To solve the problem of finding the velocity of the car, we utilize the Doppler effect, which describes the change in frequency or wavelength of a wave in relation to an observer moving relative to the wave source.
The frequency \( f' \) of the sound heard by the driver after it reflects off the cliff can be related to the original frequency \( f \) and the velocity of the car, \( v_c \), using the Doppler Effect formula for sound:
First, consider the sound wave emitted by the car horn as it approaches the cliff:
\( f' = \left(\frac{v+v_c}{v}\right)f \)
Where:
Next, the sound wave reflects off the cliff and moves back towards the car. As the car is also moving towards the source (cliff), the frequency observed by the driver is altered again:
\( f'' = \left(\frac{v}{v-v_c}\right)f' \)
Given that the overall reflected frequency \( f'' = 2f \), we substitute for \( f' \):
\( 2f = \left(\frac{v}{v-v_c}\right)\left(\frac{v+v_c}{v}\right)f \)
Simplifying this equation:
\( 2 = \left(\frac{v+v_c}{v-v_c}\right) \)
Cross-multiply to solve for \( v_c \):
\( 2(v-v_c) = v+v_c \)
\( 2v - 2v_c = v + v_c \)
\( 2v - v = 3v_c \)
\( v = 3v_c \)
Thus, the velocity of the car \( v_c \) is:
\( v_c = \frac{v}{3} \)
Therefore, the correct answer is: \( \frac{v}{3} \)
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: