Center of mass of fluid in rotating cylinder

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The discussion focuses on deriving the equation for the locus of the center of mass of a fluid in a rotating cylindrical canister as it pivots around a rod. The canister has a specified height and radius, and the fluid's volume is limited to a fraction of the cylinder's capacity. It is assumed that the fluid remains stationary at each angle of tilt, ensuring that its surface remains horizontal, which simplifies the determination of its shape and center of mass. The challenge lies in conceptualizing the method to solve for the center of mass as the cylinder tilts from -80 to +80 degrees. The discussion emphasizes the importance of maintaining a slow pivot to avoid complex fluid dynamics.
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Homework Statement


A closed cylindrical canister with central axis coincident with the Z axis has a height H and a radius R. It is suspended by a rod coincident with the Y axis that passes through the canister, transecting its central axis at a height h above the bottom surface of the canister with h > 0.5H.
A volume V of a uniform fluid with density d is placed in the canister (V ≤ 0.2∏R^2H). Derive the equation describing the locus in the XZ plane of the center of mass of the fluid as the cylinder pivots around the rod such that the axis of the cylinder with respect to the Z axis varies from -80 to +80 degrees.


Homework Equations


V=∏R^2H
For other equations see http://mathworld.wolfram.com/CylindricalWedge.html
and http://mathworld.wolfram.com/CylindricalSegment.html.



The Attempt at a Solution


I have been working on this for a week and cannot seem to conceptualize a method for solving the problem. I would greatly appreciate any help and/or suggestions.
 
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I think you need to assume that the fluid is stationary at any position of the cylinder. Meaning that the cylinder moves very very slowly. Because if not, arbitrary motions of the cylinder could produce very violent motions in the fluid, which one could model only numerically.

Assuming the fluid is stationary at every angle of tilt, its surface must be horizontal. That's enough to determine its shape and with the shape its center of mass. Then you do this for all the possible angles of tilt, and you get the locus.
 
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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