M2 June 2014 (R) Q3
3.

A non-uniform rod, \(AB\), of mass \(m\) and length \(2l\), rests in equilibrium with one end \(A\) on a rough horizontal floor and the other end \(B\) against a rough vertical wall. The rod is in a vertical plane perpendicular to the wall and makes an angle of 60\(^\circ\) with the floor as shown in Figure 1. The coefficient of friction between the rod and the floor is \(\dfrac{1}{4}\) and the coefficient of friction between the rod and the wall is \(\dfrac{2}{3}\). The rod is on the point of slipping at both ends.
The centre of mass of the rod is at \(G\).

| Scheme | Marks |
|---|---|
| \(R = F\) | B1 |
| \(S + Q = mg\) | B1 |
| \(Q = \dfrac{2}{3}R,\ \ F = \dfrac{1}{4}S\) | B1 |
| \(Q = \dfrac{2}{3}R = \dfrac{2}{3} \times \dfrac{1}{4}S,\ \ \ S + \dfrac{1}{6}S = mg,\ \ S = \dfrac{6}{7}mg\) | M1 A1 |
| (5) |
Notes
B1 Resolve horizontally
B1 Resolve vertically (requires Q acting upwards)
B1 Use both coefficients of friction
M1 Solve to find \(S\) in terms of \(m\) & \(g\). (Can be scored if Q is acting downwards)
NB As the rod is not uniform, the use of moments equations is not helpful in part (a).
| Scheme | Marks |
|---|---|
| M\((A)\) \(\ mg \times x\cos 60 = Q \times 2l\cos 60 + R \times 2l\sin 60\) | M1 |
| M \((B)\) \(\ mg(2l - x)\cos 60 + F \times 2l\sin 60 = S \times 2l\cos 60\) | |
| M (c of m) \(\ Sx\cos 60 = Fx\sin 60 + R(2l - x)\sin 60 + Q(2l - x)\cos 60\) | A2 |
| \(mgx\cos 60 = \dfrac{1}{6} \times \dfrac{6}{7}mg \times 2l\cos 60 + \dfrac{1}{4} \times \dfrac{6}{7}mg \times 2l\sin 60\) | DM1 |
| \(\dfrac{1}{2}x = \dfrac{1}{7} \times 2l \times \dfrac{1}{2} + \dfrac{3}{14} \times l\sqrt{3}\) | |
| \(AG = x = 1.028\ldots l\ \ \ x = 1.03l\) | A1 |
| (5) | |
| (10 marks) |
Notes
M1 Moments equation – must include all terms. Condone sign errors and sin/cos confusion
A2 Correct unsimplified equation (for their \(S\).) -1 each error
DM1 Form an equation in \(x\). Depends on the preceding M
A1 \(1.03l\) or better \(\ \dfrac{l\left(2 + 3\sqrt{3}\right)}{7}\)