The First Law of Thermodynamics
|
|
- Rodger Hampton
- 5 years ago
- Views:
Transcription
1 Chapter 9 The First Law of Thermodynamics Topics for Chapter 9 I. First Law of Thermodynamics Internal energy, concept of state variables Difference between Work and Heat II. Examine various types of thermodynamic processes: Constant volume Constant pressure PowerPoint Lectures for University Physics, Twelfth Edition Hugh D. Young and Roger A. Freedman Lectures by James Pazun Modified by P. Lam 8_6_00 Constant temperature Zero heat transfer - adiabatic process First Law of Thermodynamics st Law of Thermodynamics is a statement about conservation of energy and it categorizes the method of energy transfer into two basic forms: work (W) and heat (Q). The internal energy of a system (U) (for a container of ideal gas, U =kinetic energy of the molecules) can be changed by transferring heat to and from the environment and/or performing work on or by the environment. U f!u i = "U = Q - W Positive Q # heat input to the system from the environment Negative Q # heat output from the system to the environment Positive W # work done by the system on the environment Negative W # work done on the system by the environment Note : The combined energy of the system and the environment is conserved; energy merely transferred to and from system and environment. Internal energy, concept of state variables Internal energy = energy of the system with respect to the center of mass reference; we are not concerned with the situation where the entire system is moving. Example: The internal energy of n moles of monatomic ideal gas is the kinetic energy of the gas with respect to the center of mass reference frame and it is U=3/nRT=3/PV. U is called a state variable because once the state of the system is specified, such as the number of moles and the temperature or pressure and volume, U has an unique value, that is U is function U(n,T) or U(P,V). The change of a state variable does not depend on how the system goes from the initial to the final state. For example, you can add heat or do work to change the system s from T i to T f, then ΔU=3/nRT f -3/nRT i no matter what methods was used.
2 Work = pressure x change of volume Consider the work done by the system (e.g. a gas) on the environment. W = Fdx = PAdx = PdV If dx > 0! dv > 0! volume expands! system does positive work on the enviroment According to the first Law : load "U = Q - W! positive work on the evironment lowers the internal energy of the system If dx < 0! compression, then W < 0 and the internal energy increases. (see picture to the right) Work done by a varying pressure is given by integration V f W =! P(V )dv V i Note : ()The direction of the path (indicated by an arrow) determines whether W is positive or negative. () W depends on the path going from initial to final state (see next slide) " W is NOT a state variable; there is NO such thing as #W = W f $W i Work done depends on the path. Shown below 3 different paths going from state to state ; the work done are different. What is energy transfer by heat? Imagine heating water with a burner. Energy is transferred from the fast moving molecules in the flame to the slow moving molecules in the pot and then to the slow moving molecules in the water by means of random collisions. At the microscopic level, the molecules in the flame are doing work (force x displacement) on the molecules in the pot which in turns are doing work on the water molecules. At this level, there no different between this method of energy transfer and the one described previously by pushing a piston. However, on the macroscopic level, work done by pushing a piston is done uniformly by changing the volume while heat can be added/removed without changing the volume. The first Law of thermodynamics treat work and heat on equal footing. The second Law of thermodynamics will treat heat differently than work.
3 II. Examine various types of thermodynamic processes Constant volume - isochoric process Process from to 4 is an isochoric process. = 3x0 5 N m,p =x0 5 N m =0! m 3,n = moles Evaluate "U,W,Q, and "T for the process to 4. Since there is no volume change! W = " PdV = 0 that is why it is called "isochoric".! #U = Q We won't be able to say anything further unless we know something about the system. Let the system be n moles of monatomic ideal gas, then U = 3 nrt = 3 PV, #U = U f = 3 P V $ 3 P = negative = $3kJ (OR use #U = U f = 3 nrt 4 $ 3 nrt = negative;t 4 = 60K,T =80K)! In this process, heat is released at constant volume to lower the pressure of the gas (lower the temperature of the gas) II. Examine various types of thermodynamic processes Constant pressure - isobaric process Process from to 3 is an isobaric process. W =! PdV = P ( - ) = +6kJ " #U = Q - P ( - ) We won't be able to say anything further unless we know something about the system. Let the system be n moles of monatomic ideal gas, then U = 3 nrt = 3 PV, = 3x0 N 5 m,p N #U = U f = 3 PV $ 3 PV = 3 =x05 m P (V $V ) = +9kJ =0! m 3, Evaluate "U,W,Q,and "T (OR use #U = U f = 3 nr(t $ T ) 3 " Q = #U +W = 5 P ( $ ) = 5 nr(t 3 $ T ) =5kJ In this process, heat is must be added to keep the pressure constant while doing work on the environment. II. Examine various types of thermodynamic processes Constant temperature - isothermal process Let process from to be an isothermal process. In this case, we won't be able to say anything at all unless we know something about the system (such as P vs V curve for T = constant). Let the system be n moles of monatomic ideal gas, then P = nrt V, T = constant = T = T =80K W =! Pd =! nrt V d = nrt ln = 3ln3 (kj) = 3x0 N 5 m,p =x0 N 5 m U = 3 nrt " #U = 3 nr#t = 0 =0! m 3, Evaluate "U,W,Q,and "T (Note : isothermal strictly means constant T; for ideal gas it also implies constant U, not true for real gases) Q = #U +W = W In this process, heat is must added to keep the temperature constant while doing work on the environment. Aside - Re-enforce the concept of state variables N = 3x0 5 m,p N =x05 m =0! m 3, of monatomic ideal gas Evaluate "U,W,Q,and "T for the path - > 3- > and compare with the isothermal process - > 3
4 II. Examine various types of thermodyanmic processes No heat transfer (Q=0) - adiabatic process Let process from to be an adiabtic process. All we can say is!u = Q - W = -W We won't be able to say anything further unless we know something about the system (such as P vs V curve when Q = 0). Let the system be n moles of monatomic ideal gas, then P = nrt V, however T " constant, T =80K nrt W = # Pd = V dv V # " nrt ln Let P = 3x0 N 5 m,p =??? because T is also a function of V for this path. =0! m 3, Evaluate "U,W,Q,and "T Since W = positive (see direction of arrow => expansion) $!U = Q - W = -W = negative $ T decreases along the path. For monatomic ideal gas, we can use!u = 3 nr ( T % T ) = %W but need to know T (see next slide) Adiabatic PV curve for monatomic ideal gas In an adiabatic process, no heat is transferred from system and Derive the adiabatic PV curve for an ideal gas. surroundings. = P a = 3x0 5 N m,p = P b =??? = V a =0! m 3, = V b Evaluate "U,W,Q,and "T Use differential form of the st Law : du = dq - dw = -dw = -PdV For ideal gas : U = 3 nrt = 3 PV! du = 3 PdV + 3 VdP! 3 PdV + 3 VdP = "PdV! 5 PdV = " 3 VdP! 5 dv V = " 3 dp P! 5 lnv V = " 3 lnp P P! 5 ln V = " 3 ln P P! V 5 / % ( = P "3 / % ( = P 3 / % ( $ ' $ P ' $ P ' # V! P = P & # V & % ( in particular : P = P % ( $ ' = 3x0 5 5/3 N % $ 3 ( ' m Use P = nrt / 3 / 3 V! T = T # & # V % (! T = T & % ( $ ' =80 /3 % $ 3 ( K ' V # V W = ) PdV = & 5 / ) P % ( dv = P V 3 " 3 V * V - " / 3 +,. / = 3 * P " / 3 -, % ( / +, $ './ = 3 P " 3 P = 3 nr ( T " T ) = "0U Compare the four processes on a PV diagram Notice the subtle differences for each curve in Figure 9.6. Cyclic process - complete cycle Cyclic process :! 3!! 4! No matter what the substance is, "U complete cycle = 0 because it comes back to the same state "U = U # U 4
5 Relating heat capacities at constant volume and pressure Compare molar heat capacities, c V and c P, for monatomic ideal gas Constant volume (W = 0) : Q =!U = 3 nr!t " c V = 3 R Constant pressure : W = -P!V " Q =!U +W =!U +P!V PV = nrt " P!V = nr!t (for constant P) " Q = 3 nr!t + nr!t = n(c + R)!T v " c p = c v + R It requires more heat to raise the temperature at constant pressure vs constant volume because some of the heat is spent in doing work, expanding the volume. Measuring heat capacities Heat capacities may be measured at constant volume in a fairly complex process using a bomb calorimeter. Heat capacities may be measured at constant pressure using equipment as simple as a coffee cup. For solids, c p # c v, because the volume does not expand as easily as a gas. Nonetheless c p is always greater than c v. Heat capacities tabulated for selected gasses J c p = c v + R; R ~ 8.3 mol K monatomic : c v = 3 R! c p = 5 R! c p c v = 5 3 ".67 diatomic : c v = 5 R (without vibration)! c p = 7 R! c p c v = 7 5 ".4 5
Chapter 19 The First Law of Thermodynamics
Chapter 19 The First Law of Thermodynamics The first law of thermodynamics is an extension of the principle of conservation of energy. It includes the transfer of both mechanical and thermal energy. First
More informationThe First Law of Thermodynamics
Chapter 19 The First Law of Thermodynamics PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman Lectures by Wayne Anderson Goals for Chapter 19 To represent
More informationLecture 5. PHYC 161 Fall 2016
Lecture 5 PHYC 161 Fall 2016 Ch. 19 First Law of Thermodynamics In a thermodynamic process, changes occur in the state of the system. Careful of signs! Q is positive when heat flows into a system. W is
More informationEnthalpy and Adiabatic Changes
Enthalpy and Adiabatic Changes Chapter 2 of Atkins: The First Law: Concepts Sections 2.5-2.6 of Atkins (7th & 8th editions) Enthalpy Definition of Enthalpy Measurement of Enthalpy Variation of Enthalpy
More informationChapter 19 The First Law of Thermodynamics
Chapter 19 The First Law of Thermodynamics Lecture by Dr. Hebin Li Assignment Due at 11:59pm on Sunday, December 7 HW set on Masteringphysics.com Final exam: Time: 2:15pm~4:15pm, Monday, December 8. Location:
More informationThermal Properties of Matter (Microscopic models)
Chapter 18 Thermal Properties of Matter (Microscopic models) PowerPoint Lectures for University Physics, Twelfth Edition Hugh D. Young and Roger A. Freedman Lectures by James Pazun Modified by P. Lam 6_18_2012
More informationSpecific Heat of Diatomic Gases and. The Adiabatic Process
Specific Heat of Diatomic Gases and Solids The Adiabatic Process Ron Reifenberger Birck Nanotechnology Center Purdue University February 22, 2012 Lecture 7 1 Specific Heat for Solids and Diatomic i Gasses
More informationChapter 15 Thermal Properties of Matter
Chapter 15 Thermal Properties of Matter To understand the mole and Avogadro's number. To understand equations of state. To study the kinetic theory of ideal gas. To understand heat capacity. To learn and
More informationThe first law of thermodynamics continued
Lecture 7 The first law of thermodynamics continued Pre-reading: 19.5 Where we are The pressure p, volume V, and temperature T are related by an equation of state. For an ideal gas, pv = nrt = NkT For
More informationLecture 7: Kinetic Theory of Gases, Part 2. ! = mn v x
Lecture 7: Kinetic Theory of Gases, Part 2 Last lecture, we began to explore the behavior of an ideal gas in terms of the molecules in it We found that the pressure of the gas was: P = N 2 mv x,i! = mn
More informationChapter 3 - First Law of Thermodynamics
Chapter 3 - dynamics The ideal gas law is a combination of three intuitive relationships between pressure, volume, temp and moles. David J. Starling Penn State Hazleton Fall 2013 When a gas expands, it
More informationChemistry. Lecture 10 Maxwell Relations. NC State University
Chemistry Lecture 10 Maxwell Relations NC State University Thermodynamic state functions expressed in differential form We have seen that the internal energy is conserved and depends on mechanical (dw)
More informationUnit 05 Kinetic Theory of Gases
Unit 05 Kinetic Theory of Gases Unit Concepts: A) A bit more about temperature B) Ideal Gas Law C) Molar specific heats D) Using them all Unit 05 Kinetic Theory, Slide 1 Temperature and Velocity Recall:
More informationChapter 14 Kinetic Theory
Chapter 14 Kinetic Theory Kinetic Theory of Gases A remarkable triumph of molecular theory was showing that the macroscopic properties of an ideal gas are related to the molecular properties. This is the
More informationInternal Energy (example)
Internal Energy (example) A bucket of water KEs: translational: rotational: vibrational: PEs: within molecules: between molecules: @ rest on the table molecular bonds dipole-dipole interactions Internal
More informationSpeed Distribution at CONSTANT Temperature is given by the Maxwell Boltzmann Speed Distribution
Temperature ~ Average KE of each particle Particles have different speeds Gas Particles are in constant RANDOM motion Average KE of each particle is: 3/2 kt Pressure is due to momentum transfer Speed Distribution
More informationU = 4.18 J if we heat 1.0 g of water through 1 C. U = 4.18 J if we cool 1.0 g of water through 1 C.
CHAPER LECURE NOES he First Law of hermodynamics: he simplest statement of the First Law is as follows: U = q + w. Here U is the internal energy of the system, q is the heat and w is the work. CONVENIONS
More informationMore Thermodynamics. Specific Specific Heats of a Gas Equipartition of Energy Reversible and Irreversible Processes
More Thermodynamics Specific Specific Heats of a Gas Equipartition of Energy Reversible and Irreversible Processes Carnot Cycle Efficiency of Engines Entropy More Thermodynamics 1 Specific Heat of Gases
More informationCh. 19: The Kinetic Theory of Gases
Ch. 19: The Kinetic Theory of Gases In this chapter we consider the physics of gases. If the atoms or molecules that make up a gas collide with the walls of their container, they exert a pressure p on
More informationPhysics Fall Mechanics, Thermodynamics, Waves, Fluids. Lecture 32: Heat and Work II. Slide 32-1
Physics 1501 Fall 2008 Mechanics, Thermodynamics, Waves, Fluids Lecture 32: Heat and Work II Slide 32-1 Recap: the first law of thermodynamics Two ways to raise temperature: Thermally: flow of heat Energy
More informationThe goal of thermodynamics is to understand how heat can be converted to work. Not all the heat energy can be converted to mechanical energy
Thermodynamics The goal of thermodynamics is to understand how heat can be converted to work Main lesson: Not all the heat energy can be converted to mechanical energy This is because heat energy comes
More informationWork and heat. Expansion Work. Heat Transactions. Chapter 2 of Atkins: The First Law: Concepts. Sections of Atkins
Work and heat Chapter 2 of Atkins: The First Law: Concepts Sections 2.3-2.4 of Atkins Expansion Work General Expression for Work Free Expansion Expansion Against Constant Pressure Reversible Expansion
More informationPhysics 53. Thermal Physics 1. Statistics are like a bikini. What they reveal is suggestive; what they conceal is vital.
Physics 53 Thermal Physics 1 Statistics are like a bikini. What they reveal is suggestive; what they conceal is vital. Arthur Koestler Overview In the following sections we will treat macroscopic systems
More informationHeat and Thermodynamics. February. 2, Solution of Recitation 2. Consider the first case when air is allowed to expand isothermally.
Heat and Thermodynamics. February., 0 Solution of Recitation Answer : We have given that, Initial volume of air = = 0.4 m 3 Initial pressure of air = P = 04 kpa = 04 0 3 Pa Final pressure of air = P =
More informationChapter 19. First Law of Thermodynamics. Dr. Armen Kocharian, 04/04/05
Chapter 19 First Law of Thermodynamics Dr. Armen Kocharian, 04/04/05 Heat and Work Work during volume change Work in Thermodynamics Work can be done on a deformable system, such as a gas Consider a cylinder
More informationIntroduction to thermodynamics
Chapter 6 Introduction to thermodynamics Topics First law of thermodynamics Definitions of internal energy and work done, leading to du = dq + dw Heat capacities, C p = C V + R Reversible and irreversible
More informationProblem: Calculate the entropy change that results from mixing 54.0 g of water at 280 K with 27.0 g of water at 360 K in a vessel whose walls are
Problem: Calculate the entropy change that results from mixing 54.0 g of water at 280 K with 27.0 g of water at 360 K in a vessel whose walls are perfectly insulated from the surroundings. Is this a spontaneous
More informationPhysics 4C Chapter 19: The Kinetic Theory of Gases
Physics 4C Chapter 19: The Kinetic Theory of Gases Whether you think you can or think you can t, you re usually right. Henry Ford The only thing in life that is achieved without effort is failure. Source
More informationWork and heat. Heat Transactions Calorimetry Heat Capacity. Last updated: Sept. 24, 2018, slide 1
Work and heat Chapter 2 of Atkins: The First Law: Concepts Sections 2.3-2.4 of Atkins (7th, 8th & 9th editions) Section 2.1 of Atkins (10th, 11th editions) Expansion Work General Expression for Work Free
More informationADIABATIC PROCESS Q = 0
THE KINETIC THEORY OF GASES Mono-atomic Fig.1 1 3 Average kinetic energy of a single particle Fig.2 INTERNAL ENERGY U and EQUATION OF STATE For a mono-atomic gas, we will assume that the total energy
More informationCHEM Thermodynamics. Work. There are two ways to change the internal energy of a system:
There are two ways to change the internal energy of a system: Thermodynamics Work 1. By flow of heat, q Heat is the transfer of thermal energy between and the surroundings 2. By doing work, w Work can
More information16-1. Sections Covered in the Text: Chapter 17. Example Problem 16-1 Estimating the Thermal Energy of a gas. Energy Revisited
Heat and Work Sections Covered in the Text: Chapter 17 In this note we continue our study of matter in bulk. Here we investigate the connection between work and heat in bulk matter. Work and heat are both
More information(Heat capacity c is also called specific heat) this means that the heat capacity number c for water is 1 calorie/gram-k.
Lecture 23: Ideal Gas Law and The First Law of Thermodynamics 1 (REVIEW) Chapter 17: Heat Transfer Origin of the calorie unit A few hundred years ago when people were investigating heat and temperature
More informationApplied Thermodynamics for Marine Systems Prof. P. K. Das Department of Mechanical Engineering Indian Institute of Technology, Kharagpur
Applied Thermodynamics for Marine Systems Prof. P. K. Das Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Lecture - 8 Introduction to Vapour Power Cycle Today, we will continue
More informationPhysics 2 week 7. Chapter 3 The Kinetic Theory of Gases
Physics week 7 Chapter 3 The Kinetic Theory of Gases 3.1. Ideal Gases 3.1.1. Experimental Laws and the Equation of State 3.1.. Molecular Model of an Ideal Gas 3.. Mean Free Path 3.3. The Boltzmann Distribution
More informationHence. The second law describes the direction of energy transfer in spontaneous processes
* Heat and Work The first law of thermodynamics states that: Although energy has many forms, the total quantity of energy is constant. When energy disappears in one form, it appears simultaneously in other
More informationWhat is thermodynamics? and what can it do for us?
What is thermodynamics? and what can it do for us? The overall goal of thermodynamics is to describe what happens to a system (anything of interest) when we change the variables that characterized the
More informationSpeed Distribution at CONSTANT Temperature is given by the Maxwell Boltzmann Speed Distribution
Temperature ~ Average KE of each particle Particles have different speeds Gas Particles are in constant RANDOM motion Average KE of each particle is: 3/2 kt Pressure is due to momentum transfer Speed Distribution
More informationLecture 7, 8 and 9 : Thermodynamic process by: Asst. lect. Karrar Al-Mansoori CONTENTS. 7) Thermodynamic process, path and cycle 2
CONTENTS Topics pages 7) Thermodynamic process, path and cycle 8) Reversibility and irreversibility 4 9) Thermodynamic processes and calculation of work 5 9.: Constant pressure process or isobaric process
More information6) BTW: Your TA has Exam3. It should have been returned to you on Nov 16 (Mon) at Recitation if you
Chap. 15: pv = nrt Mole and Avogadro s number. Equations of state. Kinetic theory of an ideal gas. Heat capacities. First Law of Thermodynamics. Thermodynamic processes. Properties of an ideal gas. 1 3
More informationChapter 18 Heat and the First Law of Thermodynamics
Chapter 18 Heat and the First Law of Thermodynamics Heat is the transfer of energy due to the difference in temperature. The internal energy is the total energy of the object in its centerofmass reference
More informationMP203 Statistical and Thermal Physics. Jon-Ivar Skullerud and James Smith
MP203 Statistical and Thermal Physics Jon-Ivar Skullerud and James Smith October 27, 2017 1 Contents 1 Introduction 3 1.1 Temperature and thermal equilibrium.................... 4 1.1.1 The zeroth law
More informationFinal Review Solutions
Final Review Solutions Jared Pagett November 30, 206 Gassed. Rapid Fire. We assume several things when maing the ideal gas approximation. With inetic molecular theory, we model gas molecules as point particles
More informationPhase Changes and Latent Heat
Review Questions Why can a person remove a piece of dry aluminum foil from a hot oven with bare fingers without getting burned, yet will be burned doing so if the foil is wet. Equal quantities of alcohol
More informationFirst Law of Thermo.
Quiz 8, MONDAY Please send me an email ASAP if you are away Monday, Nov. 25. You can take the quiz on Friday Nov 22, during your usual time. (You ll have to miss the Friday lecture). First Law of Thermo.
More information19-9 Adiabatic Expansion of an Ideal Gas
19-9 Adiabatic Expansion of an Ideal Gas Learning Objectives 19.44 On a p-v diagram, sketch an adiabatic expansion (or contraction) and identify that there is no heat exchange Q with the environment. 19.45
More information12.1 Work in Thermodynamic Processes
Name APPH7_Notes3key Page 1 of 6 AP Physics Date Notes: Thermodynamics 12.1 Work in Thermodynamic Processes First Law of Thermodynamics The First Law of Thermodynamics tells us that the internal energy
More informationThermodynamic Processes and Thermochemistry
General Chemistry Thermodynamic Processes and Thermochemistry 박준원교수 ( 포항공과대학교화학과 ) 이번시간에는! Systems, states, and processes The first law of thermodynamics: internal energy, work, and heat Heat capacity,
More informationOutline of the Course
Outline of the Course 1) Review and Definitions 2) Molecules and their Energies 3) 1 st Law of Thermodynamics 4) 2 nd Law of Thermodynamics 5) Gibbs Free Energy 6) Phase Diagrams and REAL Phenomena 7)
More informationWeek 5. Energy Analysis of Closed Systems. GENESYS Laboratory
Week 5. Energy Analysis of Closed Systems Objectives 1. Examine the moving boundary work or PdV work commonly encountered in reciprocating devices such as automotive engines and compressors 2. Identify
More informationNOTE: Only CHANGE in internal energy matters
The First Law of Thermodynamics The First Law of Thermodynamics is a special case of the Law of Conservation of Energy It takes into account changes in internal energy and energy transfers by heat and
More informationCHAPTER 17 WORK, HEAT, & FIRST LAW OF THERMODYNAMICS
CHAPTER 17 WORK, HEAT, and the FIRST LAW OF THERMODYNAMICS In this chapter, we will examine various thermal properties of matter, as well as several mechanisms by which energy can be transferred to and
More information2/18/2019. Ideal-Gas Processes. Thermodynamics systems. Thermodynamics systems
Thermodynamics systems A thermodynamic system is any collection of objects that may exchange energy with its surroundings. The popcorn in the pot is a thermodynamic system. In the thermodynamic process
More informationThermodynamics systems
Thermodynamics systems A thermodynamic system is any collection of objects that may exchange energy with its surroundings. The popcorn in the pot is a thermodynamic system. In the thermodynamic process
More informationUNIVERSITY OF SOUTHAMPTON
UNIVERSITY OF SOUTHAMPTON PHYS1013W1 SEMESTER 2 EXAMINATION 2014-2015 ENERGY AND MATTER Duration: 120 MINS (2 hours) This paper contains 8 questions. Answers to Section A and Section B must be in separate
More informationMatter exchange - type of wall Yes - permeable - absence of wall. Energy exchange - type of wall. - diathermic - moving wall. Yes
I. The concept of work, expansion and additional (useful) work. II. The concept of heat. III. Definition of internal energy and its molecular interpretation. I. Different forms of the first law of thermodynamics..
More informationGeneral Physics I (aka PHYS 2013)
General Physics I (aka PHYS 2013) PROF. VANCHURIN (AKA VITALY) University of Minnesota, Duluth (aka UMD) OUTLINE CHAPTER 12 CHAPTER 19 REVIEW CHAPTER 12: FLUID MECHANICS Section 12.1: Density Section 12.2:
More informationPhysics 121, April 24. Heat and the First Law of Thermodynamics. Department of Physics and Astronomy, University of Rochester
Physics 121, April 24. Heat and the First Law of Thermodynamics. Physics 121. April 24, 2008. Course Information Topics to be discussed today: Heat First law of thermodynamics Second law of thermodynamics
More informationPhysics 121, April 24. Heat and the First Law of Thermodynamics. Physics 121. April 24, Physics 121. April 24, Course Information
Physics 121, April 24. Heat and the First Law of Thermodynamics. Physics 121. April 24, 2008. Course Information Topics to be discussed today: Heat First law of thermodynamics Second law of thermodynamics
More informationHonors Physics. Notes Nov 16, 20 Heat. Persans 1
Honors Physics Notes Nov 16, 20 Heat Persans 1 Properties of solids Persans 2 Persans 3 Vibrations of atoms in crystalline solids Assuming only nearest neighbor interactions (+Hooke's law) F = C( u! u
More informationThe First Law of Thermodynamics. Lecture 5
The First Law of Thermodynamics Lecture 5 First Law of Thermodynamics Overlooks the fine microscopic details (which in many cases are irrelevant). Describes the conversion of one form of energy (heat)
More informationEQUILIBRIUM IN CHEMICAL REACTIONS
EQUILIBRIUM IN CHEMICAL REACTIONS CHAPTER 12 Thermodynamic Processes and Thermochemistry CHAPTER 13 Spontaneous Processes and Thermodynamic Equilibrium CHAPTER 14 Chemical Equilibrium CHAPTER 15 Acid-Base
More informationLecture. Polymer Thermodynamics 0331 L First and Second Law of Thermodynamics
1 Prof. Dr. rer. nat. habil. S. Enders Faculty III for Process Science Institute of Chemical Engineering Department of hermodynamics Lecture Polymer hermodynamics 0331 L 337 2.1. First Law of hermodynamics
More informationHeat What is heat? Work = 2. PdV 1
eat What is heat? eat (Q) is the flow or transfer of energy from one system to another Often referred to as heat flow or heat transfer Requires that one system must be at a higher temperature than the
More informationThe Kinetic Theory of Gases
PHYS102 Previous Exam Problems CHAPTER 19 The Kinetic Theory of Gases Ideal gas RMS speed Internal energy Isothermal process Isobaric process Isochoric process Adiabatic process General process 1. Figure
More informationFor more info visit
Basic Terminology: Terms System Open System Closed System Isolated system Surroundings Boundary State variables State Functions Intensive properties Extensive properties Process Isothermal process Isobaric
More informationPhysics 2B Chapter 17 Notes - First Law of Thermo Spring 2018
Internal Energy o a Gas Work Done by a Gas Special Processes The First Law o Thermodynamics p Diagrams The First Law o Thermodynamics is all about the energy o a gas: how much energy does the gas possess,
More informationChapter 19: The Kinetic Theory of Gases Questions and Example Problems
Chapter 9: The Kinetic Theory of Gases Questions and Example Problems N M V f N M Vo sam n pv nrt Nk T W nrt ln B A molar nmv RT k T rms B p v K k T λ rms avg B V M m πd N/V Q nc T Q nc T C C + R E nc
More informationChapter 15: Thermal Properties of Matter
Chapter 15 Lecture Chapter 15: Thermal Properties of Matter Goals for Chapter 15 To understand and learn to use the mole and Avogadro's number. To see applications for equations of state. To study the
More informationThermodynamic Variables and Relations
MME 231: Lecture 10 Thermodynamic Variables and Relations A. K. M. B. Rashid Professor, Department of MME BUET, Dhaka Today s Topics Thermodynamic relations derived from the Laws of Thermodynamics Definitions
More informationChemistry 163B Winter Lectures 2-3. Heat and Work
Chemistry 163B Winter 2014 Lectures 2-3 Heat and Work Chemistry 163B reserve books 2014 (S&E Library) handout #7 heat capacity (E&R section 2.5) -d q C heat capacity 1 J K dt the amount of heat requires
More informationHomework: 13, 14, 18, 20, 24 (p )
Homework: 13, 14, 18, 0, 4 (p. 531-53) 13. A sample of an ideal gas is taken through the cyclic process abca shown in the figure below; at point a, T=00 K. (a) How many moles of gas are in the sample?
More informationPhysics 231. Topic 14: Laws of Thermodynamics. Alex Brown Dec MSU Physics 231 Fall
Physics 231 Topic 14: Laws of Thermodynamics Alex Brown Dec 7-11 2015 MSU Physics 231 Fall 2015 1 8 th 10 pm correction for 3 rd exam 9 th 10 pm attitude survey (1% for participation) 10 th 10 pm concept
More informationTemperature Thermal Expansion Ideal Gas Law Kinetic Theory Heat Heat Transfer Phase Changes Specific Heat Calorimetry Heat Engines
Temperature Thermal Expansion Ideal Gas Law Kinetic Theory Heat Heat Transfer Phase Changes Specific Heat Calorimetry Heat Engines Zeroeth Law Two systems individually in thermal equilibrium with a third
More informationRelationships between WORK, HEAT, and ENERGY. Consider a force, F, acting on a block sliding on a frictionless surface. x 2
Relationships between WORK, HEAT, and ENERGY Consider a force, F, acting on a block sliding on a frictionless surface x x M F x Frictionless surface M dv v dt M dv dt v F F F ; v mass velocity in x direction
More informationMonday, October 21, 13. Copyright 2009 Pearson Education, Inc.
Lecture 4 1st Law of Thermodynamics (sections 19-4 to 19-9) 19-4 Calorimetry 19-5 Latent Heat 19-6 The 1st Law of Thermodynamics 19-7 Gas: Calculating the Work 19-8 Molar Specific Heats 19-9 Adiabatic
More information, is placed in thermal contact with object B, with mass m, specific heat c B. and initially at temperature T B
4C_PLC http://www.cabrillo.edu/~jmccullough/physics4c/files/4c_plc/4c_plc.htm Page 1 of 8 /6/201 1. The heat capacity at constant volume and the heat capacity at constant pressure have different values
More informationThermodynamics General
Thermodynamics General Lecture 5 Second Law and Entropy (Read pages 587-6; 68-63 Physics for Scientists and Engineers (Third Edition) by Serway) Review: The first law of thermodynamics tells us the energy
More informationThermodynamics part III.
Thermodynamics part III. a.) Fenomenological thermodynamics macroscopic description b.) Molecular thermodynamics microscopic description b1.) kinetical gas theory b2.) statistical thermodynamics Laws of
More informationThermodynamics 1 Lecture Note 2
Thermodynamics 1 Lecture Note 2 March 20, 2015 Kwang Kim Yonsei University kbkim@yonsei.ac.kr 39 8 7 34 53 Y O N Se I 88.91 16.00 14.01 78.96 126.9 Physical Chemistry Chemistry is the study of Matter and
More informationIrreversible Processes
Lecture 15 Heat Engines Review & Examples p p b b Hot reservoir at T h p a a c adiabats Heat leak Heat pump Q h Q c W d V 1 V 2 V Cold reservoir at T c Lecture 15, p 1 Irreversible Processes Entropy-increasing
More informationTODAY 0. Why H = q (if p ext =p=constant and no useful work) 1. Constant Pressure Heat Capacity (what we usually use)
361 Lec 7 Fri 9sep15 TODAY 0. Why H = q (if p ext =p=constant and no useful work) 1. Constant Pressure Heat Capacity (what we usually use) 2. Heats of Chemical Reactions: r H (mechanics of obtaining from
More informationChapter 19 Entropy Pearson Education, Inc. Slide 20-1
Chapter 19 Entropy Slide 20-1 Ch 19 & 20 material What to focus on? Just put out some practice problems for Ch. 19/20 Ideal gas how to find P/V/T changes. How to calculate energy required for a given T
More informationConservation of Energy
Conservation of Energy Energy can neither by created nor destroyed, but only transferred from one system to another and transformed from one form to another. Conservation of Energy Consider at a gas in
More informationStuff. ---Tonight: Lecture 3 July Assignment 1 has been posted. ---Presentation Assignment on Friday.
Stuff ---Tonight: Lecture 3 July 0 ---Assignment 1 has been posted. Work from gravitational forces: h F gravity dx = h 0 0 mgh mg dx Where m (kg) and g is gravitational constant 9.8 m/s ---Presentation
More informationHandout 12: Thermodynamics. Zeroth law of thermodynamics
1 Handout 12: Thermodynamics Zeroth law of thermodynamics When two objects with different temperature are brought into contact, heat flows from the hotter body to a cooler one Heat flows until the temperatures
More informationHandout 11: Ideal gas, internal energy, work and heat. Ideal gas law
Handout : Ideal gas, internal energy, work and heat Ideal gas law For a gas at pressure p, volume V and absolute temperature T, ideal gas law states that pv = nrt, where n is the number of moles and R
More informationFirst Law of Thermodynamics
First Law of Thermodynamics September 11, 2013 The first law of thermodynamics is the conservation of energy applied to thermal systems. Here, we develop the principles of thermodynamics for a discrete
More informationThe First Law of Thermodynamics
he First Law of hermodynamics he First Law of hermodynamics states that the energy of an isolated system is constant. If a system does an amount of work w, its internal energy (U) falls by the amount w.
More informationModule 5 : Electrochemistry Lecture 21 : Review Of Thermodynamics
Module 5 : Electrochemistry Lecture 21 : Review Of Thermodynamics Objectives In this Lecture you will learn the following The need for studying thermodynamics to understand chemical and biological processes.
More informationHandout 11: Ideal gas, internal energy, work and heat. Ideal gas law
Handout : Ideal gas, internal energy, work and heat Ideal gas law For a gas at pressure p, volume V and absolute temperature T, ideal gas law states that pv = nrt, where n is the number of moles and R
More informationPart I: Basic Concepts of Thermodynamics
Part I: Basic Concepts of Thermodynamics Lecture 3: Heat and Work Kinetic Theory of Gases Ideal Gases 3-1 HEAT AND WORK Here we look in some detail at how heat and work are exchanged between a system and
More informationTHE SECOND LAW OF THERMODYNAMICS. Professor Benjamin G. Levine CEM 182H Lecture 5
THE SECOND LAW OF THERMODYNAMICS Professor Benjamin G. Levine CEM 182H Lecture 5 Chemical Equilibrium N 2 + 3 H 2 2 NH 3 Chemical reactions go in both directions Systems started from any initial state
More informationThe Second Law of Thermodynamics (Chapter 4)
The Second Law of Thermodynamics (Chapter 4) First Law: Energy of universe is constant: ΔE system = - ΔE surroundings Second Law: New variable, S, entropy. Changes in S, ΔS, tell us which processes made
More informationPhysics 111. Thursday, Dec. 9, 3-5pm and 7-9pm. Announcements. Thursday, December 9, 2004
ics day, ember 9, 2004 Ch 18: diagrams isobaric process isochoric process isothermal process adiabatic process 2nd Law of Thermodynamics Class Reviews/Evaluations For the rest of the semester day,. 9,
More informationHandout 12: Thermodynamics. Zeroth law of thermodynamics
1 Handout 12: Thermodynamics Zeroth law of thermodynamics When two objects with different temperature are brought into contact, heat flows from the hotter body to a cooler one Heat flows until the temperatures
More informationMCQs THERMODYNAMICS. Physics Without Fear.
MCQs THERMODYNAMICS Physics Without Fear Thermodynamics: At a glance Zeroth law of thermodynamics: Two systems A and B each in thermal equilibrium with a third system C are in thermal equilibrium with
More informationDistinguish between an isothermal process and an adiabatic process as applied to an ideal gas (2)
1. This question is about thermodynamic processes. (a) Distinguish between an isothermal process and an adiabatic process as applied to an ideal gas.......... An ideal gas is held in a container by a moveable
More informationFirst Law of Thermodynamics Second Law of Thermodynamics Mechanical Equivalent of Heat Zeroth Law of Thermodynamics Thermal Expansion of Solids
Slide 1 / 66 1 What is the name of the following statement: "When two systems are in thermal equilibrium with a third system, then they are in thermal equilibrium with each other"? A B C D E First Law
More informationVersion 001 HW 15 Thermodynamics C&J sizemore (21301jtsizemore) 1
Version 001 HW 15 Thermodynamics C&J sizemore 21301jtsizemore 1 This print-out should have 38 questions. Multiple-choice questions may continue on the next column or page find all choices before answering.
More information