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One end of a horizontal rope is attached to a prong of an electrically driven tuning fork that vibrates the rope transversely at 120 Hz. The other end passes over a pulley and supports a 1.50-kg mass. The linear mass density of the rope is 0.0480 kg/m. (a) What is the speed of a transverse wave on the rope? (b) What is the wavelength? (c) How would your answers to parts (a) and (b) change if the mass were increased to 3.00 kg?

Short Answer

Expert verified
(a) 17.46 m/s; (b) 0.1455 m; increasing mass to 3.00 kg gives (c) 24.67 m/s and 0.2056 m respectively.

Step by step solution

01

Understanding Wave Speed on a String

The wave speed \( v \) on a string is determined by the formula \( v = \sqrt{\frac{T}{\mu}} \), where \( T \) is the tension in the string and \( \mu \) is the linear mass density. The tension \( T \) is the weight of the mass and is given by \( T = mg \), where \( m \) is the mass and \( g \) is the acceleration due to gravity (approximately 9.8 \( m/s^2 \)).
02

Calculating Tension with 1.50 kg Mass

Calculate the tension in the rope when the mass is 1.50 kg. Using \( T = mg \), we find \( T = (1.50 \, \text{kg}) \times (9.8 \, \text{m/s}^2) = 14.7 \, \text{N} \).
03

Calculating Wave Speed with 1.50 kg Mass

Substitute the values of \( T \) (14.7 N) and \( \mu \) (0.0480 kg/m) into the wave speed formula: \( v = \sqrt{\frac{14.7}{0.0480}} \). This results in a wave speed \( v \approx 17.46 \, \text{m/s} \).
04

Calculating Wavelength for 1.50 kg Mass

The wavelength \( \lambda \) can be determined from the relationship \( v = f \lambda \), where \( f = 120 \, \text{Hz} \). Using \( v = 17.46 \, \text{m/s} \), solve for \( \lambda \): \( \lambda = \frac{v}{f} = \frac{17.46}{120} \approx 0.1455 \, \text{m} \).
05

Calculating Wave Speed with 3.00 kg Mass

Now increase the mass to 3.00 kg. Calculate the tension: \( T = (3.00 \, \text{kg}) \times (9.8 \, \text{m/s}^2) = 29.4 \, \text{N} \). Then the wave speed is \( v = \sqrt{\frac{29.4}{0.0480}} \approx 24.67 \, \text{m/s} \).
06

Calculating Wavelength for 3.00 kg Mass

Using the new wave speed \( v = 24.67 \, \text{m/s} \), calculate the new wavelength: \( \lambda = \frac{v}{f} = \frac{24.67}{120} \approx 0.2056 \, \text{m} \).

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Key Concepts

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

Transverse Waves
Transverse waves are a type of wave where the motion of the medium is perpendicular to the direction of the wave. In the case of a rope being vibrated by a tuning fork, the rope moves up and down, while the wave travels horizontally along the rope. These waves occur frequently in various forms, such as waves on a string or ripples on the surface of water.
Understanding transverse waves is crucial as it helps us analyze how energy is transferred through these mediums without the medium itself moving far from its original position. This concept applies not just to physical ropes but also to electromagnetic waves, where electric and magnetic fields oscillate perpendicular to the direction of wave travel.
For students working through the exercise, visualizing the up-and-down movement of the rope while picturing the wave moving forward can clarify the transverse nature of these waves.
Wave Speed
Wave speed is how fast a wave travels through a medium. For transverse waves on a string, the wave speed can be calculated using the formula: \[ v = \sqrt{\frac{T}{\mu}} \]where \( v \) is the wave speed, \( T \) is the tension in the string, and \( \mu \) is the linear mass density of the string.
This formula illustrates that the speed of the wave is influenced by both the tension and the mass density of the string.
  • If the tension is higher, the wave speed increases. Think of pulling a string very tight - vibrations move faster because there's more force along the string.
  • a higher mass density (meaning the string is "heavier" for its length) slows down the wave, much like pushing a denser object takes more energy.
Understanding these factors helps in predicting and explaining the behavior of different waves in physics and in practical scenarios.
Wavelength
Wavelength refers to the distance between two consecutive crests or troughs of a wave. It represents one complete cycle of the wave. For the exercise, the wavelength was calculated using the equation:\[ \lambda = \frac{v}{f} \]where \( \lambda \) is the wavelength, \( v \) is the wave speed, and \( f \) is the frequency.
The frequency in this context is how often the wave cycles occur per second, measured in hertz (Hz). A higher wave speed or a lower frequency results in a longer wavelength.
  • This means with a faster or less frequent wave, the distance between peaks will increase.
  • Conversely, if a wave is traveling slower or cycling rapidly, the wavelength shortens.
When calculating, never forget that any change in wave speed or frequency impacts the wavelength directly, showing the dynamic nature of waves in physics.
Tension in Strings
Tension in strings is a critical factor influencing wave mechanics. It is the force exerted along the string when it is pulled tight. In the exercise, the tension \( T \) is calculated using:\[ T = mg \]where \( m \) is the mass hanging from the string and \( g \) is the acceleration due to gravity \((9.8 \, \text{m/s}^2)\).
This tension is what allows the wave to travel through the string. Larger masses increase the tension, leading to faster waves because the stronger force makes the string more responsive to vibrational movements. Conversely, less tension slows the wave. Consider:
  • A dramatically tighter string (more tension) supports faster traveling waves, like a drum, which is taut so it can produce sound efficiently.
  • If the string is loose, the wave speed decreases, leading to a less "energetic" system.
Understanding tension and its impact on wave speed is essential for studying mechanical waves and their applications in areas from music to engineering.

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Most popular questions from this chapter

A 1.50-m-long rope is stretched between two supports with a tension that makes the speed of transverse waves 62.0 m/s. What are the wavelength and frequency of (a) the fundamental; (b) the second overtone; (c) the fourth harmonic?

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?

Provided the amplitude is sufficiently great, the human ear can respond to longitudinal waves over a range of frequencies from about 20.0 Hz to about 20.0 kHz. (a) If you were to mark the beginning of each complete wave pattern with a red dot for the long-wavelength sound and a blue dot for the short- wavelength sound, how far apart would the red dots be, and how far apart would the blue dots be? (b) In reality would adjacent dots in each set be far enough apart for you to easily measure their separation with a meter stick? (c) Suppose you repeated part (a) in water, where sound travels at 1480 m/s. How far apart would the dots be in each set? Could you readily measure their separation with a meter stick?

A fellow student with a mathematical bent tells you that the wave function of a traveling wave on a thin rope is \(y(x, t) = 2.30 \, \mathrm{mm} \, \mathrm{cos} [(6.98 \, \mathrm{rad/m})x \space + 1742 \, \mathrm{rad/s})t]\). Being more practical, you measure the rope to have a length of 1.35 m and a mass of 0.00338 kg. You are then asked to determine the following: (a) amplitude; (b) frequency; (c) wavelength; (d) wave speed; (e) direction the wave is traveling; (f) tension in the rope; (g) average power transmitted by the wave.

A 1.50-m string of weight 0.0125 N is tied to the ceiling at its upper end, and the lower end supports a weight W. Ignore the very small variation in tension along the length of the string that is produced by the weight of the string. When you pluck the string slightly, the waves traveling up the string obey the equation $$y(x, t) = (8.50 \, \mathrm{mm}) \mathrm{cos}(172 \, \mathrm{rad/m} \space x - 4830 \, \mathrm{rad/s} \space t)$$ Assume that the tension of the string is constant and equal to \(W\). (a) How much time does it take a pulse to travel the full length of the string? (b) What is the weight \(W\)? (c) How many wavelengths are on the string at any instant of time? (d) What is the equation for waves traveling \(down\) the string?

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