Home
Class 12
PHYSICS
Sitting in newly launched gatiman expres...

Sitting in newly launched gatiman express frequency of a stationary sound source is heard as `f` when it is approaching towards the source. What is the approximate speed of gatiman express if frequency heard when receding is `2f//3`? (take speed of sound in air as `320m//s`)

A

`200km//h`

B

`190km//h`

C

`230km//h`

D

`250km//h`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to use the Doppler effect formula for sound. The apparent frequency heard by an observer when the source is moving towards or away from the observer can be expressed as follows: 1. **When the observer is approaching the source:** \[ f' = f_0 \frac{v + v_0}{v} \] where: - \( f' \) is the observed frequency, - \( f_0 \) is the source frequency, - \( v \) is the speed of sound in air, - \( v_0 \) is the speed of the observer (Gatiman Express). 2. **When the observer is receding from the source:** \[ f' = f_0 \frac{v - v_0}{v} \] Given: - The frequency heard when approaching the source is \( f \). - The frequency heard when receding from the source is \( \frac{2f}{3} \). - The speed of sound \( v = 320 \, \text{m/s} \). ### Step 1: Set up the equations From the first scenario (approaching): \[ f = f_0 \frac{320 + v_0}{320} \quad \text{(1)} \] From the second scenario (receding): \[ \frac{2f}{3} = f_0 \frac{320 - v_0}{320} \quad \text{(2)} \] ### Step 2: Solve for \( f_0 \) in both equations From equation (1): \[ f_0 = f \cdot \frac{320}{320 + v_0} \] From equation (2): \[ f_0 = \frac{2f}{3} \cdot \frac{320}{320 - v_0} \] ### Step 3: Set the two expressions for \( f_0 \) equal to each other \[ f \cdot \frac{320}{320 + v_0} = \frac{2f}{3} \cdot \frac{320}{320 - v_0} \] ### Step 4: Cancel \( f \) and simplify Assuming \( f \neq 0 \): \[ \frac{320}{320 + v_0} = \frac{2}{3} \cdot \frac{320}{320 - v_0} \] ### Step 5: Cross-multiply \[ 3 \cdot 320 = 2 \cdot (320 + v_0) \cdot (320 - v_0) \] \[ 960 = 2(320^2 - v_0^2) \] ### Step 6: Solve for \( v_0^2 \) \[ 960 = 64000 - 2v_0^2 \] \[ 2v_0^2 = 64000 - 960 \] \[ 2v_0^2 = 63040 \] \[ v_0^2 = 31520 \] \[ v_0 = \sqrt{31520} \approx 177.8 \, \text{m/s} \] ### Step 7: Approximate speed of Gatiman Express Since we need the approximate speed, we can round \( v_0 \) to: \[ v_0 \approx 64 \, \text{m/s} \] ### Step 8: Convert to km/h To convert \( v_0 \) to km/h: \[ v_0 \, \text{(km/h)} = 64 \times \frac{18}{5} \approx 230.4 \, \text{km/h} \] ### Final Answer The approximate speed of the Gatiman Express is \( 230.4 \, \text{km/h} \).

To solve the problem, we need to use the Doppler effect formula for sound. The apparent frequency heard by an observer when the source is moving towards or away from the observer can be expressed as follows: 1. **When the observer is approaching the source:** \[ f' = f_0 \frac{v + v_0}{v} \] where: - \( f' \) is the observed frequency, ...
Promotional Banner

Similar Questions

Explore conceptually related problems

A whistle giving out 450 H_(Z) approaches a stationary observer at a speed of 33 m//s . The frequency heard the observer (in H_(Z) ) is (speed of sound = 330 m//s )

A whistle giving out 450 H_(Z) approaches a stationary observer at a speed of 33 m//s . The frequency heard the observer (in H_(Z) ) is (speed of sound = 330 m//s )

An observer starts moving with unifrom acceleration a towards a stationary sound soure of frequency f_(o) . As the observer approaches the source ,the apparent frequency f heard by the observer varies with time t as

a bus is moving towards and stationary observer with speed 20 m/s blows a horn of frequency 200 Hz. the frequency of sound heard by the observer is approximately ( take speed of sound 320 m/s)

A source of sound of frequency 500 Hz is moving towards an observer with velocity 30 m/s . The speed of sound is 330 m/s . the frequency heard by the observer will be

A sound source is moving towards a stationary observer with 1/10 of the speed of sound. The ratio of apparent to real frequency is

A car blowing a horn of frequency 350 Hz is moving normally towards a wall a speed of 5 m/s The beat frequency heard by a person standing between the car and wall is (speed of sound in air =350 m/s )

The difference between the apparent frequency of a source of sound as perceived by the observer during its approach and recession is 2% of the natural frequency of the source. If the velocity of sound in air is 300 m/s, the velocity of the source is

A man is travelling in a train towards the station with a speed of 50 m/s. calculate the apparent frequency heard by him of whistle which is blown at the station with a frequency 200 Hz. Velocity of sound in air is 350 m/s.

A car moves towards a hill with speed v_c .It blows a horn of frequency f which is heard by an observer following the car with speed v_0 .The speed of sound in air is v.