ABSTRACT
The demand for electric power has been increasing due to the increase in population and the development of the cities. Therefore, there is a need to avoid processes that use large amounts of electric power. Ammonia-water absorption systems run by replacing the electric compressor by a thermal-driven unit, for cooling or refrigeration. In this study, Beirut weather conditions are used to estimate the required heat input available from a 42 m2 parabolic trough concentrating solar collector system that supplies heat to an ammonia refrigeration cycle. The highest COP attained was 0.65 at an evaporator temperature of −5°C. The required storage tank volume was found to be 2.6 m3 at the maximum available energy in July. The absorption system is seen to be capable of operating all day and night using solar energy in June and July.
Nomenclature
= | Aperture area of the collector (L*W) (aaaaaaaa) | |
= | Energy storage density of the used material in the tank (kWh/m3) | |
= | Collector efficiency factor | |
= | Specific enthalpy in liquid phase (kJ/kg) | |
= | Specific enthalpy in gas phase (kJ/kg) | |
= | Specific volume of the ammonia–water solution (m3/kg) | |
= | Heat rate absorbed by the evaporator (kW). | |
= | Heat rate rejected by the condenser (kW). | |
= | Heat rate absorbed by the generator (kW). | |
= | Heat rate rejected by the absorber (kW). | |
= | Strong solution mass flow rate (kg/s). | |
= | Weak solution mass flow rate (kg/s). | |
= | Heat exchanger effectiveness. | |
= | Solar useful heat gain (kW). | |
= | Total rate of solar radiation incident on the parabolic collector aperture | |
= | Overall collector heat loss coefficient (W/m2 ◦C) | |
= | Fluid temperature in collector | |
= | Air ambient temperature | |
x | = | Ammonia mole fraction in the liquid phase |
= | Ammonia mass fraction in the liquid phase | |
y | = | Ammonia mole fraction in the gas phase |
= | Optical efficiency of collector system |