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The equation for a standing wave on a string with mass density \(\mu\) is \(y(x, t)=2 A \cos (\omega t) \sin (\kappa x) .\) Show that the average kinetic energy and potential energy over time for this wave per unit length are given by \(K_{\text {ave }}(x)=\mu \omega^{2} A^{2} \sin ^{2} \kappa x\) and \(U_{\text {ave }}(x)=T(\kappa A)^{2}\left(\cos ^{2} \kappa x\right)\)

Short Answer

Expert verified
The average kinetic energy per unit length is given by: \(K_{\text {ave }}(x)=\mu \omega^{2} A^{2} \sin ^{2} \kappa x\) The average potential energy per unit length is given by: \(U_{\text {ave }}(x)=T(\kappa A)^{2}\left(\cos ^{2} \kappa x\right)\)

Step by step solution

01

Find the velocity of the string at each point

To find the velocity of the string at each point, we need to differentiate y(x, t) with respect to time (t): \(v(x, t) = \frac{\partial y(x, t)}{\partial t}\) Applying the partial derivative, we get: \(v(x, t) = -2 A \omega \sin(\omega t) \sin(\kappa x)\)
02

Find the acceleration of the string at each point

Now, we will differentiate the velocity v(x, t) with respect to time (t) to find the acceleration: \(a(x, t) = \frac{\partial v(x, t)}{\partial t}\) Applying the partial derivative, we get: \(a(x, t) = -2 A \omega^2 \cos(\omega t) \sin(\kappa x)\)
03

Calculate the kinetic energy at each point

The kinetic energy per unit length at each point is given by: \(K(x, t) = \frac{1}{2} \mu v^2(x, t)\) Substitute the expression for v(x, t), and get: \(K(x, t) = \frac{1}{2}\mu (2 A \omega \sin(\omega t) \sin(\kappa x))^2\) Simplify the expression: \(K(x, t) = 2 \mu A^2 \omega^2 \sin^2(\omega t) \sin^2(\kappa x)\)
04

Calculate the average kinetic energy over time

To find the average kinetic energy over a full time period [0, T], we need to integrate K(x, t) over the time and divide by the period: \(K_{\text{ave}}(x) = \frac{1}{T} \int_{0}^{T} K(x, t) dt\) Substitute the expression for K(x, t), and get: \(K_{\text{ave}}(x) = \frac{1}{T} \int_{0}^{T} 2 \mu A^2 \omega^2 \sin^2(\omega t) \sin^2(\kappa x) dt\) The term \(\sin^2(\omega t)\) has an average value of \(\frac{1}{2}\), so the integral simplifies to: \(K_{\text{ave}}(x) = \mu \omega^2 A^2 \sin^2(\kappa x)\)
05

Calculate the potential energy at each point

The potential energy per unit length at each point is given by: \(U(x, t) = \frac{1}{2} T(\kappa y(x, t))^2\) Substitute the expression for y(x, t), and get: \(U(x, t) = \frac{1}{2} T(\kappa(2 A \cos(\omega t) \sin(\kappa x)))^2\) Simplify the expression: \(U(x, t) = 2 T \kappa^2 A^2 \cos^2(\omega t) \sin^2(\kappa x)\)
06

Calculate the average potential energy over time

To find the average potential energy over a full time period [0, T], we need to integrate U(x, t) over the time and divide by the period: \(U_{\text{ave}}(x) = \frac{1}{T} \int_{0}^{T} U(x, t) dt\) Substitute the expression for U(x, t), and get: \(U_{\text{ave}}(x) = \frac{1}{T} \int_{0}^{T} 2 T \kappa^2 A^2 \cos^2(\omega t) \sin^2(\kappa x) dt\) The term \(\cos^2(\omega t)\) has an average value of \(\frac{1}{2}\), so the integral simplifies to: \(U_{\text{ave}}(x) = T (\kappa A)^2 \cos^2(\kappa x)\) Thus, the average kinetic energy per unit length is \(K_{\text {ave }}(x)=\mu \omega^{2} A^{2} \sin ^{2} \kappa x\) and the average potential energy per unit length is \(U_{\text {ave }}(x)=T(\kappa A)^{2}\left(\cos ^{2} \kappa x\right)\).

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Key Concepts

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

Kinetic Energy
Kinetic energy is a crucial concept when studying standing waves on a string. It describes the energy associated with the motion of the wave. In the context of standing waves, each point on the string oscillates up and down, and therefore possesses kinetic energy as it moves.

The kinetic energy per unit length for a string wave can be expressed using the velocity of the wave at each point. When we differentiate the displacement function, \( y(x, t) = 2 A \cos(\omega t) \sin(\kappa x) \), with respect to time, we obtain the velocity function: \( v(x, t) = -2 A \omega \sin(\omega t) \sin(\kappa x) \).

This velocity function helps us to calculate the kinetic energy at any given point by using the formula for kinetic energy per unit length: \( K(x, t) = \frac{1}{2} \mu v^2(x, t) \).

By substituting and simplifying, we derive the expression for the kinetic energy over time. Finally, integrating this expression over a complete time period helps us find the average kinetic energy: \(K_{\text{ave}}(x) = \mu \omega^2 A^2 \sin^2(\kappa x)\).

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Most popular questions from this chapter

One of the main things allowing humans to determine whether a sound is coming from the left or the right is the fact that the sound will reach one ear before the other. Given that the speed of sound in air is \(343 \mathrm{~m} / \mathrm{s}\) and that human ears are typically \(20.0 \mathrm{~cm}\) apart, what is the maximum time resolution for human hearing that allows sounds coming from the left to be distinguished from sounds coming from the right? Why is it impossible for a diver to be able to tell from which direction the sound of a motor boat is coming? The speed of sound in water is \(1.50 \cdot 10^{3} \mathrm{~m} / \mathrm{s}\).

If transverse waves on a string travel with a velocity of \(50 \mathrm{~m} / \mathrm{s}\) when the string is under a tension of \(20 \mathrm{~N},\) what tension on the string is required for the waves to travel with a velocity of \(30 \mathrm{~m} / \mathrm{s} ?\) a) \(7.2 \mathrm{~N}\) c) \(33 \mathrm{~N}\) e) \(45 \mathrm{~N}\) b) \(12 \mathrm{~N}\) d) \(40 \mathrm{~N}\) f) \(56 \mathrm{~N}\)

A string is made to oscillate, and a standing wave with three antinodes is created. If the tension in the string is increased by a factor of 4 a) the number of antinodes increases. b) the number of antinodes remains the same. c) the number of antinodes decreases. d) the number of antinodes will equal the number of nodes.

Consider a guitar string stretching \(80.0 \mathrm{~cm}\) between its anchored ends. The string is tuned to play middle \(\mathrm{C},\) with a frequency of \(256 \mathrm{~Hz}\), when oscillating in its fundamental mode, that is, with one antinode between the ends. If the string is displaced \(2.00 \mathrm{~mm}\) at its midpoint and released to produce this note, what are the wave speed, \(v\), and the maximum speed, \(V_{\text {max }}\), of the midpoint of the string?

A string with a mass of \(30.0 \mathrm{~g}\) and a length of \(2.00 \mathrm{~m}\) is stretched under a tension of \(70.0 \mathrm{~N}\). How much power must be supplied to the string to generate a traveling wave that has a frequency of \(50.0 \mathrm{~Hz}\) and an amplitude of \(4.00 \mathrm{~cm} ?\)

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