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DEPARTMENT OF PHYSICS AND ASTRONOMY
APPALACHIAN STATE UNIVERSITY
In-Lab Assignment: Thermal Expansion of
Solids
PHY 1104, Section
203
Date:
2/25/21
Name:
Kristina Hicks
●
Make sure that you read the Introduction to the lab and complete the
Pre-lab Quiz
on
Asulearn before starting the lab activities.
●
Note: You need to make a copy of this document and save to your own google drive
using “
File>Make a Copy
” in order to have editing permission. Do not email asking for
permission to edit this document. Use the question forum if you have questions on the
Quiz or the lab. Someone else may have the answer or the same question!
●
After completing the lab, make sure that you
download your document as a pdf
and
contribute to the Post-lab Discussion forum
!
This lab will be conducted on-line and
each student will submit an individual lab report
. You are
allowed to work on the lab content with another student, but you MUST SUBMIT YOUR OWN
UNIQUE images, data, calculations, graphs, explanations, conclusions, etc. Copying items on Lab
Assignments constitutes an academic integrity code violation and will be brought before the Office
of Student Conduct.
I worked on this lab with:
All images, data, calculations, graphs, explanations,
conclusions in this lab assignment are my own and
are not copied from another student or a previous
semester.
Type your name below to accept the honor
statement.
Kristina Hicks
Purpose
Investigate how the dimensions of solid materials change with temperature by taking
measurements and plotting results.
By the end of this lab students will:
●
Use a spec sheet to determine the precision of a digital thermometer in order to
determine the uncertainty in temperature that may be less than what the digital display
indicates.
●
Read a change in length from a micrometer dial.
●
Plot change in length as temperature changes to determine the coefficient of thermal
expansion of a copper tube.
Necessary Equipment
Vernier Graphical Analysis App
:
There is a help document on
Graphical Analysis
if you need help downloaded and using it.
PHY 1104: Thermal Expansion of Solids, Page | 1
DEPARTMENT OF PHYSICS AND ASTRONOMY
APPALACHIAN STATE UNIVERSITY
Introduction: Thermal Expansion of Solids
The materials that we touch and come into contact with every day are made of atoms and
molecules that are bonded together and separated by very small distances. These bonds
act like springs such that they keep materials together and that they can stretch. In general,
when these materials are cold, the bonds between atoms and molecules have the lowest
energy level, IE they contain the smallest amount of every. When materials are warmed, the
atoms and molecules are given energy and this has the effect of stretching these bonds or
increasing the distance between the particles. We can measure this thermally induced
expansion, called thermal expansion, and define it to be the tendency of matter to change
in size in response to a change in temperature. We know from the study of
thermodynamics that an object's temperature using the Kelvin [K] scale is proportional to
the object's internal kinetic energy. When energy in the form of heat, which is measured in
Joules [J], is transferred to an object, its constituent particles maintain a greater average
separation. Since all the distances between particles increases, the material’s volume will
expand. While not impossible, materials which contract with increasing temperature are
uncommon. Water, over a very narrow range of temperatures, is such a material.
Linear Thermal Expansion
Consider an object that is being thermally excited. We will look at just one dimension of the
material: for example, if we have a long metal rod we will look at its length. The specifics of
exactly how the material changes shape with temperature depends on many material
properties and many physical laws, such as those of quantum mechanics. Luckily, many
materials behave in a very reproducible and linear way over a rather wide range of
temperatures around room temperature. Specifically, many materials will expand linearly
with the change in temperature. Thus, if we double the temperature change, we double the
change in length. This relationship is called
linear thermal expansion
. Since materials differ
greatly in terms of chemical and physical construct, each material has its own coefficient of
linear thermal expansion coefficient
α
. This coefficient indicates the fractional change of its
original length per change in temperature °C. The coefficient is found by dividing the
percent change in length by the change in temperature
, Thus the change in
Δ𝑇 = (𝑇
?
− 𝑇
𝑖
)
length
ΔL
of an object will be equal to the linear thermal expansion coefficient
α
times
original length
L
o
times change in temperature
ΔT:
(1)
∆𝐿 = 𝐿
?
α ∆𝑇
(
)
where
ΔT
is the change in temperature or
T
f
– T
i
. We can rewrite equation 1 as:
(2)
∆𝐿 = 𝐿
?
α(𝑇
?
− 𝑇
𝑖
)
This week, you will set up an experiment to measure how the length of an object changes
with temperature. If this relationship is linear, the linear thermal expansion coefficient
α
can be determined and compared to an accepted value, such as that given by table 13-1 in
your textbook.
PHY 1104: Thermal Expansion of Solids, Page | 2
DEPARTMENT OF PHYSICS AND ASTRONOMY
APPALACHIAN STATE UNIVERSITY
If steam is sent through a metal pipe which is at room temperature, the pipe will expand as
the pipe warms up. The amount of expansion is not large and must be measured using a
precise micrometer. For such an experiment, the pipe and other components will be hot
and we have provided an assembly similar to that shown in Figure 1 to allow for the
measurement of small distances effectively and safely.
Using the assembly shown in Figure 1, we will start with a metal rod at room temperature
(around 20
℃
). After measuring the initial temperature and length, we will fill the rod with
steam. After the rod is the same temperature as the steam (around 100
℃
), we will
measure the final temperature and change in length of the rod. From the measured values
of initial length, change in length, and the initial and final temperature of a metal rod, we
can experimentally determine the coefficient of linear expansion for the rod.
PHY 1104: Thermal Expansion of Solids, Page | 3
DEPARTMENT OF PHYSICS AND ASTRONOMY
APPALACHIAN STATE UNIVERSITY
The Micrometer Metric Dial
Examine the micrometer metric dial in figure 2, a similar
metric dial is attached to the apparatus we will use in this
experiment to measure the change in distance of two different
types of metal rods as they expand and contract due to
temperature changes.
The micrometer metric dial is used to measure very small
changes in distance. The least count, or distance between the
smallest tick marks, of the big needle is 0.01 mm. There are
100 increments in a full circle of the needle. The small needle
counts the number of times the large needle has made a
complete circle; we will not use this needle since the dial will
not make a full rotation in today’s experiment. There is a set
screw on the side of the dial that will allow one to zero the markers to the needle, then
retighten. You can estimate the needle position to the nearest half of a division, which will
give you an estimated error of 0.005 mm.
For example, consider the micrometer dial in the picture.
This micrometer is reading 0.628 mm +/- 0.005 mm = 0.000628 m
+/- 0.0000005 m
If you are uncertain about how to use this device, there are many
articles and
videos
on the web, use the search term “How to read a
metric dial indicator”.
We will not be using the smaller dial at all
(this measures mm), just the large outer dial which measures hundredths of a mm and has
a least count of 0.001 mm.
The Digital Thermometer
To measure temperature, we will use an Extech EasyView digital thermometer (or a similar
device) placed into the end of the metal sample to measure temperature. The digital
thermometer is an example of digital reading where the device is less accurate than the
display implies.
PHY 1104: Thermal Expansion of Solids, Page | 4
DEPARTMENT OF PHYSICS AND ASTRONOMY
APPALACHIAN STATE UNIVERSITY
An excerpt of the user manual is shown in figure 3. Examine the section that describes the
accuracy of the digital thermometer. This accuracy describes the confidence or uncertainty
of the reading in a particular temperature range.
Notice that the accuracy of the
measurement is a percentage of the temperature itself plus an additional amount of error.
The steps you must take to determine the measurement uncertainty are a little bit different
than for other digital devices that are more accurate than the display shows. For the
thermometer the accuracy depends on what temperature you are measuring, and is
reported as a percentage of the measurement with an additional uncertainty.
Steps to take to find uncertainty in a digital thermometer
Determine the uncertainty in your measurement (with units):
1.
Consider the temperature range that you will be using to find the correct uncertainty
formula in the manual.
2.
Take your measurement.
3.
Calculate the uncertainty for that measurement using the correct formula for the range
you are in.
Express your measurement with uncertainty in the correct format:
4.
Round your uncertainty to one DIGIT. Keep in mind that you will be rounding the value
up, except in extreme cases.
5.
Determine the place (tens, ones, tenths, hundreds) where the uncertainty digit is.
Round your measurement to that place, making sure that both the measurement and
uncertainty have the same units. You are rounding your measurement to the least
significant digit, since any digit in a place less than the least significant one is
INSIGNIFICANT.
6.
Report your measurement and uncertainty with the same number of decimal places
and units.
PHY 1104: Thermal Expansion of Solids, Page | 5
DEPARTMENT OF PHYSICS AND ASTRONOMY
APPALACHIAN STATE UNIVERSITY
???? ?𝑖?ℎ ??𝑖?? ± ???????𝑖??? ?𝑖?ℎ ??𝑖??
It is easier to describe in an example of the temperature
of steam:
1.
Steam should fall in the range of -93°C to 1000°C which means the device has an
accuracy of
+/- (0.3% reading + 1°C)
2.
Take the measurement:
96.7°C
3.
Calculate the uncertainty in the measurement:
+/- (0.003*96.7°C + 1°C) = 1.29°C
4.
Round the error up and to 1 digit : 2°C
The error should be rounded to one digit, which is in the ones place. It should also be
rounded up, not down, so the calculated uncertainty of 1.29°C rounds to 2°C.
5.
Round your measurement to the ones place to re
port: 97°C +/- 2°C
PHY 1104: Thermal Expansion of Solids, Page | 6
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pV
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3po
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As you know, the parameters of an ideal gas are described by
the equation
PV = nRT,
where p is the pressure of the gas, V is the volume of the
gas, n is the number of moles, R is the universal gas
constant, and T is the absolute temperature of the gas. It
follows that, for a portion of an ideal gas,
One can see that, if the amount of gas remains constant, it is
impossible to change just one parameter of the gas: At least
one more parameter would also change. For instance, if the
pressure of the gas is changed, we can be sure that either the
volume or the temperature of the gas (or, maybe, both!) would
also change.
To explore these changes, it is often convenient to draw a
graph showing one parameter as a function of the other.
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diagram.
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T
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► View Available Hint(s)
Previous Answers
AL = 11
Submit
VΠ ΑΣΦ
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?
X Incorrect; Try Again; 14 attempts remaining
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The figure is a histogram showing the speeds of the molecules in a very small gas.
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Figure
N
4-
3
2
ili.
4
6 8
2
v (m/s)
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Part B
μA
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μÅ
•
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μÅ
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Learning Goal:
To understand the meaning and the basic applications
of pV diagrams for an ideal gas.
As you know, the parameters of an ideal gas are
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where p is the pressure of the gas, V is the volume of
the gas, n is the number of moles, R is the universal
gas constant, and I is the absolute temperature of the
gas. It follows that, for a portion of an ideal gas,
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One can see that. if the amount of aas remains
Figure
ЗРО
2po
Po
Vo
4
6
2V 3V
V
1 of 1
▼
Calculate the work W done by the gas during process 1-3→6.
Express your answer in terms of po and Vo.
W = 4po Vo
Submit
✓ Correct
Part E
Calculate the work W done by the gas during process 2→6.
Express your answer in terms of po and Vo.
VE ΑΣΦ
W =
Previous Answers
Submit
Provide Feedback
Request Answer
Part F Complete previous part(s)
Part G Complete previous part(s)
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- Please look at my wrong answers so you don’t accidentally get one of those as well. I need the correct value of N. Thanks!arrow_forwardx Course Home MasteringPhysics: HW4 M Your Physics answer is ready. - sa X b Answered: A jet pilot takes his air X session.masteringphysics.com/myct/itemView?offset=next&assignmentProblemiD=135028808 Apps (1) NN P4... YouTube to MP3 Co.. phone cover for mo... AGARWAL-PHY-166 KHW4 Item 12 The space shuttle releases a satellite into a circular orbit 710 km above the Earth. Part A How fast must the shuttle be moving (relative to Earth) when the release occurs? Express your answer using three significant figures and include the appropriate units. Value Units Submit Request Answer Provide Feedback IIarrow_forwardParts A-carrow_forward
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- Problem 2 Calculate the specific heat of Lead (Pb), using both the Einstein model and the Debye model, for temperatures equal to 2, 10, 20, 50, 100, 200, 300, 600, and 800 K. Use ] = 88 K and = 65 K since the specific heat calculated with these values agree with the data well for the whole temperature range. Compare your answer with the values from Touloukian and Buyco*. Explain the low-temperature and high-temperature behavior. *Y.S. Touloukain and E.H. Buyco, Thermophysical Properties of Matter, Vol. 4: Specific Heat-Metallic Elements and Alloys; Vol. 5: Specific Heat-Nonmetallic Solids, IFI/Plenum, New York, 1970.arrow_forwardThe Arhennius viscosity model describes how viscosity u depends on temperature 1: u = uo e E/RT 1 DVD DVD Here u is viscosity (Pa.s), I is the temperature (in "Kelvin), E is the activation energy (J mol¹), R is the universal gas constant (R = 8.3145 J mol¹¹ K¹) and U is a constant (Pa s). Ensure all your numerical answers are provided, accurate to 4 significant figures. Linearise this non-linear equation to allow the least squares fitting, i.e. write it in the form y = a + a₁x. Identify the independent (x) and dependent (y) variables and write the linearised equation in the answer boxes, clearly defining what ao and a₁ are equal to in terms of up, E and R. y: ao: a₁: X: IOHO OHO Manarrow_forwardThe last slide of the video on applications of the Boltzmann distribution describes the behavior of vibrations and rotations of hydrogen (H2) molecules in a gas at thermal equilibrium. Choose the correct statements below. a. The energy separation between rotational energy levels is the same as the separation between vibrational energy levels. b. Hydrogen molecules in a gas will rotate if the temperature is in the range 100 K < T < 1000 K, but not outside that range. c. The thermal energy is smaller than the energy difference between vibrational energy levels for T >> 1000 K. d. Vibrational energy levels are separated by an energy ε ≈ 1000 k. e. Most hydrogen molecules in a gas at 2000 K are vibrating, but most do not vibrate at 500 K.arrow_forward
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