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Fig. 1. Vapor compression refrigeration cycle. The system has four components: a
compressor, a condenser, an expansion valve, and an evaporator.
where ˙ m k is the mass flow rate of the refrigerant through the compressor,
ω k is the motor shaft speed, V k is the effective displacement volume of the
compressor, C k and D k are volumetric eciency coecients for the compressor,
n is the polytropic coecient, P ki and P ko are the inlet pressure and outlet
pressure across the compressor, respectively.
2) Condenser: According to the state of refrigerant, the condenser can be
divided into three sections: a subcooled liquid section, a two-phase section and
a superheated vapor section. The condenser model has 7 states and 5 inputs. It
can be expressed by a non-linear state space form shown below:
Z c ( x c ,u c )
·
x c = f c ( x c ,u c )
(2)
where the state variables are: length of the two condensation regions L c 1 and L c 2 ;
refrigerant pressure P c ; refrigerant outlet enthalpy h co ; the wall temperatures in
the three regions T cw 1 , T cw 2 ,and T cw 3 , respectively, the input variables are mass
flow rate of the inlet and outlet, ˙ m ci and ˙ m co ; refrigerant inlet enthalpy h ci ;air
temperature T ca and air mass flow rate ˙ m ca ; respectively.
3) Expansion valve: The expansion valve is also modeled as a static compo-
nent; its mass flow rate can be calculated from the orifice equation
P vo )] n
˙ m v = C v A v [ ρ v ( P vi
(3)
where ˙ m v is the mass flow rate of refrigerant through expansion valve, C v is the
orifice coecient, A v is the opening area, ρ v is the refrigerant density. P vi and
P vo are the inlet and outlet pressure across the expansion valve, respectively.
4) Evaporator: Similar to the condenser model, the evaporator can be di-
vided into two regions, i.e., a two-phase region with a mean void fraction, and a
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