JEE Challenger
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Frequency Spread Observed by Passengers in Moving Train

Comprehension Passage

Two trains AA and BB are moving with speeds 20 m/s20\text{ m/s} and 30 m/s30\text{ m/s} respectively in the same direction on the same straight track, with BB ahead of AA. The engines are at the front ends. The engine of train AA blows a long whistle.

Assume that the sound of the whistle is composed of components varying in frequency from f1=800 Hzf_1 = 800\text{ Hz} to f2=1120 Hzf_2 = 1120\text{ Hz}. The speed of sound in still air is 340 m/s340\text{ m/s}.

The spread of frequency as observed by the passengers in train B is

Options

A

310 Hz310\text{ Hz}

Correct
B

330 Hz330\text{ Hz}

C

350 Hz350\text{ Hz}

D

290 Hz290\text{ Hz}

Step-by-Step Solution

To find the spread of frequency observed by the passengers in train B, we analyze the Doppler effect for the continuous band of frequencies emitted by the whistle.

1. Identifying the Parameters from the Passage

From the passage of IIT-JEE 2007:

  • Speed of sound in still air: v=340 m/sv = 340\text{ m/s}
  • Speed of train A: vA=20 m/sv_A = 20\text{ m/s}
  • Speed of train B: vB=30 m/sv_B = 30\text{ m/s}
  • Trains A and B are moving in the same direction on parallel tracks, with train A behind train B.
  • The whistle is blown from train A and emits a uniform spread of sound frequencies ranging from f1=800 Hzf_1 = 800\text{ Hz} to f2=1120 Hzf_2 = 1120\text{ Hz}, which gives an emitted frequency spread of:
    Δf=f2−f1=1120 Hz−800 Hz=320 Hz\Delta f = f_2 - f_1 = 1120\text{ Hz} - 800\text{ Hz} = 320\text{ Hz}

2. Doppler Effect Formulation

Since train A (the source) is moving towards train B at speed vAv_A, and train B (the observer) is moving away from train A at speed vBv_B in the same direction:

  • The sound waves travel from train A to train B in the direction of motion.
  • The frequency f′f' perceived by an observer in train B for an emitted frequency ff is given by the Doppler effect formula:
    f′=f(v−vBv−vA)f' = f \left( \frac{v - v_B}{v - v_A} \right)

3. Calculating the Spread of Observed Frequency

The observed frequency spread Δf′\Delta f' corresponds to the difference between the observed upper and lower frequencies:
Δf′=f2′−f1′=(f2−f1)(v−vBv−vA)=Δf(v−vBv−vA)\Delta f' = f_2' - f_1' = (f_2 - f_1) \left( \frac{v - v_B}{v - v_A} \right) = \Delta f \left( \frac{v - v_B}{v - v_A} \right)

Substituting the given values:

  • v=340 m/sv = 340\text{ m/s}
  • vA=20 m/sv_A = 20\text{ m/s}
  • vB=30 m/sv_B = 30\text{ m/s}
  • Δf=320 Hz\Delta f = 320\text{ Hz}

We obtain:
Δf′=320×(340−30340−20)\Delta f' = 320 \times \left( \frac{340 - 30}{340 - 20} \right)
Δf′=320×(310320)=310 Hz\Delta f' = 320 \times \left( \frac{310}{320} \right) = 310\text{ Hz}

Therefore, the spread of frequency as observed by the passengers in train B is 310 Hz310\text{ Hz}.

The correct option is A.