PHY 341641 Thermodynamics and Statistical Physics Lecture 3
- Slides: 14
PHY 341/641 Thermodynamics and Statistical Physics Lecture 3 1. Introduction to thermodynamics (Chapter 2) a. Definition of “the system” b. Thermodynamic variables (T, P, V, N, …) 2. First law of thermodynamics -- the sign of work a. Some examples for ideal gas systems b. Some cyclic processes c. Efficiency of process 9/15/2020 PHY 341/641 Spring 2012 -- Lecture 3 1
Macroscopic viewpoint – thermodynamics (start reading Chapter 2) System of study Controlling medium 9/15/2020 PHY 341/641 Spring 2012 -- Lecture 3 2
Thermodynamic process -- WORK various sign conventions !!!#$#!!! 9/15/2020 PHY 341/641 Spring 2012 -- Lecture 3 3
Work sign conventions in various text books: Work done BY the system Work done ON the system Textbook Gould & Tobochnik, Statistical and Thermal Physics (2010) Sign - Kittel & Kroemer, Thermal Physics (1980) -/+ Serway & Jewitt, Physics (8 th Ed. ) (2010) - Serway & Beichner, Physics (5 th Ed. ) (2000) + Baierlein, Thermal Physics (1999) + Callen, Thermodynamics (1985) - Bailyn, A Survey of Thermodynamics (1994) + Fermi, Thermodynamics (1936) + 9/15/2020 PHY 341/641 Spring 2012 -- Lecture 3 4
First law of thermodynamics W Q System of study Controlling medium 9/15/2020 PHY 341/641 Spring 2012 -- Lecture 3 5
Examples of heat and work performed by ideal gas 9/15/2020 PHY 341/641 Spring 2012 -- Lecture 3 6
Various ideal gas processes (assuming N constant) Process Variables Constant V V 1, P 1, T 1 V 1, P 2, T 2 Constant P V 1, P 1, T 1 V 2, P 1, T 2 Constant T V 1, P 1, T 1 V 2, P 2, T 1 Q=0 V 1, P 1, T 1 V 2, P 2, T 2 9/15/2020 Q W DU 0 0 0 PHY 341/641 Spring 2012 -- Lecture 3 7
Some details of the adiabatic case: Q = 0 9/15/2020 PHY 341/641 Spring 2012 -- Lecture 3 8
Ideal gas expansions DT = 0 DQ = 0 9/15/2020 PHY 341/641 Spring 2012 -- Lecture 3 9
Work performed during a cyclic process: 9/15/2020 PHY 341/641 Spring 2012 -- Lecture 3 10
Efficiency of cyclic processes: The notions of work and heat can be used for practical devices Example: Internal combustion engine Otto cycle: http: //www. howstuffworks. com/engine 1. htm General measure of process efficiency (assuming no frictional losses; “completely reversible processes”): 9/15/2020 PHY 341/641 Spring 2012 -- Lecture 3 11
9/15/2020 PHY 341/641 Spring 2012 -- Lecture 3 12
Analysis of an ideal heat engine Nicholas Carnot (French Engineer) 1834 ad ia tic a b isothermal ad iab isothermal 9/15/2020 at ic PHY 341/641 Spring 2012 -- Lecture 3 13
Analysis of Carnot cycle for ideal gas system 9/15/2020 PHY 341/641 Spring 2012 -- Lecture 3 14
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