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If transverse waves on a string travel with a velocity of \(50 \mathrm{~m} / \mathrm{s}\) when the string is under a tension of \(20 \mathrm{~N},\) what tension on the string is required for the waves to travel with a velocity of \(30 \mathrm{~m} / \mathrm{s} ?\) a) \(7.2 \mathrm{~N}\) c) \(33 \mathrm{~N}\) e) \(45 \mathrm{~N}\) b) \(12 \mathrm{~N}\) d) \(40 \mathrm{~N}\) f) \(56 \mathrm{~N}\)

Short Answer

Expert verified
Answer: (a) 7.2 N

Step by step solution

01

Write down given information

We are given the following information: Initial wave speed \(v_1 = 50 \mathrm{~m} / \mathrm{s}\) Initial tension \(T_1 = 20 \mathrm{~N}\) Desired wave speed \(v_2 = 30 \mathrm{~m} / \mathrm{s}\) We need to find the desired tension \(T_2\).
02

Write down wave speed formula

We'll use the wave speed formula: \(v = \sqrt{\frac{T}{\mu}}\), where \(v\) is the wave speed, \(T\) is the tension, and \(\mu\) is the mass per unit length of the string.
03

Set up the relationship between initial and desired wave speeds and tension

We have the two wave speeds related to two different tensions, \(v_1 = \sqrt{\frac{T_1}{\mu}}\) and \(v_2 = \sqrt{\frac{T_2}{\mu}}\). Divide the first equation by the second equation to eliminate \(\mu\): \(\frac{v_1}{v_2}=\sqrt{\frac{T_1}{T_2}}\)
04

Solve for desired tension

Now we have a relationship we can use to find \(T_2\). First, square both sides of the equation: \(\frac{v_1^2}{v_2^2}=\frac{T_1}{T_2}\) Next, solve for \(T_2\): \(T_2 = T_1 \cdot \frac{v_2^2}{v_1^2}\) Plug the given values for \(v_1\), \(v_2\), and \(T_1\): \(T_2 = 20 \mathrm{N} \cdot \frac{(30 \mathrm{~m} / \mathrm{s})^2}{(50 \mathrm{~m} / \mathrm{s})^2}\) Solve for \(T_2\): \(T_2 = 20 \mathrm{N} \cdot \frac{900}{2500} \Rightarrow T_2 = 20 \mathrm{N} \cdot 0.36 \Rightarrow T_2 = 7.2 \mathrm{~N}\) The required tension for the waves to travel with a velocity of \(30 \mathrm{~m} / \mathrm{s}\) is \(7.2 \mathrm{~N}\), which corresponds to answer (a).

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Key Concepts

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

Wave Speed
Wave speed is simply the distance a wave travels per unit of time, or how fast the wave moves through a medium. In physics, wave speed is an essential concept because it ties together the physical properties of the medium and the wave properties themselves, such as frequency and wavelength.
To calculate wave speed, we use the formula \( v = \sqrt{\frac{T}{\mu}} \), where \( v \) is the wave speed, \( T \) is the tension in the medium (such as a string), and \( \mu \) is the mass per unit length.
For example, suppose a wave travels at 50 m/s on a string with a tension of 20 N. If the tension changes, the wave speed will also change, reflecting how tension in strings affects wave propagation.
Tension in Strings
Tension in strings significantly impacts wave behavior, particularly how fast the waves travel along the string. The tension refers to the pulling force applied along the string, which influences the string's tightness.
When a string is pulled tighter (increased tension), waves move faster across it. Conversely, if tension decreases, the wave speed lowers. This relationship stems from the inherent characteristic of mechanical waves: they require a medium to travel through, and that medium's properties, like tension, affect the wave's speed.
  • Positive correlation: Higher tension, higher wave speed.
  • Negative correlation: Lower tension, slower wave speed.
This concept is crucial in various applications, such as musical instruments, where string tension dictates the pitch of sound produced.
Transverse Waves
Transverse waves are waves where the direction of oscillation is perpendicular to the direction of the wave's movement. A common example includes waves on a string or the ripples on the water surface.
These waves can be visualized as a series of crests and troughs moving through the medium. For a transverse wave on a string, the motion of the string is up and down, while the wave propagates horizontally.
The wave speed in transverse waves, especially on strings, can be influenced by:
  • The tension in the string.
  • The mass per unit length of the string.
The higher the speed of transverse waves, the more energy is transferred in a given amount of time. Understanding transverse waves helps unveil how energy is distributed in waves, which is pivotal in fields such as acoustics and communication technologies.
Mass per Unit Length
Mass per unit length, denoted as \( \mu \), refers to the amount of mass contained in a segment of the string. It is calculated by dividing the total mass of the string by its length.
This parameter is crucial in determining the wave speed in strings because it directly influences how quickly waves can propagate. The formula showing this relationship is \( v = \sqrt{\frac{T}{\mu}} \), indicating that for a fixed tension, a string with lower mass per unit length will allow faster wave speeds.
  • Influences wave properties: Less mass, faster wave speed for a given tension.
  • Determines wave performance in musical instruments, engineering applications, etc.
Understanding mass per unit length helps optimize applications where wave speed regulation is vital, ensuring the desired performance and efficiency in real-world applications.

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Most popular questions from this chapter

Consider a linear array of \(n\) masses, each equal to \(m,\) connected by \(n+1\) springs, all massless and having spring constant \(k\), with the outer ends of the first and last springs fixed. The masses can move without friction in the linear dimension of the array. a) Write the equations of motion for the masses. b) Configurations of motion for which all parts of a system oscillate with the same angular frequency are called normal modes of the system; the corresponding angular frequencies are the system's normal-mode angular frequencies. Find the normal-mode angular frequencies of this array.

a) Starting from the general wave equation (equation 15.9 ), prove through direct derivation that the Gaussian wave packet described by the equation \(y(x, t)=(5.00 m) e^{-0.1(x-5 t)^{2}}\) is indeed a traveling wave (that it satisfies the differential wave equation). b) If \(x\) is specified in meters and \(t\) in seconds, determine the speed of this wave. On a single graph, plot this wave as a function of \(x\) at \(t=0, t=1.00 \mathrm{~s}, t=2.00 \mathrm{~s},\) and \(t=3.00 \mathrm{~s}\) c) More generally, prove that any function \(f(x, t)\) that depends on \(x\) and \(t\) through a combined variable \(x \pm v t\) is a solution of the wave equation, irrespective of the specific form of the function \(f\)

Students in a lab produce standing waves on stretched strings connected to vibration generators. One such wave is described by the wave function \(y(x, t)=(2.00 \mathrm{~cm}) \sin \left[\left(20.0 \mathrm{~m}^{-1}\right) x\right] \cos \left[\left(150 . \mathrm{s}^{-1}\right) t\right],\) where \(y\) is the transverse displacement of the string, \(x\) is the position along the string, and \(t\) is time. Rewrite this wave function in the form for a right- moving and a left-moving wave: \(y(x, t)=\) \(f(x-v t)+g(x+v t)\); that is, find the functions \(f\) and \(g\) and the speed, \(v\)

The tension in a 2.7 -m-long, 1.0 -cm-diameter steel cable \(\left(\rho=7800 \mathrm{~kg} / \mathrm{m}^{3}\right)\) is \(840 \mathrm{~N}\). What is the fundamental frequency of vibration of the cable?

A particular steel guitar string has mass per unit length of \(1.93 \mathrm{~g} / \mathrm{m}\). a) If the tension on this string is \(62.2 \mathrm{~N},\) what is the wave speed on the string? b) For the wave speed to be increased by \(1.0 \%\), how much should the tension be changed?

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