cube root of the initial velocity
square of the initial velocity
The stopping distance \( d \) of a moving vehicle is related to the initial velocity \( v_0 \) by the work-energy principle. The kinetic energy of the vehicle is given by:
\[ E_k = \frac{1}{2} m v_0^2 \]
Where: - \( m \) is the mass of the vehicle, - \( v_0 \) is the initial velocity. The work done by the braking force \( F \) is equal to the kinetic energy, and the stopping distance \( d \) is related to the work done by the formula: \[ F \cdot d = \frac{1}{2} m v_0^2 \] Assuming that the braking force \( F \) is constant, we can solve for the stopping distance \( d \): \[ d \propto \frac{v_0^2}{F} \] Since the braking force is constant, we can conclude that the stopping distance is proportional to the square of the initial velocity \( v_0 \). Thus, the correct relationship is: \[ d \propto v_0^2 \] Therefore, the stopping distance is proportional to the square of the initial velocity.
Correct Answer: (D) square of the initial velocity
A body of mass 1000 kg is moving horizontally with a velocity of 6 m/s. If 200 kg extra mass is added, the final velocity (in m/s) is: