SlideShare a Scribd company logo
Reading Quiz
• A container of helium gas is heated,
raising the temperature of the gas.
This causes
• the average kinetic energy of the gas
molecules to increase.
• the average potential energy of the gas
molecules to increase.
• the average acceleration of the gas molecules
to increase
The internal energy U of a system is increased by
the transfer of either heat or work into the system.
ΔU = Q −W
Frist Law of Thermodynamics
Internal Energy = Added Heat - Work done by the system
A falling mass turns a paddle in an insulated beaker of
water in this schematic representation of Joule’s
apparatus for measuring the temperature increase
produced by doing mechanical work on a system.
Steam issuing from the kettle makes the pinwheel
turn in this simple steam turbine. Work could be
done to lift a small weight with such an engine.
Heat released by
burning gasoline in the
cylinder of an
automobile engine
causes the piston to
move, converting some
of the heat to work.
The internal energy U of a system is increased by
the transfer of either heat or work into the system.
Zeroth Law of Thermodynamics
Two objects in thermal equilibium have the same temperature
What is INTERNAL ENERGY?
The internal energy of the system is the sum
of the kinetic and potential energies of the
atoms and molecules making up the system.
The First Law of Thermodynamics:
The increase in the internal energy of a system is
equal to the amount of heat added to the system,
plus the amount of work done on the system.
The increase in the internal energy of a system is
equal to the amount of heat added to the system,
minus the amount of work done by the system.
U = Q - W
Q=heat add to system
W = work done by system
Quiz 1
The first Law of Thermodynamics, U = Q - W, means:
A. Heat cannot be added to a system without work being
done.
B. Work cannot be done without heat being added.
C. The amount of work done always equals the amount
of heat added.
D. The total internal energy of a system is conserved.
E. All of the above
F. None of the above are true.
CHOOSE THE TRUE STATEMENT.
Work done by a movable piston
Work=F x d = F/A x d x A = P V
Quiz 2
• If the temperature of a gas is held constant
during compression or expansion it is
called
1. Equation of state
2. Isobaric
3. Isothermal
4. Thermal conductivity
5. convection
Convection
Motion of a fluid
Quiz 3
Heat can be transferred by
1. Thermal Conduction
2. Convection
3. Radiation
4. All of the above
5. None of the above
Head Flow
Heat Transfer
What is a heat engine?
• Thermal heat QH is introduced into the engine.
• Some of this is converted into mechanical work, W.
• Some heat is released into the environment at a lower temperature, QC.
What does the First Law tell us about heat engines?
U = Q - W = QH - QC -W
, the internal energy U of a heat engine
does not change from cycle to cycle, so U =0.
Hence, Q = W.
The net heat flowing into the engine equals the work done by
the engine:
W = QH - QC
The Second Law of Thermodynamics
The Carnot engine is an ideal system which turns out to have the
maximum possible efficiency:
If TH is the hottest temperature in the engine, and TC is temperature
outside the engine (in Kelvin), then the efficiency is:
ec = (TH - TC )/ TH
=W/QH
This shows that it is not possible too have an efficiency of 100%.
You always lose some energy into heating the environment.
This can be restated as a version of the Second Law:
No engine, working in a continuous cycle, can take heat from
a reservoir at a single temperature and convert that heat
completely into work.
A restatement of the Second Law which turns out to be
equivalent:
Heat will not flow from a colder body to a hotter body unless
some other process (which does work) is also involved.
Another restatement to be discussed next time:
The entropy of an isolated system can only increase or
remain constant. Its entropy cannot decrease.
According to the Second Law of Thermodynamics,
heat will not flow from a colder body to a warmer
body.
1. True
2. False
According to the Second Law of Thermodynamics,
heat will not flow from a colder body to a warmer
body.
1. True
2. False
A schematic representation
of a heat engine. Heat is
taken in at high
temperatures, TH. Some
heat is converted to work,
and the remainder is
released at a lower
temperature, TC.
The arrow widths depict the quantities of
energy in the sample exercise in box 11.1.
The efficiency of a heat engine is defined as
e = W/ QH .
Engines are more efficient if there is a large
difference between the high temperature inside
and the low temperature outside.
For an ideal heat engine,
ec = (TH - TC )/ TH

More Related Content

PPT
Reaction in chemical engineering ppt.ppt
PDF
laws-of-thermo.pdf
PPT
thermal2n.ppt
PPTX
Thermodynamic3
PPT
chapter 12 The laws of thermodynamics.ppt
PPTX
heat engine overview
PPTX
The laws of thermodynamics
PDF
Ch4_EnginesRefrigerators-converted.pdf
Reaction in chemical engineering ppt.ppt
laws-of-thermo.pdf
thermal2n.ppt
Thermodynamic3
chapter 12 The laws of thermodynamics.ppt
heat engine overview
The laws of thermodynamics
Ch4_EnginesRefrigerators-converted.pdf

Similar to Lecture22Kinetic model of gas. as level.ppt (20)

PPTX
kelompokppt.pptx
PPT
Chapter 10 Powerpoint
PPTX
Themordynamics Unit 2 Mechanical First year
PPT
Hp10win 1229233665242059-1
PPTX
Thermodynamics
PPT
Ch4_EnginesRefrigerators.pptCh4_EnginesRefrigeratorsCh4_EnginesRefrigerators
PPT
lecture notes on engines and refrigerators
PPT
Lecture No.2.ppt
PPT
ap physics b lesson 68 heat engines and the carnot cycle.ppt
DOCX
thermodynamic chemistry-heat engine
PDF
entropy and second law of thermodynamics
PPTX
Chapter10[1]
PPTX
Second law of thermodynamics in chemical engineering.pptx
PPT
Hp 10 win
PPT
Physics P P Presentation Ch 10
PDF
Chapter 15 thermodynamics
PPT
Heat engine 2nd law
PPT
Thermodynamics
PPTX
The First Law of Thermodynamics
kelompokppt.pptx
Chapter 10 Powerpoint
Themordynamics Unit 2 Mechanical First year
Hp10win 1229233665242059-1
Thermodynamics
Ch4_EnginesRefrigerators.pptCh4_EnginesRefrigeratorsCh4_EnginesRefrigerators
lecture notes on engines and refrigerators
Lecture No.2.ppt
ap physics b lesson 68 heat engines and the carnot cycle.ppt
thermodynamic chemistry-heat engine
entropy and second law of thermodynamics
Chapter10[1]
Second law of thermodynamics in chemical engineering.pptx
Hp 10 win
Physics P P Presentation Ch 10
Chapter 15 thermodynamics
Heat engine 2nd law
Thermodynamics
The First Law of Thermodynamics
Ad

More from SIVAPRIYATM (6)

PPT
PHYSICS>> FORCES>Scalars-and-Vectors.ppt
PPT
projectile motion STA 2012.pptvvvvvvvvvv
PPT
Work_ Energy_ and Power.ppt vvvvvvvvvvvv
PPT
PP7_-_2_Equation_of_Motion_for_Accelerated_Motion.ppt
PPT
phyo_c1.ppt
PPT
clem_waves_lesson02_presentation.ppt
PHYSICS>> FORCES>Scalars-and-Vectors.ppt
projectile motion STA 2012.pptvvvvvvvvvv
Work_ Energy_ and Power.ppt vvvvvvvvvvvv
PP7_-_2_Equation_of_Motion_for_Accelerated_Motion.ppt
phyo_c1.ppt
clem_waves_lesson02_presentation.ppt
Ad

Recently uploaded (20)

PDF
O7-L3 Supply Chain Operations - ICLT Program
PPTX
Microbial diseases, their pathogenesis and prophylaxis
PDF
Classroom Observation Tools for Teachers
PDF
grade 11-chemistry_fetena_net_5883.pdf teacher guide for all student
PDF
3rd Neelam Sanjeevareddy Memorial Lecture.pdf
PDF
GENETICS IN BIOLOGY IN SECONDARY LEVEL FORM 3
PPTX
Final Presentation General Medicine 03-08-2024.pptx
PPTX
Presentation on HIE in infants and its manifestations
PPTX
human mycosis Human fungal infections are called human mycosis..pptx
PPTX
Pharmacology of Heart Failure /Pharmacotherapy of CHF
PDF
Complications of Minimal Access Surgery at WLH
PDF
ANTIBIOTICS.pptx.pdf………………… xxxxxxxxxxxxx
PPTX
Lesson notes of climatology university.
PPTX
master seminar digital applications in india
PDF
STATICS OF THE RIGID BODIES Hibbelers.pdf
PDF
Computing-Curriculum for Schools in Ghana
PDF
2.FourierTransform-ShortQuestionswithAnswers.pdf
PDF
RMMM.pdf make it easy to upload and study
PDF
Abdominal Access Techniques with Prof. Dr. R K Mishra
PPTX
school management -TNTEU- B.Ed., Semester II Unit 1.pptx
O7-L3 Supply Chain Operations - ICLT Program
Microbial diseases, their pathogenesis and prophylaxis
Classroom Observation Tools for Teachers
grade 11-chemistry_fetena_net_5883.pdf teacher guide for all student
3rd Neelam Sanjeevareddy Memorial Lecture.pdf
GENETICS IN BIOLOGY IN SECONDARY LEVEL FORM 3
Final Presentation General Medicine 03-08-2024.pptx
Presentation on HIE in infants and its manifestations
human mycosis Human fungal infections are called human mycosis..pptx
Pharmacology of Heart Failure /Pharmacotherapy of CHF
Complications of Minimal Access Surgery at WLH
ANTIBIOTICS.pptx.pdf………………… xxxxxxxxxxxxx
Lesson notes of climatology university.
master seminar digital applications in india
STATICS OF THE RIGID BODIES Hibbelers.pdf
Computing-Curriculum for Schools in Ghana
2.FourierTransform-ShortQuestionswithAnswers.pdf
RMMM.pdf make it easy to upload and study
Abdominal Access Techniques with Prof. Dr. R K Mishra
school management -TNTEU- B.Ed., Semester II Unit 1.pptx

Lecture22Kinetic model of gas. as level.ppt

  • 1. Reading Quiz • A container of helium gas is heated, raising the temperature of the gas. This causes • the average kinetic energy of the gas molecules to increase. • the average potential energy of the gas molecules to increase. • the average acceleration of the gas molecules to increase
  • 2. The internal energy U of a system is increased by the transfer of either heat or work into the system. ΔU = Q −W Frist Law of Thermodynamics Internal Energy = Added Heat - Work done by the system
  • 3. A falling mass turns a paddle in an insulated beaker of water in this schematic representation of Joule’s apparatus for measuring the temperature increase produced by doing mechanical work on a system.
  • 4. Steam issuing from the kettle makes the pinwheel turn in this simple steam turbine. Work could be done to lift a small weight with such an engine.
  • 5. Heat released by burning gasoline in the cylinder of an automobile engine causes the piston to move, converting some of the heat to work.
  • 6. The internal energy U of a system is increased by the transfer of either heat or work into the system. Zeroth Law of Thermodynamics Two objects in thermal equilibium have the same temperature
  • 7. What is INTERNAL ENERGY? The internal energy of the system is the sum of the kinetic and potential energies of the atoms and molecules making up the system.
  • 8. The First Law of Thermodynamics: The increase in the internal energy of a system is equal to the amount of heat added to the system, plus the amount of work done on the system. The increase in the internal energy of a system is equal to the amount of heat added to the system, minus the amount of work done by the system. U = Q - W Q=heat add to system W = work done by system
  • 9. Quiz 1 The first Law of Thermodynamics, U = Q - W, means: A. Heat cannot be added to a system without work being done. B. Work cannot be done without heat being added. C. The amount of work done always equals the amount of heat added. D. The total internal energy of a system is conserved. E. All of the above F. None of the above are true. CHOOSE THE TRUE STATEMENT.
  • 10. Work done by a movable piston Work=F x d = F/A x d x A = P V
  • 11. Quiz 2 • If the temperature of a gas is held constant during compression or expansion it is called 1. Equation of state 2. Isobaric 3. Isothermal 4. Thermal conductivity 5. convection
  • 13. Quiz 3 Heat can be transferred by 1. Thermal Conduction 2. Convection 3. Radiation 4. All of the above 5. None of the above
  • 16. What is a heat engine? • Thermal heat QH is introduced into the engine. • Some of this is converted into mechanical work, W. • Some heat is released into the environment at a lower temperature, QC.
  • 17. What does the First Law tell us about heat engines? U = Q - W = QH - QC -W , the internal energy U of a heat engine does not change from cycle to cycle, so U =0. Hence, Q = W. The net heat flowing into the engine equals the work done by the engine: W = QH - QC
  • 18. The Second Law of Thermodynamics The Carnot engine is an ideal system which turns out to have the maximum possible efficiency: If TH is the hottest temperature in the engine, and TC is temperature outside the engine (in Kelvin), then the efficiency is: ec = (TH - TC )/ TH =W/QH This shows that it is not possible too have an efficiency of 100%. You always lose some energy into heating the environment.
  • 19. This can be restated as a version of the Second Law: No engine, working in a continuous cycle, can take heat from a reservoir at a single temperature and convert that heat completely into work.
  • 20. A restatement of the Second Law which turns out to be equivalent: Heat will not flow from a colder body to a hotter body unless some other process (which does work) is also involved. Another restatement to be discussed next time: The entropy of an isolated system can only increase or remain constant. Its entropy cannot decrease.
  • 21. According to the Second Law of Thermodynamics, heat will not flow from a colder body to a warmer body. 1. True 2. False
  • 22. According to the Second Law of Thermodynamics, heat will not flow from a colder body to a warmer body. 1. True 2. False
  • 23. A schematic representation of a heat engine. Heat is taken in at high temperatures, TH. Some heat is converted to work, and the remainder is released at a lower temperature, TC.
  • 24. The arrow widths depict the quantities of energy in the sample exercise in box 11.1.
  • 25. The efficiency of a heat engine is defined as e = W/ QH . Engines are more efficient if there is a large difference between the high temperature inside and the low temperature outside. For an ideal heat engine, ec = (TH - TC )/ TH