A spool is pulled at an angle θ with the horizontal on a rough horizontal surface as shown in the figure. If the spool remains at rest, the angle θ is equal to
A
cos−1(Rr)
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B
π−sin−1(√1−r2R2)
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C
sin−1(rR)
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D
cos−1(rR)
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Solution
The correct option is Dcos−1(rR)
Let F= applied force and f= force of friction (left wards)
As spool is in equilibrium, ∴Fcosθ=f.....(1)
Net torque about centre =0 F.r=fR ⇒FR=fr⇒Ff=Rr ⇒fF=rR......(2)
From equation (1) and (2) cosθ=rR ⇒θ=cos−1(rR)