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A \(100 \mathrm{~g}\) wire is held under a tension of \(250 \mathrm{~N}\) with one end at \(x=0\) and the other at \(x=10.0 \mathrm{~m}\). At time \(t=0\), pulse 1 is sent along the wire from the end at \(x=10.0 \mathrm{~m}\). At time \(t=30.0\) \(\mathrm{ms}\), pulse 2 is sent along the wire from the end at \(x=0 .\) At what position \(x\) do the pulses begin to meet?

Short Answer

Expert verified
The pulses meet at 4.74 m from x = 0.

Step by step solution

01

Calculate the Speed of the Waves on the Wire

To find the speed of the waves on the wire, we need to use the formula for wave speed on a stretched string: \[ v = \sqrt{\frac{T}{\mu}} \]where \( T = 250 \text{ N} \) is the tension, and \( \mu \) is the linear mass density of the wire. The mass of the wire is \( 100\, \text{g} \) which is \( 0.1\, \text{kg} \), and the length of the wire is \( 10.0\, \text{m} \). Thus, \( \mu = \frac{0.1}{10.0} = 0.01\, \text{kg/m} \). Substitute in the values:\[v = \sqrt{\frac{250}{0.01}} = \sqrt{25000} = 158.11\, \text{m/s} \]

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Key Concepts

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

Tension in a String
Tension plays a crucial role in determining the speed at which waves travel along a string or wire. In physics, tension refers to the pulling force exerted by a string, cable, chain, or similar object when it is stretched tightly. This force is essential for understanding how waves move through strings or wires.

When dealing with tension, we utilize the formula for wave speed on a string, which is given by \( v = \sqrt{\frac{T}{\mu}} \), where \( T \) stands for the tension force within the string. The higher the tension, the faster a wave can travel along the string.

In practical scenarios, increasing the tension increases the wave speed — think of a guitar string becoming stiffer and producing a higher frequency sound when tightened. Thus, understanding tension helps in applications such as musical instruments, engineering designs, and various physics experiments.
Linear Mass Density
Linear mass density is a measure of how much mass is distributed along a unit length of a string or wire. It is represented by the symbol \( \mu \). The formula to determine linear mass density is \( \mu = \frac{m}{L} \), where \( m \) is the mass of the string, and \( L \) is its length.

In our context, a wire with a mass of 100 g (or 0.1 kg) and a length of 10.0 m gives us a linear mass density of \( \mu = 0.01 \text{ kg/m} \).

Understanding the impact of linear mass density is essential because it directly influences the wave speed through a string — lower density can lead to higher wave speeds, assuming tension is constant. This principle is useful in designing wires and strings for specific wave speeds, especially in scenarios where precise control over wave propagation is necessary.
Wave Interference
Wave interference occurs when two or more waves travel through the same medium, interacting with each other as they overlap. When wave pulses are sent along a wire from opposite directions, they meet at some point and exhibit interference — either constructive or destructive.

Constructive interference happens when waves meet in phase, merging to create a wave of greater amplitude. Conversely, destructive interference occurs when waves meet out of phase, resulting in diminished or canceled amplitudes.

In the exercise scenario, pulses are sent from either end of the wire at different times. Calculating the speed helped us determine when and where these pulses would begin to meet, providing us a practical application of wave interference. Eventually, understanding how and where waves meet helps in numerous fields such as acoustics (sound waves), optics (light waves), and even in analyzing tidal patterns (water waves).

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Most popular questions from this chapter

A transverse sinusoidal wave is generated at one end of a long, horizontal string by a bar that moves up and down through a distance of \(1.00 \mathrm{~cm} .\) The motion is continuous and is repeated regularly 120 times per second. The string has linear density \(120 \mathrm{~g} / \mathrm{m}\) and is kept under a tension of \(90.0 \mathrm{~N}\). Find the maximum value of (a) the transverse speed \(u\) and (b) the transverse component of the tension \(\tau\). (c) Show that the two maximum values calculated above occur at the same phase values for the wave. What is the transverse displacement \(y\) of the string at these phases? (d) What is the maximum rate of energy transfer along the string? (e) What is the transverse displacement \(y\) when this maximum transfer occurs? (f) What is the minimum rate of energy transfer along the string? (g) What is the transverse displacement \(y\) when this minimum transfer occurs?

The speed of a transverse wave on a string is \(170 \mathrm{~m} / \mathrm{s}\) when the string tension is \(120 \mathrm{~N}\). To what value must the tension be changed to raise the wave speed to \(180 \mathrm{~m} / \mathrm{s}\) ?

The type of rubber band used inside some baseballs and golf balls obeys Hooke's law over a wide range of elongation of the band. A segment of this material has an unstretched length \(\ell\) and a mass \(m\). When a force \(F\) is applied, the band stretches an additional length \(\Delta \ell\). (a) What is the speed (in terms of \(m, \Delta \ell\), and the spring constant \(k\) ) of transverse waves on this stretched rubber band? (b) Using your answer to (a), show that the time required for a transverse pulse to travel the length of the rubber band is proportional to \(1 / \sqrt{\Delta \ell}\) if \(\Delta \ell \ll \ell\) and is constant if \(\Delta \ell \geqslant \ell\).

The equation of a transverse wave on a string is $$ y=(2.0 \mathrm{~mm}) \sin \left[\left(20 \mathrm{~m}^{-1}\right) x-\left(600 \mathrm{~s}^{-1}\right) t\right] $$ The tension in the string is \(15 \mathrm{~N}\). (a) What is the wave speed? (b) Find the linear density of this string in grams per meter.

The linear density of a string is \(1.6 \times 10^{-4} \mathrm{~kg} / \mathrm{m}\). A transverse wave on the string is described by the equation $$ y=(0.021 \mathrm{~m}) \sin \left[\left(2.0 \mathrm{~m}^{-1}\right) x+\left(30 \mathrm{~s}^{-1}\right) t\right] $$ What are (a) the wave speed and (b) the tension in the string?

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