## Energy and Power of a Simple Harmonic Wave on a String

As a mechanical wave propagates in a medium, it transfers energy form one particle to another and the successive particles get the disturbance. In Figure 1 we consider a transverse wave travelling in a string positive x-direction of our coordinate system. We consider a particular point $p$ in the string which is disturbed by the wave. The string on the left of the point $p$ exerts tension on the point which has two components namely $F_\text{x}$ and $F_\text{y}$. The transverse force $F_y$ exerts transverse force on the particle and hence does work on the particle. Note that the component $F_x$ is the tension the string would have in undisturbed condition of the string. The wave has constant amplitude and constant frequency.

The slope at the point $p$ is the negative of the ratio $F_y /F_x$ because $F_y$ is negative but the slope is positive. The slope is also equal to the derivative of wave function with respect to position $x$ keeping time $t$ constant, therefore the slope at the point $p$ is

\[\begin{align*} \frac{{\partial y}}{{\partial x}} &= \frac{{ - {F_y}}}{{{F_x}}}\\ {\rm{or,}}\quad {F_y} &= - {F_x}\frac{{\partial y}}{{\partial x}} \tag{1} \label{1} \end{align*}\]

The power is the rate of doing work and the instantaneous power at the point $p$ is the product of downward force $F_y$ and the downward velocity $v_y$ at that point. So,

\[P = {F_y}{v_y} = - {F_x}\frac{{\partial y}}{{\partial x}}{v_y} \tag{2} \label{2}\]

The wave function for a simple harmonic wave travelling in positive x-direction is $y = A\cos (kx - \omega t)$ and you can find;

\[\begin{align*} \frac{{\partial y}}{{\partial x}} &= - Ak\sin (kx - \omega t)\\ {\rm{and,}}\quad {v_y} &= \frac{{\partial y}}{{\partial t}} = A\omega \sin (kx - \omega t) \end{align*}\]

Therefore, substituting the values of $\partial y /\partial x$ and $v_y$ in Eq. \eqref{2}, you'll get the power which is

\[P = {F_x}{A^2}\omega k{\kern 1pt}{\sin ^2}(kx - \omega t) \tag{3} \label{3}\]

We have determined from the article of web speeds (you may need to read this article which is also the previous article of this article) that $F_x = {v^2}\mu $ and $k = \omega/v$, the above equation can be rewritten as

\[P = {A^2}\omega^2\mu v {\kern 1pt}{\sin ^2}(kx - \omega t) \tag{4} \label{4}\]

The value of ${\sin ^2}$ function oscillates between $0$ and $1$ and hence its average value is $1/2$. So, the average value of ${\sin ^2}(kx - \omega t)$ in the above equation is $1/2$ and the average power is

\[{P_{av}} = \frac{1}{2}{A^2} \omega^2 \mu v \tag{5} \label{5}\]

The above equation shows the the average rate of energy transfer, that is average power of a simple harmonic or sinusoidal wave along a string is proportional to the square of amplitude, square of angular frequency, linear density of the string and the wave speed.

## Wave Intensity

Sound waves spread out in three-dimensional space form the source of sound so the sound wave is three dimensional wave while the transverse wave in a string is one dimensional. We use power to define the strength of one dimensional waves, however, *intensity* is used for three dimensional waves.

Intensity of a wave is the average rate of energy transfer per unit area perpendicular to the direction of the propagation of the wave. It's the same as the average power of the wave per unit area. You can see in Figure 2 that a sound source emits sound waves in three dimensional space. The imaginary spherical surfaces of radius $r_1$ and $r_2$ enclose the source of sound. The average power $P_\text{av}$ through both spherical surfaces is the same. Now the intensity $I_1$ through the spherical surface of radius $r_1$ is $I_1 = P_\text{av} /4\pi {r_1}^2$ and the intensity $I_2$ through the spherical surface of radius $r_2$ is $I_2 = P_\text{av} /4\pi {r_2}^2$. Therefore,

\[\frac{{{I_1}}}{{{I_2}}} = \frac{{P_\text{av}/4\pi {r_1}^2}}{{P_\text{av}/4\pi {r_2}^2}} = \frac{{{r_2}^2}}{{{r_1}^2}} \tag{6} \label{6}\]

The above equation tells us that the intensity of a sound wave is inversely proportional to the square of distance from the source of sound. The above equation is called inverse square law for three dimensional waves.