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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="doi">10.3389/fphys.2021.783457</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Physiology</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Subject-Specific Pressure Normalization of Local Pulse Wave Velocity: Separating Intrinsic From Acute Load-Dependent Stiffening in Hypertensive Patients</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name><surname>Giudici</surname> <given-names>Alessandro</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/1374644/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Palombo</surname> <given-names>Carlo</given-names></name>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/23207/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Kozakova</surname> <given-names>Michaela</given-names></name>
<xref ref-type="aff" rid="aff3"><sup>3</sup></xref>
</contrib>
<contrib contrib-type="author">
<name><surname>Morizzo</surname> <given-names>Carmela</given-names></name>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
</contrib>
<contrib contrib-type="author">
<name><surname>Cruickshank</surname> <given-names>J. Kennedy</given-names></name>
<xref ref-type="aff" rid="aff4"><sup>4</sup></xref>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name><surname>Khir</surname> <given-names>Ashraf W.</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="corresp" rid="c001"><sup>&#x002A;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/887711/overview"/>
</contrib>
</contrib-group>
<aff id="aff1"><sup>1</sup><institution>Brunel Institute for Bioengineering, Brunel University London</institution>, <addr-line>Uxbridge</addr-line>, <country>United Kingdom</country></aff>
<aff id="aff2"><sup>2</sup><institution>Department of Surgical, Medical, Molecular Pathology and Critical Area Medicine, University of Pisa</institution>, <addr-line>Pisa</addr-line>, <country>Italy</country></aff>
<aff id="aff3"><sup>3</sup><institution>Department of Clinical and Experimental Medicine, University of Pisa</institution>, <addr-line>Pisa</addr-line>, <country>Italy</country></aff>
<aff id="aff4"><sup>4</sup><institution>School of Life-Course/Nutritional Sciences, King&#x2019;s College, St. Thomas&#x2019; and Guy&#x2019;s Hospitals</institution>, <addr-line>London</addr-line>, <country>United Kingdom</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Dimitrios Terentes-Printzios, University of Oxford, United Kingdom</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Zhe Sun, University of Missouri, United States; Spyretta Golemati, National and Kapodistrian University of Athens, Greece</p></fn>
<corresp id="c001">&#x002A;Correspondence: Ashraf W. Khir, <email>ashraf.w.khir@durham.ac.uk</email></corresp>
<fn fn-type="other" id="fn004"><p>This article was submitted to Vascular Physiology, a section of the journal Frontiers in Physiology</p></fn>
</author-notes>
<pub-date pub-type="epub">
<day>15</day>
<month>02</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2021</year>
</pub-date>
<volume>12</volume>
<elocation-id>783457</elocation-id>
<history>
<date date-type="received">
<day>26</day>
<month>09</month>
<year>2021</year>
</date>
<date date-type="accepted">
<day>14</day>
<month>12</month>
<year>2021</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x00A9; 2022 Giudici, Palombo, Kozakova, Morizzo, Cruickshank and Khir.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Giudici, Palombo, Kozakova, Morizzo, Cruickshank and Khir</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>Pulse wave velocity (PWV) is a powerful predictor of cardiovascular events. However, its intrinsic blood pressure (BP)-dependency complicates distinguishing between acute and chronic effects of increased BP on arterial stiffness. Based on the assumption that arteries exhibit a nearly exponential pressure-area (<italic>P</italic>-<italic>A</italic>) relationship, this study proposes a method to assess intersubject differences in local PWV independently from BP. The method was then used to analyze differences in local carotid PWV (cPWV) between hypertensive and healthy normotensive people before and after BP-normalization. Pressure (<italic>P</italic>) and diameter (<italic>D</italic>) waveforms were simultaneously acquired <italic>via</italic> tonometer at the left and ultrasound scanning at right common carotid artery (CCA), respectively, in 22 patients with Grade 1 or 2 hypertension and 22 age- and sex-matched controls. cPWV was determined using the <italic>D</italic><sup>2</sup><italic>P</italic>-loop method. Then, the exponential modeling of the <italic>P</italic>-area (<italic>A</italic> = &#x03C0;<italic>D</italic><sup>2</sup>/4) relationships allowed defining a mathematical formulation to compute subject-specific changes in cPWV associated with BP changes, thus enabling the normalization of cPWV against intersubject differences in BP at the time of measurement. Carotid systolic BP (SBP) and diastolic BP (DBP) were, on average, 17.7 (<italic>p</italic> &#x003C; 0.001) and 8.9 mmHg (<italic>p</italic> &#x003C; 0.01) higher in hypertensives than controls, respectively. cPWV was 5.56 &#x00B1; 0.86 m/s in controls and 6.24 &#x00B1; 1.22 m/s in hypertensives. BP alone accounted for 68% of the cPWV difference between the two groups: 5.80 &#x00B1; 0.84 vs. 6.03 &#x00B1; 1.07 m/s after BP-normalization (<italic>p</italic> = 0.47). The mechanistic normalization of cPWV was in agreement with that estimated by analysis of covariance (ANCOVA). In conclusion, the proposed method, which could be easily implemented in the clinical setting, allows to assess the intersubject differences in PWV independently of BP. Our results suggested that mild hypertension in middle-aged subjects without target organ damage does not significantly alter the stiffness of the CCA wall independently of acute differences in BP. The results warrant further clinical investigations to establish the potential clinical utility of the method.</p>
</abstract>
<kwd-group>
<kwd>pressure-independent PWV</kwd>
<kwd>hypertension</kwd>
<kwd>arterial stiffness</kwd>
<kwd>common carotid arteries</kwd>
<kwd>blood pressure</kwd>
</kwd-group>
<contract-num rid="cn001">Innovative Medicines Initiative (IMI-EU) grant "Surrogate markers for Micro- and Macro-vascular hard endpoints for innovative diabetes tools: SUMMIT".</contract-num>
<contract-sponsor id="cn001">Innovative Medicines Initiative <named-content content-type="fundref-id">10.13039/501100010767</named-content></contract-sponsor>
<contract-sponsor id="cn002">Addenbrooke's Charitable Trust, Cambridge University Hospitals <named-content content-type="fundref-id">10.13039/501100002927</named-content></contract-sponsor>
<counts>
<fig-count count="4"/>
<table-count count="2"/>
<equation-count count="13"/>
<ref-count count="49"/>
<page-count count="10"/>
<word-count count="7641"/>
</counts>
</article-meta>
</front>
<body>
<sec id="S1" sec-type="intro">
<title>Introduction</title>
<p>Arterial stiffness as pulse wave velocity (PWV) is a powerful predictor of mortality and cardiovascular events in hypertensive patients, above and beyond traditional risk factors (<xref ref-type="bibr" rid="B5">Boutouyrie et al., 2002</xref>; <xref ref-type="bibr" rid="B27">Laurent et al., 2003</xref>; <xref ref-type="bibr" rid="B9">Cardoso et al., 2019</xref>). The arterial wall, however, presents a complex microstructure where different wall constituents, mainly collagen, elastin, and smooth muscle, play different but equally important roles in arterial function (<xref ref-type="bibr" rid="B4">Boutouyrie et al., 1998</xref>; <xref ref-type="bibr" rid="B11">Cruickshank et al., 2002</xref>; <xref ref-type="bibr" rid="B24">Krasny et al., 2017</xref>; <xref ref-type="bibr" rid="B21">Giudici et al., 2021e</xref>). The heterogeneous microstructure of the arterial wall makes its behavior highly nonlinear (<xref ref-type="bibr" rid="B18">Giudici et al., 2021b</xref>) so that arterial stiffness and, consequently, PWV are intrinsically blood pressure (BP)-dependent (<xref ref-type="bibr" rid="B43">Spronck et al., 2015b</xref>). This fact complicates distinguishing between chronic (i.e., actual BP-induced wall remodeling) and acute effects (i.e., transitional shift to a different working point in the nonlinear behavior of the arterial wall) of increased BP on arterial structure and mechanics. Most clinical studies address the issue of the BP-dependency of PWV <italic>via</italic> statistical methods, using BP as a confounding factor for PWV (<xref ref-type="bibr" rid="B12">Desamericq et al., 2015</xref>; <xref ref-type="bibr" rid="B13">Diaz et al., 2018</xref>; <xref ref-type="bibr" rid="B46">Valbusa et al., 2019</xref>). However, statistical methods suffer some limitations: (1) they lack subject specificity and, hence, are less likely to be used in clinical practice, (2) they may fail to discriminate between acute and chronic effects of increased BP on the wall stiffness (<xref ref-type="bibr" rid="B39">Spronck, 2021</xref>), and (3) the choice of the normalizing pressure, i.e., the subject-specific pressure level to be used as the confounder in multivariate analysis, is not trivial and largely affects the size of the correction itself (<xref ref-type="bibr" rid="B17">Giudici et al., 2021a</xref>). While, in clinical investigations, statistical adjustments for systolic BP (SBP) (<xref ref-type="bibr" rid="B46">Valbusa et al., 2019</xref>), mean BP (MBP) (<xref ref-type="bibr" rid="B12">Desamericq et al., 2015</xref>), and pulse pressure (PP) (<xref ref-type="bibr" rid="B7">Brandts et al., 2012</xref>) are often made, most regional PWV metrics (e.g., carotid-femoral and brachial-ankle PWV), use the foot of arterial waves as the fiducial point, suggesting that diastolic BP (DBP) likely represent a more appropriate choice for their pressure-normalization (<xref ref-type="bibr" rid="B41">Spronck et al., 2017b</xref>). As intergroup differences in SBP are typically larger than those in DBP, widely used SBP- and MBP-statistical adjustments likely lead to overcorrections of PWV and potentially limit our understanding of pressure-induced chronic vascular damage (<xref ref-type="bibr" rid="B41">Spronck et al., 2017b</xref>).</p>
<p>In the past two decades, researchers have attempted to address the BP-dependency of PWV using mechanistic approaches that rely chiefly on the assumption that, in the physiological pressure range, the pressure (<italic>P</italic>)-area (<italic>A</italic>)/diameter (<italic>D</italic>) relationship of arteries resembles an exponential function (<xref ref-type="bibr" rid="B15">Gavish and Izzo, 2016</xref>). If the fitting exponential function is opportunely formulated, its constant can be used as a BP-normalized index of arterial stiffness (<xref ref-type="bibr" rid="B40">Spronck et al., 2017a</xref>; <xref ref-type="bibr" rid="B17">Giudici et al., 2021a</xref>). In 2006, Shirai et al. introduced the cardio-ankle vascular index (CAVI) that uses the heart-to-ankle PWV (haPWV), a regional PWV metric quantifying the average properties of the entire heart-to-ankle arterial pathway, to estimate Kawasaki&#x2019;s stiffness index &#x03B2;, defining the exponential relationship between <italic>P</italic> and <italic>D</italic>. A decade later, however, <xref ref-type="bibr" rid="B40">Spronck et al. (2017a)</xref> raised concerns related to the actual (in)dependency of CAVI from BP at the time of measurement, due to the inherent dependency of &#x03B2; from the subject-specific DBP. They proposed a revised metric CAVI<sub>0</sub> that relies on Hayashi&#x2019;s stiffness index &#x03B2;<sub>0</sub>, which, unlike &#x03B2;, is defined with respect to a standardized reference pressure (<italic>P</italic><sub>ref</sub>). Furthermore, CAVI and CAVI<sub>0</sub> differ also in the normalizing pressure used to estimate &#x03B2; from haPWV, raising once more the question of which is the most appropriate pressure level for the normalization of PWV metrics (<xref ref-type="bibr" rid="B17">Giudici et al., 2021a</xref>).</p>
<p>Similar methods have been devised to correct local PWV estimates, which, unlike regional PWVs, provide information on the stiffness of a specific location of the arterial tree. <xref ref-type="bibr" rid="B42">Spronck et al. (2015a)</xref> used the exponential <italic>P-A</italic> relationship proposed by <xref ref-type="bibr" rid="B31">Meinders and Hoeks (2004)</xref> to effectively predict the changes in local carotid PWV (cPWV), estimated <italic>via</italic> a linearized Bramwell-Hill equation (<xref ref-type="bibr" rid="B6">Bramwell et al., 1923</xref>), associated with the BP lowering achieved with 3-months of antihypertensive treatment in hypertensive patients. A considerably more complex approach was proposed by <xref ref-type="bibr" rid="B29">Ma et al. (2018)</xref> who used Fung&#x2019;s exponential hyperelastic strain energy function to define the relationship between BP and local PWV. While undoubtedly elegant, this approach is unlikely to be used in clinical practice due to the difficulty in estimating subject-specific parameters for the mathematical model describing the artery behavior.</p>
<p>Using a similar mechanistic approach based on the exponential modeling of the <italic>P</italic>-<italic>A</italic> relationship of arteries (<xref ref-type="bibr" rid="B43">Spronck et al., 2015b</xref>,<xref ref-type="bibr" rid="B40">2017a</xref>), our current study analyzed differences in local cPWV between healthy controls and patients with hypertension, aiming to distinguish between acute and chronic effects of high BP on carotid function. We also aimed to compare mechanistic and statistical correction of cPWV, analyzing the impact of the choice of the normalizing pressure on the size of the correction and on inter-group differences.</p>
</sec>
<sec id="S2" sec-type="materials|methods">
<title>Materials and Methods</title>
<sec id="S2.SS1">
<title>Theoretical Background</title>
<p>Tube laws mathematically define the relationship between <italic>P</italic> and <italic>A</italic> in flexible tubes. The pressure-normalization method adopted in this study is based on the tube law proposed by <xref ref-type="bibr" rid="B31">Meinders and Hoeks (2004)</xref>:</p>
<disp-formula id="S2.E1">
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<p>where <italic>D</italic> is the luminal diameter (<italic>A</italic> is assumed to be circular, <italic>A</italic> = &#x03C0;<italic>D</italic><sup>2</sup>/4), <italic>P</italic><sub>ref</sub> is a reference pressure, <italic>D</italic><sub>ref</sub> is the diameter at <italic>P</italic><sub>ref</sub>, and &#x03B3;<sub>0</sub> is an index of arterial stiffness defining the exponential relationship between <italic>P</italic> and <italic>D</italic><sup>2</sup>. Note that identical <italic>P</italic>-<italic>D</italic><sup>2</sup> relationships can be obtained with opportunely different combinations of <italic>P</italic><sub>ref</sub>, <italic>D</italic><sub>ref</sub>, and &#x03B3;<sub>0</sub> (<xref ref-type="bibr" rid="B17">Giudici et al., 2021a</xref>). Eq. 1 represents a generalized form of the tube law proposed by Meinders and Hoeks who chose <italic>P</italic><sub>ref</sub> = DBP. While <italic>P</italic><sub>ref</sub> does not have any physiological meaning and its choice is arbitrary, fixing <italic>P</italic><sub>ref</sub> to a constant value makes &#x03B3;<sub>0</sub> a pressure-normalized index of arterial stiffness. Following previous studies (<xref ref-type="bibr" rid="B17">Giudici et al., 2021a</xref>; <xref ref-type="bibr" rid="B47">van der Bruggen et al., 2021</xref>), we chose <italic>P</italic><sub>ref</sub> = 100 mmHg. This value represents the most commonly established value for mean pressure of healthy adults and allows direct comparison with previous studies.</p>
<p>The Bramwell-Hill equation (<xref ref-type="bibr" rid="B6">Bramwell et al., 1923</xref>), defining the relationship between arterial distensibility and local PWV, suggests that PWV at a given pressure level <italic>P</italic><sub><italic>c</italic></sub> can be expressed as a function of the slope of the tangent to the <italic>P</italic>-<italic>D</italic><sup>2</sup> relationship at <italic>P</italic><sub><italic>c</italic></sub>.</p>
<disp-formula id="S2.E2">
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<p>where &#x03C1; is the blood density, here assumed as 1,060 kg/m<sup>3</sup>. Using Eq. 1 to determine the derivative term in Eq. 2 and rearranging using Eq. 1 leads to the following relationship between PWV and &#x03B3;<sub>0</sub>, as previously demonstrated (<xref ref-type="bibr" rid="B20">Giudici et al., 2021d</xref>) (refer to Eqs A1&#x2013;A7 in <xref ref-type="app" rid="S11">Appendix</xref> for the detailed calculations):</p>
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<p>Eq. 3 indicates that PWV at any <italic>P</italic><sub><italic>c</italic></sub> can be directly estimated using &#x03B3;<sub>0</sub> and <italic>P</italic><sub>ref</sub>.</p>
<p>Let us define a target pressure <italic>P</italic><sub>T</sub> as the pressure level to which normalization is required. Given that PWV was measured at the pressure <italic>P</italic><sub><italic>c</italic></sub> [i.e., PWV(<italic>P</italic><sub><italic>c</italic></sub>)], the pressure change used to normalize PWV(<italic>P</italic><sub><italic>c</italic></sub>) is determined as the difference between the two pressure levels: <italic>P</italic><sub>T</sub>&#x2013;<italic>P</italic><sub><italic>c</italic></sub>. Following from Eq. 3, PWV at <italic>P</italic><sub>T</sub> can be determined as follows:</p>
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<label>(4)</label>
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<p>By combining Eq. 3 and 4, we obtain as follows:</p>
<disp-formula id="S2.E5">
<label>(5)</label>
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<p>Eq. 5 allows us to convert PWV at pressure <italic>P</italic><sub><italic>c</italic></sub> to the desired target pressure <italic>P</italic><sub>T</sub>. We noted that <italic>P</italic><sub><italic>c</italic></sub> is generally unknown and depends on the choice of the method used to estimate PWV. However, if &#x03B3;<sub>0</sub> is known, <italic>P</italic><sub><italic>c</italic></sub> for any PWV estimation method can be numerically estimated by solving Eq. 3.</p>
</sec>
<sec id="S2.SS2">
<title>Study Population and Data Acquisition</title>
<p>The study sample came from individuals undergoing standard outpatient cardiovascular risk assessment at the Pisa University Hospital (Pisa, Italy), omitting anyone with carotid atherosclerotic plaque, diabetes, and history of major cardiovascular events, atrial fibrillation, malignancy, or chronic inflammatory disease. Hypertension was defined as brachial SBP (SBP<sub>b</sub>) &#x003E; 140 mmHg and/or DBP &#x003E; 90 mmHg or based on active antihypertensive treatment. The final study population included <italic>n</italic> = 22 healthy normotensive controls and <italic>n</italic> = 22 patients with mild-to-moderate (or Grade 1&#x2013;2) hypertension (<xref ref-type="bibr" rid="B49">Williams et al., 2018</xref>), of which 41% (<italic>n</italic> = 9) were treated (treatment duration &#x003C; 1 year). The protocol of the study followed the principles of the Declaration of Helsinki and was approved by the institutional ethics committee &#x201C;Comitato Etico di Area Vasta Nord Ovest&#x201D; (reference number: 3146/2010). All subjects gave their informed consent to participate.</p>
<p>Both SBP<sub>b</sub> and DBP were measured using a digital Omron device (model 705cp, Kyoto, Japan) after subjects had rested for at least 15 min in the supine position. Then, the pressure waveform of the left common carotid artery (CCA) and the diameter waveform of the right CCA were simultaneously acquired by tonometry (PulsePen, DiaTecne, Milan, Italy; sampling frequency = 1 kHz) and ultrasound scanning (Aloka Prosound 10, Hitachi Ltd., Japan), respectively. A similar coupling of waveforms acquired at the contralateral CCAs has been performed previously to achieve correspondence in heartbeats between the pressure and diameter signals, under the assumption that hemodynamic features are similar in the two CCAs due to their similar geometrical characteristics and downstream branching (<xref ref-type="bibr" rid="B16">Giannattasio et al., 2008</xref>). The ultrasound machine was equipped with a 10.0 MHz linear array probe with radiofrequency data output at the frequency of 1 kHz. In the longitudinal right CCA view, a single scan line was aligned perpendicularly to the vessel walls, approximately 1.5 cm proximal to the carotid bulb, as reported previously (<xref ref-type="bibr" rid="B45">Uejima et al., 2019</xref>). The cursors were then placed by the experienced operator at the anterior and posterior carotid walls to enable wall tracking. PulsePen recordings were calibrated assuming constant DBP and MBP along the arterial tree. Brachial MBP was estimated from SBP<sub>b</sub> and DBP assuming a form factor of 0.43: MBP = DBP+0.43 (SBP<sub>b</sub>&#x2013;DBP) (<xref ref-type="bibr" rid="B37">Segers et al., 2009</xref>). Both acquisitions lasted for approximately 10 s, yielding 7&#x2013;10 overlapping pressure and diameter cardiac cycles to be used in the analysis. The two main peaks of the second derivatives (i.e., acceleration) of the pressure and diameter signals (identifying the foot of the wave and dicrotic notch, respectively) were used as fiducial points for the alignment of the two waveforms, as previously described (<xref ref-type="bibr" rid="B19">Giudici et al., 2021c</xref>). <xref ref-type="fig" rid="F1">Figures 1A,B</xref> provide examples of aligned left CCA pressure and right CCA diameter waveforms in a representative normotensive and hypertensive person, respectively.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption><p>Examples of left common carotid artery (CCA) pressure and right CCA diameter distension waveforms of a representative normotensive (control) person <bold>(A)</bold> and hypertensive patient <bold>(B)</bold>. Pressure and diameter waveforms were aligned using the two major peaks of their second derivative, representing the foot of the wave and the dicrotic notch, as fiducial points. In <bold>(C)</bold>, representative pressure-area (<italic>P</italic>-<italic>A</italic>) relationships were obtained by ensemble averaging pressure and diameter heartbeats [the luminal area (<italic>A</italic>) was calculated from the diameter <italic>(D)</italic> assuming a circular luminal area: <italic>A</italic> = &#x03C0;<italic>D</italic><sup>2</sup>/4]. <bold>(C)</bold> Illustrates how the exponential relationship in Eq. 1 was fitted on the measured subject-specific <italic>P</italic>-<italic>A</italic> relationships to estimate the stiffness index &#x03B3;<sub>0</sub> (notably, in reality, this was performed on a beat-to-beat basis rather than on the ensemble-averaged curves).</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fphys-12-783457-g001.tif"/>
</fig>
</sec>
<sec id="S2.SS3">
<title>Data Analysis</title>
<p>cPWV was estimated using the <italic>D</italic><sup>2</sup><italic>P</italic>-loop method (<xref ref-type="bibr" rid="B1">Alastruey, 2011</xref>), a linearization of the Bramwell-Hill equation (Eq. 2) over the late diastolic part of the <italic>P</italic>-<italic>D</italic><sup>2</sup> relationship (i.e., the diastolic decay spanning from the pressure at the dicrotic notch, <italic>P</italic><sub>notch</sub>, to DBP), as described previously (<xref ref-type="bibr" rid="B19">Giudici et al., 2021c</xref>).</p>
<disp-formula id="S2.E6">
<label>(6)</label>
<mml:math id="M6" display="block">
<mml:mtable displaystyle="true">
<mml:mtr>
<mml:mtd columnalign="center">
<mml:mrow>
<mml:mpadded width="+3.3pt">
<mml:mtext>cPWV</mml:mtext>
</mml:mpadded>
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<mml:mrow>
<mml:mfrac>
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</disp-formula>
<p>where <italic>D</italic><sub>d</sub> is the diameter at DBP, and the derivative term d<italic>P</italic>/d<italic>D</italic><sup>2</sup> indicates the slope of the linear regression of the late diastolic part of the <italic>P</italic>-<italic>D</italic><sup>2</sup> relationship.</p>
<p>As detailed in the theoretical background section, the accurate BP-normalization of cPWV requires knowledge of the pressure, <italic>P</italic><sub><italic>c</italic></sub>, that drives the BP-dependency of cPWV estimated with the <italic>D</italic><sup>2</sup><italic>P</italic>-loop method. As indicated above, the <italic>D</italic><sup>2</sup><italic>P</italic>-loop method estimates cPWV over the pressure range between <italic>P</italic><sub>notch</sub> and DBP. Therefore, the representative <italic>P</italic><sub><italic>c</italic></sub> is expected to fall within these two pressure levels. To estimate the most suitable <italic>P</italic><sub><italic>c</italic></sub> for the <italic>D</italic><sup>2</sup><italic>P</italic>-loop method, the beat-to-beat relationships between left CCA <italic>P</italic> and right CCA <italic>D</italic><sup>2</sup> were fitted using Eq. 1, as shown in <xref ref-type="fig" rid="F1">Figure 1C</xref>, to estimate &#x03B3;<sub>0</sub>. For each heartbeat, this step entailed determining the combination of &#x03B3;<sub>0</sub> and <italic>D</italic><sub>ref</sub> that minimizes the difference between the measured <italic>P</italic> waveform and that estimated using Eq. 1, given the <italic>D</italic> waveform as input. Then, the most suitable <italic>P</italic><sub><italic>c</italic></sub> was numerically determined by solving Eq. 3, given &#x03B3;<sub>0</sub> and cPWV. Notably, for each patient, the used &#x03B3;<sub>0</sub> and cPWV were the mean values of the 7&#x2013;10 simultaneously recorded heartbeats. Finally, cPWV was pressure-normalized using Eq. 5.</p>
</sec>
<sec id="S2.SS4">
<title>Statistical Analysis</title>
<p>Statistical analysis was performed using SPSS 23 (SPSS, IBM Corp., Chicago, IL, United States). Comparison of variables between the two groups was first performed using Student&#x2019;s <italic>t</italic>-test and then adjusting for potential confounders using analysis of covariance (ANCOVA). The BP-normalization of cPWV was performed using both mechanistic (Eq. 5) and statistical (ANCOVA) methods and considering four different pressure levels as normalizing pressure: (1) <italic>P</italic><sub><italic>c</italic></sub>, determined numerically by solving Eq. 3, (2) DBP, (3) MBP, and (4) SBP. The latter three pressure levels were chosen because often used as normalizing pressures in clinical studies. For each pressure level, <italic>P</italic><sub>T</sub> in Eq. 5 was set to the average <italic>P</italic><sub><italic>c</italic></sub>, DBP, MBP, or SBP across groups. Data are generally presented as average &#x00B1; standard deviation (SD). ANCOVA estimates are presented as average (95% CI). The <italic>p</italic>-value &#x003C; 0.05 was considered statistically significant.</p>
</sec>
</sec>
<sec id="S3" sec-type="results">
<title>Results</title>
<sec id="S3.SS1">
<title>Group Characteristics</title>
<p>Group characteristics are presented in <xref ref-type="table" rid="T1">Table 1</xref>. Hypertensive and control groups were matched in age and gender, but not heart rate (HR) that was on average 6 bpm higher in hypertensives (<italic>p</italic> = 0.021). Carotid SBP was, on average 17.7 mmHg higher in hypertensives than controls (<italic>p</italic> &#x003C; 0.001), while the difference in DBP was approximately half (<italic>p</italic> &#x003C; 0.01). As a result, PP was also 8.7 mmHg higher in hypertensives than controls. Average CCA diameters at SBP and DBP were slightly higher in hypertensives than controls, but differences were not significant and were reduced further after appropriate SBP and DBP adjustments [7.62 (7.23&#x2013;8.02) vs. 7.76 (7.37&#x2013;8.16) mm and 7.15 (6.77&#x2013;7.53) vs. 7.33 (6.95&#x2013;7.71) mm]. Conversely, carotid IMT and IMT/<italic>D</italic><sub>d</sub> were higher in hypertensives than controls (<italic>p</italic> = 0.005 and <italic>p</italic> = 0.058, respectively).</p>
<table-wrap position="float" id="T1">
<label>TABLE 1</label>
<caption><p>Characteristics and carotid artery dimensions of control and hypertension groups.</p></caption>
<table cellspacing="5" cellpadding="5" frame="hsides" rules="groups">
<thead>
<tr>
<td valign="top" align="left"/>
<td valign="top" align="center">Controls</td>
<td valign="top" align="center">Hypertensives</td>
<td/>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Age [years]</td>
<td valign="top" align="center">55 &#x00B1; 6</td>
<td valign="top" align="center">56 &#x00B1; 9</td>
<td valign="top" align="center"><italic>p</italic> = 0.77</td>
</tr>
<tr>
<td valign="top" align="left">Male : Females</td>
<td valign="top" align="center">13 : 9</td>
<td valign="top" align="center">13 : 9</td>
<td valign="top" align="center"><italic>p</italic> = 0.77</td>
</tr>
<tr>
<td valign="top" align="left">HR [bpm]</td>
<td valign="top" align="center">60 &#x00B1; 7</td>
<td valign="top" align="center">66 &#x00B1; 9</td>
<td valign="top" align="center"><italic>p</italic> = 0.021</td>
</tr>
<tr>
<td valign="top" align="left">SBP<sub>b</sub> [mmHg]</td>
<td valign="top" align="center">116.6 &#x00B1; 12.2</td>
<td valign="top" align="center">133.7 &#x00B1; 17.9</td>
<td valign="top" align="center"><italic>p</italic> &#x003C; 0.001</td>
</tr>
<tr>
<td valign="top" align="left">SBP [mmHg]</td>
<td valign="top" align="center">113.9 &#x00B1; 11.4</td>
<td valign="top" align="center">131.6 &#x00B1; 17.9</td>
<td valign="top" align="center"><italic>p</italic> &#x003C; 0.001</td>
</tr>
<tr>
<td valign="top" align="left">DBP [mmHg]</td>
<td valign="top" align="center">74.9 &#x00B1; 8.7</td>
<td valign="top" align="center">83.8 &#x00B1; 9.8</td>
<td valign="top" align="center"><italic>p</italic> = 0.003</td>
</tr>
<tr>
<td valign="top" align="left">MBP [mmHg]</td>
<td valign="top" align="center">92.7 &#x00B1; 9.5</td>
<td valign="top" align="center">105.1 &#x00B1; 12.2</td>
<td valign="top" align="center"><italic>p</italic> &#x003C; 0.001</td>
</tr>
<tr>
<td valign="top" align="left">PP [mmHg]</td>
<td valign="top" align="center">39.0 &#x00B1; 7.4</td>
<td valign="top" align="center">47.7 &#x00B1; 12.6</td>
<td valign="top" align="center"><italic>p</italic> = 0.009</td>
</tr>
<tr>
<td valign="top" align="left"><italic>P</italic><sub>notch</sub> [mmHg]</td>
<td valign="top" align="center">100.0 &#x00B1; 9.9</td>
<td valign="top" align="center">114.6 &#x00B1; 14.6</td>
<td valign="top" align="center"><italic>p</italic> &#x003C; 0.001</td>
</tr>
<tr>
<td valign="top" align="left"><italic>D</italic><sub>s</sub> [mm]</td>
<td valign="top" align="center">7.54 &#x00B1; 0.84</td>
<td valign="top" align="center">7.85 &#x00B1; 0.82</td>
<td valign="top" align="center"><italic>p</italic> = 0.23</td>
</tr>
<tr>
<td valign="top" align="left"><italic>D</italic><sub>d</sub> [mm]</td>
<td valign="top" align="center">7.08 &#x00B1; 0.83</td>
<td valign="top" align="center">7.40 &#x00B1; 0.81</td>
<td valign="top" align="center"><italic>p</italic> = 0.21</td>
</tr>
<tr>
<td valign="top" align="left">IMT [&#x03BC;m]</td>
<td valign="top" align="center">711 &#x00B1; 145</td>
<td valign="top" align="center">819 &#x00B1; 138</td>
<td valign="top" align="center"><italic>p</italic> = 0.005</td>
</tr>
<tr>
<td valign="top" align="left">IMT/<italic>D</italic><sub>d</sub> [&#x2013;]</td>
<td valign="top" align="center">0.101 &#x00B1; 0.017</td>
<td valign="top" align="center">0.111 &#x00B1; 0.015</td>
<td valign="top" align="center"><italic>p</italic> = 0.058</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn><p><italic>The p-values are the results of the independent Student&#x2019;s t-test.</italic></p></fn>
<fn><p><italic>D<sub>d</sub>, diastolic diameter; D<sub>s</sub>, systolic diameter; DBP, diastolic blood pressure; HR, heart rate; IMT, intima-media thickness; MBP, mean blood pressure; P<sub>notch</sub>, pressure at the dicrotic notch; PP, pulse pressure; SBP, carotid systolic blood pressure; SBP<sub>b</sub>, brachial systolic blood pressure. Data are presented as mean &#x00B1; standard deviation (SD).</italic></p></fn>
</table-wrap-foot>
</table-wrap>
<p>As expected, before accounting for BP differences, cPWV, calculated using Eq. 6, was on average 12% higher in hypertensives than controls (6.24 &#x00B1; 1.22 vs. 5.56 &#x00B1; 0.86 m/s, <italic>p</italic> &#x003C; 0.05) (<xref ref-type="fig" rid="F2">Figure 2</xref>, left, and <xref ref-type="table" rid="T2">Table 2</xref>), even after HR adjustments (<italic>p</italic> &#x003C; 0.05). However, the pressure-normalized stiffness index &#x03B3;<sub>0</sub> did not differ significantly (3.48 &#x00B1; 1.04 vs. 3.77 &#x00B1; 1.27, <italic>p</italic> = 0.41), suggesting that increased cPWV in hypertensives was likely mainly related to BP differences between groups. In fact, the average estimated <italic>P-A</italic> relationships of the two groups (<xref ref-type="fig" rid="F3">Figure 3</xref>) run almost parallel to each other and are largely superimposed, suggesting that the mechanical response of the carotid arteries in the two groups was similar.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption><p>Local carotid pulse wave velocity (cPWV) in control and hypertensive people before and after pressure-normalization using Eq. 5. Bars indicate minimum and maximum.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fphys-12-783457-g002.tif"/>
</fig>
<table-wrap position="float" id="T2">
<label>TABLE 2</label>
<caption><p>Comparison between mechanistic and statistical blood pressure adjustment of the local carotid pulse wave velocity (cPWV) using different normalizing pressures.</p></caption>
<table cellspacing="5" cellpadding="5" frame="hsides" rules="groups">
<thead>
<tr>
<td valign="top" align="left"/>
<td valign="top" align="center" colspan="2">Controls<hr/></td>
<td valign="top" align="center" colspan="2">Hypertensives<hr/></td>
</tr>
<tr>
<td valign="top" align="left"/>
<td valign="top" align="center">Mechanistic</td>
<td valign="top" align="center">Statistical</td>
<td valign="top" align="center">Mechanistic</td>
<td valign="top" align="center">Statistical</td>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Uncorrected</td>
<td valign="top" align="center" colspan="2">5.56 &#x00B1; 0.86</td>
<td valign="top" align="center" colspan="2">6.24 &#x00B1; 1.22</td>
</tr>
<tr>
<td valign="top" align="left">SBP</td>
<td valign="top" align="center">5.88 &#x00B1; 0.84</td>
<td valign="top" align="center">5.85 (5.40&#x2013;6.30)</td>
<td valign="top" align="center">5.95 &#x00B1; 0.98</td>
<td valign="top" align="center">5.95 (5.50&#x2013;6.40)</td>
</tr>
<tr>
<td valign="top" align="left">MBP</td>
<td valign="top" align="center">5.82 &#x00B1; 0.89</td>
<td valign="top" align="center">5.80 (5.34&#x2013;6.26)</td>
<td valign="top" align="center">6.00 &#x00B1; 1.00</td>
<td valign="top" align="center">6.00 (5.54&#x2013;6.46)</td>
</tr>
<tr>
<td valign="top" align="left"><italic>P</italic><sub><italic>c</italic></sub></td>
<td valign="top" align="center">5.80 &#x00B1; 0.95</td>
<td valign="top" align="center">5.77 (5.33&#x2013;6.20)</td>
<td valign="top" align="center">6.04 &#x00B1; 1.07</td>
<td valign="top" align="center">6.03 (5.54&#x2013;6.46)</td>
</tr>
<tr>
<td valign="top" align="left">DBP</td>
<td valign="top" align="center">5.80 &#x00B1; 0.94</td>
<td valign="top" align="center">5.69 (5.21&#x2013;6.17)</td>
<td valign="top" align="center">6.03 &#x00B1; 1.05</td>
<td valign="top" align="center">6.11 (5.59&#x2013;6.47)</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn><p><italic>DBP, diastolic blood pressure; MBP, mean blood pressure; P<sub>c</sub>, numerically determined local carotid PWV relevant pressure level; SBP, systolic blood pressure. Uncorrected and mechanistically corrected cPWV data are presented as mean &#x00B1; standard deviation (SD). Statistically corrected cPWV data are presented as mean (95% confidence interval).</italic></p></fn>
</table-wrap-foot>
</table-wrap>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption><p>Average estimated <italic>P</italic>-<italic>A</italic> relationships of the control and hypertensive groups. Average curves have been built by estimating &#x03B3;<sub>0</sub> for all the subjects included in the two groups. Then, the subject-specific estimated <italic>P</italic>-<italic>A</italic> relationship was built using Eq. 1 and assuming a circular luminal area (i.e., <italic>A</italic> = &#x03C0;<italic>D</italic><sup>2</sup>/4, where <italic>D</italic> is the diameter). Finally, ensemble averaging was performed between all people in each group. Solid lines indicate the average relationship, and areas delimited by dotted lines indicate &#x00B1; standard deviation (SD).</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fphys-12-783457-g003.tif"/>
</fig>
</sec>
<sec id="S3.SS2">
<title>Pressure-Normalized Carotid PWV</title>
<p><italic>P</italic><sub><italic>c</italic></sub>, estimated from cPWV and &#x03B3;<sub>0</sub> by numerically solving Eq. 3, was 87.5 &#x00B1; 10.3 in hypertensives and 78.4 &#x00B1; 10.3 in controls, corresponding approximately to DBP + 0.085 (SBP&#x2013;DBP) for both groups (<xref ref-type="fig" rid="F3">Figure 3</xref>). Notably, in both groups, <italic>P</italic><sub>notch</sub> (<xref ref-type="table" rid="T1">Table 1</xref>) was, on average, (0.65 &#x00B1; 0.10) PP above DBP. In a first BP-normalization, <italic>P</italic><sub>T</sub> was set to the average <italic>P</italic><sub><italic>c</italic></sub> across groups: 83.1 mmHg. After the BP-normalization, the difference in cPWV between the two groups reduced by 68%: 5.80 &#x00B1; 0.94 m/s in controls and 6.03 &#x00B1; 1.05 m/s in hypertensives (<italic>p</italic> = 0.47) (<xref ref-type="fig" rid="F2">Figure 2</xref>, right). In fact, except for a single hypertensive subject whose cPWV largely exceeded those of controls both before and after the pressure-normalization, all other hypertensives had normalized cPWV within the control range. Similar results were obtained when normalizing using ANCOVA with <italic>P</italic><sub><italic>c</italic></sub> as a confounder: 5.77 (5.33&#x2013;6.20) vs. 6.03 (5.59&#x2013;6.47) m/s (<italic>p</italic> = 0.41) (62% of the total cPWV difference).</p>
<p><xref ref-type="table" rid="T2">Table 2</xref> reports the comparison between the BP-normalization using Eq. 5 and ANCOVA and using <italic>P</italic><sub><italic>c</italic></sub>, SBP, MBP, and DBP as normalizing pressures. As expected, the corrections of cPWV were stronger when using higher values of normalizing pressure and, except when the normalizing pressure was set to DBP, showed good agreement between statistical and mechanistic methods. BP accounted for 90 (mechanistic) and 84% (statistical) with SBP as confounder, 75 and 69% with MBP, and 65 and 39% with DBP.</p>
</sec>
</sec>
<sec id="S4" sec-type="discussion">
<title>Discussion</title>
<p>The BP-dependency of arterial stiffness limits the ability of PWV to define changes in the mechanical properties of the arterial wall in response to cardiovascular pathologies and wall remodeling and damage (<xref ref-type="bibr" rid="B39">Spronck, 2021</xref>). This fact assumes particular relevance when evaluating changes in arterial mechanics in response to hypertension since elevated BP drives the short-term increase in PWV and potentially the long-term damage to the wall microstructure that, in turn, could result in a chronic increase in PWV. The BP-dependency of PWV has been typically addressed <italic>via</italic> statistical methods (<xref ref-type="bibr" rid="B12">Desamericq et al., 2015</xref>; <xref ref-type="bibr" rid="B46">Valbusa et al., 2019</xref>). More recently, methods that rely on the exponential modeling of the wall behavior have allowed to mathematically predict subject-specific changes in PWV in response to acute changes in BP (<xref ref-type="bibr" rid="B38">Shirai et al., 2006</xref>; <xref ref-type="bibr" rid="B40">Spronck et al., 2017a</xref>). Using a similar approach, we aimed to characterize differences in CCA stiffness between healthy controls and hypertensive patients, providing subject-specific BP-normalization of cPWV. Furthermore, we aimed to compare the mechanistic BP-normalization with that obtained using statistical methods, as well as investigate the impact of the choice of the normalizing pressure on the obtained correction. Our results indicated that BP alone accounted for 68% of the cPWV difference between groups.</p>
<p>The association between hypertension and increased PWV has long been known (<xref ref-type="bibr" rid="B44">The Reference Values for Arterial Stiffness&#x2019; Collaboration, 2010</xref>). However, understanding the causal relationships between the two is less trivial; on the one hand, studies have shown that PWV is an independent predictor of the longitudinal increase in SBP (<xref ref-type="bibr" rid="B33">Najjar et al., 2008</xref>), so that increased PWV drives the development of hypertension. On the other hand, PWV intrinsically depends on the BP level at the time of the data acquisition, and the subject-specific PWV can vary considerably in response to BP changes (<xref ref-type="bibr" rid="B43">Spronck et al., 2015b</xref>). This two-way relationship between PWV and BP complicates investigating the consequences of increased BP on arterial mechanics. Methods for the BP-normalization of PWV aim to address this issue, providing stiffness metrics that refer to a predefined reference pressure level and are, hence, independent from the BP level at the time of the measurement (<xref ref-type="bibr" rid="B40">Spronck et al., 2017a</xref>; <xref ref-type="bibr" rid="B17">Giudici et al., 2021a</xref>).</p>
<p>In this study, we analyzed differences in CCA PWV between normotensive and Grade 1&#x2013;2 hypertensive individuals. In agreement with previous studies (<xref ref-type="bibr" rid="B30">Maritz et al., 2016</xref>; <xref ref-type="bibr" rid="B34">Park et al., 2020</xref>), our results indicated that the cPWV was, in fact, higher in hypertensives than in controls at their relative working pressure: 12% difference with a 13 and 12% difference in SBP and DBP, respectively. Notably, while age and sex are key determinants of arterial stiffness (<xref ref-type="bibr" rid="B44">The Reference Values for Arterial Stiffness&#x2019; Collaboration, 2010</xref>), our studied groups were well-matched, so that these factors unlikely played a role in inter-group differences in cPWV. Our finding is in agreement with previous work (<xref ref-type="bibr" rid="B25">Laurent et al., 1994</xref>) where distensibility of the CCA at MBP was reduced by &#x223C;33% in hypertensive people compared to healthy controls but with a &#x223C;30% difference in SBP/DBP. Similar results have also been reported for regional carotid-femoral PWV (<xref ref-type="bibr" rid="B44">The Reference Values for Arterial Stiffness&#x2019; Collaboration, 2010</xref>). However, the pressure-normalization of cPWV proposed here indicated that more than two-thirds of this difference had to be imputed to BP differences between the two groups (<xref ref-type="fig" rid="F2">Figure 2</xref>) and that, in absolute terms, the CCA of hypertensive patients was not intrinsically stiffer than that of healthy people. Notably, as suggested by the Moens-Kortweg equation (<xref ref-type="bibr" rid="B32">Moens, 1878</xref>; <xref ref-type="bibr" rid="B28">Li et al., 2021</xref>), PWV quantifies the structural stiffness of an artery as a whole (i.e., including both wall material stiffness and geometrical features). As hypertensives here had a higher IMT and IMT/<italic>D</italic><sub>d</sub> ratio than controls, residual differences in PWV after pressure-normalization may, at least in part, be attributable to these structural differences, rather than pure differences in wall material properties. This finding was further confirmed by the exponential modeling of the <italic>P</italic>-<italic>A</italic> relationships, with the average hypertensive curve running almost parallel to that of controls, independently of pressure. Our findings are in agreement with seminal works of <xref ref-type="bibr" rid="B25">Laurent et al. (1994)</xref> and <xref ref-type="bibr" rid="B2">Armentano et al. (1995)</xref>, who showed that CCA distensibility-pressure relationships of controls and hypertensives are almost superimposed. These results suggest that wall stiffening in response to increased BP is mild at the CCA. It is worth considering, however, that patients in our study presented only mild-to-moderate hypertension with a relatively short time between the diagnosis of the condition and the time of the examination (&#x003C; 1 year). Therefore, it is possible that longer exposure to severely increased BP might trigger intensive remodeling and, consequently, intrinsic stiffening (i.e., BP-independent) of the carotid wall.</p>
<p>Whether accounting for the BP-dependency of PWV with statistical or mechanistic methods, the choice of the normalizing pressure has an important quantitative impact on the size of the correction. While the most widely adopted choices in clinical studies are SBP or MBP (<xref ref-type="bibr" rid="B12">Desamericq et al., 2015</xref>; <xref ref-type="bibr" rid="B46">Valbusa et al., 2019</xref>), it has been previously argued that the BP-dependency of most metrics pertaining to PWV, especially those relying on the foot-to-foot detection technique, is likely governed by DBP (i.e., the pressure at the foot of the wave) rather than either SBP or MBP (<xref ref-type="bibr" rid="B43">Spronck et al., 2015b</xref>,<xref ref-type="bibr" rid="B40">2017a</xref>; <xref ref-type="bibr" rid="B17">Giudici et al., 2021a</xref>). In this study, cPWV was estimated <italic>via</italic> linear regression of the <italic>P</italic>-<italic>D</italic><sup>2</sup> relationship in late diastole, i.e., the diastolic decay after the dicrotic notch (<xref ref-type="bibr" rid="B19">Giudici et al., 2021c</xref>). Although this phase of the cardiac cycle spanned between DBP and &#x223C;65% of the PP, our results indicated that, on average, <italic>P</italic><sub><italic>c</italic></sub> was determined for its 91.5% by DBP and only for its 8.5% by SBP (<xref ref-type="fig" rid="F4">Figure 4</xref>). We obtained similar results when estimating cPWV <italic>via</italic> the ln<italic>DU</italic>-loop method, a linear regression between blood velocity (<italic>U</italic>) and the natural logarithm of the diameter distension (ln<italic>D</italic>) in early systole (<xref ref-type="bibr" rid="B20">Giudici et al., 2021d</xref>). These findings suggest that, as regional PWV, loop methods provide nearly diastolic measures of PWV and that DBP should be regarded as the main driver of their BP-dependency. Notably, however, in this study, DBP-adjustment provided the largest difference between statistical and mechanistic methods for the cPWV correction. This result warrants caution when performing statistical DBP-adjustment of all arterial stiffness metrics that are notably <italic>purely</italic> diastolic.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption><p>Correlation between <italic>P</italic><sub><italic>c</italic></sub>, the pressure value linking cPWV to &#x03B3;<sub>0</sub>, and DBP + 0.085 (SBP-DBP). SBP, systolic blood pressure; DBP, diastolic blood pressure.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fphys-12-783457-g004.tif"/>
</fig>
<p>As other local techniques (<xref ref-type="bibr" rid="B36">Rabben et al., 2004</xref>; <xref ref-type="bibr" rid="B23">Khir and Parker, 2005</xref>; <xref ref-type="bibr" rid="B14">Feng and Khir, 2010</xref>; <xref ref-type="bibr" rid="B8">Campos Arias et al., 2019</xref>), the <italic>D</italic><sup>2</sup><italic>P</italic>-loop method (<xref ref-type="bibr" rid="B1">Alastruey, 2011</xref>) is based on the coupling of two arterial waveforms to provide an estimate of the wave speed at a single location of the arterial tree (i.e., local wave speed). In contrast, regional PWVs, such as the carotid-femoral PWV (<xref ref-type="bibr" rid="B26">Laurent et al., 2006</xref>), provide insights into the average arterial stiffness along a given wave path, which inevitably includes arteries with different wall structures. This is particularly relevant when considering that elastic and muscular arteries have shown to be affected differently by aging and disease (<xref ref-type="bibr" rid="B3">Borlotti et al., 2012</xref>). Furthermore, local methods are not affected by known limitations of regional PWVs, such as the possible inaccuracies in the estimation of the true arterial pathway length (<xref ref-type="bibr" rid="B22">Huybrechts et al., 2011</xref>; <xref ref-type="bibr" rid="B17">Giudici et al., 2021a</xref>). Finally, local arterial properties can be useful to predict damage of target organs located in the vicinity of the measurement site; for example, carotid stiffening and function have been associated with cognitive decline (<xref ref-type="bibr" rid="B10">Chiesa et al., 2019</xref>). For the aforementioned reasons, results reported here on differences in arterial wall stiffness between normotensives and hypertensives concern the carotid artery and should not be generalized to other locations or regions of the arterial tree.</p>
</sec>
<sec id="S5">
<title>Limitations</title>
<p>In this study, we assumed the existence of an exponential <italic>P</italic>-<italic>A</italic> relationship for the CCA. While it is generally accepted that the <italic>P</italic>-<italic>A</italic> relationship of arteries closely resembles an exponential function in the physiological range of pressure (<xref ref-type="bibr" rid="B15">Gavish and Izzo, 2016</xref>), the subject-specific <italic>P</italic>-<italic>A</italic> relationships might not be exactly exponential, especially in young subjects at low pressures (<xref ref-type="bibr" rid="B48">Vande Geest et al., 2004</xref>). It is therefore possible that, for some subjects, the mechanistic method failed to accurately predict the relationship between BP and cPWV. It is, however, unlikely that this has significantly affected the cPWV-normalization since similar methods showed good ability in predicting changes in both local and regional PWV, given a BP change (<xref ref-type="bibr" rid="B43">Spronck et al., 2015b</xref>; <xref ref-type="bibr" rid="B35">Pucci et al., 2020</xref>).</p>
</sec>
<sec id="S6" sec-type="conclusion">
<title>Conclusion</title>
<p>We concluded that mild hypertension does not chronically affect the stiffness of the CCA wall, at least in the middle-aged subjects without target organ damage.</p>
<p>Assuming an exponential <italic>P</italic>-<italic>A</italic> relationship, we proposed a method that allows for determining arterial stiffness, as PWV, independently of BP. The proposed method is non-invasive and provides a subject-specific normalization of PWV which could be implemented in the clinical setting. The results warrant further investigations to establish the potential clinical utility of the method.</p>
</sec>
<sec id="S7" sec-type="data-availability">
<title>Data Availability Statement</title>
<p>The raw data supporting the conclusions of this article will be made available by the authors, upon reasonable request.</p>
</sec>
<sec id="S8">
<title>Ethics Statement</title>
<p>The studies involving human participants were reviewed and approved by Comitato Etico di Area Vasta Nord Ovest (reference number: 3146/2010), Italy. The patients/participants provided their written informed consent to participate in this study.</p>
</sec>
<sec id="S9">
<title>Author Contributions</title>
<p>AG contributed to the conceptualization, data analysis, manuscript drafting, and editing. AG and AK developed the analytical method. AK, CP, JC, and MK contributed to the conceptualization, manuscript editing, and project supervision. CM contributed to the data acquisition and management. All authors contributed to the article and approved the submitted version.</p>
</sec>
<sec id="conf1" sec-type="COI-statement">
<title>Conflict of Interest</title>
<p>JC was a past president of the ARTERY (Association for Research into Arterial Structure and Physiology) society. MK was responsible for clinical studies at Esaote SpA (Genova, Italy). The remaining authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec id="pudiscl1" sec-type="disclaimer">
<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>
</body>
<back>
<sec id="S10" sec-type="funding-information">
<title>Funding</title>
<p>This study was partially supported by an Innovative Medicines Initiative (IMI-EU) grant &#x201C;Surrogate markers for Micro- and Macrovascular hard endpoints for innovative diabetes tools: SUMMIT.&#x201D; AG was supported by Addenbrooke&#x2019;s Hospital (Cambridge, United Kingdom) (Grant No. 10696100).</p>
</sec>
<sec id="S11">
<title>APPENDIX</title>
<p>The tube law proposed (Eq. 1 in the main manuscript text) by <xref ref-type="bibr" rid="B31">Meinders and Hoeks (2004)</xref> relates changes in pressure (<italic>P</italic>) to those in the cross-sectional area (assumed circular: <italic>A</italic> = &#x03C0;<italic>D</italic><sup>2</sup>/4):</p>
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<p>where <italic>P</italic><sub>ref</sub> is a reference pressure, <italic>D</italic><sub>ref</sub> is the arterial diameter at <italic>P</italic><sub>ref</sub>, and &#x03B3;<sub>0</sub> is an arterial stiffness index.</p>
<p>The Bramwell-Hill equation (<xref ref-type="bibr" rid="B6">Bramwell et al., 1923</xref>) indicates that pulse wave velocity (PWV) at a given pressure level <italic>P</italic><sub><italic>c</italic></sub> can be expressed as a function of the slope of the tangent to the <italic>P</italic>-<italic>D</italic><sup>2</sup> relationship at <italic>P</italic><sub><italic>c</italic></sub>.</p>
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<p>where &#x03C1;=1,060 kg/m<sup>3</sup> is the blood density.</p>
<p>Given Eq. A1, the derivative term in Eq. A2 can be rewritten as follows:</p>
<disp-formula id="S11.E9">
<label>(A3)</label>
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</mml:mtable>
</mml:math>
</disp-formula>
<p>where <italic>D</italic><sub><italic>c</italic></sub> is the diameter value corresponding to the pressure level <italic>P</italic><sub><italic>c</italic></sub> [i.e., <italic>P</italic><sub><italic>c</italic></sub> = <italic>P</italic>(<italic>D</italic><sub><italic>c</italic></sub>)]. Inverting Eq. A1 to express diameter as a function of pressure leads to the following relationship:</p>
<disp-formula id="S11.E10">
<label>(A4)</label>
<mml:math id="M10" display="block">
<mml:mtable displaystyle="true">
<mml:mtr>
<mml:mtd columnalign="center">
<mml:mrow>
<mml:mrow>
<mml:mpadded width="+3.3pt">
<mml:mi>D</mml:mi>
</mml:mpadded>
<mml:mo rspace="5.8pt">=</mml:mo>
<mml:mrow>
<mml:msub>
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</mml:mrow>
</mml:mtd>
</mml:mtr>
</mml:mtable>
</mml:math>
</disp-formula>
<p>so that <italic>D</italic><sub><italic>c</italic></sub> becomes as follows:</p>
<disp-formula id="S11.E11">
<label>(A5)</label>
<mml:math id="M11" display="block">
<mml:mtable displaystyle="true">
<mml:mtr>
<mml:mtd columnalign="center">
<mml:mrow>
<mml:mrow>
<mml:mpadded width="+3.3pt">
<mml:msub>
<mml:mi>D</mml:mi>
<mml:mi>c</mml:mi>
</mml:msub>
</mml:mpadded>
<mml:mo rspace="5.8pt">=</mml:mo>
<mml:mrow>
<mml:mpadded width="+1.7pt">
<mml:msub>
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<mml:mrow>
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</mml:mtable>
</mml:math>
</disp-formula>
<p>Substituting Eq. A5 in Eq. A3 yields as follows:</p>
<disp-formula id="S11.E12">
<label>(A6)</label>
<mml:math id="M12" display="block">
<mml:mtable displaystyle="true">
<mml:mtr>
<mml:mtd columnalign="center">
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</mml:mtable>
</mml:math>
</disp-formula>
<p>Replacing the derivative in Eq. A1 with Eq. A6 and rearranging using Eq. A5 then leads to Eq. A7 (corresponding to Eq. 3 in the main manuscript text):</p>
<disp-formula id="S11.E13">
<label>(A7)</label>
<mml:math id="M13" display="block">
<mml:mtable displaystyle="true">
<mml:mtr>
<mml:mtd columnalign="center">
<mml:mrow>
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</mml:mtr>
</mml:mtable>
</mml:math>
</disp-formula>
</sec>
<ref-list>
<title>References</title>
<ref id="B1"><citation citation-type="journal"><person-group person-group-type="author"><name><surname>Alastruey</surname> <given-names>J.</given-names></name></person-group> (<year>2011</year>). <article-title>Numerical assessment of time-domain methods for the estimation of local arterial pulse wave speed</article-title>. <source><italic>J. Biomech.</italic></source> <volume>44</volume> <fpage>885</fpage>&#x2013;<lpage>891</lpage>.</citation></ref>
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