We present a quenching result for semilinear parabolic equations with dynamic boundary conditions in bounded domains with a smooth boundary.
A note on boundary conditions for quantum hydrodynamic equations
β Scribed by R. Pinnau
- Publisher
- Elsevier Science
- Year
- 1999
- Tongue
- English
- Weight
- 284 KB
- Volume
- 12
- Category
- Article
- ISSN
- 0893-9659
No coin nor oath required. For personal study only.
β¦ Synopsis
Communicated by P. Markowich
Abstract--The asymptotic behavior of the thermal equilibrium state of a bipolar quantum hydrodynamic model is considered. The quantum limit L ---, 0, L denoting a characteristic device length, is carried out rigorously. It shows that the classical assumption of charge neutrality at the boundary becomes invalid for ultra small semiconductor devices, whereas the assumption of vanishing boundary quantum effects will be confirmed. Furthermore, numerical simulations are presented, which give insight in the quantitative behavior.
π SIMILAR VOLUMES
The quantum hydrodynamic model is primary used for the simulation of resonant tunneling diodes. The current-voltage characteristics of these diodes show negative differential resistance (NDR) effects. For two simplified one-dimensional quantum models derived by means of asymptotic analysis, explicit
In a recent article the authors study the effect of replacing the standard no-slip boundary condition with a nonlinear Navier boundary condition for the boundary layer equations. The resulting equations contain an arbitrary index parameter, denoted by n, and it is found that the case n = 1 correspon
Letters to the E&tors the heatmg se&Ion because the presence of the hot lammar sub-layer prevents the temperature decay m the wall These results show how local values of the heat transfer coefficient can &ffer from the average values, and Illustrate the approxunate nature of the model based on the b
We consider a semilinear parabolic equation subject to a nonlinear dynamical boundary condition that is related to the so-called Wentzell boundary condition. First we prove the existence and uniqueness of global solutions as well as the existence of a global attractor. Then we derive a suitable Εoja
The boundary condition, zero solids pressure at the top of a particle bed of maximum spoutable height, H m , is shown to eliminate any resort to empiricism in the derivation of the fluid velocity in the annulus of a spouted bed for which both viscous and inertial effects are taken into account. The