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
sin−1(√1−r2R2)
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C
π−cos−1(rR)
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D
sin−1(rR)
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Solution
The correct option is Asin−1(√1−r2R2) Let F= the applied force and f= force of friction (leftwards) Net horizontal force =0∴Fcosθ=f.....(i) Net torque about centre =0 F⋅r=fR Substituting fR=rR in Eq.(I) we have, cosθ=rRorsinθ=√1−r2R2 ∴θ=sin−1(√1−r2R2)