Moment of Inertia of a Right Triangle

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SUMMARY

The moment of inertia for a thin, uniform right triangle sign with base length b and height h, rotating about the side of length h, is calculated using the integral I = ∫r² dm. The correct approach involves expressing density (ρ) in terms of mass (m) and area (A), leading to the formula I = (1/6)Mb². The discussion highlights the importance of accurately defining the relationship between the triangle's dimensions and the integration variables to arrive at the correct result.

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Homework Statement


A metal sign for a car dealership is a thin, uniform right triangle with base length b and height h. The sign has mass m. What is the moment of inertia of the sign for rotation about the side of length h?




Homework Equations



I = \intr^{2}dm





The Attempt at a Solution




Alright so I started off by trying to convert the integral so that it is in terms of dr rather than dm. So, I calculated that dm = \rho dA.

then from there, the integral can be written as I = \ointr^{2}\rho(h/b)rdr


A little bit of simplifying will give us I = \intr^{3}\rho(h/b)dr

bounded from 0 to b.

If we solve the integral, we get I = (1/4)b^{4}\rho(h/b) - 0


Which we can simplify further to I = (1/4)b^{3}\rhoh



The only problem is, the question asks for I to be in terms of the given values, so I have to somehow change \rho into something in terms of b, h, and m. I'm not sure how to do this though because a 2D object shouldn't even have density, should it?



Thanks for the help!
 
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It has mass and area, so it has density = mass/area = m/(.5bh).

I fear you may have a mistake in the early stage where you have not shown enough detail for me to follow. I made a diagram showing a "slice" of the triangle at x, part way between x=0 and b along the base. The slice is trapezoidal but can be safely approximated as a rectangle. It's area dA = y*dx where y is the height of the slice. I think your r is my x. Tricky little relationship between y and x; I guess it is the formula for the line forming the hypotenuse. If I were you I would write out those steps carefully to make sure you have the right expression before integrating.
 
so y = mx + b and we can calculate that y = (-h/b) x assuming the point of rotation is aligned at the origin right?which means dA = (-h/b) x dxNow since r is the distance from the origin, or the point of rotation, can we say that r is equal to x and dx is equal to dr?then now that we know that density = mass/area, density equals mass/(0.5*b*h) right?
This is how I derived my integral for Inertia, but it gives me the wrong answer. What did I do wrong?
By the way the answer I got was
I = 1/2 M b^2
 
Last edited:
so y = mx + b and we can calculate that y = (-h/b) x assuming the point of rotation is aligned at the origin right?
It says "rotation about the side of length h" so it seems to me that at x = 0, we must have y = h. At x = b, y = 0. If you plug those two points into y = mx + b, you'll get a different and more complex formula for y.
 
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ah youre right.so would the equation for y then be y = -(h/b)x + h?If I use this as my equation for y, and plug it into the integral for inertia, I come up with an answer of 1/6 Mb^2.this is the correct answer. thanks for walking me through this problem. I greatly appreciate it!
 
Most welcome!
 

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