
To solve this problem, we need to determine the distance covered by a particle projected from the bottom of an inclined plane with an initial speed \( u \) before it comes to rest. The plane is inclined at an angle \( \theta \) with the horizontal.
The only force acting against the motion along the inclined plane is the component of gravity. This component is \( g \sin \theta \), where \( g \) is the acceleration due to gravity.
Using the equations of motion, the final velocity \( v \) at the point where the particle comes to rest is 0. The initial velocity \( u \) and the acceleration is \( -g \sin \theta \) (negative because it opposes the motion).
The equation of motion is:
\(v^2 = u^2 + 2as\)
Substituting the known values (with \( v = 0 \), \( a = -g \sin \theta \)), we get:
\(0 = u^2 - 2g \sin \theta \cdot s\)
Solving for \( s \):
\(u^2 = 2g \sin \theta \cdot s\)
Therefore, the distance \( s \) is:
\(s = \frac{u^2}{2g \sin \theta}\)
Thus, the correct answer is \(\frac{u^2}{2g \sin \theta}\), which matches the first option.

