/*! 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 13 A U.S. penny has a diameter of \... [FREE SOLUTION] | 91Ó°ÊÓ

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A U.S. penny has a diameter of \(1.9000 \mathrm{~cm}\) at \(20.0^{\circ} \mathrm{C}\). The coin is made of a metal alloy (mostly zinc) for which the coefficient of linear expansion is \(2.6 \times 10^{-5} \mathrm{~K}^{-1}\). What would its diameter be on a hot day in Death Valley \(\left(48.0^{\circ} \mathrm{C}\right) ?\) On a cold night in the mountains of Greenland \(\left(-53^{\circ} \mathrm{C}\right) ?\)

Short Answer

Expert verified
The diameter of the penny in the Death Valley would be about 1.9014032 cm, and in the mountains of Greenland, it would be about 1.8964118 cm.

Step by step solution

01

Identify given dimensions

The initial diameter of the penny is given as \( L_{0} = 1.9 \, cm \). The coefficient of thermal expansion \( \alpha = 2.6 \times 10^{-5} 1/K \). The initial temperature is \( 20.0^{\circ}C \).
02

Calculate the new diameter at Death Valley

The change in temperature, \( \Delta T \), is the final temperature minus the initial temperature, \( \Delta T = T_{f} - T_{i} \). The final temperature at Death Valley is \( 48.0^{\circ}C \), hence the change in temperature is \( \Delta T = 48.0 - 20.0 = 28.0^{\circ}C \). Plug these values into the formula for change in dimension: \( \Delta L = L_{0} \alpha \Delta T = 1.9cm * 2.6 \times 10^{-5} 1/K * 28.0 K = 0.0014032 cm \). The new diameter is then \( L_{0} + \Delta L = 1.9000 cm + 0.0014032 cm = 1.9014032 cm \).
03

Calculate the new diameter in the mountains of Greenland

The final temperature in the mountains of Greenland is \( -53.0^{\circ}C \), so the change in temperature is \( \Delta T = -53.0 - 20.0 = -73.0^{\circ}C \). Plug these values into the formula for change in dimension: \( \Delta L = L_{0} \alpha \Delta T = 1.9 cm * 2.6 \times 10^{-5} 1/K * -73.0 K = -0.0035882 cm \). The new diameter is then \( L_{0} + \Delta L = 1.9000 cm - 0.0035882 cm = 1.8964118 cm \)

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Key Concepts

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

Linear Expansion Coefficient
The linear expansion coefficient is a crucial concept in understanding how materials respond to temperature changes. This small value, often represented by the symbol \( \alpha \), indicates how much a material will expand or contract for each degree change in temperature.

In our exercise, the penny's metal alloy has a linear expansion coefficient of \( 2.6 \times 10^{-5} \, \mathrm{K}^{-1} \). This number tells us that for every degree Kelvin (or Celsius, since the scale increment is the same), one meter of this material will expand by \( 2.6 \times 10^{-5} \) meters.
  • A higher linear expansion coefficient means the material expands more with temperature.
  • A lower coefficient indicates lesser expansion or contraction with temperature changes.
Having a solid grasp on this concept helps predict the dimensional changes of materials such as metals or any other substance when subjected to different thermal environments.
Understanding the linear expansion coefficient is essential in engineering and construction, where precise measurements are critical.
Temperature Change
Temperature change, denoted by \( \Delta T \), plays a significant role in the material's dimensional change.

In thermal expansion problems like ours, you would calculate \( \Delta T \) simply by subtracting the initial temperature from the final temperature.
For instance:
  • In Death Valley, the temperature change is \( 48.0^{\circ}\mathrm{C} - 20.0^{\circ}\mathrm{C} = 28.0^{\circ}\mathrm{C} \).
  • In the mountains of Greenland, it’s \( -53.0^{\circ}\mathrm{C} - 20.0^{\circ}\mathrm{C} = -73.0^{\circ}\mathrm{C} \).
Knowing \( \Delta T \) is crucial because it directly influences how much a material will expand or contract.
The larger the temperature change, the more pronounced the effect on the object's dimensions.
Accurately measuring and understanding these temperature differences is vital for predicting how objects behave in various thermal conditions.
Dimension Change Calculation
The dimension change calculation is where the principles of thermal expansion come to life.

To find the change in an object’s dimensions due to temperature variation, you utilize the formula:
\[ \Delta L = L_0 \alpha \Delta T \]
Where:
  • \( \Delta L \) is the change in length (in this case, the change in diameter).
  • \( L_0 \) is the original length or diameter of the object.
  • \( \alpha \) is the linear expansion coefficient.
  • \( \Delta T \) is the temperature change.
For example, in Death Valley, we calculated the new diameter with:
\( \Delta L = 1.9 \mathrm{cm} \times 2.6 \times 10^{-5} \, \mathrm{K}^{-1} \times 28.0^{\circ} \mathrm{C} = 0.0014032 \mathrm{cm} \).
  • Add \( \Delta L \) to the original diameter to get the new diameter.
  • Similarly, apply this formula to calculate the diameter in Greenland.
Such calculations are immensely useful in predicting and understanding how temperature variations affect the practical use of materials across different climates.
Thermal Physics
Thermal physics is a broad field that encompasses how energy, in the form of heat, affects matter.

It includes studying how objects expand when heated and contract when cooled, as well as various other heat-related phenomena.
Thermal expansion is just one aspect of this field and is particularly significant in areas where thermal stress or measurement precision is critical.
  • Understanding thermal physics helps in designing structures that can withstand temperature changes.
  • It is crucial for manufacturing processes, where metal precision is important.
  • It also aids in everyday objects, like ensuring that a bridge doesn't buckle or shrink excessively with seasonal changes.
By learning about concepts like thermal expansion, we can create more durable designs and predict how everyday materials behave under temperature variations.

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Most popular questions from this chapter

A laboratory technician drops a \(0.0850 \mathrm{~kg}\) sample of unknown solid material, at \(100.0^{\circ} \mathrm{C}\), into a calorimeter. The calorimeter can, initially at \(19.0^{\circ} \mathrm{C},\) is made of \(0.150 \mathrm{~kg}\) of copper and contains \(0.200 \mathrm{~kg}\) of water. The final temperature of the calorimeter can and contents is \(26.1^{\circ} \mathrm{C}\). Compute the specific heat of the sample.

Hot Air in a Physics Lecture. (a) A typical student listening attentively to a physics lecture has a heat output of \(100 \mathrm{~W}\). How much heat energy does a class of 140 physics students release into a lecture hall over the course of a 50 min lecture? (b) Assume that all the heat energy in part (a) is transferred to the \(3200 \mathrm{~m}^{3}\) of air in the room. The air has specific heat \(1020 \mathrm{~J} / \mathrm{kg} \cdot \mathrm{K}\) and density \(1.20 \mathrm{~kg} / \mathrm{m}^{3} .\) If none of the heat escapes and the air conditioning system is off, how much will the temperature of the air in the room rise during the 50 min lecture? (c) If the class is taking an exam, the heat output per student rises to \(280 \mathrm{~W}\). What is the temperature rise during \(50 \mathrm{~min}\) in this case?

You put a bottle of soft drink in a refrigerator and leave it until its temperature has dropped \(10.0 \mathrm{~K}\). What is its temperature change in (a) \(\mathrm{F}^{\circ}\) and \((\mathrm{b}) \mathrm{C}^{\circ} ?\)

Consider a poor lost soul walking at \(5 \mathrm{~km} / \mathrm{h}\) on a hot day in the desert, wearing only a bathing suit. This person's skin temperature tends to rise due to four mechanisms: (i) energy is generated by metabolic reactions in the body at a rate of \(280 \mathrm{~W},\) and almost all of this energy is converted to heat that flows to the skin; (ii) heat is delivered to the skin by convection from the outside air at a rate equal to \(k^{\prime} A_{\mathrm{skin}}\left(T_{\mathrm{air}}-T_{\mathrm{skin}}\right),\) where \(k^{\prime}\) is \(54 \mathrm{~J} / \mathrm{h} \cdot \mathrm{C}^{\circ} \cdot \mathrm{m}^{2},\) the exposed skin area \(A_{\text {skin }}\) is \(1.5 \mathrm{~m}^{2},\) the air temperature \(T_{\text {air }}\) is \(47^{\circ} \mathrm{C},\) and the skin temperature \(T_{\text {skin }}\) is \(36^{\circ} \mathrm{C} ;\) (iii) the skin absorbs radiant energy from the sun at a rate of \(1400 \mathrm{~W} / \mathrm{m}^{2} ;\) (iv) the skin absorbs radiant energy from the environment, which has temperature \(47^{\circ} \mathrm{C}\). (a) Calculate the net rate (in watts) at which the person's skin is heated by all four of these mechanisms. Assume that the emissivity of the skin is \(e=1\) and that the skin temperature is initially \(36^{\circ} \mathrm{C}\). Which mechanism is the most important? (b) At what rate (inL/h) must perspiration evaporate from this person's skin to maintain a constant skin temperature? (The heat of vaporization of water at \(36^{\circ} \mathrm{C}\) is \(2.42 \times 10^{6} \mathrm{~J} / \mathrm{kg} .\) ) (c) Suppose the person is protected by light-colored clothing \((e \approx 0)\) and only \(0.45 \mathrm{~m}^{2}\) of skin is exposed. What rate of perspiration is required now? Discuss the usefulness of the traditional clothing worn by desert peoples.

To measure the specific heat in the liquid phase of a newly developed cryoprotectant, you place a sample of the new cryoprotectant in contact with a cold plate until the solution's temperature drops from room temperature to its freezing point. Then you measure the heat transferred to the cold plate. If the system isn't sufficiently isolated from its roomtemperature surroundings, what will be the effect on the measurement of the specific heat? (a) The measured specific heat will be greater than the actual specific heat; (b) the measured specific heat will be less than the actual specific heat; (c) there will be no effect because the thermal conductivity of the cryoprotectant is so low; (d) there will be no effect on the specific heat, but the temperature of the freezing point will change.

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