Question #125351

A ladder rests in limiting equilibrium against a rough vertical wall and with its foot on rough horizontal ground, the coefficient of friction at both points of contact being 0.5. The ladder is uniform and weighs 300N. Find the angle

Expert's answer


The forces equilibrium conditions give


Fx=0:  N1Ff2=0;Fy=0:  N2+Ff1mg=0\sum F_x=0:\; N_1-F_{f2}=0;\\ \sum F_y=0:\; N_2+F_{f1}-mg=0


The friction force is related with normal reaction by relation

Ff1=μN1;Ff2=μN2F_{f1}=\mu N_1;\: F_{f2}=\mu N_2

Hence


N2=mgμ2+1,N1=μmgμ2+1N_2=\frac{mg}{\mu^2+1},\: N_1=\frac{\mu mg}{\mu^2+1}

The momentum equilibrium condition gives


Ff1Lcosα+N1LsinαmgL2cosα=0F_{f1}L\cos\alpha+N_1L\sin\alpha-mg\frac{L}{2}\cos\alpha=0

So


tanα=mg/2Ff1N1=mg/2μN1N1\tan\alpha=\frac{mg/2-F_{f1}}{N_1}=\frac{mg/2-\mu N_1}{N_1}

=mg2N1μ=μ2+12μμ=1μ22μ=\frac{mg}{2N_1}-\mu=\frac{\mu^2+1}{2\mu}-\mu=\frac{1-\mu^2}{2\mu}

Finally

α=tan1(1μ22μ)=tan1(10.522×0.5)=37\alpha=\tan^{-1}\left(\frac{1-\mu^2}{2\mu}\right)=\tan^{-1}\left(\frac{1-0.5^2}{2\times 0.5}\right)=37^{\circ}
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