Thermal Expansion Experiment

This document introduces the Thermal Expansion Experiment from the Physics laboratory at the University of Toronto. It is intended to be used before you begin the experiment. The Preparatory Questions at the end of this document should be answered and turned in to your Demonstrator before you begin to work on the experiment.

Requirements

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Introduction

Most materials expand as they are heated and contract if they are cooled. Thus their length is a function of temperature. If the length of an object is L and the temperature changes by a differential amount dT, then the differential change in the length dL is given by:

  dL = Greek letter "alpha" L dT (1)

where Greek letter "alpha" is the coefficient of linear expansion.

The photograph to the right shows railroad tracks distorted because of thermal expansion on a very hot July day.

The photograph is from Halliday, Resnick and Walker, Fundamentals of Physics, 6th ed., Enhanced Problems Version, Figure 19-9 (Wiley, 2003), and is used by permission.

Thermal expansion of train tracks

For small ranges of temperature, we can treat Greek letter "alpha" as a constant for a particular material; in the experiment this is a reasonable approximation. You will determine Greek letter "alpha" for aluminum and copper.


In the figure to the right we show an aluminum rod. The length of the rod is defined in the figure, and is similar but not identical to the definition you will use in the experiment. The rod is at a temperature T0 and has a length of L0.

Length L0 at temperature T0

In the figure, you can see a tab on the right-hand side of the rod, and we measure the length of the rod to the right-hand side of the tab. In the actual experiment there is a line inscribed on the top of the tab, and you will measure the length of the rod from the left-hand side to the line inscribed on the tab. Thus the lengths and changes in length of the rod shown in the figures are only similar to the actual definitions you will use in the experiment.


We heat the rod up to a temperature T > T0, and its length increases to L.

Length L at temperature T

We shall call the change in temperature:

Greek letter DeltaT is defined as T - T0

and the corresponding change in length:

Greek letter DeltaL is defined as L - L0

Then if the product:

Greek letter "alpha" × Greek letter DeltaT

is small, Equation 1 becomes approximately:

  Greek letter DeltaL is approximately equal to Greek letter "alpha" L0 Greek letter DeltaT (2)

You will use Equation 2 in the experiment.

You are supplied with two rods, made of aluminum and copper. Briefly, for each rod you will:

  1. Determine the length L0 of a rod at a reference temperature T0. Room temperature is a good choice for the reference temperature.
  2. Heat up the rod by pumping heated water through it. When the rod reaches a constant uniform temperature T measure its change in length Greek letter DeltaL.
  3. Repeat Step 2 for a number of temperatures.
  4. Use your data and Equation 2 to determine Greek letter "alpha".

Getting from Equation 1 to Equation 2 involves solving the differential Equation 1, expanding the result in a Taylor series, and dropping higher order terms from the expansion. This sort of mathematical manipulation, which is part of theoretical physics, is what you are learning in the lecture component of your course. The laboratory is teaching the "better half" of physics: experimental physics.

The Apparatus

In order to perform the experiment you will need to know how to read a Micrometer. An introduction to micrometers may be accessed by clicking on the blue button to the right. It will appear in a separate window and has a file size of 86k.

Click here for the Micrometer document

We have prepared a video in various formats to introduce you to the apparatus; the running time of the video is about 4:10 minutes. Links to the video appear below. You will wish to adjust the volume of the speakers on your computer so that you can easily hear the soundtrack. For the higher resolution RealMedia version, you may also wish to increase the size of the video using the controls provided by the player.

You may download a pdf version of the soundtrack of the video by clicking on the red button to the right. It will appear in a separate window, and has a file size of 59k. Click here for the soundtrack

The Streaming video will be played by the RealMedia player as it is delivered to your computer by the network. The Download versions of the video will be downloaded to a temporary area on your local hard disc and then shown if your browser is configured to use the appropriate player. You may save these Download versions to a more permanent place that you specify on your computer's discs by right clicking on the link and then saving the Target (Internet Explorer) or Link (Netscape).

RealMedia logo RealMedia Streaming
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A Flash animation of the apparatus with the rod undergoing temperature changes is available. It may be accessed by clicking on the yellow button to the right. It will appear in a separate window and has a file size of 19k. You should assume that the "Thermometer" in the animation is measuring the actual temperature of the rod in Celsius.

Click here for the animation

A Flash animation of what you will see when you look through the traveling microscope at the stationary tab on the rod as you move the microscope is available. The animation includes the line inscribed on the top of the tab, which we discussed above. The animation may be accessed by clicking on the orange button to the right. It will appear in a separate window and has a file size of 31k.

Click here for the microscope animation

The figure to the right shows the part of the apparatus that heats the water and pumps it through the rod.

Note that the level of water must be above the hole that lets water into the pump. You are supplied a pitcher with which you can add water if needed.

The heater and pump

Data Collection and Analysis

You will determine the coefficient of thermal expansion Greek letter "alpha" for the copper and the aluminum tube. For each:

Summary

As promised, we have prepared a summary of the background information presented above. It does not attempt to provide a full discussion, but just reviews the "high points" from above.

You may access the summary by clicking on the green button to the right. The summary is in pdf format, will appear in separate window, and has a file size of 14k. You may wish to print this document.

Click here for the summary

Preparatory Questions

These questions should be answered and turned in to your Demonstrator before beginning the experiment. They replace the questions in the Guide Sheet for the experiment: if you are using this web-document as the introduction to the experiment you should answer these questions and not the ones in the Guide Sheet.

Note:
These questions are intended to guide you in your preparation for the experiment. They do not have any "tricks."
  1. What are the units of Greek letter "alpha"?
  2. Usually when temperatures are written as T they refer to values in Kelvin; temperatures written as the lower case letter t usually refer to the value in Celsius. Above we have used T for temperature, while the thermometers you will use measure in Celsius. Does it make any difference? Why?
  3. Values of Greek letter "alpha" are typically on the order of 10-5 in SI units. Imagine a rod with exactly this value of Greek letter "alpha" that has a length of exactly one meter when its temperature is 20oC.
    1. If its temperature changes from 20oC to 80oC what is its change in length?
    2. What is the percentage change in its length?
  4. A rod made of the same material as in Question 3 has a length of exactly 100 meters when its temperature is 20oC.
    1. What is the percentage change in its length if its temperature changes from 20oC to 80oC?
    2. How does your answer compare to your answer to the second part of Question 3?
    3. Why did your answer to Question 4.2 come out as it did?
  5. You will measure the temperature of the water when it enters the tube and again when it leaves the tube, using two thermometers. Particularly at temperatures much above room temperature, at equilibrium the two values may not be the same: the temperature of the water exiting the tube may be less than the water entering it.
    1. What is an explanation of why this is occurring?
    2. What is a reasonable value for the temperature of the rod in this case?
    3. If the difference in temperatures measured by the thermometers is greater than the reading errors of the thermometers, what is a reasonable value of the error in the measurement of the temperature of the rod?

Authors and Copyright

Earlier versions of the Guide Sheet for this experiment have been worked on by David Harrison (1983), Joe Vise (1988), Claude Plante (1993) and others.

This web version is by David M. Harrison, May 2003.

This is $Revision: 0.2 $, $Date: 2003/05/02 18:42:59 $ (y/m/d UTC).