The two waves \(\eta_{1}=6 \cos \left(k x-\omega t+\frac{1}{8} \pi\right)\) and \(\eta_{2}=8 \sin \left(k x-\omega t+\frac{1}{8} \pi\right)\) are traveling on a stretched string. ( \(a\) ) Find the complex representation of these waves. \((b)\) Find the complex wave equivalent to their sum \(\eta_{1}+\eta_{2}\) and the physical (real) wave that it represents. (c) Endeavor to combine the two waves by working only with trigonometric identities in the real domain.

Short Answer

Expert verified
Answer: The real wave that represents the sum of the two given waves is \(\eta_1 + \eta_2 = 2\{3\cos(kx-\omega t+\frac{1}{8}\pi) + 4\sin(kx-\omega t+\frac{1}{8}\pi)\}\).

Step by step solution

01

Convert waves to complex form

Using Euler's formula, we can convert the trigonometric functions in the given waves into complex exponentials: \(\eta_1 = 6 \cos(kx-\omega t+\frac{1}{8}\pi) = 3e^{i(kx-\omega t+\frac{1}{8}\pi)} + 3e^{-i(kx-\omega t+\frac{1}{8}\pi)}\) \(\eta_2 = 8 \sin(kx-\omega t+\frac{1}{8}\pi) = 4ie^{i(kx-\omega t+\frac{1}{8}\pi)} - 4ie^{-i(kx-\omega t+\frac{1}{8}\pi)}\)
02

Add complex forms of waves

To find the complex wave equivalent to their sum, we add the complex forms of \(\eta_1\) and \(\eta_2\) together: \(\eta_1 + \eta_2 = (3 + 4i)e^{i(kx-\omega t+\frac{1}{8}\pi)} + (3 - 4i)e^{-i(kx-\omega t+\frac{1}{8}\pi)}\)
03

Convert complex wave sum back to real form

Now we need to convert this complex wave back to a real wave, using Euler's formula again: \(\eta_1 + \eta_2 = 2\{(3 + 4i)\cos(kx-\omega t+\frac{1}{8}\pi) + (3 - 4i)\cos(-kx+\omega t-\frac{1}{8}\pi)\}\) \(\eta_1 + \eta_2 = 2\{3\cos(kx-\omega t+\frac{1}{8}\pi) + 4\sin(kx-\omega t+\frac{1}{8}\pi)\}\)
04

Combine waves using trigonometric identities

In this step, we will attempt to combine the real waves given, using trigonometric identities, and compare the result with our solution from Step 3: \(\eta_1 + \eta_2 = 6 \cos(kx-\omega t+\frac{1}{8}\pi) + 8 \sin(kx-\omega t+\frac{1}{8}\pi)\) Using the angle addition formula \(\cos(A+B)=\cos(A)\cos(B)-\sin(A)\sin(B)\) and \(\sin(A+B)=\sin(A)\cos(B)+\cos(A)\sin(B)\), we rewrite the sum as: \(\eta_1 + \eta_2 = 2\{3\cos(kx-\omega t+\frac{1}{8}\pi) + 4\sin(kx-\omega t+\frac{1}{8}\pi)\}\) This matches the result in Step 3, hence the answer is consistent. The real wave that represents the sum of the two waves is given by: \(\eta_1 + \eta_2 = 2\{3\cos(kx-\omega t+\frac{1}{8}\pi) + 4\sin(kx-\omega t+\frac{1}{8}\pi)\}\)

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 Vaia!

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

Show how the solution \((1.5 .5)\) of the wave equation can be transformed into a general traveling-wave solution.

Three long identical strings of linear mass density \(\lambda_{0}\) are joinzd together at a common point forming a symmetrical Y. Thus they lie in a plane \(120^{\circ}\) apart. Each is given the same tension \(\tau_{0 .}\) A distant source of sinusoidal waves sends transverse waves, with motion perpendicular to the plane of the strings, down one of the strings. Find the reflection and transmission coefficients that characterize the junction.

Show that energy flow and total energy are related by the continuity equation (see Prob. 1.8.4) $$ \frac{\partial P}{\partial x}=-\frac{\partial E_{1}}{\partial t} $$ by multiplying each side of the wave equation \((1,11,6)\) by \(\partial_{\eta} / \partial l\) and carrying out a development analogous to that leading to \((1.11 .15)\). Using \((1.11 .15)\) and \((1.11 .20)\), show that \(P, g_{x}\), and \(E_{1}\) are all solutions of the usual wave equation, with the wave velocity \(c=\left(r_{0} / \lambda_{0}\right)^{1 / 2}\).

It is desired to express the function \(y(x)=l x-x^{2}\) in the interval \(0 \leq x \leq l / 2\) by a Fourier series. Investigate how to piece it out so that it becomes a periodic function, of period \(2 l\), so that the Fourier series converges as rapidly as possible. Obtain the Fourier series and plot curves showing the sum of one, two, and three terms of the series, as well as the function \(y(x)\) that it represents.

The two waves \(\eta_{1}=A_{1} \cos (\kappa x-\omega t)\) and \(\eta_{2}=A_{2} \cos (\kappa x+\omega t)\) travel together on a stretched string. Show how the wave amplitude ratio \(A_{1} / A_{2}\) can be found from a measurement of the so-called standing-wave ratio \(S\) of the resulting wave pattern, which is defined as the ratio of the maximum amplitude to the minimum amplitude of the envelope of this pattern. Note that \(S\) and the position and amplitude of the minima (or maxima) wave disturbance uniquely determine the two traveling waves that give rise to the standing-wave pattern.

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.

Sign-up for free