Flow Profile Distribution in Narrow Annuli Using Modified Yield Power-Law Fluid Model

ICIPEG 2014 ◽  
2015 ◽  
pp. 209-217
Author(s):  
T. N. Ofei ◽  
S. Irawan ◽  
W. Pao
2013 ◽  
Vol 14 (2) ◽  
pp. 73
Author(s):  
Riri Jonuarti

Simulation of blood flow behaviour in the arteries and in arterial stenosis has been made and will be discussed in this paper. This simulation uses pulsatile flow and blood flow in artery without stenosis is considered as a dynamic fluid, compressed and condensed. Whereas, in the case of arterial stenosis has been used Casson and Power-law fluid models. In the arteries without stenosis, blood flow velocity profiles show the same pattern for each Womersley number, but with different speed value. In the case of arterial stenosis, blood flow rate decreases with increasing stenosis position away from axis of blood vessels. Resistances to flow are increases with increasing the size (height and length) of stenosis, both for the Casson and Power-law fluid models. If resistance to flow increases, it is more difficult for the blood to pass through an artery, result the flow decreases and heart has to work harder to maintain adequate circulation.Keywords : Artery, blood flow, power-law fluid, Casson fluid, stenosis  


2011 ◽  
Vol 217 (17) ◽  
pp. 7108-7116 ◽  
Author(s):  
S. Nadeem ◽  
Noreen Sher Akbar ◽  
Awatif A. Hendi ◽  
T. Hayat

2006 ◽  
Vol 39 (11) ◽  
pp. 1474-1481 ◽  
Author(s):  
Hsiao-Ming Chu ◽  
Wang-Long Li ◽  
Yuh-Ping Chang

Author(s):  
Saeed Islam ◽  
Kamran Nazir Memon ◽  
Abdul Majeed Siddiqui ◽  
Syed Feroz Shah

This paper investigates the tank drainage problem of an isothermal, unsteady, incompressible electrically conducting Power law fluid. Analytic solution have been obtained from governing continuity and momentum equations subject to appropriate boundary conditions by using Perturbation method. The Power law fluid model solution without MHD is retrieved from this proposed model on substitution . Declaration on behalf of velocity profile, volume flux, average velocity, connection of time with respect to length of the tank and requirement of time for whole drainage of fluid are acquired. Special effects of numerous emerging parameter’s on velocity profile vz and depth of the fluid in the tank are graphically presented. Keywords: Tank drainage, Power law MHD fluid, Analytical solution.


2014 ◽  
Vol 93 (1) ◽  
pp. 150-165 ◽  
Author(s):  
Titus Ntow Ofei ◽  
Sonny Irawan ◽  
William Pao ◽  
Reza Ettehadi Osgouei

2015 ◽  
Vol 39 (3) ◽  
pp. 547-556 ◽  
Author(s):  
Li-Ming Chu ◽  
Hsiang-Chen Hsu ◽  
Chia-Hsiang Su

The modified Reynolds equation for power-law fluid is derived from the viscous adsorption theory for thin film elastohydrodynamic lubrication (TFEHL) of circular contacts. The lubricating film between solid surfaces is modeled as three fixed layers, which are two adsorption layers on each surface and a middle layer. The differences between classical EHL and TFEHL with power-law lubricants are discussed. Results show that the TFEHL power law model can reasonably calculate the pressure distribution, the film thickness, and the velocity distribution. The thickness and viscosity of the adsorption layer and the flow index significantly influence the lubrication characteristics of the contact conjunction.


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