Paperwork Assignments fo 18&19 due next week Today 20.4-20.5 Problems for 18&19 Will finish chapter 20 Monday (Guest) Tuesday – Lab3 & Quiz3 Wed – Problems.

Slides:



Advertisements
Similar presentations
Chapter 24 Thermodynamics
Advertisements

Chapter 15. Work, Heat, and the First Law of Thermodynamics
PA2001: Time and Energy Thermodynamics 2 nd Law Cycles Efficiency Heat engines and refrigerators Entropy Kinetic theory of gasses Maxwell’s demon Tipler.
Kinetic Theory and Thermodynamics
Heat Engines. The Heat Engine  A heat engine typically uses energy provided in the form of heat to do work and then exhausts the heat which cannot.
Short Version : 18. Heat, Work, & First Law of Thermodynamics.
L 19 - Thermodynamics [4] Change of phase ice  water  steam
Physics 207: Lecture 27, Pg 1 Lecture 26Goals: Chapters 18, entropy and second law of thermodynamics Chapters 18, entropy and second law of thermodynamics.
Chapter 10 Thermodynamics
First Law of Thermodynamics Physics 102 Professor Lee Carkner Lecture 6 “of each the work shall become manifest, for the day shall declare it, because.
Chapter 18 The Second Law of Thermodynamics. Irreversible Processes Irreversible Processes: always found to proceed in one direction Examples: free expansion.
How much work is done by the gas in the cycle shown? A] 0 B] p 0 V 0 C] 2p 0 V 0 D] -2p 0 V 0 E] 4 p 0 V 0 How much total heat is added to the gas in the.
Dr Roger Bennett Rm. 23 Xtn Lecture 8.
Thermo & Stat Mech - Spring 2006 Class 5 1 Thermodynamics and Statistical Mechanics Heat Engines and Refrigerators.
The Second Law of Thermodynamics Physics 102 Professor Lee Carkner Lecture 7.
For the cyclic process shown, W is:D A] 0, because it’s a loop B] p 0 V 0 C] - p 0 V 0 D] 2 p 0 V 0 E] 6 p 0 V 0 For the cyclic process shown,  U is:
Copyright © 2009 Pearson Education, Inc. Lecture 11: Laws of Thermodynamics.
Physics 207: Lecture 26, Pg 1 Dec. 1. Physics 207: Lecture 26, Pg 2 Lecture 26, Dec. 1 Goals: Chapter 19 Chapter 19  Understand the relationship between.
Chapter Thermodynamics
1 L 19 - Thermodynamics [4] Change of phase ice  water  steam The Laws of Thermodynamics –The 1 st Law –The 2 nd Law –Applications Heat engines Refrigerators.
Warm up!  What is the difference between Isothermal and Adiabatic?  Describe the difference using the relationship between Internal energy(  U), heat(Q),
Chapter 15. ThermodynamicsThermodynamics  The name we give to the study of processes in which energy is transferred as heat and as work  There are 4.
Gas molar specific heats Mean kinetic energy of a gas molecule: If we have n moles of gas: Then molar specific heat at constant volume should be: What.
Paperwork HMWK deadline off by one hour –Everyone get some bonus? Guest Instructors –Monday – Chapter –Week After Mon & Fri That’s when the exam.
17.4 State Variables State variables describe the state of a system
THERMODYNAMICS Branch of science which deals with the processes involving heat and temperature inter conversion of heat and other forms of energy.
Chapter 15: Thermodynamics
Heat, Work, and Internal Energy Thermodynamic Processes.
Physics 101: Lecture 28, Pg 1 Physics 101: Lecture 28 Thermodynamics II l Today’s lecture will cover Textbook Chapter Final.
Thermodynamics … the study of how thermal energy can do work
Laws of Thermodynamics Thermal Physics, Lecture 4.
Heat Engines and The Carnot Cycle. First Statement of the Second Law of Thermodynamics The first statement of the second law is a statement from common.
Thermodynamics The First Law of Thermodynamics Thermal Processes that Utilize an Ideal Gas The Second Law of Thermodynamics Heat Engines Carnot’s Principle.
Review First Law. Work Work is energy transferred when directed motion is achieved against an external force. There are many types of forces available.
Thermal contact Two systems are in thermal (diathermic) contact, if they can exchange energy without performing macroscopic work. This form of energy.
Physics 101: Lecture 28, Pg 1 Physics 101: Lecture 28 Thermodynamics II l Today’s lecture will cover Textbook Chapter Final Check Final Exam.
Thermodynamics How Energy Is Transferred As Heat and Work Animation Courtesy of Louis Moore.
The internal energy of a substance can be changed in different ways. Work can transfer energy to a substance and increase its internal energy.
Thermodynamics Physics H Mr. Padilla Thermodynamics The study of heat and its transformation into mechanical energy. Foundation – Conservation of energy.
Chapter 13: Thermodynamics
Ch15 Thermodynamics Zeroth Law of Thermodynamics If two systems are in thermal equilibrium with a third system, then they are in thermal equilibrium with.
CHAPTER 15 Thermodynamics Thermodynamic Systems and Their Surroundings Thermodynamics is the branch of physics that is built upon the fundamental.
Physics 207: Lecture 27, Pg 1 Physics 207, Lecture 27, Dec. 6 l Agenda: Ch. 20, 1 st Law of Thermodynamics, Ch. 21  1 st Law of thermodynamics (  U=
Physics 1210/1310 Mechanics&Thermodynamics Lecture 39~40 Thermodynamics.
Chapter 11 Laws of Thermodynamics. Chapter 11 Objectives Internal energy vs heat Work done on or by a system Adiabatic process 1 st Law of Thermodynamics.
Thermodynamics Davidson College APSI Ideal Gas Equations P 1 V 1 / T 1 = P 2 V 2 / T 2 PV = n R T (using moles) P V = N k B T (using molecules)  P:
Chapter 12 Thermal Energy.
Thermodynamics Thermodynamics is a branch of physics concerned with heat and temperature and their relation to energy and work.
L 20 Thermodynamics [5] heat, work, and internal energy heat, work, and internal energy the 1 st law of thermodynamics the 1 st law of thermodynamics the.
Physics 101: Lecture 28, Pg 1 Physics 101: Lecture 28 Thermodynamics II l Today’s lecture will cover Textbook Chapter Final Check Final Exam.
Thermodynamic Processes
Chapter 23 The First Law of Thermodynamics. Thermal Physics Macroscopic Microscopic The Diffusion The Viscous The Transfer of Heat Exchange molecule T.
Chapter 11 Thermodynamics Heat and Work and Internal Energy o Heat = Work and therefore can be converted back and forth o Work  heat if work.
Physics 101: Lecture 26, Pg 1 Physics 101: Lecture 26 Thermodynamics II Final.
Thermodynamics II Thermodynamics II. THTH TCTC QHQH QCQC W HEAT ENGINE THTH TCTC QHQH QCQC W REFRIGERATOR system l system taken in closed cycle   U.
Lecture 26: Thermodynamics II l Heat Engines l Refrigerators l Entropy l 2 nd Law of Thermodynamics l Carnot Engines.
Chapter 12 Laws of Thermodynamics. Chapter 12 Objectives Internal energy vs heat Work done on or by a system Adiabatic process 1 st Law of Thermodynamics.
Chapter 20 - Thermodynamics A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.
Heat Engines A gasoline engine is a form of a heat engine, e.g. a 4-stroke engine INTAKE stroke: the piston descends from the top to the bottom of the.
Work in Thermodynamic Processes
THERMODYNAMICS THE NEXT STEP. THERMAL PROPERTIES OF MATTER STATE VARIABLES – DESCRIBE THE SUBSTANCE –PRESSURE –TEMPERATURE –VOLUME –QUANITY OF SUBSTANCE.
Chapter 20 Lecture 35: Entropy and the Second Law of Thermodynamics HW13 (problems):19.3, 19.10, 19.44, 19.75, 20.5, 20.18, 20.28,
Lecture 27Purdue University, Physics 2201 Lecture 27 Thermodynamics II Physics 220.
Engines—examples and efficiency
Introduction To Thermodynamics
Mechanics & Thermodynamics
B.Sc.I, Paper II ( I Semester)
Engines—examples and efficiency
Engines—examples and efficiency
Presentation transcript:

Paperwork Assignments fo 18&19 due next week Today Problems for 18&19 Will finish chapter 20 Monday (Guest) Tuesday – Lab3 & Quiz3 Wed – Problems for Ch. 20 Fri – Ch.21 (Guest) Exam Following Friday

Engines = Cyclic Processes Initial State = Final State Q =  U + W What does this imply about  U?  U = U F – U 0 = U – U = 0 Engine returns to starting state (p,V,T) But Heat can enter system (Fuel, Energy In) Work is Done (Energy Out) –Q = 0 + W

Engine QHQH QCQC Work Some Energy tapped to do work. Some Lost. Not Path Independent means non-conservative! Heat not a liquid, but think H 2 0 Tower

Perpetual Motion? QHQH QCQC Work Why must some heat (energy) be lost to cold side?

WaterWheel Converts Water Flow (H20 KE) to Usable Energy (Wheel KE)

WaterWheel – on a H20 Tower Tower Reservoir - Higher Graviational PE Ground - Lower Graviational PE Not all H20 Energy Used Some flows to ground Could convert all?

WaterWheel – on a H20 Tower Tower Reservoir - Higher Graviational PE Stop flow down just means higher “ground” H20 KE less, also stops wheel from turning Same Problem with heat Need a “sink” to direct flow

Perpetual Motion? QHQH QCQC Work Why must some heat (energy) be lost to cold side? No cold sink, no heat flow! [Warning heat is NOT a liquid]

What Happens if I Reverse W? QHQH QCQC Work Work Entering System instead of Work being done by system. dQ = dU + W (Here, W <1)

What Happens if I Reverse W? QHQH QCQC Work Work Entering System instead of Work being done by system. dQ = dU + W (Here, W <1) Can Make dQ negative (Flow backwards)

Makes cold side colder? At least it removes heat energy QHQH QCQC Work |Q H |+|W|=|Q C | Q C is heat taken out of cold side (what you want done) W is work it takes to do this Q H is heat that goes into hot side (Q H >Q C ) Fridge exhaust - RT, Hotter or Colder?

Refrigerator QHQH QCQC Work Fridges have K, like efficiency:

Efficiency If 100% efficient –Perpetual Motion (patents everwhere…) Engines – Not all Heat converted to work Fridge – Need some work to force heat to flow from cold object to hot object Statements = 2 nd law of thermodynamics –No Free Lunch?

?’s

Choose 1 If you increase the temperature of an ideal gas? –its volume must increase –its pressure must increase –the speed of its molecules must increase –the average distance a molecule travels between collisions must increase –the average time between collisions of its molecules must increase. Answer – speed. Implications of each?

Choose 1? Which of the following is FALSE? –A dumbbell molecule like O2 is considered to have eight degrees of freedom. –The average kinetic energy of a molecule moving in three dimensions is always 3kT/2. –Rotational motion, as well as translational motion, can contribute to the heat capacities of gases. –The average kinetic energy associated with each degree of freedom of a molecule is 1/2kT. –Vibrational motion, as well as translational motion, can contribute to the heat capacities of gases. 5 not 8. Remainder?

Choose 1 Q =  U + W. Which of the following statements is FALSE? –W is the work done by the system, and not on the system. –Q can be positive or negative. –This is called the law of conservation of energy. –This is called the First Law of Thermodynamics. – It follows that since Q and W are path dependent, then  U must also be path dependent. Last One – Internal Energy depends only on Temp for ideal gas (+ KE, PE’s, etc… for others)

Choose Any Which of the following are true statements about an ideal gas? (What is isochoric?) –During an isochoric process, the change in the internal energy of the gas is exactly equal to the amount of heat that goes into (or out of) the gas. –During an isothermal process, no heat enters or leaves the gas. –During an isochoric process, no work is done on or by the gas. –During an isothermal process, the temperature of the gas does not change. –During an adiabatic process, the temperature of the gas does not change. Only 1 st one. What about 3 rd one?

Choose any? Which of the following is an accurate statement? –A typical gasoline engine has an efficiency of about 2%. –An important distinction between the Diesel cycle and the Otto cycle is that for the Diesel cycle high efficiencies may be obtained with low compression ratios. –An important distinction between the Diesel cycle and the Otto cycle is that there is no fuel in the cylinder at the beginning of the compression stroke and no spark plug is used. –Because a Diesel engine requires no fuel ignition system, Diesel engines tend to be lighter and easier to start than a comparable gasoline engine. –The efficiency of the Otto cycle does not depend on the compression ratio. Middle: Implications of others?

Friday Return Quiz 1 Cover one problem each from 18,19,20 –Or at least 18&19