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The wave function of a standing wave is \(y(x, t)=(4.44 \mathrm{~mm})\) \(\sin [(32.5 \mathrm{rad} / \mathrm{m}) x] \sin [(754 \mathrm{rad} / \mathrm{s}) t] .\) For the two traveling waves that make up this standing wave, find the (a) amplitude; (b) wavelength; (c) frequency; (d) wave speed; (e) wave functions. (f) From the information given, can you determine which harmonic this is? Explain.

Short Answer

Expert verified
The amplitude is 4.44mm, the wavelength is 0.193 m, the frequency is 120 Hz, the wave speed is 23.2 m/s, the wave functions are \( y1(x,t) = (4.44 \, mm) \sin[(32.5 \, rad/m) x - (754 \, rad/s) t] \) and \( y2(x,t) = (4.44 \, mm) \sin[(32.5 \, rad/m) x + (754 \, rad/s) t] \). It's impossible to determine the harmonic from the given information.

Step by step solution

01

Determine the Amplitude

The amplitude is the number that multiplies the trigonometric equation. For this wave, the amplitude (A) is 4.44mm.
02

Determine the Wavelength

The wavelength can be obtained using the formula \( k = 2\pi/\lambda \), where \( k = 32.5 \, rad/m \) is the wave number. Solving for \( \lambda \) gives the wavelength \( \lambda = 2\pi/k = 0.193 \, m \) .
03

Determine the Frequency

The frequency can be calculated using the formula \( \omega = 2\pi f \), where \( \omega = 754 \, rad/s \) is the angular frequency. Solving for \( f \) gives the frequency \( f = \omega /2\pi = 120 \, Hz \)
04

Determine the Wave Speed

The wave speed \( v \) can be found using the relationship \( v = \omega/k \). Substituting the given values, we find \( v = 754/32.5 = 23.2 \, m/s \)
05

Determine the Wave Functions

The traveling waves that make up the standing wave can be written as \( y1(x,t) = (4.44 \, mm) \sin[(32.5 \, rad/m) x - (754 \, rad/s) t] \) and \( y2(x,t) = (4.44 \, mm) \sin[(32.5 \, rad/m) x + (754 \, rad/s) t] \)
06

Determine the Harmonic

Without additional data such as the length of the string or distance between the nodes, it's impossible to identify which harmonic this standing wave represents.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Wave Function Analysis
Analyzing wave functions is essential in understanding the behavior of waves, particularly standing waves, which are formed by the superposition of two traveling waves. The wave function given in the exercise,
\( y(x, t) = (4.44 \, \text{mm}) \sin [(32.5 \, \text{rad/m}) x] \sin [(754 \, \text{rad/s}) t] \),
provides all the necessary information to determine the properties of the individual traveling waves that combine to create the standing wave. By inspecting the wave function, we can grasp that the sine components refer to the spatial and temporal oscillations, respectively.

Interpreting the Wave Function

The spatial part, \( \sin [(32.5 \, \text{rad/m}) x] \), indicates how the wave varies along the x-axis, while the temporal part, \( \sin [(754 \, \text{rad/s}) t] \), shows how the wave oscillates over time. Together, they form a pattern that does not travel through space but instead oscillates in a fixed position, characteristic of standing waves. For a student striving to visualize this concept, it might be helpful to picture the wave as a vibrating string fixed at both ends, with certain points, called nodes, remaining stationary, while antinodes achieve the maximum amplitude of vibration.
Traveling Wave Equations
Traveling wave equations describe the motion and form of waves as they propagate through space. In the context of the exercise, the two traveling waves that combine to form the standing wave have specific equations based on the given wave function.

Constructing the Traveling Waves

To construct the equations of the individual traveling waves, we utilize the principle that standing waves are the result of the interference of two traveling waves moving in opposite directions. These traveling waves have wave functions expressed as:
  • \( y_1(x,t) = A \sin(kx - \omega t) \)
  • \( y_2(x,t) = A \sin(kx + \omega t) \)
Where \( A \) is the amplitude, \( k \) the wave number related to wavelength, and \( \omega \) the angular frequency related to the frequency of the waves. The negative sign in the first equation indicates that the wave travels in the positive x-direction, while the positive sign in the second equation implies that the wave travels in the negative x-direction. With this understanding, one can tackle a range of wave-related problems and decipher the behavior of moving wave phenomena.
Wavelength Calculation
Understanding how to calculate the wavelength of a wave is crucial in physics and engineering. The wavelength is the physical distance between successive points of the same phase in the wave, such as peak to peak or trough to trough.

Deducing Wavelength from the Wave Number

The step-by-step solution demonstrates that the wave number \( k \) contains the information needed for calculating the wavelength \( \lambda \). The relationship between the two is given by \( k = \frac{2\pi}{\lambda} \). By rearranging this equation and substituting the given wave number, we find:
  • \( \lambda = \frac{2\pi}{k} \)
In the context of our exercise, with \( k = 32.5 \, \text{rad/m} \), the computed wavelength is \( \lambda = 0.193 \, \text{m} \). Knowing the wavelength is essential for applications involving tuning musical instruments or designing antennas where specific wave properties are needed.
Frequency Determination
Frequency is a key concept when dealing with waves as it defines the number of oscillations that occur in one second, and it's inversely related to the period of the wave. In a practical context, frequency can affect everything from the pitch of a sound to the color of light perceived by our eyes.

Calculating Frequency from Angular Frequency

The angular frequency \( \omega \) provided in the wave function is directly proportional to the frequency \( f \), with the relationship given by \( \omega = 2\pi f \). By solving for \( f \) using the value of \( \omega \) from the problem, we establish the frequency of the wave:
  • \( f = \frac{\omega}{2\pi} \)
For our exercise, with \( \omega = 754 \, \text{rad/s} \), the frequency is \( f = 120 \, \text{Hz} \). Identifying the frequency is crucial for many applications such as diagnosing medical conditions with ultrasound, broadcasting radio signals, or even simply setting up a Wi-Fi network at home.

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Most popular questions from this chapter

Standing waves are produced on a string that is held fixed at both ends. The tension in the string is kept constant. (a) For the second overtone standing wave the node-to-node distance is \(8.00 \mathrm{~cm} .\) What is the length of the string? (b) What is the node-to-node distance for the fourth harmonic standing wave?

You are exploring a newly discovered planet. The radius of the planet is \(7.20 \times 10^{7} \mathrm{~m}\). You suspend a lead weight from the lower end of a light string that is \(4.00 \mathrm{~m}\) long and has mass \(0.0280 \mathrm{~kg}\). You measure that it takes \(0.0685 \mathrm{~s}\) for a transverse pulse to travel from the lower end to the upper end of the string. On the earth, for the same string and lead weight, it takes \(0.0390 \mathrm{~s}\) for a transverse pulse to travel the length of the string. The weight of the string is small enough that you ignore its effect on the tension in the string. Assuming that the mass of the planet is distributed with spherical symmetry, what is its mass?

A piano wire with mass \(3.00 \mathrm{~g}\) and length \(80.0 \mathrm{~cm}\) is stretched with a tension of \(25.0 \mathrm{~N}\). A wave with frequency \(120.0 \mathrm{~Hz}\) and amplitude \(1.6 \mathrm{~mm}\) travels along the wire. (a) Calculate the average power carried by the wave. (b) What happens to the average power if the wave amplitude is halved?

In your physics lab, an oscillator is attached to one end of a horizontal string. The other end of the string passes over a frictionless pulley. You suspend a mass \(M\) from the free end of the string, producing tension \(M g\) in the string. The oscillator produces transverse waves of frequency \(f\) on the string. You don't vary this frequency during the experiment, but you try strings with three different linear mass densities \(\mu .\) You also keep a fixed distance between the end of the string where the oscillator is attached and the point where the string is in contact with the pulley's rim. To produce standing waves on the string, you vary \(M ;\) then you measure the node-to-node distance \(d\) for each standing-wave pattern and obtain the following data: $$ \begin{array}{l|lllll} \text { String } & \text { A } & \text { A } & \text { B } & \text { B } & \text { C } \\ \hline \mu(\mathrm{g} / \mathrm{cm}) & 0.0260 & 0.0260 & 0.0374 & 0.0374 & 0.0482 \\ M(\mathrm{~g}) & 559 & 249 & 365 & 207 & 262 \\ d(\mathrm{~cm}) & 48.1 & 31.9 & 32.0 & 24.2 & 23.8 \end{array} $$ (a) Explain why you obtain only certain values of \(d\). (b) Graph \(\mu d^{2}(\) in \(\mathrm{kg} \cdot \mathrm{m})\) versus \(M(\) in \(\mathrm{kg}) .\) Explain why the data plotted this way should fall close to a straight line. (c) Use the slope of the best straightline fit to the data to determine the frequency \(f\) of the waves produced on the string by the oscillator. Take \(g=9.80 \mathrm{~m} / \mathrm{s}^{2}\). (d) For string A \((\mu=0.0260 \mathrm{~g} / \mathrm{cm}),\) what value of \(M\) (in grams) would be required to produce a standing wave with a node-to-node distance of \(24.0 \mathrm{~cm}\) ? Use the value of \(f\) that you calculated in part (c).

A thin, taut string tied at both ends and oscillating in its third harmonic has its shape described by the equation \(y(x, t)=(5.60 \mathrm{~cm}) \sin [(0.0340 \mathrm{rad} / \mathrm{cm}) x] \sin [(50.0 \mathrm{rad} / \mathrm{s}) t],\) where the origin is at the left end of the string, the \(x\) -axis is along the string, and the \(y\) -axis is perpendicular to the string. (a) Draw a sketch that shows the standing-wave pattern. (b) Find the amplitude of the two traveling waves that make up this standing wave. (c) What is the length of the string? (d) Find the wavelength, frequency, period, and speed of the traveling waves. (e) Find the maximum transverse speed of a point on the string. (f) What would be the equation \(y(x, t)\) for this string if it were vibrating in its eighth harmonic?

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