ElectricPotentialCondition[pred,vars,pars]
表示偏微分方程的电势表面边界条件,谓词 pred 指示其适用位置,并具有模型变量 vars 和全局参数 pars.
ElectricPotentialCondition[pred,vars,pars,lkey]
表示电势表面边界条件,其局部参数在 pars[lkey] 中指定.
ElectricPotentialCondition
ElectricPotentialCondition[pred,vars,pars]
表示偏微分方程的电势表面边界条件,谓词 pred 指示其适用位置,并具有模型变量 vars 和全局参数 pars.
ElectricPotentialCondition[pred,vars,pars,lkey]
表示电势表面边界条件,其局部参数在 pars[lkey] 中指定.
更多信息
- ElectricPotentialCondition 为 ElectrostaticPDEComponent 和 ElectricCurrentPDEComponent 指定狄利克雷(Dirichlet)边界条件.
- ElectricPotentialCondition 为 ElectrostaticPDEComponent 和 ElectricCurrentPDEComponent 指定边界条件.
- ElectricPotentialCondition 通常用于在边界上设置特定电势. 常见示例包括通过施加电压差来充电的电容器设备.
- ElectricPotentialCondition 在具有因变量
和自变量
的边界上设置特定的电势. - 静态变量 vars 为 vars={V[x1,…,xn],{x1,…,xn}}.
- 频率相关变量 vars 为 vars={V[x1,…,xn],ω,{x1,…,xn}}.
- 静态或频域电动势条件 ElectricPotentialCondition 模型
,其中,
[
] 是给定的表面电动势. - 可以给出以下附加模型参数 pars:
-
参数 默认值 符号 "ElectricPotential" 0
,表面电势,单位为 [
] - 模型参数 pars 被指定为 ElectrostaticPDEComponent 和 ElectricCurrentPDEComponent 的参数.
- 规定的电动势条件边界可用于:
-
分析类型 applicable 频率响应 Yes 静态 Yes - ElectricPotentialCondition 运算为 DirichletCondition.
- 边界谓词 pred 可以像在 DirichletCondition 中一样指定.
- 如果 ElectricPotentialCondition 取决于在关联 pars 中指定为 …,keypi…,pivi,… 的参数
,则参数
将替换为
.
范例
打开所有单元 关闭所有单元基本范例 (3)
ElectricPotentialCondition[x ≥ 0, {V[x, y], {x, y}}, <|"ElectricPotential" -> Subscript[V, s][x, y]|>]ElectricPotentialCondition[x ≥ 0, {V[x, y], {x, y}}, <||>]计算模型变量
和参数
下的电势分布,其中左边界的电势
为
[
] ,右边界为接地电势:
vars = {V[x], {x}};
pars = <|"RelativePermittivity" -> 2|>;Vfun = NDSolveValue[{ElectrostaticPDEComponent[vars, pars] == 0, {ElectricPotentialCondition[x == 0, vars, pars, <|"ElectricPotential" -> 10|>], ElectricPotentialCondition[x == 1 / 5, vars, pars, <|"ElectricPotential" -> 0|>]}}, V, x∈Line[{{0}, {1 / 5}}]];Plot[Vfun[x], {x, 0, 1 / 5}, AxesLabel -> {"x", "V"}]范围 (4)
使用模型参数 pars 和多个特定参数边界条件定义静电分析的模型变量 vars:
vars = {V[x, y], {x, y}};
pars = <|"RelativePermittivity" -> 1, "BoundaryCondition1" -> <|<|"ElectricPotential" -> V1|>|>, "BoundaryCondition2" -> <|<|"ElectricPotential" -> V2|>|>|>;ElectricPotentialCondition[x == 0, vars, pars, "BoundaryCondition1"]ElectricPotentialCondition[x == 1, vars, pars, "BoundaryCondition2"]一维 (1)
计算距离
[
] 且垂直于
轴放置的两个平行板之间的电势分布. 左侧平板保持恒定电势
[
],而右侧平板接地,
. 平板之间的区域具有相对介电常数
和均匀的电荷密度
[
]. 要在模型中使用的方程如下:
vars = {V[x], {x}};Ω = Line[{{0}, {0.08}}];pars = <|"RelativePermittivity" -> 1, "VolumeChargeDensity" -> -10*^-8|>;Subscript[Γ, v] = {ElectricPotentialCondition[x == 0, vars, pars, <|"ElectricPotential" -> 1|>], ElectricPotentialCondition[x == 0.08, vars, pars]}eqn = ElectrostaticPDEComponent[vars, pars] == 0Vfun = NDSolveValue[{eqn, Subscript[Γ, v]}, V, x∈Ω]Plot[Vfun[x], x∈Ω]二维 (1)
求解导电率为
的三压开关中的电动标量电势. 模型中使用的方程为:
vars = {V[x, y], {x, y}};Ω = RegionUnion[Rectangle[{0, 2.5}, {10, 7.5}], Rectangle[{9, -2.5}, {10 + 9, 2.5}], Rectangle[{0, -7.5}, {10, -2.5}]];pars = <|"ElectricalConductivity" -> 6*^7|>;Subscript[Γ, ground] = ElectricPotentialCondition[y == -7.5, vars, pars, <|"ElectricPotential" -> 0|>];Subscript[Γ, potential] = ElectricPotentialCondition[y == 7.5, vars, pars, <|"ElectricPotential" -> 5|>];Vfun = NDSolveValue[{ElectricCurrentPDEComponent[vars, pars] == 0, Subscript[Γ, ground], Subscript[Γ, potential]}, V, {x, y}∈Ω];Jfield = -6*^7 * Grad[Vfun[x, y], {x, y}];VectorPlot[Jfield, {x, y}∈Ω, AspectRatio -> Automatic]三维 (1)
建立一个简化的变压器套管绝缘子模型,在与高压导体接触的内壁上设置电动势条件,在一个表面板(
)上设置接地电势边界. 模型中使用的方程为:
vars = {V[x, y, z], {x, y, z}};insulator = \!\(\*Graphics3DBox[«7»]\);pars = <|"RelativePermittivity" -> 5|>;Subscript[Γ, ground] = ElectricPotentialCondition[z == 0.2, vars, pars, <|"ElectricPotential" -> 0|>];Subscript[Γ, potential] = ElectricPotentialCondition[x ^ 2 + y ^ 2 <= 0.2 ^ 2, vars, pars, <|"ElectricPotential" -> 10 ^ 3|>];eqn = ElectrostaticPDEComponent[vars, pars] == 0;Vfun = NDSolveValue[{eqn, Subscript[Γ, ground], Subscript[Γ, potential]}, V, {x, y, z}∈insulator]Legended[RegionPlot3D[insulator, ColorFunction -> Function[{x, y, z}, ColorData[{"Rainbow", MinMax[Vfun["ValuesOnGrid"]]}][Vfun[x, y, z]]], ...], BarLegend[...]]技术笔记
-
▪
- 静电学 ▪
- Electric currents
相关指南
-
▪
- 电磁偏微分方程以及边界条件 ▪
- 偏微分方程术语
文本
Wolfram Research (2024),ElectricPotentialCondition,Wolfram 语言函数,https://reference.wolfram.com/language/ref/ElectricPotentialCondition.html (更新于 2024 年).
CMS
Wolfram 语言. 2024. "ElectricPotentialCondition." Wolfram 语言与系统参考资料中心. Wolfram Research. 最新版本 2024. https://reference.wolfram.com/language/ref/ElectricPotentialCondition.html.
APA
Wolfram 语言. (2024). ElectricPotentialCondition. Wolfram 语言与系统参考资料中心. 追溯自 https://reference.wolfram.com/language/ref/ElectricPotentialCondition.html 年
BibTeX
@misc{reference.wolfram_2026_electricpotentialcondition, author="Wolfram Research", title="{ElectricPotentialCondition}", year="2024", howpublished="\url{https://reference.wolfram.com/language/ref/ElectricPotentialCondition.html}", note=[Accessed: 09-September-2026]}
BibLaTeX
@online{reference.wolfram_2026_electricpotentialcondition, organization={Wolfram Research}, title={ElectricPotentialCondition}, year={2024}, url={https://reference.wolfram.com/language/ref/ElectricPotentialCondition.html}, note=[Accessed: 09-September-2026]}