% For plane slider: H = Ho + a(1-x)
Ho = 1;
alpha = 0.1;
eps = 0.1;
a = 1.0;
lbar = 0.1;
SIGMA = 0:0.05:0.15;
sigma = zeros(1,length(SIGMA));
for j = 1:length(SIGMA)
sigma = SIGMA(j);
H = @(x) Ho + a*(1 - x); % For plane slider: H = Ho + a(1-x)
G1 = @(x) H(x).^3 + 3 .* H(x).^2 .* alpha + 3 .* H(x) .* alpha^2 + 3 .* H(x) .* sigma^2 + eps + 3*sigma^2*alpha + alpha^3 - 12*lbar^2 .* (H(x) + alpha);
G2 = @(x) 24 * lbar^3 .* tanh(H(x)./(2*lbar));
G3 = @(x) (12*lbar^2*alpha - eps - alpha^3 - 3*sigma^2*alpha) .* (1 - (tanh(H(x)./(2*lbar))).^2);
G = @(x) G1(x) + G2(x) + G3(x);
Hm1 = @(x) H(x).* (1 ./ G(x));
Hm2 = @(x) (1 ./ G(x));
IntHm1 = integral(Hm1,0,1);
IntHm2 = integral(Hm2,0,1);
Hm = IntHm1 / IntHm2;
P1 = @(x) 6 .* (1 ./ G(x)) .* (H(x) - Hm);
P2 = @(x) integral(P1,0,x);
% Calculating dimensionless load carrying capacity(W):
W(j) = integral(P2,0,1, 'ArrayValued', true)
% Calculating non dimensional Frictional Force(F):
F1 = @(x) (H(x).* P1(x)) ./2 + (1 ./ H(x));
F(j) = integral(F1,0,1)
% Calculating coefficient of friction(f):
f(j) = F(j)/W(j)
% Calculating non dimensional temperature rise(deltaT):
deltaT(j) = F(j)/Hm
% Calculating the center of pressure(Xbar):
Xbar1 = @(x) P2(x) .* x;
Xbar(j) = integral(Xbar1, 0, 1, 'ArrayValued', true)/W(j)
end

 Akzeptierte Antwort

Voss
Voss am 7 Jun. 2022

0 Stimmen

SIGMA is of size 1-by-4, and the loop goes from 1 to length(SIGMA) (which is 4), so what else would you expect?
SIGMA = 0:0.05:0.15 % 1-by-4
SIGMA = 1×4
0 0.0500 0.1000 0.1500
for j = 1:length(SIGMA) % 1:4
disp(j)
end
1 2 3 4

4 Kommentare

AVINASH SAHU
AVINASH SAHU am 7 Jun. 2022
Thank you for clarification and is there any way that I can get only the final result?
Voss
Voss am 7 Jun. 2022
Bearbeitet: Voss am 7 Jun. 2022
If, for instance, when the code is complete, you want Xbar to contain just the final element of Xbar that's calculated inside the loop, you can do this after the loop:
Xbar = Xbar(end);
Is that what you mean by "final result"?
AVINASH SAHU
AVINASH SAHU am 7 Jun. 2022
Yes, thank you!
Voss
Voss am 7 Jun. 2022
You're welcome!

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