Moment of Inertia: Calculation Method

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The discussion focuses on calculating the ratio of the moment of inertia of a circle to that of a square with the same area about their centroidal axis. The derived formula indicates that the ratio is influenced by the dimensions of both shapes, specifically through the relationship between their areas. Clarifications are made regarding the interpretation of the centroidal axis, emphasizing the importance of consistency in the chosen axis for accurate calculations. A correction is noted in the final step of the calculation, reinforcing the need for precision in mathematical expressions. Overall, the conversation highlights the nuances in calculating moments of inertia for different geometric shapes.
Benjamin_harsh
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Homework Statement
Ratio of moment of inertia of a circle and that of a square having same area about their centroidal axis is:
Relevant Equations
Why they calculated ##\large\frac{d}{a}## in first step?
Ratio of moment of inertia of a circle and that of a square having same area about their centroidal axis is:

Sol: both area and square have same area:

##a^2 = \large\frac{π}{4}\normalsize d^{2}; \large\frac{d}{a} =\large \sqrt\frac{4}{p}##

Ratio of moment of inertia of a circle and that of a square about their centroidal axis is:

##\large\frac{I_{c}}{I_{s}} = \large\frac{\frac{π}{64}d^4}{\frac{a^{4}}{12}} = \large\frac{12π}{64}\frac{d}{a}^{4}##

##\large\frac{3π}{16}(\sqrt\frac{4}{p})^{4} = \frac{3}{π}##
 
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It could have been calculated later, but that ratio is needed for the equal areas
is
 
Benjamin_harsh said:
moment of inertia of a circle and that of a square having same area about their centroidal axis
These questions you are working through keep referring, ambiguously, to "the" centroidal axis. I have tended to assume they mean the one normal to the plane. In the present question it doesn’t matter whether it is that axis or any axis in the plane as long as the choice is consistent, but looking at the detailed calculation they seem to be referring to an axis in the plane. If they meant normal to the plane then both values would be doubled.
Interesting...
 
Correction in last step: ##\large\frac{3π}{16}(\sqrt\frac{4}{π})^{4} = \large \frac{3}{π}##.
 
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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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