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Superposition of Shear Stress 4

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flyforever85

New member
Jun 22, 2010
178
Hi all,
I'm having trouble solving this problem. I have a pipe, on a certain section this pipe has a shear load and torque applied, they both generate shear stress on the same plane.

A is the point at the top of the pipe section (12 o'clock), B at 3 o'clock etc, C at 6 o'clock and D at 9 o'clock.
We know that:
[ul]
[li]shear stress from shear load is max at B and D and 0 at A and C[/li]
[li]shear stress from torque is max at any point of the outer circumference so at A, B, C and D[/li][/ul]

When the shear stress ARE NOT directed in the same direction, but they are on the same plane (for example between A and B at 45 degrees) how do I sum them?

I need to find a tau xy to put in Von Mises equation.

Thank you
 
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-It is true that ,shear stress from shear load is max at B and D and 0 at A and C.
-It is also true that ,shear stress from torque is constant at any point having the same radius and tangential to tge circumference so at A, B, C and D ..

Another truth is the shear stress must be tangential for circular sections at the extreme edges for equilibrium .

Assuming the shear load vertical and downward, and torsion clockwise,
-Betwen A to C; total shear stress = shear stress from shear load + shear stress from torque
-Between C to A ; total shear stress = shear stress from shear load - shear stress from torque

But, if you have shear load P, the same section SHALL experience bending stresses..

 
I'm with HT (I think).
If I am understanding your problem (like a homework out of a mechanics of materials textbook), the shear stress from pure shear in a single plane and torsional shear are simply additive (not SRSS). The peak happens at a single point.
For steel, you can compare you demand (summation of shear stresses) with the capacity = tau_max = 0.577 * F_yield (also considering safety factors as req'd).
 
I'd've drawn the shear flows along the thin wall CL. I don't think there's vector addition, only scalar addition.


another day in paradise, or is paradise one day closer ?
 
The derivation below profs me wrong. Since the shear flow/distribution manners are the same, scalar addition is correct. Apologize for my ignorance. (Previous erroneous comments have been deleted)

image_xqr5oa.png
 
Shear stress due to bending of a hollow circular tube is shown in the first sketch below. An expression for the maximum value is shown in the second sketch. Other values can be determined using the relationship s = VQ/Ib where s is shear stress due to bending. Shear stress is always tangential to the circle, so the combined stress due to torsion and bending are found by scalar addition.

image_afmlij.png


image_wrlant.png


EDIT: Unless I made a mistake, that doesn't seem to agree with (4) by r13.

[highlight #FCE94F]If r1 = 1, r2 = 2 then the bracketed expression is (4 + 2 + 1)/(4 + 1) = 7/5 = 1.4
and Taumax = 4*1.4/3 *V/A = 1.867V/A (93% of r13's 2V/A)
can anyone see the problem?
r13, what is your source and what is equation (1)?[/highlight]

BA
 
I see the problem now. r13 is using a line element for the circle whereas I was using the exact area.

BA
 
BA,

Here is the link. Link Do you have anything on shear stress over solid rod? It looks like that's the form you got.
 
r13,

Yes, for solid rod we agree on 4V/3A for maximum shear stress.

The difference in the hollow cylinder involves an approximation. Your source used radius r to the middle of the ring whereas my source considered separate values for r1 and r2. In most cases, the value of t (thickness) is small compared to r, so it makes very little difference which way you do it.

For example, if r1 = 1 and r2 = 1.1, then the bracketed expression is (1.21 + 1.1 + 1)/(1.21 + 1) = 3.31/2.21 = 1.49774
and Taumax = 4*1.49774/3 *V/A = 1.997V/A (close enough to r13's 2V/A)

BA
 
BA,

Good work. Seems you still have lots of math in you, and having fun :)
 
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