2014
DOI: 10.1016/j.compfluid.2014.03.021
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A FEM approach to biomagnetic fluid flow in multiple stenosed channels

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Cited by 18 publications
(17 citation statements)
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“…Equation 18is then discsretised using second order central difference, and substituting the relations from Equations (35) and (36), the boundary conditions for the vorticity on the lower and upper walls are then proved to be [33]…”
Section: Boundary Conditionsmentioning
confidence: 99%
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“…Equation 18is then discsretised using second order central difference, and substituting the relations from Equations (35) and (36), the boundary conditions for the vorticity on the lower and upper walls are then proved to be [33]…”
Section: Boundary Conditionsmentioning
confidence: 99%
“…In addition, ferrofluid can exhibit non-Newtonian behaviour [26][27][28][29]. However, most of the available works reported only on the effect of FHD on Newtonian fluid [2,23,[30][31][32][33][34][35][36][37][38][39][40][41][42][43]. Even if the magnetic field effect is included in power-law fluid flow, the works only used magnetic field effect of MHD [44][45][46][47][48][49].…”
Section: Introductionmentioning
confidence: 99%
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“…Tzirtzilakis [87] 拓展了生物磁流体模型, 引入了弱导电性和 能量输运, 为后续研究奠定了理论基础. Türk等人 [88] 采用有限元法, 首次模拟了生物磁流体在多种复杂 [88] ; (b) 不同Mason数下的热磁对流温 度场、流场分布 [12] Figure 9 (Color online) Simulation results of biomagnetic fluid. (a) Streamlines, vorticity contours and isotherms of biomagnetic fluid in a stenosed channel [88] ; (b) isotherms and streamlines of thermomagnetic convection for different Mason numbers [12] 应的影响还鲜有研究.…”
Section: 生物磁流体的数值模拟mentioning
confidence: 99%