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Question: A stationary source sends forth monochromatic sound with speed $v = 330$ m/s. A wall is moving towar...

A stationary source sends forth monochromatic sound with speed v=330v = 330 m/s. A wall is moving towards it with speed u=33u = 33 cm/s. How does the observed wavelength change after reflection from the wall?

A

decreases by 0.2%

B

increases by 0.2%

C

decreases by 0.1%

D

increases by 0.1%

Answer

decreases by 0.2%

Explanation

Solution

The problem involves the Doppler effect for sound waves, occurring in two stages:

  1. Sound waves from the stationary source incident on the moving wall.
  2. Sound waves reflected from the wall (which acts as a moving source) back into the medium.

Let:

  • vv be the speed of sound in the medium (v=330v = 330 m/s).
  • uu be the speed of the wall (u=33u = 33 cm/s = 0.330.33 m/s).
  • ff be the frequency of the sound emitted by the stationary source.
  • λ\lambda be the wavelength of the sound emitted by the stationary source.

The original wavelength is λ=vf\lambda = \frac{v}{f}.

Step 1: Frequency observed by the wall (ff').

The wall acts as an observer moving towards a stationary source. The formula for the observed frequency when an observer moves towards a stationary source is:

f=f(v+uv)f' = f \left( \frac{v + u}{v} \right)

Step 2: Frequency of the sound reflected from the wall (ff'').

The wall now acts as a source emitting sound of frequency ff'. This source (the wall) is moving towards the original source's position (or effectively, towards a stationary observer in the medium). The formula for the observed frequency when a source moves towards a stationary observer is:

f=f(vvu)f'' = f' \left( \frac{v}{v - u} \right)

Substitute the expression for ff' into the equation for ff'':

f=f(v+uv)(vvu)f'' = f \left( \frac{v + u}{v} \right) \left( \frac{v}{v - u} \right)

f=f(v+uvu)f'' = f \left( \frac{v + u}{v - u} \right)

Step 3: Wavelength of the reflected sound (λ\lambda'').

The wavelength of the reflected sound in the medium is given by λ=vf\lambda'' = \frac{v}{f''}. Substitute the expression for ff'':

λ=vf(v+uvu)\lambda'' = \frac{v}{f \left( \frac{v + u}{v - u} \right)}

λ=vf(vuv+u)\lambda'' = \frac{v}{f} \left( \frac{v - u}{v + u} \right)

Since λ=vf\lambda = \frac{v}{f}, we have:

λ=λ(vuv+u)\lambda'' = \lambda \left( \frac{v - u}{v + u} \right)

Step 4: Percentage change in wavelength.

The change in wavelength is Δλ=λλ\Delta \lambda = \lambda'' - \lambda. The percentage change is Δλλ×100%\frac{\Delta \lambda}{\lambda} \times 100\%.

Δλλ=λλλ=λ(vuv+u)λλ\frac{\Delta \lambda}{\lambda} = \frac{\lambda'' - \lambda}{\lambda} = \frac{\lambda \left( \frac{v - u}{v + u} \right) - \lambda}{\lambda}

Δλλ=(vuv+u)1\frac{\Delta \lambda}{\lambda} = \left( \frac{v - u}{v + u} \right) - 1

Δλλ=(vu)(v+u)v+u\frac{\Delta \lambda}{\lambda} = \frac{(v - u) - (v + u)}{v + u}

Δλλ=vuvuv+u\frac{\Delta \lambda}{\lambda} = \frac{v - u - v - u}{v + u}

Δλλ=2uv+u\frac{\Delta \lambda}{\lambda} = \frac{-2u}{v + u}

Now, substitute the given values:

v=330v = 330 m/s u=0.33u = 0.33 m/s

Percentage change =(2×0.33330+0.33)×100%= \left( \frac{-2 \times 0.33}{330 + 0.33} \right) \times 100\%

Percentage change =(0.66330.33)×100%= \left( \frac{-0.66}{330.33} \right) \times 100\%

Percentage change 0.00199806×100%\approx -0.00199806 \times 100\%

Percentage change 0.1998%\approx -0.1998\%

Rounding to one decimal place, the percentage change is approximately 0.2%-0.2\%. The negative sign indicates a decrease in wavelength.

Thus, the observed wavelength decreases by 0.2%.