Moment of Inertia of equilateral triangle about vertex

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SUMMARY

The moment of inertia of a thin uniform wire bent into an equilateral triangle about a vertex is calculated using the principles of slender rods and the parallel axis theorem. The correct approach involves treating each side of the triangle as a slender rod, with the mass M representing the total mass of the wire. The final moment of inertia is derived as I = (1/2)Mb², correcting the initial miscalculation of (3/2)Mb² by recognizing that M should be divided by 3 for each side.

PREREQUISITES
  • Understanding of moment of inertia concepts
  • Familiarity with the parallel axis theorem
  • Knowledge of slender rod moment of inertia equations
  • Basic geometry, particularly properties of equilateral triangles
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  • Study the derivation of the moment of inertia for various geometric shapes
  • Learn about the parallel axis theorem in greater detail
  • Explore applications of moment of inertia in real-world engineering problems
  • Investigate the effects of mass distribution on rotational dynamics
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Students in physics or engineering courses, particularly those studying mechanics, as well as educators looking for examples of moment of inertia calculations involving complex shapes.

oohaithere
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Homework Statement


A piece of thin uniform wire of mass m and length 3b is bent into an equilateral triangle. Find the moment of inertia of the wire triangle about an axis perpendicular to the plane of the triangle and passing through one of its vertices.

Homework Equations


Slender rod, axis through one end: I=\frac 1 3ML2
Parallel axis theorem: Ip=Icm+Md2
Slender rod, axis through center: I=\frac {1} {12}ML2

The Attempt at a Solution


First I drew the figure as an equilateral triangle with the axis at the top point and set each side equal to B.[/B]

34qlqms.jpg


Then I considered the 2 sides to be slender rods with the axis through one end.
So, ΣI=\frac 1 3Mb2+\frac 1 3Mb2

The third side I figured would be a slender rod with the axis in the middle but moved up a distance d which would equal \sqrt{ b^2- {\frac 1 4} b^2 }.

Ip=\frac {1} {12}Mb2+M\sqrt{ b^2- {\frac 1 4} b^2 }2

Then I added them all up to get the moment of inertia for the whole triangle.

ΣI=\frac 1 3Mb2+\frac 1 3Mb2+\frac {1} {12}Mb2+Mb2-\frac 1 4Mb2

But I get \frac 3 2Mb2 when the answer is supposed to be \frac 1 2Mb2.

Am I maybe missing a negative or calculating one of the moments wrong?
 
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Hello there, haithere, :welcome:
Is M the mass of one side, or of the whole thing ?
 
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BvU said:
Hello there, haithere, :welcome:
Is M the mass of one side, or of the whole thing ?
M is the mass of the whole wire so should I be using M/3 for the value of M in each moment I'm adding?
edit: I tried it and it works thanks for pointing that out
 
can you show how you found the distance d?
'
 
Hello Muz, :welcome:

Thing to do in PF is start your own thread instead of continuing someone else's solved thread.

Never mind: if you cut an equilateral triangle (sides length b) in half you can use Pythagoras to find ##d^2 = b^2 - ({1\over 2}b)^2 \ \ ##
 

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