5.1. Gas heat pump and refrigeration cycle¶
Gas heat pumps and gas regrigerators are basically following the reverse Brayton cycle (or Joule cycle).
As for any heat pump or refrigerator, (Eq.2.11, and Eq.2.10) the coefficients of performance of Reverse Brayton cycle are:
Considering the working fluid as an ideal gas, and because no machine is working in transformations 2-3 and 4-1, application of the balance energy equation reads:
such that the COPs of Reverse Brayton cycle become:
As for gas turbine, it is possible to determine gas temperatures after the compressor and the turbine thanks to isentropic relations for ideal gases:
we finally obtain:
(5.1)¶
where is the pressure ratio.
Figure 5.2: reveals that the performance of such machine is good for low pressure ratio.
Remarks
As for gas turbine, it is possible to easily account for the adiabatic compressor and adiabatic turbine irreversibilities by using the isentropic efficiency of both components (see Section 4.2.3: ).
It is also possible to improve the cycle using regeneration (see Section 4.2.4: )
Heat pumps and Refrigerators using the reverse Brayton cycle have low performances and are used only for specific applications.