Refrigeration Cycle

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During compression, droplets present in liquid are vaporised by the internal heat transfer process which requires finite
Basic Refrigeration Cycle

Reversed Carnot Cycle

Reversed Carnot Cycle Refrigeration Cycle Dr. M. Zahurul Haq Professor Department of Mechanical Engineering Bangladesh University of Engineering & Technology (BUET) Dhaka-1000, Bangladesh [email protected] http://teacher.buet.ac.bd/zahurul/

ME 415: Refrigeration & Building Mechanical Systems

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Coefficient of Performance, COP =

c Dr. M. Zahurul Haq (BUET)

Refrigeration Cycle

Basic Refrigeration Cycle

ME 415 (2011)

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Reversed Carnot Cycle

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Reversed Carnot Cycle

Carnot cycle demands that the expansion take place isentropically and that the resulting work be used to help drive the compressor. Practical difficulties, however, militate against the expansion engine: the possible work that can be derived from the engine is small fraction that must be supplied to the compressor. practical problems such as lubrication intrude when a fluid of two phases drives the engine.

In wet compression, the droplets of the liquids may wash the lubricating oil from the walls of the cylinder, accelerating wear. Dry compression takes place with no droplets and is preferable. Liquid refrigerants may be trapped in the head of reciprocating compressor by the rising piston, possibly damaging the valves or the cylinder head.

ME 415 (2011)

ME 415 (2011)

Expansion Process in Carnot Cycle

During compression, droplets present in liquid are vaporised by the internal heat transfer process which requires finite time. High-speed compressors are susceptible to damage by liquid because of the short time available.

Refrigeration Cycle

Refrigeration Cycle

Basic Refrigeration Cycle

Wet Compression in Carnot Cycle vs. Dry Compression

c Dr. M. Zahurul Haq (BUET)

c Dr. M. Zahurul Haq (BUET)

TL QL = Wnet TH − TL

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the economics of the power recovery have in past not justified the cost of the expansion engine. A throttling device, such as a valve or other restriction, is almost universally used for this purpose.

c Dr. M. Zahurul Haq (BUET)

Refrigeration Cycle

ME 415 (2011)

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Basic Refrigeration Cycle

Ideal Vapour Compression Refrigeration Cycle

Basic Refrigeration Cycle

Ideal Vapour Compression Refrigeration Cycle

Ideal Vapour Compression Refrigeration Cycle

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Refrigeration Cycle

Basic Refrigeration Cycle

ME 415 (2011)

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c Dr. M. Zahurul Haq (BUET)

Ideal Vapour Compression Refrigeration Cycle

Refrigeration Cycle

Basic Refrigeration Cycle

ME 415 (2011)

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Ideal Vapour Compression Refrigeration Cycle

Processes of VC System

QL QH Win COP

= = = =

Q41 = m(h1 − h4 ) Q23 = m(h2 − h3 ) W12 = m(h2 − h1 ) QL /Win

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1 → 2: Isentropic compression, Pevap → Pcond 2 → 3: Isobaric heat rejection, QH

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3 → 4: Isenthalpic expansion, Pcond → Pevap

Simple vapour compression cycle with pressure & enthalpy values for R134a

4 → 1: Isobaric heat extraction, QL c Dr. M. Zahurul Haq (BUET)

Refrigeration Cycle

ME 415 (2011)

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c Dr. M. Zahurul Haq (BUET)

Refrigeration Cycle

ME 415 (2011)

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Basic Refrigeration Cycle

Ideal Vapour Compression Refrigeration Cycle

Basic Refrigeration Cycle

Effect of Evaporator Temperature

A theoretical single stage cycle using R134a as refrigerant operates with a condensing temperature of 30o C and an evaporator temperature of -20o C. The system produces 50 kW of refrigeration effect. Estimate:

o

R134a: RE = 50 kW, Tcond = 30 C

10

0.40

9

0.39

1

Coefficient of performance, COP

8

0.38

2

Refrigerant mass flow rate, m

7

0.37

Ref. flow rate

QL

COP

6

= Q41 = m(h1 − h4 ) = 50 kW m = 0.345 Kg/s = W12 = m(h2 − h1 ) = 12.5 kW = QL /Win = 50.0/12.5 = 4.0

Win COP

0.36

COP

5

0.35

4

0.34

3

0.33

2

0.32

1

0.31 0.30

0 -50

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Refrigerant flow rate (kg/s)

Example

Ideal Vapour Compression Refrigeration Cycle

-45

-40

-35

-30

-25

-20

-15

-10

-5

0

o

Tevap ( C)

e497 c Dr. M. Zahurul Haq (BUET)

Refrigeration Cycle

Basic Refrigeration Cycle

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c Dr. M. Zahurul Haq (BUET)

Ideal Vapour Compression Refrigeration Cycle

Basic Refrigeration Cycle

Effect of Condenser Temperature

10

10

0.40

9

9

0.38

0.34

7

Ref. flow rate

5

5

0.30

4

0.28

3

0.26

1

2

0.24 50

0

20

25

30

35

40

45

Tcond = 30 C

6

0.32

15

o

7

6

10

o

Tcond = 20 C

8

COP

0.36

COP

5

4

o

Tcond = 40 C

3 2

-50

-45

o

Tcond ( C) e499 Refrigeration Cycle

-40

-35

-30

-25

-20

-15

-10

-5

0

o

e498 c Dr. M. Zahurul Haq (BUET)

Ideal Vapour Compression Refrigeration Cycle

11

0.42

Refrigerant flow rate (kg/s)

COP

0.44

11

0

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12

o

8

ME 415 (2011)

Effect of Evaporator & Condenser Temperatures

R134a: RE = 50 kW, Tevap = -20 C

12

Refrigeration Cycle

ME 415 (2011)

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c Dr. M. Zahurul Haq (BUET)

Tevap ( C) Refrigeration Cycle

ME 415 (2011)

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Deviation from Simple Cycle

Deviation from Simple Cycle

Deviations from Ideal Cycle

Super-heating & Sub-cooling

1

Refrigerant pressure drop in piping, evaporator, condenser, receiver tank, and through the valves and passages.

2

Sub-cooling of liquid leaving the condenser.

3

Super-heating of vapour leaving the evaporator.

4

Compression process is not isentropic.

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Sub-cooling of liquid serves a desirable function of ensuring that 100% liquid will enter the expansion device. Super-heating of vapour ensures no droplets of liquid being carried over into the compressor. Even through refrigeration effect is increased, compression work is greater & probably has negligible thermodynamic advantages.

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Refrigeration Cycle

ME 415 (2011)

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c Dr. M. Zahurul Haq (BUET)

Refrigeration Cycle

ME 415 (2011)

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