Thermodynamics: An Engineering Approach, 6 th Edition Yunus A. Cengel, Michael A. Boles McGraw-Hill, 2008

Similar documents
Chapter 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES

Chapter 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES

Chapter 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES

CHAPTER 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES

ME 215. Mass and Energy Analysis of Control Volumes CH-6 ÇANKAYA UNIVERSITY. Mechanical Engineering Department. Open Systems-Control Volumes (CV)

AREN 2110: Thermodynamics Spring 2010 Homework 7: Due Friday, March 12, 6 PM

Chapter 5. In Chap. 4, we applied the general energy balance relation MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES. Objectives

Chapters 5, 6, and 7. Use T 0 = 20 C and p 0 = 100 kpa and constant specific heats unless otherwise noted. Note also that 1 bar = 100 kpa.

Chapter 5. In Chap. 4, we applied the general energy balance relation MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES. Objectives

CONTROL VOLUME ANALYSIS USING ENERGY. By Ertanto Vetra

R13. II B. Tech I Semester Regular/Supplementary Examinations, Oct/Nov THERMODYNAMICS (Com. to ME, AE, AME) Time: 3 hours Max.

ME ENGINEERING THERMODYNAMICS UNIT III QUESTION BANK SVCET

Chapter 10 VAPOR AND COMBINED POWER CYCLES

MECHANICAL ENGINEERING THERMAL AND FLUID SYSTEMS STUDY PROBLEMS

Enhancement of CO2 Refrigeration Cycle Using an Ejector: 1D Analysis

LECTURE-14. Air Refrigeration Cycles. Coefficient of Performance of a Refrigerator:

Chapter 1 STEAM CYCLES

flow work, p. 173 energy rate balance, p. 174 nozzle, p. 177 diffuser, p. 177 turbine, p. 180 compressor, p. 184 (4.4b) p. 166

Review Questions for the FE Examination

Lecture No.1. Vapour Power Cycles

Chapter 6 THE SECOND LAW OF THERMODYNAMICS

EXTRA CREDIT OPPORTUNITY: Due end of day, Thursday, Dec. 14

Chapter 10 Vapor and Combined Power Cycles

OUTCOME 2 TUTORIAL 2 STEADY FLOW PLANT

HW-1: Due Tuesday 13 Jun 2017 by 2:00:00 pm EDT to Your Division s GradeScope Site

Thermodynamics: Homework A Set 3 Jennifer West (2004)

MCE535 Thermal Power and Propulsive Systems. Lecture 04: 04/10/2017

Chapter 9: Vapor Power Systems

CHAPTER 1 BASIC CONCEPTS


a. The power required to drive the compressor; b. The inlet and output pipe cross-sectional area. [Ans: kw, m 2 ] [3.34, R. K.

ES Fluid & Thermal Systems Page 1 of 6 STEAM TURBINE LABORATORY

Thermodynamic analysis on post combustion CO 2 capture of natural gas fired power plant

Enthalpy Calculations. Change in enthalpy can occur because of change in temperature, change in phase, or mixing of solutions and reactions.

semester + ME6404 THERMAL ENGINEERING UNIT III NOZZLES, TURBINES & STEAM POWER CYCLES UNIT-III

Faculty of Engineering 2 nd year 2016 Mechanical Engineering Dep. Final-exam (code: M 1222)

Chapter 10 POWER CYCLES. Department of Mechanical Engineering

International Journal of Advance Engineering and Research Development

Chapter 5: Thermodynamic Processes and Cycles

Thermodynamics: An Engineering Approach, 6 th Edition Yunus A. Cengel, Michael A. Boles McGraw-Hill, 2008

ESO 201A Thermodynamics

Application of Exergy Analysis. Value and Limitations

Eng Thermodynamics I - Examples 1

Eng Thermodynamics I: Sample Final Exam Questions 1

Eng Thermodynamics I - Examples 1

In this lecture... Solve problems related to First law of thermodynamics for closed and open systems Heat engines Refrigerators and heat pumps

THE SECOND LAW OF THERMODYNAMICS

Problems in chapter 9 CB Thermodynamics

Chapter 1 Basic Concepts

Second Law of Thermodynamics

A Scroll Expander with Heating Structure and Their Systems

PARAMETRIC STUDY OF GAS TURBINE CYCLE COUPLED WITH VAPOR COMPRESSION REFRIGERATION CYCLE FOR INTAKE AIR COOLING

Chapter 10. In Chap. 9 we discussed gas power cycles for which the VAPOR AND COMBINED POWER CYCLES. Objectives

Div. 5 7:30 am Div. 2 10:30 am Div. 4 12:30 am Prof. Naik Prof. Braun Prof. Bae

Chapter 10. In Chap. 9 we discussed gas power cycles for which the VAPOR AND COMBINED POWER CYCLES. Objectives

S.Y. Diploma : Sem. III [PG/PT/ME] Thermal Engineering

Principles of. Turbomachinery. Seppo A. Korpela. The Ohio State University WILEY A JOHN WILEY & SONS, INC., PUBLICATION

20/06/2011 Seminar on Geothermal Exploitation Santiago de Chile

MCG THERMODYNAMICS II. 22 April 2008 Page 1 of 7 Prof. W. Hallett

HW-1: Due Friday 25 August 2017 by 4:30:00 pm EDT To Your Division s GradeScope Site

FLUID MECHANICS PROF. DR. METİN GÜNER COMPILER

SIMPACK - MODEL DEVELOPMENT PACKAGE FOR POWER PLANTS

K.S. Rawat 1, H. Khulve 2, A.K. Pratihar 3 1,3 Department of Mechanical Engineering, GBPUAT, Pantnagar , India

R.A. Chaplin Chemical Engineering, University of New Brunswick, Canada

Ejector Expansion Refrigeration Systems

CHAPTER 1 BASIC CONCEPTS THEORY

World Journal of Engineering Research and Technology WJERT

Thermo-fluid Dynamics, Design and Performance

Engineering Thermodynamics

Chapter 6. The Second Law of Thermodynamics. by Asst. Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn

LECTURE-15. Ideal Reverse Brayton Cycle. Figure (6) Schematic of a closed reverse Brayton cycle

Performance Benefits for Organic Rankine Cycles with Flooded Expansion

Chapter 9: Applications of the Laws of Thermodynamics

Efficiency improvement of steam power plants in Kuwait

Appendix B. Glossary of Steam Turbine Terms

Turbomachinery. Overview

Permanent City Research Online URL:

ME 331 Thermodynamics II

EXERGY ANALYSIS P.V. Aravind Assistant Professor, Delft University of Technology Visiting Lecturer, TU Munich

Chapter 6 THE SECOND LAW OF THERMODYNAMICS

COMPARATIVE ANALYSES OF TWO IMPROVED CO 2 COMBINED COOLING, HEATING, AND POWER SYSTEMS DRIVEN BY SOLAR ENERGY

Ph.D. Qualifying Exam. Thermodynamics. Spring 2011

A. the temperature of the steam at the turbine exhaust increases. B. additional moisture is removed from the steam entering the turbine.

2 nd Law of Thermodynamics

W t. Strategy: We need to step through the equipments and figure out the inlets and outlets to allow us to calculate the work and heat terms.

Alpha College of Engineering

ANALYSIS OF DIFFERENT TYPES OF REGULATION AND ITS EFFICIENCY IN STEAM POWER CYCLES MASTER THESIS

MEM 310 Design Project Assignment

Combined Mass and Energy Transients

2. The data at inlet and exit of the turbine, running under steady flow, is given below.

Exergy in Processes. Flows and Destruction of Exergy

ES 3001 Thermodynamics

Parametric Study of a Vapor Compression Refrigeration Cycle Using a Two-Phase Constant Area Ejector

Revue des Energies Renouvelables Spécial ICT3-MENA Bou Ismail (2015) Numerical study of a single effect ejector-absorption cooling system

Development of Terry Turbine Analytical Models for RCIC Off-Design Operation Conditions

Chapter 8. Vapor Power Systems

- 2 - SME Q1. (a) Briefly explain how the following methods used in a gas-turbine power plant increase the thermal efficiency:

CHAPTER 4 STEAM TURBINE and CYCLE HEAT BALANCE

MECHANICAL ENGINEERING DEPARTMENT, OITM

International Journal of Informative & Futuristic Research ISSN (Online):

Transcription:

Thermodynamics: An Engineering Approach, 6 th Edition Yunus A. Cengel, Michael A. Boles McGraw-Hill, 2008 Chapter 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES SUMMARY 1

CONSERVATION OF MASS Conservation of mass: Mass, like energy, is a conserved property, and it cannot be created or destroyed during a process. Closed systems: The mass of the system remain constant during a process. Control volumes: Mass can cross the boundaries, and so we must keep track of the amount of mass entering and leaving the control volume. 2

Mass and Volume Flow Rates Definition of average velocity The average velocity V avg is defined as the average speed through a cross section. 3

Mass and Volume Flow Rates Volume flow rate The volume flow rate is the volume of fluid flowing through a cross section per unit time. 4

Conservation of Mass Principle The conservation of mass principle for a control volume: The net mass transfer to or from a control volume during a time interval Δt is equal to the net change (increase or decrease) in the total mass within the control volume during Δt. 5

Mass Balance for Steady-Flow Processes During a steady-flow process, the total amount of mass contained within a control volume does not change with time (m CV = constant). Then the conservation of mass principle requires that the total amount of mass entering a control volume equal the total amount of mass leaving it. For steady-flow processes, we are interested in the amount of mass flowing per unit time, that is, the mass flow rate. Multiple inlets and exits Single stream Many engineering devices such as nozzles, diffusers, turbines, compressors, and pumps involve a single stream (only one inlet and one outlet). Conservation of mass principle for a twoinlet one-outlet steady-flow system. 6

Special Case: Incompressible Flow The conservation of mass relations can be simplified even further when the fluid is incompressible, which is usually the case for liquids. Steady, incompressible Steady, incompressible flow (single stream) There is no such thing as a conservation of volume principle. However, for steady flow of liquids, the volume flow rates, as well as the mass flow rates, remain constant since liquids are essentially incompressible substances. During a steady-flow process, volume flow rates are not necessarily conserved although mass flow rates are. 7

FLOW WORK AND THE ENERGY OF A FLOWING FLUID Flow work, or flow energy: The work (or energy) required to push the mass into or out of the control volume. This work is necessary for maintaining a continuous flow through a control volume. Schematic for flow work 8

Total Energy of a Flowing Fluid h = u + Pv The flow energy is automatically taken care of by enthalpy. In fact, this is the main reason for defining the property enthalpy. The total energy consists of three parts for a non-flowing fluid and four parts for a flowing fluid. 9

Energy Transport by Mass When the kinetic and potential energies of a fluid stream are negligible When the properties of the mass at each inlet or exit change with time as well as over the cross section The product & mθ i i is the energy transported into control volume by mass per unit time. 10

ENERGY ANALYSIS OF STEADY-FLOW SYSTEMS Under steady-flow conditions, the mass and energy contents of a control volume remain constant. Under steady-flow conditions, the fluid properties at an inlet or exit remain constant (do not change with time). 11

Mass for a steady-flow process Mass balance A water heater in steady operation 12

Energy balances for a steady-flow process Energy balance 13

Energy balance relations with sign conventions (i.e., heat input and work output are positive) when kinetic and potential energy changes are negligible 14

Nozzles and Diffusers A nozzle is a device that increases the velocity of a fluid at the expense of pressure. A diffuser is a device that increases the pressure of a fluid by slowing it down. The cross-sectional area of a nozzle decreases in the flow direction for subsonic flows and increases for supersonic flows. The reverse is true for diffusers. Energy balance for a nozzle or diffuser: 15

Turbines and Compressors Compressors, as well as pumps and fans, are devices used to increase the pressure of a fluid. Work is supplied to these devices from an external source through a rotating shaft. A compressor is capable of compressing the gas to very high pressures. A fan increases the pressure of a gas slightly and is mainly used to mobilize a gas. Pumps work very much like compressors except that they handle liquids instead of gases. Turbine drives the electric generator in steam, gas, or hydroelectric power plants. 16

Compressors Energy balance for the compressor in this Figure 17

Throttling valves Throttling valves are any kind of flow-restricting devices that cause a significant pressure drop in the fluid. What is the difference between a turbine and a throttling valve? The pressure drop in the fluid is often accompanied by a large drop in temperature, and for that reason throttling devices are commonly used in refrigeration and air-conditioning applications. Energy balance 18

Throttling valves The temperature of an ideal gas does not change during a throttling (h = constant) process since h = h(t). During a throttling process, the enthalpy of a fluid remains constant. But internal and flow energies may be converted to each other. 19

Mixing chambers Energy balance for the Adiabatic mixing chamber in the Figure is: 60 C 140 kpa 10 C 43 C 20

Heat exchangers Heat exchangers are devices where two moving fluid streams exchange heat without mixing. Heat exchangers are widely used in various industries, and they come in various designs. A heat exchanger can be as simple as two concentric pipes. The heat transfer associated with a heat exchange may be zero or nonzero depending on how the control volume is selected. 21

Heat exchangers Mass and energy balances for the Adiabatic heat exchanger in the Figure is: 22

Pipe and Duct Flow The transport of liquids or gases in pipes and ducts is of great importance in many engineering applications. Flow through a pipe or a duct usually satisfies the steady-flow conditions. Pipe or duct flow may involve more than one form of work at the same time Heat losses from a hot fluid flowing through an uninsulated pipe or duct to the cooler environment may be very significant. 23

Pipe and Duct Flow Pipe or duct flow may involve more than one form of work at the same time Energy balance for the pipe flow shown in the Figure is 24

ENERGY ANALYSIS OF UNSTEADY-FLOW PROCESSES Many processes of interest, however, involve changes within the control volume with time. Such processes are called unsteady-flow, or transient-flow, processes. Charging of a rigid tank from a supply line is an unsteady-flow process since it involves changes within the control volume. 25

ENERGY ANALYSIS OF UNSTEADY-FLOW PROCESSES Most unsteady-flow processes can be represented reasonably well by the uniform-flow process. Uniform-flow process: The fluid flow at any inlet or exit is uniform and steady, and thus the fluid properties do not change with time or position over the cross section of an inlet or exit. If they do, they are averaged and treated as constants for the entire process. The shape and size of a control volume may change during an unsteady-flow process. 26

Mass balance 27

Energy balance The energy equation of a uniform-flow system reduces to that of a closed system when all the inlets and exits are closed. 28

THE END 29