Moments of inertia of a rectangular plate

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The discussion focuses on proving that the moment of inertia (MOI) of a rectangular plate around its diagonal is equal to that around a line parallel to one of its edges through the center. The initial calculation involved dividing the plate into triangles and rectangles, leading to the conclusion that the MOI is the same for both axes due to symmetry. Participants suggest that understanding principal axes can simplify the analysis, emphasizing that any axis in the plane of the square will yield the same MOI. A request for simpler resources on the topic is made, avoiding complex mathematical concepts like determinants and tensors. Ultimately, the symmetry of the square is key to understanding the equality of the moments of inertia.
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Homework Statement


Show that the moment of inertia of a rectangular plate round it's diagonal, line B-B is equal to the one round a line parallel to one of the edges and passing through the center, line C-C

Homework Equations


Moment of inertia: ##I=mr^2##

The Attempt at a Solution


For the first case, round the diagonal: the MOI of a straight angle and isosceles triangle round one of the 2 identical edges is ##I=\frac{1}{6}ma^2##, and if i divide the plate into 4 such rectangles and calculate MOI it equals the one round line C-C.
But is there an easier way?
 

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Depending on your background knowledge, the symmetry of the square will tell you that they have to be equal.
 
Orodruin said:
Depending on your background knowledge, the symmetry of the square will tell you that they have to be equal.
I have little background knowledge, please hint the subject that i have to study, is it principal axes? as far as i (think) i know i can't know anything about the MOI itself around principal axis, especially if they aren't orthogonal, but i am not sure.
Please guide me to a book or publication that explains this topic, but, if possible, without the complexity of determinants, tensors etc.
 
Last edited:
You can do it with principal axes, but all that is required is noting that an axis through the corners is a linear combination of the axes through the center and the center of the sides, which must have the same moment of inertia due to symmetry.
 
Orodruin said:
all that is required is noting that an axis through the corners is a linear combination of the axes through the center and the center of the sides, which must have the same moment of inertia due to symmetry.
So i just have to know the formula for modifying MOI with the changing of the angle of the axis?
 
If you want to call it a formula, fine. The point is that any axis in the plane of the square has the same moment of inertia because the axes spanning the plane do.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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