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Copy pathYLMeff_SingleCrystal.m
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YLMeff_SingleCrystal.m
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clear;
% close;
CS = crystalSymmetry('-43m');
%% Creating Bishop Hill stress state matrix from the text file named: BHfile.txt
B = fopen('BHfile.txt');
BH = textscan(B, ' %f %f %f %f %f %f');
fclose(B);
%% ppt details
% shape = 'Needle'; %or 'Plate
d1 = '100';d2 = '110';d3 = '111';
Dircn = {d1, d2, d3};
colr = ['r' ,'m', 'k'];
f = 0.008;
sigma_bar = 10000e6;
tau = 88e6;
w = 1; % this code has not incoporated w. We have to figure out how to get it incase of other habits
%% Reading the orientation file
prompt = 'The euler angle file name with .txt extension \n';
g_vectorfile = input(prompt);
file_g = fopen(g_vectorfile);
g_matrix = textscan(file_g, '%f %f %f');
fclose(file_g);
l_g = length(g_matrix{1,1});
%% Reading the strain file
S = fopen('strains.txt');
strain = textscan(S, ' %f %f %f ');
l_s = length(strain{1,1});
fclose(S);
Meff = zeros(l_s,11);
ro = zeros(l_s,11);
g = zeros(l_s,11);
for di=1:1:3
[DC_ppt,n_varient,varient]= DC_ppt_function(CS,Dircn{di});
for u=1:1:l_s
for v = 1:1:11
gamma12 = -1 + 0.2*(v-1);
e_ext=[strain{1,1}(u),gamma12,0;gamma12,strain{1,2}(u),0;0,0,strain{1,3}(u)];
Weff= zeros(l_g,1);
for c=1:1:l_g
A = DC_matrix_function(g_matrix{1,1}(c),g_matrix{1,2}(c),g_matrix{1,3}(c));
[e]= transform_e_function(e_ext,A);
N = Nxtal_general_function(A,e_ext,DC_ppt,n_varient);
% [N,w]= Nxtal_calc_function1(A,e_ext);
W= zeros(1,56);
BH_state = zeros(56,6);
for m=1:1:56
W(m)= -(BH{1,2}(m)*e(1,1))+ BH{1,1}(m)*e(2,2)+ BH{1,4}(m)*(e(2,3)+e(3,2))+BH{1,5}(m)*(e(1,3)+e(3,1))+BH{1,6}(m)*(e(1,2)+e(2,1));
BH_state(m,:) = [BH{1,1}(m),BH{1,2}(m),BH{1,3}(m),BH{1,4}(m),BH{1,5}(m),BH{1,6}(m)]; % [A,B,C,F,G,H]
end
Wmax = max(abs(W));
Weff(c) = (1-f)*Wmax + f*w*N*sigma_bar/(tau);
end
Meff(u,v) = mean(Weff)/e_ext(1,1);
ro(u,v) = -strain{1,2}(u)/strain{1,1}(u);
g(u,v) = gamma12/strain{1,1}(u);
end
end
%% Section Contour calculation
% change the range of kk to 1:6 to plot sections along various
% Txy
kk = 1;
for u=1:1:l_s
for v=1:1:11
%aX+bY = M - cZ, a =1; b = -rho
b= -ro(u,v);
c= 2*g(u,v);
Txy = 0.1*(kk-1);
m = Meff(u,v)-c*Txy;
lineq = [-1/b,m/b];
Y = polyval(lineq,-5:0.5:5);
plot(-5:0.5:5,Y)
hold on
end
end
pbaspect([1 1 1])
grid on;
text(-1,0,Dircn(di),'Color','black','FontSize',16);
xlim([-4 4]);
ylim([-4 4]);
xlabel('SigmaXX');
ylabel('SigmaYY');
figure
end
% clearvars A B BH_State W e Wmax gamma12 e_ext g_matrix g_vectorfile l_g g Meff Y b c Txy;
%% Now for solutionized state
f = 0;
for u=1:1:l_s
for v = 1:1:11
gamma12 = -1 + 0.2*(v-1);
e_ext=[strain{1,1}(u),gamma12,0;gamma12,strain{1,2}(u),0;0,0,strain{1,3}(u)];
Weff= zeros(l_g,1);
for c=1:1:l_g
A = DC_matrix_function(g_matrix{1,1}(c),g_matrix{1,2}(c),g_matrix{1,3}(c));
[e]= transform_e_function(e_ext,A);
% N = Nxtal_general_function(A,e_ext,DC_ppt,n_varient);
% % [N,w]= Nxtal_calc_function1(A,e_ext);
W= zeros(1,56);
BH_state = zeros(56,6);
for m=1:1:56
W(m)= -(BH{1,2}(m)*e(1,1))+ BH{1,1}(m)*e(2,2)+ BH{1,4}(m)*(e(2,3)+e(3,2))+BH{1,5}(m)*(e(1,3)+e(3,1))+BH{1,6}(m)*(e(1,2)+e(2,1));
BH_state(m,:) = [BH{1,1}(m),BH{1,2}(m),BH{1,3}(m),BH{1,4}(m),BH{1,5}(m),BH{1,6}(m)]; % [A,B,C,F,G,H]
end
Wmax = max(abs(W));
Weff(c) = Wmax;
end
Meff(u,v) = mean(Weff)/e_ext(1,1);
ro(u,v) = -strain{1,2}(u)/strain{1,1}(u);
g(u,v) = gamma12/strain{1,1}(u);
end
end
%% Section Contour calculation
kk = 1;
for u=1:1:l_s
for v=1:1:11
%aX+bY = M - cZ, a =1; b = -rho
b= -ro(u,v);
c= 2*g(u,v);
Txy = 0.1*(kk-1);
m = Meff(u,v)-c*Txy;
lineq = [-1/b,m/b];
Y = polyval(lineq,-5:0.5:5);
plot(-5:0.5:5,Y)
hold on
end
end
pbaspect([1 1 1])
grid on;
text(-1,0,'No ppt','Color','black','FontSize',16);
xlim([-4 4]);
ylim([-4 4]);
xlabel('SigmaXX');
ylabel('SigmaYY');
% clearvars A B BH_State W e Wmax gamma12 strain e_ext g_matrix g_vectorfile l_g ;