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Q. A block is kept on a frictionless inclined surface with angle of inclination $\alpha$ as shown in figure. The incline is given an acceleration $a$ to keep the block stationary. Then $a$ is equal to
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Laws of Motion

Solution:

The incline is given an acceleration $a$. Acceleration of the block is to the right. Pseudo acceleration $a$ acts on the block to the left. As it is clear from figure, the block will remain stationary, when
$m a \cos \alpha=m g \sin \alpha$ or $a=\frac{g \sin \alpha}{\cos \alpha}=g \tan \alpha$
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