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The lever ABC of a component of a machine is hinged at B, and is subjected to a system of coplanar forces. Neglecting friction, find the magnitude of the force P to keep the lever in equilibrium.

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The lever ABC is in equilibrium under the action of the forces 200KN, 300KN, P and RB, where RB required reaction of the hinge B on the lever.

Hence the algebraic sum of the moments of above forces about any point in their plane is zero. Moment of RB and B is zero, because the line of action of RB passes through B. Taking moment about B, we get

200 × BE – 300 × CE – P × BF = 0 

since CE = BD, 

200 × BE – 300 × BD – P × BF = 0

200 × BC cos 30° – 300 × BC sin 30° – P × AB sin 60° = 0

200 × 12 × cos 30° – 300 × 12 × sin 30° – P × 10 × sin 60° = 0

P = 32.10 KN

Let 

RBH = Resolved part of RB along a horizontal direction BE 

RBV = Resolved part of RB along a horizontal direction BD 

∑H = Algebraic sum of the Resolved parts of the forces along horizontal direction 

∑v = Algebraic sum of the Resolved parts of the forces along vertical direction

∑H = 300 + RBH – P cos 20°

∑H = 300 + RBH – 32.1 cos 20° .......(i)

∑v = 200 + RBV – Psin 20°

∑v = 200 + RBV – 32.1 sin 20° ......(ii)

Since the lever ABC is in equilibrium

∑H = RV = 0, We get

RBH = –269.85KN

RBV = –189.021KN

RB = {(RBH)2 +(RBV)2}1/2

RB = {(–269.85)2 + (–189.02)2}1/2

RB = 329.45KN

Let θ = Angle made by the line of action of RB with the horizontal 

Then, tanθ = RBV/RBH = –189.021/–269.835 

θ = 35.01°

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