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Homework no.5
Ply mechanics
Problem (5-2)
%% Problem 5.2%%
%%used material carbon epoxy(AS4/3501-6)%%
%for this material F1t=1830, F2t=57 , F6=71%
clear all;
clc;
sigmax=10;
sigmay=5;
sigmaxy=2.5;
m=cosd(60);
n=sind(60);
T=[m^2 n^2 2*n*m; n^2 m^2 -2*m*n; -m*n m*n (m^2)-(n^2)];
sigma=[sigmax;sigmay;sigmaxy];
sigmadash=T*sigma
RESULT:
sigmadash =
8.4151
6.5849
-3.4151
F1t=1830>8.41 F2t=57>6.584, F6=71>3.415
Then  F.s=allowable strength/applied load=57/6.584=8.6
Problem (5-3)
clear all;
clc;
E1=35;
E2=3.5;
neu12=0.3;
neu21=(E2*neu12)/E1;
G12=1.75;
delta=1-(neu12*neu21);
Q=[E1/delta (E2*neu12)/delta 0; neu12*E2/delta E2/delta 0; 0 0
G12]
m=cosd(45);
n=sind(45);
T=[m^2 n^2 2*n*m; n^2 m^2 -2*m*n; -m*n m*n (m^2)-(n^2)];
Tinverse=inv(T);
Qbar=Tinverse*Q*T
Results
Q =
35.3179 1.0595 0
1.0595 3.5318 0
0 0 1.7500
Qbar =
11.1172 9.3672 15.8930
9.3672 11.1172 15.8930
7.9465 7.9465 18.3653
Problem (5-5)
%problem (5-5)
clear all;
clc;
%geometry
w=10;
t=0.01;
L=150;
E1=35;
A1=w*t;
A2=L*t;
A12=L*w;
%material property
E2=3.5;
neu12=0.3;
neu21=(E2*neu12)/E1;
G12=1.75;
delta=1-(neu12*neu21);
Q=[E1/delta (E2*neu12)/delta 0; neu12*E2/delta E2/delta 0; 0 0
G12]
%transformation
m=cosd(10);
n=sind(10);
T=[m^2 n^2 2*n*m; n^2 m^2 -2*m*n; -m*n m*n (m^2)-(n^2)];
Tinverse=inv(T);
Qbar=Tinverse*Q*T
%applied forces and stresses
Faxial=200;
sigma1=Faxial/A1;
sigma2=Faxial/A2;
sigma12=Faxial/A12;
sigma=[sigma1; sigma2 ;sigma12];
%(a)stress strain relation in local coordinate
epsilon=inv(Q)*sigma
%(b)strain in global coordinate
epsilondash=Tinverse*epsilon
Results
Q =
35.3179 1.0595 0
1.0595 3.5318 0
0 0 1.7500
Qbar =
33.3876 2.0313 10.7758
2.0313 3.5184 0.0957
5.3879 0.0478 3.6936
epsilon =
56.0000
20.9524
0.0762
epsilondash =
54.9171
22.0353
6.0651

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Hw5

  • 2. Problem (5-2) %% Problem 5.2%% %%used material carbon epoxy(AS4/3501-6)%% %for this material F1t=1830, F2t=57 , F6=71% clear all; clc; sigmax=10; sigmay=5; sigmaxy=2.5; m=cosd(60); n=sind(60); T=[m^2 n^2 2*n*m; n^2 m^2 -2*m*n; -m*n m*n (m^2)-(n^2)]; sigma=[sigmax;sigmay;sigmaxy]; sigmadash=T*sigma RESULT: sigmadash = 8.4151 6.5849 -3.4151 F1t=1830>8.41 F2t=57>6.584, F6=71>3.415 Then  F.s=allowable strength/applied load=57/6.584=8.6
  • 3. Problem (5-3) clear all; clc; E1=35; E2=3.5; neu12=0.3; neu21=(E2*neu12)/E1; G12=1.75; delta=1-(neu12*neu21); Q=[E1/delta (E2*neu12)/delta 0; neu12*E2/delta E2/delta 0; 0 0 G12] m=cosd(45); n=sind(45); T=[m^2 n^2 2*n*m; n^2 m^2 -2*m*n; -m*n m*n (m^2)-(n^2)]; Tinverse=inv(T); Qbar=Tinverse*Q*T Results Q = 35.3179 1.0595 0 1.0595 3.5318 0 0 0 1.7500 Qbar = 11.1172 9.3672 15.8930 9.3672 11.1172 15.8930 7.9465 7.9465 18.3653
  • 4. Problem (5-5) %problem (5-5) clear all; clc; %geometry w=10; t=0.01; L=150; E1=35; A1=w*t; A2=L*t; A12=L*w; %material property E2=3.5; neu12=0.3; neu21=(E2*neu12)/E1; G12=1.75; delta=1-(neu12*neu21); Q=[E1/delta (E2*neu12)/delta 0; neu12*E2/delta E2/delta 0; 0 0 G12] %transformation m=cosd(10); n=sind(10); T=[m^2 n^2 2*n*m; n^2 m^2 -2*m*n; -m*n m*n (m^2)-(n^2)]; Tinverse=inv(T); Qbar=Tinverse*Q*T %applied forces and stresses Faxial=200; sigma1=Faxial/A1; sigma2=Faxial/A2; sigma12=Faxial/A12; sigma=[sigma1; sigma2 ;sigma12]; %(a)stress strain relation in local coordinate epsilon=inv(Q)*sigma %(b)strain in global coordinate
  • 5. epsilondash=Tinverse*epsilon Results Q = 35.3179 1.0595 0 1.0595 3.5318 0 0 0 1.7500 Qbar = 33.3876 2.0313 10.7758 2.0313 3.5184 0.0957 5.3879 0.0478 3.6936 epsilon = 56.0000 20.9524 0.0762 epsilondash = 54.9171 22.0353 6.0651