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AP Physics Rapid Learning Series - 13
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Rapid Learning Center
Chemistry :: Biology :: Physics :: Math
Rapid Learning Center Presents …p g
Teach Yourself
AP Physics in 24 Hours
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*AP is a registered trademark of the College Board, which does not endorse, nor is
affiliated in any way with the Rapid Learning courses.
H t d Th d iHeat and Thermodynamics
Physics Rapid Learning Series
Rapid Learning Center
www.RapidLearningCenter.com/
© Rapid Learning Inc. All rights reserved.
Wayne Huang, Ph.D.
Keith Duda, M.Ed.
Peddi Prasad, Ph.D.
Gary Zhou, Ph.D.
Michelle Wedemeyer, Ph.D.
Sarah Hedges, Ph.D.
AP Physics Rapid Learning Series - 13
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Learning Objectives
Temperature: Understand the
definition of temperature.
By completing this tutorial, you will learn:
Energy in Thermal Processes.
Understand the relationship
between heat and internal
energy.
Thermal Processes in your
world. Global warming and
greenhouse gasses.
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Laws of Thermodynamics.
Apply the laws of
thermodynamics to real life
problems such as engines and
human metabolism.
Concept Map
Physics
Studies
Previous content
New content
Thermodynamics
The field of
Matter and EnergyMatter and Energy
Heat Energy
One type of energy is
2nd Law1st Law
Expansion
Thermal
Expansion
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Heated objectsHeated objects
expand
Energy is
destroyed
Energy is
neither created nor
destroyed
Entropy
increases
Entropy
always
increases
States thatStates that States that
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ThermodynamicsThermodynamics
and Thermal
Expansion
Thermometers and Temperature Scales.
Thermal expansion of Solids and Liquids
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Thermal expansion of Solids and Liquids
Thermodynamics and Temperature
How does temperature affect materials and how is
this used to measure temperature?
Linear expansion
Volume expansion
The physics of thermostats
The physics of
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thermometers
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Definition - Thermodynamics
Thermodynamics - The branch of
physics that deals with conversionsphysics that deals with conversions
between heat energy and other forms
of energy.
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Thermal Expansion
As solids and liquids are heated, they expand because
their molecules gain kinetic energy and move around
more.
Expansions of solids can be
predicted using the linear
expansion equation.
Expansions of liquids can be
predicted using the volume
expansion equation.
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p q
The ticking noises heard after a
hot car is shut down are due the
shape changes of engine parts as
they cool.
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Linear Expansion Equation
The linear expansion equation is of the form:
Where:
L = length of object
T = temperature
∆TαL∆L ××=
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p
α = coefficient of linear expansion [units = per degree]
∆ = Greek letter “delta”, change in.
Volume Expansion Equation
Similarly, the volume expansion equation is of the form:
∆TβV∆V ××=
Where:
V = volume of object
T = temperature
∆TβV∆V ××=
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ß = coefficient of volume expansion [units = per degree]
∆ = Greek letter “delta”, change in.
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Expansion Coefficients
Note the units of the expansion coefficients:
1∆L
α ×=
1∆V
β ×=
The linear and volume expansion coefficients are
Thus, length and volume cancel. Both expansion
coefficients have units of “per degree”
∆TL
α ×
∆TV
β ×
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The linear and volume expansion coefficients are
related to each other by the following relationship:
Typical values for expansion coefficients may be
found in your physics textbook.
α3β ×=
Sample Problem: Thermal Expansion
Question: How much will the volume of a 2 cm3 aluminum
cube change if the temperature changes from 12°C to 32°C?
The linear expansion coefficient, α, of aluminum is 23x10-6/°C.
S l tiSolution:
Step 1: Use the volume expansion equation.
∆V = Vß * ∆T
Step 2: Calculate ∆T.
∆T = Tfinal –Tinitial = 32°C – 12°C = 20°C
St 3 C l l t ß
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Step 3: Calculate ß.
ß = 3α = 3 * 23 x10-6/°C = 69 x 10-6/°C
Step 4: Plug in the values.
∆V = Vß * ∆T = (2cm3) * (69x10-6/°C) * (20°C)
Answer: ∆V = 2.76x10-3 cm3
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Note - Units and Temperature Change
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Thermostats - 1
Thermostats are designed to measure temperature
by applying the principle of linear expansion.
A thermostat uses two fused
strips of metal, each with a
different linear expansion
coefficient.
As the strip heats up one strip
lengthens faster so the strips
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bend away from the longer
strip.
Typically the bent strips will
make contact with a circuit.
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Thermostats - 2
Imagine a thermostat made up of two metal strips
as shown below. The yellow strip has a larger
linear expansion coefficient.
Heat
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Heat
The strip bends towards the side with the lower
linear expansion coefficient.
Thermometers
Thermometers are designed to measure
temperature by applying the principle of thermal
expansion.
Most home thermometers use
mercury or alcohol inside a
narrow glass tube.
As the temperature rises, both
the glass and liquid expand.
The liquid has a higher volume
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The liquid has a higher volume
expansion coefficient than the
glass tube so it rises within the
tube to tell you the temperature.
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Thermal Expansion: Stop-And-Think
Question: Why would engineers need to take
thermal expansion into account in the design
of bridges?
On hot days, the metal supports of a bridge will
expand and buckle if the bridge is not designed
to expand. Similarly, the bridge will crack as
the supports shrink on a cold day.
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Energy in Thermal
Processes
Heat and Internal Energy
Specific Heat
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Specific Heat
Calorimetry
Latent Heat and Phase Change
Energy Transfer
Global Warming and Greenhouse Gasses
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System vs. Surroundings
Calculations of heat and internal energy are based
on the definition of a system and its surroundings.
System - The system
refers to the object
being studied.
Surroundings -
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g
Everything not
included in the system.
Example - System v. Surroundings
Example: a beaker
The system refers to
the contents of the
beaker.
Th di f
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The surroundings refer
to everything else.
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Heat and Internal Energy Equation
Internal energy of a system is defined as:
1) The ability to do work on an object.
2) The ability to transfer heat to an object.
U = q + w
Heat
Heat energy of the
system
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q
Internal Energy
Work
System internal
energy
Work done on the
system or energy
available for the
system to do work.
Definition - Energy Units
Calorie (cal) - Heat is measured in
calories. A calorie is the amount of
heat required to heat 1 gram of water
1°C.
Joule (J) - Energy is measured in
Joules. One calorie (cal) is equal to
4 18J
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4.18J.
4.18 J = 1 cal
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Definition - State Function
State Function - n. A state function is
a quantity of the object that isa quantity of the object that is
dependent on the current state. A
state function is independent of the
path taken to reach the current state.
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Temperature, kinetic energy, and
potential energy are all state functions.
Temperature is a State Function
Temperature is an example of a state function.
Your coffee can be 40°C whether you heated it in
the microwave or on the stove.
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40°C
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Note: the Food Calorie
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Definition - Specific Heat
Specific Heat (CP) - n. Specific heatp ( P) p
is a material property that defines the
quantity of heat, q, required to raise
1g of a specific material 1°C.
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units of cp = [cal/gram*K]
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Specific Heat Equation
T T
The specific heat may be used as follows:
Q = CPm * ∆T
Specific Heat
Change in
Temperature
Tfinal - Tinitial
(K) or (°C)
Proportionality
Constant
J/g*K or cal/g*K
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P
Heat
Total Heat Energy
(J)
Mass
Mass of Object
(g)
Interpretation of Specific Heat
What are the practical implications of specific heat?
High Specific Heat Low Specific Heat
Large amount of energy to
change temperature
Small amount of energy can
change temperature
Heats up slowly
Cools down slowly
Small temperature changes with
condition changes
e g Water Cast iron
Heats up quickly
Cools down quickly
Quickly readjusts to new
conditions
e g Air aluminum foil
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e.g. Water, Cast-iron e.g. Air, aluminum foil
A pool takes a long time to warm up and remains fairly warm over night.
The air warms quickly on a sunny day, but cools quickly at night
A cast-iron pan stays hot for a long time after removing from oven.
Aluminum foil can be grabbed by your hand from a hot oven
because it cools so quickly
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Specific Heat and Heat Capacity
Thus, if the specific heat and the mass of any
object are known, then the amount of heat need to
raise the temperature by any given amount may be
calculated.
The heat capacity C of an object may be
determined from its specific heat CP and its mass
m as follows:
CmC ×
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C = heat capacity
CP = specific heat
m = mass of object
pCmC ×=
Definition - Heat Capacity
Heat Capacity (C) - The amount of heat Q
required to raise the temperature of an
object by ∆T is given by:
Q = C * ∆T
Heat Capacity
Proportionality
Constant
J/K or cal/K
object by ∆T is given by:
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Q = C * ∆T
Heat Change in Temperature
Tfinal - Tinitial
(K) or (°C)
Total Heat Energy
(J)
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Definition - Enthalpy (H)
Enthalpy of Reaction (H) - The enthalpy of a
reaction is the heat energy (J) gained or lost
during a reaction. Enthalpy is a state function.during a reaction. Enthalpy is a state function.
Reaction
Bonds of reactants
broken. Bonds of
products formed.
Bonds of reactants have
hi h th
Bonds of products have
higher energy than
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higher energy than
bonds of products.
higher energy than
bonds of reactants.
Exothermic Endothermic
Heat given
off by system
Heat
absorbed by
system
Endothermic vs. Exothermic
Exothermic - If the system looses net
heat during a reaction, the reaction isg ,
exothermic.
Endothermic - If the system gains net
∆Hsystem = Hfinal – Hinitial < 0
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y g
heat energy during a reaction, the
reaction is endothermic.
∆Hsystem = Hfinal – Hinitial > 0
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Definition - Calorimetry
Calorimetry. n.
Calorimetry is aCalorimetry is a
laboratory technique
used to determine the
amount of heat Q
taken up or given off
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by a reaction.
Procedure - Calorimetry
A small beaker is immersed in an insulated1
How to determine the heat of a reaction using
calorimetry.
beaker filled with a known amount of water.
The initial temperature of the water is noted.
A known amount of the reactants are
placed in the small reaction beaker.
The temperature of the water is recorded at
1
2
3
4
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regular intervals as the reaction proceeds.
The change is temperature is plotted versus time.
4
5
6
The heat given off by the reaction is calculated
from the total change in temperature of the water.
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Example - Calorimetry
(1) Large,
insulated beaker
(2) Water initial(2) Water, initial
temperature Tinitial
(3) Reaction beaker
(4) Initiate reaction
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(5) Flow of heat energy
to water
(6) Measure final water
temperature, Tfinal
(7) Calculate ∆H from
∆Twater and the specific
heat of water, CP.
Endothermic vs. Exothermic Reactions
Endothermic Exothermic
Heat moves from Heat moves from system
surroundings to system
Internal energy of
system increases
KEAVE of system
molecules increases
Internal energy of system
decreases
KEAVE of the system
decreases
to surroundings.
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Temperature of the
system increases
Bonds of reaction
products have greater
energy than bonds of
reactants
Temperature of the
system decreases.
Chemical bonds of
reactants have greater
energy than bonds of
products.
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Stop and Think- Calorimetry
Question: If the temperature of the water in a
l i t i t i i th ticalorimetry experiment rises, is the reaction
endothermic or exothermic?
Answer: The reaction is exothermic because heat
energy is moving from the system (the reaction) to
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energy is moving from the system (the reaction) to
the surroundings (the water).
Latent Heat and Phase Change
A rise in temperature
Internal energy increases
When a solid is heated it undergoes the following:
Internal energy increases
Molecules oscillate more rapidly
A phase change from solid to liquid
Molecules oscillate so rapidly they loose their crystalline form
There is no increase in temperature during the transition
Another rise in temperature
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Another rise in temperature
A phase change from liquid to gas
Molecules oscillate so rapidly they escape the intermolecular
forces that bind them together and enter the gas phase
There is no increase in temperature during the transition.
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Heats of Fusion and Vaporization
The amount of heat Qfus needed to melt m grams of a
substance is given by the following equation:
fusfus Lm∆Q ×=
Qfus = heat energy = [calories]
m = mass = [grams]
Lfus = Heat of Fusion = [calories/gram]
The amount of heat Qvap needed to vaporize m grams
of a substance is given by the following equation:
fusfus Lm∆Q ×
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Qvap = heat = [calories]
m = mass = [grams]
Lvap = Heat of Vaporization = [calories/gram]
of a substance is given by the following equation:
vapvap Lm∆Q ×=
Latent Heat and Phase Change
Gas
Temperatureof
Substance
Phase
Liquid
Phase
Solid
Tboil
Tmelt
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Increase in Heat Energy, ∆Q
Solid
Phase
Qmelt
Qboil
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Example - Heats of Transformation
Question: How much heat energy is required for 10 grams of ice
at 0°C to transition to liquid? To evaporate? The heat of fusion
for water is 333 KJ/kg. The heat of vaporization is 2256 KJ/kg.
Solution:Solution:
1) Calculate the heat energy required to melt 10 grams (0.01Kg) of ice.
Qfus = Lfus * m = 333 KJ/kg * 0.01 Kg = 3.33 KJ
2) Calculate the heat energy needed to raised the temperature of the
water from 0°C to 100°C.
Q = 0.00418 KJ/g*°C * 10.0 g * (100-0)°C = 4.18 kJ
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3) Calculate the heat energy required to vaporize 10g of water.
Qvap = Lvap * m = 2256 KJ/kg * 0.01Kg = 22.56 KJ
4) The total heat required is the sum of 1-3.
Qtot = 3.33 KJ + 4.18 KJ + 22.56 KJ = 30.07 KJ
Answer: Qtot = 30.07 KJ
Stop-and-think- Sweating
Question: Why is sweating an effective cooling
mechanism?
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Answer: As sweat evaporates from your skin it
transitions from the liquid to the gas phase. This
phase transition requires a transfer of heat energy
from the skin to the liquid, cooling the skin.
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Global Warming & Greenhouse Gases
1) Heat energy radiates from the
sun to the earth
2) Some of the heat energy is
reflected off greenhouse gasesreflected off greenhouse gases
in the earth’s atmosphere.
3) Some of the heat energy is
reflected of the earth’s surface.
4) Some of the energy reflected off
the surface is trapped by
greenhouse gases in the
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atmosphere.
5) As the concentration of
greenhouse gases is increased
due to emissions from cars and
factories, the temperature of the
earth rises.
The Laws of
Thermodynamics
The Zeroth Law of Thermodynamics
Work in Thermodynamic Processes
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Work in Thermodynamic Processes
The First Law of Thermodynamics
Heat, Engines, and the Second Law of
Thermodynamics
Entropy
Human Metabolism
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Heat Energy and the Laws of Thermodynamics
The Zeroth Law of Thermodynamics
states that objects in thermal
ilib i t th
The laws of thermodynamics govern energy
exchanges:
equilibrium are at the same
temperature.
The internal energy of a system is the
sum of the heat energy of the system
and the work done on or by the system.
The 1st Law of Thermodynamics states
that energy can change state but cannot
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gy g
be created or destroyed.
The 2nd Law of Thermodynamics states
that the total entropy, or disorder, of the
universe can increase or stay the same
but never decrease. The universe tends
towards disorder.
Definition: Thermal Equilibrium
Thermal Equilibrium - Two objects are
thermal equilibrium are at the sameq
temperature. That is, when put in contact
they remain at the same temperature and
no longer exchange net heat energy.
A and B areIf A is placed inThe temperature
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A and B are
said to be in
thermal
equilibrium.
p
contact with B,
they both
remain at 10C°.
The temperature
of A is 10C° and
the temperature
of B is 10C°
Note that if objects are in thermal equilibrium, their
molecules also have the same average kinetic energy
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Zeroth Law of Thermodynamics
Zeroth Law - If object A is in thermal
equilibrium with object B and object C,
then objects B and C are also in thermalthen objects B and C are also in thermal
equilibrium.
A
10 degrees
Celsius
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B C
10 degrees
Celsius
10 degrees
Celsius
Note that if B and C are in thermal equilibrium with A,
then they must also be at 10 degrees Celsius.
Work in Thermodynamics
As mentioned before:
U = q +U = q + w
U = system internal energy
q = heat energy
w = work done on or by the system
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Pressure-Volume Work
For constant pressure:
∆W = -P * ∆V
∆W = work done on or by the system
P = pressure
∆V = volume change of the system
One common type of application of this equation
is in calculating pressure-volume work done by
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engines.
Applied Pressure-Volume Work
If the system expands, work is done by
the system on the surroundings. The
internal energy of the systeminternal energy of the system
decreases.
If the system contracts, work is done
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by the surroundings on the system.
The internal energy of the system
increases.
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The First Law of Thermodynamics
Energy in a reaction may be changed
from one form to another but it is neither
t d d t d ti fcreated nor destroyed – conservation of
energy.
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Application of The 1st Law
This implies that:
Q Q
∆U = ∆q + ∆w
Change in Heat Energy
W k d t b
Qinitial -Qfinal
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Change in System
Internal Energy
Work done to or by
the system
Ufinal - Uinitial Win -Wout
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Work and the 1st Law
There are 4 special applications of the
1st Law:
1) Adiabatic: Q = 0, ∆U = -W
2) Constant-volume: W = 0, ∆U = Q
3) Cyclical: ∆U = 0, Q = -W
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4) Free expansion processes: ∆U = Q = W
Adiabatic Work
An example of adiabatic work is a closed system with a
piston. If pressure is applied rapidly to depress the
piston, the volume of the system will decrease. Work W
is done on the system by the surroundings, but there is
∆V ≥ 0
Q = 0, ∆U = -W = -P*∆V
is done on the system by the surroundings, but there is
no change in heat Q so the change in internal energy ∆U
is equal to –W.
W
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W
Vinitial
Vfinal
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Constant-Volume Work
An example of constant-volume work is heating a
sealed cylinder. There is no volume change so the
change in internal energy is equal to the change in heat
energyenergy.
Tinitial Tfinal
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∆V = 0 so W = 0
∆T ≥ 0 so Q ≥ 0
∆U = Q
Cyclical Work and Engines
In an engine, heat is used to increase pressure leading to an
increase in volume. The change in volume does work on the
surroundings. The work energy is transferred back from the
surroundings to compress the cylinder back to its original size
and the cycle repeatsand the cycle repeats.
∆U = 0
Q W
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Q = -W
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Free Expansion Work
Connecting a pressurized system to a vacuum is an
example of free-expansion work. The gas from the
pressurized system will immediately and irreversibly
expand to fill the vacuum The process occurs rapidlyexpand to fill the vacuum. The process occurs rapidly,
but unlike adiabatic work the process is irreversible.
∆U = Q = W = 0
Heating an open beaker may be considered free-
i k Th t th t t f th
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expansion work. The system, the contents of the
beaker, are open to the surroundings so there can be no
volume changes or heat exchanges.
Energy Calculations: Example
Question: If the volume of a sealed balloon
increases from 10mL to 100mL when heated and
then shrinks back to 10mL as it cools, what
f tapplication of the 1st Law is this?
Constant-volume
Adiabatic
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Cyclical
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Energy Calculations: Answer
Question: If the volume of a sealed balloon
increases from 10mL to 100mL when heated and
then shrinks back to 10mL as it cools, what
f tapplication of the 1st Law is this?
Constant-volume
Adiabatic
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Cyclical
Definition - Entropy
Entropy (S) - n. Entropy is a measure of
the disorder of a system or its
surroundings.surroundings.
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A landfill possesses lots of entropy!
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The 2nd Law of Thermodynamics
The 2nd Law of Thermodynamics states that the
total entropy of the universe can never decrease,
it can only increase or stay the same.
∆Stotal ≥ 0
Note that the entropy of the system may
decrease, so long as the entropy of the
s rro ndings increases b an eq al or greater
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surroundings increases by an equal or greater
amount.
Thus,
∆Ssys + ∆Ssur ≥ 0
Relative Entropies
Low entropy states are more organized than high
entropy states.
Lower Entropy Higher Entropy
Your clean bedroom Your room after finals
Solids Liquids
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Liquids
Salt tablets in water
Gases
Dissolved salt in water
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Definition - Engine Efficiency
In a real combustion engine such as your car, some of the
work energy is lost to the surroundings as heat rather than
transferred to pressure-volume work which moves a piston.
The efficiency of an engine is the ratio of the heat energy put
in (for example by combustion) to the work output by the
engine (such as movement of the wheels of a car).
ε = Wout / Qin
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If the efficiency of an engine is 0.7, the 30% of the heat
from combustion is lost as heat to the surroundings. In
the real world, this would be a very efficient engine!!!
Entropy and Human Metabolism
Question: Metabolic processes in the body, such as
the building of proteins and DNA, lead to increased
order. How does this not violate the 2nd Law?
Answer: Although the building of
structural proteins in the body lead
to increased order in the system,
which is the body, they lead to
increased disorder in the
surroundings through loss of heat.
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surroundings through loss of heat.
Metabolic processes are usually
linked to a catabolic process such
as the combustion of glucose or
the flow of ions down a
concentration gradient.
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Entropy: Stop-and-Think Question
Question: When an ice cube melts, does system
entropy increase, decrease, or remain the same?
Pick the best answerPick the best answer.
A. Remain the same because
there is no reaction, only a
state change.
B. Increase because the
molecules are changing
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g g
from an ordered crystalline
state to a disordered liquid
state.
C. Decrease because heat
is absorbed to melt the ice.
Entropy: Stop-and-Think Answer
Question: When an ice cube melts, does system
entropy increase, decrease, or remain the same?
Pick the best answerPick the best answer.
A. Remains the same because
there is no reaction, only a
state change.
B. Increases because the
molecules are changing
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g g
from an ordered crystalline
state to a disordered liquid
state.
C. Decreases because heat
is absorbed to melt the ice.
AP Physics Rapid Learning Series - 13
© Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 34
Entropy is aEntropy is a
Expansion
coefficients
measure how
Expansion
coefficients
measure how
The 2nd Law
states that net
entrop can
The 2nd Law
states that net
entrop can
Learning Summary
Heat energy mayHeat energy may
measure of
disorder.
measure of
disorder.
measure how
much objects
expand when
heated.
measure how
much objects
expand when
heated.
entropy can
never
decrease.
entropy can
never
decrease.
The 1st LawThe 1st Law
67/67
Heat energy may
be gained or lost
to the
surroundings
during work.
Heat energy may
be gained or lost
to the
surroundings
during work.
The 1 Law
states that
energy is never
created or
destroyed.
The 1 Law
states that
energy is never
created or
destroyed.
Congratulations
Y h f ll l t dYou have successfully completed
the tutorial
Heat and
Thermodynamics
68/67
Rapid Learning Center
AP Physics Rapid Learning Series - 13
© Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 35
Rapid Learning Center
Wh t’ N t
Chemistry :: Biology :: Physics :: Math
What’s Next …
Step 1: Concepts – Core Tutorial (Just Completed)
Step 2: Practice – Interactive Problem Drill
Step 3: Recap – Super Review Cheat Sheet
69/67
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Heat and Thermodynamics

  • 1. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 1 Rapid Learning Center Chemistry :: Biology :: Physics :: Math Rapid Learning Center Presents …p g Teach Yourself AP Physics in 24 Hours 1/67 *AP is a registered trademark of the College Board, which does not endorse, nor is affiliated in any way with the Rapid Learning courses. H t d Th d iHeat and Thermodynamics Physics Rapid Learning Series Rapid Learning Center www.RapidLearningCenter.com/ © Rapid Learning Inc. All rights reserved. Wayne Huang, Ph.D. Keith Duda, M.Ed. Peddi Prasad, Ph.D. Gary Zhou, Ph.D. Michelle Wedemeyer, Ph.D. Sarah Hedges, Ph.D.
  • 2. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 2 Learning Objectives Temperature: Understand the definition of temperature. By completing this tutorial, you will learn: Energy in Thermal Processes. Understand the relationship between heat and internal energy. Thermal Processes in your world. Global warming and greenhouse gasses. 3/67 Laws of Thermodynamics. Apply the laws of thermodynamics to real life problems such as engines and human metabolism. Concept Map Physics Studies Previous content New content Thermodynamics The field of Matter and EnergyMatter and Energy Heat Energy One type of energy is 2nd Law1st Law Expansion Thermal Expansion 4/67 17 : 3/68 Heated objectsHeated objects expand Energy is destroyed Energy is neither created nor destroyed Entropy increases Entropy always increases States thatStates that States that
  • 3. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 3 ThermodynamicsThermodynamics and Thermal Expansion Thermometers and Temperature Scales. Thermal expansion of Solids and Liquids 5/67 Thermal expansion of Solids and Liquids Thermodynamics and Temperature How does temperature affect materials and how is this used to measure temperature? Linear expansion Volume expansion The physics of thermostats The physics of 6/67 thermometers
  • 4. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 4 Definition - Thermodynamics Thermodynamics - The branch of physics that deals with conversionsphysics that deals with conversions between heat energy and other forms of energy. 7/67 Thermal Expansion As solids and liquids are heated, they expand because their molecules gain kinetic energy and move around more. Expansions of solids can be predicted using the linear expansion equation. Expansions of liquids can be predicted using the volume expansion equation. 8/67 p q The ticking noises heard after a hot car is shut down are due the shape changes of engine parts as they cool.
  • 5. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 5 Linear Expansion Equation The linear expansion equation is of the form: Where: L = length of object T = temperature ∆TαL∆L ××= 9/67 p α = coefficient of linear expansion [units = per degree] ∆ = Greek letter “delta”, change in. Volume Expansion Equation Similarly, the volume expansion equation is of the form: ∆TβV∆V ××= Where: V = volume of object T = temperature ∆TβV∆V ××= 10/67 ß = coefficient of volume expansion [units = per degree] ∆ = Greek letter “delta”, change in.
  • 6. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 6 Expansion Coefficients Note the units of the expansion coefficients: 1∆L α ×= 1∆V β ×= The linear and volume expansion coefficients are Thus, length and volume cancel. Both expansion coefficients have units of “per degree” ∆TL α × ∆TV β × 11/67 The linear and volume expansion coefficients are related to each other by the following relationship: Typical values for expansion coefficients may be found in your physics textbook. α3β ×= Sample Problem: Thermal Expansion Question: How much will the volume of a 2 cm3 aluminum cube change if the temperature changes from 12°C to 32°C? The linear expansion coefficient, α, of aluminum is 23x10-6/°C. S l tiSolution: Step 1: Use the volume expansion equation. ∆V = Vß * ∆T Step 2: Calculate ∆T. ∆T = Tfinal –Tinitial = 32°C – 12°C = 20°C St 3 C l l t ß 12/67 Step 3: Calculate ß. ß = 3α = 3 * 23 x10-6/°C = 69 x 10-6/°C Step 4: Plug in the values. ∆V = Vß * ∆T = (2cm3) * (69x10-6/°C) * (20°C) Answer: ∆V = 2.76x10-3 cm3
  • 7. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 7 Note - Units and Temperature Change 13/67 Thermostats - 1 Thermostats are designed to measure temperature by applying the principle of linear expansion. A thermostat uses two fused strips of metal, each with a different linear expansion coefficient. As the strip heats up one strip lengthens faster so the strips 14/67 bend away from the longer strip. Typically the bent strips will make contact with a circuit.
  • 8. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 8 Thermostats - 2 Imagine a thermostat made up of two metal strips as shown below. The yellow strip has a larger linear expansion coefficient. Heat 15/67 Heat The strip bends towards the side with the lower linear expansion coefficient. Thermometers Thermometers are designed to measure temperature by applying the principle of thermal expansion. Most home thermometers use mercury or alcohol inside a narrow glass tube. As the temperature rises, both the glass and liquid expand. The liquid has a higher volume 16/67 The liquid has a higher volume expansion coefficient than the glass tube so it rises within the tube to tell you the temperature.
  • 9. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 9 Thermal Expansion: Stop-And-Think Question: Why would engineers need to take thermal expansion into account in the design of bridges? On hot days, the metal supports of a bridge will expand and buckle if the bridge is not designed to expand. Similarly, the bridge will crack as the supports shrink on a cold day. 17/67 Energy in Thermal Processes Heat and Internal Energy Specific Heat 18/67 Specific Heat Calorimetry Latent Heat and Phase Change Energy Transfer Global Warming and Greenhouse Gasses
  • 10. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 10 System vs. Surroundings Calculations of heat and internal energy are based on the definition of a system and its surroundings. System - The system refers to the object being studied. Surroundings - 19/67 g Everything not included in the system. Example - System v. Surroundings Example: a beaker The system refers to the contents of the beaker. Th di f 20/67 The surroundings refer to everything else.
  • 11. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 11 Heat and Internal Energy Equation Internal energy of a system is defined as: 1) The ability to do work on an object. 2) The ability to transfer heat to an object. U = q + w Heat Heat energy of the system 21/67 q Internal Energy Work System internal energy Work done on the system or energy available for the system to do work. Definition - Energy Units Calorie (cal) - Heat is measured in calories. A calorie is the amount of heat required to heat 1 gram of water 1°C. Joule (J) - Energy is measured in Joules. One calorie (cal) is equal to 4 18J 22/67 4.18J. 4.18 J = 1 cal
  • 12. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 12 Definition - State Function State Function - n. A state function is a quantity of the object that isa quantity of the object that is dependent on the current state. A state function is independent of the path taken to reach the current state. 23/67 Temperature, kinetic energy, and potential energy are all state functions. Temperature is a State Function Temperature is an example of a state function. Your coffee can be 40°C whether you heated it in the microwave or on the stove. 24/67 40°C
  • 13. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 13 Note: the Food Calorie 25/67 Definition - Specific Heat Specific Heat (CP) - n. Specific heatp ( P) p is a material property that defines the quantity of heat, q, required to raise 1g of a specific material 1°C. 26/67 units of cp = [cal/gram*K]
  • 14. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 14 Specific Heat Equation T T The specific heat may be used as follows: Q = CPm * ∆T Specific Heat Change in Temperature Tfinal - Tinitial (K) or (°C) Proportionality Constant J/g*K or cal/g*K 27/67 P Heat Total Heat Energy (J) Mass Mass of Object (g) Interpretation of Specific Heat What are the practical implications of specific heat? High Specific Heat Low Specific Heat Large amount of energy to change temperature Small amount of energy can change temperature Heats up slowly Cools down slowly Small temperature changes with condition changes e g Water Cast iron Heats up quickly Cools down quickly Quickly readjusts to new conditions e g Air aluminum foil 28/67 e.g. Water, Cast-iron e.g. Air, aluminum foil A pool takes a long time to warm up and remains fairly warm over night. The air warms quickly on a sunny day, but cools quickly at night A cast-iron pan stays hot for a long time after removing from oven. Aluminum foil can be grabbed by your hand from a hot oven because it cools so quickly
  • 15. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 15 Specific Heat and Heat Capacity Thus, if the specific heat and the mass of any object are known, then the amount of heat need to raise the temperature by any given amount may be calculated. The heat capacity C of an object may be determined from its specific heat CP and its mass m as follows: CmC × 29/67 C = heat capacity CP = specific heat m = mass of object pCmC ×= Definition - Heat Capacity Heat Capacity (C) - The amount of heat Q required to raise the temperature of an object by ∆T is given by: Q = C * ∆T Heat Capacity Proportionality Constant J/K or cal/K object by ∆T is given by: 30/67 Q = C * ∆T Heat Change in Temperature Tfinal - Tinitial (K) or (°C) Total Heat Energy (J)
  • 16. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 16 Definition - Enthalpy (H) Enthalpy of Reaction (H) - The enthalpy of a reaction is the heat energy (J) gained or lost during a reaction. Enthalpy is a state function.during a reaction. Enthalpy is a state function. Reaction Bonds of reactants broken. Bonds of products formed. Bonds of reactants have hi h th Bonds of products have higher energy than 31/67 higher energy than bonds of products. higher energy than bonds of reactants. Exothermic Endothermic Heat given off by system Heat absorbed by system Endothermic vs. Exothermic Exothermic - If the system looses net heat during a reaction, the reaction isg , exothermic. Endothermic - If the system gains net ∆Hsystem = Hfinal – Hinitial < 0 32/67 y g heat energy during a reaction, the reaction is endothermic. ∆Hsystem = Hfinal – Hinitial > 0
  • 17. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 17 Definition - Calorimetry Calorimetry. n. Calorimetry is aCalorimetry is a laboratory technique used to determine the amount of heat Q taken up or given off 33/67 by a reaction. Procedure - Calorimetry A small beaker is immersed in an insulated1 How to determine the heat of a reaction using calorimetry. beaker filled with a known amount of water. The initial temperature of the water is noted. A known amount of the reactants are placed in the small reaction beaker. The temperature of the water is recorded at 1 2 3 4 34/67 regular intervals as the reaction proceeds. The change is temperature is plotted versus time. 4 5 6 The heat given off by the reaction is calculated from the total change in temperature of the water.
  • 18. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 18 Example - Calorimetry (1) Large, insulated beaker (2) Water initial(2) Water, initial temperature Tinitial (3) Reaction beaker (4) Initiate reaction 35/67 (5) Flow of heat energy to water (6) Measure final water temperature, Tfinal (7) Calculate ∆H from ∆Twater and the specific heat of water, CP. Endothermic vs. Exothermic Reactions Endothermic Exothermic Heat moves from Heat moves from system surroundings to system Internal energy of system increases KEAVE of system molecules increases Internal energy of system decreases KEAVE of the system decreases to surroundings. 36/67 Temperature of the system increases Bonds of reaction products have greater energy than bonds of reactants Temperature of the system decreases. Chemical bonds of reactants have greater energy than bonds of products.
  • 19. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 19 Stop and Think- Calorimetry Question: If the temperature of the water in a l i t i t i i th ticalorimetry experiment rises, is the reaction endothermic or exothermic? Answer: The reaction is exothermic because heat energy is moving from the system (the reaction) to 37/67 energy is moving from the system (the reaction) to the surroundings (the water). Latent Heat and Phase Change A rise in temperature Internal energy increases When a solid is heated it undergoes the following: Internal energy increases Molecules oscillate more rapidly A phase change from solid to liquid Molecules oscillate so rapidly they loose their crystalline form There is no increase in temperature during the transition Another rise in temperature 38/67 Another rise in temperature A phase change from liquid to gas Molecules oscillate so rapidly they escape the intermolecular forces that bind them together and enter the gas phase There is no increase in temperature during the transition.
  • 20. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 20 Heats of Fusion and Vaporization The amount of heat Qfus needed to melt m grams of a substance is given by the following equation: fusfus Lm∆Q ×= Qfus = heat energy = [calories] m = mass = [grams] Lfus = Heat of Fusion = [calories/gram] The amount of heat Qvap needed to vaporize m grams of a substance is given by the following equation: fusfus Lm∆Q × 39/67 Qvap = heat = [calories] m = mass = [grams] Lvap = Heat of Vaporization = [calories/gram] of a substance is given by the following equation: vapvap Lm∆Q ×= Latent Heat and Phase Change Gas Temperatureof Substance Phase Liquid Phase Solid Tboil Tmelt 40/67 Increase in Heat Energy, ∆Q Solid Phase Qmelt Qboil
  • 21. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 21 Example - Heats of Transformation Question: How much heat energy is required for 10 grams of ice at 0°C to transition to liquid? To evaporate? The heat of fusion for water is 333 KJ/kg. The heat of vaporization is 2256 KJ/kg. Solution:Solution: 1) Calculate the heat energy required to melt 10 grams (0.01Kg) of ice. Qfus = Lfus * m = 333 KJ/kg * 0.01 Kg = 3.33 KJ 2) Calculate the heat energy needed to raised the temperature of the water from 0°C to 100°C. Q = 0.00418 KJ/g*°C * 10.0 g * (100-0)°C = 4.18 kJ 41/67 3) Calculate the heat energy required to vaporize 10g of water. Qvap = Lvap * m = 2256 KJ/kg * 0.01Kg = 22.56 KJ 4) The total heat required is the sum of 1-3. Qtot = 3.33 KJ + 4.18 KJ + 22.56 KJ = 30.07 KJ Answer: Qtot = 30.07 KJ Stop-and-think- Sweating Question: Why is sweating an effective cooling mechanism? 42/67 Answer: As sweat evaporates from your skin it transitions from the liquid to the gas phase. This phase transition requires a transfer of heat energy from the skin to the liquid, cooling the skin.
  • 22. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 22 Global Warming & Greenhouse Gases 1) Heat energy radiates from the sun to the earth 2) Some of the heat energy is reflected off greenhouse gasesreflected off greenhouse gases in the earth’s atmosphere. 3) Some of the heat energy is reflected of the earth’s surface. 4) Some of the energy reflected off the surface is trapped by greenhouse gases in the 43/67 atmosphere. 5) As the concentration of greenhouse gases is increased due to emissions from cars and factories, the temperature of the earth rises. The Laws of Thermodynamics The Zeroth Law of Thermodynamics Work in Thermodynamic Processes 44/67 Work in Thermodynamic Processes The First Law of Thermodynamics Heat, Engines, and the Second Law of Thermodynamics Entropy Human Metabolism
  • 23. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 23 Heat Energy and the Laws of Thermodynamics The Zeroth Law of Thermodynamics states that objects in thermal ilib i t th The laws of thermodynamics govern energy exchanges: equilibrium are at the same temperature. The internal energy of a system is the sum of the heat energy of the system and the work done on or by the system. The 1st Law of Thermodynamics states that energy can change state but cannot 45/67 gy g be created or destroyed. The 2nd Law of Thermodynamics states that the total entropy, or disorder, of the universe can increase or stay the same but never decrease. The universe tends towards disorder. Definition: Thermal Equilibrium Thermal Equilibrium - Two objects are thermal equilibrium are at the sameq temperature. That is, when put in contact they remain at the same temperature and no longer exchange net heat energy. A and B areIf A is placed inThe temperature 46/67 A and B are said to be in thermal equilibrium. p contact with B, they both remain at 10C°. The temperature of A is 10C° and the temperature of B is 10C° Note that if objects are in thermal equilibrium, their molecules also have the same average kinetic energy
  • 24. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 24 Zeroth Law of Thermodynamics Zeroth Law - If object A is in thermal equilibrium with object B and object C, then objects B and C are also in thermalthen objects B and C are also in thermal equilibrium. A 10 degrees Celsius 47/67 B C 10 degrees Celsius 10 degrees Celsius Note that if B and C are in thermal equilibrium with A, then they must also be at 10 degrees Celsius. Work in Thermodynamics As mentioned before: U = q +U = q + w U = system internal energy q = heat energy w = work done on or by the system 48/67
  • 25. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 25 Pressure-Volume Work For constant pressure: ∆W = -P * ∆V ∆W = work done on or by the system P = pressure ∆V = volume change of the system One common type of application of this equation is in calculating pressure-volume work done by 49/67 engines. Applied Pressure-Volume Work If the system expands, work is done by the system on the surroundings. The internal energy of the systeminternal energy of the system decreases. If the system contracts, work is done 50/67 by the surroundings on the system. The internal energy of the system increases.
  • 26. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 26 The First Law of Thermodynamics Energy in a reaction may be changed from one form to another but it is neither t d d t d ti fcreated nor destroyed – conservation of energy. 51/67 Application of The 1st Law This implies that: Q Q ∆U = ∆q + ∆w Change in Heat Energy W k d t b Qinitial -Qfinal 52/67 Change in System Internal Energy Work done to or by the system Ufinal - Uinitial Win -Wout
  • 27. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 27 Work and the 1st Law There are 4 special applications of the 1st Law: 1) Adiabatic: Q = 0, ∆U = -W 2) Constant-volume: W = 0, ∆U = Q 3) Cyclical: ∆U = 0, Q = -W 53/67 4) Free expansion processes: ∆U = Q = W Adiabatic Work An example of adiabatic work is a closed system with a piston. If pressure is applied rapidly to depress the piston, the volume of the system will decrease. Work W is done on the system by the surroundings, but there is ∆V ≥ 0 Q = 0, ∆U = -W = -P*∆V is done on the system by the surroundings, but there is no change in heat Q so the change in internal energy ∆U is equal to –W. W 54/67 W Vinitial Vfinal
  • 28. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 28 Constant-Volume Work An example of constant-volume work is heating a sealed cylinder. There is no volume change so the change in internal energy is equal to the change in heat energyenergy. Tinitial Tfinal 55/67 ∆V = 0 so W = 0 ∆T ≥ 0 so Q ≥ 0 ∆U = Q Cyclical Work and Engines In an engine, heat is used to increase pressure leading to an increase in volume. The change in volume does work on the surroundings. The work energy is transferred back from the surroundings to compress the cylinder back to its original size and the cycle repeatsand the cycle repeats. ∆U = 0 Q W 56/67 Q = -W
  • 29. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 29 Free Expansion Work Connecting a pressurized system to a vacuum is an example of free-expansion work. The gas from the pressurized system will immediately and irreversibly expand to fill the vacuum The process occurs rapidlyexpand to fill the vacuum. The process occurs rapidly, but unlike adiabatic work the process is irreversible. ∆U = Q = W = 0 Heating an open beaker may be considered free- i k Th t th t t f th 57/67 expansion work. The system, the contents of the beaker, are open to the surroundings so there can be no volume changes or heat exchanges. Energy Calculations: Example Question: If the volume of a sealed balloon increases from 10mL to 100mL when heated and then shrinks back to 10mL as it cools, what f tapplication of the 1st Law is this? Constant-volume Adiabatic 58/67 Cyclical
  • 30. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 30 Energy Calculations: Answer Question: If the volume of a sealed balloon increases from 10mL to 100mL when heated and then shrinks back to 10mL as it cools, what f tapplication of the 1st Law is this? Constant-volume Adiabatic 59/67 Cyclical Definition - Entropy Entropy (S) - n. Entropy is a measure of the disorder of a system or its surroundings.surroundings. 60/67 A landfill possesses lots of entropy!
  • 31. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 31 The 2nd Law of Thermodynamics The 2nd Law of Thermodynamics states that the total entropy of the universe can never decrease, it can only increase or stay the same. ∆Stotal ≥ 0 Note that the entropy of the system may decrease, so long as the entropy of the s rro ndings increases b an eq al or greater 61/67 surroundings increases by an equal or greater amount. Thus, ∆Ssys + ∆Ssur ≥ 0 Relative Entropies Low entropy states are more organized than high entropy states. Lower Entropy Higher Entropy Your clean bedroom Your room after finals Solids Liquids 62/67 Liquids Salt tablets in water Gases Dissolved salt in water
  • 32. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 32 Definition - Engine Efficiency In a real combustion engine such as your car, some of the work energy is lost to the surroundings as heat rather than transferred to pressure-volume work which moves a piston. The efficiency of an engine is the ratio of the heat energy put in (for example by combustion) to the work output by the engine (such as movement of the wheels of a car). ε = Wout / Qin 63/67 If the efficiency of an engine is 0.7, the 30% of the heat from combustion is lost as heat to the surroundings. In the real world, this would be a very efficient engine!!! Entropy and Human Metabolism Question: Metabolic processes in the body, such as the building of proteins and DNA, lead to increased order. How does this not violate the 2nd Law? Answer: Although the building of structural proteins in the body lead to increased order in the system, which is the body, they lead to increased disorder in the surroundings through loss of heat. 64/67 surroundings through loss of heat. Metabolic processes are usually linked to a catabolic process such as the combustion of glucose or the flow of ions down a concentration gradient.
  • 33. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 33 Entropy: Stop-and-Think Question Question: When an ice cube melts, does system entropy increase, decrease, or remain the same? Pick the best answerPick the best answer. A. Remain the same because there is no reaction, only a state change. B. Increase because the molecules are changing 65/67 g g from an ordered crystalline state to a disordered liquid state. C. Decrease because heat is absorbed to melt the ice. Entropy: Stop-and-Think Answer Question: When an ice cube melts, does system entropy increase, decrease, or remain the same? Pick the best answerPick the best answer. A. Remains the same because there is no reaction, only a state change. B. Increases because the molecules are changing 66/67 g g from an ordered crystalline state to a disordered liquid state. C. Decreases because heat is absorbed to melt the ice.
  • 34. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 34 Entropy is aEntropy is a Expansion coefficients measure how Expansion coefficients measure how The 2nd Law states that net entrop can The 2nd Law states that net entrop can Learning Summary Heat energy mayHeat energy may measure of disorder. measure of disorder. measure how much objects expand when heated. measure how much objects expand when heated. entropy can never decrease. entropy can never decrease. The 1st LawThe 1st Law 67/67 Heat energy may be gained or lost to the surroundings during work. Heat energy may be gained or lost to the surroundings during work. The 1 Law states that energy is never created or destroyed. The 1 Law states that energy is never created or destroyed. Congratulations Y h f ll l t dYou have successfully completed the tutorial Heat and Thermodynamics 68/67 Rapid Learning Center
  • 35. AP Physics Rapid Learning Series - 13 © Rapid Learning Inc. All rights reserved. - http://www.RapidLearningCenter.com 35 Rapid Learning Center Wh t’ N t Chemistry :: Biology :: Physics :: Math What’s Next … Step 1: Concepts – Core Tutorial (Just Completed) Step 2: Practice – Interactive Problem Drill Step 3: Recap – Super Review Cheat Sheet 69/67 Go for it! http://www.RapidLearningCenter.com