## 25+(1 -L)u,=O aty2=0 dyz to determine J,, we ensure that the zero-order solution does not have a boundary layer. In other words the higher-order terms will be of the order-of s/(1 -1) and, thus, will be small. Now, condition (8) is mathematically equivalent to d2u 2 = 0 dyt at yz = 0. (9)
β¦ LIBER β¦
Self-similar problems of convective diffusion in the presence of heterogeneous chemical reactions with allowance for thermal diffusion effects
β Scribed by A. M. Suponitskii
- Publisher
- SP MAIK Nauka/Interperiodica
- Year
- 1969
- Tongue
- English
- Weight
- 178 KB
- Volume
- 7
- Category
- Article
- ISSN
- 0021-8944
No coin nor oath required. For personal study only.
π SIMILAR VOLUMES
A spline collocation method for the solu
β
M.A. Soliman
π
Article
π
1992
π
Elsevier Science
π
English
β 428 KB
Lie group analysis for thermal-diffusion
β
P. Puvi Arasu; P. Loganathan; R. Kandasamy; I. Muhaimin
π
Article
π
2011
π
Elsevier
π
English
β 416 KB
On imperfect contacting in batch heterog
β
A.E. de Gance; L.E. Johns
π
Article
π
1974
π
Elsevier Science
π
English
β 592 KB
For a certain simple class of chemical reaction networks, viz. rank E = 1, the introduction of an effective scalar diffusion coefficient allows the vector integro-differential equation describing the performance of a multicomponent batch heterogeneous chemical reaction system to be reduced to the sc
Group theory transformation for Soret an
β
R. Kandasamy; T. Hayat; S. Obaidat
π
Article
π
2011
π
Elsevier Science
π
English
β 466 KB
Lie group analysis for the effect of tem
β
Ramasamy Kandasamy; Ismoen Muhaimin; Hashim Bin Saim
π
Article
π
2010
π
Elsevier Science
π
English
β 602 KB