Internal stresses of an accelerating body

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SUMMARY

The discussion centers on calculating inertial stresses in a deformable solid, specifically a wing attached to a main body under acceleration. The original poster (OP) attempts to use bending stress formulas for cantilever beams but realizes that this approach may not be suitable due to the non-rigid nature of the body. Participants recommend treating the wing as a separate body and using distributed loads rather than concentrated forces. A shift towards modeling the problem as plate bending rather than beam bending is advised to achieve accurate results.

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  • Understanding of inertial stresses in deformable solids
  • Familiarity with bending stress formulas for cantilever beams
  • Knowledge of plate bending theory
  • Ability to construct shear force and moment diagrams
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Mike J
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Homework Statement


Refer to image attached.
accelerating_body.png

Lets say I have a deformable solid that is being accelerated by a force that is equally distributed along the back face of the Main Body that is drawn in the picture. Attached to this Main Body is a Wing. At high accelerations, there will be inertial stresses that reach a maximum at the base of the wing where it is attached to the Main Body. How can I calculate those stresses? I need to find these stresses so that I can determine how large d has to be in order to prevent material failure. I am kind of lost at where to start.

Homework Equations



The Attempt at a Solution


My attempt:


I tried making a cut at the base of the wing (viewed from bottom of the picture shown above)

cut.png

From here I can take sum of the moments to find the bending stress caused by the moment, M.

The equation I get is:

-M = mwingaw/2.

Then I plug into bending stress formula for cantilever beam and compare to the yield stress:

max|=|M|d / (2I) ≤ σyield

where I = 1/12 L d3

If I solve the equations above for d so that σ does not exceed my yield stress, I end up getting unrealistically small values for d. I don't think my approach is correct because I believe it assumes rigid body acceleration when this is not the case. Maybe there's a continuum mechanics approach that involves solving a differential equation to take into account these inertial stresses of a non-rigid accelerating body.

Any help would be appreciated!
 
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Mike J said:
I don't think my approach is correct because I believe it assumes rigid body acceleration when this is not the case.
It looks ok to me, provided the deformation of the wing is relatively small. If it flexes hugely then of course the moment is reduced a little.
Mike J said:
If I solve the equations above for d so that σ does not exceed my yield stress, I end up getting unrealistically small values for d
Please show your working and result, and say why you think it is unrealistic.
 
You have treated the acceleration as a D'Alembert force. This is often very confusing. Instead, I recommend simply treating the wind as a separate body (as you have done), and write F = M*a and the corresponding moment equation. The validity of the whole process should become more evident when you do.
 
You have tried to treat the acceleration using a D'Alembert force. This is often confusing.

Instead, treat the wing as a separate body with a required (known, specified) acceleration, write F = m*a and the corresponding moment equation, and solve for the internal moment and shear force.
 
This should be modeled as a plate rather than a beam. In addition, the load should be distributed, rather than concentrated at the center of mass. Also, there is a shear force at the built-in end. Let's see your shear force diagram, and your moment diagram.
 
Chestermiller said:
the load should be distributed, rather than concentrated at the center of mass
Does that matter if we only want the moment at the point of attachment?
 
Chestermiller said:
This should be modeled as a plate rather than a beam. In addition, the load should be distributed, rather than concentrated at the center of mass. Also, there is a shear force at the built-in end. Let's see your shear force diagram, and your moment diagram.

In actual fact, there is no load at the center of mass or anywhere else except at the connection with the main body. The "load" that Chestermiller refers to presumably is the m*a "force" which is no force at all. There is no need to distribute any load, particularly one that is not there. This can all be handled by treating the wing as a single rigid body, and writing F = m*a and the corresponding rotational equation.
 
Dr.D said:
In actual fact, there is no load at the center of mass or anywhere else except at the connection with the main body. The "load" that Chestermiller refers to presumably is the m*a "force" which is no force at all. There is no need to distribute any load, particularly one that is not there. This can all be handled by treating the wing as a single rigid body, and writing F = m*a and the corresponding rotational equation.
I prefer inertial frames too, but both methods are perfectly valid
 
  • #10
Done correctly, D'Alembert will get to the answer, but I think that this is the whole reason we are discussing this thread, that is, the confusion it so often causes.
 
  • #11
Dr.D said:
I think that this is the whole reason we are discussing this thread, that is, the confusion it so often causes.
It may be the reason you are posting on this thread but I see no evidence the OP is concerned about that. @Mike J wrote that he didn't believe the answers he got, but as he has so far failed to respond with any data on those answers or why he does not believe them it's hard to take it any further.
 
  • #12
haruspex said:
Does that matter if we only want the moment at the point of attachment?
No. I stand corrected. However, I still contend that the stress should be calculated as for plate bending rather than beam bending (because of the low aspect ratio of the piece).
 

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