/*! 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 35 Standing waves on a wire are des... [FREE SOLUTION] | 91Ó°ÊÓ

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Standing waves on a wire are described by Eq. (15.28), with \(A_{\mathrm{SW}}=2.50 \mathrm{~mm}, \omega=942 \mathrm{rad} / \mathrm{s},\) and \(k=0.750 \pi \mathrm{rad} / \mathrm{m} .\) The left end of the wire is at \(x=0 .\) At what distances from the left end are (a) the nodes of the standing wave and (b) the antinodes of the standing wave?

Short Answer

Expert verified
The positions of the nodes are \(x_n = \frac{n}{0.750}\) m and the positions of the antinodes are \(x_a = \frac{(2n+1)}{1.50}\) m, where \(n\) is an integer.

Step by step solution

01

Understanding the property of a node

A node is a point of zero amplitude. In a standing wave, the nodes occur where \(kx = n\pi\), where \(n\) is an integer.
02

Calculation of node positions

Rearrange the equation \(kx = n\pi\) to find \(x\). Given that \(k = 0.750\pi \) rad/m, the equation becomes \(x_n = \frac{n}{0.750}\) m, for \(n = 0, 1, 2, 3, ... \).
03

Understanding the property of an antinode

An antinode is a point of maximum amplitude. In a standing wave, the antinodes occur where \(kx = (n+1/2)\pi\), where \(n\) is an integer.
04

Calculation of antinode positions

Rearrange the equation \(kx = (n+1/2)\pi\) to find \(x\). Given that \(k = 0.750\pi \) rad/m, the equation becomes \(x_a = \frac{(2n+1)}{1.50}\) m, for \(n = 0, 1, 2, 3, ... \).

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Key Concepts

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

Node and Antinode
Standing waves are unique phenomena where certain points called nodes and antinodes depict the extremities of motion. A node is a point along the medium where the wave has zero amplitude at all times. In simpler terms, it's a stationary point that doesn't move as the wave passes through. On the other side, an antinode is a point where the wave exhibits maximum amplitude, meaning it oscillates with the greatest possible distance from the rest point. In standing waves, these points are alternately spaced; where you find a node, an antinode will always be half a wavelength away. The difference between nodes and antinodes is a critical foundation for understanding wave behavior in various physical systems, from musical instruments to the quantum realms.

Wave Amplitude
The amplitude of a wave is indicative of its energy and is defined as the maximum distance from the equilibrium position that points on the wave reach during oscillation. For standing waves, like the ones described in our problem, the amplitude is represented by the symbol \( A_{\mathrm{SW}} \: 2.50 \mathrm{~ mm} \) indicating the peak value of the wave's displacement from its rest position. When considering standing waves on a wire, the amplitude is the distance between the center line of the wire and the highest point that it reaches. Amplitude plays a central role in the properties of a wave, affecting not just its power but also the energy transferred through the medium.

Angular Wave Number
The angular wave number, represented by the symbol \(k\), is a measure of the number of wave cycles that fit within a unit length. Technically, it relates to the spatial frequency of a wave and is proportional to 2\(\pi\) divided by the wavelength. For our standing waves on a wire, \(k = 0.750 \pi \mathrm{rad} / \mathrm{m} \), offering insight into the wave's structure and how tightly packed each oscillation is. A higher value of \(k\) means more waves per meter, implying a shorter wavelength. Angular wave number is pivotal in solving standing wave problems as it connects the general wave properties with specific positions of nodes and antinodes.

Wavelength of Standing Waves
The wavelength is the distance over which the wave's shape repeats. It determines the length between consecutive points in phase, such as node to node or antinode to antinode. For standing waves, the wavelength can be determined using the relationship between the angular wave number and the integral multiples of \(\pi\). As standing waves are formed by the interference of two waves with the same wavelength moving in opposite directions, understanding the wavelength is key to constructing and analyzing these wave patterns. It's an essential component in the calculation of both nodes and antinodes positions. In musical instruments, for instance, the wavelength governs the pitch of the note played, showing the widespread importance of this concept.

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Most popular questions from this chapter

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?

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?

You must determine the length of a long, thin wire that is suspended from the ceiling in the atrium of a tall building. A \(2.00-\mathrm{cm}\) -long piece of the wire is left over from its installation. Using an analytical balance, you determine that the mass of the spare piece is \(14.5 \mu \mathrm{g}\). You then hang a \(0.400 \mathrm{~kg}\) mass from the lower end of the long, suspended wire. When a small-amplitude transverse wave pulse is sent up that wire, sensors at both ends measure that it takes the wave pulse \(26.7 \mathrm{~ms}\) to travel the length of the wire. (a) Use these measurements to calculate the length of the wire. Assume that the weight of the wire has a negligible effect on the speed of the transverse waves. (b) Discuss the accuracy of the approximation made in part (a).

A fisherman notices that his boat is moving up and down periodically, owing to waves on the surface of the water. It takes \(2.5 \mathrm{~s}\) for the boat to travel from its highest point to its lowest, a total distance of \(0.53 \mathrm{~m} .\) The fisherman sees that the wave crests are spaced \(4.8 \mathrm{~m}\) apart. (a) How fast are the waves traveling? (b) What is the amplitude of each wave? (c) If the total vertical distance traveled by the boat were \(0.30 \mathrm{~m}\) but the other data remained the same, how would the answers to parts (a) and (b) change?

One end of a horizontal rope is attached to a prong of an electrically driven tuning fork that vibrates the rope transversely at \(120 \mathrm{~Hz}\). The other end passes over a pulley and supports a \(1.50 \mathrm{~kg}\) mass. The linear mass density of the rope is \(0.0480 \mathrm{~kg} / \mathrm{m} .\) (a) What is the speed of a transverse wave on the rope? (b) What is the wavelength? (c) How would your answers to parts (a) and (b) change if the mass were increased to \(3.00 \mathrm{~kg} ?\)

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