id>
</citation>
</ref>
<ref id="B49">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Lai</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Monnet</surname>
<given-names>X.</given-names>
</name>
<name>
<surname>Teboul</surname>
<given-names>J. L.</given-names>
</name>
</person-group> (<year>2023</year>). <article-title>Hemodynamic implications of prone positioning in patients with ARDS</article-title>. <source>Crit. Care</source> <volume>27</volume> (<issue>1</issue>), <fpage>98</fpage>. <pub-id pub-id-type="doi">10.1186/s13054-023-04369-x</pub-id>
</citation>
</ref>
<ref id="B50">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Lansdorp</surname>
<given-names>B.</given-names>
</name>
<name>
<surname>Hofhuizen</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>van Lavieren</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>van Swieten</surname>
<given-names>H.</given-names>
</name>
<name>
<surname>Lemson</surname>
<given-names>J.</given-names>
</name>
<name>
<surname>van Putten</surname>
<given-names>M. J.</given-names>
</name>
<etal/>
</person-group> (<year>2014</year>). <article-title>Mechanical ventilation-induced intrathoracic pressure distribution and heart-lung interactions&#x2a;</article-title>. <source>Crit. Care Med.</source> <volume>42</volume> (<issue>9</issue>), <fpage>1983</fpage>&#x2013;<lpage>1990</lpage>. <pub-id pub-id-type="doi">10.1097/CCM.0000000000000345</pub-id>
</citation>
</ref>
<ref id="B51">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Maas</surname>
<given-names>J. J.</given-names>
</name>
<name>
<surname>Geerts</surname>
<given-names>B. F.</given-names>
</name>
<name>
<surname>van den Berg</surname>
<given-names>P. C.</given-names>
</name>
<name>
<surname>Pinsky</surname>
<given-names>M. R.</given-names>
</name>
<name>
<surname>Jansen</surname>
<given-names>J. R.</given-names>
</name>
</person-group> (<year>2009</year>). <article-title>Assessment of venous return curve and mean systemic filling pressure in postoperative cardiac surgery patients</article-title>. <source>Crit. Care Med.</source> <volume>37</volume> (<issue>3</issue>), <fpage>912</fpage>&#x2013;<lpage>918</lpage>. <pub-id pub-id-type="doi">10.1097/CCM.0b013e3181961481</pub-id>
</citation>
</ref>
<ref id="B52">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Maas</surname>
<given-names>J. J.</given-names>
</name>
<name>
<surname>Pinsky</surname>
<given-names>M. R.</given-names>
</name>
<name>
<surname>Geerts</surname>
<given-names>B. F.</given-names>
</name>
<name>
<surname>de Wilde</surname>
<given-names>R. B.</given-names>
</name>
<name>
<surname>Jansen</surname>
<given-names>J. R.</given-names>
</name>
</person-group> (<year>2012</year>). <article-title>Estimation of mean systemic filling pressure in postoperative cardiac surgery patients with three methods</article-title>. <source>Intensive Care Med.</source> <volume>38</volume> (<issue>9</issue>), <fpage>1452</fpage>&#x2013;<lpage>1460</lpage>. <pub-id pub-id-type="doi">10.1007/s00134-012-2586-0</pub-id>
</citation>
</ref>
<ref id="B53">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Magder</surname>
<given-names>S.</given-names>
</name>
</person-group> (<year>2012</year>). <article-title>Bench-to-bedside review: An approach to hemodynamic monitoring--Guyton at the bedside</article-title>. <source>Crit. Care</source> <volume>16</volume> (<issue>5</issue>), <fpage>236</fpage>. <pub-id pub-id-type="doi">10.1186/cc11395</pub-id>
</citation>
</ref>
<ref id="B54">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Magder</surname>
<given-names>S.</given-names>
</name>
</person-group> (<year>2004</year>). <article-title>Clinical usefulness of respiratory variations in arterial pressure</article-title>. <source>Am. J. Respir. Crit. care Med.</source> <volume>169</volume> (<issue>2</issue>), <fpage>151</fpage>&#x2013;<lpage>155</lpage>. <pub-id pub-id-type="doi">10.1164/rccm.200211-1360CC</pub-id>
</citation>
</ref>
<ref id="B55">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Magder</surname>
<given-names>S.</given-names>
</name>
</person-group> (<year>2016</year>). <article-title>Volume and its relationship to cardiac output and venous return</article-title>. <source>Crit. Care</source> <volume>20</volume> (<issue>1</issue>), <fpage>271</fpage>. <pub-id pub-id-type="doi">10.1186/s13054-016-1438-7</pub-id>
</citation>
</ref>
<ref id="B56">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Marini</surname>
<given-names>J. J.</given-names>
</name>
<name>
<surname>Culver</surname>
<given-names>B. H.</given-names>
</name>
<name>
<surname>Butler</surname>
<given-names>J.</given-names>
</name>
</person-group> (<year>1981</year>). <article-title>Effect of positive end-expiratory pressure on canine ventricular function curves</article-title>. <source>J. Appl. Physiol. Respir. Environ. Exerc Physiol.</source> <volume>51</volume> (<issue>6</issue>), <fpage>1367</fpage>&#x2013;<lpage>1374</lpage>. <pub-id pub-id-type="doi">10.1152/jappl.1981.51.6.1367</pub-id>
</citation>
</ref>
<ref id="B57">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Marini</surname>
<given-names>J. J.</given-names>
</name>
<name>
<surname>Gattinoni</surname>
<given-names>L.</given-names>
</name>
</person-group> (<year>2021</year>). <article-title>Improving lung compliance by external compression of the chest wall</article-title>. <source>Crit. Care</source> <volume>25</volume> (<issue>1</issue>), <fpage>264</fpage>. <pub-id pub-id-type="doi">10.1186/s13054-021-03700-8</pub-id>
</citation>
</ref>
<ref id="B58">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Marini</surname>
<given-names>J. J.</given-names>
</name>
<name>
<surname>Hotchkiss</surname>
<given-names>J. R.</given-names>
</name>
<name>
<surname>Broccard</surname>
<given-names>A. F.</given-names>
</name>
</person-group> (<year>2003</year>). <article-title>Bench-to-bedside review: Microvascular and airspace linkage in ventilator-induced lung injury</article-title>. <source>Crit. Care</source> <volume>7</volume> (<issue>6</issue>), <fpage>435</fpage>&#x2013;<lpage>444</lpage>. <pub-id pub-id-type="doi">10.1186/cc2392</pub-id>
</citation>
</ref>
<ref id="B59">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Matejovic</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Rokyta</surname>
<given-names>R.</given-names>
<suffix>Jr.</suffix>
</name>
<name>
<surname>Radermacher</surname>
<given-names>P.</given-names>
</name>
<name>
<surname>Krouzecky</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Sramek</surname>
<given-names>V.</given-names>
</name>
<name>
<surname>Novak</surname>
<given-names>I.</given-names>
</name>
</person-group> (<year>2002</year>). <article-title>Effect of prone position on hepato-splanchnic hemodynamics in acute lung injury</article-title>. <source>Intensive Care Med.</source> <volume>28</volume> (<issue>12</issue>), <fpage>1750</fpage>&#x2013;<lpage>1755</lpage>. <pub-id pub-id-type="doi">10.1007/s00134-002-1524-y</pub-id>
</citation>
</ref>
<ref id="B60">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Mead</surname>
<given-names>J.</given-names>
</name>
<name>
<surname>Takishima</surname>
<given-names>T.</given-names>
</name>
<name>
<surname>Leith</surname>
<given-names>D.</given-names>
</name>
</person-group> (<year>1970</year>). <article-title>Stress distribution in lungs: A model of pulmonary elasticity</article-title>. <source>J. Appl. Physiol.</source> <volume>28</volume> (<issue>5</issue>), <fpage>596</fpage>&#x2013;<lpage>608</lpage>. <pub-id pub-id-type="doi">10.1152/jappl.1970.28.5.596</pub-id>
</citation>
</ref>
<ref id="B61">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Mekontso Dessap</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Boissier</surname>
<given-names>F.</given-names>
</name>
<name>
<surname>Charron</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>B&#xe9;got</surname>
<given-names>E.</given-names>
</name>
<name>
<surname>Repess&#xe9;</surname>
<given-names>X.</given-names>
</name>
<name>
<surname>Legras</surname>
<given-names>A.</given-names>
</name>
<etal/>
</person-group> (<year>2016</year>). <article-title>Acute cor pulmonale during protective ventilation for acute respiratory distress syndrome: Prevalence, predictors, and clinical impact</article-title>. <source>Intensive Care Med.</source> <volume>42</volume> (<issue>5</issue>), <fpage>862</fpage>&#x2013;<lpage>870</lpage>. <pub-id pub-id-type="doi">10.1007/s00134-015-4141-2</pub-id>
</citation>
</ref>
<ref id="B62">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Moller</surname>
<given-names>P. W.</given-names>
</name>
<name>
<surname>Berger</surname>
<given-names>D. C.</given-names>
</name>
</person-group> (<year>2023</year>). <article-title>Commentary: Feasibility to estimate mean systemic filling pressure with inspiratory holds at the bedside</article-title>. <source>Front. Physiology</source> <volume>14</volume>, <fpage>1135769</fpage>. <pub-id pub-id-type="doi">10.3389/fphys.2023.1135769</pub-id>
</citation>
</ref>
<ref id="B63">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Moller</surname>
<given-names>P. W.</given-names>
</name>
<name>
<surname>Parkin</surname>
<given-names>W. G.</given-names>
</name>
</person-group> (<year>2022</year>). <article-title>Correct calculation of the mean systemic pressure analogue</article-title>. <source>Intensive Care Med.</source> <volume>48</volume> (<issue>11</issue>), <fpage>1679</fpage>&#x2013;<lpage>1680</lpage>. <pub-id pub-id-type="doi">10.1007/s00134-022-06862-3</pub-id>
</citation>
</ref>
<ref id="B64">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Moller</surname>
<given-names>P. W.</given-names>
</name>
<name>
<surname>Winkler</surname>
<given-names>B.</given-names>
</name>
<name>
<surname>Hurni</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Heinisch</surname>
<given-names>P. P.</given-names>
</name>
<name>
<surname>Bloch</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Sondergaard</surname>
<given-names>S.</given-names>
</name>
<etal/>
</person-group> (<year>2017</year>). <article-title>Right atrial pressure and venous return during cardiopulmonary bypass</article-title>. <source>Am. J. Physiol. Heart Circ. Physiol.</source> <volume>313</volume> (<issue>2</issue>), <fpage>H408</fpage>&#x2013;<lpage>h420</lpage>. <pub-id pub-id-type="doi">10.1152/ajpheart.00081.2017</pub-id>
</citation>
</ref>
<ref id="B65">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Papazian</surname>
<given-names>L.</given-names>
</name>
<name>
<surname>Aubron</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Brochard</surname>
<given-names>L.</given-names>
</name>
<name>
<surname>Chiche</surname>
<given-names>J. D.</given-names>
</name>
<name>
<surname>Combes</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Dreyfuss</surname>
<given-names>D.</given-names>
</name>
<etal/>
</person-group> (<year>2019</year>). <article-title>Formal guidelines: Management of acute respiratory distress syndrome</article-title>. <source>Ann. Intensive Care</source> <volume>9</volume> (<issue>1</issue>), <fpage>69</fpage>. <pub-id pub-id-type="doi">10.1186/s13613-019-0540-9</pub-id>
</citation>
</ref>
<ref id="B66">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Parkin</surname>
<given-names>W. G.</given-names>
</name>
<name>
<surname>Leaning</surname>
<given-names>M. S.</given-names>
</name>
</person-group> (<year>2008</year>). <article-title>Therapeutic control of the circulation</article-title>. <source>J. Clin. Monit. Comput.</source> <volume>22</volume> (<issue>6</issue>), <fpage>391</fpage>&#x2013;<lpage>400</lpage>. <pub-id pub-id-type="doi">10.1007/s10877-008-9147-7</pub-id>
</citation>
</ref>
<ref id="B67">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Pelosi</surname>
<given-names>P.</given-names>
</name>
<name>
<surname>Tubiolo</surname>
<given-names>D.</given-names>
</name>
<name>
<surname>Mascheroni</surname>
<given-names>D.</given-names>
</name>
<name>
<surname>Vicardi</surname>
<given-names>P.</given-names>
</name>
<name>
<surname>Crotti</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Valenza</surname>
<given-names>F.</given-names>
</name>
<etal/>
</person-group> (<year>1998</year>). <article-title>Effects of the prone position on respiratory mechanics and gas exchange during acute lung injury</article-title>. <source>Am. J. Respir. Crit. care Med.</source> <volume>157</volume> (<issue>2</issue>), <fpage>387</fpage>&#x2013;<lpage>393</lpage>. <pub-id pub-id-type="doi">10.1164/ajrccm.157.2.97-04023</pub-id>
</citation>
</ref>
<ref id="B68">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Permutt</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Riley</surname>
<given-names>R. L.</given-names>
</name>
</person-group> (<year>1963</year>). <article-title>Hemodynamics of collapsible vessels with tone: The vascular waterfall</article-title>. <source>J. Appl. Physiol.</source> <volume>18</volume>, <fpage>924</fpage>&#x2013;<lpage>932</lpage>. <pub-id pub-id-type="doi">10.1152/jappl.1963.18.5.924</pub-id>
</citation>
</ref>
<ref id="B69">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Persichini</surname>
<given-names>R.</given-names>
</name>
<name>
<surname>Lai</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Teboul</surname>
<given-names>J. L.</given-names>
</name>
<name>
<surname>Adda</surname>
<given-names>I.</given-names>
</name>
<name>
<surname>Gu&#xe9;rin</surname>
<given-names>L.</given-names>
</name>
<name>
<surname>Monnet</surname>
<given-names>X.</given-names>
</name>
</person-group> (<year>2022</year>). <article-title>Venous return and mean systemic filling pressure: Physiology and clinical applications</article-title>. <source>Crit. Care</source> <volume>26</volume> (<issue>1</issue>), <fpage>150</fpage>. <pub-id pub-id-type="doi">10.1186/s13054-022-04024-x</pub-id>
</citation>
</ref>
<ref id="B70">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Pinsky</surname>
<given-names>M. R.</given-names>
</name>
</person-group> (<year>2021</year>). <article-title>Cardiovascular effects of prone positioning in acute respiratory distress syndrome patients: The circulation does not take it lying down</article-title>. <source>Crit. Care Med.</source> <volume>49</volume> (<issue>5</issue>), <fpage>869</fpage>&#x2013;<lpage>873</lpage>. <pub-id pub-id-type="doi">10.1097/CCM.0000000000004858</pub-id>
</citation>
</ref>
<ref id="B71">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Pinsky</surname>
<given-names>M. R.</given-names>
</name>
</person-group> (<year>1984</year>). <article-title>Instantaneous venous return curves in an intact canine preparation</article-title>. <source>J. Appl. Physiol. Respir. Environ. Exerc Physiol.</source> <volume>56</volume> (<issue>3</issue>), <fpage>765</fpage>&#x2013;<lpage>771</lpage>. <pub-id pub-id-type="doi">10.1152/jappl.1984.56.3.765</pub-id>
</citation>
</ref>
<ref id="B72">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Repess&#xe9;</surname>
<given-names>X.</given-names>
</name>
<name>
<surname>Charron</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Vieillard-Baron</surname>
<given-names>A.</given-names>
</name>
</person-group> (<year>2016</year>). <article-title>Acute respiratory distress syndrome: The heart side of the moon</article-title>. <source>Curr. Opin. Crit. Care</source> <volume>22</volume> (<issue>1</issue>), <fpage>38</fpage>&#x2013;<lpage>44</lpage>. <pub-id pub-id-type="doi">10.1097/MCC.0000000000000267</pub-id>
</citation>
</ref>
<ref id="B73">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Rothe</surname>
<given-names>C. F.</given-names>
</name>
</person-group> (<year>1993</year>). <article-title>Mean circulatory filling pressure: Its meaning and measurement</article-title>. <source>J. Appl. Physiol. (1985)</source> <volume>74</volume> (<issue>2</issue>), <fpage>499</fpage>&#x2013;<lpage>509</lpage>. <pub-id pub-id-type="doi">10.1152/jappl.1993.74.2.499</pub-id>
</citation>
</ref>
<ref id="B74">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Rothe</surname>
<given-names>C. F.</given-names>
</name>
</person-group> (<year>1986</year>). <article-title>Physiology of venous return. An unappreciated boost to the heart</article-title>. <source>Arch. Intern Med.</source> <volume>146</volume> (<issue>5</issue>), <fpage>977</fpage>&#x2013;<lpage>982</lpage>. <pub-id pub-id-type="doi">10.1001/archinte.146.5.977</pub-id>
</citation>
</ref>
<ref id="B75">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Ruste</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Bitker</surname>
<given-names>L.</given-names>
</name>
<name>
<surname>Yonis</surname>
<given-names>H.</given-names>
</name>
<name>
<surname>Riad</surname>
<given-names>Z.</given-names>
</name>
<name>
<surname>Louf-Durier</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Lissonde</surname>
<given-names>F.</given-names>
</name>
<etal/>
</person-group> (<year>2018</year>). <article-title>Hemodynamic effects of extended prone position sessions in ARDS</article-title>. <source>Ann. Intensive Care</source> <volume>8</volume> (<issue>1</issue>), <fpage>120</fpage>. <pub-id pub-id-type="doi">10.1186/s13613-018-0464-9</pub-id>
</citation>
</ref>
<ref id="B76">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Scharf</surname>
<given-names>S. M.</given-names>
</name>
<name>
<surname>Caldini</surname>
<given-names>P.</given-names>
</name>
<name>
<surname>Ingram</surname>
<given-names>R. H.</given-names>
<suffix>Jr.</suffix>
</name>
</person-group> (<year>1977</year>). <article-title>Cardiovascular effects of increasing airway pressure in the dog</article-title>. <source>Am. J. Physiol.</source> <volume>232</volume> (<issue>1</issue>), <fpage>H35</fpage>&#x2013;<lpage>H43</lpage>. <pub-id pub-id-type="doi">10.1152/ajpheart.1977.232.1.H35</pub-id>
</citation>
</ref>
<ref id="B77">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Scharf</surname>
<given-names>S. M.</given-names>
</name>
<name>
<surname>Ingram</surname>
<given-names>R. H.</given-names>
<suffix>Jr.</suffix>
</name>
</person-group> (<year>1977</year>). <article-title>Influence of abdominal pressure and sympathetic vasoconstriction on the cardiovascular response to positive end-expiratory pressure</article-title>. <source>Am. Rev. Respir. Dis.</source> <volume>116</volume> (<issue>4</issue>), <fpage>661</fpage>&#x2013;<lpage>670</lpage>. <pub-id pub-id-type="doi">10.1164/arrd.1977.116.4.661</pub-id>
</citation>
</ref>
<ref id="B78">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Sylvester</surname>
<given-names>J. T.</given-names>
</name>
<name>
<surname>Goldberg</surname>
<given-names>H. S.</given-names>
</name>
<name>
<surname>Permutt</surname>
<given-names>S.</given-names>
</name>
</person-group> (<year>1983</year>). <article-title>The role of the vasculature in the regulation of cardiac output</article-title>. <source>Clin. Chest Med.</source> <volume>4</volume> (<issue>2</issue>), <fpage>333</fpage>&#x2013;<lpage>348</lpage>. <pub-id pub-id-type="doi">10.1016/s0733-8651(18)30629-5</pub-id>
</citation>
</ref>
<ref id="B79">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Takata</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Robotham</surname>
<given-names>J. L.</given-names>
</name>
</person-group> (<year>1992</year>). <article-title>Effects of inspiratory diaphragmatic descent on inferior vena caval venous return</article-title>. <source>J. Appl. Physiol. (1985)</source> <volume>72</volume> (<issue>2</issue>), <fpage>597</fpage>&#x2013;<lpage>607</lpage>. <pub-id pub-id-type="doi">10.1152/jappl.1992.72.2.597</pub-id>
</citation>
</ref>
<ref id="B80">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Takata</surname>
<given-names>M.</given-names>
</name>
<name>
<surname>Wise</surname>
<given-names>R. A.</given-names>
</name>
<name>
<surname>Robotham</surname>
<given-names>J. L.</given-names>
</name>
</person-group> (<year>1990</year>). <article-title>Effects of abdominal pressure on venous return: Abdominal vascular zone conditions</article-title>. <source>J. Appl. Physiol. (1985)</source> <volume>69</volume> (<issue>6</issue>), <fpage>1961</fpage>&#x2013;<lpage>1972</lpage>. <pub-id pub-id-type="doi">10.1152/jappl.1990.69.6.1961</pub-id>
</citation>
</ref>
<ref id="B81">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Tyberg</surname>
<given-names>J. V.</given-names>
</name>
</person-group> (<year>2002</year>). <article-title>How changes in venous capacitance modulate cardiac output</article-title>. <source>Pflugers Arch.</source> <volume>445</volume> (<issue>1</issue>), <fpage>10</fpage>&#x2013;<lpage>17</lpage>. <pub-id pub-id-type="doi">10.1007/s00424-002-0922-x</pub-id>
</citation>
</ref>
<ref id="B82">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Vieillard-Baron</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Charron</surname>
<given-names>C.</given-names>
</name>
<name>
<surname>Caille</surname>
<given-names>V.</given-names>
</name>
<name>
<surname>Belliard</surname>
<given-names>G.</given-names>
</name>
<name>
<surname>Page</surname>
<given-names>B.</given-names>
</name>
<name>
<surname>Jardin</surname>
<given-names>F.</given-names>
</name>
</person-group> (<year>2007</year>). <article-title>Prone positioning unloads the right ventricle in severe ARDS</article-title>. <source>Chest</source> <volume>132</volume> (<issue>5</issue>), <fpage>1440</fpage>&#x2013;<lpage>1446</lpage>. <pub-id pub-id-type="doi">10.1378/chest.07-1013</pub-id>
</citation>
</ref>
<ref id="B83">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Werner-Moller</surname>
<given-names>P.</given-names>
</name>
<name>
<surname>Berger</surname>
<given-names>D.</given-names>
</name>
<name>
<surname>Takala</surname>
<given-names>J.</given-names>
</name>
</person-group> (<year>2020</year>). <article-title>Letter to the Editor: Venous return and the physical connection between distribution of segmental pressures and volumes</article-title>. <source>Am. J. Physiol. Heart Circ. Physiol.</source> <volume>318</volume> (<issue>1</issue>), <fpage>H203</fpage>&#x2013;<lpage>h204</lpage>. <pub-id pub-id-type="doi">10.1152/ajpheart.00698.2019</pub-id>
</citation>
</ref>
<ref id="B84">
<citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname>Werner-Moller</surname>
<given-names>P.</given-names>
</name>
<name>
<surname>Heinisch</surname>
<given-names>P. P.</given-names>
</name>
<name>
<surname>Hana</surname>
<given-names>A.</given-names>
</name>
<name>
<surname>Bachmann</surname>
<given-names>K. F.</given-names>
</name>
<name>
<surname>Sondergaard</surname>
<given-names>S.</given-names>
</name>
<name>
<surname>Jakob</surname>
<given-names>S. M.</given-names>
</name>
<etal/>
</person-group> (<year>2022</year>). <article-title>Experimental validation of a mean systemic pressure analog against zero-flow measurements in porcine VA-ECMO</article-title>. <source>J. Appl. Physiology</source> <volume>132</volume> (<issue>3</issue>), <fpage>726</fpage>&#x2013;<lpage>736</lpage>. <pub-id pub-id-type="doi">10.1152/japplphysiol.00804.2021</pub-id>
</citation>
</ref>
</ref-list>
</back>
</article>