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NEET Hard

A block of mass m is placed on a smooth inclined wedge ABC of inclination  as shown in the figure. The wedge is given an acceleration 'a' towards the right. The relation between a and  for the block to remain stationary on the wedge is

A

a=gcosθa = g \cos \theta

B

a=gsinθa = \frac{g}{\sin \theta}

C

a=gcosec θa = \frac{g}{\text{cosec } \theta}

D

a=gtanθa = g \tan \theta

Step-by-Step Solution

In non-inertial frame,

Nsinθ=ma(i)N \sin \theta = ma \quad \dots(i)

Ncosθ=mg(ii)N \cos \theta = mg \quad \dots(ii)

Dividing equation (i) by (ii), we get: tanθ=ag\tan \theta = \frac{a}{g}

a=gtanθa = g \tan \theta

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