Exactly one turn of a flexible rope with mass m is wrapped around a uniform cylinder with mass M and radius R The cylinder rotates without friction about a horizontal axle along the cylinder axis. One end of the rope is attached to the cylinder. The cylinder starts with angular speed wo. After one revolution of the cylinder the rope has unwrapped and, at this instant, hangs vertically down, tangent to the cylinder. Part A Find the angular speed of the cylinder at this time. You can ignore the thickness of the rope. (Hint: Use Equation U = Mgyem ) Express your answer in terms of the variables m, M, R, wo, and the acceleration due to gravity g. Πνα ΑΣφ Part B

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Chapter12: Rotation I: Kinematics And Dynamics
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Exactly one turn of a flexible rope with mass m is wrapped
around a uniform cylinder with mass M and radius R. The
cylinder rotates without friction about a horizontal axle along
the cylinder axis. One end of the rope is attached to the
cylinder. The cylinder starts with angular speed wo. After one
revolution of the cylinder the rope has unwrapped and, at this
instant, hangs vertically down, tangent to the cylinder.
Part A
Find the angular speed of the cylinder at this time. You can ignore the thickness of the rope. (Hint: Use Equation U = Mgyem -)
Express your answer in terms of the variables m, M, R, wo, and the acceleration due to gravity g.
| ν ΑΣφ
?
Part B
Find the linear speed of the lower end of the rope at this time.
Express your answer in terms of the variables m, M, R, wo, and the acceleration due to gravity g.
Hνα ΑΣφ
?
v =
Transcribed Image Text:Exactly one turn of a flexible rope with mass m is wrapped around a uniform cylinder with mass M and radius R. The cylinder rotates without friction about a horizontal axle along the cylinder axis. One end of the rope is attached to the cylinder. The cylinder starts with angular speed wo. After one revolution of the cylinder the rope has unwrapped and, at this instant, hangs vertically down, tangent to the cylinder. Part A Find the angular speed of the cylinder at this time. You can ignore the thickness of the rope. (Hint: Use Equation U = Mgyem -) Express your answer in terms of the variables m, M, R, wo, and the acceleration due to gravity g. | ν ΑΣφ ? Part B Find the linear speed of the lower end of the rope at this time. Express your answer in terms of the variables m, M, R, wo, and the acceleration due to gravity g. Hνα ΑΣφ ? v =
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