Waves


Physics of Sound

  1. An observer moves towards a stationary source of sound with a speed 1/5th of the speed of sound. The wavelength and frequency of the sound emitted are λ and ƒ respectively. The apparent frequency and wavelength recorded by the observer are respectively.









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    ƒapparent =
    u + u/5
    ƒ =
    6
    ƒ = 1.2 ƒ
    u5

    Wavelength remains constant (unchanged) in this case.

    Correct Option: C

    ƒapparent =
    u + u/5
    ƒ =
    6
    ƒ = 1.2 ƒ
    u5

    Wavelength remains constant (unchanged) in this case.


  1. A whistle of frequency 385 Hz rotates in a horizontal circle of radius 50 cm at an angular speed of 20 radians s–1. The lowest frequency heard by a listener a long distance away at rest with respect to the
    centre of the circle, given velocity of sound equal to 340 ms–1, is









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    Velocity of source
    vs = rω = 0.50 × 20 = 10 ms-1

    n' =
    v
    n =
    340 × 385
    = 374 Hz
    v - vs340 + 10

    Correct Option: C

    Velocity of source
    vs = rω = 0.50 × 20 = 10 ms-1

    n' =
    v
    n =
    340 × 385
    = 374 Hz
    v - vs340 + 10



  1. A vehicle, with a horn of frequency n is moving with a velocity of 30 m/s in a direction perpendicular to the straight line joining the observer and the vehicle. The observer perceives the sound to have a frequency n + n1. Then (if the sound velocity in air is 300 m/s)









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    As the source is not moving towards or away from the observer in a straight line, so the Doppler’s effect will not be observed by the observer.

    Correct Option: B

    As the source is not moving towards or away from the observer in a straight line, so the Doppler’s effect will not be observed by the observer.


  1. A star, which is emitting radiation at a wavelength of 5000 Å, is approaching the earth with a velocity of 1.50 × 106 m/s. The change in wavelength of the radiation as received on the earth is









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    Given : Wavelength (λ) = 5000 Å
    velocity of star (v) = 1.5 × 106 m/s.
    We know that wavelength of the approaching star (λ')

    (λ') = λ
    c - v
    c

    or,
    λ'
    =
    c - v
    = 1 -
    v
    λcc

    or,
    v
    = 1 -
    λ'
    =
    λ - λ'
    =
    Δλ
    cλλλ

    Therefore,
    Δλ = λ ×
    v
    = 5000 ×
    1.5 × 106
    = 25 Å
    c3 × 10 × 108

    [where ∆λ = Change in the wavelength]

    Correct Option: C

    Given : Wavelength (λ) = 5000 Å
    velocity of star (v) = 1.5 × 106 m/s.
    We know that wavelength of the approaching star (λ')

    (λ') = λ
    c - v
    c

    or,
    λ'
    =
    c - v
    = 1 -
    v
    λcc

    or,
    v
    = 1 -
    λ'
    =
    λ - λ'
    =
    Δλ
    cλλλ

    Therefore,
    Δλ = λ ×
    v
    = 5000 ×
    1.5 × 106
    = 25 Å
    c3 × 10 × 108

    [where ∆λ = Change in the wavelength]



  1. A cylindrical resonance tube open at both ends, has a fundamental frequency, ƒ, in air. If half of the length is dipped vertically in water, the fundamental frequency of the air column will be









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    Fundamental frequency of open pipe,

    ƒ =
    v
    2l

    When half of tube is filled with water, then the length of air column becomes half
    l' =
    l
    2

    and the pipe becomes closed.
    So, new fundamental frequency
    ƒ' =
    v
    =
    v
    =
    v
    4l'4
    l
    2l
    2

    Clearly ƒ' = ƒ.

    Correct Option: C

    Fundamental frequency of open pipe,

    ƒ =
    v
    2l

    When half of tube is filled with water, then the length of air column becomes half
    l' =
    l
    2

    and the pipe becomes closed.
    So, new fundamental frequency
    ƒ' =
    v
    =
    v
    =
    v
    4l'4
    l
    2l
    2

    Clearly ƒ' = ƒ.