In an alien planet, an alien wants to play yo-yo. The gigantic yo-yo consists of two solid disks, each of mass and radius , connected by a central spindle of radius and negligible mass. A string is coiled around the central spindle. The yo-yo then is placed upright on a rough flat surface and the string is pulled gently with a tension of at an angle to the horizontal. The pull is gentle enough to ensure that that yo-yo does not slip nor lifts off the ground.
The acceleration of the center of mass of the yo-yo can be expressed in the form . Where is as large as possible, and =1. What is the value of ?
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This problem is quite tricky because you have to account for the rotational and linear motions. I've solved a simpler problem involving pulling a hockey puck (only one radius and disk).
For the rotational motion, we begin with the torque of the system. If we were to draw a free-body diagram, the large radius is tangential to the force of friction D (D for dissipative) while the small radius is tangential to the tension of the string. Since we have two solid disks, the moment of inertia I is M R 2 . Hence the total torque can be summed up as: R D − r T = M R 2 α = M R a or D − R r T = M a .
For the linear motion, we derive the net force T c o s ( 3 0 ) − D = 2 M a .
Substituting the value of Ma from the linear motion to the rotational motion D − R r T = 2 T c o s ( 3 0 ) − D
which can be rearranged as: D = 3 T ( c o s ( 3 0 ) + R 2 r ) .
Now we substitute this equation for D, and isolate the acceleration we arrive at the final equation: a = 3 M T ( c o s ( 3 0 ) − R r ) .
I also noticed an error with the question. The gcd(a,d) = 5.