ES 202 Fluid and Thermal Systems Lecture 18: Making the Connection (1/23/2003)

Slides:



Advertisements
Similar presentations
Properties of a Pure Substance
Advertisements

Chapter 12 Thermodynamic Property Relations Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 7th edition by Yunus.
ES 202 Fluid and Thermal Systems Lecture 15: Properties in Two-Phase Region (1/16/2003)
Properties of Pure Substances
Department of Mechanical Engineering ME 322 – Mechanical Engineering Thermodynamics Lecture 19 Calculation of Entropy Changes.
EGR 334 Thermodynamics Chapter 3: Section 6-8
Pure Substances Thermodynamics Professor Lee Carkner Lecture 5.
EGR 334 Thermodynamics Chapter 6: Sections 1-5
Entropy Cengel & Boles, Chapter 6 ME 152.
Entropy Change Property diagrams (T-s and h-s diagrams) –From the definition of the entropy, it is known that  Q=TdS during a reversible process. –Hence.
EGR 334 Thermodynamics Chapter 6: Sections 6-8
Department of Mechanical Engineering ME 322 – Mechanical Engineering Thermodynamics Lecture 6 Thermodynamic Diagrams Phase Change Determination of Properties.
Lec 18: Isentropic processes, TdS relations, entropy changes
QUIZ 2 A refrigerator uses refrigerant-134a as the working fluid and operates on an ideal vapor-compression refrigeration cycle between 0.18 and 0.9 MPa.
1 Lec 8: Real gases, specific heats, internal energy, enthalpy.
Heating at constant pressure. T-v curves for a range of pressures.
ES 202 Fluid and Thermal Systems Lecture 2 (12/03/2002)
Thermodynamic Property Relations
Specific Heat Thermodynamics Professor Lee Carkner Lecture 8.
ES 202 Fluid and Thermal Systems Lecture 5: Buoyancy & ES 201 Review (12/10/2002)
ES 202 Fluid and Thermal Systems Lecture 6: ES 201 Review & Steady State Devices (12/12/2002)
ES 202 Fluid & Thermal Systems
ME1521 Properties of Pure Substances Reading: Cengel & Boles, Chapter 2.
ES 202 Fluid and Thermal Systems Lecture 17: More on properties and phases (1/21/2003)
ES 202 Fluid and Thermal Systems Lecture 21: Isentropic Efficiencies (1/30/2003)
ES 202 Fluid and Thermal Systems Lecture 20: Isentropic Processes (1/28/2003)
ES 202 Fluid and Thermal Systems Lecture 24: Power Cycles (II) (2/6/2003)
ES 202 Fluid and Thermal Systems Lecture 16: Property Tables (1/20/2003)
Chapter 4 ENERGY ANALYSIS OF CLOSED SYSTEMS
Chapter 3 PROPERTIES OF PURE SUBSTANCES
Department of Mechanical Engineering ME 322 – Mechanical Engineering Thermodynamics Review For Exam 1.
Chap. 3 (Sec. 3-5 to End of Chapter) Mass Flow Rate =  A V (kg/s) Volume Flow Rate = A V (m 3 /s) V = velocity.
ES 202 Fluid and Thermal Systems Lecture 14: Phase Change (1/14/2003)
MEL140 Properties of pure substances. Pure substance A pure substance has the same chemical composition throughout. Are the following confined in a fixed.
THERMODYNAMIC PROPERTY RELATIONS
Properties of ideal gases / liquids / solids Ideal gases (and sometimes liquids / solids) are ‘special cases’ where properties behave in relatively simple.
CHAPTER 4 ENERGY ANALYSIS OF CLOSED SYSTEMS
Properties, states and phases of a pure substance I am teaching Engineering Thermodynamics using the textbook by Cengel and Boles. Many figures in the.
Thermodynamics I Inter - Bayamon Lecture 4 Thermodynamics I MECN 4201 Professor: Dr. Omar E. Meza Castillo
Properties, states and phases of a pure substance I am teaching Engineering Thermodynamics using the textbook by Cengel and Boles. Many figures in the.
Ch# 2 Properties of Pure Substances. Objectives Introduce the concept of a pure substance. Introduce the concept of a pure substance. Discuss the physics.
Steam Engine Sliding valve Steam enters chamber from left, leaving from right both valves closed, piston moves to the right Steam enters from right, leaving.
1 The Second Law of Thermodynamics (II). 2 The Fundamental Equation We have shown that: dU = dq + dw plus dw rev = -pdV and dq rev = TdS We may write:
MAE 219: THERMODYNAMICS by Professor YVES NGABONZIZA MAE 219: THERMODYNAMICS I.
ENGR 2213 Thermodynamics F. C. Lai School of Aerospace and Mechanical Engineering University of Oklahoma.
Properties of Pure Substances Chapter 3. Why do we need physical properties?  As we analyze thermodynamic systems we describe them using physical properties.
Lecture # 4 PROPERTIES OF PURE SUBSTANCES PURE SUBSTANCE.
PURE SUBSTANCE I am teaching Engineering Thermodynamics using the textbook by Cengel and Boles. Many figures in the slides are taken from that book, and.
Entropy Property Relationships Chapter 7b. The T-ds relations Consider an internally reversible process occurring in a closed system.
Pressure – Volume – Temperature Relationship of Pure Fluids.
1 Property Relationships Chapter 6. 2 Apply the differential form of the first law for a closed stationary system for an internally reversible process.
WCB/McGraw-Hill © The McGraw-Hill Companies, Inc.,1998 Thermodynamics Çengel Boles Third Edition 2 CHAPTER Properties of Pure Substances.
Chapter 12 THERMODYNAMIC PROPERTY RELATIONS
Chapter 5 ENERGY ANALYSIS OF CLOSED SYSTEMS
Chapter 3 PROPERTIES OF PURE SUBSTANCES Dr. Kagan ERYURUK Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Chapter 4 ENERGY ANALYSIS OF CLOSED SYSTEMS
Thermodynamics I. Examples  2.25  2.74  2.89 Wrap-up  Heat – work equivalent  Chapter 2 Equations  One-Minute Paper  Test 1: 1/27 Chapter 2 Text.
Properties of Pure Substances. 2 We now turn our attention to the concept of pure substances and the presentation of their data. Simple System A simple.
CHAPTER 12 THERMODYNAMIC PROPERTY RELATIONS
Chapter 4 ENERGY ANALYSIS OF CLOSED SYSTEMS
Chapter 12 THERMODYNAMIC PROPERTY RELATIONS
Satish Pradhan Dnyanasadhana college, Thane
Thermodynamics I Chapter 2 Properties of Pure Substances
THERMODYNAMICS SKMU 2113 LECTURER: PROFESSOR DR. MAZLAN ABDUL WAHID
Chapter 4 ENERGY ANALYSIS OF CLOSED SYSTEMS
Review For Exam 1.
Chapter 3 Properties of Engineering Working Fluid
CHAPTER 4 ENERGY ANALYSIS OF CLOSED SYSTEMS
Chapter 3: Evaluating Properties
11 CHAPTER Thermodynamic Property Relations.
Presentation transcript:

ES 202 Fluid and Thermal Systems Lecture 18: Making the Connection (1/23/2003)

Lecture 18ES 202 Fluid & Thermal Systems2 Assignments Homework: –5-78, 3-93 in Cengel & Turner Reading assignment –7-7, 7-9 in Cengel & Turner –ES 201 notes

Lecture 18ES 202 Fluid & Thermal Systems3 Announcements No office hour tomorrow (out of town for a presentation) –You may send me s if you have question (I will check my s upon return on Saturday)

Lecture 18ES 202 Fluid & Thermal Systems4 Road Map of Lecture 18 The “How to” of linear interpolation Review of what you can do –property tables (compressed liquid, saturated mixture, superheated vapor) –Compressed Liquid Approximation Relationship between property tables and your familiar models in ES 201 (ideal gas, incompressible substance) –fill in the gaps to make the picture complete –coupling between new and old materials Application of conservation and accounting principles to real substance Emphasis on thinking in terms of P-v, T-v and P-T diagrams

Lecture 18ES 202 Fluid & Thermal Systems5 Illustration on Interpolation Consider the following figure with two known data points (x 1, y 1 ), (x 2, y 2 ) and a “to be determined” data point (X, Y): Simple fact: If three points lie on a straight line, the slope of the line segment formed between any two points must be the same as that of other line segments. Mathematically, the above statement can be expressed as x y x2x2 x1x1 y1y1 y2y2 X Y

Lecture 18ES 202 Fluid & Thermal Systems6 Phase determination of a substance at a specific set of conditions Find out thermodynamics properties from appropriate tables: –compressed liquid table –saturated mixture table (quality of a mixture) –superheated vapor table –interpolation procedure Compressed Liquid Approximation Familiarity with phase diagrams (P-v, T-v, P-T) –constant pressure line (piston-cylinder model) –constant specific volume line (rigid system boundaries) –constant temperature line (isothermal process) A Check List for You

Lecture 18ES 202 Fluid & Thermal Systems7 Making the Connection (I) Recall your familiar models in ES 201: –ideal gas –incompressible substance These models are limited and represent “simplified” behavior of real substances under particular conditions: –ideal gas (good for gases at low pressures) –incompressible substance (good for liquids and solids) The models are good as long as the working conditions are not far from the underlying assumptions. The phase and property tables tabulate the exact measures of real substance behavior, i.e. tells you the true stories over the range reported on tables.

Lecture 18ES 202 Fluid & Thermal Systems8 Making the Connection (II) Conceptually, you can think of the tables as the data which fills in the gaps between different models. –provides a larger range of applicability and operation The conservation and accounting principles which you learned in ES 201 are still true no matter you are working with models or real substances. They are physical principles which cannot be violated. –conservation of mass –conservation of linear and angular momentum –conservation of energy –production of entropy However, changes in properties can be obtained differently now.

Lecture 18ES 202 Fluid & Thermal Systems9 Making the Connection (III) For examples: In the perfect gas model, the specific heats are taken to be constant. In this way, the change in specific internal energy or enthalpy can be related to the change in temperature directly. In treating real substances, such assumptions are not necessary. You can directly find out the specific internal energy or enthalpy from the property tables if you know any two independent, intensive properties about the state (State Principle). Main point: The rest of the engineering analysis (involving conservation laws) remains exactly the same. No new materials here!! It is a matter of working out familiar problems with new properties.

Lecture 18ES 202 Fluid & Thermal Systems10 Goal: Integration of different pieces of materials learned in ES 201 and ES 202 to do system analysis for a general substance

Lecture 18ES 202 Fluid & Thermal Systems11 Example Problems