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If two traveling waves have the same wavelength, frequency, and amplitude and are added appropriately, the result is a standing wave. Is it possible to combine two standing waves in some way to give a traveling wave?

Short Answer

Expert verified
If so, under what conditions can this be achieved? Answer: Yes, it is possible to create a traveling wave by combining two standing waves. This can be achieved when the two standing waves have the same amplitude, wave number, and angular frequency, but with a phase shift of π/2 between them.

Step by step solution

01

Understand the properties of standing waves and traveling waves

A standing wave is a wave that remains in a constant position and does not appear to move along the medium, whereas a traveling wave is a wave that moves along the medium while transferring energy. The key to creating a traveling wave from two standing waves is to determine if the properties of the two standing waves can be combined in such a way that the resultant wave has the properties of a traveling wave.
02

Consider the wave equations of standing waves and traveling waves

The wave equation for a standing wave can be written as: y(x,t) = 2A sin(kx) cos(ωt), where A is the amplitude, k is the wave number, ω is the angular frequency, x is the position, and t is the time. The wave equation for a traveling wave can be written as: y(x,t) = A sin(kx - ωt) or y(x,t) = A sin(kx + ωt), depending on the direction of propagation.
03

Combine two standing waves and analyze the result

Now, let's consider two standing waves y1 and y2 with the same amplitude A, wave number k, and angular frequency ω, but with a phase shift of π/2 between them: y1(x,t) = 2A sin(kx) cos(ωt) y2(x,t) = 2A cos(kx) sin(ωt) Now, we can try to combine the two standing waves using linear superposition: y_total(x,t) = y1(x,t) + y2(x,t) = 2A sin(kx) cos(ωt) + 2A cos(kx) sin(ωt) Now let's simplify the total wave equation using the trigonometric identity sin(A)cos(B) + cos(A)sin(B) = sin(A+B): y_total(x,t) = 2A [sin(kx) cos(ωt) + cos(kx) sin(ωt)] = 2A sin(kx + ωt)
04

Analyze the combined wave equation

Observing the simplified equation y_total(x,t) = 2A sin(kx + ωt), we can see that it resembles the equation of a traveling wave moving in the positive x-direction with amplitude 2A, wave number k, and angular frequency ω. Therefore, it is possible to combine two standing waves to create a traveling wave by ensuring that one wave has a phase shift of π/2 concerning the other.

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Key Concepts

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

Wave Superposition
The concept of wave superposition is a fundamental principle in physics that explains how waves interact with each other. When two or more waves travel through the same medium, they meet and combine to form a new wave; this process is called superposition. The resulting wave's amplitude at any point is the algebraic sum of the amplitudes of the individual waves at that point.

In the exercise, we explored how two standing waves could interact to form a traveling wave. Standing waves typically don't transfer energy from one place to another, while traveling waves do. By applying the principle of superposition, we can determine if the combination of two standing waves can result in a wave that has the properties of a traveling wave. When we combine two standing waves correctly, with a specific phase shift, we find that indeed a traveling wave can be created.

Moreover, superposition is not limited to standing waves; it applies to any kind of waves, including sound waves, light waves, and water waves. This principle helps us understand various phenomena in acoustics, optics, and fluid dynamics.
Wave Equations
The wave equation is a mathematical representation of the motion of waves through a medium. For different types of waves, the wave equation can take on different forms. Traveling and standing waves, for instance, are described by equations that highlight their distinct characteristics.

The equation given in the exercise for a standing wave—\( y(x,t) = 2A \sin(kx) \cos(\omega t) \)—illustrates a wave that oscillates in time but does not progress through space. In contrast, the equation for a traveling wave—either \( y(x,t) = A \sin(kx - \omega t) \) or \( y(x,t) = A \sin(kx + \omega t) \)—shows how the wave moves along the medium over time.

Understanding these equations is crucial because they tell us how wave properties like amplitude, wavelength, and frequency are related and how they affect the wave's behavior. These relationships are essential when studying wave interactions through the principle of superposition and identifying how to combine waves to achieve a desired effect.
Phase Shift
Phase shift in wave motion refers to a change in the phase of one wave relative to another. This can occur for a variety of reasons but often involves a difference in the starting point, or initial phase, of the waves. Phase shift can deeply affect the way waves combine and can be particularly important when trying to create a specific type of wave interaction, such as creating a traveling wave from two standing waves.

In the exercise we are considering, introducing a phase shift of \( \pi/2 \) between two standing waves and then applying wave superposition allows us to create a new wave characteristic—namely, a traveling wave. This phase shift is mathematically represented by a constant addition or subtraction in the sine or cosine functions within the wave equations. It leads to constructive and destructive interference that can either enhance or reduce the amplitude of the resultant wave at various points along the medium.
Trigonometric Identities
Trigonometric identities are mathematical equations that relate the sine, cosine, and tangent functions to one another. These identities are tools that help to simplify and manipulate expressions involving trigonometric functions. In the context of wave behavior, trigonometric identities allow us to combine wave equations in ways that might not be immediately obvious.

One crucial identity used in the step-by-step solution is \( \sin(A)\cos(B) + \cos(A)\sin(B) = \sin(A+B) \). By utilizing this identity, we can transform the combined equation of two standing waves into the equation for a traveling wave. This example underscores the significance of trigonometric identities in solving problems in wave mechanics and elsewhere in physics. Understanding these identities can give students a powerful resource for working with wave equations and analyzing wave interactions.

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Most popular questions from this chapter

Noise results from the superposition of a very large number of sound waves of various frequencies (usually in a continuous spectrum), amplitudes, and phases. Can interference arise with noise produced by two sources??

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 motorboat is coming? The speed of sound in water is \(1.50 \cdot 10^{3} \mathrm{~m} / \mathrm{s}\).

A string with linear mass density \(\mu=0.0250 \mathrm{~kg} / \mathrm{m}\) under a tension of \(F=250 . \mathrm{N}\) is oriented in the \(x\) -direction. Two transverse waves of equal amplitude and with a phase angle of zero (at \(t=0\) ) but with different angular frequencies \((\omega=3000 . \mathrm{rad} / \mathrm{s}\) and \(\omega / 3=1000 . \mathrm{rad} / \mathrm{s})\) are created in the string by an oscillator located at \(x=0 .\) The resulting waves, which travel in the positive \(x\) -direction, are reflected at a distant point where both waves have a node, so there is a similar pair of waves traveling in the negative \(x\) -direction. Find the values of \(x\) at which the first two nodes in the standing wave are produced by these four waves.

A traveling wave propagating on a string is described by the following equation: $$ y(x, t)=(5.00 \mathrm{~mm}) \sin \left(\left(157.08 \mathrm{~m}^{-1}\right) x-\left(314.16 \mathrm{~s}^{-1}\right) t+0.7854\right) $$ a) Determine the minimum separation, \(\Delta x_{\text {min }}\), between two points on the string that oscillate in perfect opposition of phases (move in opposite directions at all times). b) Determine the minimum separation, \(\Delta x_{A B}\), between two points \(A\) and \(B\) on the string, if point \(B\) oscillates with a phase difference of \(0.7854 \mathrm{rad}\) compared to point \(A\). c) Find the number of crests of the wave that pass through point \(A\) in a time interval \(\Delta t=10.0 \mathrm{~s}\) and the number of troughs that pass through point \(B\) in the same interval.

Fans at a local football stadium are so excited that their team is winning that they start "the wave" in celebration. Which of the following four statements is (are) true? I. This wave is a traveling wave. II. This wave is a transverse wave. III. This wave is a longitudinal wave. IV. This wave is a combination of a longitudinal wave and a transverse wave. a) I and II c) III only e) I and III b) II only d) I and IV

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