(c) Here, $\sin\theta = \frac{1}{l}$
[image:5_image177.emf]
Let required acceleration of inclined plane to be $a$ for the object to remain stationary relative to incline, we have
$ma\cos{\theta = mg\sin\theta}$
$a = g\tan\theta = g\frac{1}{\sqrt{l^{2} - 1}}$