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<article id="iwj14192" xml:lang="en" article-type="research-article" dtd-version="1.4"><?da-xref-anchor-style superscripted?><processing-meta base-tagset="archiving" mathml-version="3.0" table-model="xhtml" tagset-family="jats"><restricted-by>pmc</restricted-by></processing-meta><front><journal-meta><journal-id journal-id-type="nlm-ta">Int Wound J</journal-id><journal-id journal-id-type="iso-abbrev">Int Wound J</journal-id><journal-id journal-id-type="pmc-domain-id">4015</journal-id><journal-id journal-id-type="pmc-domain">iwj</journal-id><journal-id journal-id-type="nlm-id">101230907</journal-id><journal-id journal-id-type="publisher-id">IWJ</journal-id><journal-title-group><journal-title>International Wound Journal</journal-title></journal-title-group><issn pub-type="ppub">1742-4801</issn><issn pub-type="epub">1742-481X</issn><?publisher_abbrev blackwell?><publisher><publisher-name>Wiley</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="pmcid">PMC10502263</article-id><article-id pub-id-type="pmcid-ver">PMC10502263.1</article-id><article-id pub-id-type="pmcaid">10502263</article-id><article-id pub-id-type="pmcaiid">10502263</article-id><article-id pub-id-type="pmid">37073432</article-id><article-id pub-id-type="doi">10.1111/iwj.14192</article-id><article-id pub-id-type="publisher-id">IWJ14192</article-id><article-version article-version-type="pmc-version">1</article-version><article-categories><subj-group subj-group-type="overline"><subject>Original Article</subject></subj-group><subj-group subj-group-type="heading"><subject>Original Articles</subject></subj-group></article-categories><title-group><article-title>The biomechanical efficacy of a hybrid support surface in protecting supine patients from sacral pressure ulcers</article-title><alt-title alt-title-type="left-running-head">Katz and Gefen</alt-title></title-group><contrib-group><contrib id="iwj14192-cr-0001" contrib-type="author"><name name-style="western"><surname>Katz</surname><given-names initials="T">Tomer</given-names></name><xref rid="iwj14192-aff-0001" ref-type="aff">
<sup>1</sup>
</xref></contrib><contrib id="iwj14192-cr-0002" contrib-type="author" corresp="yes"><name name-style="western"><surname>Gefen</surname><given-names initials="A">Amit</given-names></name><contrib-id contrib-id-type="orcid" authenticated="false">https://orcid.org/0000-0002-0223-7218</contrib-id><xref rid="iwj14192-aff-0001" ref-type="aff">
<sup>1</sup>
</xref><address><email>gefen@tauex.tau.ac.il</email></address></contrib></contrib-group><aff id="iwj14192-aff-0001">
<label>
<sup>1</sup>
</label>
<named-content content-type="organisation-division">Department of Biomedical Engineering, Faculty of Engineering</named-content>
<institution>Tel Aviv University</institution>
<city>Tel Aviv</city>
<country country="IL">Israel</country>
</aff><author-notes><corresp id="correspondenceTo">
<label>*</label>
<bold>Correspondence</bold>
<break/>
Amit Gefen, PhD, Professor of Biomedical Engineering, The Herbert J. Berman Chair in Vascular Bioengineering, Department of Biomedical Engineering, Faculty of Engineering, Tel Aviv University, Tel Aviv 69978, Israel.<break/>
Email: <email>gefen@tauex.tau.ac.il</email>
<break/>
</corresp></author-notes><pub-date pub-type="epub"><day>18</day><month>4</month><year>2023</year></pub-date><pub-date pub-type="collection"><month>10</month><year>2023</year></pub-date><volume>20</volume><issue seq="220">8</issue><issue-id pub-id-type="pmc-issue-id">445364</issue-id><issue-id pub-id-type="doi">10.1111/iwj.v20.8</issue-id><fpage>3148</fpage><lpage>3156</lpage><history>
<date date-type="received"><day>20</day><month>2</month><year>2023</year></date>
<date date-type="accepted"><day>30</day><month>3</month><year>2023</year></date>
</history><pub-history><event event-type="pmc-release"><date><day>18</day><month>04</month><year>2023</year></date></event><event event-type="pmc-live"><date><day>16</day><month>09</month><year>2023</year></date></event><event event-type="pmc-last-change"><date iso-8601-date="2023-09-16 00:25:23.273"><day>16</day><month>09</month><year>2023</year></date></event></pub-history><permissions><copyright-statement content-type="article-copyright">© 2023 The Authors. <italic toggle="yes">International Wound Journal</italic> published by Medicalhelplines.com Inc and John Wiley &amp; Sons Ltd.</copyright-statement><license><ali:license_ref xmlns:ali="http://www.niso.org/schemas/ali/1.0/" specific-use="textmining" content-type="ccbyncndlicense">https://creativecommons.org/licenses/by-nc-nd/4.0/</ali:license_ref><license-p>This is an open access article under the terms of the <ext-link xmlns:xlink="http://www.w3.org/1999/xlink" ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by-nc-nd/4.0/">http://creativecommons.org/licenses/by-nc-nd/4.0/</ext-link> License, which permits use and distribution in any medium, provided the original work is properly cited, the use is non‐commercial and no modifications or adaptations are made.</license-p></license></permissions><self-uri xmlns:xlink="http://www.w3.org/1999/xlink" content-type="pmc-pdf" xlink:href="IWJ-20-3148.pdf"><?pdf-name IWJ-20-3148.pdf?><?pdf-size 3035402?><?pdf-md5 6e1dbcd2be3f0f0a029e0beb80e0c448?><?pdf-image-server-status NEVER_LOAD?><?pdf-cloudpmc-urn urn:app:5603/10502263/6e1dbcd2be3f/IWJ-20-3148.pdf?></self-uri><self-uri xmlns:xlink="http://www.w3.org/1999/xlink" content-type="pdf" xlink:href="file:IWJ-20-3148.pdf"/><abstract><title>Abstract</title><p>Support surfaces are the most important pressure ulcer/injury prevention technology available to clinicians for protecting their at‐risk patients. A hybrid support surface marries the benefits of reactive and active support surfaces, by using high‐quality foam material inside inflatable air cells. When used in its “static mode”, it is a constant low air pressure mattress which delivers pressure redistribution in response to patient bodyweight and movements, by maximising the immersion and envelopment performance of the support surface. When used in its powered “dynamic mode”, this system further delivers alternating pressure care via the connected foam and air cells. Modes of action of hybrid support surfaces were never studied quantitatively before, excluding through the limited scope of interface pressure mapping. In this work, we developed a novel computational modelling framework and simulations to visualise and quantify the state of soft tissue loading at the buttocks of a supine patient positioned on a hybrid support surface, in both the static and dynamic modes. We found that the dynamic mode effectively shifts deep concentrated soft tissue loading from under the sacral bone (towards the sacral promontory) to the tip of the sacrum (coccyx) and vice versa, and thereby, generates a deep tissue offloading effect.</p></abstract><kwd-group kwd-group-type="author-generated"><kwd id="iwj14192-kwd-0001">alternating pressure therapy</kwd><kwd id="iwj14192-kwd-0002">computational simulations in wound care</kwd><kwd id="iwj14192-kwd-0003">computer finite element model</kwd><kwd id="iwj14192-kwd-0004">medical mattress</kwd><kwd id="iwj14192-kwd-0005">pressure injury</kwd></kwd-group><funding-group><award-group id="funding-0001"><funding-source>Direct Healthcare Group</funding-source></award-group><award-group id="funding-0002"><funding-source><institution-wrap><institution>Ministry of Science, Technology and Space
</institution><institution-id institution-id-type="doi">10.13039/501100001738</institution-id></institution-wrap></funding-source><award-id>Medical Devices Program Grant no. 3‐17421 (AG)</award-id></award-group></funding-group><counts><fig-count count="4"/><table-count count="2"/><page-count count="9"/><word-count count="4821"/></counts><custom-meta-group><custom-meta><meta-name>pmc-status-qastatus</meta-name><meta-value>0</meta-value></custom-meta><custom-meta><meta-name>pmc-status-live</meta-name><meta-value>yes</meta-value></custom-meta><custom-meta><meta-name>pmc-status-embargo</meta-name><meta-value>no</meta-value></custom-meta><custom-meta><meta-name>pmc-status-released</meta-name><meta-value>yes</meta-value></custom-meta><custom-meta><meta-name>pmc-prop-open-access</meta-name><meta-value>yes</meta-value></custom-meta><custom-meta><meta-name>pmc-prop-olf</meta-name><meta-value>no</meta-value></custom-meta><custom-meta><meta-name>pmc-prop-manuscript</meta-name><meta-value>no</meta-value></custom-meta><custom-meta><meta-name>pmc-prop-legally-suppressed</meta-name><meta-value>no</meta-value></custom-meta><custom-meta><meta-name>pmc-prop-has-pdf</meta-name><meta-value>yes</meta-value></custom-meta><custom-meta><meta-name>pmc-prop-has-supplement</meta-name><meta-value>no</meta-value></custom-meta><custom-meta><meta-name>pmc-prop-pdf-only</meta-name><meta-value>no</meta-value></custom-meta><custom-meta><meta-name>pmc-prop-suppress-copyright</meta-name><meta-value>no</meta-value></custom-meta><custom-meta><meta-name>pmc-prop-is-real-version</meta-name><meta-value>no</meta-value></custom-meta><custom-meta><meta-name>pmc-prop-is-scanned-article</meta-name><meta-value>no</meta-value></custom-meta><custom-meta><meta-name>pmc-prop-preprint</meta-name><meta-value>no</meta-value></custom-meta><custom-meta><meta-name>pmc-prop-in-epmc</meta-name><meta-value>yes</meta-value></custom-meta><custom-meta><meta-name>pmc-license-ref</meta-name><meta-value>CC BY-NC-ND</meta-value></custom-meta><custom-meta><meta-name>source-schema-version-number</meta-name><meta-value>2.0</meta-value></custom-meta><custom-meta><meta-name>cover-date</meta-name><meta-value>October 2023</meta-value></custom-meta><custom-meta><meta-name>details-of-publishers-convertor</meta-name><meta-value>Converter:WILEY_ML3GV2_TO_JATSPMC version:6.3.3 mode:remove_FC converted:15.09.2023</meta-value></custom-meta></custom-meta-group></article-meta><notes><p content-type="self-citation">
<mixed-citation publication-type="journal" id="iwj14192-cit-9001">
<string-name name-style="western">
<surname>Katz</surname>
<given-names>T</given-names>
</string-name>, <string-name name-style="western">
<surname>Gefen</surname>
<given-names>A</given-names>
</string-name>. <article-title>The biomechanical efficacy of a hybrid support surface in protecting supine patients from sacral pressure ulcers</article-title>. <source>Int Wound J</source>. <year>2023</year>;<volume>20</volume>(<issue>8</issue>):<fpage>3148</fpage>‐<lpage>3156</lpage>. doi:<pub-id pub-id-type="doi">10.1111/iwj.14192</pub-id>
<pub-id pub-id-type="pmcid">PMC10502263</pub-id><pub-id pub-id-type="pmid">37073432</pub-id></mixed-citation>
</p></notes></front><body id="iwj14192-body-0001"><def-list list-content="abbreviations" id="iwj14192-lp-0001"><title>Abbreviations</title><def-item><term id="iwj14192-li-0006">ECMO</term><def id="iwj14192-li-0007"><p>extracorporeal membrane oxygenation</p></def></def-item><def-item><term id="iwj14192-li-0008">FE</term><def id="iwj14192-li-0009"><p>finite element</p></def></def-item><def-item><term id="iwj14192-li-0010">HSS</term><def id="iwj14192-li-0011"><p>hybrid support surface</p></def></def-item><def-item><term id="iwj14192-li-0012">MOA</term><def id="iwj14192-li-0013"><p>mode of action</p></def></def-item><def-item><term id="iwj14192-li-0014">PI</term><def id="iwj14192-li-0015"><p>pressure injury</p></def></def-item><def-item><term id="iwj14192-li-0016">PU</term><def id="iwj14192-li-0017"><p>pressure ulcer</p></def></def-item></def-list><sec id="iwj14192-sec-0003"><label>1</label><title>INTRODUCTION</title><p>Pressure ulcers (PUs), also known as pressure injuries (PIs), form in body sites of sustained soft tissue stress concentrations associated with either bodyweight‐induced or medical device‐related mechanical forces.<xref rid="iwj14192-bib-0001" ref-type="bibr">
<sup>1</sup>
</xref> The vicious cycle of PUs/PIs is triggered by sustained, localised tissue deformations which lead to the initial deformation‐induced cell‐scale damage, then causing secondary inflammatory damage and tertiary ischemic damage, and eventually, tissue death and the clinical presentation of these wounds.<xref rid="iwj14192-bib-0001" ref-type="bibr">
<sup>1</sup>
</xref> Hence, minimising the exposure to sustained or prolonged soft tissue stress concentrations is the most effective, scientifically proven approach to reducing the occurrence of PUs/PIs in clinical settings, as the 2019 International PU/PI Prevention and Treatment Guideline state.<xref rid="iwj14192-bib-0001" ref-type="bibr">
<sup>1</sup>
</xref>
</p><p>Advanced medical support surfaces are designed to reduce the exposure to localised interface pressures and sustained soft tissue deformations, and therefore, the risk for PUs/PIs. These devices are commonly categorised into two main types: (i) Support surfaces that redistribute pressures and thereby, disperse tissue stresses but do not affect the patient positioning, and which are termed <italic toggle="yes">reactive</italic> support surfaces. (ii) Support surfaces that periodically relieve interface pressures by influencing the patient positioning, called <italic toggle="yes">active</italic> support surfaces. More specifically, the reactive principle is based on immersion and envelopment to distribute the body weight of a user over a larger surface area, thus alleviating the peak interface pressures. The active support surface type is electrically powered (often with battery backup), and cyclically inflates and deflates regions under the patient by means of an air pump. Consequently, elevated interface pressures are transferred back and forth under different body regions to reduce the duration (but not necessarily the magnitude) of exposure to the interface pressures.</p><p>A hybrid support surface (HSS) marries the reactive and active features in a single device, and can therefore act at each mode.<xref rid="iwj14192-bib-0002" ref-type="bibr">
<sup>2</sup>
</xref> This combined ability is achieved by using high‐quality foam material inside the inflatable air cells in a technology termed “foam‐in‐air”.<xref rid="iwj14192-bib-0002" ref-type="bibr">
<sup>2</sup>
</xref>, <xref rid="iwj14192-bib-0003" ref-type="bibr">
<sup>3</sup>
</xref> In a HSS, even if the air cells are all partially deflated while low constant pressure is kept by the pump for maximising the immersion (which is termed the “static mode” of operation), pressure redistribution occurs through envelopment, but when the active feature is turned on, periodic pressure reliefs ensue (which is termed the “dynamic mode”). A HSS is advantageous to use for at‐risk patients, particularly those who do not accommodate to, or do not clinically fit the classic “alternating pressure” mattress choice (eg, become nauseated or it affects their sleep quality).<xref rid="iwj14192-bib-0003" ref-type="bibr">
<sup>3</sup>
</xref> The protective performance of support surfaces including HSS in mitigating the risk of PUs/PIs is commonly assessed using traditional interface pressure mapping that visualises and quantifies the contact pressures of users. However, this approach of merely measuring the interface pressures is limited as it does not directly address the fundamental cause of PUs/PIs, namely, the sustained exposure to soft tissue stress concentrations.<xref rid="iwj14192-bib-0001" ref-type="bibr">
<sup>1</sup>
</xref> Computer modelling and simulations (also termed “in silico experiments”) are more contemporary and relevant, and are highly effective at showing the tissue loading state within the body on a support surface<xref rid="iwj14192-bib-0004" ref-type="bibr">
<sup>4</sup>
</xref>, <xref rid="iwj14192-bib-0005" ref-type="bibr">
<sup>5</sup>
</xref> but such an approach was not employed for studying the effectiveness of a HSS yet. Accordingly, the goal of this study was to create a new computer modelling framework for quantitatively describing the mode of action (MOA) of a HSS, in terms of the effect of this technology on the internal tissue loading state at the sacral region of patients in a supine posture.</p></sec><sec sec-type="methods" id="iwj14192-sec-0004"><label>2</label><title>METHODS</title><sec id="iwj14192-sec-0005"><label>2.1</label><title>Geometry</title><p>To examine the effects of the two modes of operation of the hybrid support surface, that is, static and dynamic (alternating pressure) modes, on the loading state of the soft tissues in the sacral region (for a supine lying position), a three‐dimensional computational finite element (FE) modelling framework was developed. The buttocks model used in the current modelling was previously developed and experimentally validated by our research group<xref rid="iwj14192-bib-0004" ref-type="bibr">
<sup>4</sup>
</xref>, <xref rid="iwj14192-bib-0005" ref-type="bibr">
<sup>5</sup>
</xref> and is based on MRI slices acquired from a healthy female subject (age 28 years, bodyweight 61 kg). Using the Scan‐IP module of the Simpleware® software package (Synopsis Inc., Mountain View, CA, USA), the MRI dataset was segmented into the different tissue components including the pelvic/sacral bones, skeletal muscle, adipose and skin tissues (Figure <xref rid="iwj14192-fig-0001" ref-type="fig">1A</xref>). The maximum dimensions of the buttocks model are 38.2 × 22.3 × 23 (width × height × length). Meshing of the buttocks was also performed using Scan‐IP whereas meshing of the HSS was conducted by means of the ABAQUS FE software mesh generator (Dassault Systems, Vélizy‐Villacoublay, France).<xref rid="iwj14192-bib-0006" ref-type="bibr">
<sup>6</sup>
</xref> To analyse the stresses and strains in the soft tissues at the sacral region resulting from the bodyweight forces, two volumes of interest (VOIs) were defined: VOI#1 was skin and VOI#2 was adipose and muscle at the buttocks (Figure <xref rid="iwj14192-fig-0001" ref-type="fig">1B</xref>).</p><fig position="float" fig-type="FIGURE" id="iwj14192-fig-0001" orientation="portrait"><label>FIGURE 1</label><caption><p>Geometry of the computational (finite element) buttocks model: (A) The undeformed buttocks incorporating the skin, fat and skeletal muscle tissue structures that envelop the pelvic and sacral bones and the proximal femurs (reproduced from<xref rid="iwj14192-bib-0005" ref-type="bibr">
<sup>5</sup>
</xref> with permission under the terms of the Creative Commons licence). (B) The volumes of interest (VOIs) of the soft tissues at the sacral region, for computational analyses of skin (VOI #1) and subdermal (adipose and muscle; VOI #2) tissue exposures to strains and stresses.</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" position="anchor" id="jats-graphic-1" orientation="portrait" xlink:href="IWJ-20-3148-g001.jpg"><?image-name IWJ-20-3148-g001.jpg?><?image-size 69729?><?image-md5 0f236a3927a219e2b69c4203a1716b58?><?image-image-server-status LOAD_COMPLETED?><?image-original-height 951?><?image-original-width 1064?><?image-scaled-height 634?><?image-scaled-width 709?><?image-cloudpmc-urn urn:cdn:blobs/5603/10502263/0f236a3927a2/IWJ-20-3148-g001.jpg?><?thumb-name IWJ-20-3148-g001.gif?><?thumb-size 3958?><?thumb-md5 f05577c2500324905c051ed31db7dfee?><?thumb-image-server-status NEVER_LOAD?><?thumb-scaled-height 89?><?thumb-scaled-width 100?><?thumb-cloudpmc-urn urn:cdn:blobs/5603/10502263/f05577c25003/IWJ-20-3148-g001.gif?></graphic></fig><p>Modelling of the HSS was based on the Dyna‐Form® SMARTresponse® device specifications (Direct Healthcare Group, Caerphilly, United Kingdom).<xref rid="iwj14192-bib-0002" ref-type="bibr">
<sup>2</sup>
</xref> Three identical and parallel air cells of the HSS located under the buttocks were represented in the modelling, each sized 80 × 7 × 10 cm and a gap of 1 mm is considered between two adjacent cells (Figure <xref rid="iwj14192-fig-0002" ref-type="fig">2A</xref>). The air cells had two components; a foam core sized 80 × 6 × 7.5 cm enveloped by an inflatable cell membrane made of poly‐vinyl‐chloride (PVC; modelled as a “shell”) with wall thickness of 0.5 mm. The foam core and cell membrane share the same base as the HSS, such that when the PVC membrane is deflated, 64% of the cell volume is occupied by the foam core. The model was solved in two variants, static mode where all the air cells are at the same (low) pressure level of 1 kPa (Figure <xref rid="iwj14192-fig-0002" ref-type="fig">2B</xref>) and the dynamic (alternating pressure) mode where nonadjacent air cells are cyclically inflated and deflated to alternate between pressure levels of 3.5 and 1 kPa (ie, between cycles A and B; Figure <xref rid="iwj14192-fig-0002" ref-type="fig">2C</xref>).</p><fig position="float" fig-type="FIGURE" id="iwj14192-fig-0002" orientation="portrait"><label>FIGURE 2</label><caption><p>Modelling the interaction of the buttocks with (supporting three air cells of) the hybrid mattress: (A) The boundary and loading conditions of the model. The partial bodyweight that represents the mass of the pelvic region is applied on the skeleton (black arrows) and the inferior aspect of the support surface is fixed for all (translational and rotational) motions. (B) Model representation of the static pressure mode of the hybrid mattress where all the air cells are at the same pressure level of <italic toggle="yes">S</italic> = 1 kPa. (C) Model representation of the alternating pressure mode (cycles A and B) where nonadjacent air cells are cyclically inflated and deflated to alternate between pressure levels of <italic toggle="yes">H</italic> = 3.5 kPa and <italic toggle="yes">L</italic> = 1 kPa.</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" position="anchor" id="jats-graphic-3" orientation="portrait" xlink:href="IWJ-20-3148-g002.jpg"><?image-name IWJ-20-3148-g002.jpg?><?image-size 66082?><?image-md5 88c1a982c5422a80667920a2f542c71f?><?image-image-server-status LOAD_COMPLETED?><?image-original-height 938?><?image-original-width 1064?><?image-scaled-height 625?><?image-scaled-width 709?><?image-cloudpmc-urn urn:cdn:blobs/5603/10502263/88c1a982c542/IWJ-20-3148-g002.jpg?><?thumb-name IWJ-20-3148-g002.gif?><?thumb-size 3707?><?thumb-md5 ab275318a60fe75db5dcf3c3115bce4b?><?thumb-image-server-status NEVER_LOAD?><?thumb-scaled-height 88?><?thumb-scaled-width 100?><?thumb-cloudpmc-urn urn:cdn:blobs/5603/10502263/ab275318a60f/IWJ-20-3148-g002.gif?></graphic></fig></sec><sec id="iwj14192-sec-0006"><label>2.2</label><title>Mechanical properties of the model components</title><p>All the materials, including the body tissue and HSS components were assumed to be homogenous and isotropic, and their constitutive laws and mechanical properties were adopted from the literature (Table <xref rid="iwj14192-tbl-0001" ref-type="table">1</xref>). Specifically, bone tissues were modelled as a linear‐elastic material with elastic modulus of 7 GPa and Poisson's ratio of 0.3.<xref rid="iwj14192-bib-0007" ref-type="bibr">
<sup>7</sup>
</xref> The skin, adipose and muscle tissues were assumed to behave as nearly incompossible, hyperelastic neo‐Hookean materials<xref rid="iwj14192-bib-0004" ref-type="bibr">
<sup>4</sup>
</xref>, <xref rid="iwj14192-bib-0008" ref-type="bibr">
<sup>8</sup>
</xref>, <xref rid="iwj14192-bib-0009" ref-type="bibr">
<sup>9</sup>
</xref> with strain energy density<disp-formula id="iwj14192-disp-0001">
<label>(1)</label>
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="jats-math-1" display="block" overflow="scroll"><mml:mrow><mml:mi>W</mml:mi><mml:mo linebreak="goodbreak">=</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mn>10</mml:mn></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:mover accent="true"><mml:msub><mml:mi>I</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:mo stretchy="true">¯</mml:mo></mml:mover><mml:mo linebreak="goodbreak">−</mml:mo><mml:mn>3</mml:mn></mml:mrow></mml:mfenced><mml:mo linebreak="goodbreak">+</mml:mo><mml:mfrac><mml:mn>1</mml:mn><mml:msub><mml:mi>D</mml:mi><mml:mn>1</mml:mn></mml:msub></mml:mfrac><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mi mathvariant="italic">el</mml:mi></mml:msub><mml:mo linebreak="goodbreak">−</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:mfenced><mml:mn>2</mml:mn></mml:msup></mml:mrow></mml:math>
</disp-formula>function <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="jats-math-2" display="inline" overflow="scroll"><mml:mrow><mml:mi>W</mml:mi></mml:mrow></mml:math>:where <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="jats-math-3" display="inline" overflow="scroll"><mml:mrow><mml:mover accent="true"><mml:msub><mml:mi>I</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:mo stretchy="true">¯</mml:mo></mml:mover></mml:mrow></mml:math> is the first invariant of the right Cauchy‐Green deformation tensor, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="jats-math-4" display="inline" overflow="scroll"><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mi mathvariant="italic">el</mml:mi></mml:msub></mml:mrow></mml:math> is the determinant of the deformation gradient tensor, and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="jats-math-5" display="inline" overflow="scroll"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn>10</mml:mn></mml:msub><mml:mspace width="0.25em"/><mml:mtext mathvariant="italic">and</mml:mtext><mml:mspace width="0.25em"/><mml:msub><mml:mi>D</mml:mi><mml:mn>1</mml:mn></mml:msub></mml:mrow></mml:math> are material parameters representing the shear (<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="jats-math-6" display="inline" overflow="scroll"><mml:mrow><mml:msub><mml:mi>μ</mml:mi><mml:mn>0</mml:mn></mml:msub></mml:mrow></mml:math>) and bulk (<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="jats-math-7" display="inline" overflow="scroll"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mn>1</mml:mn></mml:msub></mml:mrow></mml:math>) modulus respectively and defined as: <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="jats-math-8" display="inline" overflow="scroll"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn>10</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:msub><mml:mi>μ</mml:mi><mml:mn>0</mml:mn></mml:msub><mml:mn>2</mml:mn></mml:mfrac><mml:mo>,</mml:mo><mml:msub><mml:mi>D</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mfrac><mml:mn>2</mml:mn><mml:msub><mml:mi>K</mml:mi><mml:mn>1</mml:mn></mml:msub></mml:mfrac></mml:mrow></mml:math>. The foam cores of air cells in the HSS were assumed to be linear‐elastic with an elastic modulus of 15 kPa and a Poisson's ratio of 0.3.<xref rid="iwj14192-bib-0004" ref-type="bibr">
<sup>4</sup>
</xref> The PVC cell membrane was modelled as an incompressible hyperelastic Mooney‐Rivlin material<xref rid="iwj14192-bib-0010" ref-type="bibr">
<sup>10</sup>
</xref>, <xref rid="iwj14192-bib-0011" ref-type="bibr">
<sup>11</sup>
</xref> with the coefficients set as <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="jats-math-9" display="inline" overflow="scroll"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn>10</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn>1.44</mml:mn><mml:mspace width="0.25em"/><mml:mfenced open="[" close="]"><mml:mi mathvariant="italic">MPa</mml:mi></mml:mfenced><mml:mo>,</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mn>01</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn>1.74</mml:mn><mml:mspace width="0.25em"/><mml:mfenced open="[" close="]"><mml:mi mathvariant="italic">MPa</mml:mi></mml:mfenced><mml:mo>,</mml:mo><mml:msub><mml:mi>D</mml:mi><mml:mn>1</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn>0</mml:mn></mml:mrow></mml:math>.</p><table-wrap position="float" id="iwj14192-tbl-0001" content-type="TABLE" orientation="portrait"><label>TABLE 1</label><caption><p>The material parameters of the model components.</p></caption><table frame="hsides" rules="cols"><col align="left" span="1"/><col align="left" span="1"/><col align="left" span="1"/><col align="left" span="1"/><col align="left" span="1"/><col align="char" char="." span="1"/><thead valign="bottom"><tr style="border-bottom:solid 1px #000000"><th align="left" valign="bottom" rowspan="1" colspan="1">Material type</th><th align="left" valign="bottom" rowspan="1" colspan="1">Shear modulus [KPa]</th><th align="left" valign="bottom" rowspan="1" colspan="1">Bulk modulus [KPa]</th><th align="left" valign="bottom" rowspan="1" colspan="1">Elastic modulus [KPa]</th><th align="left" valign="bottom" rowspan="1" colspan="1">Poisson's ratio</th><th align="left" valign="bottom" rowspan="1" colspan="1">Number of elements</th></tr></thead><tbody valign="top"><tr><td align="left" valign="top" rowspan="1" colspan="1">Skin</td><td align="left" valign="top" rowspan="1" colspan="1">8</td><td align="left" valign="top" rowspan="1" colspan="1">666.67</td><td align="left" valign="top" rowspan="1" colspan="1">‐</td><td align="left" valign="top" rowspan="1" colspan="1">0.495</td><td align="char" valign="top" rowspan="1" colspan="1">163 395</td></tr><tr><td align="left" valign="top" rowspan="1" colspan="1">Adipose</td><td align="left" valign="top" rowspan="1" colspan="1">0.8</td><td align="left" valign="top" rowspan="1" colspan="1">66.67</td><td align="left" valign="top" rowspan="1" colspan="1">‐</td><td align="left" valign="top" rowspan="1" colspan="1">0.495</td><td align="char" valign="top" rowspan="1" colspan="1">261 487</td></tr><tr><td align="left" valign="top" rowspan="1" colspan="1">Muscle</td><td align="left" valign="top" rowspan="1" colspan="1">0.45</td><td align="left" valign="top" rowspan="1" colspan="1">37.5</td><td align="left" valign="top" rowspan="1" colspan="1">‐</td><td align="left" valign="top" rowspan="1" colspan="1">0.495</td><td align="char" valign="top" rowspan="1" colspan="1">128 379</td></tr><tr><td align="left" valign="top" rowspan="1" colspan="1">Bone</td><td align="left" valign="top" rowspan="1" colspan="1">‐</td><td align="left" valign="top" rowspan="1" colspan="1">‐</td><td align="left" valign="top" rowspan="1" colspan="1">7 × 10<sup>6</sup>
</td><td align="left" valign="top" rowspan="1" colspan="1">0.3</td><td align="char" valign="top" rowspan="1" colspan="1">12 728</td></tr><tr><td align="left" valign="top" rowspan="1" colspan="1">Foam</td><td align="left" valign="top" rowspan="1" colspan="1">‐</td><td align="left" valign="top" rowspan="1" colspan="1">‐</td><td align="left" valign="top" rowspan="1" colspan="1">15</td><td align="left" valign="top" rowspan="1" colspan="1">0.3</td><td align="char" valign="top" rowspan="1" colspan="1">70 312</td></tr><tr><td align="left" valign="top" rowspan="1" colspan="1">PVC cell walls</td><td align="left" valign="top" rowspan="1" colspan="1">3180</td><td align="left" valign="top" rowspan="1" colspan="1">‐</td><td align="left" valign="top" rowspan="1" colspan="1">‐</td><td align="left" valign="top" rowspan="1" colspan="1">0.5</td><td align="char" valign="top" rowspan="1" colspan="1">13 296</td></tr></tbody></table><table-wrap-foot id="iwj14192-ntgp-0001"><fn id="iwj14192-note-0001"><p>Abbreviation: PVC, polyvinyl chloride.</p></fn></table-wrap-foot></table-wrap></sec><sec id="iwj14192-sec-0007"><label>2.3</label><title>Boundary conditions and interfaces</title><p>The bodyweight forces of supine lying were represented through downward displacements applied to the femurs until a force of 90 N, perpendicular to the HSS (representing the partial body weight of the pelvic region for the modelled subject), was reached. The femurs were fixed in all the other directions. To represent the continued cell pattern of the mattress, interfaces to the non‐modelled air cells supporting the trunk and leg regions were considered rigid (to account for the resistance from these cells to the inflation pressure of the 3 modelled cells). Likewise, the proximal and distal surfaces of the buttocks were fixed for movement along the longitudinal body axis to simulate a continuum of tissues. All the segmented body tissues were assigned tied interfaces at the tissue‐tissue boundaries. The inferior surfaces of the air cells were fixed for translations in all directions, but rotation of surface nodes was allowed. Frictional sliding was defined between the buttocks and air cells, as well as between the inner surfaces of the inflatable PVC membrane and the foam core, with a coefficient of friction (COF) of 0.15. Finally, frictionless self‐contact was applied to potentially contact skin surfaces at the inner thighs and intergluteal cleft to avoid element penetration.</p><p>To simulate the inflation of the air cells, each cell was assigned a fluid cavity boundary condition. The fluid cavity confining surfaces for each cell were the inner surface of the PVC membrane and the outer surface of the foam core. The fluid in the cavity was defined as air acting as an ideal gas<disp-formula id="iwj14192-disp-0002">
<label>(2)</label>
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="jats-math-10" display="block" overflow="scroll"><mml:mrow><mml:mi>P</mml:mi><mml:mo linebreak="goodbreak">=</mml:mo><mml:mi>ρ</mml:mi><mml:mfrac><mml:mover accent="true"><mml:mi>R</mml:mi><mml:mo stretchy="true">~</mml:mo></mml:mover><mml:mi mathvariant="italic">MW</mml:mi></mml:mfrac><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>θ</mml:mi><mml:mo linebreak="goodbreak">−</mml:mo><mml:msup><mml:mi>θ</mml:mi><mml:mi>Z</mml:mi></mml:msup></mml:mrow></mml:mfenced><mml:mo linebreak="goodbreak">−</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mi>A</mml:mi></mml:msub></mml:mrow></mml:math>
</disp-formula>following the ideal gas law:where <italic toggle="yes">P</italic> (in MPa) is the absolute air cell pressure, <italic toggle="yes">P</italic>
<sub>
<italic toggle="yes">A</italic>
</sub> is the ambient pressure (set to zero to focus on the differential pressure), <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="jats-math-11" display="inline" overflow="scroll"><mml:mrow><mml:mi>θ</mml:mi></mml:mrow></mml:math> (in degrees Kelvin) is the current temperature, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="jats-math-12" display="inline" overflow="scroll"><mml:mrow><mml:msup><mml:mi>θ</mml:mi><mml:mi>Z</mml:mi></mml:msup></mml:mrow></mml:math> is the absolute zero (0 K), ρ is the air density, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="jats-math-13" display="inline" overflow="scroll"><mml:mrow><mml:mover accent="true"><mml:mi>R</mml:mi><mml:mo stretchy="true">~</mml:mo></mml:mover></mml:mrow></mml:math> is the universal gas constant and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="jats-math-14" display="inline" overflow="scroll"><mml:mrow><mml:mi mathvariant="italic">MW</mml:mi></mml:mrow></mml:math> is the molecular weight of air.</p><p>The initial inflation process and the air cell distortion because of the bodyweight forces applied to the air cells were assumed to be isothermal, that is, the internal air cell temperature was assumed to be constant at 298 K and unaffected by either the inflation or the body. With that said, the downward displacement of the buttocks was commenced only after the cells were inflated to the defined pressure.</p></sec><sec id="iwj14192-sec-0008"><label>2.4</label><title>Numerical method</title><p>The buttocks were meshed using four‐node tetrahedral elements: Bones were meshed with first order linear elements (C3D4) whereas for the soft tissues, first order linear hybrid elements (C3D4H) were used. The foam core was meshed using eight‐node hexahedral elements with reduced integration (C3D8RH), and the PVC membrane was meshed using four‐node shell element with reduced integration (S4R). The numbers of elements used to mesh each of the model components are detailed in Table <xref rid="iwj14192-tbl-0001" ref-type="table">1</xref>. The FE simulations were set up and solved using the Abaqus/CAE 2020 software suit. The runtime for each model variant was approximately 6 h using six parallel cores of a 64‐bit Windows 10 PC with Intel Core i7 processor, 3.00 GHz and 32 GB of RAM.</p></sec><sec id="iwj14192-sec-0009"><label>2.5</label><title>Outcome measures and model validation</title><p>For each model variant (that is, the static mode and the two cycles A and B of the alternating mode; Figure <xref rid="iwj14192-fig-0002" ref-type="fig">2B,C</xref>), the tissue strain and stress distributions (Figure <xref rid="iwj14192-fig-0003" ref-type="fig">3</xref>) were calculated within the two VOIs (ie, VOI#1 for skin and VOI#2 for adipose and muscle). Histograms of these soft tissue strains and stresses were further plotted for the fourth quartile of the corresponding loading measure domain, to focus on the tissue strain/stress concentrations (Figure <xref rid="iwj14192-fig-0004" ref-type="fig">4</xref>). A <italic toggle="yes">Z</italic>‐score test with a threshold of 4 was ran on each of these tissue strain/stress datasets to exclude numerical outliers because of excessively distorted elements, and it was found that such excessive element distortion sites, if existing, did not exceed a total volume of 0.05% per each VOI. The transient tissue relief from the sustained tissue strain/stress concentration exposures achieved by activation of the alternating mode of the HSS was then further evaluated by calculating the change in the area bounded by the corresponding histogram curves and the <italic toggle="yes">x</italic>‐axis with respect to the curve of the static mode. This latter outcome measure was defined as the percent change in volumetric tissue exposure to loading (%‐CVTEL), and was calculated separately for the tissue strain and stress datasets (per each cycle, A or B).</p><fig position="float" fig-type="FIGURE" id="iwj14192-fig-0003" orientation="portrait"><label>FIGURE 3</label><caption><p>The effective soft tissue strain (A) and stress (B) distributions in the buttocks for supine lying on the hybrid mattress. The tissue loading states are shown in sagittal (top) and transverse (bottom) cross‐sections, for (from the left to right panels:) cycles A and B of the alternating mode and the static (S) mode.</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" position="anchor" id="jats-graphic-5" orientation="portrait" xlink:href="IWJ-20-3148-g003.jpg"><?image-name IWJ-20-3148-g003.jpg?><?image-size 180188?><?image-md5 dacc5512f393d15f4a5f35f015925315?><?image-image-server-status LOAD_COMPLETED?><?image-original-height 1620?><?image-original-width 1064?><?image-scaled-height 1079?><?image-scaled-width 709?><?image-cloudpmc-urn urn:cdn:blobs/5603/10502263/dacc5512f393/IWJ-20-3148-g003.jpg?><?thumb-name IWJ-20-3148-g003.gif?><?thumb-size 7819?><?thumb-md5 4a9a5bbda4bf8026723c8278a2458ad5?><?thumb-image-server-status NEVER_LOAD?><?thumb-scaled-height 152?><?thumb-scaled-width 100?><?thumb-cloudpmc-urn urn:cdn:blobs/5603/10502263/4a9a5bbda4bf/IWJ-20-3148-g003.gif?></graphic></fig><fig position="float" fig-type="FIGURE" id="iwj14192-fig-0004" orientation="portrait"><label>FIGURE 4</label><caption><p>The volumetric soft tissue exposures to effective strains (left panels) and stresses (right panels) above the 3rd‐quartile in the volumes of interest (VOIs) for (A) skin (VOI#1) and (B) muscle and adipose (VOI#2) tissues.</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" position="anchor" id="jats-graphic-7" orientation="portrait" xlink:href="IWJ-20-3148-g004.jpg"><?image-name IWJ-20-3148-g004.jpg?><?image-size 54557?><?image-md5 2e400aa71b71c9a4db37a020437de12f?><?image-image-server-status LOAD_COMPLETED?><?image-original-height 939?><?image-original-width 1064?><?image-scaled-height 626?><?image-scaled-width 709?><?image-cloudpmc-urn urn:cdn:blobs/5603/10502263/2e400aa71b71/IWJ-20-3148-g004.jpg?><?thumb-name IWJ-20-3148-g004.gif?><?thumb-size 2656?><?thumb-md5 336a8486f12d37dfec7c2497e415e70a?><?thumb-image-server-status NEVER_LOAD?><?thumb-scaled-height 88?><?thumb-scaled-width 100?><?thumb-cloudpmc-urn urn:cdn:blobs/5603/10502263/336a8486f12d/IWJ-20-3148-g004.gif?></graphic></fig><p>The current simulation data was validated by comparing model‐predicted hydrostatic pressures (<italic toggle="yes">P</italic> = <italic toggle="yes">σ</italic>
<sub>ii</sub>/3) for the skin elements in contact with cell #2 (Figure <xref rid="iwj14192-fig-0002" ref-type="fig">2A</xref>) to corresponding interface pressure data acquired using calibrated pressure mapping systems from the sacral regions of subjects lying on the same HSS and reported by the manufacturer of the HSS or in the literature.<xref rid="iwj14192-bib-0002" ref-type="bibr">
<sup>2</sup>
</xref>, <xref rid="iwj14192-bib-0012" ref-type="bibr">
<sup>12</sup>
</xref> The model‐predicted sacral peak pressures in the static mode, cycle A and cycle B differed from the means of reported real‐world experimental interface peak pressures by 3%, 14% and 10%, respectively, which is considered to indicate excellent agreement given the inherent anatomical variability across subjects.</p></sec></sec><sec sec-type="results" id="iwj14192-sec-0010"><label>3</label><title>RESULTS</title><p>The distributions of the soft tissue strains and stresses at the sacral region are considerably different between the static and the alternating (cycles A and B) modes of the HSS, which is evident both visually (Figure <xref rid="iwj14192-fig-0003" ref-type="fig">3</xref>) and quantitatively (Figure <xref rid="iwj14192-fig-0004" ref-type="fig">4</xref>). Specifically, temporarily deflating the air cell directly under the coccyx (ie, cycle A of the alternating mode) reduces the magnitudes and dispersal of the deep tissue strain/stress concentrations around the coccyx with respect to the static mode. However, this deflation action in turn increases the strain/stress exposure under the sacral bone with respect to both the static mode and cycle B of the alternating mode (Figure <xref rid="iwj14192-fig-0003" ref-type="fig">3</xref>; left panels versus right panels of the sagittal views). Alternating between cycles A and B in the alternating mode of the HSS thereby effectively shifts concentrated tissue loading from under the sacral bone (towards the sacral promontory) to the tip of the sacrum (coccyx) and vice versa (Figure <xref rid="iwj14192-fig-0003" ref-type="fig">3</xref>).</p><p>The strain/stress histograms for the skin and subdermal tissues are all consistently demonstrating that the static mode of the HSS induces tissue loading levels that are between those of cycles A and B of the alternating mode, which is a further indication that the alternating mode of the HSS fluctuates the tissue strain/stress concentrations around the “baseline” static mode (Figure <xref rid="iwj14192-fig-0004" ref-type="fig">4</xref>). With that said, there is considerable cyclic spatial shift of tissue loading sites as noted above between the coccyx and sacral promontory (Figure <xref rid="iwj14192-fig-0003" ref-type="fig">3</xref>). Consistently with the results plotted in Figure <xref rid="iwj14192-fig-0003" ref-type="fig">3</xref>, the %‐CVTEL data are all negative for cycle A, that is, the tissue strain/stress concentrations are generally alleviated with respect to the static mode of the HSS, and the %‐CVTEL data are all positive for cycle B which indicates that the tissue strain/stress concentration magnitudes overall increase for cycle B (Table <xref rid="iwj14192-tbl-0002" ref-type="table">2</xref>). However, this latter effect is essential for achieving the spatial cyclic redistribution of concentrated tissue loading as demonstrated in Figure <xref rid="iwj14192-fig-0003" ref-type="fig">3</xref>.</p><table-wrap position="float" id="iwj14192-tbl-0002" content-type="TABLE" orientation="portrait"><label>TABLE 2</label><caption><p>Percent change in volumetric tissue exposure to loading (%‐CVTEL) for tissue strain and stress and for cycles A and B with respect to the static mode of the hybrid support surface.</p></caption><table frame="hsides" rules="groups"><col align="left" span="1"/><col align="center" span="1"/><col align="char" char="." span="1"/><col align="center" span="1"/><col align="char" char="." span="1"/><thead valign="bottom"><tr style="border-bottom:solid 1px #000000"><th style="border-bottom:solid 1px #000000" align="left" valign="bottom" rowspan="1" colspan="1"/><th colspan="2" style="border-bottom:solid 1px #000000" align="left" valign="bottom" rowspan="1">%‐CVTEL strain</th><th colspan="2" style="border-bottom:solid 1px #000000" align="left" valign="bottom" rowspan="1">%‐CVTEL stress</th></tr><tr style="border-bottom:solid 1px #000000"><th align="left" valign="bottom" rowspan="1" colspan="1"/><th align="left" valign="bottom" rowspan="1" colspan="1">Cycle A</th><th align="left" valign="bottom" rowspan="1" colspan="1">Cycle B</th><th align="left" valign="bottom" rowspan="1" colspan="1">Cycle A</th><th align="left" valign="bottom" rowspan="1" colspan="1">Cycle B</th></tr></thead><tbody valign="top"><tr><td align="left" valign="top" rowspan="1" colspan="1">Skin (VOI#1)</td><td align="char" char="." valign="top" rowspan="1" colspan="1">−10.3</td><td align="char" valign="top" rowspan="1" colspan="1">36.2</td><td align="char" char="." valign="top" rowspan="1" colspan="1">−8.7</td><td align="char" valign="top" rowspan="1" colspan="1">39.2</td></tr><tr><td align="left" valign="top" rowspan="1" colspan="1">Muscle and adipose (VOI#2)</td><td align="char" char="." valign="top" rowspan="1" colspan="1">−7.5</td><td align="char" valign="top" rowspan="1" colspan="1">29.0</td><td align="char" char="." valign="top" rowspan="1" colspan="1">−5.1</td><td align="char" valign="top" rowspan="1" colspan="1">59.3</td></tr></tbody></table></table-wrap></sec><sec sec-type="discussion" id="iwj14192-sec-0011"><label>4</label><title>DISCUSSION</title><p>Support surfaces are the most important PU/PI prevention technology available to health care professionals for protecting their at‐risk patients. The preventative efficacy of the HSS investigated here was already clinically proven, with a reduction of 56% in the number of PUs/PIs achieved for the 6 months post‐deployment of this HSS in an acute hospital setting.<xref rid="iwj14192-bib-0013" ref-type="bibr">
<sup>13</sup>
</xref> With that said, the MOA of this specific HSS has not been investigated before, and more generally, the literature is missing quantitative bioengineering methodologies for standardised evaluations of the protective efficacy of dynamic (alternating pressure) support surfaces.<xref rid="iwj14192-bib-0003" ref-type="bibr">
<sup>3</sup>
</xref> Advanced computational modelling is powerful in both identifying the MOA and in providing the performance metrics for specific support surface technologies, particularly with regards to deep tissue load states and how these are affected by the support surface design features,<xref rid="iwj14192-bib-0005" ref-type="bibr">
<sup>5</sup>
</xref> and potentially, its dynamic action.</p><p>Previous published work focused on reactive (static) support surfaces rather than on active or alternating pressure mattresses.<xref rid="iwj14192-bib-0005" ref-type="bibr">
<sup>5</sup>
</xref>, <xref rid="iwj14192-bib-0014" ref-type="bibr">
<sup>14</sup>
</xref>, <xref rid="iwj14192-bib-0015" ref-type="bibr">
<sup>15</sup>
</xref>, <xref rid="iwj14192-bib-0016" ref-type="bibr">
<sup>16</sup>
</xref>, <xref rid="iwj14192-bib-0017" ref-type="bibr">
<sup>17</sup>
</xref>, <xref rid="iwj14192-bib-0018" ref-type="bibr">
<sup>18</sup>
</xref>, <xref rid="iwj14192-bib-0019" ref-type="bibr">
<sup>19</sup>
</xref>, <xref rid="iwj14192-bib-0020" ref-type="bibr">
<sup>20</sup>
</xref> The literature reporting computational modelling studies of advanced support surfaces is overall still sparse,<xref rid="iwj14192-bib-0016" ref-type="bibr">
<sup>16</sup>
</xref>, <xref rid="iwj14192-bib-0017" ref-type="bibr">
<sup>17</sup>
</xref> and none specifically refers to HSS. Hence the novel aspects in the current work are the focus on deep tissue load changes occurring when the support surface action changes from static to dynamic/alternating, and in particular, on identifying the MOA of the studied HSS in protecting patients at‐risk for PUs/PIs. We found that when used in its powered, alternating (active) mode, the HSS effectively shifts deep concentrated tissue loading from under the sacral bone (towards the sacral promontory) to the tip of the sacrum (coccyx), and vice versa. This aligns with the concept of internal load shifting in soft tissues by means of an alternating pressure mattress that periodically relieves localised tissue stresses, but for the first time in the literature, the current work visualises and quantifies this phenomenon for an HSS with the analyses encompassing both its static and dynamic modes of operation.</p><p>One of the core and unique features of the specific HSS technology studied here is that it is continuously monitoring for patient movements, and more specifically, for a prolonged period of non‐movement. When the “Auto Start” feature of this HSS is turned on, the HSS will automatically transition from its static to dynamic modes if three distinct and separate functional movements of the user are not detected within 1 h (‘functional’ is determined through four different weight categories).<xref rid="iwj14192-bib-0002" ref-type="bibr">
<sup>2</sup>
</xref> This is in fact an automated risk assessment followed by an immediate auto‐intervention when a PU/PI risk is detected because of the lack of movement. For the first time in the literature, the current work visualises and quantitatively demonstrates the effectiveness of such automated risk assessment and response to a detected risk, in the aspect of redistributing the deep tissue loads to mitigate that risk.</p><p>When evaluating the performance of a hybrid mattress, analysing the static mode in addition to the dynamic/alternating action is of great importance as well. The treatment plan for patients may not require continuous alternating pressure intervention, or the patient may at times feel uncomfortable or nauseated, or their sleep quality may be affected by the inflating and deflating cells, and there is also the unlikely scenario of a power failure.<xref rid="iwj14192-bib-0021" ref-type="bibr">
<sup>21</sup>
</xref> An HSS is designed to be able to cope with all these aforementioned situations. The foam core included in each of the air cells ensures that the patient will always remain on a high‐quality foam surface when the cells are completely deflated (ie, if there is no power).<xref rid="iwj14192-bib-0003" ref-type="bibr">
<sup>3</sup>
</xref> Our current results support the intended design of the foam core by showing that the foam cores adequately support the bodyweight of the patient when a cell is deflated, in which case the tissue loading levels are between those associated with cycles A and B of the alternating mode (Figure <xref rid="iwj14192-fig-0004" ref-type="fig">4</xref> and Table <xref rid="iwj14192-tbl-0002" ref-type="table">2</xref>). The support of the foam cores, in the static and alternating modes alike, further improves the comfort of the patient on the HSS and assists in repositioning and performing independent movements in bed, which in turn contributes to improving the quality of life of the treated patient and ultimately, to better wound prevention and management outcomes.<xref rid="iwj14192-bib-0018" ref-type="bibr">
<sup>18</sup>
</xref>
</p><p>The modelling is based on several assumptions, including that it does not represent the entire range of anatomical variations of at‐risk patients, nor the possible deviation in tissue mechanical properties and how these are affected by chronic conditions (eg, diabetes or scarring from a previous PU/PI that has healed). Likewise, COFs may vary depending on the individual skin characteristics, the bedlinen type and moisture at the body‐support interfaces. Finally, postures that vary from the pure supine position modelled here, such as a rotated trunk or suspended heels, may affect the currently reported results. Accordingly, interpretation of the data reported here should focus on the trends of changes of the tissue load states between the modes of the HSS rather than on specific tissue stress values. Future steps in the efficacy research of the studied HSS can address specific patient populations with distinct anatomical characteristics such as underweight or obese, or consider a case of an existing PU/PI which needs to be treated while the patient is supine (for example if that patient is ventilated or is connected to an extracorporeal membrane oxygenation ‐ ECMO machine). In addition, the protective effect of the HSS can be investigated for other anatomical regions (eg, the head, shoulders, or heels), or body postures, for example, for side or prone lying.</p><p>In conclusion, this study demonstrated a deep tissue offloading effect of the studied HSS, achieved by cyclically inflating and deflating the air cells, which shifts the internal tissue loads from under the sacral bone to the tip of the sacrum, and vice versa with the inflation/deflation cycles, thereby periodically relieving soft tissue sites at risk for a PU/PI.</p></sec></body><back><ack id="iwj14192-sec-0012"><title>ACKNOWLEDGEMENTS</title><p>This work was partially supported by the Israeli Ministry of Science &amp; Technology (Medical Devices Program Grant no. 3‐17421, awarded to Professor Amit Gefen in 2020) and by an unrestricted educational grant from Direct Healthcare Group (Caerphilly, United Kingdom).</p></ack><sec sec-type="data-availability" id="iwj14192-sec-0014"><title>DATA AVAILABILITY STATEMENT</title><p>The data that support the findings of this study are available from the corresponding author upon reasonable request.</p></sec><ref-list id="iwj14192-bibl-0001" content-type="cited-references"><title>REFERENCES</title><ref id="iwj14192-bib-0001"><label>1</label><mixed-citation publication-type="journal" id="iwj14192-cit-0001">
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