Debye layer in Poisson–Boltzmann model with isolated singularities
CY Hsieh, Y Yu - Archive for Rational Mechanics and Analysis, 2020 - Springer
CY Hsieh, Y Yu
Archive for Rational Mechanics and Analysis, 2020•SpringerWe show the existence of solutions to the charge conserved Poisson–Boltzmann equation
with a Dirichlet boundary condition on ∂ Ω∂ Ω. Here Ω Ω is a smooth simply connected
bounded domain in R^ n R n with n\geqslant 2 n⩾ 2. When n= 2 n= 2, the solutions can have
isolated singularities at prescribed points in Ω Ω, in which case they are essentially weak
solutions of the charge conserved Poisson–Boltzmann equations with Dirac measures as
source terms. By contrast, for higher dimensional cases n\geqslant 3 n⩾ 3, all the isolated …
with a Dirichlet boundary condition on ∂ Ω∂ Ω. Here Ω Ω is a smooth simply connected
bounded domain in R^ n R n with n\geqslant 2 n⩾ 2. When n= 2 n= 2, the solutions can have
isolated singularities at prescribed points in Ω Ω, in which case they are essentially weak
solutions of the charge conserved Poisson–Boltzmann equations with Dirac measures as
source terms. By contrast, for higher dimensional cases n\geqslant 3 n⩾ 3, all the isolated …
Abstract
We show the existence of solutions to the charge conserved Poisson–Boltzmann equation with a Dirichlet boundary condition on . Here is a smooth simply connected bounded domain in with . When , the solutions can have isolated singularities at prescribed points in , in which case they are essentially weak solutions of the charge conserved Poisson–Boltzmann equations with Dirac measures as source terms. By contrast, for higher dimensional cases , all the isolated singularities are removable. As a small parameter tends to zero, and the solutions develop a Debye boundary layer near the boundary . In the interior of , the solutions converge to a unique constant. The limiting constant is explicitly calculated in terms of a novel formula which depends only on the supplied Dirichlet data on . In addition we also give a quantitative description on the asymptotic behaviour of the solutions as .
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