diancixue.rar_artbog_计算方法_matlab_计算电磁_边界元_边界元 电磁

% BEM_SIMPLE.m % 本程序用边界元方法求解正方形柱体内电位分布 % 编程人 沙威(Wei Sha) 安徽大学(Anhui University) [email protected] clear;clc; %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% 1.常数定义 a=6; % 正方形长 N=3; % 每边点数 minstep=a/N; % 最小离散步长 TOTAL=N*4; % 所有点数 C=1/2; % 常数定义 NN=100; % 积分离散精度 V_L=300; % 已知电压矩阵 xx=a/2; % 方形内部任意一点X坐标 yy=a/2; % 方形内部任意一点Y坐标 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% 2.坐标定位 % 以方柱左下角为坐标原点建立坐标系 % 匹配点采用逆时针方向从(0,a/6)坐标点依次编号 % 方柱左右两边X为常数,方柱上下两边Y为常数 value_b=-minstep/2; % 下侧初值 value_r=-minstep/2; % 右侧初值 value_t=a+minstep/2; % 上测初值 value_l=a+minstep/2; % 左侧初值 for i=1:TOTAL; if (i>0 & i<N+1) % 下侧 value_b=value_b+minstep; point(1,i)=value_b; point(2,i)=0; elseif (i>N & i<2*N+1) % 右侧 value_r=value_r+minstep; point(1,i)=a; point(2,i)=value_r; elseif (i>2*N & i<3*N+1) % 上侧 value_t=value_t-minstep; point(1,i)=value_t; point(2,i)=a; else % 左侧 value_l=value_l-minstep; point(1,i)=0; point(2,i)=value_l; end; end; %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% 3.H矩阵h_st确定 for s=1:TOTAL % 场点循环 for t=1:TOTAL % 源点循环 if (s==t) % 奇异点处理 h_st(s,t)=C; else fieldpoint_x=point(1,s); % 场点X坐标 currentpoint_x=point(1,t); % 源点X坐标 fieldpoint_y=point(2,s); % 场点Y坐标 currentpoint_y=point(2,t); % 源点Y坐标 current_x=linspace(currentpoint_x-minstep/2,currentpoint_x+minstep/2,NN); % X积分变量离散 current_y=linspace(currentpoint_y-minstep/2,currentpoint_y+minstep/2,NN); % Y积分变量离散 if (t>0 & t<N+1)|(t>2*N & t<3*N+1) % 上下侧 quad=abs(fieldpoint_y-currentpoint_y)./... ((fieldpoint_x-current_x).^2+(currentpoint_y-fieldpoint_y).^2); h_st(s,t)=-(1/(2*pi))*trapz(current_x,quad); else % 左右侧 quad=abs(fieldpoint_x-currentpoint_x)./... ((fieldpoint_x-currentpoint_x).^2+(current_y-fieldpoint_y).^2); h_st(s,t)=-(1/(2*pi))*trapz(current_y,quad); end; end; end; end; %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% 4.K矩阵k_st确定 for s=1:TOTAL % 场点循环 for t=1:TOTAL % 源点循环 if (s==t) % 奇异点处理 k_st(s,t)=-(log(minstep/2)-1)*minstep/(2*pi); else fieldpoint_x=point(1,s); % 场点X坐标 currentpoint_x=point(1,t); % 源点X坐标 fieldpoint_y=point(2,s); % 场点Y坐标 currentpoint_y=point(2,t); % 源点Y坐标 current_x=linspace(currentpoint_x-minstep/2,currentpoint_x+minstep/2,NN); % X积分变量离散 current_y=linspace(currentpoint_y-minstep/2,currentpoint_y+minstep/2,NN); % Y积分变量离散 if ((t>0 & t<N+1)|(t>2*N & t<3*N+1)) % 上下侧 quad=log( ( (fieldpoint_x-current_x).^2 + ... (currentpoint_y-fieldpoint_y).^2 ).^(1/2) ); k_st(s,t)=-(1/(2*pi))*trapz(current_x,quad); else % 左右侧 quad=log( ( (fieldpoint_x-currentpoint_x).^2 + ... (current_y-fieldpoint_y).^2 ).^(1/2) ); k_st(s,t)=-(1/(2*pi))*trapz(current_y,quad); end; end; end; end; %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% 5.矩阵整序 % 上下侧电荷分布已知 % 左右侧电压分布已知 H_K1=[h_st(:,[1:N]),-k_st(:,[N+1:2*N]),h_st(:,[2*N+1:3*N]),-k_st(:,[3*N+1:4*N])]; H_K2=[k_st(:,[1:N]),-h_st(:,[N+1:2*N]),k_st(:,[2*N+1:3*N]),-h_st(:,[3*N+1:4*N])]; %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% 6.已知部分电压和电荷矩阵g_u确定 for u=1:TOTAL; if ( (u>3*N) & (u<4*N+1) ) % 上侧 g_u(u)=V_L; else g_u(u)=0; end; end; %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% 7.求解剩下电荷电压分布并显示 charge_voltage=(H_K1)^(-1)*H_K2*g_u.'; disp('下侧电位从左到右:'); disp(charge_voltage(1:N)); disp('上侧电位从左到右:') disp(charge_voltage(3*N:-1:2*N+1)); disp('右侧电荷从上到下:'); disp(charge_voltage(2*N:-1:N+1)); disp('左侧电荷从上到下:'); disp(charge_voltage(3*N+1:4*N)); voltage=[charge_voltage(1:N);g_u(N+1:2*N)';charge_voltage(2*N+1:3*N);g_u(3*N+1:4*N)']; charge= [g_u(1:N)';charge_voltage(N+1:2*N);g_u(:,[2*N+1:3*N])';charge_voltage(3*N+1:4*N)]; %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% 8.方形内部测试点H1矩阵h_st1确定 for t=1:TOTAL % 源点循环 fieldpoint_x=xx; % 场点X坐标 currentpoint_x=point(1,t); % 源点X坐标 fieldpoint_y=yy; % 场点Y坐标 currentpoint_y=point(2,t); % 源点Y坐标 current_x=linspace(currentpoint_x-minstep/2,currentpoint_x+minstep/2,NN); % X积分变量离散 current_y=linspace(currentpoint_y-minstep/2,currentpoint_y+minstep/2,NN); % Y积分变量离散 if (t>0 & t<N+1)|(t>2*N & t<3*N+1) % 上下侧 quad=abs(fieldpoint_y-currentpoint_y)./... ((fieldpoint_x-current_x).^2+(currentpoint_y-fieldpoint_y).^2); h_st1(t)=-(1/(2*pi))*trapz(current_x,quad); else % 左右侧 quad=abs(fieldpoint_x-currentpoint_x)./... ((fieldpoint_x-currentpoint_x).^2+(current_y-fieldpoint_y).^2); h_st1(t)=-(1/(2*pi))*trapz(current_y,quad); end; end; %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% 9.方形内部测试点K1矩阵k_st1确定 for t=1:TOTAL % 源点循环 fieldpoint_x=xx; % 场点X坐标 currentpoint_x=point(1,t); % 源点X坐标 fieldpoint_y=yy; % 场点Y坐标 currentpoint_y=point(2,t); % 源点Y坐标 current_x=linspace(currentpoint_x-minstep/2,currentpoint_x+minstep/2,NN); % X积分变量离散 current_y=linspace(currentpoint_y-minstep/2,currentpoint_y+minstep/2,NN); % Y积分变量离散 if ((t>0 & t<N+1)|(t>2*N & t<3*N+1)) % 上下侧 quad=log( ( (fieldpoint_x-current_x).^2 + ... (currentpoint_y-fieldpoint_y).^2 ).^(1/2) ); k_st1(t)=-(1/(2*pi))*trapz(current_x,quad); else % 左右侧 quad=log( ( (fieldpoint_x-currentpoint_x).^2 + ... (current_y-fieldpoint_y).^2 ).^(1/2) ); k_st1(t)=-(1/(2*pi))*trapz(current_y,quad); end; end; %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% 10.求解内部测试点电位与解析解 resolve=k_st1*charge-h_st1*voltage; % 代入离散化泊松公式 show=[xx,yy]; disp('在方柱内部电位值'); disp(' x= y='); disp(show); disp('BEM方法为:'); disp(resolve); analysis=V_L*(a-xx)/a; disp('解析解为:') disp(analysis)