/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 70 A steel wire has density \(7800 ... [FREE SOLUTION] | 91Ó°ÊÓ

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A steel wire has density \(7800 \mathrm{~kg} / \mathrm{m}^{3}\) and mass \(2.50 \mathrm{~g}\). It is stretched between two rigid supports separated by \(0.400 \mathrm{~m}\). (a) When the temperature of the wire is \(20.0^{\circ} \mathrm{C}\), the frequency of the fundamental standing wave for the wire is \(440 \mathrm{~Hz}\). What is the tension in the wire? (b) What is the temperature of the wire if its fundamental standing wave has frequency \(460 \mathrm{~Hz}\) ? For steel the coefficient of linear expansion is \(1.2 \times 10^{-5} \mathrm{~K}^{-1}\) and Young's modulus is \(20 \times 10^{10} \mathrm{~Pa}\)

Short Answer

Expert verified
The tension in the wire is 780 N. Assuming the wire is in thermal equilibrium with the surrounding and the initial temperature is 20°C, the final temperature is calculated in Celsius.

Step by step solution

01

Calculate the linear mass density \(\mu\)

From the given mass and length, the linear mass density \(\mu\) of the string can be calculated as \(\mu = \frac{mass}{length}= \frac{2.5 g}{0.4 m} = 6.25 \times 10^{-3} \mathrm{~kg/m}\)
02

Calculate the tension in the wire

We can rearrange the wave speed equation to solve for Tension as \(T = \mu v^{2}\). The speed of wave \(v\) is given as \(v = f \lambda\). The frequency \(f\) is given as 440 Hz. For a string fixed at both ends, the wavelength of the fundamental frequency is twice the length of the string, i.e. \(\lambda = 2L = 2 \times 0.400 m = 0.800 m\). So, \(v = 440 Hz \times 0.800 m = 352 m/s\). Substituting the values, we get \(T = 6.25 \times 10^{-3} \mathrm{~kg/m} \times (352 m/s)^{2} = 780 N\) for the tension.
03

Calculate the change in the length of the wire

Using Young’s modulus \(Y = \frac{\sigma}{\epsilon}\), we can calculate the strain \(\epsilon = \frac{\sigma}{Y}\). The stress \(\sigma\) is the force per unit area. Assuming the cross section area A is uniform along the wire's length, the force on it is just the tension T. So, \(\sigma = \frac{F}{A} = \frac{T}{A}\). Substituting the values, \(\epsilon = \frac{780 N}{\pi r^{2}} / 20 \times 10^{10} Pa\). This gives the fractional change in length.
04

Calculate the temperature change

The change in length from original length is equal to the fractional length change \( \Delta L/ L = \alpha \Delta T\). The coefficient of linear expansion is given as \( \alpha = 1.2 \times 10^{-5} K^{-1}\). Solving for the change in temperature \( \Delta T = \Delta L / L \alpha\). The new length of the wire \(L_{new} = L + \Delta L = L (1 + \epsilon) = 0.400 m (1 + \epsilon)\). From step 3, we can find the value of \(\epsilon\). The tension does not change when the temperature changes, so the string's fundamental frequency with new length is given by \(f_{new} = \frac{v}{\lambda_{new}} = \frac{v}{2L_{new}}\). We can solve for \(L_{new}\) and thereafter \(\Delta L/L\). Hence, we can solve for \( \Delta T = \Delta L / L \alpha \). The final temperature is \(T_{final} = T_{initial} + \Delta T = 20.0 °C + \Delta T\). The absolute temperature is calculated in Celsius so the final answer should be transformed back into Celsius.

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Key Concepts

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

Density of Material
Density is a key concept in physics that describes how much mass is contained in a given volume of a substance. It is a measure of how tightly the material's particles are packed together.
In mathematical terms, density (\(\rho\)) is defined as \(\rho = \frac{m}{V}\), where \(m\) is mass and \(V\) is volume.
For the problem mentioned, the density of the steel wire is given as \(7800 \, \text{kg/m}^3\). This value tells us that each cubic meter of the steel wire contains \(7800\) kilograms of mass.
Understanding density helps in calculating other properties like linear mass density, which is essential in determining characteristics such as tension and wave speed in a wire.
Coefficient of Linear Expansion
Materials expand or contract with temperature changes, and the coefficient of linear expansion helps quantify this behavior. It indicates how much a material will expand per degree of temperature increase.
For steel, the coefficient of linear expansion (\(\alpha\)) is given as \(1.2 \times 10^{-5} \, \text{K}^{-1}\). This coefficient represents the fractional change in length per temperature unit change.
In practical terms, if a steel wire is heated or cooled, the total change in its length (\(\Delta L\)) can be calculated using the formula \(\Delta L = \alpha \times L \times \Delta T\), where \(\Delta T\) is the change in temperature and \(L\) is the original length.
This property is vital in scenarios where precision in length is essential, such as wire tension applications, as it directly affects properties like wave frequency.
Young's Modulus
Young's Modulus (\(E\)) is a measure of a material's ability to withstand changes in length when subjected to tension or compression forces. It is a fundamental concept that describes the stiffness of a material.
The formula for Young's Modulus is given as:\[E = \frac{\sigma}{\epsilon}\]where \(\sigma\) is the stress (force per unit area) and \(\epsilon\) is the strain (the fractional change in length).
In the context of a steel wire, Young's Modulus can be utilized to determine how the wire will deform under a given load (tension). For steel, it's typically large, indicating that steel is relatively stiff and doesn't stretch much under tension.
Calculating Young's Modulus allows us to predict how materials will behave when subject to various forces, which is crucial when dealing with materials under tension.
Fundamental Frequency of Standing Waves
Standing waves occur when a wave reflects back upon itself, creating areas of constructive and destructive interference. For a wire fixed at both ends, its fundamental frequency is the lowest frequency at which it vibrates.
The fundamental frequency (\(f\)) is given by the formula:\[f = \frac{v}{2L}\]where \(v\) is the wave speed and \(L\) is the length of the wire.
For the steel wire problem, the fundamental frequency was given as \(440 \, \text{Hz}\) at \(20^{\circ} \text{C}\).
Variables such as tension, length, and linear mass density help determine this frequency. A change in any of these aspects alters the frequency, as demonstrated by the temperature-induced frequency shift to \(460 \, \text{Hz}\) in the problem.
Understanding the fundamentals of standing waves is crucial for applications like musical instruments and other technologies that rely on specific wave frequencies.

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Most popular questions from this chapter

A metal sphere with radius \(3.20 \mathrm{~cm}\) is suspended in a large metal box with interior walls that are maintained at \(30.0^{\circ} \mathrm{C}\). A small electric heater is embedded in the sphere. Heat energy must be supplied to the sphere at the rate of \(0.660 \mathrm{~J} / \mathrm{s}\) to maintain the sphere at a constant temperature of \(41.0^{\circ} \mathrm{C}\). (a) What is the emissivity of the metal sphere? (b) What power input to the sphere is required to maintain it at \(82.0^{\circ} \mathrm{C}\) ? What is the ratio of the power required for \(82.0^{\circ} \mathrm{C}\) to the power required for \(41.0^{\circ} \mathrm{C}\) ? How does this ratio compare with \(2^{4}\) ? Explain.

At very low temperatures the molar heat capacity of rock salt varies with temperature according to Debye's \(T^{3}\) law: $$ C=k \frac{T^{3}}{\theta^{3}} $$ where \(k=1940 \mathrm{~J} / \mathrm{mol} \cdot \mathrm{K}\) and \(\theta=281 \mathrm{~K}\). (a) How much heat is required to raise the temperature of \(1.50 \mathrm{~mol}\) of rock salt from \(10.0 \mathrm{~K}\) to \(40.0 \mathrm{~K} ?\) (Hint: Use Eq. (17.18) in the form \(d Q=n C d T\) and integrate.) (b) What is the average molar heat capacity in this range? (c) What is the true molar heat capacity at \(40.0 \mathrm{~K} ?\)

In an effort to stay awake for an all-night study session, a student makes a cup of coffee by first placing a \(200 \mathrm{~W}\) electric immersion heater in \(0.320 \mathrm{~kg}\) of water. (a) How much heat must be added to the water to raise its temperature from \(20.0^{\circ} \mathrm{C}\) to \(80.0^{\circ} \mathrm{C} ?\) (b) How much time is required? Assume that all of the heater's power goes into heating the water.

A plastic cup of negligible mass contains \(0.280 \mathrm{~kg}\) of an unknown liquid at a temperature of \(30.0^{\circ} \mathrm{C}\). A \(0.0270 \mathrm{~kg}\) mass of ice at a temperature of \(0.0^{\circ} \mathrm{C}\) is added to the liquid, and when thermal equilibrium is reached the temperature of the combined substances is \(14.0^{\circ} \mathrm{C}\). Assuming no heat is exchanged with the surroundings, what is the specific heat capacity of the unknown liquid?

A carpenter builds a solid wood door with dimensions \(2.00 \mathrm{~m} \times 0.95 \mathrm{~m} \times 5.0 \mathrm{~cm} .\) Its thermal conductivity is \(k=0.120 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). The air films on the inner and outer surfaces of the door have the same combined thermal resistance as an additional \(1.8 \mathrm{~cm}\) thickness of solid wood. The inside air temperature is \(20.0^{\circ} \mathrm{C},\) and the outside air temperature is \(-8.0^{\circ} \mathrm{C}\). (a) What is the rate of heat flow through the door? (b) By what factor is the heat flow increased if a window \(0.500 \mathrm{~m}\) on a side is inserted in the door? The glass is \(0.450 \mathrm{~cm}\) thick, and the glass has a thermal conductivity of \(0.80 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\). The air films on the two sides of the glass have a total thermal resistance that is the same as an additional \(12.0 \mathrm{~cm}\) of glass.

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