Hvac CH 3
Hvac CH 3
Hvac CH 3
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►Engineering model:
►Each component is analyzed as a control
volume at steady state.
►Dry compression is presumed: the
refrigerant is a vapor.
►The compressor operates adiabatically.
►The refrigerant expanding through the valve
undergoes a throttling process.
►Kinetic and potential energy changes are
ignored.
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►Performance parameters
Coefficient of Performance (COP)
ℎ −ℎ
= =
ℎ −ℎ
=
−
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Example 4.1
Refrigerant-134a enters the compressor of a vapor-compression refrigeration cycle at
120 kPa as a saturated vapor and leaves at 900 kPa and 75 ◦C (Figure 4.2a) . The
refrigerant leaves the condenser as a saturated liquid. The rate of cooling provided by
the system is 18,000 Btu/h. Determine (a) the mass flow rate of R-134a and (b) the
COP of the cycle. (c) Also, determine the COP of the cycle if the expansion valve is
replaced by an isentropic turbine. Do you recommend such a replacement
for refrigeration systems? (d) Determine the COP if the evaporator pressure is 160 kPa
and other values remain the same. (e) Determine the COP if the condenser pressure is
800 kPa and other values remain the same
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Subcooling
Superheating
As mentioned before, the purpose of superheating is to avoid compressor slugging
damage. Superheating is shown in Fig. The degree of superheat depends mainly on
the type of refrigerant feed and compressor as well as the construction of the
evaporator
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Working principle of a flash tank Expansion process using a flash tank on P-h diagram
Dr. Abduljalil Al-Abidi HVAC
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2. Liquid refrigerant enters the evaporator at a lower enthalpy and increases the
refrigeration effect.
3. Discharge gas from the low-stage compressor can be desuperheated at the
interstage pressure.
This results in a lower discharge temperature from the high-stage compressor
than would be
produced by a single-stage system at the same pressure differential between
condensing and
evaporating pressures.
4. Two or three compressors in a multistage system provide much greater
flexibility to accommodate
the variation of refrigeration loads at various evaporating temperatures during
part-load operation.
The drawbacks of the multistage system are higher initial cost and a more
complicated system
than that for a single-stage system.
Interstage Pressure
Interstage pressure is usually set so that the compression ratio at each stage is
nearly the same for higher COPs. For a two-stage compound system, Interstage
pressure pi, psia (kPa abs.), can be calculated
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Two-stage compound system with a flash cooler: (a) schematic diagram; (b) refrigeration cycle.
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A two-stage compression system with flash tank for flash gas removal only (a) System
schematic; (b) Cycle on P-h diagram
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where P1 and P2 are the inlet and exit pressures of the compressor, v1 is the specific
volume of the refrigerant vapour at the inlet to the compressor and n is the polytropic
exponent. From the above expression, it can be seen that specific work input reduces
as specific volume, v1 is reduced. At a given pressure, the specific volume can be
reduced by reducing the temperature. This is the principle behind intercooling in
multi-stage compression. Figures (a) and (b) show the process of intercooling in two-
stage compression on Pressure-specific volume (P-v) and P-h diagrams.
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Intercooling using external water cooled heat Intercooling using liquid refrigerant in flash
exchanger tank
Two —stage vapour compression refrigeration Two —stage vapour compression refrigeration
system with flash gas removal using a flash system with flash gas removal using a flash
tank and intercooling tank and intercooling — P—h diagram
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A two-stage compression system with the flash tank used for intercooling only (a) System
schematic (b) Cycle on P-h diagram
(a) A two-stage vapor-compression refrigeration system, (b) its T−s diagram, and (c)
its log P−h diagram.
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Two-stage compound system with a vertical coil intercooler: (a) schematic diagram; (b)
refrigeration cycle.
Dr. Abduljalil Al-Abidi HVAC
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(a) Schematic of a two-stage (binary) cascade refrigeration system, (b) its T–s
diagram, and (c) its log P–h diagram.
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Example:
Consider a two-stage cascade refrigeration system operating between the pressure
limits of 1.6MPa and 180 kPa with refrigerant-134a as the working fluid (Figure 5.5).
Heat rejection from the lower cycle to the upper cycle takes place in an adiabatic
counter-flow heat exchanger where the pressure in the upper and lower cycles are
0.4 and 0.5MPa, respectively. In both cycles, the refrigerant is a saturated liquid at
the condenser exit and a saturated vapor at the compressor inlet, and the
isentropic efficiency of the compressor is 85%. If the mass flow rate of the refrigerant
through the lower cycle is 0.07 kg/s, (a) draw the temperature–entropy diagram of the
cycle indicating pressures; determine (b) the mass flow rate of the refrigerant through
the upper cycle, (c) the rate of heat removal from the refrigerated space, and (d) the
COP of this refrigerator; and (e) determine the rate of heat removal and the COP if
this refrigerator operated on a single-stage cycle between the same pressure limits
with the same compressor efficiency. Also, take the mass flow rate of R-134a
through the cycle to be 0.07 kg/s.
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