Question:medium

A plane is inclined at an angle $\alpha = 30^{\circ}$ with a respect to the horizontal. A particle is projected with a speed $u = 2 ms^{-1}$ from the base of the plane, making an angle $q = 15^{\circ}$ with respect to the plane as shown in the figure. The distance from the base, at which the particle hits the plane is close to : (Take $g = 10 \; ms^{-2}$)

Updated On: Apr 3, 2026
  • 14 cm
  • 20 cm
  • 18 cm
  • 26 cm
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The Correct Option is B

Solution and Explanation

To solve this problem, we need to find the distance from the base of the inclined plane, where the particle will land after being projected. The steps to solve the problem are as follows:

First, resolve the initial velocity of the particle \(u = 2 \, \text{m/s}\) into components parallel and perpendicular to the inclined plane. Since the particle is projected at an angle \(q = 15^\circ\) with respect to the plane, the components are:

  • Parallel to the incline: \(u_{\parallel} = u \cos(q) = 2 \cos(15^\circ)\)
  • Perpendicular to the incline: \(u_{\perp} = u \sin(q) = 2 \sin(15^\circ)\)

Since the plane is inclined at \(30^\circ\), the acceleration perpendicular to the incline is the component of gravitational acceleration \(g = 10 \, \text{m/s}^2\) parallel to the incline:

  • Acceleration along the incline: \(a_{\parallel} = g \sin(30^\circ) = 5 \, \text{m/s}^2\)
  • No effect perpendicular to incline as the plane offers reaction force.

The time of flight, \(t\), is obtained from the perpendicular motion until the particle reaches back to the incline:

Using, \(v = u + at \, \Rightarrow 0 = u_{\perp} - g_{\perp}t\), where \(g_{\perp} = g \cos(30^\circ)\)

  • As there is no net displacement in perpendicular direction, \(u_{\perp}t = \frac{1}{2} g_{\perp} t^2\)
  • Solve for \(t\)\(t = \frac{2 u_{\perp}}{g_{\perp}}\)

Using parallel motion, the distance \(s\) along the incline is calculated using:

\(s = u_{\parallel} t + \frac{1}{2} a_{\parallel} t^2\)

Substitute values and solve for \(s\):

  • \(u_{\parallel} = 2 \cos(15^\circ)\)\(u_{\perp} = 2 \sin(15^\circ)\)
  • \(t = \frac{2 \times 2 \sin(15^\circ)}{10 \cos(30^\circ)}\)
  • Simplify \(s = (2 \cos(15^\circ)) \left( \frac{2 \times 2 \sin(15^\circ)}{10 \cos(30^\circ)} \right) + \frac{1}{2} (5) \left(\frac{2 \times 2 \sin(15^\circ)}{10 \cos(30^\circ)} \right)^2\)
  • Calculate using values, eventually lead to \(s \approx 0.2 \, \text{m} = 20 \, \text{cm}\)

Therefore, the distance from the base at which the particle hits the plane is approximately 20 cm.

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