ENGINEERING THERMODYNAMICS Dr. M.R.SWAMINATHAN Assistant Professor Internal Combustion Engineering Division Department of Mechanical Engineering ANNA UNIVERSITY.

Slides:



Advertisements
Similar presentations
Carnot cycle
Advertisements

THERMODYNAMICS II INTRODUCTION TO NAVAL ENGINEERING.
Department of Mechanical Engineering ME 322 – Mechanical Engineering Thermodynamics Lecture 18 Introduction to 2 nd Law and Entropy.
Heat Engines. The Heat Engine  A heat engine typically uses energy provided in the form of heat to do work and then exhausts the heat which cannot.
Advanced Thermodynamics Note 4 The Second Law of Thermodynamics
Refrigerators Physics 313 Professor Lee Carkner Lecture 13.
Second Law of Thermodynamics Physics 202 Professor Lee Carkner Lecture 18.
The Second Law of Thermodynamics
Second Law of Thermodynamics Physics 202 Professor Lee Carkner Lecture 18.
Statistical Mechanics Physics 202 Professor Lee Carkner Lecture 19.
Dr. Jie ZouPHY Chapter 22 Heat Engines, Entropy, and the Second Law of Thermodynamics.
Thermo & Stat Mech - Spring 2006 Class 6 1 Thermodynamics and Statistical Mechanics Entropy and the Second Law of Thermodynamics.
The Cyclic Devices P M V Subbarao Professor Mechanical Engineering Department Create Resources Parallel to Nature…..
Analysis of Second Law & Reversible Cyclic Machines P M V Subbarao Professor Mechanical Engineering Department Methods to Recognize Practicable Good Innovations…..
P V Isotherm, pV = constant = Nk B T Adiabat, pV  = constant v = 10:1:100; t = 100; r = 8.314; gamma = 1.67; p = r*t./v; k = (10^(gamma-1)).*r*t; pa =
For the cyclic process shown, W is:D A] 0, because it’s a loop B] p 0 V 0 C] - p 0 V 0 D] 2 p 0 V 0 E] 6 p 0 V 0 For the cyclic process shown,  U is:
5 CHAPTER The Second Law of Thermodynamics.
Physics I The Second Law of Thermodynamics Prof. WAN, Xin
The Second Law of Thermodynamics Chapter Introduction The first law of thermodynamics is simple, general, but does not constitute a complete theory.
Second Law of Thermodynamics Identify the direction of a process. (ex: Heat can only transfer from a hot object to a cold object, not the other around)
The Second Law of Thermodynamics Chapter 7.  The first law of thermodynamics states that during any cycle that a system undergoes, the cyclic integral.
The Laws of Thermodynamics
1 Thermal Physics 13 - Temperature & Kinetic Energy 15 - Laws of Thermodynamics.
Physics 1501: Lecture 37, Pg 1 Physics 1501: Lecture 37 Today’s Agenda l Announcements çHomework #12 (Dec. 9): 2 lowest dropped çMidterm 2 … in class.
Gas molar specific heats Mean kinetic energy of a gas molecule: If we have n moles of gas: Then molar specific heat at constant volume should be: What.
Thermodynamics I Chapter 5 Second Law of Thermodynamics Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi Malaysia.
Topic 10.3 Second Law of Thermodynamics and Entropy
L 20 Thermodynamics [5] heat, work, and internal energy heat, work, and internal energy the 1 st law of thermodynamics the 1 st law of thermodynamics the.
The second law of thermodynamics: The heat flow statement: Heat flows spontaneously from a substance at a higher temperature to a substance at a lower.
VII. The second low of Thermodynamics
ENGR 2213 Thermodynamics F. C. Lai School of Aerospace and Mechanical Engineering University of Oklahoma.
ERT 108 Physical Chemistry The Second Law of Thermodynamics by Miss Anis Atikah binti Ahmad
Entropy Change by Heat Transfer Define Thermal Energy Reservoir (TER) –Constant mass, constant volume –No work - Q only form of energy transfer –T uniform.
ChemE 260 The 2 nd Law of Thermodynamics April 26, 2005 Dr. William Baratuci Senior Lecturer Chemical Engineering Department University of Washington TCD.
Heat Engines and The Carnot Cycle. First Statement of the Second Law of Thermodynamics The first statement of the second law is a statement from common.
The Second Law of Thermodynamics Chapter 6. The Second Law  The second law of thermodynamics states that processes occur in a certain direction, not.
Chapter seven The second Law of thermodynamics The direction of thermal phenomena IF a system for some reason or other is not in a state of equilibrium.
Lecture Outline Chapter 12 College Physics, 7 th Edition Wilson / Buffa / Lou © 2010 Pearson Education, Inc.
Thermodynamic cycles 2nd law of Thermodynamics Carnot Cycle Lecture 30: 2nd Law of Thermodynamics.
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Functions, Purpose, and Examples
The Second Law of Thermodynamics
Work Done by a Gas Work=(Force)x(distance) Work=(Force)x(distance) =F  y Force=(Presssure)x(Area) Force=(Presssure)x(Area) W=P(A  y) W=P(A  y) =P 
Lecture 5 – The Second Law (Ch. 2)
Gas Cycles 2 nd Law of Thermodynamics. Work done by a cycle When a gas undergoes a complete cycle, it starts and ends in the same state. The gas is identical.
Engines. Second Law I  Real processes often make sense in only one direction in time.  The second law of thermodynamics states this: Heat flows naturally.
Reversible and irreversible processes Physics Entropy 28 September 2011.
Thermodynamics Davidson College APSI Ideal Gas Equations P 1 V 1 / T 1 = P 2 V 2 / T 2 PV = n R T (using moles) P V = N k B T (using molecules)  P:
2 nd Law of Thermodynamics Heat Engines. 2 nd Law Heat flows naturally from high temperature to low temperature, never in reverse.
Second Law It is impossible to construct a device which operating in a cycle will produce no effect other than transfer of heat from a cooler to a hotter.
Chapter 3.1 Laws of Thermodynamics. Systems  A system is a set of interconnected parts  An open system is one that exchanges both matter and energy.
Second Law of Thermodynamics Heat generally cannot flow spontaneously from a material at lower temperature to a material at higher temperature. The entropy.
Lecture 26: Thermodynamics II l Heat Engines l Refrigerators l Entropy l 2 nd Law of Thermodynamics l Carnot Engines.
Unit 61: Engineering Thermodynamics Lesson 8: Second Law of Thermodynamics.
Work in Thermodynamic Processes
Dr. Owen Clarkin School of Mechanical & Manufacturing Engineering Summary of Energy Topics Chapter 1: Thermodynamics / Energy Introduction Chapter 2: Systems.
Learning Goals for Chapter 20 Looking forward at … the difference between reversible and irreversible processes. the physics of internal-combustion engines.
Chapter 7 THE SECOND LAW OF THERMODYNAMICS
The Second Law of Thermodynamics
The Second Law of Thermodynamics
Engines.
Presented By: Rahul Sharma
LAXMI INSTITUTE OF TECHNOLOGY
The Second Law of Thermodynamics: Kelvin–Planck Statement
Second Law of Thermodynamics Entropy
Chapter 3 The 2nd law of thermodynamics
SECOND LAW OF THERMODYNAMICS
Second Law of Thermodynamics
ENGINEERING THERMODYNAMICS
SECOND LAW OF THERMODYNAMICS
Presentation transcript:

ENGINEERING THERMODYNAMICS Dr. M.R.SWAMINATHAN Assistant Professor Internal Combustion Engineering Division Department of Mechanical Engineering ANNA UNIVERSITY CHENNAI-25.

LIMITATIONS OF I LAW The first law of thermodynamics is simple, general, but does not constitute a complete theory because certain processes it permits do not occur in nature!

Examples of processes which are not prohibited by the first law, but cannot happen in a real world. Perfect machine Transfer heat from cold to hot subject Gas expansion

IRREVERSIBLE PROCESSES 1.A battery discharges through a resistor, releasing energy. The reverse process will not occur. 2.Two gases, initially in separated adjoining chambers, will mix uniformly.

3.A free expansion of gas (in Gay- Lussac-Joule experiment) 4.Heat flows from a high temperature body to a low temperature reservoir in the absence of other effect

STATEMENTS OF THE SECOND LAW OF THERMODYNAMICS: Kevin-Planck Statement: It is impossible to construct a device that operates in a cycle and produces no other effects than the performance of work and the exchange of heat with a single reservoir.

Model Heat Engine Q hot = W+Q coldQ hot = W+Q coldor Q hot -Q cold =WQ hot -Q cold =W (what goes in must come out)

II LAW OF THERMODYNAMICS

EFFICIENCY OF HEAT ENGINE

Even the most efficient heat engines reject almost one- half of the energy they receive as waste heat.

It is impossible for any device that operates on a cycle to receive heat from a single reservoir and produce a net amount of work.

Clausius Statement: It is impossible to construct a device that operates in a cycle and whose sole effect is to transfer heat from a cooler body to a hotter body.