

The cabin rotates with angular velocity $\omega$ & radius R
$\therefore$ The particle experiences a force $\text{mR}\omega^2$
The component of $\text{mR}\omega^2$ along the groove provides the required force to the particle to move along AB.
$\therefore$ $\text{mR}\omega^2\cos\theta=\text{ma}$
$\Rightarrow\text{a}=\text{R}\omega^2\cos\theta$
length of groove = L
$\text{L}=\text{ut}+\frac{1}{2}\text{at}^2$
$\Rightarrow\text{L}=\frac{1}{2}\text{R}\omega^2\cos\theta\text{ t}^2$
$\Rightarrow\text{t}^2=\frac{2\text{L}}{\text{R}\omega^2\cos\theta}$
$\Rightarrow\text{t}=\sqrt{\frac{2\text{L}}{\text{R}\omega^2\cos\theta}}$
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