Finding the Angle in Radial-Transverse Motion: A Scientific Approach

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The discussion focuses on solving a physics problem related to radial-transverse motion, specifically finding the angle at which an object is about to slip. Participants emphasize the importance of analyzing forces acting on the object and using free body diagrams to derive equations. They suggest breaking down equilibrium equations into radial and transverse components to find the angle. The condition of impending slip indicates that static friction is about to be overcome by gravitational forces. Overall, the conversation provides guidance on applying these principles to determine the required angle.
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Hi Jason03,

You follow the same procedure as you did part a. At point B (right before it slips) you know the total acceleration (magnitude and direction.) What forces are acting on the object? What information does being on the verge of slipping tell you? From your free body diagram you can write the components of the forces; some of these will contain theta and you can then solve for theta. What do you get?
 
You say that I know the acceleration, so does that mean its the same as in part A?...and the condition right before it slips is when static friction is about to be overcome by the force of gravity.
 
Hi, Jason. It's been a while but I will try to get you started. I will assume that you have already drawn your FBD and KD for when the block is just about to slip. Breaking Equilibrium equations into radial and transverse components should be your next move. What do have so far?
 
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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