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[SOLVED] Classical mechanics: ball rolling in a hollow sphere
This problem is from Gregory:
A uniform ball of radius a and centre G can roll without slipping on the inside surface of a fixed hollow sphere of (inner) radius b and centre O. The ball undergoes planar motion in a vertical plane through O. Find the energy conservation equation for the ball in terms of the variable \theta, the angle between the line OG and the downward vertical. Deduce the period of small oscillations of the ball about the equilibrium position.
So in summary, we have:
a: radius of ball
m: mass of ball
\theta: angle of the ball's position, relative to the vertical line connecting the center and bottom of the hollow sphere
I: moment of inertia of ball
\omega: rotational velocity of ball
T: kinetic energy of ball
V: potential energy of ball (V=0 at height \theta=\pi/2, the center of the sphere)
E: total energy of ball
g: acceleration due to gravity
I = 2/5ma^2
First of all, I'm assuming that \omega=\theta'. It sounds intuitive, but I could be wrong there.
I'm given, as a solution, that the period of small oscillation (that is, sin(\theta)=\theta) is 2\pi(7(b-a)/5g)^(1/2), which I'm not getting in my results. I have a very strong hunch that my mistake comes from bad energy equations. So, would you mind taking a look of these?
T = 1/2mv^2 + 1/2I\omega^2
v = \omega*(b-a)
So T = 1/2m(\omega*(b-a))^2 + 1/2(2/5ma^2)\omega^2
T = m\omega^2/10(7a^2-10ab+5b^2)
V = -(b-a)mgcos(\theta)
So E = T + V = that stuff
Am I correct here?
Homework Statement
This problem is from Gregory:
A uniform ball of radius a and centre G can roll without slipping on the inside surface of a fixed hollow sphere of (inner) radius b and centre O. The ball undergoes planar motion in a vertical plane through O. Find the energy conservation equation for the ball in terms of the variable \theta, the angle between the line OG and the downward vertical. Deduce the period of small oscillations of the ball about the equilibrium position.
So in summary, we have:
a: radius of ball
m: mass of ball
\theta: angle of the ball's position, relative to the vertical line connecting the center and bottom of the hollow sphere
I: moment of inertia of ball
\omega: rotational velocity of ball
T: kinetic energy of ball
V: potential energy of ball (V=0 at height \theta=\pi/2, the center of the sphere)
E: total energy of ball
g: acceleration due to gravity
Homework Equations
I = 2/5ma^2
The Attempt at a Solution
First of all, I'm assuming that \omega=\theta'. It sounds intuitive, but I could be wrong there.
I'm given, as a solution, that the period of small oscillation (that is, sin(\theta)=\theta) is 2\pi(7(b-a)/5g)^(1/2), which I'm not getting in my results. I have a very strong hunch that my mistake comes from bad energy equations. So, would you mind taking a look of these?
T = 1/2mv^2 + 1/2I\omega^2
v = \omega*(b-a)
So T = 1/2m(\omega*(b-a))^2 + 1/2(2/5ma^2)\omega^2
T = m\omega^2/10(7a^2-10ab+5b^2)
V = -(b-a)mgcos(\theta)
So E = T + V = that stuff
Am I correct here?