Abstract:In 1940's, Schultz-Grunow proposed that time-average value of friction factor, λ u,ta was similar to its corresponding steady state value, λ for the presence of gradual and slow oscillations in pulsatile flows. A recent approach was available for low frequency pulsatile flows through narrow channels in transitional and turbulent regimes by Zhuang et al, in 2016 and 2017. In this analysis; extensive experimental data of , in fully laminar and turbulent sinusoidal flow are processed in the measured time-average … Show more
“…Figure 5 shows the velocity comparisons between the Womersley velocity profile (shown in solid line) and the Poiseuille function profile (indicated with dots) in different sections (denoted with A, B, C, D, and E) for different times relating to the cardiac cycle defined with Equation (8). Based on pure observation, the results clearly show that there is no evident difference between the two studied velocity profiles.…”
Section: Case Studymentioning
confidence: 88%
“…Figure 5 shows the velocity comparisons between t (shown in solid line) and the Poiseuille function profile (in sections (denoted with A, B, C, D, and E) for different tim defined with Equation (8). Based on pure observation, the is no evident difference between the two studied velocity p Second-order numerical schemes for spatial and temporal discretization have been selected.…”
Section: Case Studymentioning
confidence: 99%
“…Since then, the Womersley function has been widely used in hemodynamics. In the context of computational fluid dynamics modelization of arteries and blood vessels, several works employ the Womersley function in the inlet velocity boundary condition (see [2][3][4][5][6][7][8][9]).…”
As it is known, the Womersley function models velocity as a function of radius and time. It has been widely used to simulate the pulsatile blood flow through circular ducts. In this context, the present study is focused on the introduction of a simple function as an approximation of the Womersley function in order to evaluate its accuracy. This approximation consists of a simple quadratic function, suitable to be implemented in most commercial and non-commercial computational fluid dynamics codes, without the aid of external mathematical libraries. The Womersley function and the new function have been implemented here as boundary conditions in OpenFOAM ESI software (v.1906). The discrepancy between the obtained results proved to be within 0.7%, which fully validates the calculation approach implemented here. This approach is valid when a simplified analysis of the system is pointed out, in which flow reversals are not contemplated.
“…Figure 5 shows the velocity comparisons between the Womersley velocity profile (shown in solid line) and the Poiseuille function profile (indicated with dots) in different sections (denoted with A, B, C, D, and E) for different times relating to the cardiac cycle defined with Equation (8). Based on pure observation, the results clearly show that there is no evident difference between the two studied velocity profiles.…”
Section: Case Studymentioning
confidence: 88%
“…Figure 5 shows the velocity comparisons between t (shown in solid line) and the Poiseuille function profile (in sections (denoted with A, B, C, D, and E) for different tim defined with Equation (8). Based on pure observation, the is no evident difference between the two studied velocity p Second-order numerical schemes for spatial and temporal discretization have been selected.…”
Section: Case Studymentioning
confidence: 99%
“…Since then, the Womersley function has been widely used in hemodynamics. In the context of computational fluid dynamics modelization of arteries and blood vessels, several works employ the Womersley function in the inlet velocity boundary condition (see [2][3][4][5][6][7][8][9]).…”
As it is known, the Womersley function models velocity as a function of radius and time. It has been widely used to simulate the pulsatile blood flow through circular ducts. In this context, the present study is focused on the introduction of a simple function as an approximation of the Womersley function in order to evaluate its accuracy. This approximation consists of a simple quadratic function, suitable to be implemented in most commercial and non-commercial computational fluid dynamics codes, without the aid of external mathematical libraries. The Womersley function and the new function have been implemented here as boundary conditions in OpenFOAM ESI software (v.1906). The discrepancy between the obtained results proved to be within 0.7%, which fully validates the calculation approach implemented here. This approach is valid when a simplified analysis of the system is pointed out, in which flow reversals are not contemplated.
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