Title: Principles of Technology/Physics in Context (PT/PIC)
1Principles of Technology/Physics in Context
(PT/PIC)
- Chapter 8
- Internal Energy and
- Properties of Matter 1
- Text p. 150 -154
2Key Objectives
- At the conclusion of this chapter youll be able
to - Define the following terms internal energy and
temperature, absolute zero, heat energy and
specific heat, and pressure. - State the fixed points on the Celsius temperature
scale and the fixed point on the Kelvin
temperature scale.
3Key Objectives
- At the conclusion of this chapter youll be able
to - Relate Kelvin and Celsius temperatures, and solve
problems involving this relationship. - State the equation that relates heat energy,
specific heat, and temperature changes, and solve
problems using this equation. - Define the term thermal equilibrium, and solve
thermal equilibrium problems.
48.1 INTERNAL ENERGY AND WORK
- Suppose we use a force to move an object along a
horizontal table at constant speed. - We know from Chapter 7 that we have done work on
the object, but what has this work accomplished? - The kinetic energy has not changed because the
speed has been kept constant.
58.1 INTERNAL ENERGY AND WORK
- The gravitational potential energy has not
changed because the table is horizontal. - Our work has been used to overcome the friction
between the object and the table, and, therefore
we say that the internal energy of the
object-table system has been increased by the
work we have done.
6Assessment Question 1
- Suppose we use a force to move an object along a
horizontal table at constant speed. - All of the following are true EXCEPT
- No work is done on the object.
- The kinetic energy has not changed because the
speed has been kept constant. - The gravitational potential energy has not
changed because the table is horizontal. - The internal energy of the object-table system
has been increased by the work we have done.
78.1 INTERNAL ENERGY AND WORK
- Roughly speaking, the internal energy (Q) of a
system is the total kinetic and potential
energies of the atoms and molecules that make up
the system. - A change in the internal energy of an object is
usually accompanied by a change in its
temperature.
88.2 TEMPERATURE AND TEMPERATURE SCALES
- Temperature is a measure of the hotness of an
object with respect to some predefined standard. - It is a scalar quantity.
- We will see in Section 8.4 that the temperature
of an object is related to the average kinetic
energy of its molecules.
98.2 TEMPERATURE AND TEMPERATURE SCALES
- When mercury is placed in a thin tube (whose
diameter is uniform), the length of the mercury
column increases with rising temperature. - Such a device is called a thermometer
10Assessment Question 2
- All of the following are true EXCEPT
- A change in the internal energy of an object is
usually accompanied by a change in its
temperature. - Temperature is a measure of the hotness of an
object with respect to some predefined standard. - Temperature is a vector quantity measured by a
device called a temperaguage. - The temperature of an object is related to the
average kinetic energy of its molecules.
118.2 TEMPERATURE AND TEMPERATURE SCALES
- To measure temperature, we need a property that
changes regularly with changes in temperature. - One such property is the volume of a liquid such
as mercury.
128.2 TEMPERATURE AND TEMPERATURE SCALES
- We also need to establish a scale of measurement.
- To do this, one or more fixed reference points
must be set.
138.2 TEMPERATURE AND TEMPERATURE SCALES
- On the Celsius scale, the freezing and boiling
points of water (at 1 atmosphere of pressure) are
assigned the respective temperatures of 0C and
100C. - (The Fahrenheit scale sets these points at 32F
and 2 12F.)
148.2 TEMPERATURE AND TEMPERATURE SCALES
- Another scale is the Kelvin or absolute
temperature scale. - Its single reference point is the temperature at
which water exists simultaneously as a gas,
liquid, and solid.
158.2 TEMPERATURE AND TEMPERATURE SCALES
- The temperature assigned to this triple point
is 273.16 K. - On the Kelvin scale, zero kelvin (0 K) is the
lowest temperature possible and is known as
absolute zero. - At this temperature, molecular motion is at a
minimum.
16Assessment Question 3
- All of the following are true EXCEPT
- On the Celsius scale, the freezing and boiling
points of water (at 1 atmosphere of pressure) are
assigned the respective temperatures of 0C and
100C. - On the Fahrenheit scale the freezing and boiling
points of water (at 1 atmosphere of pressure) are
assigned the respective temperatures of 32F and
212F. - The quadruple point is the temperature at which
water exists simultaneously as a gas, liquid,
solid and plasma the temperature is -250 K. - On the Kelvin scale, zero kelvin (0 K) is the
lowest temperature possible and is known as
absolute zero. At this temperature, molecular
motion is at a minimum.
178.2 TEMPERATURE AND TEMPERATURE SCALES
- The relationship between the Celsius (TC) and
Kelvin (TK) temperature scales is as follows
188.2 TEMPERATURE AND TEMPERATURE SCALES
- PROBLEM
- (a) Convert 37C (TC) to the Kelvin scale (TK)
198.2 TEMPERATURE AND TEMPERATURE SCALES
- PROBLEM
- (a) Convert 37C to the Kelvin scale.
- SOLUTION
- (a) TKTC 273 37C 273 310K
20Assessment Question 4
- Convert 97C (TC) to the Kelvin scale (TK)
- TKTC 273 97C 273
- -75 K
- 176 K
- 260 K
- 370 K
218.2 TEMPERATURE AND TEMPERATURE SCALES
- PROBLEM
- (b) Convert 0 K (TK) to the Celsius scale (TC) .
228.2 TEMPERATURE AND TEMPERATURE SCALES
- PROBLEM
- (b) Convert 0 K to the Celsius scale.
- SOLUTION
- (a) TKTC 273
- (a) TC TK - 273 0 K - 273 -273 C
23Assessment Question 5
- Convert 57 K (TK) to the Celsius scale (TC)
- TKTC 273
- TC TK - 273 57 K - 273
- -1550 C
- -216 C
- 220 C
- 330 C
248.2 TEMPERATURE AND TEMPERATURE SCALES
- Frequently, scientists refer to standard
temperature, which has a defined value of 273 K
(the freezing point of water at 1 atmosphere of
pressure).
258.3 HEAT AND INTERNAL ENERGY
- An object can change its internal energy by
absorbing or releasing heat energy. - If no phase changes (e.g., freezing, boiling) are
occurring, the absorption or release of heat
energy is accompanied by a change in temperature.
268.3 HEAT AND INTERNAL ENERGY
- The amount of heat energy absorbed or released is
directly related to three factors the substance
itself, its mass, and the size of the temperature
change.
278 HEAT AND INTERNAL ENERGY
- These three quantities can be combined into a
single equation
288.3 HEAT AND INTERNAL ENERGY
- where Q stands for the amount of heat energy in
joules, m is the mass of the substance in
kilograms, and ?TC is the temperature change of
the substance in Celsius degrees (C).
298.3 HEAT AND INTERNAL ENERGY
- The symbol c stands for the specific heat of the
substance. - The value of the specific heat identifies the
substance its units are kilojoules per kilogram
per Celsius degree (kJ/kg C).
308.3 HEAT AND INTERNAL ENERGY
- The lower the specific heat of a substance, the
more readily it changes its temperature in
response to heat loss or heat gain. - For example, dry land has a much lower specific
heat than water. - For this reason, landlocked areas tend to have
much larger changes in temperature (warmer
summers and colder winters) than areas that are
near large bodies of water.
31Assessment Question 6
- All of the following are true EXCEPT
- An object can change its internal energy by
absorbing or releasing heat energy. If no phase
changes (e.g., freezing, boiling) are occurring,
the absorption or release of heat energy is
accompanied by a change in temperature. - The amount of heat energy absorbed or released is
directly related to three factors the substance
itself, its mass, and the size of the temperature
change. - The lower the specific heat of a substance, the
more readily it changes its temperature in
response to heat loss or heat gain. - Dry land has a much larger specific heat than
water so landlocked areas tend to have small
changes in temperature (cool summers and mild
winters) and areas near large bodies of water
have large changes in temperature (hot summers
and cold winters).
328.3 HEAT AND INTERNAL ENERGY
- A table of specific heats for various substances
is given below
338.3 HEAT AND INTERNAL ENERGY
- PROBLEM
- How much heat energy (Q) is needed to raise the
temperature of 20 kilograms (m) of liquid water
from 5C to 20C (?T)?
348.3 HEAT AND INTERNAL ENERGY
- SOLUTIONHow much heat energy (Q) is needed to
raise the temperature of 20 kilograms (m) of
liquid water from 5C to 20C (?T)?
35Assessment Question 7
- How much heat energy (Q) is needed to raise the
temperature of 50 kilograms (m) of liquid water
from 15C to 40C (?T)? - Q cm ?T
- Q 4.19 kJ/kgCo)(50 kg) (40C - 15C)
- 50 J
- 250 J
- 5200 J
- 7500 J
368.3 HEAT AND INTERNAL ENERGY
- The positive sign associated with Q is a result
of the sign of ?TC and indicates that heat has
been absorbed. - If the temperature had decreased, ?TC would have
been negative, as would Q. - This would mean that heat had been released.
378.3 HEAT AND INTERNAL ENERGY
- Suppose two objects with different temperatures
are brought into contact. - Experience tells us that heat energy is always
transferred from the hotter object to the colder
one until they both reach the same final
temperature.
388.3 HEAT AND INTERNAL ENERGY
- At this point, we say that the objects have
reached thermal equilibrium the final
temperature is known as the equilibrium
temperature. - This will occur, regardless of the nature of the
objects or their masses. - (The identity of the objects and their masses
will determine the value of the final
temperature, however.)
398.3 HEAT AND INTERNAL ENERGY
- Problems involving heat-energy transfer utilize
the relationship Q cm ?TC - However, this relationship must be used
twiceonce for the object that releases (loses)
heat energy, and once for the object that absorbs
(gains) it.
408.3 HEAT AND INTERNAL ENERGY
- We assume that the total internal energy is
conserved therefore, the heat energy lost by
the hotter object is set equal to the heat energy
gained by the colder object.
41Assessment Question 8
- Suppose two objects with different temperatures
are brought into contact. - All of the following are true EXCEPT
- Heat energy is always transferred from the hotter
object to the colder one until they both reach
the same final temperature. - When both objects are at the same temperature the
objects have reached thermal equilibrium the
final temperature is known as the equilibrium
temperature. This will occur, regardless of the
nature of the objects or their masses. - The objects will always reach the same final
temperature regardless of the identity of the
objects and their masses. - The total internal energy is conserved
therefore, the heat energy lost by the hotter
object is set equal to the heat energy gained
by the colder object.
428.3 HEAT AND INTERNAL ENERGY
- The equations look like this
438.3 HEAT AND INTERNAL ENERGY
- The vertical bars (J ) indicate that we are
interested only in the (absolute) value of the
quantity, not whether it is positive or negative.
- The quantity k is evaluated by subtracting the
smaller temperature from the larger temperature.
448.3 HEAT AND INTERNAL ENERGY
- PROBLEM
- A 10-kilogram (m) block of copper at 60C is
placed in contact with an identical 10-kilogram
(m) block of copper at 20C. - What is the equilibrium temperature of both
blocks?
458.3 HEAT AND INTERNAL ENERGY
- SOLUTION
- We could guess at the answer (40C, the midpoint
temperature between 20C and 60C), and we would
be correct! But lets see why this is so.
468.3 HEAT AND INTERNAL ENERGY
- SOLUTION
- Both blocks have the same mass (10 kg), and both
are composed of the same substance (copper). - The change in heat energy should therefore affect
the temperature of each block equally (but in
opposite directions). - If both blocks must reach the same final temp the
midpoint temperature of 40C is the only
temperature that satisfies these requirements.
478.3 HEAT AND INTERNAL ENERGY
- SOLUTION
- Now lets prove that this is the case by solving
the pair of equations given above
48Assessment Question 9
- A 5.0 kilogram (m) block of copper at 90C is
placed in contact with an identical 5.0 kilogram
(m) block of copper at 10C. - What is both blocks equilibrium temperature?
- Qlost Qgained (cm?T)lost
(cm?T)gained - (0.39 kJ/kgC)(5 kg)(90C-Tfinal) (0.39
kJ/kgC)(5 kg)(Tfinal-10C) - (90C-Tfinal) (Tfinal-10C)
- Tfinal (90C 10C) / 2
- A. 10C C. 80C
- B. 50C D. 100C
498.3 HEAT AND INTERNAL ENERGY
- PROBLEM
- Calculate the equilibrium temperature (Tfinal)
when a 5.0-kilogram (mplatinum) block of platinum
(specific heat 0.13 kJ/kgC) at 20C
(Tplatinum) is placed in contact with a
10.-kilogram (msilver) block of silver (specific
heat 0.24 kJ/kgC) at 40C (Tsilver).
508.3 HEAT AND INTERNAL ENERGY
518.3 HEAT AND INTERNAL ENERGY
- We see that the equilibrium temperature is much
closer to the initial temperature of the silver. - This is a direct result of the fact that the mass
and specific heat of the silver are larger than
the mass and specific heat of the platinum.
52Conclusion
- Temperature is the quantity used to measure the
hotness of a body. A thermometer and an
appropriate scale are needed to make this
measurement.
53Conclusion
- Heat energy is the energy associated with changes
in internal energy. - If no phase changes occur, the transfer of heat
energy is accompanied by a change in temperature.
54Conclusion
- The specific heat of a sub stance indicates how
much heat energy is needed to cause a given
change in the substances temperature. - When two objects are brought into contact, heat
energy will be exchanged until the temperatures
of the objects are equal.
55Assessment Question 10
- Calculate the equilibrium temperature (Tfinal)
when a 15 kg (mplatinum) block of platinum
(specific heat 0.13 kJ/kgC) at 10C
(Tplatinum) is placed in contact with a 25 kg
(msilver) block of silver (specific heat 0.24
kJ/kgC) at 90C (Tsilver). - Qlost Qgained (cm?T)silver
(cm?T)platinum - (0.24 kJ/kgC)(25 kg)(90C-Tfinal) (0.13
kJ/kgC)(15 kg)(Tfinal-10C) - 6 kJ/C (90C-Tfinal) 2 kJ/C (Tfinal-10C)
- Tfinal 3(90C 10C) / 2
- A. -15C B. 75C C. 150C D. 300C