Shear Flow Box Beam (Close to the answer)

In summary, a shear flow box beam is a structural element commonly used in construction to resist bending and shear forces. Shear flow refers to the distribution of shear stress along the cross-section of the beam, which is determined by the shear force and moment of inertia. The equation for shear flow in a box beam is Q = VQ/I. This information is used to analyze the beam and ensure it can withstand the applied loads. Several factors, such as cross-section shape and dimensions, applied loads, and material properties, can affect shear flow in a box beam.
  • #1
zack7
55
0

Homework Statement


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Homework Equations


The moment and shear flow equations

Solved with Matlab


The Attempt at a Solution



I am getting real close to the answer but something is off and I can't figure it out.

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The full code (Matlab)
Code:
deg = pi/180;
G   = 4.e6;

%...Flange areas (in^2):
Af = [1 0.5 0.5 1 1 0.5 0.5 1];
nstringers = length(Af);

%...Flange coordinates (in):
z = [ 0 6 14 24 24 14 6 0];
y = [ 0  0  0  0  10  10  10 10];

%...Wall thicknesses (in):
t = [0.04 0.04 0.04 0.05 0.04 0.04 0.04 0.05 0.025 0.025];
npanels = length(t);

%...Wall connectivity:
node = [1 2
        2 3
        3 4
        4 5
        5 6
        6 7
        7 8
        8 1
        7 2
        6 3];

%...Wall lengths:
for i = 1:npanels
    s(i) = norm([y(node(i,2)) - y(node(i,1)) z(node(i,2)) - z(node(i,1))]);
end

%...Locate the centroid:
zG = sum(z.*Af)/sum(Af);
yG = sum(y.*Af)/sum(Af);

%...Compute the centroidal moments of inertia:
Iy  = sum(Af.*(z - zG).^2);
Iz  = sum(Af.*(y - yG).^2);
Iyz = sum(Af.*(y - yG).*(z - zG));

%...Flange load gradients, Equation [4.8.2]:
syms Vy Vz
dPdx = 1/(Iy*Iz - Iyz^2)...
                       *( (Iy*Vy - Iyz*Vz)*(y - yG)...
                         +(Iz*Vz - Iyz*Vy)*(z - zG)).*Af;

%...Stringer equilibrium at flanges 1 through 7:
syms  q1  q2  q3  q4  q5  q6  q7  q8  q9  q10
eq1 = q1 - q8 -       dPdx(1);
eq2 = q2 - q1 -  q9 - dPdx(2);
eq3 = q3 - q2 - q10 - dPdx(3);
eq4 = q4 - q3 -       dPdx(4);
eq5 = q5 - q4 -       dPdx(5);
eq6 = q6 - q5 + q10 - dPdx(6);
eq7 = q7 - q6 +  q9 - dPdx(7);

%...Moment equivalence about flange 8, including dummy torque T:
syms T
A1 = 1/2*s(1)*s(8);
A2 = 1/2*s(2)*s(8);
A3 = 1/2*s(3)*s(8);
A4 = 1/2*s(4)*(s(1) + s(2) + s(3));
A9 = 1/2*s(9)*s(1);
A10 = 1/2*s(10)*(s(1) + s(3));
eq8 = 2*A1*q1 + 2*A2*q2 + 2*A3*q3 + 2*A4*q4 - 2*A9*q9 - 2*A10*q10 - ...
      (-Vy*14 - Vz*0) - T;

%...Solve the above eight equations for the shear flows q1 through q8
%   in terms of the redundants q9 & q10, the applied loads Vy & Vz and
%   the dummy torque T:
solution = solve(eq1,eq2,eq3,eq4,eq5,eq6,eq7,eq8, ...
                  q1, q2, q3, q4, q5, q6, q7, q8);

%...Store the results (Equations [f] of the text) in the vector 'q':
q = [solution.q1 solution.q2 solution.q3 solution.q4 ...
     solution.q5 solution.q6 solution.q7 solution.q8 ...
     q9 q10];

%...Obtain the virtual shear flows from the actual ones by zeroing the
%   applied loads and replacing the true redundant shear flows by
%   their virtual counterparts and the dummy torque T by the virtual
%   torque dT:
syms dq9 dq10 dT
dq = subs(q, {q9 q10 Vy Vz T}, {dq9 dq10 0 0 dT});

%...Substitute the values of the external loads into the shear flow
%   expressions:
 q = subs(q, {Vy Vz T}, {-8000 0 0});

%...Calculate the internal complementary virtual work:
syms L
dWint = -L/G*sum(s./t.*q.*dq);

%...The external complementary virtual work:
syms theta
dWext = theta*dT;

%...PCVW:
dW = dWint + dWext;

%...This results in an equation of the form  c1*dq9 + c2*dq10 + c3*dT = 0.
%   Isolate c1, c2 and c3:
c1 = subs(dW, {dq9 dq10 dT}, {1 0 0});
c2 = subs(dW, {dq9 dq10 dT}, {0 1 0});
c3 = subs(dW, {dq9 dq10 dT}, {0 0 1});

%...Solve these three equations for q9, q10 and theta:
solution = solve(c1, c2, c3, q9, q10, theta);

%...Substitute the shear flow results into the expressions for
%   q1 through q8:
q     = subs(q,{q9 q10},{solution.q9 solution.q10});

theta = solution.theta;

fprintf('\n----------------------------------------------------\n')
disp(probTitle)
fprintf('\n %s\n %s\n\n', programmer, date)
disp(probStatement)

fprintf('\n Flange   z(in)    y(in)   A(in^2)')
for i = 1:8
    fprintf('\n %4.0f %8.2f %8.2f %8.2f',i,z(i),y(i),Af(i))
end

fprintf('\n\n Wall Thickness(in) Length(in)')
for i = 1:10
    fprintf('\n%4.0f %8.2f       %8.4f',i,t(i),s(i))
end

fprintf('\n\n Centroid coordinates (in.)')
fprintf('\n    zG = %g    yG = %g \n', zG, yG)

fprintf('\n Moments of inertia (in.^4):')
fprintf('\n    IGz = %g   IGy = %g    IGyz = %g \n', Iz, Iy, Iyz)

fprintf('\n Shear loads:')
fprintf('\n    Vy = -8000 lb     Vz = 0 lb \n')

fprintf('\n Shear flows (lb/in):\n')
for i = 1:10
    fprintf('    q%g = %10.4f\n', i, double(q(i)))
end

fprintf('\n Angle of twist:')
fprintf('\n    theta/L = %g degrees/in', double(theta/deg/L))

fprintf('\n----------------------------------------------------\n\n')
 

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  • #2



I am not sure what the specific issue is with your code without seeing it, but here are a few general tips for troubleshooting:

1. Double check your equations: Make sure you have the correct equations for moment and shear flow, and that you are using the correct variables and units.

2. Check your input values: Make sure you are using the correct values for the flange areas, wall thicknesses, and wall lengths. Double check your calculations to ensure they are correct.

3. Use debugging tools: Many programming languages have debugging tools that allow you to step through your code and see the values of variables at each step. This can help you identify where the issue is occurring.

4. Print out intermediate values: You can use the "disp" function in Matlab to print out values at various points in your code. This can help you identify where the issue is occurring.

5. Use online resources: There are many online resources available for troubleshooting code, such as forums, tutorials, and step-by-step guides. You can also reach out to other scientists or programmers for help.
 

1. What is a shear flow box beam?

A shear flow box beam is a structural element that consists of a top and bottom flange connected by vertical webs, forming a hollow rectangular box shape. It is commonly used in construction to resist bending and shear forces.

2. How does shear flow work in a box beam?

Shear flow is the distribution of shear stress along the cross-section of a beam. In a box beam, shear flow is determined by the shear force acting on the beam and the moment of inertia of the cross-section. The shear force causes a shear stress on the top and bottom flanges, while the moment of inertia determines the distribution of shear stress on the vertical webs.

3. What is the equation for shear flow in a box beam?

The equation for shear flow in a box beam is Q = VQ/I, where Q is the shear flow, V is the shear force, Q is the moment of inertia, and I is the moment of inertia of the cross-section.

4. How is shear flow used to analyze a box beam?

Shear flow is used to calculate the shear stress at different points along the cross-section of a box beam. This information is then used to determine the maximum shear stress, which is compared to the maximum allowable shear stress to ensure the beam can withstand the applied loads.

5. What factors can affect shear flow in a box beam?

Several factors can affect shear flow in a box beam, including the shape and dimensions of the cross-section, the type and magnitude of applied loads, and the material properties of the beam. The shear flow can also be influenced by the presence of cutouts, openings, or other irregularities in the beam's cross-section.

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