Modern PhysicsWaves with Calculus

Energy and Power of a Wave

A wave on a string carries power P = ½μω²A²v, so doubling the amplitude carries four times the power.

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A wave carries energy without carrying matter. Shake one end of a long rope and, a moment later, a bit of rope far away starts moving: energy has traveled down the rope. How much power does a wave deliver, and how does it depend on how hard you shake? You know the wave function $y = A\sin(kx - \omega t)$; the answer follows from it.

Key idea

A sinusoidal wave on a string with linear mass density $\mu$ carries the average power $$P_{\text{avg}} = \tfrac{1}{2}\,\mu\,\omega^2 A^2\,v.$$ Power grows with the square of the amplitude and the square of the frequency: double $A$ and the power is 4 times as large.

Why it works

Each bit of string of mass $\Delta m = \mu\,\Delta x$ moves up and down in simple harmonic motion with amplitude $A$ and angular frequency $\omega$. A simple harmonic oscillator's total energy equals its maximum kinetic energy, $\tfrac{1}{2}\Delta m\,(A\omega)^2$. So one wavelength of string holds energy $E_\lambda = \tfrac{1}{2}\mu\lambda\,\omega^2A^2$. One wavelength passes any point every period $T$, so the power is $$P = \frac{E_\lambda}{T} = \tfrac{1}{2}\mu\omega^2A^2\,\frac{\lambda}{T} = \tfrac{1}{2}\mu\omega^2A^2\,v.$$ The square comes from kinetic energy: speed squared, and the bit's top speed $A\omega$ is proportional to $A$.

Energy per meter of string is $\tfrac{1}{2}\mu\omega^2A^2$, and that energy moves at speed $v$: power is energy per length times speed, the same idea as a flow rate. For sound and light the same reasoning gives intensity proportional to the amplitude squared.

Worked examples

Worked example: Power on a rope

A rope with $\mu = 0.25$ kg/m carries waves at 12 m/s. You shake it at 2.0 Hz with amplitude 4.0 cm. What average power do you supply?
  1. $\omega = 2\pi f = 2\pi(2.0) = 12.57$ rad/s.
  2. $$P = \tfrac{1}{2}(0.25\ \text{kg/m})(12.57\ \text{rad/s})^2$$ $$\times\,(0.040\ \text{m})^2(12\ \text{m/s})$$
  3. $= 0.5 \times 0.25 \times 157.9 \times 0.0016 \times 12 = 0.379$ W.
  4. Units: (kg/m)(1/s²)(m²)(m/s) = kg·m²/s³ = W.

Answer: $P \approx 0.38$ W

Worked example: Scaling

You now shake the same rope with three times the amplitude and half the frequency. By what factor does the power change?
  1. $P \propto \omega^2 A^2$ when $\mu$ and $v$ stay the same (same rope, same tension).
  2. Amplitude: $3^2 = 9$. Frequency: $(\tfrac{1}{2})^2 = \tfrac{1}{4}$.
  3. Together: $9 \times \tfrac{1}{4} = 2.25$.

Answer: $2.25$ times the power

Worked example: Amplitude for a target power

A string has $\mu = 5.0 \times 10^{-3}$ kg/m and tension 80 N. What amplitude at 60 Hz carries an average power of 2.0 W?
  1. Wave speed: $v = \sqrt{F_T/\mu} = \sqrt{80/0.0050} = 126.5$ m/s.
  2. $\omega = 2\pi(60) = 377$ rad/s.
  3. Solve for $A$: $$A = \sqrt{\frac{2P}{\mu\omega^2 v}} = \sqrt{\frac{2(2.0)}{(0.0050)(377)^2(126.5)}}.$$
  4. $= \sqrt{4.45 \times 10^{-5}\ \text{m}^2} = 6.7 \times 10^{-3}$ m.

Answer: $A \approx 6.7$ mm

Common mistake

Assuming the power grows in proportion to the amplitude. It grows with the square: twice the amplitude means twice the top speed of each bit, so four times the kinetic energy. A quick check: if $A$ goes up by 10%, $P$ goes up by about 21%, since $1.1^2 = 1.21$.

Common mistake

Changing the wave speed when the frequency changes. On a given string under a given tension, $v = \sqrt{F_T/\mu}$ does not depend on $f$. A higher frequency gives a shorter wavelength, not a faster wave.
Raise the amplitude and watch the red particle: it covers more distance in the same period, so its top speed and its kinetic energy rise. Doubling $A$ doubles the speed and quadruples the energy.

Practice

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Sources and further reading

  • OpenStax University Physics Volume 1, 16.4 Energy and Power of a Wave
  • MIT OpenCourseWare 8.03SC Physics III: Vibrations and Waves (Fall 2016)
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