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    Physiological Flow Simulation in Residual Human Stenoses After Coronary Angioplasty

    Source: Journal of Biomechanical Engineering:;2000:;volume( 122 ):;issue: 004::page 310
    Author:
    Rupak K. Banerjee
    ,
    Staff Scientist
    ,
    Lloyd H. Back
    ,
    Martin R. Back
    ,
    Assistant Professor of Surgery
    ,
    Young I. Cho
    DOI: 10.1115/1.1287157
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: To evaluate the local hemodynamic implications of coronary artery balloon angioplasty, computational fluid dynamics (CFD) was applied in a group of patients previously reported by [Wilson et al. (1988), 77 , pp. 873–885] with representative stenosis geometry post-angioplasty and with measured values of coronary flow reserve returning to a normal range (3.6±0.3). During undisturbed flow in the absence of diagnostic catheter sensors within the lesions, the computed mean pressure drop Δp̃ was only about 1 mmHg at basal flow, and increased moderately to about 8 mmHg for hyperemic flow. Corresponding elevated levels of mean wall shear stress in the midthroat region of the residual stenoses, which are common after angioplasty procedures, increased from about 60 to 290 dynes/cm2 during hyperemia. The computations (R̃ee≃100–400;αe=2.25) indicated that the pulsatile flow field was principally quasi-steady during the cardiac cycle, but there was phase lag in the pressure drop−mean velocity (Δp−ū) relation. Time-averaged pressure drop values, Δp̃, were about 20 percent higher than calculated pressure drop values, Δps, for steady flow, similar to previous in vitro measurements by Cho et al. (1983). In the throat region, viscous effects were confined to the near-wall region, and entrance effects were evident during the cardiac cycle. Proximal to the lesion, velocity profiles deviated from parabolic shape at lower velocities during the cardiac cycle. The flow field was very complex in the oscillatory separated flow reattachment region in the distal vessel where pressure recovery occurred. These results may also serve as a useful reference against catheter-measured pressure drops and velocity ratios (hemodynamic endpoints) and arteriographic (anatomic) endpoints post-angioplasty. Some comparisons to previous studies of flow through stenoses models are also shown for perspective purposes. [S0148-0731(00)00304-6]
    keyword(s): Flow (Dynamics) , Shear (Mechanics) , Vessels , Pressure , Pressure drop , Stress , Cycles , Measurement , Shapes AND Flow simulation ,
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      Physiological Flow Simulation in Residual Human Stenoses After Coronary Angioplasty

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    http://yetl.yabesh.ir/yetl1/handle/yetl/123346
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    • Journal of Biomechanical Engineering

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    contributor authorRupak K. Banerjee
    contributor authorStaff Scientist
    contributor authorLloyd H. Back
    contributor authorMartin R. Back
    contributor authorAssistant Professor of Surgery
    contributor authorYoung I. Cho
    date accessioned2017-05-09T00:01:51Z
    date available2017-05-09T00:01:51Z
    date copyrightAugust, 2000
    date issued2000
    identifier issn0148-0731
    identifier otherJBENDY-25902#310_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/123346
    description abstractTo evaluate the local hemodynamic implications of coronary artery balloon angioplasty, computational fluid dynamics (CFD) was applied in a group of patients previously reported by [Wilson et al. (1988), 77 , pp. 873–885] with representative stenosis geometry post-angioplasty and with measured values of coronary flow reserve returning to a normal range (3.6±0.3). During undisturbed flow in the absence of diagnostic catheter sensors within the lesions, the computed mean pressure drop Δp̃ was only about 1 mmHg at basal flow, and increased moderately to about 8 mmHg for hyperemic flow. Corresponding elevated levels of mean wall shear stress in the midthroat region of the residual stenoses, which are common after angioplasty procedures, increased from about 60 to 290 dynes/cm2 during hyperemia. The computations (R̃ee≃100–400;αe=2.25) indicated that the pulsatile flow field was principally quasi-steady during the cardiac cycle, but there was phase lag in the pressure drop−mean velocity (Δp−ū) relation. Time-averaged pressure drop values, Δp̃, were about 20 percent higher than calculated pressure drop values, Δps, for steady flow, similar to previous in vitro measurements by Cho et al. (1983). In the throat region, viscous effects were confined to the near-wall region, and entrance effects were evident during the cardiac cycle. Proximal to the lesion, velocity profiles deviated from parabolic shape at lower velocities during the cardiac cycle. The flow field was very complex in the oscillatory separated flow reattachment region in the distal vessel where pressure recovery occurred. These results may also serve as a useful reference against catheter-measured pressure drops and velocity ratios (hemodynamic endpoints) and arteriographic (anatomic) endpoints post-angioplasty. Some comparisons to previous studies of flow through stenoses models are also shown for perspective purposes. [S0148-0731(00)00304-6]
    publisherThe American Society of Mechanical Engineers (ASME)
    titlePhysiological Flow Simulation in Residual Human Stenoses After Coronary Angioplasty
    typeJournal Paper
    journal volume122
    journal issue4
    journal titleJournal of Biomechanical Engineering
    identifier doi10.1115/1.1287157
    journal fristpage310
    journal lastpage320
    identifier eissn1528-8951
    keywordsFlow (Dynamics)
    keywordsShear (Mechanics)
    keywordsVessels
    keywordsPressure
    keywordsPressure drop
    keywordsStress
    keywordsCycles
    keywordsMeasurement
    keywordsShapes AND Flow simulation
    treeJournal of Biomechanical Engineering:;2000:;volume( 122 ):;issue: 004
    contenttypeFulltext
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