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E λ = U λ + K λ , E λ = 1 4 μ A 2 ω 2 λ + 1 4 μ A 2 ω 2 λ = 1 2 μ A 2 ω 2 λ .

The time-averaged power of a sinusoidal mechanical wave, which is the average rate of energy transfer associated with a wave as it passes a point, can be found by taking the total energy associated with the wave divided by the time it takes to transfer the energy. If the velocity of the sinusoidal wave is constant, the time for one wavelength to pass by a point is equal to the period of the wave, which is also constant. For a sinusoidal mechanical wave, the time-averaged power is therefore the energy associated with a wavelength divided by the period of the wave. The wavelength of the wave divided by the period is equal to the velocity of the wave,

P ave = E λ T = 1 2 μ A 2 ω 2 λ T = 1 2 μ A 2 ω 2 v .

Note that this equation for the time-averaged power of a sinusoidal mechanical wave shows that the power is proportional to the square of the amplitude of the wave and to the square of the angular frequency of the wave. Recall that the angular frequency is equal to ω = 2 π f , so the power of a mechanical wave is equal to the square of the amplitude and the square of the frequency of the wave.

Power supplied by a string vibrator

Consider a two-meter-long string with a mass of 70.00 g attached to a string vibrator as illustrated in [link] . The tension in the string is 90.0 N. When the string vibrator is turned on, it oscillates with a frequency of 60 Hz and produces a sinusoidal wave on the string with an amplitude of 4.00 cm and a constant wave speed. What is the time-averaged power supplied to the wave by the string vibrator?

Strategy

The power supplied to the wave should equal the time-averaged power of the wave on the string. We know the mass of the string ( m s ) , the length of the string ( L s ) , and the tension ( F T ) in the string. The speed of the wave on the string can be derived from the linear mass density and the tension. The string oscillates with the same frequency as the string vibrator, from which we can find the angular frequency.

Solution

  1. Begin with the equation of the time-averaged power of a sinusoidal wave on a string:
    P = 1 2 μ A 2 ω 2 v .

    The amplitude is given, so we need to calculate the linear mass density of the string, the angular frequency of the wave on the string, and the speed of the wave on the string.
  2. We need to calculate the linear density to find the wave speed:
    μ = m s L s = 0.070 kg 2.00 m = 0.035 kg/m .
  3. The wave speed can be found using the linear mass density and the tension of the string:
    v = F T μ = 90.00 N 0.035 kg/m = 50.71 m/s .
  4. The angular frequency can be found from the frequency:
    ω = 2 π f = 2 π ( 60 s −1 ) = 376.80 s −1 .
  5. Calculate the time-averaged power:
    P = 1 2 μ A 2 ω 2 v = 1 2 ( 0.035 kg m ) ( 0.040 m ) 2 ( 376.80 s −1 ) 2 ( 50.71 m s ) = 201.59 W .

Significance

The time-averaged power of a sinusoidal wave is proportional to the square of the amplitude of the wave and the square of the angular frequency of the wave. This is true for most mechanical waves. If either the angular frequency or the amplitude of the wave were doubled, the power would increase by a factor of four. The time-averaged power of the wave on a string is also proportional to the speed of the sinusoidal wave on the string. If the speed were doubled, by increasing the tension by a factor of four, the power would also be doubled.

Practice Key Terms 1

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Source:  OpenStax, University physics volume 1. OpenStax CNX. Sep 19, 2016 Download for free at http://cnx.org/content/col12031/1.5
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