As shown in figure, there is a flat plank at rest on a very slippery surface. You have disc of radius a and mass equal to the mass of the disc (say M). You rotated the disc with an initial angular speed
Both v should be the same.
"\\mu gt=\u03c9_0\u03b1 -3 \\mu gt \\\\\n\n\u03c9_0\u03b1= 4 \\mu gt \\\\\n\nt = \\frac{\u03c9_0\u03b1}{\\mu g}"
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