ES-7A Thermodynamics HW 8: 9-22, 29, 67, 84; 10-11, 19, 38, 86 Spring 2003 Page 1 of 9

Size: px
Start display at page:

Download "ES-7A Thermodynamics HW 8: 9-22, 29, 67, 84; 10-11, 19, 38, 86 Spring 2003 Page 1 of 9"

Transcription

1 ES-7A ermodynamic HW : 9-, 9, 7, ; 0-, 9,, Sprg 00 Page of 9 9- Ideal Ranke Cycle Given: Steam power plant wit ideal Ranke cycle. Net power output i MW. Steam enter te at 7 MPa and 00 C. e team i cooled te at 0 kpa ug coolg water at a rate of 000 kg/. Fd: a) termal efficiency of te cycle, b) ma flow rate of te team, and c) temperature rie of te coolg water. Draw te - diagram. At tate, P 7 MPa and 00 C. We ave upereated vapor: 0. kj/kg and.797 kj/kgk. boiler At tate, and P 0 kpa. At 0 kpa, f 0.9 kj/kgk and fg kj/kgk x f 9. kj/kg and fg 9. kj/kgk. kj/kg. At tate, we ave aturated liquid at 0 kpa v v f m /kg, f 9. kj/kg. e work conumed by te i: w v (P P ) (0 7000) kj/kg. State i found by: w w 9. (-7.099) 9.9 kj.kg. e work produced by te i: w kj/kg. a) e termal efficiency i: w w + w net η t 0.9, or.9 percent. q b) e ma flow rate i: MW/w net,000/0..99 kg/. Q & m& MW. c) e eat given off te i: ( ) ( ) i amount of eat i beg aborbed by te coolg water: Q & m& c Q& m& c 7000 ( 000. ). C. cw cw p cw cw p e - diagram i own on te rigt. Some of te feature are: o tate i aturated liquid o tate i aturated mixture o tate i upereated o and are ientropic o P P ; P P.

2 ES-7A ermodynamic HW : 9-, 9, 7, ; 0-, 9,, Sprg 00 Page of Reeat Ranke Cycle Given: Steam power plant tat operate on a reeat Rake cycle wit 0 MW of net output. Steam enter te ig preure at 0 MPa and 00 C, and te low preure at MPa and 00 C. Steam leave te a a aturated liquid at 0 kpa. Ientropic efficiencie of te and compreor are 0 percent and 9 percent, repectively. Fd: a) quality or temperature of team at exit, b) termal efficiency of te cycle, and c) ma flow rate of te team. Draw te - diagram. State i aturated liquid at 0 kpa: f 9. kj/kg, v v f m /kg. State i at 0 MPa. e ideal work of te i: w v (P P ) v (P P ) (0 0,000) 0.9 kj/kg. State a i found from te ientropic efficiency of te compreor: η c ( )/( a ) a ( )/η c + (0.9 9.)/ kj/kg. State i at 0 MPa and 00 C: 7.7 kj/kg,.9 kj/kgk. State i at MPa and : terpolate between at and 00 C to get 7.7 kj/kg. State a i found from te ientropic efficiency of : η t ( a )/( ) a η t ( ) + 0.( ) kj/kg. State i at MPa and 00 C: 7. kj/kg, 7.7 kj/kgk. State i at 0 kpa and : i i aturated mixture. f 0.9 kj/kgk, fg kj/kgk. x ( f )/ fg ( )/ f 9. kj/kg, fg 9. kj/kg 0. kj/kg. State a i found from te ientropic efficiency of : a η t ( ) + 0.(0. 7.) kj/kg. a) i i greater tan g, o we ave a upereated vapor. Interpolate between 0 C and 00 C to fd 7. C. b) e termal efficiency of te reeat cycle i given by: η t w q net , or.0 percent. 79. c) e ma flow rate i given by: 0 MW/w net 0,000 /7.. kg/. e important feature of te - diagram are: o tate i aturated liquid o tate i aturated mixture o tate,, a,, a are upereated o ; P P ; P P ; P P. boiler a a a

3 ES-7A ermodynamic HW : 9-, 9, 7, ; 0-, 9,, Sprg 00 Page of Combed ga-team power plant Given: Combed ga-team power plant wit net power output of 0 MW. Ga cycle a a preure ratio of. Air enter te compreor at 00 K and te at 00 K. e combution gae at exaut i ued to eat te team at MPa to 00 C a eat excanger. e combution gae leave te eat excanger at 0 K. An open feedwater eater te team cycle operate at 0. MPa. e preure i 0 kpa. Fd: a) ma flow rate ratio of air to team; b) required eat put to te combution camber; c) termal efficiency of te combed cycle. e air cycle i an ideal Brayton cycle. Ug variable pecific eat: State : 00 K 00.9 kj/kg, P r.0 State : P P r Pr P Interpolate between 0 K and 0 K. kj/kg. State : 00 K. kj/kg, P r 0. State : P P r Pr 0./.79 P Interpolate between 70 K and 70 K 7. kj/kg. comp. State *: At te exaut of te eat excanger, * 0 K *.0 kj/kg. * combution camber eat excanger open 7 FWH 0 9 e team cycle i a regenerative Ranke cycle wit open feedwater eater. State i a aturated liquid at 0 kpa:.0 kj/kg, v m /kg. State i at te feedwater preure of 0. MPa. w, v (P P ) (0 00) kj/kg. w,.0 (-0.99).99 kj/kg. State 7 i aturated liquid at 0. MPa: kj/kg, v m /kg. State i at MPa. w, v 7 (P 7 P ) 0.000(00 000) -.7 kj/kg. 7 w, 70. (-.7) 7.7 kj/kg. State 9 i at MPa and 00 C: 9. kj/kg, 9. kj/kgk. State 0 i at 0. MPa and 0 9 : f.9 kj/kgk and fg. kj/kgk x f 70. kj/kg, fg 0. kj/kg 0. kj/kg State i at 0 kpa and 9 : f 0.0 kj/kgk and fg 7.07 kj/kgk x 0.7. f.0 kj/kg, fg. kj/kg 09.7 kj/kg Heat balance around te open FWH to fd y: y 0 + ( y) y

4 ES-7A ermodynamic HW : 9-, 9, 7, ; 0-, 9,, Sprg 00 Page of (contued) a) e air-to-team ratio i found from eat balance around te eat excanger: m& m& air ( * ) m& team ( 9 ) m& b) We firt need to fd te ma flow rate. air team * e net work of te Brayton cycle i: w net,b kj/kg of air. e work from te Ranke cycle i: w,r y( 9 0 ) + ( y)( 9 ) 0.79(..) + ( 0.79)(. 09.7) 9.70 kj/kg of team. e net work from te Ranke cycle i: w net,r w, + w, + w,r (-0.99) + (-.7) kj/kg. e net work i: & & & & + & W net mair w net, B + m teamw net, R. 9m teamw net, B m teamw net, R Rearrange to olve for ma flow rate: W& net 0,000 m& team 9.9 kg/ of team.9w net, B + w net, R.9(. ) m &. 9 &. kg/ of air air m team e required eat put i: Q m& ( ) & air.(..) 70. MW. c) e termal efficiency i: η W & Q& , or. percent. t net 9- Reeat-Regenerative Ranke Cycle Given: Ideal reeat-regenerative Ranke cycle wit one open feedwater eater. e boiler preure i 0 MPa, preure i kpa, reeater preure i MPa, and feedwater preure i 0. MPa. Steam enter te ig and low preure at 00 C. Fd: a) fraction of team extracted for regeneration (y), and b) termal efficiency of te cycle. Draw te - diagram. State i aturated liquid at te preure of kpa:.9 kj/kg, v m /kg. State i at te feedwater preure of 0. MPa: w, v (P P ) 0.000( 00) -0.9 kj/kg. w,.9 (-0.9). kj/kg. State i aturated liquid at 0. MPa: 70. kj/kg, v m /kg. State i at te boiler preure of 0 MPa: w, v (P P ) 0.000(00 0,000) -0.9 kj/kg. w, 70. (-0.9) 0.9 kj/kg. boiler open FWH 7 9

5 ES-7A ermodynamic HW : 9-, 9, 7, ; 0-, 9,, Sprg 00 Page of 9 9- (contued) State i at 0 MPa and 00 C: 7.7 kj/kg,.9 kj/kgk. State i at te reeater preure of MPa and : Interpolate between at. temperature and 00 C 7.7 kj/kg. State 7 i at MPa and 00 C: 7 7. kj/kg, kj/kgk. State i at 0. MPa and 7 : terpolate between 00 C and 00 C 09. kj/kg. State 9 i at kpa and 9 7 : x 9 0.9, 9. kj/kg. a) e fraction of team extracted for regeneration i found from a eat balance around te open feedwater eater: y + ( y) 70.. y b) e termal efficiency of te cycle i found from w net /q. e work for te ig-preure i: w, kj/kg. e work for te low-preure i: w, y( 7 ) + ( y)( 7 9 ) 0.(7. 09.) + ( 0.)(7..). kj/kg. e net work i: w, + w, + w, + w, kj/kg. e eat put i: q kj/kg. e termal efficiency i: w net /q./. 0.09, or. percent. e - diagram ould ave te followg feature: o tate and are aturated liquid 7 o tate,, 7, are upereated vapor o tate 9 i aturated mixture o P P 9 ; P P P ; P P ; P P 7 o,,, and 7 9 are ientropic o tate and 7 ave te ame temperature 9

6 ES-7A ermodynamic HW : 9-, 9, 7, ; 0-, 9,, Sprg 00 Page of 9 0- Ideal Refrigeration Cycle Given: An ideal vapor-compreion refrigeration cycle ue R-a between 0. and 0.7 MPa. e ma flow rate i 0.0 kg/. Fd: a) Rate of eat removal from refrigerated pace and te power put to te compreor; b) rate of eat rejection to te environment; and c) coefficient of performance. Draw te - diagram. State i aturated vapor at 0. MPa g. kj/kg, g 0.9 kj/kgk. State i at 0.7 MPa, and. Interpolate beween 0 C and 0 C to get 70. kj/kg. State i aturated liquid at 0.7 MPa. f.7 kj/kg. State i at 0. MPa, and. a) e eat removal from refrigerated pace i between tate and : ( ) 0.0. (.7) & m& 7. kw. Q e power put to te compreor i between tate and : ( ) 0.0. ( 70.) & m& -. kw, or. kw of power put. W b) Heat i rejected between tate and : & m& kw, or 9.7 kw of eat rejected. Q out ( ) ( ) c) COP Q & & W eat excanger comp. e - diagram i caracterized by: o tate i aturated vapor o tate i upereated vapor o tate i aturated liquid o tate i aturated mixture o P P ; P P. o i ientropic

7 ES-7A ermodynamic HW : 9-, 9, 7, ; 0-, 9,, Sprg 00 Page 7 of Non-Ideal Refrigeration Cycle Given: R-a enter te compreor of a refrigeration cycle at 0 kpa and -0 C at a rate of 0. m /m, and leave at MPa. e ientropic efficiency of te compreor i 7 percent. e refrigerant enter te trottlg valve at 0.9 MPa and 0 C, and leave te evaporator a aturated vapor at -. C. Fd: a) Power put to te compreor; b) rate of eat removal from te refrigerated pace; and c) preure drop and te rate of eat gaed te le between evaporator and compreor. Draw te - diagram. State i upereated at 0 kpa and -0 C:.0 kj/kg, 0.90 kj/kgk, v 0.9 m /kg. e ma flow rate i: m m V& 0. m 0ec m& 0.07 kg/ v 0.9 State i at MPa, and. Interpolate between 0 C and 0 C to get.0 kj/kg. State can be found from te ientropic efficiency of te compreor. η c ( )/( a ) a ( )/η c + (.0.0)/ kj/kg. State i at 0.9 MPa and 0 C, wic i a compreed liquid. We will ue te propertie of aturated liquid at 0 C: 9.9 kj/kg. State i a aturated mixture at -. C, and. State * i a aturated vapor at -. C. We can terpolate between -0 C and - C to fd *. kj/kg and P * P at.7 kpa. a) e power put to te compreor i between tate and : ( ) ( 9.07) W & & -.79 kw, or.79 kw of power put. m a b) e eat removal from refrigerated pace i between tate and *: & m& kw. Q ( ) ( ) * c) e preure drop between tate * and i: kpa. & 0. kw e rate of eat gaed i: Q m& ( * ) (.) evaporator * comp. e - diagram i caracterized by: a o tate * i aturated vapor o tate,, and a are upereated vapor o tate i compreed liquid o tate i aturated mixture * o P P ; P P * o i ientropic

8 ES-7A ermodynamic HW : 9-, 9, 7, ; 0-, 9,, Sprg 00 Page of 9 0- Cacade Refrigeration Cycle Given: wo-tage cacade refrigeration ytem operatg between 0. MPa and 0. MPa. Eac tage i an ideal vapor-compreion cycle wit R-a. Heat rejection from te lower cycle to te upper cycle take place an adiabatic eat excanger were bot tream enter at 0. MPa. e ma flow rate of te refrigerant troug te upper cycle i 0. kg/. Fd: a) ma flow rate of te refrigerant troug lower cycle; b) rate of eat removal from te refrigerated pace and te power put to te compreor; c) coefficient of performance. Lower Cycle: State i a aturated vapor at 0. MPa.0 kj/kg, 0.9 kj/kgk. State i at 0. MPa and. Interpolate between 0 C and 0 C to get 7.9 kj/kg. State i a aturated liquid at 0. MPa.00 kj/kg. State i a aturated mixture at 0. MPa, and. Upper Cycle: State i a aturated vapor at 0. MPa. kj/kg, 0.9 kj/kgk. State i at 0. MPa and. Interpolate between at and 0 C to get.9 kj/kg. State 7 i a aturated liquid at 0. MPa 9. kj/kg. State i a aturated mixture at 0. MPa, and. 7 eat excanger evaporator comp. comp. a) e ma flow rate of te lower cycle i found from a eat balance around te eat excanger: m& U ( ) m& ( ) L. 9. m& m& L U kg/ b) e eat removal from refrigerated pace i between tate and : ( ) (.00) Q& m&.97 kw. L e total power put to te compreor i: W& m& + m& L ( ) U ( ) ( 7.9) + 0.(..9) kw, or 7. kw power put. c) e coefficient of performance i: COP Q & & W

9 ES-7A ermodynamic HW : 9-, 9, 7, ; 0-, 9,, Sprg 00 Page 9 of 9 0- Heat Pump Given: A eat operate on an ideal vapor-compreion cycle wit R-a. e ma flow rate i 0. kg/. e condenor and evaporator preure are 900 kpa and 0 kpa, repectively. Fd: a) rate of eat upplied to te oue; b) volume flow of te refrigerant at te compreor let; and c) coefficient of performance of te eat. Sow te - diagram. State i a aturated vapor at 0 kpa.09 kj/kg, 0.9 kj/kgk, v 0.0 m /kg. State i at 900 kpa and. Interpolate between 0 C and 0 C to get 7. kj/kg. State i a aturated liquid at 900 kpa 99. kj/kg. State i a aturated mixture at 0 kpa, and. eat excanger comp. a) e eat upplied to te oue come from te, : ( ) ( 7.) & m& -. kw, or. kw upplied to te oue. Q out b) e volume flow rate of te refrigerant at te compreor let (tate ) i: V & m & v m /. ( ) c) e coefficient of performance i: Q& COP W& & W out ( ) 0.(.09 7.) m& COP./ kw, or.7 kw power put. e - diagram a te followg feature: o tate i aturated vapor o tate i upereated vapor o tate i aturated liquid o i ientropic o P P ; P P.

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

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

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

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

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 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

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 apter 7 Exaple 7.- 6 ---------------------------------------------------------------------------------- Refrigerant 4a i te working fluid in an ideal vapor-opreion refrigeration yle tat ouniate terally

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

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

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

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

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

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

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

ME 201 Thermodynamics

ME 201 Thermodynamics ME 0 Thermodynamics Second Law Practice Problems. Ideally, which fluid can do more work: air at 600 psia and 600 F or steam at 600 psia and 600 F The maximum work a substance can do is given by its availablity.

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

An analysis of a thermal power plant working on a Rankine cycle: A theoretical investigation

An analysis of a thermal power plant working on a Rankine cycle: A theoretical investigation An analysis of a thermal power plant working on a Rankine cycle: A theoretical investigation R K Kapooria Department of Mechanical Engineering, BRCM College of Engineering & Technology, Bahal (Haryana)

More information

C H A P T E R T W O. Fundamentals of Steam Power

C H A P T E R T W O. Fundamentals of Steam Power 35 C H A P T E R T W O Fundamentals of Steam Power 2.1 Introduction Much of the electricity used in the United States is produced in steam power plants. Despite efforts to develop alternative energy converters,

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

6 18 A steam power plant receives heat from a furnace at a rate of 280 GJ/h. Heat losses to the surrounding air from the steam as it passes through

6 18 A steam power plant receives heat from a furnace at a rate of 280 GJ/h. Heat losses to the surrounding air from the steam as it passes through 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 6:Chapter 6 6 17 A 600-MW steam power

More information

1. A belt pulley is 3 ft. in diameter and rotates at 250 rpm. The belt which is 5 ins. wide makes an angle of contact of 190 over the pulley.

1. A belt pulley is 3 ft. in diameter and rotates at 250 rpm. The belt which is 5 ins. wide makes an angle of contact of 190 over the pulley. Sample Questions REVISED FIRST CLASS PARTS A1, A2, AND A3 (NOTE: these questions are intended as representations of the style of questions that may appear on examinations. They are not intended as study

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

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

The Second Law of Thermodynamics

The Second Law of Thermodynamics The Second aw of Thermodynamics The second law of thermodynamics asserts that processes occur in a certain direction and that the energy has quality as well as quantity. The first law places no restriction

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

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

Air-sourced 90 Hot Water Supplying Heat Pump "HEM-90A"

Air-sourced 90 Hot Water Supplying Heat Pump HEM-90A Air-sourced 90 Hot Water Supplying Heat Pump "HEM-90A" Takahiro OUE *1, Kazuto OKADA *1 *1 Refrigeration System & Energy Dept., Compressor Div., Machinery Business Kobe Steel has developed an air-sourced

More information

Energy Analysis and Comparison of Advanced Vapour Compression Heat Pump Arrangements

Energy Analysis and Comparison of Advanced Vapour Compression Heat Pump Arrangements Energy Analysis and Comparison of Advanced Vapour Compression Heat Pump Arrangements Stuart Self 1, Marc Rosen 1, and Bale Reddy 1 1 University of Ontario Institute of Technology, Oshawa, Ontario Abstract

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

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

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

2B.1 Chilled-Water Return (and Supply) Temperature...119. 2B.3 Cooling-Water Supply Temperature / Flow... 124

2B.1 Chilled-Water Return (and Supply) Temperature...119. 2B.3 Cooling-Water Supply Temperature / Flow... 124 Appendix 2B: Chiller Test Results...119 2B.1 Chilled-Water Return (and Supply) Temperature...119 2B.2 Chilled-Water Flow... 122 2B.3 Cooling-Water Supply Temperature / Flow... 124 2B.4 Pressure/Temperature...

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

THE PSYCHROMETRIC CHART: Theory and Application. Perry Peralta NC State University

THE PSYCHROMETRIC CHART: Theory and Application. Perry Peralta NC State University THE PSYCHROMETRIC CHART: Theory and Application Perry Peralta NC State University PSYCHROMETRIC CHART Identify parts of the chart Determine moist air properties Use chart to analyze processes involving

More information

DET: Mechanical Engineering Thermofluids (Higher)

DET: Mechanical Engineering Thermofluids (Higher) DET: Mechanical Engineering Thermofluids (Higher) 6485 Spring 000 HIGHER STILL DET: Mechanical Engineering Thermofluids Higher Support Materials *+,-./ CONTENTS Section : Thermofluids (Higher) Student

More information

Daikin Altherma hybrid heat pump. The natural combination

Daikin Altherma hybrid heat pump. The natural combination Daikin Altherma hybrid heat pump The natural combination Daikin Altherma hybrid heat pump, the natural combination Why choose Daikin Altherma hybrid heat pump? What the customer wants: more energy efficient

More information

FEASIBILITY OF A BRAYTON CYCLE AUTOMOTIVE AIR CONDITIONING SYSTEM

FEASIBILITY OF A BRAYTON CYCLE AUTOMOTIVE AIR CONDITIONING SYSTEM FEASIBILITY OF A BRAYTON CYCLE AUTOMOTIVE AIR CONDITIONING SYSTEM L. H. M. Beatrice a, and F. A. S. Fiorelli a a Universidade de São Paulo Escola Politécnica Departamento de Engenharia Mecânica Av. Prof.

More information

Chapter 3.4: HVAC & Refrigeration System

Chapter 3.4: HVAC & Refrigeration System Chapter 3.4: HVAC & Refrigeration System Part I: Objective type questions and answers 1. One ton of refrigeration (TR) is equal to. a) Kcal/h b) 3.51 kw c) 120oo BTU/h d) all 2. The driving force for refrigeration

More information

Research on the Air Conditioning Water Heater System

Research on the Air Conditioning Water Heater System Purdue University Purdue e-pubs International Refrigeration and Air Conditioning Conference School of Mechanical Engineering 28 Research on the Air Conditioning Water Heater System Fei Liu Gree Electric

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

Stirling heat engine Internal combustion engine (Otto cycle) Diesel engine Steam engine (Rankine cycle) Kitchen Refrigerator

Stirling heat engine Internal combustion engine (Otto cycle) Diesel engine Steam engine (Rankine cycle) Kitchen Refrigerator Lecture. Real eat Engines and refrigerators (Ch. ) Stirling heat engine Internal combustion engine (Otto cycle) Diesel engine Steam engine (Rankine cycle) Kitchen Refrigerator Carnot Cycle - is not very

More information

The Second Law of Thermodynamics

The Second Law of Thermodynamics Objectives MAE 320 - Chapter 6 The Second Law of Thermodynamics The content and the pictures are from the text book: Çengel, Y. A. and Boles, M. A., Thermodynamics: An Engineering Approach, McGraw-Hill,

More information

THEORETICAL ANALYSIS OF THE PERFORMANCE OF DUAL PRESSURE CONDENSER IN A THERMAL POWER PLANT

THEORETICAL ANALYSIS OF THE PERFORMANCE OF DUAL PRESSURE CONDENSER IN A THERMAL POWER PLANT INTERNATIONAL JOURNAL OF MECHANICAL ENGINEERING AND TECHNOLOGY (IJMET) International Journal of Mechanical Engineering and Technology (IJMET), ISSN 0976 6340(Print), ISSN 0976 6340 (Print) ISSN 0976 6359

More information

Business Model of Micro-Chp Efficiency and Energy Requirements

Business Model of Micro-Chp Efficiency and Energy Requirements Micro Cooling, Heating, and Power (Micro-CHP) and Bio-Fuel Center Mississippi State University 1. THERMOECONOMIC MODELING OF MICRO-CHP (MICRO-COOLING, HEATING, AND POWER) FOR SMALL COMMERCIAL APPLICATIONS

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

Air Water Vapor Mixtures: Psychrometrics. Leon R. Glicksman c 1996, 2010

Air Water Vapor Mixtures: Psychrometrics. Leon R. Glicksman c 1996, 2010 Air Water Vapor Mixtures: Psychrometrics Leon R. Glicksman c 1996, 2010 Introduction To establish proper comfort conditions within a building space, the designer must consider the air temperature and 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

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

Test Report issued under the responsibility of:

Test Report issued under the responsibility of: Test Report issued under the responsibility of: TEST REPORT EHPA-DACH Testing Regulation Supplemental requirements for granting the international quality label for heat pumps Testing of Air/Water Heat

More information

POSSIBILITY FOR MECHANICAL VAPOR RE-COMPRESSRION FOR STEAM BASED DRYING PROCESSES

POSSIBILITY FOR MECHANICAL VAPOR RE-COMPRESSRION FOR STEAM BASED DRYING PROCESSES POSSIBILITY FOR MECHANICAL VAPOR RE-COMPRESSRION FOR STEAM BASED DRYING PROCESSES M. Bantle 1, I. Tolstorebrov, T. M. Eikevik 2 1 Department of Energy Efficiency, SINTEF Energy Research, Trondheim, Norway,

More information

HVAC Efficiency Definitions

HVAC Efficiency Definitions HVAC Efficiency Definitions Term page EER - 2 SEER - 3 COP - 4 HSPF - 5 IPLV - 6 John Mix May 2006 Carrier Corporation 1 Energy Efficiency Ratio (EER) The energy efficiency ratio is used to evaluate the

More information

Research Article Performance Evaluation of a Small Scale Modular Solar Trigeneration System

Research Article Performance Evaluation of a Small Scale Modular Solar Trigeneration System Photoenergy, Article ID 964021, 9 pages http://dx.doi.org/10.1155/2014/964021 Research Article Performance Evaluation of a Small Scale Modular Solar Trigeneration System Handong Wang M. & E. School of

More information

Development of Air-to-Water Heat Pump for Home Air conditioning/hot Water Supply Combination System with Chilled/Hot Water in European Markets

Development of Air-to-Water Heat Pump for Home Air conditioning/hot Water Supply Combination System with Chilled/Hot Water in European Markets 2 Development of Air-to-Water Heat Pump for Home Air conditioning/hot Water Supply Combination System with Chilled/Hot Water in European Markets - Extending Use of New Heat Pump System in Cold Regions

More information

Forgotten savings: Heat recovery from surface blowdown

Forgotten savings: Heat recovery from surface blowdown Forgotten savings: Heat recovery from surface blowdown 1. Introduction The purpose of this article is to inform thermal plant operators of the interesting fuel savings that can be obtained by recovering

More information

LG Electronics AE Company, Commercial Air Conditioning

LG Electronics AE Company, Commercial Air Conditioning www.lgeaircon.com New concept Ecofriendly Highefficiency Heating solution Total heating & Hot water Solution for MULTI V LG Electronics AE Company, Commercial Air Conditioning 2 Yeouidodong, Yeongdeungpogu,

More information

How To Know If A Refrigeration System Is Efficient

How To Know If A Refrigeration System Is Efficient Universitatea de Ştiinţe Agricole şi Medicină Veterinară Iaşi ASSESSMENT OF E SUBCOOLING CAPABILITIES OF A ERMOELECTRIC DEVICE IN A VAPOR COMPRESSION REFRIGERATION SYSTEM R. ROŞCA 1, I. ŢENU 1, P. CÂRLESCU

More information

Regency TAFE, SA. An evaluation of the effects of PermaFrost treatment on a Fujitsu Heat Pump. July 2008. Prepared by

Regency TAFE, SA. An evaluation of the effects of PermaFrost treatment on a Fujitsu Heat Pump. July 2008. Prepared by Regency TAFE, SA An evaluation of the effects of PermaFrost treatment on a Fujitsu Heat Pump July 2008 Prepared by Andrew Pang Andrew Pang & Associates Pty Ltd Phone: 0438 188 180 Facsimile: 9331 0898

More information

GLOBACON 05 HVAC Systems for Cogen

GLOBACON 05 HVAC Systems for Cogen GLOBACON 05 HVAC Systems for Cogen Track 2, Session 2B Advanced HVAC and Building Systems Date: March 24th, 2005 Gearoid Foley President Integrated CHP Systems Corp. Integrated CHP Systems Corp. Electricity

More information

0.002432 1.002432. where x is check for normality T 105.67 5.2546

0.002432 1.002432. where x is check for normality T 105.67 5.2546 6 PRACTICAL NUMERICAL METHODS Chapter 3 VBA Practice Problem Ue Excel and VBA to olve the following problem. Document your olution uing the Expert Problem Solving tep outlined in Table 1.2. 1.961 x 0.5

More information

Condensers & Evaporator Chapter 5

Condensers & Evaporator Chapter 5 Condensers & Evaporator Chapter 5 This raises the condenser temperature and the corresponding pressure thereby reducing the COP. Page 134 of 263 Condensers & Evaporator Chapter 5 OBJECTIVE QUESTIONS (GATE,

More information

AIR CONDITION & REFRIGERATION INSTALLATION & REPAIR

AIR CONDITION & REFRIGERATION INSTALLATION & REPAIR AIR CONDITION & REFRIGERATION INSTALLATION & REPAIR SERVICE CAPACITY (Value) : Rs. 15,40,000/- MONTH AND YEAR : July, 2014 OF PREPARATION PREPARED BY : Sh. Sunil Arora Investigator (Mechanical) 1. INTRODUCTION

More information

Modelling and Simulation of the Freezing Systems and Heat Pumps Using Unisim Design

Modelling and Simulation of the Freezing Systems and Heat Pumps Using Unisim Design Modelling and Simulation of the Freezing Systems and Heat Pumps Using Unisim Design C. Patrascioiu Abstract The paper describes the modeling and simulation of the heat pumps domain processes. The main

More information

Efficiency of Hydrogen Liquefaction Plants

Efficiency of Hydrogen Liquefaction Plants Efficiency of Hydrogen Liquefaction Plants Takashi FUKANO**, Urs FITZI*, Karl LÖHLEIN*, Isabelle VINAGE* * Linde Kryotechnik AG, CH-8422 Pfungen, Switzerland ** Nippon Sanso Corporation, JP-210-0861 Kawasaki-City,

More information

The final numerical answer given is correct but the math shown does not give that answer.

The final numerical answer given is correct but the math shown does not give that answer. Note added to Homework set 7: The solution to Problem 16 has an error in it. The specific heat of water is listed as c 1 J/g K but should be c 4.186 J/g K The final numerical answer given is correct but

More information

PERFORMANCE EVALUATION OF NGCC AND COAL-FIRED STEAM POWER PLANTS WITH INTEGRATED CCS AND ORC SYSTEMS

PERFORMANCE EVALUATION OF NGCC AND COAL-FIRED STEAM POWER PLANTS WITH INTEGRATED CCS AND ORC SYSTEMS ASME ORC 2015 3rd International Seminar on ORC Power Systems 12-14 October 2015, Brussels, Belgium PERFORMANCE EVALUATION OF NGCC AND COAL-FIRED STEAM POWER PLANTS WITH INTEGRATED CCS AND ORC SYSTEMS Vittorio

More information

ARP Food Industry, Portugal

ARP Food Industry, Portugal Food Industry, Portugal In a Portuguese food company colibri will install a twostage ammonia-water-absorption refrigeration system. The 1st refrigeration stage provides the customer with liquid ammonia

More information

HEAT PUMPS A KEY COMPONENT IN LOW CARBON FUTURE

HEAT PUMPS A KEY COMPONENT IN LOW CARBON FUTURE HEAT PUMPS A KEY COMPONENT IN LOW CARBON FUTURE Satish Joshi Managing Director CONTENTS 1. INTRODUCTION, APPLICATIONS 2. TECHNOLOGY, PROJECTS DONE, COST COMPARISION 3. HEAT PUMPS IN THE RENEWABLES DIRECTIVE,

More information

A Comparison of an R22 and an R410A Air Conditioner Operating at High Ambient Temperatures

A Comparison of an R22 and an R410A Air Conditioner Operating at High Ambient Temperatures R2-1 A Comparison of an R22 and an R410A Air Conditioner Operating at High Ambient Temperatures W. Vance Payne and Piotr A. Domanski National Institute of Standards and Technology Building Environment

More information

CONTROL VALVE PRESSURE DROP AND SIZING

CONTROL VALVE PRESSURE DROP AND SIZING CONTENT Chapter Description Page I Purpose of Control Valve II Type and Main Components of Control Valve 3 III Power 5 IV. Pressure Drop Across Control Valve 7 V. Symbols and Units 10 VI. Unit Conversion

More information

Performance Evaluation of a Heat Pump System for Simultaneous Heating and Cooling

Performance Evaluation of a Heat Pump System for Simultaneous Heating and Cooling for Simultaneous Heating and Cooling F. Sustainable Energy Centre, University of South Australia Mawson Lakes Boulevard, Mawson Lakes 5095 AUSTRALIA E-mail: Frank.@UniSA.edu.au Abstract The high efficiency

More information

A Performance Comparison of Vapour Compression Refrigeration System Using Eco Friendly Refrigerants of Low Global Warming Potential

A Performance Comparison of Vapour Compression Refrigeration System Using Eco Friendly Refrigerants of Low Global Warming Potential International Journal of Scientific and Research Publications, Volume 2, Issue 9, September 2012 1 A Performance Comparison of Vapour Compression Refrigeration System Using Eco Friendly Refrigerants of

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

OPTIMAL POLYGEN COOLING CONCEPT FOR ST. OLAVS HOSPITAL IN TRONDHEIM, NORWAY

OPTIMAL POLYGEN COOLING CONCEPT FOR ST. OLAVS HOSPITAL IN TRONDHEIM, NORWAY 1st European Conference on Polygeneration OPTIMAL POLYGEN COOLING CONCEPT FOR ST. OLAVS HOSPITAL IN TRONDHEIM, NORWAY G. Eggen 1, A. Utne 2 1) COWI A/S, PB 2564 Sentrum, NO-7414 Trondheim, Norway, e-mail:

More information

SIMULATION OF THERMODYNAMIC ANALYSIS OF CASCADE REFRIGERATION SYSTEM WITH ALTERNATIVE REFRIGERANTS

SIMULATION OF THERMODYNAMIC ANALYSIS OF CASCADE REFRIGERATION SYSTEM WITH ALTERNATIVE REFRIGERANTS INTERNATIONAL JOURNAL OF MECHANICAL ENGINEERING AND TECHNOLOGY (IJMET) International Journal of Mechanical Engineering and Technology (IJMET), ISSN 0976 6340(Print), ISSN 0976 6340 (Print) ISSN 0976 6359

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

Mohan Chandrasekharan #1

Mohan Chandrasekharan #1 International Journal of Students Research in Technology & Management Exergy Analysis of Vapor Compression Refrigeration System Using R12 and R134a as Refrigerants Mohan Chandrasekharan #1 # Department

More information

Engine Efficiency and Power Density: Distinguishing Limits from Limitations

Engine Efficiency and Power Density: Distinguishing Limits from Limitations Engine Efficiency and Power Density: Distinguishing Limits from Limitations Chris F. Edwards Advanced Energy Systems Laboratory Department of Mechanical Engineering Stanford University Exergy to Engines

More information

Diesel Cycle Analysis

Diesel Cycle Analysis Engineering Software P.O. Box 1180, Germantown, MD 20875 Phone: (301) 540-3605 FAX: (301) 540-3605 E-Mail: info@engineering-4e.com Web Site: http://www.engineering-4e.com Diesel Cycle Analysis Diesel Cycle

More information

Evaluation of mobile storage systems for heat transport. G. Storch, A. Hauer, A. Krönauer ZAE Bayern, Walther-Meißner-Str. 6, 85748 Garching, Germany

Evaluation of mobile storage systems for heat transport. G. Storch, A. Hauer, A. Krönauer ZAE Bayern, Walther-Meißner-Str. 6, 85748 Garching, Germany Evaluation of mobile storage systems for heat transport G. Storch, A. Hauer, A. Krönauer ZAE Bayern, Walther-Meißner-Str. 6, 85748 Garching, Germany Outline Introduction Mobile Storage Units Case Studies:

More information

Author's personal copy

Author's personal copy Energy Conversion and Management 50 (2009) 2768 2781 Contents lists available at ScienceDirect Energy Conversion and Management journal homepage: www.elsevier.com/locate/enconman Thermoeconomic analysis

More information

COGENERATION. This section briefly describes the main features of the cogeneration system or a Combined Heat & Power (CHP) system. 36 Units.

COGENERATION. This section briefly describes the main features of the cogeneration system or a Combined Heat & Power (CHP) system. 36 Units. COGENERATION 1. INTRODUCTION... 1 2. TYPES OF COGENERATION SYSTEMS... 2 3. ASSESSMENT OF COGENERATION SYSTEMS... 10 4. ENERGY EFFICIENCY OPPORTUNITIES... 14 5. OPTION CHECKLIST... 16 6. WORKSHEETS... 17

More information

APPLIED THERMODYNAMICS. TUTORIAL No.3 GAS TURBINE POWER CYCLES. Revise gas expansions in turbines. Study the Joule cycle with friction.

APPLIED THERMODYNAMICS. TUTORIAL No.3 GAS TURBINE POWER CYCLES. Revise gas expansions in turbines. Study the Joule cycle with friction. APPLIED HERMODYNAMICS UORIAL No. GAS URBINE POWER CYCLES In this tutorial you will do the following. Revise gas expansions in turbines. Revise the Joule cycle. Study the Joule cycle with friction. Extend

More information

The natural ombination

The natural ombination The natural ombination DAIKIN ALTHERMA HYBRID HEAT PUMP 2 A new pportunity in residential heating! There is a growing demand from home owners to replace heating systems, especially replacing of gas boilers,

More information

8. Heat pumps, heat pipes, cold thermal energy storage

8. Heat pumps, heat pipes, cold thermal energy storage Kylteknik ( KYL ) Refrigeration course # 424503.0 v. 2014 8. Heat pumps, heat pipes, cold thermal energy storage Ron Zevenhoven Åbo Akademi University Thermal and Flow Engineering Laboratory / Värme- och

More information

THEORETICAL AND EXPERIMENTAL EVALUATION OF AUTOMOBILE AIR-CONDITIONING SYSTEM USING R134A

THEORETICAL AND EXPERIMENTAL EVALUATION OF AUTOMOBILE AIR-CONDITIONING SYSTEM USING R134A THEORETICAL AND EXPERIMENTAL EVALUATION OF AUTOMOBILE AIR-CONDITIONING SYSTEM USING R134A Jignesh K. Vaghela Assistant Professor, Mechanical Engineering Department, SVMIT, Bharuch-392001, (India) ABSTRACT

More information

Open Cycle Refrigeration System

Open Cycle Refrigeration System Chapter 9 Open Cycle Refrigeration System Copy Right By: Thomas T.S. Wan 温 到 祥 著 Sept. 3, 2008 All rights reserved An open cycle refrigeration system is that the system is without a traditional evaporator.

More information

Technical data. Danfoss DHP-A

Technical data. Danfoss DHP-A Technical data Danfoss DHP-A An air heat pump which produces both heat and hot water Can operate efficiently down to -0 C Danfoss TWS tank gives plenty of hot water quickly and with low operating costs

More information

Increasing the evaporation temperature with the help of an internal heat exchanger

Increasing the evaporation temperature with the help of an internal heat exchanger Increasing the evaporation temperature with the help of an internal heat exchanger A. TAMBOVTSEV (a), H. QUACK (b) (a,b) Technische Universität Dresden, D-01062, Dresden, Germany (a) Fax: (+49351) 463-37247,

More information

STEAM TURBINE 1 CONTENT. Chapter Description Page. V. Steam Process in Steam Turbine 6. VI. Exhaust Steam Conditions, Extraction and Admission 7

STEAM TURBINE 1 CONTENT. Chapter Description Page. V. Steam Process in Steam Turbine 6. VI. Exhaust Steam Conditions, Extraction and Admission 7 STEAM TURBINE 1 CONTENT Chapter Description Page I Purpose 2 II Steam Turbine Types 2 2.1. Impulse Turbine 2 2.2. Reaction Turbine 2 III Steam Turbine Operating Range 2 3.1. Curtis 2 3.2. Rateau 2 3.3.

More information

Theoretical Study on Separate Sensible and Latent Cooling Air-Conditioning System

Theoretical Study on Separate Sensible and Latent Cooling Air-Conditioning System Purdue University Purdue e-pubs International Refrigeration and Air Conditioning Conference School of Mechanical Engineering 2008 Theoretical Study on Separate Sensible and Latent Cooling Air-Conditioning

More information

Analytical Study of Vapour Compression Refrigeration System Using Diffuser and Subcooling

Analytical Study of Vapour Compression Refrigeration System Using Diffuser and Subcooling IOSR Journal of Mechanical and Civil Engineering (IOSR-JMCE) e-issn: 2278-1684,p-ISSN: 2320-334X, Volume 11, Issue 3 Ver. VII (May- Jun. 2014), PP 92-97 Analytical Study of Vapour Compression Refrigeration

More information

Daikin Altherma. hybrid heat pump. The natural combination

Daikin Altherma. hybrid heat pump. The natural combination Daikin Altherma hybrid heat pump The natural combination Why choose Daikin? As an industry leader, Daikin combines broad experience, technical innovation and responsive customer service to help you meet

More information

Cooling kw 5.2 6.0 7.1 Heating kw 5.65 6.35 7.75

Cooling kw 5.2 6.0 7.1 Heating kw 5.65 6.35 7.75 Specifications COOLING ONLY / HEAT PUMP 005 006 007 Capacity (Eurovent) Cooling kw 5.2 6.0 7.1 Heating kw 5.65 6.35 7.75 Nominal input (Eurovent) Cooling kw 1.89 2.35 2.95 Heating kw 1.97 2.24 2.83 EER

More information

1D STEADY STATE HEAT

1D STEADY STATE HEAT D SEADY SAE HEA CONDUCION () Pabal alukda Aociate Pofeo Depatment of Mecanical Engineeing II Deli E-mail: pabal@mec.iitd.ac.in Palukda/Mec-IID emal Contact eitance empeatue ditibution and eat flow line

More information

Chapter 14. At temperatures below the critical temperature, the gas GAS VAPOR MIXTURES AND AIR-CONDITIONING. Objectives

Chapter 14. At temperatures below the critical temperature, the gas GAS VAPOR MIXTURES AND AIR-CONDITIONING. Objectives Chapter 14 GAS VAPOR MIXTURES AND -CONDITIONING At temperatures below the critical temperature, the gas phase of a substance is frequently referred to as a vapor. The term vapor implies a gaseous state

More information

Boiler efficiency measurement. Department of Energy Engineering

Boiler efficiency measurement. Department of Energy Engineering Boiler efficiency measurement Department of Energy Engineering Contents Heat balance on boilers Efficiency determination Loss categories Fluegas condensation principals Seasonal efficiency Emission evaluation

More information

Food industry Prosecc industry Heat & power (Production of district heating & cooling) Food industry Process industry Logistic centres Sport arenas

Food industry Prosecc industry Heat & power (Production of district heating & cooling) Food industry Process industry Logistic centres Sport arenas Johan Tallberg Food industry Process industry Logistic centres Sport arenas Synergy Food industry Prosecc industry Heat & power (Production of district heating & cooling) Maintenance services for the

More information

What are the Carrier ChillerVu Energy Dashboards?

What are the Carrier ChillerVu Energy Dashboards? Energy Dashboard CARRIER CORPORATION 2015 A member of the United Technologies Corporation family Stock symbol UTX Catalog No. 11-808-564-01 12/9/2015 Verify that you have the most current version of this

More information

Legacy Data Centres Upgrading the cooling capabilities What are the options?

Legacy Data Centres Upgrading the cooling capabilities What are the options? Legacy Data Centres Upgrading the cooling capabilities What are the options? Presentation Structure What is a Legacy Data Centre? What is CRAC cooling? ASHRAE Standards Overview Available Cooling Systems

More information

Waste Heat Recovery through Air Conditioning System

Waste Heat Recovery through Air Conditioning System International Journal of Engineering Research and Development e-issn: 2278-067X, p-issn : 2278-800X, www.ijerd.com Volume 5, Issue 3 (December 2012), PP. 87-92 Waste Heat Recovery through Air Conditioning

More information

Natural geothermal energy.

Natural geothermal energy. ROTEX ground source heat pump Natural geothermal energy. ROTEX HPU ground the ground source heat pump that heats with free geothermal energy. Compact, environmentally responsible and uniquely efficient.

More information