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Numerical Heat Transfer, Part A: Applications
An International Journal of Computation and Methodology
Volume 71, 2017 - Issue 6
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Original Articles

Three-dimensional numerical simulation of a failed coronary stent implant at different degrees of residual stenosis. Part I: Fluid dynamics and shear stress on the vascular wall

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Pages 638-652 | Received 08 Oct 2016, Accepted 20 Jan 2017, Published online: 28 Mar 2017
 

ABSTRACT

The influence of the degree of residual stenosis on the hemodynamics inside coronary arteries is investigated through three-dimensional (3D) numerical simulations. The present paper, which is the first of a series of two, focuses on the influence that the degree of residual stenosis (DOR) has on the fluid dynamics and the shear stresses acting on the stent and the artery wall. The pulsatile nature of the blood flow and its non-Newtonian features are taken into account. Four models of artery are investigated. The results show that the wall shear stress (WSS) increases monotonically, but not linearly, with the DOR.

Nomenclature

Latin=
DOR=

degree of restenosis

j=

imaginary unit

Jo=

zeroth-order Bessel function

J1=

first-order Bessel function

N=

number of harmonics

p=

static pressure, Pa

ℜ()=

real part of a complex number

Rmax=

maximum radius, m

Rmin=

minimum radius, m

Re=

Reynolds number

[S]=

rate of the strain tensor, s−1

Un=

Fourier coefficients of the pulsatile mean velocity profile

=

fluid velocity, m/s

WSS=

wall shear stress, dyne/cm2

αn=

Womersley numbers of order n

=

shear rate, s−1

ρ=

density, kg/m3

ξ = r/R=

dimensionless radial coordinate

Nomenclature

Latin=
DOR=

degree of restenosis

j=

imaginary unit

Jo=

zeroth-order Bessel function

J1=

first-order Bessel function

N=

number of harmonics

p=

static pressure, Pa

ℜ()=

real part of a complex number

Rmax=

maximum radius, m

Rmin=

minimum radius, m

Re=

Reynolds number

[S]=

rate of the strain tensor, s−1

Un=

Fourier coefficients of the pulsatile mean velocity profile

=

fluid velocity, m/s

WSS=

wall shear stress, dyne/cm2

αn=

Womersley numbers of order n

=

shear rate, s−1

ρ=

density, kg/m3

ξ = r/R=

dimensionless radial coordinate

Acknowledgments

The authors thank Dr. Leon Williams of Cranfield University for the support given with SolidWorks.

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