Thermodynamics - Thermal Expansion

In summary, the conversation discusses the concept of coefficient of linear expansion and its relationship to the lengths of two rods made of different solids. It is shown that if the lengths of the rods are inversely proportional to their respective coefficients of linear expansion, the difference in length between them will be constant at all temperatures. The second part of the conversation presents a problem where the lengths of a steel and a brass rod at 0 degrees Celsius are determined in order to have a constant difference in length of 0.30 meters at all temperatures. After calculations, it is concluded that the lengths of the rods should be 71 cm and 41 cm respectively. The conversation also acknowledges a mistake in the first part of the question, which has
  • #1
Kelvin
52
0
The following questions are extracted from "Physics" Halliday Resnick & Krane Chapter 21 problem

7.
(a) Show that if the lengths of two rods of different solids are inversely proportional to their respective coefficients of linear expansion at the same initial temperature, the difference in length between them will be constant at all temperature.​

(b) What should be the lengths of a steel and a brass rod at 0 degree celcius so that all temperatures their difference in length is 0.30 m ?​

My attempt to this question is:

The definition of the coefficient of linear expansion is
[tex]
\begin{equation}
\begin{split}
\alpha &= \frac{\Delta L_1}{\Delta T} \frac{1}{L_1}\\
\beta &= \frac{\Delta L_2}{\Delta T} \frac{1}{L_2}\\
\\
\frac{\alpha}{\beta} &= \frac{\Delta L_1}{\Delta L_2} \frac{L_2}{L_1}\\
\end{split}
\end{equation}

\begin{equation}
\begin{split}
\frac{\alpha L_1}{\beta L_2} &= \frac{\Delta L_1}{\Delta L_2} \equiv K\\
\end{split}
\end{equation}
[/tex]

Where [tex]K[/tex] is a dimensionless constant since the length is inversly proportional to the coefficient of linear expansion.

Suppose [tex]L_1'[/tex] and [tex]L_2'[/tex] are the length after the temperature change [tex]\Delta T[/tex]. The difference in length is
[tex]\begin{equation}
\begin{split}
\Delta L \equiv L_1' - L_2' &= L_1 + \Delta L_1 - \left( L_2 + \Delta L_2 \right) \\
&= L_1 - L_2 + \left( \Delta L_1 - \Delta L_2 \right)
\end{split}
\end{equation}[/tex]​

What I think is that the given condition is not sufficient, but neccessary. One more condition required such that "the difference in length between them will be constant at all temperature" is
[tex]K \equiv 1[/tex]​
If this condition is imposed,

[tex]\alpha L_1 = \beta L_2[/tex]
[tex]\Delta L_1 = \Delta L_2[/tex]
[tex]\Delta L = L_1 - L_2[/tex]

which depends on the intial length of two rods only.

(b) We want
[tex]\Delta L = 0.30 \hbox{ m} [/tex]​
for all temperature. We have the following equations:

[tex]
\begin{equation}
\begin{split}
\alpha L_1 = \beta L_2 \\
\Delta L = L_1 - L_2 = 0.30 \hbox{ m}\\


\alpha \left( \Delta L + L_2 \right) &= \beta L_2 \\
\\
L_2 &= \frac{\alpha \Delta L}{\beta - \alpha}\\
&= \frac{11 \times 10^{-6} K^{-1} \times 0.30 \hbox{ m}}{\left(19 - 11\right) \times 10^{-6} K^{-1}}\\
&= 41 \hbox{ cm}\\
L_1 &= \Delta L + L_2\\
&= 41 \hbox{ cm} + 30 \hbox{ cm}\\
&= 71 \hbox{ cm}
\end{split}
\end{equation}

[/tex]​

The part (b) result agree with the given answer. I wonder whether the part(a) question is wrong or I am wrong?

Wow, lateX is so difficult to use. It took me more than an hour to type out the equations nicely. Now I am typing the second question.
 
Last edited:
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  • #2
The first part is wrong.Check the division in the passing from the eq.(1) to eq.(2)

Daniel.
 
  • #3
dextercioby said:
The first part is wrong.Check the division in the passing from the eq.(1) to eq.(2)

Daniel.


Thank you
I have corrected that
 

1. What is thermal expansion?

Thermal expansion is the tendency of matter to change in volume in response to a change in temperature. This phenomenon is caused by the increase in kinetic energy of particles as they are heated, which causes them to vibrate and take up more space.

2. How does thermal expansion affect solids, liquids, and gases differently?

Thermal expansion affects solids the most, followed by liquids, and then gases. This is because the particles in solids are more closely packed and have stronger intermolecular bonds, making them less able to move and expand. Liquids have more space between particles, allowing them to expand more easily, while gases have the most space between particles and are able to expand the most.

3. Why is thermal expansion important?

Thermal expansion has many practical applications, such as in the design and construction of buildings, bridges, and other structures. It is also important in the functioning of everyday objects, such as thermometers and thermostats. Understanding thermal expansion is crucial in many industries, such as automotive and aerospace, where materials must be able to withstand changes in temperature without breaking or malfunctioning.

4. What is the coefficient of thermal expansion?

The coefficient of thermal expansion is a measure of how much a material expands or contracts with a change in temperature. It is expressed as a fraction of the change in length or volume per degree of temperature change. Different materials have different coefficients of thermal expansion, which must be taken into account in engineering and construction projects.

5. Can thermal expansion be prevented or controlled?

Thermal expansion cannot be completely prevented, but it can be controlled to some extent. Materials with lower coefficients of thermal expansion can be used, or structures can be designed with built-in flexibility to allow for expansion without causing damage. In some cases, cooling systems can also be used to maintain a constant temperature and minimize the effects of thermal expansion.

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