Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

A sinusoidal wave on a string is described by the equation \(y=(0.100 \mathrm{~m}) \sin (0.750 x-40.0 t),\) where \(x\) and \(y\) are in meters and \(t\) is in seconds. If the linear mass density of the string is \(10.0 \mathrm{~g} / \mathrm{m},\) determine (a) the phase constant, (b) the phase of the wave at \(x=2.00 \mathrm{~cm}\) and \(t=0.100 \mathrm{~s}\), (c) the speed of the wave, (d) the wavelength, (e) the frequency, and (f) the power transmitted by the wave.

Short Answer

Expert verified
Answer: The phase of the wave at position x = 2.00 cm and time t = 0.100 s is -4.00.

Step by step solution

01

Identify and calculate the phase constant

The phase constant is the constant term added inside the sinusoidal function. In our case, the wave equation is given by: \(y = (0.100 \mathrm{~m}) \sin(0.750x - 40.0t)\) The phase constant is the value -40.0t, so we can write that \(\phi = -40.0t\).
02

Calculate the phase of the wave at a specific position and time

To calculate the phase at position x = 2.00 cm and time t = 0.100 s, we plug in these values into the phase term we found in step 1: \(\phi(x,t) = -40.0 (0.100 \mathrm{~s}) = -4.00\)
03

Determine the wave's speed

The speed of the wave can be found from the coefficient of the time term in the phase. We have: \(\omega = 40.0 \mathrm{s}^{-1}\) The wave speed \(v\) is related to \(\omega\) and \(k\) (the coefficient of the x term) by \(v = \frac{\omega}{k}\). So, we can write: \(v = \frac{40.0 \mathrm{s}^{-1}}{0.750 \mathrm{m}^{-1}} = 53.3 \mathrm{m/s}\)
04

Calculate the wavelength

The wavelength \(\lambda\) is related to the wave number \(k\) by \(\lambda = \frac{2\pi}{k}\). So, we can write: \(\lambda = \frac{2\pi}{0.750 \mathrm{m}^{-1}} = 8.38 \mathrm{m}\)
05

Determine the frequency

The frequency \(f\) is related to the angular frequency \(\omega\) by \(f = \frac{\omega}{2\pi}\). So, we can write: \(f = \frac{40.0 \mathrm{s}^{-1}}{2\pi} = 6.37 \mathrm{Hz}\)
06

Calculate the power transmitted by the wave

The power transmitted by the wave can be calculated using the following formula: \(P = \frac{1}{2} \mu v^2 A^2 \omega^2\) where \(\mu\) is the linear mass density, \(A\) is the wave amplitude, and \(\omega\) is the angular frequency. We are given: \(\mu = 10.0 \mathrm{g/m} = 0.0100 \mathrm{kg/m}\) \(A = 0.100 \mathrm{m}\) \(\omega = 40.0 \mathrm{s}^{-1}\) We already found the wave speed \(v = 53.3 \mathrm{m/s}\). Now, we plug in these values into the power formula: \(P = \frac{1}{2} (0.0100 \mathrm{kg/m})(53.3 \mathrm{m/s})^2 (0.100 \mathrm{m})^2 (40.0 \mathrm{s}^{-1})^2\) \(P = 71.6 \mathrm{W}\) So, the power transmitted by the wave is 71.6 W.

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!

Key Concepts

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

Phase Constant
The phase constant in a sinusoidal wave equation plays a crucial role in determining the initial angle of the wave at the start of the observation. It is part of the equation that affects the horizontal shift of the wave pattern. In our exercise, the sinusoidal wave equation on a string is expressed as \(y=(0.100 \text{ m}) \sin (0.750x-40.0t)\), where \(\phi = -40.0t\) without any added constant term. This means that our phase constant \(\phi_0\) is effectively 0, as there is no separate constant value added or subtracted from the wave's expression. Therefore, the wave starts at its equilibrium position at \(t=0\).

Understanding the phase constant helps students grasp how the wave's position is affected at different times, and it is essential when studying wave interference, where the phase difference between waves can drastically change the resulting wave pattern.
Wave Speed
Wave speed is a fundamental property of a wave that describes how fast a wave travels through a medium. It is calculated from the equation of the wave, specifically from the relationship between the angular frequency \(\omega\) and the wave number \(k\). For the exercise, the angular frequency is \(\omega = 40.0 \text{s}^{-1}\) and \(k=0.750 \text{m}^{-1}\). Using the formula \(v = \frac{\omega}{k}\), we computed the wave speed to be \(v = 53.3 \text{m/s}\).

Wave speed is vital for understanding how wave properties such as wavelength and frequency are related—since \(v=\lambda f\), where \(\lambda\) is the wavelength and \(f\) is the frequency. This is why, in various applications such as communications and physics, knowing the wave speed enables us to calculate distances and signal timings effectively.
Wavelength
The wavelength, denoted by \(\lambda\), signifies the distance over which the wave's shape repeats. It is the distance between consecutive points that are in phase—meaning they are at the same stage in their oscillation. In our given problem, we determined the wavelength via the formula \(\lambda = \frac{2\pi}{k}\), which yielded a wavelength of \(\lambda = 8.38 \text{m}\).

The wavelength is directly related to the frequency of the wave, which is why these two properties are often discussed together. A shorter wavelength corresponds to a higher frequency, meaning the waves are more tightly packed, and vice versa. In practical scenarios, like sound waves or electromagnetic waves, the wavelength can determine properties like pitch and color respectively.
Frequency
Frequency is defined as the number of complete oscillations or cycles a wave undergoes per unit time, usually measured in hertz (Hz). It is calculated from the angular frequency \(\omega\) by the equation \(f = \frac{\omega}{2\pi}\). In our exercise, with an angular frequency of \(\omega = 40.0 \text{s}^{-1}\), we found the frequency of the wave to be \(f = 6.37 \text{Hz}\).

Frequency gives us an insight into how often the wave oscillates, which is essential for understanding phenomena like resonance—the tendency of a system to oscillate more powerfully at some frequencies—and wave energy. For instance, in acoustics, a higher frequency is perceived as a higher pitch.
Power Transmitted by a Wave
Power in the context of waves refers to the amount of energy that a wave carries per unit time, measured in watts (W). The power transmitted by a wave can be described using the formula \(P = \frac{1}{2} \mu v^2 A^2 \omega^2\), where \(\mu\) is the linear mass density, \(v\) is the wave speed, \(A\) is the amplitude, and \(\omega\) is the angular frequency. By substituting the given values into this formula, the exercise showed us that the power transmitted by the wave is 71.6 W.

The concept of power is crucial in many fields, from engineering and design of structures that must withstand different wave energies to the generation and transmission of electromagnetic waves in wireless communications. Understanding this aspect of wave physics can lead to the efficient transmission of energy and minimizing losses in various systems.

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

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.

The different colors of light we perceive are a result of the varying frequencies (and wavelengths) of the electromagnetic radiation. Infrared radiation has lower frequencies than does visible light, and ultraviolet radiation has higher frequencies than visible light does. The primary colors are red (R), yellow (Y), and blue (B). Order these colors by their wavelength, shortest to longest. a) \(\mathrm{B}, \mathrm{Y}, \mathrm{R}\) b) \(B, R, Y\) c) \(R, Y, B\) d) \(R, B, Y\)

A sinusoidal wave traveling in the positive \(x\) -direction has a wavelength of \(12.0 \mathrm{~cm},\) a frequency of \(10.0 \mathrm{~Hz},\) and an amplitude of \(10.0 \mathrm{~cm} .\) The part of the wave that is at the origin at \(t=0\) has a vertical displacement of \(5.00 \mathrm{~cm} .\) For this wave, determine the a) wave number, d) speed, b) period, e) phase angle, and c) angular frequency, f) equation of motion.

Two waves traveling in opposite directions along a string fixed at both ends create a standing wave described by \(y(x, t)=\) \(1.00 \cdot 10^{-2} \sin (25.0 x) \cos (1200 . t) .\) The string has a linear mass density of \(0.0100 \mathrm{~kg} / \mathrm{m},\) and the tension in the string is supplied by a mass hanging from one end. If the string vibrates in its third harmonic, calculate (a) the length of the string, (b) the velocity of the waves, and (c) the mass of the hanging mass.

A \(2.00-\mathrm{m}\) -long string of mass \(10.0 \mathrm{~g}\) is clamped at both ends. The tension in the string is \(150 .\) N. a) What is the speed of a wave on this string? b) The string is plucked so that it oscillates. What is the wavelength and frequency of the resulting wave if it produces a standing wave with two antinodes?

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