Moment of Inertia Clarification

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Discussion Overview

The discussion revolves around the moment of inertia (MOI) calculations for a long thin plate with C channels, specifically addressing confusion regarding the application of the parallel axis theorem and the interpretation of Ix and Iy in relation to bending and buckling behavior under load.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant describes a setup involving a long thin plate with C channels and questions the interpretation of Ix as the resistance to bending about the x-axis.
  • Another participant clarifies that Ix should be calculated about the neutral axis of the cross section and not an arbitrary coordinate system, asserting that Ix allows for vertical deflection.
  • There is a discussion about whether the product of inertia, Ixy, is necessary, with some participants arguing it is not needed in this context.
  • One participant suggests that the structure will deflect into a rainbow shape due to fixed edges and questions the relevance of Iy in this scenario.
  • Concerns are raised about the applicability of the parallel axis theorem, with one participant stating it only works for uniform sectional properties, while another later agrees that it applies given the interest is perpendicular.
  • Participants express uncertainty about the boundary conditions affecting the shape transformation of the structure under load.

Areas of Agreement / Disagreement

Participants express differing views on the relevance of Ix and Iy, the necessity of Ixy, and the applicability of the parallel axis theorem. The discussion remains unresolved regarding the best approach to calculate the moment of inertia for this specific setup.

Contextual Notes

Limitations include potential misunderstandings about the uniformity of the sectional properties and the specific boundary conditions affecting the structure's behavior under load.

laforzadiment
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Hi all. It's been a while since I've taken mechanics of solids, I was hoping I could get some confusion ironed out here.

I have a long thin plate with C channels welded along its length, below is a cross sectional view.
[PLAIN]http://img375.imageshack.us/img375/6672/channelexcel.jpg
As you can see, I have placed my axis about the neutral axis of the plate as well as its left edge. In my scenario I have an upwards pressure load on the bottom face of the plate.

I treated this entire setup as multiple rectangular bodies, computed the MOI about their centroids then used the parallel axis theorem to relate them to my chosen axis and combined them for the overall Ix and Iy about that origin.

My problem arises when I don't comprehend what I have found. Is Ix the resistance of this entire cross section bending in and out of the page about the x axis? So for example, a vertical strip would become a 3 dimensional U shape with the "prongs" facing the viewer?

If so, this is not what I am looking for. I need the resistance of the above shape transforming into a "rainbow" shape; it's resistance to buckling. Is this Ixy?
 
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laforzadiment: No, you need Ix about the cross section neutral axis, not about your xy coordinate system axes. Did you do this correctly, to already obtain Ix about the cross section neutral axis? If so, that is what you need.

You do not need product of inertia, Ixy.

No, Ix will not cause a vertical strip to become a U shape with the prongs facing the viewer. It will instead cause a vertical strip to rotate about the horizontal neutral axis. We cannot really say what shape your structure will transform into, because we do not know your boundary conditions. But in general, Ix will allow your cross section to deflect vertically upward.
 
nvn said:
laforzadiment: No, you need Ix about the cross section neutral axis, not about your xy coordinate system axes. Did you do this correctly, to already obtain Ix about the cross section neutral axis? If so, that is what you need.

You do not need Ixy. Product of inertia is zero here.

No, Ix will not cause a vertical strip to become a U shape with the prongs facing the viewer. It will instead cause a vertical strip to rotate about the horizontal neutral axis. We cannot really say what shape your structure will transform into, because we do not know your boundary conditions. But in general, Ix will allow your cross section to deflect vertically upward.

Thanks for your reply. Ok, so you're saying that I cannot arbitrarilly place the axis and that it must go at the centroid of the mass as a whole? Alright, I'll update my spreadsheet.

Consider the left and right end to be fixed in place so any upward uniformly distributed load will exclusively cause first order bowing until failure.

In the text you wrote it seems like you were saying Ix resists this motion:
[PLAIN]http://img806.imageshack.us/img806/9324/85217762.jpg
If this is the case, wouldn't I need Iy?
 
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laforzadiment: No, what you drew in post 3 is bending rotation about the z axis. Ix resists rotation of the vertical strip about the x axis; therefore, the top of the strip would move toward the viewer, and the bottom of the strip would move away from the viewer.

Because the left and right edges of your structure are fixed, your structure will deflect into somewhat of a rainbow shape, in the view you showed in post 1. But it will do this mainly because of Iz, instead of Ix. Ix would be more important if your structure were constrained along its front and back edge. So you need Iz of the yz cross section about its z neutral axis.
 
Ah I gotcha now. Awesome, thanks for the help!
 
laforzadiment said:
I treated this entire setup as multiple rectangular bodies, computed the MOI about their centroids then used the parallel axis theorem to relate them to my chosen axis and combined them for the overall Ix and Iy about that origin.

Parallel axis theorem WON'T work in this case. The theorem only works when the sectional property is uniform over the span of the bending member. You have non uniformity, as each segment has different properties from its adjacent neighbors.
 
skeleton said:
Parallel axis theorem WON'T work in this case. The theorem only works when the sectional property is uniform over the span of the bending member. You have non uniformity, as each segment has different properties from its adjacent neighbors.

I don't follow. The area is uniform in and out of the page, I follow the same method used for a T or I-Beam just with more components.
 
Oops. I mistakenly thought you were trying to determine the stiffness from left to right of the picture. Evidently from your comment your interest is perpendicular. In that case, I agree the theorem does apply.
 
skeleton said:
Oops. I mistakenly thought you were trying to determine the stiffness from left to right of the picture. Evidently from your comment your interest is perpendicular. In that case, I agree the theorem does apply.

No prob :) it can be difficult to convey the original problem setup only through text.
 

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