Steady state of diffusion current in semiconductors
Steady state is the state at which the parameters (e.g current density and carrier concentration) at a particular position x x do not change with time. The continuity equation related to carrier current and generation and recombination rate is. ∂p ∂t = −1 q ∂jp ∂x + G, ∂ p ∂ t = − 1 q ∂ j p ∂ x + G, where τp τ p is the ...
Characteristic time for heat diffusion - Physics Stack Exchange
2017年12月1日 · the hand-wavy way to derive the characteristic time is to replace partial differentials with finite differences and note that the thermal diffusivity D = k/ρc D = k / ρ c: ΔT Δx 2 ≈ ΔT Δt D Δ T Δ x ≈ Δ T Δ t. ≈ Δx 2 Δ t ≈ Δ x D. But note that L2/D L 2 / D is not an exact time for anything to occur—it's just an estimate.
Solution of diffusion equation with spherical sink
2018年10月24日 · 2. For steady state diffusion in an unbounded region toward a spherical sink of radius r0 r 0, we have. 4πr2Ddc dr = Q 4 π r 2 D d c d r = Q. where Q is the diffusion rate of the species toward the sink (a constant). The solution to this equation is. c =c∞ − Q 4πrD c = c ∞ − Q 4 π r D. where c∞ c ∞ is the concentration far from ...
Diffusion inside sphere - Physics Stack Exchange
1. Drop the unnecessary asterisk for simplicity: C(r, t) = R(r)T(t) After separation, drop the partials (separation separates the PDE into two ODEs), move D to the lefthand side and use separation constant − λ2, so you get two ODEs: 1 DTT ′ T = − λ2 rR ″ + 2R ′ + λ2rR = 0.
diffusion - 1-D Fick's first law - Physics Stack Exchange
2016年2月3日 · Fick's 1st law: J = −D∂C(x, t) ∂x J = − D ∂ C (x, t) ∂ x. as I understand it, applies to the steady state. For 1-D diffusion and in the steady state, why is the expression not. J = −Ddc(x) dx J = − D d c (x) d x. s there is only one spatial variable and no time dependence (steady state)? ȷ = −D∇ c(x , t). ȷ = − ∇ (x ...
diffusion - Is there a diffusive current in the steady state? - Physics ...
2020年6月7日 · is a steady-state solution that satisfies the boundary conditions. Since this is a steady-state solution, I wouldn't think there is any average current of particles. Rather if we start the system in this state, it will remain in this state forever, without any need to invoke particle creation or absorption at the boundaries.
2D advection-diffusion in a quasi 1D system - Physics Stack …
2024年1月16日 · The equation is equated to zero since we are looking for steady state. The two boundary conditions should be a no flux at the boundaries (the rim), and that the total amount of the concentration is conserved $$\int_0^{2\pi}\int_{0}^{R}c\,\mathrm{d}r\,\mathrm{d}\theta=\text{Const}$$
Why does the steady state exist In thermal conduction?
2022年1月15日 · 1. In thermal conduction,why doesn't transient state go on continuously,why does steady state exist?why after some considerable time A metal bar sttached to a sink and source comes to steady state where the the temperature of different points on bar is different but it doesn't change with time?I want to know what actually happens at molecular ...
Derivation of Einstein's relation in Drift Diffusion model for ...
2016年3月18日 · In this book he gives a derivation of the Einstein relation for the Drift Diffusion model of semiconductors, supposing equilibrim conditions (all current densities are zero) and Boltzmann statistics, that is, e.g. for the electron concentration: \begin{equation} n=n_i exp\left(-\frac{E_{Fi}-E_F}{k_BT}\right), \end{equation}
solid state physics - Diffusion current and possible electric field ...
2022年2月4日 · If the net current density $\vec{J}$ is everywhere $0$, but there is a diffusion "current", there must also be an equal and opposite drift "current" to cancel the diffusion "current". Finally, if there is a counter drift "current" within the interior of the conductor, there must be an electric field there as well to cause that drift "current ...