Chapter 7. (a) The compressor work is give by. = m (h 2 h 1 ) = (0.08 kg/s)( ) kj/kg = kw. (b) The refrigeration capacity, in tons, is

Size: px
Start display at page:

Download "Chapter 7. (a) The compressor work is give by. = m (h 2 h 1 ) = (0.08 kg/s)(416.2 398.6) kj/kg = 1.408 kw. (b) The refrigeration capacity, in tons, is"

Transcription

1 apter 7 Exaple Refrigerant 4a i te working fluid in an ideal vapor-opreion refrigeration yle tat ouniate terally wit a old region at 0 and a war region at 6. Saturated vapor enter te opreor at 0 and aturated liquid leave te ondener at 6. e a flow rate of te refrigerant i 0.08 kg/. Deterine (a) te opreor power, in k, (b) te refrigeration apaity, in ton, () te oeffiient of perforane, and (d) te oeffiient of perforane of a arnot refrigeration yle operating between war and old region at 6 and 0, repetively. Solution H H ondener Expanion valve Evaporator 4 opreor iquid 4 a b Ientalp 6 o 0 o Vapor Speifi Internal Speifi Speifi ype ep reure Volue Energy Entalpy Entropy uality ae Ma /kg kj/kg kj/kg kj/kg/k R-4a Saturated Vapor R-4a Saturated iquid R-4a Supereated Vapor (a) e opreor work i give by ( ) (0.08 kg/)( ) kj/kg.408 k (b) e refrigeration apaity, in ton, i ( 4 ) (0.08 kg/)( ) kj/kg.0 k ton (.0 kj/)(60 /in).7 ton kj/in 6 Moran, M. J. and Sapiro H. N., Fundaental of Engineering erodynai, iley, 008, pg

2 () te oeffiient of perforane i β (d) e oeffiient of perforane of a arnot refrigeration yle operating between war and old region at 6 and 0, repetively β H H H ondener iquid H Expanion valve Evaporator 4 opreor H 4 Ientalp Figure 7.- A vapor-opreion refrigeration wit irreveribilitie. Vapor Figure 7.- ow everal feature exited in atual vapor opreion yte. e eat tranfer between te refrigerant and te war and old region are not aoplied reveribly: te refrigerant teperature in te evaporator i le tan te low reervoir teperature,, and te refrigerant teperature in te ondener i greater tan te ig reervoir teperature, H. e opreor will not ave 00% effiieny o tat te fluid leaving te opreor will be at tate (), wi i at iger entropy tan te ientropi opreion tate (). e oeffiient of perforane dereae a te average teperature of te refrigerant in te evaporator dereae and a te average teperature of te refrigerant in te ondener inreae. If te teral effiieny of te opreor i known, te entapy at tate () an be deterined fro te following expreion: ( ) / η ( / ) Due to frition, tere will be preure drop a te refrigerant flow troug te evaporator, ondener, and piping onneting te variou oponent. e preure drop are ignored in ubequent alualtion for ipliity. 7-

3 Exaple Refrigerant 4a i te working fluid in an ideal vapor-opreion refrigeration yle tat ouniate terally wit a old region at 0. Saturated vapor enter te opreor at 0 and aturated liquid leave te ondener at 9 bar. e a flow rate of te refrigerant i 0.08 kg/. Deterine (a) te opreor power, in k, (b) te refrigeration apaity, in ton, () te oeffiient of perforane. Solution H H ondener Expanion valve Evaporator 4 opreor iquid 4 a b Ientalp 9 bar -0 o Vapor Speifi Internal Speifi Speifi ype ep reure Volue Energy Entalpy Entropy uality ae Ma /kg kj/kg kj/kg kj/kg/k R-4a Saturated Vapor R-4a Supereated Vapor R-4a Saturated iquid (a) e opreor work i give by ( ) (0.08 kg/)(4 9.7) kj/kg.44 k (b) e refrigeration apaity, in ton, i ( 4 ) (0.08 kg/)( ) kj/kg.4 k ton (.4 kj/)(60 /in).5 ton kj/in () e oeffiient of perforane i β Moran, M. J. and Sapiro H. N., Fundaental of Engineering erodynai, iley, 008, pg

4 Exaple Refrigerant 4a i te working fluid in an ideal vapor-opreion refrigeration yle tat ouniate terally wit a old region at 0. Saturated vapor enter te opreor at 0 and liquid leave te ondener at 9 bar and 0 o. e opreor a an effiieny of 80%. e a flow rate of te refrigerant i 0.08 kg/. Deterine (a) te opreor power, in k, (b) te refrigeration apaity, in ton, () te oeffiient of perforane. Solution Expanion valve H ondener Evaporator 4 opreor iquid 0 o -0 o 4 Ientalp 9 bar H Vapor Speifi Speifi Speifi ype ep reure Volue Entalpy Entropy uality ae Ma /kg kj/kg kj/kg/k R-4a Saturated Vapor R-4a Supereated Vapor R-4a opreed iquid 4 R-4a iquid Vapor Mixture (a) e opreor work i give by ( ) η (0.08 kg/) kj/kg. k (b) e refrigeration apaity, in ton, i ( 4 ) (0.08 kg/)( ) kj/kg.08 k ton (.08 kj/)(60 /in).44 ton kj/in () te oeffiient of perforane i β Moran, M. J. and Sapiro H. N., Fundaental of Engineering erodynai, iley, 008, pg

5 Exaple Deign a refrigeration yte, wi upplie two level of aonia refrigerant at 0 o and at 0 o to two exanger requiring dutie of 850 and,500 k, repetively. Draw a proe flow diagra (FD) owing ajor equipent, flow rate in kg/ of refrigerant, duty of ea eat exanger, duty, and orepower of ea opreor. Alo, ow teperature and preure of all trea. ere are no inter-ooler between opreor. e opreed ga fro te lat tage opreor an be ooled to aturated liquid at 0 o. Ue 75% adiabati effiieny for all opreor. Solution ,, 4, 5 E, i F V F V E E Figure 7.- A two level refrigeration yte. A deign of a two level refrigeration yte i own in Figure 7.-. Saturated liquid aonia at i i partially vaporized troug a let-down valve V to and. art of te liquid eparated by te fla dru F i ued to provide te firt level refrigeration troug te eat exanger E. e reaining liquid pae troug a eond valve were it teperature and preure i redued to and. e liquid trea fro te eond fla dru F i ued for te eond level refrigeration troug te eat exanger E were it beoe aturated vapor. i trea i obined wit te aturated vapor fro te eond fla dru and opreed bak to preure. e proble an be olved eiter wit a reure-entalpy diagra of aonia a own in Figure 7.-4 or wit a progra olving an equation of tate to obtain terodynai propertie of a pure ubtane given any two oter propertie (for exaple, teperature and preure or aturation teperature). 7-5

6 Ioter at i ritial point, i Saturated vapor Saturated liquid,,ideal Ientropi line,,, Entalpy Figure 7.-4 reure-entalpy diagra. e will ue te terodynai value fro a oputer progra a own in able 7.-. For ti exaple te preure drop aro te eat exanger and aro te fla dru will be negleted. Saturated liquid aonia at i 0 o i a defined tate at.67 Ma wit entalpy equal to.4 kj/kg a own in te firt line of te property table in Figure Siilarly, te aturated propertie of aonia at 0 o and 0 o an be obtained. e a flow rated of aturated liquid aonia,,, required to reove,500 k in eat exanger E i given by, 500k V,, kg/ In ti equation, V, and, are te entalpy of aturated vapor and liquid aonia at 0 o, repetively., i alo te liquid flow rate leaving fla dru F. e vapor flow rate, V,, leaving te eond fla dru F an be deterined fro te a and energy balane around valve V and fla dru F., + V, In ti equation i te aturated liquid aonia flow rate at and entering valve V. e energy balane i given by + ),,, + V, (, V, V, Solving for V, we ave 7-6

7 , V,, V,,, kg/ able 7.- erodynai propertie of aonia. Speifi Speifi Speifi ype ep reure Volue Entalpy Entropy uality ae Ma /kg kj/kg kj/kg/k Aonia Saturated iquid Aonia Saturated Vapor Aonia Saturated iquid 4 Aonia Saturated Vapor 5 Aonia Saturated iquid 6 Aonia Saturated Vapor 7 Aonia Supereated Vapor 8 Aonia Supereated Vapor 9 Aonia Supereated Vapor 0 Aonia Supereated Vapor Aonia Supereated Vapor e liquid flow rate troug valve V i ten kg/ e a flow rated of aturated liquid aonia, E,, required to reove 850 k in eat exanger E i given by E, 850k V,, kg/ In ti equation, V, and, are te entalpy of aturated vapor and liquid aonia at 0 o, repetively. e liquid flow rate,,, leaving fla dru F i te u of te liquid flow rate troug te eat exanger E and te liquid flow rate troug te valve V, E, kg/ Siilarly, te vapor flow rate, V,, leaving te firt fla dru F an be deterined fro te a and energy balane around valve V and fla dru F. V,, i V,, i kg/ e total a flow rate i of aonia required for te yte i ten i, + V, kg/ 7-7

8 e vapor flow rate fro bot te exanger E and te fla dru F i given by, vap E, + V, kg/,vap e now deterine te orepower of te eond opreor. e aturated vapor leaving te eond exanger E and te fla dru F ut be opreed fro Ma to 0.65 Ma. For ientropi work, te ga entering and exiting te opreor will ave te ae entropy at kj/kg o K. e entalpy of te ga leaving te eond opreor due to ientropi opreion i 50 kj/kg. For 75% adiabati effiieny, te atual entalpy of te exiting ga i given by,atual 4 + (50 4)/ kj/kg e orepower required of te eond opreor i H.0764 (50 4)/ k 68 p e atual teperature of te exiting ga i obtained fro 0.65 Ma and,atual 56 kj/kg. e ave te ga leaving te eond opreor at 5.64 o tat ut be ixed wit te aturated ga leaving te firt eat exanger E and te firt fla dru F at 0 o. e entalpy of te ga entering te firt opreor i ten kj/kg At tee ondition ( 0.65 Ma, kj/kg) o and entropy kj/kg o K, te ga will be opreed to.67 Ma. e entalpy of te ga leaving te firt opreor due to ientropi opreion i 68 kj/kg. For 75% adiabati effiieny, te atual entalpy of te exiting ga i given by 5,atual ( )/ kj/kg e orepower required of te firt opreor i H.004 ( )/ k 54 p e ga leaving te firt opreor at.67 Ma, 5,atual 66. kj/kg, it teperature 5 i 00.8 o. e ga will be ondened to aturated liquid at 0 o (.67 Ma). e duty of te eat exanger E i given by.004 (66..4) 40 k 7-8

Chapter 4. 4.3 Applications of Energy Balance

Chapter 4. 4.3 Applications of Energy Balance Capter 4 4. Appliation of Energy Balane We will diu exaple illutrating te analyi of erveral devie of interet in engineering, inluding nozzle and diffuer, turbine, opreor and pup, eat exanger, and trottling

More information

Warm medium, T H T T H T L. s Cold medium, T L

Warm medium, T H T T H T L. s Cold medium, T L Refrigeration Cycle Heat flows in direction of decreasing temperature, i.e., from ig-temperature to low temperature regions. Te transfer of eat from a low-temperature to ig-temperature requires a refrigerator

More information

ES-7A Thermodynamics HW 5: 5-62, 81, 96, 134; 7-29, 40, 42, 67, 71, 106 Spring 2003 Page 1 of 7

ES-7A Thermodynamics HW 5: 5-62, 81, 96, 134; 7-29, 40, 42, 67, 71, 106 Spring 2003 Page 1 of 7 ES-7A hermodynamic HW 5: 5-6, 8, 96, 34; 7-9, 4, 4, 67, 7, 6 Sring 3 Page of 7 5-6 Heat Pum Given: A heat um i ued to maintain a houe at 3 C. he houe loe heat to the outide at a rate of 6, kj/h, and the

More information

Chapter 10: Refrigeration Cycles

Chapter 10: Refrigeration Cycles Capter 10: efrigeration Cycles Te vapor compression refrigeration cycle is a common metod for transferring eat from a low temperature to a ig temperature. Te above figure sows te objectives of refrigerators

More information

Rayleigh Flow - Thermodynamics

Rayleigh Flow - Thermodynamics Sl f Aerae Engineering Rayleig Flw - erdynai Steady, -d, ntant area, iniid flw wit n external wrk but wit reerible eat tranfer (eating r ling) ρ Cnered uantitie (a, entu e.) ine Ant: a fluxρntant G ine

More information

ME 24-221 THERMODYNAMICS I

ME 24-221 THERMODYNAMICS I Solution to extra problem in chapter 8 Noember 9, 000 Fall 000 J. Murthy ME 4- HERMODYNAMICS I 8.5 Water i ued a the working fluid in a Carnot cycle heat engine, where it change from aturated liquid to

More information

Ideal Rankine Cycle T 1 2

Ideal Rankine Cycle T 1 2 Vapor Poer Cycle We kno that the Carnot cycle i mot efficient cycle operatg beteen to pecified temperature limit. Hoever; the Carnot cycle i not a uitable model for team poer cycle ce: he turbe ha to handle

More information

A Primer on Dimensions and Units

A Primer on Dimensions and Units 1 Dienion v Unit A Prier on Dienion and Unit Glen Thornrot Mehanial Enineerin Departent Cal Poly State Univerity, San Lui Obipo Nearly every enineerin proble you will enounter will involve dienion: the

More information

Combustion chamber. Fig.1: Schematic for an open gas-turbine cycle.

Combustion chamber. Fig.1: Schematic for an open gas-turbine cycle. Open Ga urbine Cycle Fuel Combution camber urbine Saft Compreor W net Air Combution product Woring rincipal Fig.: Scematic for an open ga-turbine cycle. Fre air enter te compreor at ambient temperature

More information

HADNOUT E.13 - EXAMPLES ON TRANSFER FUNCTIONS, POLES AND ZEROS

HADNOUT E.13 - EXAMPLES ON TRANSFER FUNCTIONS, POLES AND ZEROS Paraura Leture 3 Augut HADNOUT E3 - EXAMPLES ON TRANSFER FUNCTIONS POLES AND ZEROS Exaple Deterine the tranfer funtion of the a-pring-daper yte The governing differential equation of a a-pring-daper yte

More information

Math 22B, Homework #8 1. y 5y + 6y = 2e t

Math 22B, Homework #8 1. y 5y + 6y = 2e t Math 22B, Homework #8 3.7 Problem # We find a particular olution of the ODE y 5y + 6y 2e t uing the method of variation of parameter and then verify the olution uing the method of undetermined coefficient.

More information

ES-7A Thermodynamics HW 1: 2-30, 32, 52, 75, 121, 125; 3-18, 24, 29, 88 Spring 2003 Page 1 of 6

ES-7A Thermodynamics HW 1: 2-30, 32, 52, 75, 121, 125; 3-18, 24, 29, 88 Spring 2003 Page 1 of 6 Spring 2003 Page 1 of 6 2-30 Steam Tables Given: Property table for H 2 O Find: Complete the table. T ( C) P (kpa) h (kj/kg) x phase description a) 120.23 200 2046.03 0.7 saturated mixture b) 140 361.3

More information

Physics 110 Spring 2006 Fluid Mechanics Their Solutions

Physics 110 Spring 2006 Fluid Mechanics Their Solutions ic Sprin 00 lui Mecanic Teir Solution reure in a flui arie linearl wit ept Wat i te abolute preure at a ept of 00 in te ocean if te enit of ea i 4 k/? t ti ept wat force ut te frae aroun a circular ubarine

More information

Shell and Tube Heat Exchanger

Shell and Tube Heat Exchanger Sell and Tube Heat Excanger MECH595 Introduction to Heat Transfer Professor M. Zenouzi Prepared by: Andrew Demedeiros, Ryan Ferguson, Bradford Powers November 19, 2009 1 Abstract 2 Contents Discussion

More information

Effects of a Price Decrease. Separating Income and Substitution Effects. Hicks and Slutsky Decompositions. Hicks Substitution and Income Effects

Effects of a Price Decrease. Separating Income and Substitution Effects. Hicks and Slutsky Decompositions. Hicks Substitution and Income Effects Effect of a Price Decreae Searating Incoe and Subtitution Effect ECON 37: Microeconoic Teor Suer 24 Rice Univerit Stanle Gilbert Can be broken down into two coonent Incoe effect Wen te rice of one good

More information

Math 113 HW #5 Solutions

Math 113 HW #5 Solutions Mat 3 HW #5 Solutions. Exercise.5.6. Suppose f is continuous on [, 5] and te only solutions of te equation f(x) = 6 are x = and x =. If f() = 8, explain wy f(3) > 6. Answer: Suppose we ad tat f(3) 6. Ten

More information

External Flow Correlations (Average, Isothermal Surface)

External Flow Correlations (Average, Isothermal Surface) Externa Fow orreation (Average, Ioterma urface Fat Pate orreation Fow ondition aminar urbuent were Average et mber 1/ 0.66 Re 0. 6 /5 0.07 Re A 1/ 0.6 60 A /5 1/ 0.07 Rex, c 0.66Rex, c Re x, c Re 10 8

More information

Holcim Emission and Monitoring Guideline for Unit Conversion of Continuous Measuring Devices

Holcim Emission and Monitoring Guideline for Unit Conversion of Continuous Measuring Devices Holi Eiion and Monitoring Guideline for Unit Converion of Continuou Meauring Devie erion 004-0 / January 004 HGR-C/M J. Waltiberg ABLE F CE YMBL LI.... "RAW ALUE" AD CERED ALUE...4. "RAW ALUE"...4. CERI

More information

Thermodynamics - Example Problems Problems and Solutions

Thermodynamics - Example Problems Problems and Solutions Thermodynamics - Example Problems Problems and Solutions 1 Examining a Power Plant Consider a power plant. At point 1 the working gas has a temperature of T = 25 C. The pressure is 1bar and the mass flow

More information

PHYSICS 151 Notes for Online Lecture #11

PHYSICS 151 Notes for Online Lecture #11 PHYSICS 151 ote for Online Lecture #11 A free-bod diagra i a wa to repreent all of the force that act on a bod. A free-bod diagra ake olving ewton econd law for a given ituation eaier, becaue ou re odeling

More information

Exergy Calculation. 3.1 Definition of exergy. 3.2 Exergy calculations. 3.2.1. Exergy of environment air

Exergy Calculation. 3.1 Definition of exergy. 3.2 Exergy calculations. 3.2.1. Exergy of environment air Exergy Calculation This chapter is intended to give the user a better knoledge of exergy calculations in Cycle-Tepo. Exergy is not an absolute quantity but a relative one. Therefore, to say soething about

More information

Lecture 10: What is a Function, definition, piecewise defined functions, difference quotient, domain of a function

Lecture 10: What is a Function, definition, piecewise defined functions, difference quotient, domain of a function Lecture 10: Wat is a Function, definition, piecewise defined functions, difference quotient, domain of a function A function arises wen one quantity depends on anoter. Many everyday relationsips between

More information

Instantaneous Rate of Change:

Instantaneous Rate of Change: Instantaneous Rate of Cange: Last section we discovered tat te average rate of cange in F(x) can also be interpreted as te slope of a scant line. Te average rate of cange involves te cange in F(x) over

More information

NBR 13714 SISTEMAS DE HIDRANTES E MANGOTINHOS PARA

NBR 13714 SISTEMAS DE HIDRANTES E MANGOTINHOS PARA NBR 13714 SISTEMAS DE HIDRANTES E MANGOTINHOS PARA PEJUP-4Y68KU6Q PDF 536.63KB 25 Aug, 2014 TABLE OF CONTENT Introdution Brie Deription Main Topi Tenial Note Appendix Gloary PDF ile: nbr 13714 itea de

More information

HEAT EXCHANGERS. Associate Professor. IIT Delhi E-mail: prabal@mech.iitd.ac.in. Mech/IITD

HEAT EXCHANGERS. Associate Professor. IIT Delhi E-mail: prabal@mech.iitd.ac.in. Mech/IITD HEAT EXHANGES Prabal Talukdar Assoate Professor Departent of Meanal Engneerng IIT Del E-al: prabal@etdan Heat Exangers Heat exangers are deves tat faltate te exange of eat between two fluds tat are at

More information

EC201 Intermediate Macroeconomics. EC201 Intermediate Macroeconomics Problem set 8 Solution

EC201 Intermediate Macroeconomics. EC201 Intermediate Macroeconomics Problem set 8 Solution EC201 Intermediate Macroeconomics EC201 Intermediate Macroeconomics Prolem set 8 Solution 1) Suppose tat te stock of mone in a given econom is given te sum of currenc and demand for current accounts tat

More information

PG Student (Heat Power Engg.), Mechanical Engineering Department Jabalpur Engineering College, India. Jabalpur Engineering College, India.

PG Student (Heat Power Engg.), Mechanical Engineering Department Jabalpur Engineering College, India. Jabalpur Engineering College, India. International Journal of Emerging Trends in Engineering and Development Issue 3, Vol. (January 23) EFFECT OF SUB COOLING AND SUPERHEATING ON VAPOUR COMPRESSION REFRIGERATION SYSTEMS USING 22 ALTERNATIVE

More information

ASHRAE Journal July 2002 33

ASHRAE Journal July 2002 33 Copyright 2002, Aerican ociety of Heating, Refrigerating and Air-Conditioning Engineer, Inc. (www.ahrae.org). Reprinted by periion fro AHRAE Journal, July 2002. Thi article ay not be copied nor ditributed

More information

Three Phase Theory - Professor J R Lucas

Three Phase Theory - Professor J R Lucas Three Phae Theory - Profeor J Luca A you are aware, to tranit power with ingle phae alternating current, we need two wire live wire and neutral. However you would have een that ditribution line uually

More information

CHAPTER 7 THE SECOND LAW OF THERMODYNAMICS. Blank

CHAPTER 7 THE SECOND LAW OF THERMODYNAMICS. Blank CHAPTER 7 THE SECOND LAW OF THERMODYNAMICS Blank SONNTAG/BORGNAKKE STUDY PROBLEM 7-1 7.1 A car engine and its fuel consumption A car engine produces 136 hp on the output shaft with a thermal efficiency

More information

Development of a model for the simulation of Organic Rankine Cycles based on group contribution techniques

Development of a model for the simulation of Organic Rankine Cycles based on group contribution techniques ASME Turbo Expo Vancouver, June 6 10 2011 Development of a model for the simulation of Organic Rankine ycles based on group contribution techniques Enrico Saverio Barbieri Engineering Department University

More information

UNIT 2 REFRIGERATION CYCLE

UNIT 2 REFRIGERATION CYCLE UNIT 2 REFRIGERATION CYCLE Refrigeration Cycle Structure 2. Introduction Objectives 2.2 Vapour Compression Cycle 2.2. Simple Vapour Compression Refrigeration Cycle 2.2.2 Theoretical Vapour Compression

More information

Heat Exchangers. Heat Exchanger Types. Heat Exchanger Types. Applied Heat Transfer Part Two. Topics of This chapter

Heat Exchangers. Heat Exchanger Types. Heat Exchanger Types. Applied Heat Transfer Part Two. Topics of This chapter Applied Heat Transfer Part Two Heat Excangers Dr. Amad RAMAZANI S.A. Associate Professor Sarif University of Tecnology انتقال حرارت کاربردی احمد رمضانی سعادت ا بادی Autumn, 1385 (2006) Ramazani, Heat Excangers

More information

Design And Analysis Of Absorption Refrigeration Systems

Design And Analysis Of Absorption Refrigeration Systems Deign And Analyi Of Aborption Refrigeration Sytem Felipe Vilar da Silva, felipetaperoa@otmailcom Carlo Antonio Cabral Santo, carlocabralanto@yaoocombr Weiber Lima de Souza, weiberlima@otmailcom 1 Intuto

More information

2.1: The Derivative and the Tangent Line Problem

2.1: The Derivative and the Tangent Line Problem .1.1.1: Te Derivative and te Tangent Line Problem Wat is te deinition o a tangent line to a curve? To answer te diiculty in writing a clear deinition o a tangent line, we can deine it as te iting position

More information

Drying and Dehydration

Drying and Dehydration Drying and Dehydration Abstract. This chapter reviews basic concepts of drying and dehydration, including ass balance analyses. Equilibriu oisture content, water activity, and related paraeters are discussed.

More information

Chapter 5. Principles of Unsteady - State Heat Transfer

Chapter 5. Principles of Unsteady - State Heat Transfer Suppleental Material for ransport Process and Separation Process Principles hapter 5 Principles of Unsteady - State Heat ransfer In this chapter, we will study cheical processes where heat transfer is

More information

The modelling of business rules for dashboard reporting using mutual information

The modelling of business rules for dashboard reporting using mutual information 8 t World IMACS / MODSIM Congress, Cairns, Australia 3-7 July 2009 ttp://mssanz.org.au/modsim09 Te modelling of business rules for dasboard reporting using mutual information Gregory Calbert Command, Control,

More information

Lesson. 11 Vapour Compression Refrigeration Systems: Performance Aspects And Cycle Modifications. Version 1 ME, IIT Kharagpur 1

Lesson. 11 Vapour Compression Refrigeration Systems: Performance Aspects And Cycle Modifications. Version 1 ME, IIT Kharagpur 1 Lesson Vapour Compression Refrigeration Systems: Performance Aspects And Cycle Modifications Version ME, IIT Kharagpur The objectives of this lecture are to discuss. Performance aspects of SSS cycle and

More information

A Gas Law And Absolute Zero

A Gas Law And Absolute Zero A Gas Law And Absolute Zero Equipent safety goggles, DataStudio, gas bulb with pressure gauge, 10 C to +110 C theroeter, 100 C to +50 C theroeter. Caution This experient deals with aterials that are very

More information

A Gas Law And Absolute Zero Lab 11

A Gas Law And Absolute Zero Lab 11 HB 04-06-05 A Gas Law And Absolute Zero Lab 11 1 A Gas Law And Absolute Zero Lab 11 Equipent safety goggles, SWS, gas bulb with pressure gauge, 10 C to +110 C theroeter, 100 C to +50 C theroeter. Caution

More information

Pressure. Pressure. Atmospheric pressure. Conceptual example 1: Blood pressure. Pressure is force per unit area:

Pressure. Pressure. Atmospheric pressure. Conceptual example 1: Blood pressure. Pressure is force per unit area: Pressure Pressure is force per unit area: F P = A Pressure Te direction of te force exerted on an object by a fluid is toward te object and perpendicular to its surface. At a microscopic level, te force

More information

Lecture 24: Spinodal Decomposition: Part 3: kinetics of the

Lecture 24: Spinodal Decomposition: Part 3: kinetics of the Leture 4: Spinodal Deoposition: Part 3: kinetis of the oposition flutuation Today s topis Diffusion kinetis of spinodal deoposition in ters of the onentration (oposition) flutuation as a funtion of tie:

More information

PHASE BREW USE & CARE MANUAL 8 CUP COFFEE BREWER. For use with HG

PHASE BREW USE & CARE MANUAL 8 CUP COFFEE BREWER. For use with HG PHASE BREW 8 CUP COFFEE BREWER USE & CARE MANUAL For use wit HG Welcoe to Pase Brew! You re about to brewing better coffee in a wole new way! Te BUNN Pase Brew wit Heat & Release Tecnology is different

More information

Chapter 11 Relative Velocity

Chapter 11 Relative Velocity Chapter 11 Relatie Velocity 11 Relatie Velocity Vector add like ector, not like nuber. Except in that ery pecial cae in which the ector you are adding lie along one and the ae line, you can t jut add the

More information

Theoretical calculation of the heat capacity

Theoretical calculation of the heat capacity eoretical calculation of te eat capacity Principle of equipartition of energy Heat capacity of ideal and real gases Heat capacity of solids: Dulong-Petit, Einstein, Debye models Heat capacity of metals

More information

ú Ó Á É é ú ú É ú Á Á ú É É É ú É Ó É ó É Á ú ú ó Á Á ú Ó ú Ó ú É Á ú Á ú ó ú Á ú Á É Á Á Ó É Á ú ú é ú ú ú ú Á ú ó ú Ó Á Á Á Á ú ú ú é É ó é ó ú ú ú É é ú ú ú óú ú ú Ó Á ú ö é É ú ú ú úé ú ú É É Á É

More information

2 Limits and Derivatives

2 Limits and Derivatives 2 Limits and Derivatives 2.7 Tangent Lines, Velocity, and Derivatives A tangent line to a circle is a line tat intersects te circle at exactly one point. We would like to take tis idea of tangent line

More information

Chapter 22 Heat Engines, Entropy, and the Second Law of Thermodynamics

Chapter 22 Heat Engines, Entropy, and the Second Law of Thermodynamics apter 22 Heat Engnes, Entropy, and te Seond Law o erodynas 1. e Zerot Law o erodynas: equlbru -> te sae 2. e Frst Law o erodynas: de d + d > adabat, sobar, sovoluetr, soteral 22.1 Heat Engnes and te Seond

More information

HYDROLOGY - TUTORIAL 1 UNIFORM FLOW IN CHANNELS

HYDROLOGY - TUTORIAL 1 UNIFORM FLOW IN CHANNELS HYDROLOGY - TUTORIAL 1 UNIFORM FLOW IN CHANNELS In ti tutrial yu will Derive frmula fr flw trug nte. Slve prlem invlving flw trug nte. Define unifrm annel flw. Derive frmulae relating annel dimenin and

More information

Figure 1. Universal Hydraulic Testing Machine

Figure 1. Universal Hydraulic Testing Machine Mechanical Teting Mechanical teting i a general ter which refer to a broad range of activity involved with the deterination of echanical propertie and behavior of aterial, tructure and achine. Typically,

More information

Chapter 7 Numerical Differentiation and Integration

Chapter 7 Numerical Differentiation and Integration 45 We ave a abit in writing articles publised in scientiþc journals to make te work as Þnised as possible, to cover up all te tracks, to not worry about te blind alleys or describe ow you ad te wrong idea

More information

MATHEMATICS FOR ENGINEERING DIFFERENTIATION TUTORIAL 1 - BASIC DIFFERENTIATION

MATHEMATICS FOR ENGINEERING DIFFERENTIATION TUTORIAL 1 - BASIC DIFFERENTIATION MATHEMATICS FOR ENGINEERING DIFFERENTIATION TUTORIAL 1 - BASIC DIFFERENTIATION Tis tutorial is essential pre-requisite material for anyone stuing mecanical engineering. Tis tutorial uses te principle of

More information

HOW TO CALCULATE PRESSURE ANYWHERE IN A PUMP SYSTEM? Jacques Chaurette p. eng. www.lightmypump.com April 2003

HOW TO CALCULATE PRESSURE ANYWHERE IN A PUMP SYSTEM? Jacques Chaurette p. eng. www.lightmypump.com April 2003 HOW TO CALCULATE PRESSURE ANYWHERE IN A PUMP SYSTEM? Jaques Chaurette p. en. www.lihtmypump.om April 003 Synopsis Calulatin the total head of the pump is not the only task of the pump system desiner. Often

More information

Lecture 14: Transformers. Ideal Transformers

Lecture 14: Transformers. Ideal Transformers White, EE 3 Lecture 14 Page 1 of 9 Lecture 14: Tranforer. deal Tranforer n general, a tranforer i a ultiort ac device that convert voltage, current and iedance fro one value to another. Thi device only

More information

GEOTHERMAL POWER PLANT CYCLES AND MAIN COMPONENTS

GEOTHERMAL POWER PLANT CYCLES AND MAIN COMPONENTS Presented at Short Course on Geothermal Drilling, Resource Development and Power Plants, organized by UNU-GTP and LaGeo, in Santa Tecla, El Salvador, January -, 0. GEOTHERMAL TRAINING PROGRAMME LaGeo S.A.

More information

AC 2011-2088: ON THE WORK BY ELECTRICITY IN THE FIRST AND SECOND LAWS OF THERMODYNAMICS

AC 2011-2088: ON THE WORK BY ELECTRICITY IN THE FIRST AND SECOND LAWS OF THERMODYNAMICS AC 2011-2088: ON THE WORK BY ELECTRICITY IN THE FIRST AND SECOND LAWS OF THERMODYNAMICS Hyun W. Kim, Youngstown State University Hyun W. Kim, Ph.D., P.E. Hyun W. Kim is a professor of mechanical engineering

More information

Notes: Most of the material in this chapter is taken from Young and Freedman, Chap. 12.

Notes: Most of the material in this chapter is taken from Young and Freedman, Chap. 12. Capter 6. Fluid Mecanics Notes: Most of te material in tis capter is taken from Young and Freedman, Cap. 12. 6.1 Fluid Statics Fluids, i.e., substances tat can flow, are te subjects of tis capter. But

More information

( C) CLASS 10. TEMPERATURE AND ATOMS

( C) CLASS 10. TEMPERATURE AND ATOMS CLASS 10. EMPERAURE AND AOMS 10.1. INRODUCION Boyle s understanding of the pressure-volue relationship for gases occurred in the late 1600 s. he relationships between volue and teperature, and between

More information

Boiler Calculations. Helsinki University of Technology Department of Mechanical Engineering. Sebastian Teir, Antto Kulla

Boiler Calculations. Helsinki University of Technology Department of Mechanical Engineering. Sebastian Teir, Antto Kulla Helsinki University of Technology Department of Mechanical Engineering Energy Engineering and Environmental Protection Publications Steam Boiler Technology ebook Espoo 2002 Boiler Calculations Sebastian

More information

ESCI 340 Physical Meteorology Cloud Physics Lesson 2 Formation of Cloud Droplets

ESCI 340 Physical Meteorology Cloud Physics Lesson 2 Formation of Cloud Droplets ESCI 40 Phyical Meteorology Cloud Phyic Leon 2 Formation of Cloud Droplet Reference: A Short Coure in Cloud Phyic, Roger and Yau Reading: Roger and Yau, Chapter 6 The objective of thi leon are: 1) Undertand

More information

Chapter 5 Single Phase Systems

Chapter 5 Single Phase Systems Chapter 5 Single Phase Systems Chemial engineering alulations rely heavily on the availability of physial properties of materials. There are three ommon methods used to find these properties. These inlude

More information

f(x + h) f(x) h as representing the slope of a secant line. As h goes to 0, the slope of the secant line approaches the slope of the tangent line.

f(x + h) f(x) h as representing the slope of a secant line. As h goes to 0, the slope of the secant line approaches the slope of the tangent line. Derivative of f(z) Dr. E. Jacobs Te erivative of a function is efine as a limit: f (x) 0 f(x + ) f(x) We can visualize te expression f(x+) f(x) as representing te slope of a secant line. As goes to 0,

More information

Average and Instantaneous Rates of Change: The Derivative

Average and Instantaneous Rates of Change: The Derivative 9.3 verage and Instantaneous Rates of Cange: Te Derivative 609 OBJECTIVES 9.3 To define and find average rates of cange To define te derivative as a rate of cange To use te definition of derivative to

More information

HVAC and REFRIGERATION

HVAC and REFRIGERATION This is a preview. Some pages have been omitted. PE principles and practice prracticce of engineering mechanical: HVAC and REFRIGERATION sample questions + solutions Copyright 2011 by NCEES. All rights

More information

vap H = RT 1T 2 = 30.850 kj mol 1 100 kpa = 341 K

vap H = RT 1T 2 = 30.850 kj mol 1 100 kpa = 341 K Thermodynamics: Examples for chapter 6. 1. The boiling point of hexane at 1 atm is 68.7 C. What is the boiling point at 1 bar? The vapor pressure of hexane at 49.6 C is 53.32 kpa. Assume that the vapor

More information

Projective Geometry. Projective Geometry

Projective Geometry. Projective Geometry Euclidean versus Euclidean geometry describes sapes as tey are Properties of objects tat are uncanged by rigid motions» Lengts» Angles» Parallelism Projective geometry describes objects as tey appear Lengts,

More information

So T decreases. 1.- Does the temperature increase or decrease? For 1 mole of the vdw N2 gas:

So T decreases. 1.- Does the temperature increase or decrease? For 1 mole of the vdw N2 gas: 1.- One mole of Nitrogen (N2) has been compressed at T0=273 K to the volume V0=1liter. The gas goes through the free expansion process (Q = 0, W = 0), in which the pressure drops down to the atmospheric

More information

FUNDAMENTALS OF ENGINEERING THERMODYNAMICS

FUNDAMENTALS OF ENGINEERING THERMODYNAMICS FUNDAMENTALS OF ENGINEERING THERMODYNAMICS System: Quantity of matter (constant mass) or region in space (constant volume) chosen for study. Closed system: Can exchange energy but not mass; mass is constant

More information

Sections 3.1/3.2: Introducing the Derivative/Rules of Differentiation

Sections 3.1/3.2: Introducing the Derivative/Rules of Differentiation Sections 3.1/3.2: Introucing te Derivative/Rules of Differentiation 1 Tangent Line Before looking at te erivative, refer back to Section 2.1, looking at average velocity an instantaneous velocity. Here

More information

Combined make-to-order/make-to-stock supply chains

Combined make-to-order/make-to-stock supply chains IIE Tranaction 2009 41, 103 119 Copyright C IIE ISSN: 0740-817X print / 1545-8830 online DOI: 10.1080/07408170801975065 Cobined ake-to-order/ake-to-tock upply chain PHILIP KAMINSKY 1, and ONUR KAYA 2 1

More information

In other words the graph of the polynomial should pass through the points

In other words the graph of the polynomial should pass through the points Capter 3 Interpolation Interpolation is te problem of fitting a smoot curve troug a given set of points, generally as te grap of a function. It is useful at least in data analysis (interpolation is a form

More information

Purpose of Refrigeration

Purpose of Refrigeration Refrigeration Outline Purpose of refrigeration Examples and applications Choice of coolant and refrigerants Phase diagram of water and CO 2 Vapor compression refrigeration system Pressure enthalpy diagram

More information

The Reduced van der Waals Equation of State

The Reduced van der Waals Equation of State The Redued van der Waals Equation of State The van der Waals equation of state is na + ( V nb) n (1) V where n is the mole number, a and b are onstants harateristi of a artiular gas, and R the gas onstant

More information

Solutions by: KARATUĞ OZAN BiRCAN. PROBLEM 1 (20 points): Let D be a region, i.e., an open connected set in

Solutions by: KARATUĞ OZAN BiRCAN. PROBLEM 1 (20 points): Let D be a region, i.e., an open connected set in KOÇ UNIVERSITY, SPRING 2014 MATH 401, MIDTERM-1, MARCH 3 Instructor: BURAK OZBAGCI TIME: 75 Minutes Solutions by: KARATUĞ OZAN BiRCAN PROBLEM 1 (20 points): Let D be a region, i.e., an open connected set

More information

ACT Math Facts & Formulas

ACT Math Facts & Formulas Numbers, Sequences, Factors Integers:..., -3, -2, -1, 0, 1, 2, 3,... Rationals: fractions, tat is, anyting expressable as a ratio of integers Reals: integers plus rationals plus special numbers suc as

More information

The Dynamics of Movie Purchase and Rental Decisions: Customer Relationship Implications to Movie Studios

The Dynamics of Movie Purchase and Rental Decisions: Customer Relationship Implications to Movie Studios Te Dynamics of Movie Purcase and Rental Decisions: Customer Relationsip Implications to Movie Studios Eddie Ree Associate Professor Business Administration Stoneill College 320 Wasington St Easton, MA

More information

The paper addresses the boil-off in the cryogenic industry and details the specifics of it when applied to vehicle LNG tanks.

The paper addresses the boil-off in the cryogenic industry and details the specifics of it when applied to vehicle LNG tanks. What is Boil-off? Scope... 1 Boil-off in the cryogenic industry... 1... 1 Measures for boil-off... 2 LNG vehicle tanks... 2 Boil-off for the vehicle LNG Tank... 2 Heat management and types of fuel delivery

More information

COMPARISON INVESTIGATION ON THE HEAT TRANSFER CHARACTERISTICS FOR SUPERCRITICAL CO 2 FLUID AND CONVENTIONAL REFRIGERANTS ABSTRACT 1.

COMPARISON INVESTIGATION ON THE HEAT TRANSFER CHARACTERISTICS FOR SUPERCRITICAL CO 2 FLUID AND CONVENTIONAL REFRIGERANTS ABSTRACT 1. COMPARISON INVESTIGATION ON THE HEAT TRANSFER CHARACTERISTICS FOR SUPERCRITICAL CO FLUID AND CONVENTIONAL REFRIGERANTS JUNLAN YANG (a), YITAI MA (b), SHENGCHUN LIU (b), XIANYANG ZENG (b) (a) Department

More information

How To Calculate The Performance Of A Refrigerator And Heat Pump

How To Calculate The Performance Of A Refrigerator And Heat Pump THERMODYNAMICS TUTORIAL 5 HEAT PUMPS AND REFRIGERATION On completion of this tutorial you should be able to do the following. Discuss the merits of different refrigerants. Use thermodynamic tables for

More information

PERFORMANCE ANALYSIS OF VAPOUR COMPRESSION REFRIGERATION SYSTEM WITH R404A, R407C AND R410A

PERFORMANCE ANALYSIS OF VAPOUR COMPRESSION REFRIGERATION SYSTEM WITH R404A, R407C AND R410A Int. J. Mech. Eng. & Rob. Res. 213 Jyoti Soni and R C Gupta, 213 Research Paper ISSN 2278 149 www.ijmerr.com Vol. 2, No. 1, January 213 213 IJMERR. All Rights Reserved PERFORMANCE ANALYSIS OF VAPOUR COMPRESSION

More information

Everest. Leaders in Vacuum Booster Technology

Everest. Leaders in Vacuum Booster Technology This article has been compiled to understand the process of Solvent Recovery process generally carried out at low temperatures and vacuum. In many chemical processes solute is to be concentrated to high

More information

Heat pumps in distillation O.S.L. Bruinsma S. Spoelstra

Heat pumps in distillation O.S.L. Bruinsma S. Spoelstra Heat pumps in distillation O.S.L. ruinsma S. Spoelstra Presented at te istillation & Absorption Conference, 12-15 September 2010, Eindoven, e Neterlands ECN-M--10-090 November 2010 istillation & Absorption

More information

THE USE OF FIBER WOOD AS EVAPORATIVE PAD PACKAGING MATERIAL

THE USE OF FIBER WOOD AS EVAPORATIVE PAD PACKAGING MATERIAL VI CONGRESSO NACIONAL DE ENGENHARIA MECÂNICA VI NAIONAL CONGRESS OF MECHANICAL ENGINEERING 18 a 21 de agoto de 2010 Campina Grande Paraíba - Brail Augut 18 21, 2010 Campina Grande Paraíba Brazil HE USE

More information

Recall Gibbs eqn. ds. Using h version. for ideal gas. integrate AE3450. for ideal gas. integrate s. s(t,p) behavior? AE3450. T p.

Recall Gibbs eqn. ds. Using h version. for ideal gas. integrate AE3450. for ideal gas. integrate s. s(t,p) behavior? AE3450. T p. Enti Shl f Aeae State Engineeing Eqn. Ideal Gae du eall Gibb eqn. d f ideal ga d integate d d d Ideal Ga Enty State elatin - Cyight 03 by Jey M. Seitzman. All ight eeed. d d d d d ln d ln Enti Shl f Aeae

More information

Sheet 5:Chapter 5 5 1C Name four physical quantities that are conserved and two quantities that are not conserved during a process.

Sheet 5:Chapter 5 5 1C Name four physical quantities that are conserved and two quantities that are not conserved during a process. Thermo 1 (MEP 261) Thermodynamics An Engineering Approach Yunus A. Cengel & Michael A. Boles 7 th Edition, McGraw-Hill Companies, ISBN-978-0-07-352932-5, 2008 Sheet 5:Chapter 5 5 1C Name four physical

More information

APPLIED THERMODYNAMICS TUTORIAL 1 REVISION OF ISENTROPIC EFFICIENCY ADVANCED STEAM CYCLES

APPLIED THERMODYNAMICS TUTORIAL 1 REVISION OF ISENTROPIC EFFICIENCY ADVANCED STEAM CYCLES APPLIED THERMODYNAMICS TUTORIAL 1 REVISION OF ISENTROPIC EFFICIENCY ADVANCED STEAM CYCLES INTRODUCTION This tutorial is designed for students wishing to extend their knowledge of thermodynamics to a more

More information

SAT Subject Math Level 1 Facts & Formulas

SAT Subject Math Level 1 Facts & Formulas Numbers, Sequences, Factors Integers:..., -3, -2, -1, 0, 1, 2, 3,... Reals: integers plus fractions, decimals, and irrationals ( 2, 3, π, etc.) Order Of Operations: Aritmetic Sequences: PEMDAS (Parenteses

More information

BASIC UNDERSTANDING OF FLOW CALCULATIONS AND ESTIMATES MAKES SIZING VALVES SIMPLER

BASIC UNDERSTANDING OF FLOW CALCULATIONS AND ESTIMATES MAKES SIZING VALVES SIMPLER BASIC UNDERSTANDING OF FLOW CALCULATIONS AND ESTIMATES MAKES SIZING VALVES SIMPLER Valve size often is described by the nominal size of the end connections but a more important measure is the flow that

More information

The EOQ Inventory Formula

The EOQ Inventory Formula Te EOQ Inventory Formula James M. Cargal Matematics Department Troy University Montgomery Campus A basic problem for businesses and manufacturers is, wen ordering supplies, to determine wat quantity of

More information

Fundamentals of THERMAL-FLUID SCIENCES

Fundamentals of THERMAL-FLUID SCIENCES Fundamentals of THERMAL-FLUID SCIENCES THIRD EDITION YUNUS A. CENGEL ROBERT H. TURNER Department of Mechanical JOHN M. CIMBALA Me Graw Hill Higher Education Boston Burr Ridge, IL Dubuque, IA Madison, Wl

More information

AN INTRODUCTION TO THE CONCEPT OF EXERGY AND ENERGY QUALITY. Truls Gundersen

AN INTRODUCTION TO THE CONCEPT OF EXERGY AND ENERGY QUALITY. Truls Gundersen AN INRODUION O HE ONEP OF EXERGY AND ENERGY QUALIY by ruls Gundersen Department of Energy and Process Engineering Norwegian University of Science and echnology rondheim, Norway Version 4, March 211 ruls

More information

Verifying Numerical Convergence Rates

Verifying Numerical Convergence Rates 1 Order of accuracy Verifying Numerical Convergence Rates We consider a numerical approximation of an exact value u. Te approximation depends on a small parameter, suc as te grid size or time step, and

More information

Work, Energy, Conservation of Energy

Work, Energy, Conservation of Energy This test covers Work, echanical energy, kinetic energy, potential energy (gravitational and elastic), Hooke s Law, Conservation of Energy, heat energy, conservative and non-conservative forces, with soe

More information

How To Power A Car With A Fan And A Fan (Power)

How To Power A Car With A Fan And A Fan (Power) SPLIT TYPE ROO AIR CONDITIONER CEILING WALL TYPE INVERTER Indoor unit AWYZLBC AWYZLBC AWYZLBC AWYZLBC Outdoor unit AOYZLBC AOYZLBL AOYZLBC AOYZLBL CONTENTS SPECIFICATIONS................... OUTLINE AND

More information

Pipe Flow Calculations

Pipe Flow Calculations Pipe Flow Calculation R. Shankar Subramanian epartment o Chemical and Biomolecular Engineering Clarkon Univerity We begin with ome reult that we hall ue when making riction lo calculation or teady, ully

More information

Geometric Stratification of Accounting Data

Geometric Stratification of Accounting Data Stratification of Accounting Data Patricia Gunning * Jane Mary Horgan ** William Yancey *** Abstract: We suggest a new procedure for defining te boundaries of te strata in igly skewed populations, usual

More information

2004 Standard For Performance Rating Of Positive Displacement Refrigerant Compressors And Compressor Units

2004 Standard For Performance Rating Of Positive Displacement Refrigerant Compressors And Compressor Units 2004 Standard For Performance Rating Of Positive Displacement Refrigerant Compressors And Compressor Units ANSI/AHRI Standard 540 (formerly ARI Standard 540) IMPORTANT SAFETY RECOMMENDATIONS ARI does not

More information

M(0) = 1 M(1) = 2 M(h) = M(h 1) + M(h 2) + 1 (h > 1)

M(0) = 1 M(1) = 2 M(h) = M(h 1) + M(h 2) + 1 (h > 1) Insertion and Deletion in VL Trees Submitted in Partial Fulfillment of te Requirements for Dr. Eric Kaltofen s 66621: nalysis of lgoritms by Robert McCloskey December 14, 1984 1 ackground ccording to Knut

More information

High Pressure Ammonia Systems New Opportunities

High Pressure Ammonia Systems New Opportunities Purdue University Purdue e-pubs International Refrigeration and Air Conditioning Conference School of Mechanical Engineering 2010 High Pressure Ammonia Systems New Opportunities Andy Pearson Star Refrigeration

More information