Announcements 9/29/10 Three days to register your clicker. Exam starts Saturday Exam review session: Thurs, 8-9:30 pm, room C460 Reduced Tutorial Lab hours.

Slides:



Advertisements
Similar presentations
Heat Engines, Entropy, and the Second Law of Thermodynamics
Advertisements

Dr Roger Bennett Rm. 23 Xtn Lecture 13.
Thermodynamics April 27, 2015April 27, 2015April 27, 2015.
Lecture 8, p 1 Lecture 8 The Second Law of Thermodynamics; Energy Exchange  The second law of thermodynamics  Statistics of energy exchange  General.
Lecture 4. Entropy and Temperature (Ch. 3) In Lecture 3, we took a giant step towards the understanding why certain processes in macrosystems are irreversible.
Chapter 3 Classical Statistics of Maxwell-Boltzmann
Intermediate Physics for Medicine and Biology Chapter 3: Systems of Many Particles Professor Yasser M. Kadah Web:
Announcements 9/26/12 Prayer Exam 1 starts Saturday morning, goes until Thursday evening On Friday at the start of class I will talk a bit about what to.
Clicker question 1 Can you make it to the midterms on the evenings of Friday, Oct. 3 and Friday, Nov. 7, from 7:00-8:15 PM? A.Yes B.No.
VIII. Entropy for a reversible process at constant T dQ is path dependent dS is path independent S is function of state S is additive function for any.
MSEG 803 Equilibria in Material Systems 8: Statistical Ensembles Prof. Juejun (JJ) Hu
Quiz 8 (LAST QUIZ!) 8:30-8:50am TODAY Have your calculator ready. Cell phone calculator NOT allowed. Closed book Quiz 4 Re-evaluation Request Due this.
Lecture #8 Cassandra Paul Physics 7A Summer Session II 2008.
Announcements 2/4/11 Exam starts Tuesday, goes until next Tuesday (late fee on last day after 5 pm) Exam review session: today, 3-4:30 pm, room C261 
Announcements 9/27/10 5 days left to get your clicker registered Exam review session: Thurs, 8-9:30 pm, room C460 Reading assignment for Wednesday: a.
Introduction to Thermostatics and Statistical Mechanics A typical physical system has N A = X particles. Each particle has 3 positions and.
Announcements 10/4/10 Prayer Exam goes until Saturday a. a.Correction to syllabus: on Saturdays, the Testing Center gives out last exam at 3 pm, closes.
Announcements 9/28/11 A word about HW 13…
Announcements 9/26/11 Exam review session: Friday, 4 pm, room C460 Reading assignment for Wednesday: a. a.Section 22.8 – Especially read the marble example.
Lecture #6 Physics 7A Cassandra Paul Summer Session II 2008.
Gases and the Kinetic Molecular Theory. Speeds of gas molecules. For a single molecule. Kinetic energy is: KE = ½ mv 2 m = mass; v = velocity For a collection.
Announcements 2/2/11 Exam review session (tentative): Friday, 3-4:30 pm a. a.I will send tomorrow with final date/time, and room location. (Vote.
Thermo & Stat Mech - Spring 2006 Class 19 1 Thermodynamics and Statistical Mechanics Partition Function.
Entropy and the Second Law of Thermodynamics
The Statistical Interpretation of Entropy The aim of this lecture is to show that entropy can be interpreted in terms of the degree of randomness as originally.
Most likely macrostate the system will find itself in is the one with the maximum number of microstates. E 1  1 (E 1 ) E 2  2 (E 2 ) E 1  1 (E 1 )
Entropy Physics 202 Professor Lee Carkner Ed by CJV Lecture -last.
Lecture 27 Overview Final: May 8, SEC hours (4-7 PM), 6 problems
Microscopic definition of entropy Microscopic definition of temperature This applies to an isolated system for which all the microstates are equally probable.
1 Thermal Physics 13 - Temperature & Kinetic Energy 15 - Laws of Thermodynamics.
Chapter 15 Thermodynamics. MFMcGrawChap15d-Thermo-Revised 5/5/102 Chapter 15: Thermodynamics The first law of thermodynamics Thermodynamic processes Thermodynamic.
P340 Lecture 5 (Second Law) THE FUNDAMENTAL POSTULATE (OF THERMAL PHYSICS) Any isolated system in thermodynamic equilibrium is equally likely to be in.
Boltzmann Distribution and Helmholtz Free Energy
Entropy and the Second Law of Thermodynamics
Too many particles… can’t keep track! Use pressure (p) and volume (V) instead. Temperature (T) measures the tendency of an object to spontaneously give.
Announcements 9/24/12 Exam review session: Wed, 5-6:30 pm, room C295 Reading assignment for Wednesday, see footnote in syllabus: a. a.Lecture 13 reading:
Physics Momentum: Collisions
Q19. Second Law of Thermodynamics
Physics I Entropy: Reversibility, Disorder, and Information Prof. WAN, Xin
Statistical Thermodynamics Chapter Introduction The object: to present a particle theory which can interpret the equilibrium thermal properties.
Chapter 21ENTROPY AND THE SECOND LAW OF THERMODYNAMICS 21.1 Some One-Way Processes Consider the following examples: Example 1: If you drop a stone, it.
Lecture 15-- CALM What would you most like me to discuss tomorrow in preparation for the upcoming exam? proton)? Partition Function/Canonical Ensemble.
Lecture 15– EXAM I on Wed. Exam will cover chapters 1 through 5 NOTE: we did do a few things outside of the text: Binomial Distribution, Poisson Distr.
3.The Canonical Ensemble 1.Equilibrium between a System & a Heat Reservoir 2.A System in the Canonical Ensemble 3.Physical Significance of Various Statistical.
Lecture 9 Pg Midterm coming up… Monday April 7 pm (conflict 5:15pm) Covers: Lectures 1-12 (not including thermal radiation) HW 1-4 Discussion.
The Physics of Information: Demons, Black Holes, and Negative Temperatures Charles Xu Splash 2013.
Lecture 7, p Midterm coming up… Monday April 7 pm (conflict 5:15pm) Covers: Lectures 1-12 (not including thermal radiation) HW 1-4 Discussion.
Entropy Change (at Constant Volume) For an ideal gas, C V (and C P ) are constant with T. But in the general case, C V (and C P ) are functions of T. Then.
An Introduction to Statistical Thermodynamics. ( ) Gas molecules typically collide with a wall or other molecules about once every ns. Each molecule has.
CHAPTER 19 CHEMICAL THERMODYNAMICS SECTION 3 THE MOLECULAR INTERPRETATION OF ENTROPY.
PHYS 172: Modern Mechanics Lecture 24 – The Boltzmann Distribution Read 12.7 Summer 2012.
Announcements LAST chance to do Math Skills test is Friday (1/29) at 4:30 pm in HL G59. No class after 5pm Thursday April 1. Instead of Lab that week,
PHYS 172: Modern Mechanics Lecture 25 - Kinetic theory of gases; pressure Read 12.8 Summer 2012.
PHYS 172: Modern Mechanics Lecture 22 – Entropy and Temperature Read Summer 2012.
Boltzmann statistics, average values
To understand entropy, we need to consider probability.
Entropy and the Second Law of Thermodynamics
Thermal Physics Too many particles… can’t keep track!
Entropy and the Second Law of Thermodynamics By Dr A K Mohapatra
Quiz #1 for GP II, MATH, Spring 2012
Entropy and the Second Law of Thermodynamics
Entropy and the Second Law of Thermodynamics
PHYS 213 Midterm Exam HKN Review Session
Boltzmann statistics Reservoir R U0 -  Combined system U0 = const
Lon-Capa 4th HW assignment due tonight by 5 pm.
MIT Microstructural Evolution in Materials 3: Canonical Ensemble
PHYS 213 Midterm Exam HKN Review Session
Chapter 1: Statistical Basis of Thermodynamics
Second Law of Thermodynamics
PHYS 213 Midterm Exam HKN Review Session
Presentation transcript:

Announcements 9/29/10 Three days to register your clicker. Exam starts Saturday Exam review session: Thurs, 8-9:30 pm, room C460 Reduced Tutorial Lab hours on Saturday due to General Conference: only open 12 – 2pm. Increased Testing Center hours on Saturday due to G.C.: it opens at 8 am instead of the usual 10 am.

Thought Question A gas in contact with a thermal reservoir undergoes an isothermal expansion. The gas and the thermal reservoir are isolated from the rest of the universe. Which of the following is true? a. a.The entropy of both the gas and the reservoir will increase. b. b.The entropy of both the gas and the reservoir will decrease. c. c.The entropy of both the gas and the reservoir will not change. d. d.The entropy of the gas will go up, the entropy of the reservoir will go down, and the total entropy of the system will not change. e. e.The entropy of the gas will go up, the entropy of the reservoir will go down, and the total entropy of the system will increase.

Reading quiz Did you spend at least mins looking over Dr Colton’s “What is Entropy?” handout? a. a.Yes b. b.No Did you spend at least 5-10 mins reading the book section 22.8? a. a.Yes b. b.No

Microstates vs Macrostates Reminder a. a.Left microstate: part of the “royal flush” macrostate b. b.Right microstate: part of the “garbage” macrostate

Dice You roll two dice. What are the microstates? (1,1),(1,2),(1,3),(1,4),(1,5),(1,6),(2,1),(2,2),… How many microstates are there? How does that compare to the number of microstates for rolling one die? How many microstates if we roll 3 dice? What are the macrostates for 2 dice? (sum of numbers) What is the most likely macrostate?

MANY Dice You roll dice with your left hand. How many microstates are there? You roll dice with your right hand. How many microstates are there? How many microstates are there in the COMBINED system? Isn’t this ridiculous?

Solution: Use logarithms S = some constant  ln(#microstates) [units of J/K] a. a.Much more manageable numbers. b. b.Combining two systems: S tot = C  ln(#microstates1  #microstates2) = C  ln(#microstates1) + C  ln(#microstates2) = S 1 + S 2 c. c.System in macrostate with most microstates  system in macrostate with largest S

System and Reservoir System: E 1 Reservoir: E 2 E tot = E 1 + E 2 (const. volume so no work) 0 = dE 1 + dE 2 Want to maximize S: take dS/dE 1, set = 0

Temperature dS/dE is the same for two systems in thermal contact! Temperature is the same for two systems in thermal contact! a. a.dS/dE has units of 1/K… This “works” if the constant is chosen properly: S = k B ln(#microstates) Compare to We are assuming no work, so dE=dQ (First Law)

Small system with 2 possible energies: E 1A vs E 1B (1 microstate each) Probability of system 1 being in state A vs state B? P 1A ~ (#microstates of system 1 having energy E 1A )  (#microstates of system 2 having energy E 2A = E – E 1A ) Let #microstates of E 1A = 1 for now. Same thing for state 1B…

Math… Result: “of”, not “times”

The Boltzmann Factor Prob ~ BF; Prob = BF/(sum of all BFs) Worked Problem: Suppose an atom has only two available energy levels, which are separated by 2  J. If the temperature is 1.5 K, what is the probability the atom is in the lower state? The Boltzmann Factor

Maxwell-Boltzmann Velocity Distribution E = ½mv 2 What’s probability of having speed 5 vs speed 10? Multiplicities  (Number of states with speed v) ~ v 2

Maxwell-Boltzmann Velocity Distribution The result:  Exactly the equation given for the velocity distribution in your textbook! (after you do the integral in the denominator with, e.g. Mathematica)