Thermodynamics: Entropy Conclusion

Similar documents
Thermodynamics: More Entropy

Thermodynamics: More Entropy

Thermodynamics: Entropy

Entropy. Physics 1425 Lecture 36. Michael Fowler, UVa

Thermodynamics: Entropy

A few comments on relativity

Where we ended last time:

Chem 350: Statistical Mechanics and Chemical Kinetics. Spring Preface. Introduction 2

Announcements 12 Dec 2013

Lecture 27: Entropy and Information Prof. WAN, Xin

I think really just going over all the equations for each section and the basic theories. An equation sheet would be AWESOME!

Physics, Time and Determinism

#29: Logarithm review May 16, 2009

PHYSICS 715 COURSE NOTES WEEK 1

Physics 172H Modern Mechanics

213 Midterm coming up

Figure 1: Doing work on a block by pushing it across the floor.

Philosophy 435/635: Direction of Time, Fall 2010 M 1:30-3:20, CT Hall 104 Professor J. North

It From Bit Or Bit From Us?

First Law Limitations

Chapter 20 The Second Law of Thermodynamics

Part I Electrostatics. 1: Charge and Coulomb s Law July 6, 2008

84 My God, He Plays Dice! Chapter 12. Irreversibility. This chapter on the web informationphilosopher.com/problems/reversibility

Thermodynamics Second Law Entropy

One sided tests. An example of a two sided alternative is what we ve been using for our two sample tests:

Announcements - 9 Oct 2014

Class 22 - Second Law of Thermodynamics and Entropy

Thermodynamics. 1.1 Introduction. Thermodynamics is a phenomenological description of properties of macroscopic systems in thermal equilibrium.

Concept: Thermodynamics

Classification and Regression Trees

Before the Quiz. Make sure you have SIX pennies

Why Complexity is Different

Physics 121, April 29, The Second Law of Thermodynamics.

Gibbs Paradox Solution

BIT 1002 Thermodynamics. First Law Heat engines Second Law Entropy. What is heat?

MITOCW watch?v=8osuq1yxcci

3 Dimensional String Theory

MITOCW ocw-18_02-f07-lec02_220k

Information in Biology

The physics of information: from Maxwell s demon to Landauer. Eric Lutz University of Erlangen-Nürnberg

Lecture Notes Set 4c: Heat engines and the Carnot cycle

Course Evaluation, FYTN04 Theoretical Particle. Particle Physics, Fall 11, Department of Astronomy and Theoretical Physics

PHY101: Major Concepts in Physics I. Photo: J. M. Schwarz

Irreversible Processes

Lecture Notes Set 3a: Probabilities, Microstates and Entropy

Statistical Mechanics

PHYS Statistical Mechanics I Course Outline

University Physics (Prof. David Flory) Chapt_21 Monday, November 26, 2007 Page 1

Physics 360 Review 3

ASTRO 114 Lecture Okay. What we re going to discuss today are what we call radiation laws. We ve

Basic Thermodynamics Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

18.13 Review & Summary

Information in Biology

Survey of Thermodynamic Processes and First and Second Laws

THE PHYSICS OF STUFF: WHY MATTER IS MORE THAN THE SUM OF ITS PARTS

Accelerated Observers

STATISTICAL AND THERMAL PHYSICS

Summer Lecture Notes Thermodynamics: Fundamental Relation, Parameters, and Maxwell Relations

February 20, Week 6. Homework #4, Due tonight. Mastering Physics: 9 problems from chapters 1 and 3 Written Question: 3.56

Chemical Applications of Symmetry and Group Theory Prof. Manabendra Chandra Department of Chemistry Indian Institute of Technology, Kanpur

Chapter 4: Going from microcanonical to canonical ensemble, from energy to temperature.

Physics Oct Reading. K&K chapter 6 and the first half of chapter 7 (the Fermi gas). The Ideal Gas Again

Quantum Thermodynamics

Introduction Statistical Thermodynamics. Monday, January 6, 14

Entropy and Free Energy in Biology

PHY101: Major Concepts in Physics I

Thermodynamics System Surrounding Boundary State, Property Process Quasi Actual Equilibrium English

Light Quantum Hypothesis

Announcements Wednesday, November 15

8 Lecture 8: Thermodynamics: Principles

The SI unit for Energy is the joule, usually abbreviated J. One joule is equal to one kilogram meter squared per second squared:

Contents. Objectives Asymmetric Time World Lines Three Arrows of Time entropy memory expanding universe Wormholes Grand Unification Recap.

HEAT AND THERMODYNAMICS PHY 522 Fall, 2010

Physics is time symmetric Nature is not

PAPER No. 6: PHYSICAL CHEMISTRY-II (Statistical

MITOCW watch?v=7q32wnm4dew

Amount of Substance and Its Unit Mole- Connecting the Invisible Micro World to the Observable Macro World Part 2 (English, mp4)

Chapter 11 Heat Engines and The Second Law of Thermodynamics

Chapter 20 - Spontaneous Change and Free Energy

Bachelor s Degree in Chemistry. 1 st YEAR Mechanics and Thermodynamics ECTS credits: 6 Semester: 1. Teaching objectives

Hypothesis testing I. - In particular, we are talking about statistical hypotheses. [get everyone s finger length!] n =

Phase Diagrams: Conditions for Equilibrium (CfE)

Massachusetts Institute of Technology. Final Exam Solutions. Solution to Problem 1: Knowin the Nomenclature (9%)

Big Bang, Black Holes, No Math

ΔU = Q W. Tue Dec 1. Assign 13/14 Friday Final: Fri Dec 11 2:30PM WALTER 145. Thermodynamics 1st Law. 2 nd Law. Heat Engines and Refrigerators

Statistical Physics. How to connect the microscopic properties -- lots of changes to the macroscopic properties -- not changing much.

Alan Mortimer PhD. Ideas of Modern Physics

Decision Trees. Gavin Brown

Announcements 13 Nov 2014

Collective Effects. Equilibrium and Nonequilibrium Physics

MITOCW watch?v=ko0vmalkgj8

Conduction and Radiation Prof. C. Balaji Department of Mechanical Engineering Indian Institute of Technology, Madras

Physics 9 Wednesday, February 29, 2012

MITOCW ocw f08-lec19_300k

Collective Effects. Equilibrium and Nonequilibrium Physics

Welcome to Physics 161 Elements of Physics Fall 2018, Sept 4. Wim Kloet

The Search for a Fundamental Theory of the Universe

MITOCW MIT7_01SCF11_track24_300k.mp4

Coins and Counterfactuals

Physics 2D Lecture Slides Lecture 1: Jan

Transcription:

Thermodynamics: Entropy Conclusion

From Warmup I would like to see an overview of all the chapters covered, and if possible some of the key concepts. I would appreciate a second opinion to make sure that I have a great study paper. Review session tonight, 6pm in C266 ESC

From Warmup Lots of questions about the equation: ds = dq/t The integral of ds=qr/t seemed a ton more applicable. I find confusing that ds=0 through a Carnot engine. I think the problem is I'm not seeing how Qr is 0. Q is not zero for a Carnot cycle! Qh > Qc, but Qc is at a lower temperature. I don't understand how entropy is supposed to "tie everything together". I'm a little unclear on how they did the derivation for it (it seemed to me that they had some expression that they wasn't equated to anything and they decided to take the natural log of it and multiply it by k simply so it looked like something else and that seemed somewhat sneaky and a little bit like cheating)... The key insight is that taking the natural log and mulitplying it by k gives you an expression that looks like something you ve seen before.

Clicker Poll Is the Second Law of Thermodynamics a Fundamental Law of Physics? a) Yes b) No As we discuss this, be prepared to defend what you mean by Fundamental Law of Physics.

Clicker Poll Is Boltzmann s constant a Fundamental Physical Constant? a) Yes b) No What do we mean by a Fundamental Physical Constant?

Some Philosophical Questions Thermodynamics is driven by Entropy. Entropy depends on the definition of the macrostates. Who, or what, determines the macrostate? Is it entirely subjective? A matter of perspective? Could we choose different macrostates and get a different theory of thermodynamics? Defining different macrostates for the same system: Dice Sum of the numbers Difference of the numbers Number of 1 s Etc.

Maxwell s Demon o Maxwell imagined a microscopic demon that could violate the 2 nd law o Imagine a gas in a container with a partition and a door. o The demon lets fast moving molecules into the right half and vice versa. o Therefore (Maxwell concludes), the 2 nd law is a statistical consequence of our being big (macroscopic)

Quantifying Information A bit of information is an answer to a question with two possible responses (e.g., Yes or No) One bit distinguishes between two possibilities. How many possibilities can be resolved by 4 bits? a) 4 b) 8 c) 16 d) 32

Other units of information trit: dit nat

Entropy as information o Entropy is the amount of information needed to give a complete microscopic description of a physical system o The second law of thermodynamics means that information about the microscopic state is always being lost.

Maxwell s Demon Revisited o Maxwell s demon must process information about the speeds of approaching molecules o What does it do with this information? Record it? Erase it? o It can t record information indefinitely eventually it must erase some of its information. o Erasing information increases the entropy! o The increase in entropy caused by erasing the information is always more than the entropy decrease caused by sorting the molecules o Maxwell s demon cannot violate the second law!

Relevance to current physics: From Science (last November): When we observe systems on different scales (different macrostates), there is a loss of information (entropy) about microscopic details. This is a big part of what makes science possible: If we needed to know string theory to do Newtonian physics, Newton would never have discovered his laws. The same principles hold in other branches of science.

Macro/Micro theories in Science Science is hierarchical Branches of science related as macro/micro theories Understanding the relation between macro/micro theories remains one of the fundamental problems in science. Microtheory Kinetic/Atomic Theory String Theory Quantum Mechanics Chemistry Biology Microeconomics Weather Macrotheory Thermodynamics Quantum Field Theory Chemistry Biology Psychology Macroeconomics Climate

Outlook We have covered (4 weeks): 1. Fluids 2. Thermodynamics Up Next: 1. Waves (3-4 weeks, Exam 2) 2. Optics (electromagnetic waves, 3-4 weeks, Exam 3) 3. Special Relativity (2 weeks) Cumulative Final Exam