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Physics Bootcamp

Section 14.1 Sinusoidal Waves

When a string is shaken sinusoidally, i.e., it is vibrated such that the oscillations are sine or cosine function of time, the wave propagated in the string also has sinusoidal shape as illustrated in Figure 14.3. The period of the wave in space is called its wavelength, and it is usually denoted by the Greek letter \(\lambda\) (lambda). The absolute value of the displacement of the disturbance on either side of the equilibrium is called amplitude, usually denoted by letter \(A\text{.}\) Note that amplitude is not the entire range of displacement but half of that.
Figure 14.3. Traveling wave on a string. Figure shows wave at three instants of time. The repeating distance, denoted by \(\lambda\) is the wavelength, the absolute value of the displacement of the disturbance on either side of the equilibrium is called amplitude, and the time it takes the wave to cover a wavelength is its period, which we denote by \(T\text{.}\) The ratio \(\lambda/T\) is the wave speed, which is also called phase velocity in the case of sinusoidal waves.
As Figure 14.3 shows, the moving wave will move with some speed \(v\text{,}\) which we call wave speed. In the case of sinusoidal waves, wave speed is also called phase velocity. We will encounter another velocity associated with pulses or nonsinusoidal waves called group velocity. The wave in Figure 14.3 will travel a distance of the wavelength in some time \(T\text{,}\) which is called period of the wave. That is,
\begin{equation} vT = \lambda.\tag{14.1} \end{equation}
The inverse of the period is called frequency or cylce frequency or ordinary frequency of the wave. We will denote frequency by letter \(f\) although sometimes it is also denoted by the Greek letter \(\nu\) (nu).
\begin{equation} f = \frac{1}{T}.\tag{14.2} \end{equation}
In terms of frequency, Eq. (14.1)> takes the following form, called the fundamental equation of waves.
\begin{equation} v = \lambda\, f.\tag{14.3} \end{equation}

Subsection 14.1.1 Mathematical Description of Wave

Let string in Figure 14.3 be along \(x\) axis and oscillate along the \(y\) axis with frequency \(f\text{.}\) Let \(y(x,t)\) denote the displacement of string particle at coordinate \(x\) at time \(t\text{,}\) i.e., let the particle be at \((x,y)\) at instant t. Then, we can write the sinusoidal wave moving towards the positive \(x\)axis by
\begin{equation} y(x,t) = A\, \cos\left(\dfrac{2\pi}{\lambda} x - 2\pi f t + \phi\right),\tag{14.4} \end{equation}
where \(\phi\) is a constant, called the phase constant, and the full argument of cosine, viz., \(\left(\dfrac{2\pi}{\lambda} x - 2\pi f t + \phi\right)\) is called the phase of the wave. If diaplacement at origin at time \(t=0\) is equal to the ampitude \(A\text{,}\) then phase constant will be \(\phi=0\text{.}\) We will usually take this to be the case.
\begin{equation} y(x,t) = A\, \cos\left(\dfrac{2\pi}{\lambda} x - 2\pi f t\right).\tag{14.5} \end{equation}
Rather than write \(2\pi\) all over the place, we often write this using angular quantities by replacing frequency by angular frequency, \(\omega\text{,}\)
\begin{equation} \omega = 2\pi f,\tag{14.6} \end{equation}
and inverse wavelength by wave number, \(k\text{,}\) defined by
\begin{equation} k = \frac{2\pi}{\lambda}.\tag{14.7} \end{equation}
the speed of the wave in terms of angular quantities will be
\begin{equation} v = f\lambda = \frac{\omega}{2\pi}\times \frac{2\pi}{k} = \frac{\omega}{k}.\tag{14.8} \end{equation}
Using angular variables, the sinusoidal wave moving to the right is given by
\begin{equation} y(x,t) = A\, \cos\left(k x - \omega t\right).\tag{14.9} \end{equation}
A wave moving towards left, i.e., towards negative \(x\)-axis, will have both \(x\) and \(t\) same sign.
\begin{equation} y(x,t) = A\, \cos\left(k x + \omega t\right).\tag{14.10} \end{equation}

Exercises 14.1.2 Exercises

1. Obtaining Properties of Sinusoidal Waves from Wave Function.

The sound produced by a speaker is given by the following pressure difference wave in air.
\begin{equation*} \Delta p = (10 \text{ Pa})\, \cos(k x + 6000\, t + \pi), \end{equation*}
where \(x\) is in meters and \(t\) in seconds and \(\Delta p(x,t)\) is the difference in atmospheric pressure from the ambient pressure at location \(x\) at time \(t\text{.}\) Suppose speed of this wave is \(343\text{ m/s}\text{.}\)
(a) What is the amplitude of the wave?
(b) What is the frequency of the wave?
(c) What is the wavelength of the wave?
Hint.
The \(\Delta p\) is just a sinusoidal wave.
Answer.
(a) \(10\text{ Pa}\text{,}\) (b) \(954.9\text{ Hz}\text{,}\) (c) \(35.9\text{ cm}\text{.}\)
Solution 1. a
Here \(\Delta p\) is actually a sinusoidal wave. In the text, we used the symbol \(y\) for the wave, but here, it is \(\Delta p\text{.}\) The amplitude is just the number multiplying the oscillating part.
\begin{equation*} \text{Amplitude} = 10\text{ Pa}. \end{equation*}
Solution 2. b
We can read of angular frequency \(\omega\) from the number that multiplies \(t\) in the argument of coine, and then obtained frequency \(f\) from it.
\begin{equation*} f = \frac{\omega}{2\pi} = \frac{6000}{2\pi} = 954.9\text{ Hz}. \end{equation*}
I have used \(\text{Hz}\) for the unit since it is regular cycle per second, and not the angular cycle.
Solution 3. c
If we knew the wavenumber \(k\text{,}\) we will get \(\lambda\) from it. But, since we don’t know \(k\) yet, but we do know \(v\) and \(f\text{,}\) therefore, we will use the fundamental equation.
\begin{equation*} \lambda = \frac{v}{f} = \frac{343}{954.9} = 0.359\text{ m} = 35.9\text{ cm}. \end{equation*}

2. Obtaining Properties of Sinusoidal Waves from Wave Function.

A traveling wave along \(x\)-axis is given by the following wave function
\begin{equation*} \psi(x,t) = 5 \cos(2x-10t+0.4), \end{equation*}
where \(x\) in meter, \(t\) in seconds, and \(\psi\) in meters. Read off the appropriate quantities for this wave function and find the following characteristics of this plane wave: (a) the amplitude, (b) the frequency, (c) the wavelength, (d) the wave speed, and (e) the phase constant.
Answer.
(a) 5 m; (b) 1.6 Hz; (c)\(\pi\) m; (d) 5.1 m/s; (e) 0.4 rad.

3. Drawing Wave Profiles.

A traveling wave along \(x\)-axis is given by the following wave function
\begin{equation*} \psi(x,t) = 5 \cos(2x-10t+0.4), \end{equation*}
where \(x\) in meter, \(t\) in seconds, and \(\psi\) in meters.
(a) Plot the wave function a function of \(x\) at two different times, \(t=0\) and \(t= 0.3\) second. These plots are called wave profile. (b) Which way is this wave traveling in time?
Solution 1. a
We are going to plot for three times \(t = 0,\, 0.1\, 0.3\text{.}\) That is, we need to plot three functions: \(\psi_0(x) = 5 \cos(2x+0.4)\text{,}\) \(\psi_{0.1}(x) = 5 \cos(2x-0.6)\text{,}\) and \(\psi_{0.3}(x) = 5 \cos(2x-2.6)\text{.}\) Note: the argument is in radians. Figure 14.4 shows \(\psi_0\) (solid), \(\psi_{0.1}\) (dashed), \(\psi_{0.3}\) (dotted).
Figure 14.4.
Solution 2. b
The wave is traveling towards the positive \(x\)-axis.

4. Two Sinusiodal Waves Off by a Phase of \(\pi/2\).

(a) Plot the following two wave functions at \(t=0\text{,}\) \(\psi_1(x,t) = 10\cos(2x-10t+0.4)\) and \(\psi_2(x,t) = 10\cos(2x-10t+0.4+\pi/2)\text{,}\) and (b) give an interpretation of the difference in the phase constants of the two waves.
Solution 1. a
Figure 14.5 shows plots at \(t=0\) for the wavefunctions \(\psi_1(x,t) = 10\cos(2x-10t+0.4)\) (solid curve) and \(\psi_2(x,t) = 10\cos(2x-10t+0.4+\pi/2)\) (dashed curve).
Figure 14.5.
Solution 2. b
Since the two waves are traveling towards the positive \(x\) axis, as determined by the opposite signs of the \(x\) and \(t\) terms in the argument of the cosine, the figure shows that the wave \(\psi_2\) is behind the other wave is by a phase of \(\pi/2\) rad or quarter of a cycle.

5. Two Waves of Same Wavelength and Frequency but Travel in Different Directions.

(a) Plot the following two wave functions as a function of time at \(x=0\text{,}\) \(\psi_1(x,t) = 10\cos(2x-10t+0.4)\) and \(\psi_2(x,t) = 10\cos(2x-10t+0.4+\pi/2)\text{,}\) and (b) give an interpretation of phase constant.
Solution.
The figure below shows plots at \(x=0\) for the wavefunctions \(\psi_1(x,t) = 10\cos(2x-10t+0.4)\) (solid curve) and \(\psi_2(x,t) = 10\cos(2x-10t+0.4+\pi/2)\) (dashed curve). The figure also shows the vibrations of a particle at \(x=0\) about the equilibrium. The vibration picture is useful for thinking about the action of a wave at a particular place. The vibration picture shows that \(\psi_1\) vibration is ahead of the \(\psi_2\) wave by a quarter cycle
Figure 14.6.