<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2019.78131</article-id><article-id pub-id-type="publisher-id">JAMP-94657</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  A Research Based on Hemodynamic Model for Heart-Mural Coronary Artery-Myocardial Bridge
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kun</surname><given-names>Shang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hao</surname><given-names>Ding</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>School of Medical Instrument, Shanghai University of Medicine &amp;amp; Health Sciences, Shanghai, China</addr-line></aff><pub-date pub-type="epub"><day>12</day><month>08</month><year>2019</year></pub-date><volume>07</volume><issue>08</issue><fpage>1911</fpage><lpage>1919</lpage><history><date date-type="received"><day>16,</day>	<month>July</month>	<year>2019</year></date><date date-type="rev-recd"><day>25,</day>	<month>August</month>	<year>2019</year>	</date><date date-type="accepted"><day>28,</day>	<month>August</month>	<year>2019</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  
    An experimental model for heart-mural coronary artery-myocardial bridge was established based on the theory of hemodynamics. The application of the model demonstrated that it can repeat to great extent the phenomenon of myocardial bridge compressing mural coronary artery that results in abnormal hemodynamic characteristic. The in vitro simulation experiment indicates that the anomaly of normal stress, circumferential stress and wall shear stress mainly occurs in the proximal end. As the oppression level increases, the mean proximal stress and the oscillatory value (maximum-minimum) increase obviously. The experimental model for heart-mural coronary artery-myocardial bridge provides a method to study relationship between myocardial bridge and atherosclerosis. 
  
 
</p></abstract><kwd-group><kwd>Mural Coronary Artery</kwd><kwd> Myocardial Bridge</kwd><kwd> Wall Shear Stress</kwd><kwd>  Atherosclerosis</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Muscle overlaying the mural coronary artery (MC) is termed a myocardial bridge (MB). To objectively evaluate clinical relevance of the MB, investigating the homodynamic behavior of the MC is of great significance. The previous studies, mostly considering clinical patients or experimental animals as subjects, have their limitations. For one thing, lack of systematicness. Hemodynamic parameters (MB width, degree of the MC’s compression, blood pressure, heart rate, and so on) of research objects are stochastic, which make it difficult to conduct systematic and comprehensive research [<xref ref-type="bibr" rid="scirp.94657-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.94657-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.94657-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.94657-ref4">4</xref>]. For another, the clinical research indicates that MB has certain impacts on morphology of coronary artery and haemodynamics, and the proximal end is one of the areas with high incidence of atherosclerosis (AS) [<xref ref-type="bibr" rid="scirp.94657-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.94657-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.94657-ref7">7</xref>]. As haemodynamic factors play an important part in the occurrence and development of AS, it is of significance to understand pathogenesis of AS by extensive studies on MC haemodynamics changing caused by MB, besides, studies on the relationships between the changing and AS at the proximal end, which have a potential clinical value on treatment of MB. Starting from the fact that the segments of MC proximal end is prone to development of AS, we set up a hemodynamic model for heart-mural coronary artery-myocardial bridge based on the main characteristics of MC to analyze haemodynamic mechanism for MB easily inducing AS.</p></sec><sec id="s2"><title>2. Basic Requirements for the Model</title><p>The hemodynamic model [<xref ref-type="bibr" rid="scirp.94657-ref8">8</xref>] as illustrated in <xref ref-type="fig" rid="fig1">Figure 1</xref> is a circulatory system including a heart pump, a compliance chamber, MB, phase coronary blood flow component, after-load, a reservoir, a thermostatic device and measuring devices.</p><p>Basic requirements for the model as follows:</p><p>To function as a heart outputting “blood” with hemodynamic features (pressure and wave);</p><p>Be able to simulate the MB and hemodynamic features in the case of the MB compressing MC;</p><p>Simulating the phase characteristic of blood flow in the MC―Blood flow reaches maximum during diastole and sharply decreases during systole.</p><p>The test point 1 and 2 are set about 3 cm from the segments proximal and distal to MB at which fluid are coupled with testing devices through pressure transducers. The pressure of the segments proximal and distal to MB are displayed and recorded in the real time. The mean blood flow can be read directly through graduated cylinders connected to test point 3 locating at the end of coronary arteries. By connecting a Y-shaped tube, we can insert the Doppler-flow wire into the pipeline to measure and record the flow rate where the ultrasonic detector is located.</p></sec><sec id="s3"><title>3. Experimental Design</title><p>According to the clinical parameters of normal human [<xref ref-type="bibr" rid="scirp.94657-ref9">9</xref>], we set that the systolic normal stress of coronary artery is 120 mmHg, the diastolic pressure is 80 mmHg, the mean flux is 205 mL/min, and the heart rate is 60 min<sup>−1</sup>. During systole, the MB oppresses the MC [<xref ref-type="bibr" rid="scirp.94657-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.94657-ref2">2</xref>]. Therefore, in the experiment, the systole has the same frequency with that MB compresses MC, and the maximal output pressure and the maximal deflection of MB keep synchronous. The fluid in the tube is a mixture of low molecular dextran and normal saline with a ratio of 3:1, whose viscosity is 3.8 &#215; 10<sup>−3</sup> Pa・S [<xref ref-type="bibr" rid="scirp.94657-ref3">3</xref>].</p><p>The requirement of the experimental designation:</p><p>Contrast the MC proximal and distal pressure waves of clinical MB patients with the results of the analog device;</p><p>In the case that the external pressure of coronary artery is constant, change the press situation of MB oppression MC to observe the changes of the proximal and distal normal stress, circumferential stress, and wall shear stress.</p></sec><sec id="s4"><title>4. Results</title><sec id="s4_1"><title>4.1. Performance Evaluation</title><p>The experimental results show that the model basically meets design requirements. Special attention need to be drawn:</p><p>When the segment proximal to MB is completely compressed, its Doppler imaging is similar to the Doppler imaging of MC of clinical cases both with the “fingertip phenomenon” [<xref ref-type="bibr" rid="scirp.94657-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.94657-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.94657-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.94657-ref8">8</xref>].</p><p>The pressure curve got by simulation device is very similar to that of human body [<xref ref-type="bibr" rid="scirp.94657-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.94657-ref8">8</xref>].</p></sec><sec id="s4_2"><title>4.2. The Experimental Results</title><p>1) Normal stress</p><p>Normal stress is measured by pressure sensor directly. The test point 1 is proximal pressure sensor and test point 2 is distal pressure sensor (see <xref ref-type="fig" rid="fig1">Figure 1</xref>). Based on the measured data, the curves of the mean proximal and distal normal stress with different oppression levels are shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>. As the oppression level increases, the mean proximal normal stress increases significantly, while the mean distal normal stress remains unchanged. The oscillatory value of the proximal normal stress (maximum-minimum) is obviously higher than that of the distal. Moreover, an increasing oppression level leads to an increase in the oscillatory value of proximal normal stress (see <xref ref-type="fig" rid="fig3">Figure 3</xref>).</p><p>2) Circumferential stress</p><p>The circumferential stress is obtained indirectly from the calculation of the normal stress in MC [<xref ref-type="bibr" rid="scirp.94657-ref10">10</xref>]. As the oppression level increases, the mean proximal circumferential stress increases significantly, while the mean distal circumferential stress remains unchanged (see <xref ref-type="fig" rid="fig4">Figure 4</xref>). The oscillatory value of the proximal</p><p>circumferential stress (maximum-minimum) is obviously higher than that of the distal. Moreover, an increasing oppression level leads to an increase in the oscillatory value of proximal circumferential stress (see <xref ref-type="fig" rid="fig5">Figure 5</xref>).</p><p>3) Wall shear stress</p><p>The wall shear stress can be obtained indirectly from the calculation by measuring flow velocity of tube axis [<xref ref-type="bibr" rid="scirp.94657-ref11">11</xref>]. In this paper, we use this method to calculate wall shear stress.</p><p>As the oppression level increases, the mean distal shear stress increases (<xref ref-type="fig" rid="fig6">Figure 6</xref>). The oscillatory value of the proximal shear stress (maximum-minimum) is obviously higher than that of the distal. Moreover, an increasing oppression level leads to an increase in the oscillatory value of proximal shear stress (<xref ref-type="fig" rid="fig7">Figure 7</xref>).</p></sec></sec><sec id="s5"><title>5. Discussion</title><p>The changes of the stress, which are shown in the simulation results, actually have a common mechanical background. Because the MB presses the MC in systolic, the normal hemodynamics will be changed. The oppression made by MB is an outside forced disturbance and the disturbance is the real reason to make the hemodynamics of the MC become abnormal.</p><p>From the simulation results, the MB widely influences the mean value and the oscillatory value of the stresses in the MC, including normal stresses, circumferential stresses and shear stresses. The analyses are as follows.</p><sec id="s5_1"><title>5.1. The Mean Value of the Stresses</title><p>If the MB presses the MC, with the increase in the oppression level, the mean value of normal stress and circumferential stress will both increase at the proximal end and the mean value of the shear stress will increase at the distal end. The normal stress increases because the blood kinetic energy is transformed into the pressure energy when the MB presses the MC. Because the circumferential stress is proportional to the normal stress [<xref ref-type="bibr" rid="scirp.94657-ref10">10</xref>], the circumferential stress also increases at the proximal end. The mean value of the shear stress increases due to the increase in the blood flow at the distal end when the MB presses the MC. The experimental results show that the maximum, minimum ,mean and oscillation value of proximal wall shear stress are 14.359 Pa, 0.058 Pa, 4.17 Pa and 14.301 Pa respectively when the degree of oppression is 100%, while, the maximum, minimum, mean and oscillation value of distal wall shear stress are 11.842 Pa, 0.137 Pa, 5.07 Pa and 11.705 Pa respectively. The mean shear stress value is proportional to the mean flow-rate in a cardiac cycle, so it is reasonable that proximal flow is less than distal flow in a cycle.</p></sec><sec id="s5_2"><title>5.2. The Oscillatory Value of the Stresses</title><p>If the MB presses the MC, with the increase in the oppression level, the oscillatory value of the stresses in the MC will also increase. Meanwhile the oscillatory value of normal stress, circumferential stress and shear stress at the proximal end is larger than the one at the distal end.</p><p>At the proximal end of the MC, the normal blood flow is blocked because of the press made by the MB. Then “water hammer” happens and makes the normal stress and the circumferential stress increase sharply. Also, the blocked blood flow makes the oscillatory value of shear stress increase because of the decrease in the flow at the proximal end.</p><p>By analyzing the characteristics of the proximal hemodynamic parameters of the MC, this paper aims to analyze influence of each mechanical component to the AS from the mechanics perspective.</p><p>The above experimental results show that the mean sheer stress is higher at the distal end, while the oscillation value is larger at the proximal end. If the value of mean sheer stress decide the degree of the endothelial cells damage, and then AS would happen in the distal, which is not correspond with clinical facts. On the contrary, the value of oscillation sheer stress decide the degree of the damage, and then AS happen in the proximal. So we draw a conclusion that oscillation shear stress is the main reason caused endothelial cells damage. The shear stress oscillatory makes the proximal MC be in the fatigue load situation for a long time. Besides, the increase in the proximal oscillatory value accelerates the local fatigue damage of the MC and increases the risk that the vascular endothelial cell gets damaged, which can lead to the occurrence and development of AS [<xref ref-type="bibr" rid="scirp.94657-ref12">12</xref>].</p><p>Hypertension and AS are causal relationship [<xref ref-type="bibr" rid="scirp.94657-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.94657-ref14">14</xref>]. Therefore, the increase in the proximal normal stress of the MC caused by the MB is closely related to the AS.</p><p>The increase in the mean value of the proximal circumferential stress of the MC will cause a local tensile stress concentration phenomenon, which makes the circumferential stress of the proximal area much higher than that of the surrounding area. On the other hand, the increasing oscillatory value of the circumferential stress makes the blood vessels under higher fatigue load. Since the fatigue load is sensitive to the stress concentration, it is more likely to cause a fatigue damage of the blood vessels, which is the main reason of the multifocal distribution of AS [<xref ref-type="bibr" rid="scirp.94657-ref15">15</xref>].</p><p>To sum up, the hemodynamic factors such as the normal stress, the circumferential stress and the shear stress are main reasons to cause the change in the structure and function of cells on the vascular walls [<xref ref-type="bibr" rid="scirp.94657-ref16">16</xref>]. The hemodynamic abnormality can adjust the occurrence and development of AS by the endothelial cell surface receptors, G protein, intracellular signal transduction and gene expression [<xref ref-type="bibr" rid="scirp.94657-ref17">17</xref>]. Therefore, for different stages of hemodynamic, to effectively control AS will the focus in the future research. It will also provide a new method to effectively prevent and treat cardiovascular and cerebrovascular diseases.</p><p>A new hemodynamic model is built in this paper. Based on the abnormal physiology phenomenon that the MB oppresses the MC, this device constructs several experimental modules in vitro which is close to body conditions in some point. This device not only can provide a hemodynamics environment which is more close to the human body physiological conditions, but also can provide multiparameter and controlled experimental conditions. The hemodynamic model provides an experimental environment and method to further study the relationship between the change of homodynamic environment of MC caused by MB and the proximal atherosclerotic lesion.</p></sec></sec><sec id="s6"><title>Fund</title><p>This work was supported by the Shanghai Natural Science Foundation [grant number 17ZR1413500].</p></sec><sec id="s7"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s8"><title>Cite this paper</title><p>Ding, H. and Shang, K. (2019) A Research Based on Hemodynamic Model for Heart-Mural Coronary Artery-Myocardial Bridge. 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