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chapter1_Love_ts.m
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chapter1_Love_ts.m
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function []= chapter1_Love_ts()
clc; clear all
snapshot_time = input('请输入一个波场快照时间(单位:ms):')
tic
%%% 参数设置 %%%
N = 400;
fm = 30;
space_x = 0.5; space_z = 0.5; % 网格步长
sample_t = 0.05/1000; % 时间步长0.05ms
T = 250/1000; % 总时间为250ms
K = T/sample_t; % 外层时间循环总次数:250/0.05 = 5000次
layer = 20*space_x; % 吸收层的厚度
coefficientR = 0.0001; % 理想的反射系数：基本不反射
C1 = 1.125;
C2 = -0.04166667;
%%% 均匀半空间模型的初始化 %%%
% 预分配提速:
VP = zeros(400,400)+1000;
VS = zeros(400,400)+570;
Density = zeros(400,400)+2000;
lame1 = zeros(400,400);
lame2 = zeros(400,400);
for i = 1:N
j = 1:N; % 矢量化加速
lame1(i,j) = Density(i,j) .* (VP(i,j).^2 - 2*VS(i,j).^2);
lame2(i,j) = Density(i,j) .* VS(i,j).^2;
end
%%% Love波:速度、应力初始化 %%%
% 速度分量:
vyx = zeros(400,400);
vyz = zeros(400,400);
vy = zeros(400,400);
% 应力分量:
txy = zeros(400,400);
tzy = zeros(400,400);
% 间距:
dx = zeros(1,400);
dy = zeros(1,400);
%%% AEA 自由表面边界条件 %%%
% 其实就是把原始空间的前4行拿出来，用来做自由空间层！
% 所以差分计算时，i和j都是从4开始
for i = 1:4
for j = 1:N
Density(i,j) = 0.5*Density(i,j);
lame1(i,j) = 0;
lame2(i,j) = lame2(i,j);
end
end
%%% 开始有限差分的计算 %%%
for k = 1:K % 时间是最外层循环：相当于总的迭代次数/传播的时间
fprintf('迭代计算开始,当前是第%d次"时间"大循环!\n',k)
mibinbin = k;
% AEA 自由边界设置：
for i = 1:N
Q(i,4) = 0;
end
% 差分计算：各点的速度更新
for i = 4:(N-4)
for j = 4:(N-4)
% 区域边界的设置
if i <= 4 + layer/space_x
dx(i) = (2*VP(i,j)/layer)*log(1/coefficientR)*((4+layer/space_x-i)*space_x/layer)^4;
end
if i >= N-4-layer/space_x
dx(i) = (2*VP(i,j)/layer)*log(1/coefficientR)*((i-(N-4-layer/space_x))*space_x/layer)^4;
end
if j >= N-4-layer/space_x
% 400 - 4 - 10/0.5 = 346 每一个i下，j要在346之后才会不等于0
% fprintf('第%d次"行循环"已进入j>=346阶段,当前:j=%d\n',i,j);
% pause(1);
dy(j) = (2*VP(i,j)/layer)*log(1/coefficientR)*((j-(N-4-layer/space_x))*space_x/layer)^4;
end
% 速度迭代计算
vyx(i,j) = (vyx(i,j)*(1-sample_t*dx(i)/2)+sample_t/Density(i,j)*((C1*(txy(i,j)-txy(i,j-1))+...
C2*(txy(i,j+1)-txy(i,j-2)))/space_x))/(1+sample_t*dx(i)/2);
vyz(i,j) = (vyz(i,j)*(1-sample_t*dy(i)/2)+sample_t/Density(i,j)*((C1*(tzy(i,j)-tzy(i-1,j))+...
C2*(tzy(i+1,j)-tzy(i-2,j)))/space_z))/(1+sample_t*dy(i)/2);
vy(i,j) = vyx(i,j) + vyz(i,j);
end
end
% 差分计算：各点的应力更新
for i = 4:(N-4)
for j = 4:(N-4)
if i <= 4 + layer/space_x
dx(i) = (2*VP(i,j)/layer)*log(1/coefficientR)*((4+layer/space_x-i)*space_x/layer)^4;
end
if i >= N-4-layer/space_x
dx(i) = (2*VP(i,j)/layer)*log(1/coefficientR)*((i-(N-4-layer/space_x))*space_x/layer)^4;
end
if j >= N-4-layer/space_x
dy(j) = (2*VP(i,j)/layer)*log(1/coefficientR)*((j-(N-4-layer/space_x))*space_x/layer)^4;
end
% 震源位置设置:
vy(200,4) = 100*(1-2*(pi*fm*(k-1000)*sample_t)^2)*...
exp(-(pi*fm*(k-1000)*sample_t)^2);
% 应力设置:
txy(i,j) = (lame1(i,j)*sample_t*((C1*(vy(i,j+1)-vy(i,j))+C2*(vy(i,j+2)-vy(i,j-1))/space_x))+...
txy(i,j)*(1-sample_t*dx(i)/2))/(1+sample_t*dx(i)/2);
tzy(i,j) = (lame1(i,j)*sample_t*((C1*(vy(i+1,j)-vy(i,j))+C2*(vy(i+2,j)-vy(i-1,j))/space_z))+...
tzy(i,j)*(1-sample_t*dy(i)/2))/(1+sample_t*dy(i)/2);
end
end
% snapshot时的波场快照：k = snapshot_time*20
if k == snapshot_time*20
figure('name','Love波总速度V的波场快照');
colormap(jet);
imagesc(vy')
figure('name','Love波y-x方向速度的波场快照');
colormap(jet);
imagesc(vyx');
figure('name','Love波y-z方法速度的波场快照');
colormap(jet);
imagesc(vyz');
break;
end
end
toc
xlswrite('result_love.xls', vy', 'sheet1');
xlswrite('result_love.xls', vyx', 'sheet2');
xlswrite('result_love.xls', vyz', 'sheet3');