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°