JEE Challenger
More from Motion in a Straight Line

Displacement of Block on Oily Surface Under Exponential Velocity

A smooth flat horizontal surface is covered with a thin film of oil. A rectangular block having mass m=0.4 kgm = 0.4\text{ kg} rests on this surface. An impulse of magnitude 1.0 N s1.0\text{ N s} is imparted to the block at time t=0t = 0, causing it to move along the xx-axis with a time-dependent velocity v(t)=v0e−t/τv(t) = v_0 e^{-t/\tau}, where v0v_0 is a constant and τ=4 s\tau = 4\text{ s}. Calculate the displacement of the block, in metresmetres, at time t=τt = \tau. (Take e−1=0.37e^{-1} = 0.37).

Official Numerical Answer6.3

Step-by-Step Solution

An impulse JJ delivered to a block of mass mm initially at rest imparts an initial velocity v(0+)=v0v(0^+) = v_0. According to the impulse-momentum theorem: J=Δp=mv0−0J = \Delta p = m v_0 - 0

Given:

  • Mass of the block, m=0.4 kgm = 0.4 \text{ kg}
  • Magnitude of impulse, J=1.0 N sJ = 1.0 \text{ N s}
  • Time constant, τ=4 s\tau = 4 \text{ s}
  • e−1=0.37e^{-1} = 0.37

We can find the initial velocity v0v_0: v0=Jm=1.0 N s0.4 kg=2.5 m/sv_0 = \frac{J}{m} = \frac{1.0 \text{ N s}}{0.4 \text{ kg}} = 2.5 \text{ m/s}

The velocity of the block as a function of time tt is given by: v(t)=v0e−t/τv(t) = v_0 e^{-t/\tau}

The displacement x(t)x(t) of the block at time t=τt = \tau is obtained by integrating the velocity with respect to time from t=0t = 0 to t=τt = \tau: x(τ)=∫0τv(t) dt=∫0τv0e−t/τ dtx(\tau) = \int_{0}^{\tau} v(t) \, dt = \int_{0}^{\tau} v_0 e^{-t/\tau} \, dt

Evaluating the integral: x(τ)=v0[−τe−t/τ]0τ=v0τ(1−e−1)x(\tau) = v_0 \left[ -\tau e^{-t/\tau} \right]_{0}^{\tau} = v_0 \tau \left( 1 - e^{-1} \right)

Substituting the given and calculated values into the expression: x(τ)=(2.5 m/s)×(4 s)×(1−0.37)x(\tau) = (2.5 \text{ m/s}) \times (4 \text{ s}) \times (1 - 0.37) x(τ)=10×0.63=6.3 mx(\tau) = 10 \times 0.63 = 6.3 \text{ m}

Thus, the displacement of the block at t=τt = \tau is 6.306.30 (or 6.36.3) metres.