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Solution - American Association of Physics Teachers

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2013 F = ma Exam 1112. A spherical shell <strong>of</strong> mass M and radius R is completely filled with a frictionless fluid, also <strong>of</strong> mass M. It is releasedfrom rest, and then it rolls without slipping down an incline that makes an angle θ with the horizontal. What willbe the acceleration <strong>of</strong> the shell down the incline just after it is released? Assume the acceleration <strong>of</strong> free fall is g.The moment <strong>of</strong> inertia <strong>of</strong> a thin shell <strong>of</strong> radius r and mass m about the center <strong>of</strong> mass is I = 2 3 mr2 ; the moment<strong>of</strong> inertia <strong>of</strong> a solid sphere <strong>of</strong> radius r and mass m about the center <strong>of</strong> mass is I = 2 5 mr2 .(A) a = g sin θ(B) a = 3 4 g sin θ(C) a = 1 2 g sin θ(D) a = 3 8 g sin θ(E) a = 3 5 g sin θOne can use torque or energy to solve this problem.<strong>Solution</strong>The torque about an axis through the point <strong>of</strong> contact isThe angular acceleration is given bywhere the moment <strong>of</strong> inertia isThe acceleration is thenτ = RF sin θ = 2MgR sin θτ = IαI = 2 3 MR2 + MR 2 + MR 2 = 8 3 MR2a = αR =Alternatively, the kinetic energy <strong>of</strong> the object is2MgR sin θ83 MR2 R = 3 4 g sin θT = 1 2 (2M)v2 + 1 2 · 23 MR2 ω 2T = 4 3 Mv2The potential energy is related to the vertical position y byU = −(2M)gyand so by conservation <strong>of</strong> energyButand sod(T + U) = 0dt8 dvdyMv = −(2M)g3 dt dtdydt= −v sin θdvdt = 3 4 g sin θCopyright c○2013 <strong>American</strong> <strong>Association</strong> <strong>of</strong> <strong>Physics</strong> <strong>Teachers</strong>

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