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A transverse wave on a rope is given by $$y(x, t) = (0.750 \, \mathrm{cm}) \mathrm{cos} \space \pi[(10.400 \, \mathrm{cm}^{-1})x + (250 \mathrm s^{-1})t]$$ (a) Find the amplitude, period, frequency, wavelength, and speed of propagation. (b) Sketch the shape of the rope at these values of \(t:\) 0, 0.0005 s, 0.0010 s. (c) Is the wave traveling in the \(+x-\) or \(-x\)-direction? (d) The mass per unit length of the rope is 0.0500 kg/m. Find the tension. (e) Find the average power of this wave.

Short Answer

Expert verified
(a) A = 0.750 cm, T ≈ 0.0251 s, f ≈ 39.8 Hz, λ ≈ 0.604 cm, v ≈ 24.027 cm/s. (b) See sketched shapes. (c) -x direction. (d) T ≈ 2.89 N. (e) P ≈ 4.23 W.

Step by step solution

01

Identify Wave Parameters from Equation

The given wave equation is written as: \[ y(x, t) = (0.750 \, \mathrm{cm}) \cos \left(\pi\left[(10.400 \, \mathrm{cm}^{-1})x + (250 \, \mathrm{s}^{-1})t \right]\right) \] Comparing it with the standard wave form \( y(x,t) = A \cos(kx + \omega t) \), we identify the amplitude \(A = 0.750 \, \mathrm{cm} \), the wave number \(k = 10.400 \, \mathrm{cm}^{-1} \), and the angular frequency \(\omega = 250 \, \mathrm{s}^{-1} \).
02

Calculate the Amplitude

The amplitude \( A \) is the coefficient part of the cosine in the equation. Thus, \[ A = 0.750 \, \mathrm{cm} \].
03

Calculate the Wavelength

The wave number \( k \) is related to the wavelength \( \lambda \) by the formula \( k = \frac{2\pi}{\lambda} \). Solving for \( \lambda \) gives:\[ \lambda = \frac{2\pi}{k} = \frac{2\pi}{10.400} \approx 0.604 \, \mathrm{cm} \].
04

Calculate the Period

The angular frequency \( \omega \) is related to the period \( T \) by \( \omega = \frac{2\pi}{T} \). Solving for \( T \) gives:\[ T = \frac{2\pi}{\omega} = \frac{2\pi}{250} \approx 0.0251 \, \mathrm{s} \].
05

Calculate the Frequency

Frequency \( f \) is the reciprocal of the period. Hence,\[ f = \frac{1}{T} = \frac{1}{0.0251} \approx 39.8 \, \mathrm{Hz} \].
06

Calculate Wave Speed

The wave speed \( v \) is the product of wavelength \( \lambda \) and frequency \( f \). Thus,\[ v = \lambda f = 0.604 \, \mathrm{cm} \times 39.8 \, \mathrm{Hz} \approx 24.027 \, \mathrm{cm/s} \].
07

Determine Wave Direction

The term \([kx + \omega t]\) in the cosine argument indicates the wave is traveling in the \(-x\)-direction because the sign is positive (in the form of \(kx - \omega t\), the negative would indicate \(+x\)-direction).
08

Sketch the Shape of the Rope

For times \( t = 0, 0.0005, \text{and} \ 0.0010 \, \mathrm{s} \), calculate \( y(x, t) \) at these times and sketch the wave shape, considering shifts due to time differences.
09

Find Tension in the Rope

The wave speed \( v \) is related to tension \( T \) and linear mass density \( \mu \) by \( v = \sqrt{\frac{T}{\mu}} \). Solving for \( T \) by rearranging gives:\[ T = \mu v^2 = 0.0500 \, \mathrm{kg/m} \times (0.24027 \, \mathrm{m/s})^2 \approx 2.89 \, \mathrm{N} \].
10

Calculate Average Power of the Wave

The average power \( P \) is given by \( P = \frac{1}{2} \mu v \omega^2 A^2 \). Substituting the known values gives:\[ P = \frac{1}{2} \times 0.0500 \, \mathrm{kg/m} \times 0.24027 \, \mathrm{m/s} \times (250 \, \mathrm{s}^{-1})^2 \times (0.0075 \, \mathrm{m})^2 \approx 4.23 \, \mathrm{W} \].

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Key Concepts

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

Amplitude and Frequency
Amplitude and frequency are two key characteristics of waves. The amplitude represents the maximum displacement of a wave from its rest position. In the exercise, it is given as 0.750 cm. This is easily found by inspecting the wave equation's cosine's coefficient. The amplitude is a measure of the wave's height, indicating how far the wave's peak is from its baseline.
If you look at the wave equation, it relates amplitude to the energy a wave carries. The larger the amplitude, the more energy the wave transmits.
Frequency, on the other hand, is the number of cycles a wave completes in one second. It is found by taking the reciprocal of the wave's period. For our specific problem, the period was calculated to be approximately 0.0251 seconds. Thus, the frequency is around 39.8 Hz. Frequency indicates how fast a wave oscillates and is crucial in determining the type of sound or light emitted by the wave.
Wave Speed Calculation
Understanding wave speed is crucial as it determines how fast a wave travels through a medium. The wave speed, for this problem, is calculated using the relation between frequency and wavelength. The product of these two factors gives the wave speed:
- Wavelength (\(\lambda\)) measures the distance between consecutive wave crests, calculated as approximately 0.604 cm.
- Frequency (\(f\)) is approximately 39.8 Hz, as discussed previously.
For the given wave, these yield a wave speed, \(v\), of approximately 24.027 cm/s.
Wave speed directly depends on the properties of the medium through which the wave propagates. Different media cause waves to travel at different speeds, impacted by factors such as tension and density.
Wave Direction
The direction in which a wave travels determines how it affects its surroundings. In the context of the given exercise, determining the wave direction involves examining the sign in the wave equation. The argument of the cosine function in the wave equation uses the form \(kx + \omega t\), which indicates motion in the negative x-direction.
When you observe the formulation \(kx + \omega t\), the positive sign implies that as time progresses, the wave appears to move backwards, relative to the x-axis. Understanding wave direction is pivotal for predicting how waves interact with boundaries, other waves, and objects.
Tension in a Rope
Tension in a rope is a critical factor influencing how waves, like the one described, propagate through it. Tension refers to the force exerted along the rope that keeps it taut, and can be calculated using wave speed and the mass per unit length of the rope. For example:
- The wave speed \(v\) is approximately 24.027 cm/s.
- The linear mass density \(\mu\) is given as 0.0500 kg/m.
Using the relation \(v = \sqrt{\frac{T}{\mu}}\), we solve for tension, \(T\), which approximately equals 2.89 N in this case.
Tension affects the ease with which waves can travel, with greater tension allowing for faster wave speeds. This is crucial in applications ranging from musical instruments to engineering.
Average Power of a Wave
The average power of a wave indicates the rate at which energy is transported by the wave through the medium. In the exercise, it is given by the formula:
\[ P = \frac{1}{2} \mu v \omega^2 A^2 \]
where:
  • \(\mu\) is the linear mass density (0.0500 kg/m).
  • \(v\) is the wave speed (0.24027 m/s).
  • \(\omega\) is the angular frequency (250 s\(^{-1}\)).
  • \(A\) is the amplitude (0.0075 m).
Substituting these values results in 4.23 W, highlighting the power with which this wave transmits energy. Understanding wave power is essential for harnessing waves in technologies such as acoustics, seismology, and telecommunications.

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Most popular questions from this chapter

(a) A horizontal string tied at both ends is vibrating in its fundamental mode. The traveling waves have speed \(v\), frequency \(f\), amplitude \(A\), and wavelength \(\lambda\). Calculate the maximum transverse velocity and maximum transverse acceleration of points located at (i) \(x = \lambda/2\), (ii) \(x = \lambda /4\), and (iii) \(x = \lambda /8\), from the left-hand end of the string. (b) At each of the points in part (a), what is the amplitude of the motion? (c) At each of the points in part (a), how much time does it take the string to go from its largest upward displacement to its largest downward displacement?

A water wave traveling in a straight line on a lake is described by the equation $$y(x, t) = (\mathrm{2.75 \, cm) cos(0.410 \mathrm{rad/cm} \, \textit{x}} + 6.20 \, \mathrm{rad}/s \; t)$$ where y is the displacement perpendicular to the undisturbed surface of the lake. (a) How much time does it take for one complete wave pattern to go past a fisherman in a boat at anchor, and what horizontal distance does the wave crest travel in that time? (b) What are the wave number and the number of waves per second that pass the fisherman? (c) How fast does a wave crest travel past the fisherman, and what is the maximum speed of his cork floater as the wave causes it to bob up and down?

(a) A horizontal string tied at both ends is vibrating in its fundamental mode. The traveling waves have speed \(v\), frequency \(f\), amplitude \(A\), and wavelength \(\lambda\). Calculate the maximum transverse velocity and maximum transverse acceleration of points located at (i) \(x = \lambda/2\), (ii) \(x = \lambda\)/4, and (iii) \(x = \lambda\)8, from the left-hand end of the string. (b) At each of the points in part (a), what is the amplitude of the motion? (c) At each of the points in part (a), how much time does it take the string to go from its largest upward displacement to its largest downward displacement?

A thin string 2.50 m in length is stretched with a tension of 90.0 N between two supports. When the string vibrates in its first overtone, a point at an antinode of the standing wave on the string has an amplitude of 3.50 cm and a maximum transverse speed of 28.0 m/s. (a) What is the string's mass? (b) What is the magnitude of the maximum transverse acceleration of this point on the string?

A strong string of mass 3.00 g and length 2.20 m is tied to supports at each end and is vibrating in its fundamental mode. The maximum transverse speed of a point at the middle of the string is 9.00 m/s. The tension in the string is 330 N. (a) What is the amplitude of the standing wave at its antinode? (b) What is the magnitude of the maximum transverse acceleration of a point at the antinode?

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