- #1
bigguccisosa
- 24
- 3
Homework Statement
Imagine a ball with moment of inertia [itex]I_{cm} = \beta MR^2 [/itex] encountering a circular loop of radius [itex] R_0 > R [/itex] after rolling on a level surface at a speed of [itex]v_0[/itex]. Assume that the ball does not slip. Attached a diagram.
A) What is the minimum value of [itex] v_0[/itex] required for the ball to reach the point where the track becomes vertical?
B) What is the minimum value of [itex] v_0[/itex] required for the ball to reach the top of the track?
Homework Equations
Rotational Kinetic Energy = T = [itex] \frac{1}{2}Mv^2 + \frac{1}{2}I\omega^2 [/itex]
Total Mechanical Energy = T + U
The Attempt at a Solution
So I thought I might use energy conservation here, for part A), if the ground is taken to be zero potential energy, there is no speed when the ball just reaches the vertical track, so kinetic energy is zero, and the ball is [itex]R_0[/itex] above the ground. The centre of the ball starts [itex]R[/itex] above the ground.
[tex] MgR_0 = \frac{1}{2}Mv_0^2 + \frac{1}{2}I \omega^2 + MgR [/tex]
Replacing I and omega, [tex] MgR_0 = \frac{1}{2}Mv_0^2 + \frac{1}{2}\beta MR^2\frac{v_0^2}{R^2} + MgR [/tex]
[tex] MgR_0 - MgR = \frac{1}{2}Mv_0^2 + \frac{1}{2}\beta MR^2\frac{v_0^2}{R^2}[/tex]
[tex] Mg(R_0-R) = \frac{1}{2}Mv_0^2(1+\beta)[/tex]
solving for speed [tex] v_0 = \sqrt{\frac{2g(R_0-R)}{1+\beta}}[/tex]
For part B) did the same thing except put the height at the top of the track to be [itex]2R_0-R[/itex],
and I solved for speed again and got [tex] v_0 = 2\sqrt{\frac{g(R_0-R)}{1+\beta}}[/tex]
Is there a way to check if these are correct?, I'm unsure about how I calculated the potential energy, using the centre of mass of the ball? One of my classmates got [itex] v_0 = \sqrt{2gr_0 (1+\beta)}[/itex] for part A instead?