Chapter 19 The First Law of Thermodynamics
|
|
|
- Junior Elliott
- 6 years ago
- Views:
Transcription
1 Chapter 19 The First Law of Thermodynamics Lecture by Dr. Hebin Li
2 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: Green Library 100 On all chapters
3 Physics II (spring 2015) Physics with calculus II in spring PHY 2049-(U02 ~ U07) Lecture: Mondays 8:00 am ~ 9:40 am, AHC3-110 Recitation: Wednesdays 2:00 pm ~ 3:50 pm, locations vary Textbook: University Physics (13 th edition) by Sears & Zemansky, Volume II (Chapter 21 ~ 36) Masteringphysics will be needed for HW.
4 Goals for Chapter 19 To represent heat transfer and work done in a thermodynamic process and to calculate work To relate heat transfer, work done, and internal energy change using the first law of thermodynamics To distinguish between adiabatic, isochoric, isobaric, and isothermal processes To understand and use the molar heat capacities at constant volume and constant pressure To analyze adiabatic processes
5 Thermodynamics systems A thermodynamic system is any collection of objects that may exchange energy with its surroundings. 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 the work done by the system, so it is positive for expansion.
6 Work done during volume changes Microscopic picture: Macroscopic picture: The work done by the gas as the piston moves dx Since Then dw = Fdx = padx dv = Adx dw = pdv V 2pdV W = V 1 If the pressure is constant W = p(v 2 V 1 )
7 Work on a pv diagram The work done equals the area under the curve on a pvdiagram. Work is positive for expansion and negative for compression.
8 Work depends on the path chosen When a thermodynamic system changes from an initial state to a final state, it passes through a series of intermediate states. This series of states is the path of the process. The work done by the system depends not only on the initial and final states, but also on the intermediate states, i.e. the path.
9 Internal Energy The internal energy of a system is the sum of the kinetic energies of all particles in the system, plus the sum of all the potential energies of interaction among these particles. It is not practical to calculate or measure the absolute internal energy. The change in internal energy depends on the heat transfer and work done U 2 U 1 = U = Q W (First law of thermodynamics)
10 First Law of Thermodynamics First law of thermodynamics: The change in the internal energy U of a system is equal to the heat added minus the work done by the system: U = Q W. The first law of thermodynamics is just a generalization of the conservation of energy. Both Q and W depend on the path chosen between states, but U is independent of the path. If the changes are infinitesimal, we write the first law as du = dq dw.
11 Cyclic processes and isolated systems In a cyclic process, the system returns to its initial state. The internal energy change is zero. Then U 2 = U 1 and Q = W. A isolated system does no work and has no heat flow in or out. That is W = Q = 0 and U = 0 Heat transfer and work in the process aba.
12 Four kinds of thermodynamics processes Adiabatic: No heat is transferred into or out of the system, so Q = 0. Isochoric: The volume remains constant, so W = 0. Isobaric: The pressure remains constant, so W = p(v 2 V 1 ). Isothermal: The temperature remains constant.
13 Internal energy of an ideal gas The internal energy of an ideal gas depends only on its temperature, not on its pressure or volume. The temperature of an ideal gas does not change during a free expansion.
14 Heat capacities of an ideal gas C V is the molar heat capacity at constant volume. C p is the molar heat capacity at constant pressure. The figure at the right shows how we could measure the two molar heat capacities. To produce the same temperature change, more heat is required at constant pressure than at constant volume. ( U is the same) C p = C V + R
The 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
Lecture 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
The First Law of Thermodynamics
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
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
Thermodynamics part III.
Thermodynamics part III. a.) Fenomenological thermodynamics macroscopic description b.) Molecular thermodynamics microscopic description b1.) kinetical gas theory b2.) statistical thermodynamics Laws of
NOTE: 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
Chapter 2. Energy and the First Law of Thermodynamics
Chapter 2 Energy and the First Law of Thermodynamics Closed System Energy Balance Energy is an extensive property that includes the kinetic and gravitational potential energy of engineering mechanics.
First 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.
Lecture 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
Internal 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
U = 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
2/18/2019. 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
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
Phys 160 Thermodynamics and Statistical Physics. Lecture 4 Isothermal and Adiabatic Work Heat Capacities
Phys 160 Thermodynamics and Statistical Physics Lecture 4 Isothermal and Adiabatic Work Heat Capacities Heat and Work Much of thermodynamics deals with three closely - related concepts; temperature, energy,
Chapter 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
19-9 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
The 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.
The 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
Chemistry. 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)
Physics 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
Physics 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
The 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)
Applied 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
Work, heat and the first law of thermodynamics
Chapter 3 Work, heat and the first law of thermodynamics 3.1 Mechanical work Mechanical work is defined as an energy transfer to the system through the change of an external parameter. Work is the only
6.3 The First Law of Thermodynamics
6.3 The First Law of Thermodynamics Physics Tool box Thermodynamic System - any collection of objects that is convenient to regard as a unit, and may have the potential to exchange energy with its surroundings.
6) 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
Energy: 1. Energy is an abstract physical quantity 2. It can be measured only by means of its effect Vikasana - Bridge Course
BASICS OF THERMODYNAMICS Vikasana - Bridge Course 2012 1 Energy: 1. Energy is an abstract physical quantity 2. It can be measured only by means of its effect Vikasana - Bridge Course 2012 2 HEAT Heat is
Chemistry 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
Week 2. Energy, Energy Transfer, And General Energy Analysis
Week 2. Energy, Energy Transfer, And General Energy Analysis Objectives 1. Introduce the concept of energy and define its various forms 2. Discuss the nature of internal energy 3. Define the concept of
Hence. 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
CHEM 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
General 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:
Physics 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
The Laws of Thermodynamics
MME 231: Lecture 06 he Laws of hermodynamics he Second Law of hermodynamics. A. K. M. B. Rashid Professor, Department of MME BUE, Dhaka oday s opics Relation between entropy transfer and heat Entropy change
Specific 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 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
8.21 The Physics of Energy Fall 2009
MIT OpenCourseWare http://ocw.mit.edu 8.21 The Physics of Energy Fall 2009 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. 8.21 Lecture 9 Heat Engines
ABCD42BEF F2 F8 5 4D65F8 CC8 9
ABCD BEF F F D F CC Physics 7B Fall 2015 Midterm 1 Solutions Problem 1 Let R h be the radius of the hole. R h = 2 3 Rα R h = 2 3 R+ R h = 2 3 R(1+α ) (4 points) In order for the marble to fit through the
Heat 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 =
First 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
Physics 141. Lecture 24.
Physics 141. Lecture 24. 0.5 µm particles in water, 50/50 glycerol-water, 75/25 glycerol-water, glycerol http://www.physics.emory.edu/~weeks/squishy/brownianmotionlab.html Frank L. H. Wolfs Department
Thermodynamic system is classified into the following three systems. (ii) Closed System It exchanges only energy (not matter) with surroundings.
1 P a g e The branch of physics which deals with the study of transformation of heat energy into other forms of energy and vice-versa. A thermodynamical system is said to be in thermal equilibrium when
12.1 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
Enthalpy 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
Thermodynamics 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
PHY101: Major Concepts in Physics I
Welcome back to PHY101: Major Concepts in Physics I Photo: S. T. Cummins Photo: S. T. Cummins Announcements Today is our final class! We will first discuss more on Chapters 14-15 and then conduct a short
UNIVERSITY 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
Relationships 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
11/13/2003 PHY Lecture 19 1
Announcements 1. Schedule Chapter 19 macroscopic view of heat (today) Chapter 20 microscopic view of heat (Tuesday 11/18) Review Chapters 15-20 (Thursday 11/20) Exam 3 (Tuesday 11/25) 2. Physics colloquium
Introduction. Statistical physics: microscopic foundation of thermodynamics degrees of freedom 2 3 state variables!
Introduction Thermodynamics: phenomenological description of equilibrium bulk properties of matter in terms of only a few state variables and thermodynamical laws. Statistical physics: microscopic foundation
Physics 141. Lecture 24. December 5 th. An important day in the Netherlands. Physics 141. Lecture 24. Course Information. Quiz
Physics 141. Lecture 24. 0.5 µm particles in water, 50/50 glycerol-water, 75/25 glycerol-water, glycerol http://www.physics.emory.edu/~weeks/squishy/brownianmotionlab.html Frank L. H. Wolfs Department
MCQs 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
Lecture 3 Evaluation of Entropy
Lecture 3 Evaluation of Entropy If we wish to designate S by a proper name we can say of it that it is the transformation content of the body, in the same way that we say of the quantity U that it is the
Downloaded from
Chapter 12 (Thermodynamics) Multiple Choice Questions Single Correct Answer Type Q1. An ideal gas undergoes four different processes from the same initial state (figure). Four processes are adiabatic,
Name: Discussion Section:
CBE 141: Chemical Engineering Thermodynamics, Spring 2018, UC Berkeley Midterm 1 February 13, 2018 Time: 80 minutes, closed-book and closed-notes, one-sided 8 ½ x 11 equation sheet allowed Please show
Thermodynamic 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
Physics 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
Announcements 13 Nov 2014
Announcements 13 Nov 2014 1. Prayer 2. Exam 3 starts on Tues Nov 25 a. Covers Ch 9-12, HW 18-24 b. Late fee on Wed after Thanksgiving, 3 pm c. Closes on Thursday after Thanksgiving, 3 pm d. Jerika review
Introduction 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
ME 200 Final Exam December 12, :00 a.m. to 10:00 a.m.
CIRCLE YOUR LECTURE BELOW: First Name Last Name 7:30 a.m. 8:30 a.m. 10:30 a.m. 1:30 p.m. 3:30 p.m. Mongia Abraham Sojka Bae Naik ME 200 Final Exam December 12, 2011 8:00 a.m. to 10:00 a.m. INSTRUCTIONS
The 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
Chapter 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
dv = adx, where a is the active area of the piston. In equilibrium, the external force F is related to pressure P as
Chapter 3 Work, heat and the first law of thermodynamics 3.1 Mechanical work Mechanical work is defined as an energy transfer to the system through the change of an external parameter. Work is the only
(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
Lecture 25: Heat and The 1st Law of Thermodynamics Prof. WAN, Xin
General Physics I Lecture 5: Heat and he 1st Law o hermodynamics Pro. WAN, Xin xinwan@zju.edu.cn http://zimp.zju.edu.cn/~xinwan/ Latent Heat in Phase Changes Latent Heat he latent heat o vaporization or
Content 10 Thermodynamics of gases Objectives Objectives 10.1 Heat capacity
hermodynamics of gases ontent. Heat capacities. ork done by a gas.3 irst law of thermodynamics.4 Isothermal adiabatic changes Objectives (a) define heat capacity, specific heat capacity molar heat capacity
Last Name or Student ID
10/06/08, Chem433 Exam # 1 Last Name or Student ID 1. (3 pts) 2. (3 pts) 3. (3 pts) 4. (2 pts) 5. (2 pts) 6. (2 pts) 7. (2 pts) 8. (2 pts) 9. (6 pts) 10. (5 pts) 11. (6 pts) 12. (12 pts) 13. (22 pts) 14.
Physics 2c Lecture 29. Exam Preparation I
Physics 2c Lecture 29 Exam Preparation I Exam Preparation Thursday & Friday lectures this week provide examples of the kind of things I might ask about in the final. This is by no means complete!!! To
(prev) (top) (next) (Throughout, we will assume the processes involve an ideal gas with constant n.)
1 of 9 8/22/12 9:51 PM (prev) (top) (next) Thermodynamics 1 Thermodynamic processes can be: 2 isothermal processes, ΔT = 0 (so P ~ 1 / V); isobaric processes, ΔP = 0 (so T ~ V); isovolumetric or isochoric
Section 2: Lecture 1 Integral Form of the Conservation Equations for Compressible Flow
Section 2: Lecture 1 Integral Form of the Conservation Equations for Compressible Flow Anderson: Chapter 2 pp. 41-54 1 Equation of State: Section 1 Review p = R g T " > R g = R u M w - R u = 8314.4126
Syllabus and Topics Thermal Physics I Fall 2007
Syllabus and Topics 33-341 Thermal Physics I Fall 2007 Robert F. Sekerka 6416 Wean Hall, Phone 412-268-2362 sekerka@cmu.edu http://sekerkaweb.phys.cmu.edu August 27, 2007 Class Schedule: This class is
Distinguish 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
Work 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
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department Statistical Physics I Spring Term 2003 Solutions to Problem Set #5
MASSACUSES INSIUE OF ECNOLOGY Physics Department 8.044 Statistical Physics I Spring erm 003 Solutions to Problem Set #5 Problem 1: Equation of State for a Ferromagnet a) We are looking for the magnetization
Lecture 5. Basic Thermodynamics. The First Law. References. Typical energy estimates
Lecture 5 Basic Thermodynamics. The First Law. References. Chemistry 3, Chapter 14, Energy and Thermochemistry, pp.658-700. Elements of Physical Chemistry, 5 th edition, Atkins & de Paula, Chapter 2, Thermodynamics:
Physics 218 Lecture 13
Physics 218 Lecture 13 Dr. David Toback Physics 218, Lecture XIII 1 Checklist for Today Things due for Last Thursday: Read Chapters 7, 8 & 9 Things that were due Last Monday: Chap 5&6 turned in on WebCT
PHY101: Major Concepts in Physics I. Photo: J. M. Schwarz
PHY101: Major Concepts in Physics I Photo: J. M. Schwarz Announcements We will be talking about the laws of thermodynamics today, which will help get you ready for next week s lab on the Stirling engine.
THERMODYNAMICS b) If the temperatures of two bodies are equal then they are said to be in thermal equilibrium.
THERMODYNAMICS Important Points:. Zeroth Law of Thermodynamics: a) This law gives the concept of temperature. b) If the temperatures of two bodies are equal then they are said to be in thermal equilibrium.
Chapter 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
Heat, Work, Internal Energy, Enthalpy, and the First Law of Thermodynamics. Internal Energy and the First Law of Thermodynamics
CHAPTER 2 Heat, Work, Internal Energy, Enthalpy, and the First Law of Thermodynamics Internal Energy and the First Law of Thermodynamics Internal Energy (U) Translational energy of molecules Potential
16-1. 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
Physics 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,
Chapter 12. The Laws of Thermodynamics. First Law of Thermodynamics
Chapter 12 The Laws of Thermodynamics First Law of Thermodynamics The First Law of Thermodynamics tells us that the internal energy of a system can be increased by Adding energy to the system Doing work
Final 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
1. Second Law of Thermodynamics
1. Second Law of hermodynamics he first law describes how the state of a system changes in response to work it performs and heat absorbed. However, the first law cannot explain certain facts about thermal
1. Second Law of Thermodynamics
1. Second Law of hermodynamics he first law describes how the state of a system changes in response to work it performs and heat absorbed. he second law deals with direction of thermodynamic processes
Lecture Ch. 2a. Lord Kelvin (a.k.a William Thomson) James P. Joule. Other Kinds of Energy What is the difference between E and U? Exact Differentials
Lecture Ch. a Energy and heat capacity State functions or exact differentials Internal energy vs. enthalpy st Law of thermodynamics Relate heat, work, energy Heat/work cycles (and path integrals) Energy
Relationships between WORK, HEAT, and ENERGY. Consider a force, F, acting on a block sliding on a frictionless surface
Introduction to Thermodynamics, Lecture 3-5 Prof. G. Ciccarelli (0) 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
The 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
Unit 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:
PY2005: Thermodynamics
ome Multivariate Calculus Y2005: hermodynamics Notes by Chris Blair hese notes cover the enior Freshman course given by Dr. Graham Cross in Michaelmas erm 2007, except for lecture 12 on phase changes.
Thermodynamics and Statistical Physics. Preliminary Ph.D. Qualifying Exam. Summer 2009
Thermodynamics and Statistical Physics Preliminary Ph.D. Qualifying Exam Summer 2009 (Choose 4 of the following 6 problems) -----------------------------------------------------------------------------------------------------------
Review of classical thermodynamics
Review of classical thermodynamics Fundamental Laws, Properties and Processes (2) Entropy and the Second Law Concepts of equilibrium Reversible and irreversible processes he direction of spontaneous change
- Apply closed system energy balances, observe sign convention for work and heat transfer.
CHAPTER : ENERGY AND THE FIRST LAW OF THERMODYNAMICS Objectives: - In this chapter we discuss energy and develop equations for applying the principle of conservation of energy. Learning Outcomes: - Demonstrate
Dr. Gundersen Phy 206 Test 2 March 6, 2013
Signature: Idnumber: Name: You must do all four questions. There are a total of 100 points. Each problem is worth 25 points and you have to do ALL problems. A formula sheet is provided on the LAST page
Final Review Prof. WAN, Xin
General Physics I Final Review Prof. WAN, Xin xinwan@zju.edu.cn http://zimp.zju.edu.cn/~xinwan/ About the Final Exam Total 6 questions. 40% mechanics, 30% wave and relativity, 30% thermal physics. Pick
Minimum Bias Events at ATLAS
Camille Bélanger-Champagne McGill University Lehman College City University of New York Thermodynamics Charged Particle and Statistical Correlations Mechanics in Minimum Bias Events at ATLAS Thermodynamics
For 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
Chapter 12. The Laws of Thermodynamics
Chapter 12 The Laws of Thermodynamics First Law of Thermodynamics The First Law of Thermodynamics tells us that the internal energy of a system can be increased by Adding energy to the system Doing work
First Law of Thermodynamics Basic Concepts
236 7 PHYSICAL CHEMISTRY 7 CHAPTER First Law of Thermodynamics Basic Concepts CONTENTS THERMODYNAMIC TERMS SYSTEM, BOUNDARY, SURROUNDINGS HOMOGENEOUS AND HETEROGENEOUS SYSTEMS TYPES OF THERMODYNAMIC SYSTEMS