How Do You Calculate the Moment of Inertia for a Rotating Slab?

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Homework Help Overview

The discussion revolves around calculating the moment of inertia for a thin rectangular slab with specific dimensions and mass, rotated about an axis parallel to one edge. Participants are examining the application of the parallel axis theorem and the appropriate formulas for moment of inertia in this context.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the application of the parallel axis theorem and question the correct distance from the center of mass to the new axis. There is also debate over the appropriate formula for the moment of inertia for a rectangular slab and whether the original poster's calculations were correct.

Discussion Status

The discussion is active, with participants providing insights and corrections regarding the application of formulas. Some participants suggest reconsidering the distance used in the parallel axis theorem, while others clarify the definitions of the variables involved. There is no explicit consensus on the correct approach yet, but multiple interpretations are being explored.

Contextual Notes

Participants note potential confusion regarding the definitions of the moment of inertia formulas and the specific conditions under which they apply. There is also mention of the importance of careful calculation and rounding in the context of homework submissions.

sheepcountme
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Homework Statement


A thin rectangular slab, with dimensions 0.580 m by 0.830 m and mass 0.150 kg, is rotated about an axis passing through the slab parallel to the short edge. If the axis is 0.230 m from the short edge, what is the moment of inertia of the slab?


Homework Equations



Ip=Icm+mh^2

The Attempt at a Solution



So, I used the formula for inertia of a slap (I=1/12 x m x L^2) and plugged this in for Icm above:
Ip=1/12 x M (L^2) + M x h^2
Ip=1/12 (.150)(.83^2)+.150(.230^2)
Ip=.008611+.007935
Ip=.0165

But this wasn't correct, could you tell me where I went wrong?
 
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For problems like this I always find it useful to draw a sketch of my object along with the axes I'm taking moments of inertia around.

Having done that, I think your error is that in applying Ip=Icm+mh^2 (parallel axis theorem) you've taken H to be 0.230 - which is incorrect, since H is the distance from the centre of mass to your new axis, yet 0.230 in this case is the distance from the edge of your slab to your axis.

So you should use H = 0.185 (which is 0.830/2 - 0.230).

EDIT: Oops. I said L, but I meant H, sorry.
 
Last edited:
Also you used the moment of inertia of a rod.

You need to use the moment of inertia of a rectangular lamina which is

[tex]I_c = \frac{1}{12}M(a^2+b^2)[/tex]
 
Our book explains that I=1/12 M L^2 is also used for a slab with the axis through the center parallel to the edge. Isn't I=1/12 M (a^2 + b^2) used if the axis is through the center?
 
sheepcountme said:
Our book explains that I=1/12 M L^2 is also used for a slab with the axis through the center parallel to the edge. Isn't I=1/12 M (a^2 + b^2) used if the axis is through the center?

http://en.wikipedia.org/wiki/List_of_moments_of_inertia

[tex]Rod = \frac{1}{12}ML^2[/tex]

[tex]Rectangular Plate = \frac{1}{12}M(a^2+b^2)[/tex]
 
I'm just telling you what our book says:

http://img.photobucket.com/albums/1003/aliceinunderwear/Picture1.jpg
 
Last edited by a moderator:
I'm afraid using the L as above, and also trying to use the I=1/12 x M (a^2+b^2) were also wrong according to the book.
 
As you said, I=1/12 M L^2 is for a slab with the axis passing through the center. In this problem the axis doesn't pass through the center.
 
Yes, so I used the parallel axis theorem: Ip=Icm + Mh^2
Was this incorrect?
 
  • #10
rock.freak667 said:
http://en.wikipedia.org/wiki/List_of_moments_of_inertia

[tex]Rod = \frac{1}{12}ML^2[/tex]

[tex]Rectangular Plate = \frac{1}{12}M(a^2+b^2)[/tex]

The axis is through the centre (at least until we shift it using the parallel axis theorem), but parallel to the short edge, so the moment of inertia will actually be:

[tex]I_{cm}=\frac{1}{12}ML^2[/tex]

It's easy enough to verify this from first principles (which is normally a good idea when you're unsure if an equation is valid in a certain context) by using the definition of the moment of inertia as an integral.

Then using the parallel axis theorem and substituting:

[tex]I_{p}=\frac{1}{12}ML^2 + MH^2[/tex]

Which is the moment of inertia that you want - but of course you already figured that out. Note that here, L is 0.830m and H is the distance from the edge to the new axis (should be 0.830/2 - 0.230, just by geometry).

If it's still 'wrong', then perhaps the answer in your book is misprinted? I got:

[tex]I_{p}= 0.013745 kg m^2[/tex]

Is that the answer in your book?
 
  • #11
I misread the parallel to the edge part.
 
  • #12
Jmf - yes! Thank you so much! As it turns out I actually had it right one of the many times I calculated it but I rounded too early and our HW is online and is SO tempermental about how one enters things!
 

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