Moment of Inertia in Equilateral Triangle

In summary, the problem is to find the moment of inertia for a solid equilateral triangle about an axis at the triangle's vertex which is perpendicular to the plane of the triangle. Mass is given as M and the solution involves treating the triangle as 3 point masses at each vertex with 1/3 of the mass, resulting in a final moment of inertia of 2ML2/9. However, this approach is not equivalent to using calculus and treating dA like a thin rod, which would result in a different moment of inertia.
  • #1
mishima
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The problem is to find the moment of inertia for a solid equilateral triangle about an axis at the triangle's vertex which is perpendicular to the plane of the triangle. Mass is given as M.

I was wanting to treat it like 3 point masses at each vertex with 1/3 mass. Then I could use the sum definition of moment of inertia instead of the integral. The distance from axis at center of the equilateral triangle to each vertex is L/√3.

Ʃ mr2= 3(1/3 M * L2/9) = ML2/9

Then by the parallel axis theorem I can shift this out to a vertex using that same distance for a final result of

2ML2/9

I know it can be done by treating dA like a thin rod and using calculus, I was just curious why the above doesn't get the same answer. Isn't it dynamically the same to treat it like 3 1/3 masses on each vertex?
 
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  • #2
mishima said:
I was wanting to treat it like 3 point masses at each vertex with 1/3 mass.

You cannot just "move" all the mass to the vertices without getting a different moment of inertia. It is possible to make a 3-point-mass triangle that has an equivalent moment of inertia around the center of mass perpendicular to the plate, but each 1/3 of the mass would then have to be placed L/(2√6) from the center of mass and not at geometric vertex at distance L/√3. You can think of this as a partitioning the triangle into 3 identically diamond-shaped parts.

However, the moment of inertia around center of mass can be found fairly easy by standard integrals so you should probably be able to show how to get the moment of inertia following this approach.
 
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FAQ: Moment of Inertia in Equilateral Triangle

What is moment of inertia in an equilateral triangle?

Moment of inertia is a measurement of an object's resistance to changes in its rotational motion. In an equilateral triangle, it is the measure of the distribution of mass around the axis of rotation, and can be calculated using the formula I = (1/12) x m x a^2, where m is the mass of the triangle and a is the length of one side.

How is moment of inertia different in an equilateral triangle compared to other shapes?

In an equilateral triangle, the moment of inertia is evenly distributed as the shape is symmetrical. This means that the moment of inertia remains the same regardless of the axis of rotation. In other shapes, the moment of inertia may vary depending on the axis of rotation and the distribution of mass.

What factors affect the moment of inertia in an equilateral triangle?

The moment of inertia in an equilateral triangle is affected by the size and mass of the triangle. A larger triangle or one with a greater mass will have a larger moment of inertia. The distance of the axis of rotation from the center of mass also plays a role, with a larger distance resulting in a larger moment of inertia.

How is moment of inertia used in real-world applications?

Moment of inertia is an important concept in physics and engineering, and is used to design structures and machines that rotate or have rotational components. It is also used in the study of movement and stability in sports, such as gymnastics and figure skating.

Can the moment of inertia in an equilateral triangle be changed?

The moment of inertia in an equilateral triangle can be changed by altering the size or mass of the triangle, or by changing the distance of the axis of rotation from the center of mass. It can also be changed by changing the shape of the triangle to one with a different distribution of mass.

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