Rotational and translational energy problem

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A solid sphere is released from a height of 30 cm on a 15-degree slope and rolls without slipping to the bottom. The initial calculations for the sphere's speed at the bottom involve equating gravitational potential energy to kinetic energy, yielding a speed formula of v² = 40g. For a circular hoop, the moment of inertia is different, leading to the equation h = 40 + (1/3)R. The correct moment of inertia for the sphere is 2/5MR², which was initially miscalculated as that of a disc. The discussion highlights the importance of accurately determining the moment of inertia in rotational energy problems.
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A solid sphere of radius R is placed at a height of 30cm on a 15 deg slope. It is released and rolls, without slipping to the bottom.

a) From what height should circular hoop of radius R be released in order to equal the sphere's speed at the bottom?

First i started with the sphere
mgh=.5mv2 +.5Iw2
I=.5mR2
w=v/r
so
mgh=.5mv2+.25mv2
gh=.75v2
h=30
v2 =40g

next the hoop
the only difference is we don't know h and I is different
I=mR2
so gh=v2
therefore setting them equal, h=40.

However the answer is 43. I did neglect to include R in the height because both objects have this height R. However when i included R into h. I found 40+(1/3)R=h which leave me know where.

Any ideas? There is no mention of friction...
 
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Check your number for the sphere's moment of inertia. The value you are using is for a disc or solid cylinder.
 
Thankyou! jeez and to think i spent an hour for a little mistake. For anyone else I for a sphere is 2/5MR2
 
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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