In the figure, suppose that the system is released from rest. R R Ignoring the effects of air resistance, show that the angular speed of the pulley after the block m, falls through a distance d can be written as 4gd(mı – Hkm2) Opulley = 2(m¡ + m2)R + M(R + R;) where Hk is the coefficient of friction between the block and the horizontal surface, M is the mass of the pulley, R1 is the inner radius of the pulley, and R2 is the outer radius of the pulley. You may assume that the pulley is a hollow cylinder.

Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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In the figure, suppose that the system is released from rest.
R R
Ignoring the effects of air resistance, show that the angular speed of the pulley after
the block m, falls through a distance d can be written as
4gd(m1 – Hkm2)
@pulley =
2(mı + m2)R; + M(R² + R;)
where Hy is the coefficient of friction between the block and the horizontal surface,
M is the mass of the pulley, R1 is the inner radius of the pulley, and R2 is the outer
radius of the pulley. You may assume that the pulley is a hollow cylinder.
Transcribed Image Text:In the figure, suppose that the system is released from rest. R R Ignoring the effects of air resistance, show that the angular speed of the pulley after the block m, falls through a distance d can be written as 4gd(m1 – Hkm2) @pulley = 2(mı + m2)R; + M(R² + R;) where Hy is the coefficient of friction between the block and the horizontal surface, M is the mass of the pulley, R1 is the inner radius of the pulley, and R2 is the outer radius of the pulley. You may assume that the pulley is a hollow cylinder.
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