/*! 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 31 Two identical traveling waves, m... [FREE SOLUTION] | 91Ó°ÊÓ

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Two identical traveling waves, moving in the same direction, are out of phase by \(\pi / 2\) rad. What is the amplitude of the resultant wave in terms of the common amplitude \(y_{m}\) of the two combining waves?

Short Answer

Expert verified
The amplitude of the resultant wave is \( \sqrt{2}y_m \).

Step by step solution

01

Understand Wave Superposition

When two waves with identical frequency and amplitude travel in the same direction and combine, the resultant wave's amplitude can be determined by considering their phase difference. The principle of superposition allows us to add waves together to determine the resultant wave.
02

Represent Waves Mathematically

Let the two traveling waves be represented as: \[ y_1(x, t) = y_m \sin(kx - \omega t) \] \[ y_2(x, t) = y_m \sin(kx - \omega t + \phi) \] where \( \phi = \frac{\pi}{2} \) is the phase difference between the two waves.
03

Use Trigonometric Identity

Apply the sine addition formula to combine the waves:\[\sin A + \sin B = 2 \sin\left(\frac{A+B}{2}\right) \cos\left(\frac{A-B}{2}\right)\]For the waves, let \( A = kx - \omega t \) and \( B = kx - \omega t + \frac{\pi}{2} \), then:\[ y(x, t) = 2 y_m \sin \left( kx - \omega t + \frac{\pi}{4} \right) \cos \left( \frac{-\frac{\pi}{2}}{2} \right) \]
04

Simplify the Expression

Now evaluate the \( \cos \) term:\[\cos \left( \frac{-\pi}{4} \right) = \frac{\sqrt{2}}{2}\]So the resultant wave becomes:\[ y(x, t) = 2 y_m \cdot \frac{\sqrt{2}}{2}\sin \left( kx - \omega t + \frac{\pi}{4} \right) \]
05

Find Resultant Amplitude

Simplify the amplitude:\[ y(x, t) = \sqrt{2} \cdot y_m \cdot \sin \left( kx - \omega t + \frac{\pi}{4} \right) \]Thus, the amplitude of the resultant wave is \( \sqrt{2}y_m \).

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Key Concepts

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

Traveling Waves
Traveling waves are dynamic disturbances that move through a medium. Imagine throwing a stone into a pond. The ripples that spread outward are waves traveling away from the point of impact.
These waves carry energy and can be represented mathematically using equations that describe their sinusoidal nature, such as \(y(x, t) = y_m \sin(kx - \omega t)\) for a traveling wave. Here,
  • \(y(x, t)\) is the wave function showing how the wave varies with position \(x\) and time \(t\).
  • \(y_m\) is the amplitude, the maximum displacement of the wave.
  • \(k\) is the wave number, linking to the wavelength, which is the distance over which the wave's shape repeats.
  • \(\omega\) is the angular frequency, indicating how many cycles the wave goes through per unit of time.
Traveling waves are fundamental in understanding phenomena such as sound and light, illustrating how oscillations move through space over time.
Phase Difference
When discussing wave interference, phase difference is a crucial concept. It tells us the shift in phase between two waves. Think of phase as a fraction of a wave cycle, like a clock's hands displaying time together with the sine wave's peaks and troughs.
A phase difference occurs when two waves with similar characteristics, like frequency and amplitude, overlap but start out of sync. This difference is usually measured in radians or degrees.
In the given problem, the phase difference \(\phi\) between the waves is \(\frac{\pi}{2}\) radians. This means one wave leads or lags the other by a quarter of a wavelength.
  • If \(\phi\) is 0, waves are in phase, causing constructive interference where amplitudes add up maximally.
  • If \(\phi\) is \(\pi\), waves are out of phase, potentially leading to destructive interference where they cancel each other out.
  • Any other value of \(\phi\) results in partially constructive or destructive interference.
The specific phase difference influences the resultant wave's amplitude and can impact whether waves strengthen or weaken each other.
Sine Addition Formula
The sine addition formula is a mathematical tool used to add two sine functions together. It's particularly useful when dealing with the superposition of waves. The formula is expressed as:\[\sin A + \sin B = 2 \sin \left( \frac{A+B}{2} \right) \cos \left( \frac{A-B}{2} \right)\]This tool allows us to transform two separate sinusoidal functions into a single expression representing their combined effect.
In the exercise, each wave is characterized by its own phase, leading to a superposition problem where we need to find the resultant amplitude.
When applying this formula:
  • \(A\) and \(B\) are the phases of the individual waves.
  • The \(\sin\) terms capture the wave's shape, while the \(\cos\) term helps reflect the phase difference's impact.
  • For phases \(A = kx - \omega t\) and \(B = kx - \omega t + \frac{\pi}{2}\), the resultant wave combines these to yield a simplified single sine function.
The sine addition formula is integral in determining the amplitude modulation and the overall shape of the superposed wave and plays a key role in calculating the resultant wave's behavior.

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Most popular questions from this chapter

A \(100 \mathrm{~g}\) wire is held under a tension of \(250 \mathrm{~N}\) with one end at \(x=0\) and the other at \(x=10.0 \mathrm{~m}\). At time \(t=0\), pulse 1 is sent along the wire from the end at \(x=10.0 \mathrm{~m}\). At time \(t=30.0\) \(\mathrm{ms}\), pulse 2 is sent along the wire from the end at \(x=0 .\) At what position \(x\) do the pulses begin to meet?

(a) What is the fastest transverse wave that can be sent along a steel wire? For safety reasons, the maximum tensile stress to which steel wires should be subjected is \(7.00 \times 10^{8} \mathrm{~N} / \mathrm{m}^{2}\). The density of steel is \(7800 \mathrm{~kg} / \mathrm{m}^{3}\). (b) Does your answer depend on the diameter of the wire?

(a) Write an equation describing a sinusoidal transverse wave traveling on a cord in the positive direction of a \(y\) axis with an angular wave number of \(60 \mathrm{~cm}^{-1}\), a period of \(0.20 \mathrm{~s}\), and an amplitude of \(3.0 \mathrm{~mm}\). Take the transverse direction to be the \(z\) direction. (b) What is the maximum transverse speed of a point on the cord?

The function \(y(x, t)=(15,0 \mathrm{~cm}) \cos (\pi x-15 \pi t)\), with \(x\) in meters and \(t\) in seconds, describes a wave on a taut string. What is the transverse speed for a point on the string at an instant when that point has the displacement \(y=+12.0 \mathrm{~cm} ?\)

A sinusoidal transverse wave traveling in the negative direction of an \(x\) axis has an amplitude of \(1.00 \mathrm{~cm}\), a frequency of \(550 \mathrm{~Hz}\), and a speed of \(330 \mathrm{~m} / \mathrm{s}\). If the wave equation is of the form \(y(x, t)=y_{m} \sin (k x \pm \omega t)\), what are (a) \(y_{m},(\mathrm{~b}) \omega,(\mathrm{c}) k\), and (d) the correct choice of sign in front of \(\omega\) ?

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