Title | Lect29 - Lecture notes 29 |
---|---|
Author | kumala devi |
Course | Thermodynamic 1 |
Institution | Universitas Diponegoro |
Pages | 3 |
File Size | 198.8 KB |
File Type | |
Total Views | 110 |
Vapor Compression Refrigeration System Purpose of the system is to maintain a cold region at a temperature below the temperature of its surroundings Warm surroundings TH < T3 Cold region TC > T1 Note: Q& in referred to as the refrigeration capacity, W (u...
Vapor Compression Refrigeration System Purpose of the system is to maintain a cold region at a temperature below the temperature of its surroundings Warm surroundings TH < T3
Cold region TC > T1
Note: Q& in referred to as the refrigeration capacity, W (units: 1 ton = 711 KJ/min) Working fluid: up to 1990’s most common refrigerants were chlorinated fluorocarbons (CFCs), e.g., Freon-12 (CCl2F2), Freon-22 (CHClF2) Æ chlorine destroys earth’s ozone layer so CFCs banned A common refrigerant used in most hockey rinks in Canada is ammonia (NH3) 204
Ideal refrigeration cycle: 1 Æ 2 Isentropic compression 2 Æ 3 Constant pressure heat removal 3 Æ 4 Constant enthalpy (throttling) 4 Æ 1 Constant pressure heat addition
2
Q& out Temperature of warm region, TH Temperature of cold region, TC
Q& in
1Æ2
W& in = m& (h1 − h4 )
3 Æ 4 Throttling process 4Æ1
2Æ3
& (h2 − h3 ) Q& out = m
h3 = h4
Q& in = m& (h1 − h4 ) 205
Coefficient of Performance (COP): Q& in
β =
m& = h1 − h4 > 1 W&C h2 − h1 m&
Actual vapor-compression cycle may include: state 1 in superheated vapor region and state 3 in the compressed liquid region
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