Permeability in the Mushy Zone

2010 ◽  
Vol 649 ◽  
pp. 399-408 ◽  
Author(s):  
R.G. Erdmann ◽  
D.R. Poirier ◽  
A.G. Hendrick

When modeled at macroscopic length scales, the complex dendritic network in the solid-plus-liquid region of a solidifying alloy (the “mushy zone”) has been modeled as a continuum based on the theory of porous media. The most important property of a porous medium is its permeability, which relates the macroscopic pressure gradient to the throughput of fluid flow. Knowledge of the permeability of the mushy zone as a function of the local volume-fraction of liquid and other morphological parameters is thus essential to successfully modeling the flow of interdendritic liquid during alloy solidification. In current continuum models, the permeability of the mushy zone is given as a deterministic function of (1) the local volume fraction of liquid and (2) a characteristic length scale such as the primary dendrite arm spacing or the reciprocal of the specific surface area of the solid-liquid interface. Here we first provide a broad overview of the experimental data, mesoscale numerical flow simulations, and resulting correlations for the deterministic permeability of both equiaxed and columnar mushy zones. A extended view of permeability in mushy zones which includes the stochastic nature of permeability is discussed. This viewpoint is the result of performing extensive numerical simulations of creeping flow through random microstructures. The permeabilities obtained from these simulations are random functions with spatial autocorrelation structures, and variations in the local permeability are shown to have dramatic effects on the flow patterns observed in such microstructures. Specifically, it is found that “lightning-like” patterns emerge in the fluid velocity and that the flows in such geometries are strongly sensitive to small variations in the solid structure. We conclude with a comparison of deterministic and stochastic permeabilities which suggests the importance of incorporating stochastic descriptions of the permeability of the mushy zone in solidification modeling.


1990 ◽  
Vol 93 (5) ◽  
pp. 3452-3459 ◽  
Author(s):  
Binglin Lu ◽  
S. Torquato


2020 ◽  
Vol 24 (2 Part B) ◽  
pp. 1251-1260 ◽  
Author(s):  
Ahmed Zeeshan ◽  
Mubashir Bhatti ◽  
Nouman Ijaz ◽  
Osman Bég ◽  
Ali Kadir

Bio-inspired pumping systems exploit a variety of mechanisms including peristalsis to achieve more efficient propulsion. Non-conducting, uniformly dispersed, spherical nanosized solid particles suspended in viscoelastic medium forms a complex working matrix. Electromagnetic pumping systems often employ complex working fluids. A simulation of combined electromagnetic bio-inspired propulsion is observed in the present article. Currents formation has increasingly more applications in mechanical and medical industry. A mathematical study is conducted for MHD pumping of a bi-phase nanofluid coupled with heat transfer in a planar channel. Two-phase model is employed to separately identity the effects of solid nanoparticles. Base fluid employs Jeffery?s model to address viscoelastic characteristics. The model is simplified using long wavelength and creeping flow approximations. The formulation is taken to wave frame and non-dimensionalise the equations. The resulting boundary value problem is solved analytically, and exact expressions are derived for the fluid velocity, particulate velocity, fluid-particle temperature, fluid and particulate volumetric flow rates, axial pressure gradient and pressure rise. The influence of volume fraction density, Prandtl number, Hartmann number, Eckert number, and relaxation time on flow and thermal characteristics is evaluated in detail. The axial flow is accelerated with increasing relaxation time and greater volume fraction whereas it is decelerated with greater Hartmann number. Both fluid and particulate temperature are increased with increment in Eckert and Prandtl numbers, whereas it is reduced when the volume fraction density increases. With increasing Hartmann number pressure rise is reduced



NeuroImage ◽  
2018 ◽  
Vol 179 ◽  
pp. 275-287 ◽  
Author(s):  
Santiago Coelho ◽  
Jose M. Pozo ◽  
Marina Costantini ◽  
J. Robin Highley ◽  
Meghdoot Mozumder ◽  
...  


1998 ◽  
Vol 09 (08) ◽  
pp. 1361-1371 ◽  
Author(s):  
B. Wachmann ◽  
S. Schwarzer ◽  
K. Höfler

Two-phase continuum descriptions of the dynamical behavior of particulate suspensions require, among others, the formulation of a "local drag law". Such a "law" specifies the mean force fl on particles as a function of averaged local properties, most notably, the mean difference velocity [Formula: see text] of particles and fluid and the local volume fraction Φl. The subscript l shall indicate the dependence of these quantities on the size l of the averaging cell. We study fl by direct numerical simulation, solving the incompressible Navier–Stokes equation on a fixed, regular grid on a scale much smaller than the particle diameter. The particle–fluid interaction is computed by a method similar to the one proposed in [Fogelson and Peskin J. Comp. Phys.79, 50 (1988)]. We find a relation similar to the law of Richardson & Zaki, [Formula: see text], which relates the local phase difference velocity to the local volume fraction of the particles.



1997 ◽  
Vol 106 (7) ◽  
pp. 2741-2751 ◽  
Author(s):  
J. Quintanilla ◽  
S. Torquato


1995 ◽  
Vol 34 (9) ◽  
pp. 3154-3158 ◽  
Author(s):  
Costas Tsouris ◽  
Michael A. Norato ◽  
Lawrence L. Tavlarides


2010 ◽  
Vol 26 (8) ◽  
pp. 962-967 ◽  
Author(s):  
M. Kobayashi ◽  
Y. Dorce ◽  
H. Toda ◽  
H. Horikawa




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