Morphology Drivers for Irreversible Species Diffusion and Transport in HeteroFoaMs

2019 ◽  
Vol 167 (5) ◽  
pp. 054505
Author(s):  
Kenneth Reifsnider ◽  
Ye Cao ◽  
Rassel Raihan ◽  
Vamsee Vadlamudi
Keyword(s):  
2000 ◽  
Vol 33 (9) ◽  
pp. 566-573 ◽  
Author(s):  
O. Truc ◽  
J. -P. Ollivier ◽  
L. O. Nilsson

Author(s):  
Matthias Bernhard Lierenfeld ◽  
Xin Zhong ◽  
Eric Reusser ◽  
Karsten Kunze ◽  
Benita Putlitz ◽  
...  

1998 ◽  
Vol 120 (3) ◽  
pp. 226-232 ◽  
Author(s):  
H. Teng ◽  
C. M. Kinoshita ◽  
S. M. Masutani ◽  
J. Zhou

A comprehensive equation to determine the rate of local entropy generation in multicomponent, reacting, laminar fluid flow involving heat and mass transfer is formulated based on species-average velocity in a multicomponent continuum. The entropy-generation equation developed in this study suggests that species diffusion induces a diffusive-viscous effect, heretofore not reported in the literature, which could contribute significantly to entropy generation in multicomponent fluid systems, and that entropy generation in a multicomponent system exceeds that in a single-component fluid system having similar velocity and temperature distributions because a greater number of irreversible processes, such as species diffusion, chemical reaction, and the Soret and Dufour effects, are involved. Under appropriate conditions, if the diffusive-viscous effect is neglected, the entropy-generation equation of this study reduces to those reported in the literature for simpler fluid systems based on mean flow.


In this paper, we examine the disappearance of criticality, ignition locus and bifurcation diagrams of temperature against Rayleigh number of a one-dimensional diffusion-convection-reaction model with the assumption of infinite thermal conductivity and zero species diffusivity. The predictions of this model are compared with those of the Semenov model to determine the impact of the species diffusion term. It is shown that for large values of the Rayleigh number (R* ≫ 1), the ignition locus may be expressed in a parametric form B Ls = t /ln t + t /( t - 1) (1 < t ≼ 3.4955), ψ / R * = ( B Ls ) 2 (( t - 1)/ t ) exp{ - B Ls + B Ls / t } ln t , where B is the heat of reaction parameter, ψ is the Semenov number and Ls is a (modified) Lewis number. Criticality is found to disappear at B Ls = 4.194. When these results are compared with those of the Semenov model, it is found that neglecting the species diffusion term gives conservative approximations to the ignition locus, and criticality boundary. It is found that the lumped thermal model-I has five different types of bifurcation diagrams of temperature against Rayleigh number (single­-valued, isola, inverse S , mushroom, inverse S + isola). These diagrams are qualitatively identical to the bifurcation diagrams of temperature against flow rate for the forced convection problem under the assumption of infinite thermal conductivity and zero species diffusivity.


Sign in / Sign up

Export Citation Format

Share Document