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A transverse wave described by $$ y=(0 \cdot 02 \mathrm{~m}) \sin \left[\left(1 \cdot 0 \mathrm{~m}^{-1}\right) x+\left(30 \mathrm{~s}^{-1}\right) t\right] $$ propagates on a stretched string having a linear mass density of \(1 \cdot 2 \times 10^{-4} \mathrm{~kg} \mathrm{~m}^{-1}\). Find the tension in the string.

Short Answer

Expert verified
The tension in the string is 1.08 N.

Step by step solution

01

Identify given parameters

The transverse wave equation is given by \( y = (0.02 \text{ m}) \sin[(1.0 \text{ m}^{-1})x + (30 \text{ s}^{-1})t] \). From this, we identify: \( k = 1.0 \text{ m}^{-1} \) as the wave number and \( \omega = 30 \text{ s}^{-1} \) as the angular frequency. The linear mass density \( \mu = 1.2 \times 10^{-4} \text{ kg m}^{-1} \).
02

Use the wave speed formula

The wave speed \( v \) can be found using the relationship between angular frequency and wave number: \[ v = \frac{\omega}{k} \]Substitute \( \omega = 30 \text{ s}^{-1} \) and \( k = 1 \text{ m}^{-1} \).
03

Calculate the wave speed

Substitute the values into the formula: \[ v = \frac{30}{1} = 30 \text{ m/s} \] Thus, the wave speed is \( 30 \text{ m/s} \).
04

Use the formula for tension in the string

The tension \( T \) in the string can be found using the wave speed and linear mass density with the formula:\[ v = \sqrt{\frac{T}{\mu}} \]Rearrange to solve for \( T \):\[ T = v^2 \mu \]
05

Calculate the tension in the string

Substitute \( v = 30 \text{ m/s} \) and \( \mu = 1.2 \times 10^{-4} \text{ kg m}^{-1} \) into the tension formula: \[ T = (30)^2 \times 1.2 \times 10^{-4} = 1.08 \text{ N} \]The tension in the string is \( 1.08 \text{ N} \).

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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 an important concept when analyzing waves. It tells us how fast a wave is traveling through a medium, like a stretched string. To find the speed of a wave, we use the relationship between the angular frequency and the wave number. The formula is:
  • \( v = \frac{\omega}{k} \)
Here, \( v \) represents wave speed, \( \omega \) represents angular frequency, and \( k \) is the wave number. In our exercise, \( \omega = 30 \, \text{s}^{-1} \) and \( k = 1 \, \text{m}^{-1} \). By substituting these values into the formula, the wave speed \( v \) is calculated to be 30 meters per second. This means the wave travels at 30 m/s through the string. Understanding wave speed helps us predict how quickly and how far the wave will move along the string in a given time.
linear mass density
Linear mass density, often denoted as \( \mu \), is a measure of how much mass is distributed along a unit length of a string or other linear medium. It is expressed in kilograms per meter (kg/m). In the context of waves traveling on a string, linear mass density significantly affects the wave's properties.For this problem, the linear mass density \( \mu \) is given as \( 1.2 \times 10^{-4} \, \text{kg/m} \). This means every meter of string has a mass of \( 1.2 \times 10^{-4} \) kilograms. Linear mass density plays a crucial role in determining wave speed and tension. By understanding \( \mu \), we can better predict how the string will respond to the forces applied by the wave. The relationship between linear mass density, wave speed, and tension is vital for accurately calculating the tension in the string.
tension in string
Tension in a string refers to the force exerted along the string, which impacts how waves propagate through it. To quantify this tension, we use the wave speed formula in conjunction with the linear mass density. The formula is:
  • \( v = \sqrt{\frac{T}{\mu}} \)
Where \( v \) is the wave speed, \( T \) is the tension in the string, and \( \mu \) is the linear mass density. The rearranged formula to find tension, \( T \), is:
  • \( T = v^2 \mu \)
In our exercise, we substitute the known wave speed (\( v = 30 \, \text{m/s} \)) and linear mass density (\( \mu = 1.2 \times 10^{-4} \, \text{kg/m} \)) into the formula. Calculating further, we find the tension \( T = 1.08 \, \text{N} \). This tension supports the wave as it moves, ensuring stability in its propagation through the medium. Understanding the tension is crucial because it helps predict how the string behaves under the influence of waves.

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Most popular questions from this chapter

A \(2 \mathrm{~m}\) -long string fixed at both ends is set into vibrations in its first overtone. The wave speed on the string is \(200 \mathrm{~m} \mathrm{~s}^{-1}\) and the amplitude is \(0 \cdot 5 \mathrm{~cm}\). (a) Find the wavelength and the frequency. (b) Write the equation giving the displacement of different points as a function of time. Choose the \(X\) -axis along the string with the origin at one end and \(t=0\) at the instant when the point \(x=50 \mathrm{~cm}\) has reached its maximum displacement.

A wire, fixed at both ends is seen to vibrate at a resonant frequency of \(240 \mathrm{~Hz}\) and also at \(320 \mathrm{~Hz} .\) (a) What could be the maximum value of the fundamental frequency? (b) If transverse waves can travel on this string at a speed of \(40 \mathrm{~m} \mathrm{~s}^{-1}\), what is its length ?

A string of length \(40 \mathrm{~cm}\) and weighing \(10 \mathrm{~g}\) is attached to a spring at one end and to a fixed wall at the other end. The spring has a spring constant of \(160 \mathrm{~N} \mathrm{~m}^{-1}\) and is stretched by \(1 \cdot 0 \mathrm{~cm}\). If a wave pulse is produced on the string near the wall, how much time will it take to reach the spring?

A motorcycle has to move with a constant speed on an overbridge which is in the form of a circular arc of radius \(R\) and has a total length \(L\). Suppose the motorcycle starts from the highest point. (a) What can its maximum velocity be for which the contact with the road is not broken at the highest point ? (b) If the motorcycle goes at speed \(1 / \sqrt{2}\) times the maximum found in part (a), where will it lose the contact with the road ? (c) What maximum uniform speed can it maintain on the bridge if it does not lose contact anywhere on the bridge?

A transverse wave of amplitude \(0.50 \mathrm{~mm}\) and frequency \(100 \mathrm{~Hz}\) is produced on a wire stretched to a tension of \(100 \mathrm{~N}\). If the wave speed is \(100 \mathrm{~m} \mathrm{~s}^{-1}\), what average power is the source transmitting to the wire?

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