
(d) The situation is as shown in the figure
[image:5_image211.jpeg]
The equation of motion for body B.
$2mg\sin{45{^\circ} - \mu_{1}R_{1} - T_{1} - T_{2} = 2ma}$
$2mg\sin{45{^\circ} - \frac{1}{3}2mg\cos{45{^\circ} - T = 2ma}}$
$\Longrightarrow \ \ \ 2mg \times \frac{1}{\sqrt{2}} - \frac{1}{3}2mg\ \times \frac{1}{\sqrt{2}} - T = 2ma\ \ \ldots.(i)$
In the problem as $\left( m_{B} - m_{A} \right)g\cos{\theta = (mg/\sqrt{2}})$ is lesser than
$\left( \mu_{B}m_{B} + \mu_{A}m_{A} \right)g\cos{\theta = (4mg/3\sqrt{2})}\ $ the masses will not move and hence.
Acceleration of B = acceleration of A = 0.