Angular Momentum of Particle in Hollow Half-Ball: Calculation

AI Thread Summary
The discussion revolves around calculating the speed V_0 required for a particle to reach the top of a hollow half-ball, given its mass m and initial angle θ_0. The participant initially struggles with understanding the forces at play, including gravitational, normal, and centrifugal forces, and how to combine them in the context of angular momentum. They consider using the principle of conservation of angular momentum and energy to solve the problem. Ultimately, they successfully apply energy conservation methods to find the solution efficiently. The conversation highlights the importance of correctly identifying and applying physical principles in mechanics.
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Hello!
http://img151.imageshack.us/img151/6571/cques1vd5.gif

Homework Statement


A particle with mass m is thrown in lateral speed V_0 inside a hollow half-ball with radius R. At the beginning of it's motion the ball has an angle of \theta_0 from the perpendicular.
The gravitational force will pull the particle toward the center of the ball, while the centrifugal force will push it outwards.
Calculate the speed V_0, as a function of \theta_0, needed for the particle to reach the top of the half-ball in the peek of its motion.
Important! there's no string attached to the ball. The line on the image just indicates the radius.

Homework Equations


\overline J=m\overline r \times \overline v
\overline \omega=\overline{ \omega_0} + \overline\alpha t

The Attempt at a Solution



Well, the problem is I don't understand the forces involved.
I know there some sort of J_0 here, because there's an \overline r and a \overline v. I can also draw a forces equation. Then there's the Normal force against mg and centrifugal force (btw - can I use the centripetal force instead?), but I don't quite know how to combine the two - F and J - together.

Thank you.

[edit]
I thought of something: there are three forces: N, mg, \frac{mv^2}{R}.
also, I can do something like this: \Delta J = J_{end}-J_{start}, and J_{end}=0, because on the peak of the motions happens when v=0. also, J_{start}=mv_0R(sin\theta+cos\theta).
and also \frac{dJ}{dt}=r \times F
so if I only knew how to play the forces right, I would have it.
Is it correct? if so, how do I know the force equation?
 
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I'm not completely sure, but the N force is probably the centripetal force because it's always pointed towards the center. It is the component of ball's weight and it's equal to weight at the bottom of the half-ball.

Maybe you can solve this by using energies.
 
Thanks!
I did it with energies and it worked perfectly (through one line :) ).
 
Kindly see the attached pdf. My attempt to solve it, is in it. I'm wondering if my solution is right. My idea is this: At any point of time, the ball may be assumed to be at an incline which is at an angle of θ(kindly see both the pics in the pdf file). The value of θ will continuously change and so will the value of friction. I'm not able to figure out, why my solution is wrong, if it is wrong .
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