/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 40 The wave function of a standing ... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

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.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

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.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A transverse standing wave is set up on a string that is held fixed at both ends. The amplitude of the standing wave at an antinode is \(1.80 \mathrm{~mm}\) and the speed of propagation of transverse waves on the string is \(260 \mathrm{~m} / \mathrm{s}\). The string extends along the \(x\) -axis, with one of the fixed ends at \(x=0,\) so that there is a node at \(x=0 .\) The smallest value of \(x\) where there is an antinode is \(x=0.150 \mathrm{~m}\). (a) What is the maximum transverse speed of a point on the string at an antinode? (b) What is the maximum transverse speed of a point on the string at \(x=0.075 \mathrm{~m} ?\)

A string with both ends held fixed is vibrating in its third harmonic. The waves have a speed of \(192 \mathrm{~m} / \mathrm{s}\) and a frequency of \(240 \mathrm{~Hz}\). The amplitude of the standing wave at an antinode is \(0.400 \mathrm{~cm}\). (a) Calculate the amplitude at points on the string a distance of (i) \(40.0 \mathrm{~cm}\) (ii) \(20.0 \mathrm{~cm} ;\) and (iii) \(10.0 \mathrm{~cm}\) from the left end of the string. (b) At each point in part (a), how much time does it take the string to go from its largest upward displacement to its largest downward displacement? (c) Calculate the maximum transverse velocity and the maximum transverse acceleration of the string at each of the points in part (a).

The speed of sound in air at \(20^{\circ} \mathrm{C}\) is \(344 \mathrm{~m} / \mathrm{s}\). (a) What is the wavelength of a sound wave with a frequency of \(784 \mathrm{~Hz}\), corresponding to the note \(\mathrm{G}_{5}\) on a piano, and how many milliseconds does each vibration take? (b) What is the wavelength of a sound wave one octave higher (twice the frequency) than the note in part (a)?

With what tension must a rope with length \(2.50 \mathrm{~m}\) and mass \(0.120 \mathrm{~kg}\) be stretched for transverse waves of frequency \(40.0 \mathrm{~Hz}\) to have a wavelength of \(0.750 \mathrm{~m} ?\)

A \(1.005 \mathrm{~m}\) chain consists of small spherical beads, each with a mass of \(1.00 \mathrm{~g}\) and a diameter of \(5.00 \mathrm{~mm},\) threaded on an elastic strand with negligible mass such that adjacent beads are separated by a center-to-center distance of \(10.0 \mathrm{~mm}\). There are beads at each end of the chain. The strand has a spring constant of \(28.8 \mathrm{~N} / \mathrm{m}\). The chain is stretched horizontally on a frictionless tabletop to a length of \(1.50 \mathrm{~m}\), and the beads at both ends are fixed in place. (a) What is the linear mass density of the chain? (b) What is the tension in the chain? (c) With what speed would a pulse travel down the chain? (d) The chain is set vibrating and exhibits a standing-wave pattern with four antinodes. What is the frequency of this motion? (e) If the beads are numbered sequentially from 1 to \(101,\) what are the numbers of the five beads that remain motionless? (f) The 13th bead has a maximum speed of \(7.54 \mathrm{~m} / \mathrm{s}\). What is the amplitude of that bead's motion? (g) If \(x_{0}=0\) corresponds to the center of the 1 st bead and \(x_{101}=1.50 \mathrm{~m}\) corresponds to the center of the 101 st bead, what is the position \(x_{n}\) of the \(n\) th bead? (h) What is the maximum speed of the 30 th bead?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.