Much like the mass oscillating on a spring, there is a conservative restoring force that, when the mass element is displaced from the equilibrium position, drives the mass element back to the equilibrium position. There is also potential energy associated with the wave. Since the string has a constant linear density μ = Δ m Δ x, μ = Δ m Δ x, each mass element of the string has the mass Δ m = μ Δ x. Each mass element of the string can be modeled as a simple harmonic oscillator. As the energy propagates along the string, each mass element of the string is driven up and down at the same frequency as the wave. Consider a mass element of the string with a mass Δ m Δ m, as seen in Figure 16.16. The rod does work on the string, producing energy that propagates along the string. A string of uniform linear mass density is attached to the rod, and the rod oscillates the string, producing a sinusoidal wave. The string vibrator is a device that vibrates a rod up and down. Power in WavesĬonsider a sinusoidal wave on a string that is produced by a string vibrator, as shown in Figure 16.16. It should be noted that although the rate of energy transport is proportional to both the square of the amplitude and square of the frequency in mechanical waves, the rate of energy transfer in electromagnetic waves is proportional to the square of the amplitude, but independent of the frequency. If two mechanical waves have equal amplitudes, but one wave has a frequency equal to twice the frequency of the other, the higher-frequency wave will have a rate of energy transfer a factor of four times as great as the rate of energy transfer of the lower-frequency wave. We will see that the average rate of energy transfer in mechanical waves is proportional to both the square of the amplitude and the square of the frequency. If the energy of each wavelength is considered to be a discrete packet of energy, a high-frequency wave will deliver more of these packets per unit time than a low-frequency wave. The energy of the wave depends on both the amplitude and the frequency. The larger the amplitude, the higher the seagull is lifted by the wave and the larger the change in potential energy. Work is done on the seagull by the wave as the seagull is moved up, changing its potential energy. Consider the example of the seagull and the water wave earlier in the chapter ( Figure 16.3). Large ocean breakers churn up the shore more than small ones. Loud sounds have high-pressure amplitudes and come from larger-amplitude source vibrations than soft sounds. Large-amplitude earthquakes produce large ground displacements. The amount of energy in a wave is related to its amplitude and its frequency. This will be of fundamental importance in later discussions of waves, from sound to light to quantum mechanics. In this section, we examine the quantitative expression of energy in waves. The Richter scale rating of earthquakes is a logarithmic scale related to both their amplitude and the energy they carry. Figure 16.15 The destructive effect of an earthquake is observable evidence of the energy carried in these waves.
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