[SOLVED] Classical mechanics: ball rolling in a hollow sphere 1. The problem statement, all variables and given/known data 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 [tex]\theta[/tex], 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 [tex]\theta[/tex]: 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 [tex]\omega[/tex]: rotational velocity of ball T: kinetic energy of ball V: potential energy of ball (V=0 at height [tex]\theta[/tex]=[tex]\pi[/tex]/2, the center of the sphere) E: total energy of ball g: acceleration due to gravity 2. Relevant equations I = 2/5ma^2 3. The attempt at a solution First of all, I'm assuming that [tex]\omega[/tex]=[tex]\theta[/tex]'. It sounds intuitive, but I could be wrong there. I'm given, as a solution, that the period of small oscillation (that is, sin([tex]\theta[/tex])=[tex]\theta[/tex]) is 2[tex]\pi[/tex](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[tex]\omega[/tex]^2 v = [tex]\omega[/tex]*(b-a) So T = 1/2m([tex]\omega[/tex]*(b-a))^2 + 1/2(2/5ma^2)[tex]\omega[/tex]^2 T = m[tex]\omega[/tex]^2/10(7a^2-10ab+5b^2) V = -(b-a)mgcos([tex]\theta[/tex]) So E = T + V = that stuff Am I correct here?