Worldwide, a multitude of the industrial processes utilizes fossil fuel to supply heat and power. However, the present stock of the fossil fuel is ultimately finite and will deplete in a few decades. On the other hand, the emissions of the fossil fuel combustion process share with a vast role in the environmental problems such as global warming and air pollution. Reducing this dependence on such energy sources becomes important in refrigeration and air conditioning field as it represents one of the most energy consumption industries. Locally in Egypt, the demand for the electricity has been growing at an average rate around seven present (7 %) annually over the last ten years, since the early 2000s. Remarkably, the conventional refrigeration system has another environmental problem representing in its ozone depletion potential. Therefore, providing an alternative refrigeration technology in attenuation of these effects will be valuable. Solar adsorption chillers are technologically promising especially in the developing countries and remote areas because the system can be driven by solar energy without involving electricity. The adsorption
refrigeration systems have a great share in reducing the environmental crises by using a low-grade solar energy thus reducing the carbon footprint so, reducing the global warming potential. Therefore, it is technologically possible and socially feasible in the areas where electricity is not enough but solar energy is rather easy to obtain.
Adsorption refrigeration systems are regarded as one of promising clean technologies
since it uses low-grade heat sources, such as solar, geothermal, biomass as well
as process/waste heat. The present study provides a dynamic modeling of two-bed
adsorption chiller using both RD silica gel/water and SWS-1L/water as working
pairs. Herein, a mathematical model has been developed using MATLAB software.
Also, the mathematical model was validated with the experimental data from the
literature. The analysis is based on the following conditions; (i) the cycle time of
0 s to 900 s, (ii) hot water inlet temperature of 55�C to 95�C, (iii) cooling water
inlet temperature of 25�C to 40�C and (iv) chilled water inlet temperature of 10C to 22�C. Simulation results indicate that the coefficient of performance increases
monotonically with the adsorption/desorption cycle time whereas the system cooling
capacity increases gradually until reaches an optimum adsorption/desorption cycle
time and then reduces. RD silica gel/water and SWS-1L/water pairs provide a higher
system cooling capacity of 16 kW and 4.18 kW, respectively at the hot, cooling and
chilled water inlet temperature of 95�C, 30�C and 14�C, respectively. Interestingly, it
was found that the system cooling capacity increases gradually from 6 kW to 16 kW
as the heat source temperatures varies from 55�C to 95�C for RD silica gel/water pair.
The half cycle times are �fixed to 350 s and 280 s for both pairs, respectively which
selected based on optimum time which gives maximum cooling capacity, whereas the
switching time is set to 30 s for both working pairs.
Moreover, enhancing of the adsorption chiller performance plays an important role
not only on the energy savings but also in the environmental pollution reduction.
The present work aims to improve the system cooling capacity of an adsorption
chiller working with a silica gel/water pair by an allocation of the optimum cycle
time at di�erent operating conditions. A prediction of the optimum cycle time for
a wide range of hot (55�C to 95�C), cooling (25�C to 40�C) and chilled (10C to 22�C) water inlet temperatures. Then, correlations for the optimum cycle time
as well as system performance characteristics such as system cooling capacity and
COP were derived in terms of the system operating temperatures. The optimum
and conventional chiller performance are compared at different operating conditions.
Enhancement ratio of the system cooling capacity was tripled as the cooling water
inlet temperature increased from 25�C to 40�C at constant hot and chilled water inlet temperatures of 85�C and 14�C, respectively. Mapping the assorted operating
temperatures with an adsorption/desorption cycle time of 0 s to 500 s, provides a
superior maximum cooling capacity of 21.4 kW at the optimum cycle time of 389 s for
hot, cooling and chilled water inlet temperatures of 95�C, 25�C and 22C, respectively.
Further results can be achieved by applying the concept of the optimum cycle time allocation, the system cooling capacity enhancement ratio can be reached to 15.6%
at hot, cooling and chilled water inlet temperatures of 95�C, 40�C and 10.
Additionally, the performance indicators comparisons are conducted for various cycle times of 900 s, 700 s and the adaptive cycle time under the Egyptian climate conditions using RD silica gel/water pair. Then, temperature profi�les of the solar storage tank, adsorber, desorber, evaporator and condenser are forecasted. Simulation results show that the maximum cyclic cooling capacity of the system reaches about 14.6 kW, 14 kW and 12.8 kW for cycle time operation of 900 s, 700 s and using the adaptive cycle time, respectively. In deep, a higher cycle time duration considers as an essential parameter in optimizing the solar adsorption chillers, which achieves a higher system performance. Moreover, using the solar adsorption chiller with a cycle time of 900 s, 700 s and for the adaptive variable cycle time was achieved an electrical consumption saving by about 34.2%, 32.9% and 30.4%, respectively. Finally, A CFD simulation study is performed to investigate the effect of using different heat exchanger con�figurations on the adsorption parameters.