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Maximum Frequency Variation Received Between Oscillating Transmitter and Receiver

An audio transmitter (T) and a receiver (R) are hung vertically from two identical massless strings of length 8 m8\text{ m} with their pivots well separated along the XX axis. They are pulled from the equilibrium position in opposite directions along the XX axis by a small angular amplitude θ0=cos1(0.9)\theta_0 = \cos^{-1}(0.9) and released simultaneously. If the natural frequency of the transmitter is 660 Hz660\text{ Hz} and the speed of sound in air is 330 m/s330\text{ m/s}, the maximum variation in the frequency (in Hz) as measured by the receiver (Take the acceleration due to gravity g=10 m/s2g = 10\text{ m/s}^2) is ______

Question Diagram 1
Official Numerical Answer26 to 33

Step-by-Step Solution

To find the maximum variation in the frequency as measured by the receiver, we first determine the maximum speeds of the transmitter (TT) and the receiver (RR).

Step 1: Maximum Speed of the Pendulums

Both the transmitter and the receiver are identical simple pendulums suspended from strings of length L=8 mL = 8\text{ m}. They are released from rest from an initial angular amplitude θ0\theta_0, where cosθ0=0.9\cos\theta_0 = 0.9.

Using the principle of conservation of mechanical energy for either pendulum: mgL(1cosθ0)=12mvmax2m g L (1 - \cos\theta_0) = \frac{1}{2} m v_{\text{max}}^2

Solving for vmaxv_{\text{max}}: vmax=2gL(1cosθ0)v_{\text{max}} = \sqrt{2 g L (1 - \cos\theta_0)}

Given:

  • g=10 m/s2g = 10\text{ m/s}^2
  • L=8 mL = 8\text{ m}
  • cosθ0=0.9    1cosθ0=0.1\cos\theta_0 = 0.9 \implies 1 - \cos\theta_0 = 0.1

vmax=2×10×8×0.1=16=4 m/sv_{\text{max}} = \sqrt{2 \times 10 \times 8 \times 0.1} = \sqrt{16} = 4\text{ m/s}


Step 2: Doppler Effect Calculations

Since both pendulums are released simultaneously in opposite directions from their respective equilibrium positions, they pass through their lowest points simultaneously:

  1. Moving towards each other: Both reach their maximum speed vmax=4 m/sv_{\text{max}} = 4\text{ m/s} towards one another, yielding the maximum frequency fmaxf_{\text{max}}.
  2. Moving away from each other: Half a period later, both reach their maximum speed vmax=4 m/sv_{\text{max}} = 4\text{ m/s} directed away from one another, yielding the minimum frequency fminf_{\text{min}}.

Given parameters:

  • Natural frequency, f0=660 Hzf_0 = 660\text{ Hz}
  • Speed of sound in air, v=330 m/sv = 330\text{ m/s}

Maximum Observed Frequency (fmaxf_{\text{max}}):

fmax=f0(v+vmaxvvmax)=660×(330+43304)=660×334326676.20 Hzf_{\text{max}} = f_0 \left( \frac{v + v_{\text{max}}}{v - v_{\text{max}}} \right) = 660 \times \left( \frac{330 + 4}{330 - 4} \right) = 660 \times \frac{334}{326} \approx 676.20\text{ Hz}

Minimum Observed Frequency (fminf_{\text{min}}):

fmin=f0(vvmaxv+vmax)=660×(3304330+4)=660×326334644.19 Hzf_{\text{min}} = f_0 \left( \frac{v - v_{\text{max}}}{v + v_{\text{max}}} \right) = 660 \times \left( \frac{330 - 4}{330 + 4} \right) = 660 \times \frac{326}{334} \approx 644.19\text{ Hz}


Step 3: Maximum Variation in Frequency

The maximum variation in frequency (Δf\Delta f) is the total range between the maximum and minimum measured frequencies:

Δf=fmaxfmin\Delta f = f_{\text{max}} - f_{\text{min}}

Δf=f0(v+vmaxvvmaxvvmaxv+vmax)=f0(4vvmaxv2vmax2)\Delta f = f_0 \left( \frac{v + v_{\text{max}}}{v - v_{\text{max}}} - \frac{v - v_{\text{max}}}{v + v_{\text{max}}} \right) = f_0 \left( \frac{4 v v_{\text{max}}}{v^2 - v_{\text{max}}^2} \right)

Substituting the numerical values: Δf=660×4×330×4330242=660×528010888432.00 Hz\Delta f = 660 \times \frac{4 \times 330 \times 4}{330^2 - 4^2} = 660 \times \frac{5280}{108884} \approx 32.00\text{ Hz}

Using the approximation vvmaxv \gg v_{\text{max}}: Δff0(4vmaxv)=660×4×4330=32 Hz\Delta f \approx f_0 \left( \frac{4 v_{\text{max}}}{v} \right) = 660 \times \frac{4 \times 4}{330} = 32\text{ Hz}

The maximum variation in the frequency measured by the receiver is 32.

Maximum Frequency Variation Received Between Oscillating Transmitter and Receiver | Physics PYQ Solution - JEE Challenger