逢甲學報, Band 38逢甲大學, 2000 |
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Seite 129
... thermal conductivity ratio kr with Ta = 0 , dr = 1 and B2 = 1. For kr → 0 and kr → ∞ , from equation ( 36 ) , the fluid - solid interface becomes adiabatic and isothermal respectively . For small values of the thermal conductivity ratio ...
... thermal conductivity ratio kr with Ta = 0 , dr = 1 and B2 = 1. For kr → 0 and kr → ∞ , from equation ( 36 ) , the fluid - solid interface becomes adiabatic and isothermal respectively . For small values of the thermal conductivity ratio ...
Seite 130
... thermal conductivity ratio kr and the viscosity parameter B1 , the variations of the critical Rayleigh number Rc with the thermal conductivity ratio kr are significant , compared with those of Bi = ∞ . Modes of convective instabilities ...
... thermal conductivity ratio kr and the viscosity parameter B1 , the variations of the critical Rayleigh number Rc with the thermal conductivity ratio kr are significant , compared with those of Bi = ∞ . Modes of convective instabilities ...
Seite 131
... thermal conductivity ratio kr becomes almost negligible . While , in the limiting case dr → ∞ , the hyperbolic function is equal to unit and the thermal condition primarily depends on the thermal conductivity ratio kr . For kr → 0 ...
... thermal conductivity ratio kr becomes almost negligible . While , in the limiting case dr → ∞ , the hyperbolic function is equal to unit and the thermal condition primarily depends on the thermal conductivity ratio kr . For kr → 0 ...
Inhalt
The Research of Pegging the National Annuity Insurance Premium along | 1 |
Evidence from Taiwan and The | 11 |
The Java Processors to Enhance Execution Performance | 29 |
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