Calculate the rotational inertia of a solid hexagonal

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Homework Help Overview

The discussion revolves around calculating the rotational inertia of a solid hexagonal shape. Participants are exploring the integration methods and geometric considerations necessary for the calculation, particularly focusing on the choice of integration elements and the implications of the axis of rotation.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the integration of mass elements and the choice of variables for integration, questioning the appropriateness of using rectangular strips versus other shapes. There is also consideration of the parallel axis theorem and its relevance to the problem.

Discussion Status

The discussion is active, with participants providing insights and questioning each other's assumptions. Some guidance has been offered regarding the use of standard results and the implications of different integration approaches. However, there is no explicit consensus on the best method yet.

Contextual Notes

Participants note the need for clarity regarding the axis of rotation, which is confirmed to be perpendicular to the hexagon. There are also references to the geometric constraints of the hexagon and the integration elements being used.

Yalanhar
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Homework Statement
Calculate the rotational inertia of a solid hexagonal (side = R) about an axis perpendicular through its center.
Relevant Equations
##I=\int r^2 dm##
What I did:

##\frac{dm}{dA} = \frac{M}{\frac{3\sqrt3 R^2}{2}}##

##dm = \frac{2M}{3\sqrt3 R^2} dA## (1)

##dA=3\sqrt3 rdr## (2)

(2) in (1)

##dm = \frac{2M}{3\sqrt3 R^2} 3\sqrt3 rdr##

Now in the integral

##I = \int \frac{r^2 2Mrdr}{R^2}##

How can I solve the integral interval? I think I need to change respect to ##\theta## and integrate over 2##\pi##. Or can I change r in the integral and integrate considering dA? Then the interval would be 0 to A (## A = \frac{3\sqrt3 R^2}{2}##.

I don't quite understand how i choose the interval. In a rod to it's center is -l/2 to +l/2, but in a ring it goes from 0 to R. Why not -R to +R?
Thanks
 
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You appear to have taken the integration element to be a rectangular strip, so the points along it are not equidistant from the hexagon's centre.

If you only had a thin rectangular strip to worry about, what standard results would you employ?
 
haruspex said:
You appear to have taken the integration element to be a rectangular strip, so the points along it are not equidistant from the hexagon's centre.

If you only had a thin rectangular strip to worry about, what standard results would you employ?
Yes, i see now that if I use dr or d##\theta## it won't help me. I think I'm confusing r (distance of a infinitesimal part to the axis) to r (infinitesimal side of hexagon)
 
Yalanhar said:
Yes, i see now that if I use dr or d##\theta## it won't help me. I think I'm confusing r (distance of a infinitesimal part to the axis) to r (infinitesimal side of hexagon)
Well, you can use dθ and integrate along the strip, but there is an easier way using a couple of standard results, as I hinted.
 
haruspex said:
You appear to have taken the integration element to be a rectangular strip, so the points along it are not equidistant from the hexagon's centre.

If you only had a thin rectangular strip to worry about, what standard results would you employ?
I would use ##dA = dxdy## The rectangles are for summing them from one side and then complete the hexagon?
 
Are you familiar with the parallel axis theorem ?
 
Yalanhar said:
I would use ##dA = dxdy## The rectangles are for summing them from one side and then complete the hexagon?
They are very thin rectangles, effectively rods.
Plus what BvU asked.
 
haruspex said:
They are very thin rectangles, effectively rods.
Plus what BvU asked.
I know the theorem. I saw someone doing this theorem for 6 triangles. He calculed the moment on the center for each triangle with the theorem and summed them up. But I didnt understand the rectangle, the rectangle itself can't fill the hexagon, for the x changes between the differents dy
 
I can see that the parallel axis theorem would be useful if the axis of rotation is in the same plane as the hexagon. Is that the case, or is the axis perpendicular to the hexagon? The problem as you have stated it in the original post leaves that question unanswered.
 
  • #10
[QUOperpendicularmr post: 6260489, member: 639870"]
I can see that the parallel axis theorem would be useful if the axis of rotation is in the same plane as the hexagon. Is that the case, or is the axis perpendicular to the hexagon? The problem as you have stated it in the original post leaves that question unanswered.
[/QUOTE]
Its perpendicur. Sorry
 
  • #11
Suppose you divide the hexagon into ##12## congruent triangles, each with one vertex at the center of the hexagon. Then you could integrate ##\rho r^2## over one triangle and multiply by ##12## to get the result.
 
  • #12
Yalanhar said:
But I didnt understand the rectangle
You did not post a diagram, but I presumed from your algebra that your integration element consisted of a narrow trapezoidal strip parallel to one side of the hexagon (or maybe six such, forming a hexagon).
Concentrating one one such strip, being so narrow, it is effectively a rod. What is the moment of a rod about its centre?
tnich said:
I can see that the parallel axis theorem would be useful if the axis of rotation is in the same plane as the hexagon.
It's useful regardless.
 

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