Modeling of Collisions |
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الصفحة 97
In the one - temperature hydrodynamics approximation , electronic and ionic thermal conductivities add up in the energy equation , but the former always prevails by far , by a factor ~ Z√mi / me . Ionic conductivity is low , as well as ...
In the one - temperature hydrodynamics approximation , electronic and ionic thermal conductivities add up in the energy equation , but the former always prevails by far , by a factor ~ Z√mi / me . Ionic conductivity is low , as well as ...
الصفحة 207
P2 = 20.1 = Existence and Uniqueness of the Thermal Equilib- rium Solution Given ɛ , > 0 ( and therefore 7 > 0 ) the existence result is : η Theorem 20.1 Assume B1 , B2 . Then for all 20 Bipolar Thermal Equilibrium .
P2 = 20.1 = Existence and Uniqueness of the Thermal Equilib- rium Solution Given ɛ , > 0 ( and therefore 7 > 0 ) the existence result is : η Theorem 20.1 Assume B1 , B2 . Then for all 20 Bipolar Thermal Equilibrium .
الصفحة 215
[ 23 ] Pacard F. , Unterreiter A. , A Variational Analysis of the Thermal Equilibrium State of Charged Quantum Fluids , to appear in Commun . Partial Differ . Eq . ( 1995 ) . [ 24 ] van Roosbroeck W.V. , Theory of Flow of Electrons and ...
[ 23 ] Pacard F. , Unterreiter A. , A Variational Analysis of the Thermal Equilibrium State of Charged Quantum Fluids , to appear in Commun . Partial Differ . Eq . ( 1995 ) . [ 24 ] van Roosbroeck W.V. , Theory of Flow of Electrons and ...
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