Abstract:
The first law and second law efficiencies are determined for a stainless steel closed-tube open rectangular
cavity solar receiver. It is to be used in a small-scale solar thermal Brayton cycle using a micro-turbine
with low compressor pressure ratios. There are many different variables at play to model the air temperature
increase of the air running through such a receiver. These variables include concentrator shape,
concentrator diameter, concentrator rim angle, concentrator reflectivity, concentrator optical error, solar
tracking error, receiver aperture area, receiver material, effect of wind, receiver tube diameter, inlet temperature
and mass flow rate through the receiver. All these variables are considered in this paper. The
Brayton cycle requires very high receiver surface temperatures in order to be successful. These high temperatures,
however, have many disadvantages in terms of heat loss from the receiver, especially radiation
heat loss. With the help of ray-tracing software, SolTrace, and receiver modelling techniques, an optimum
receiver-to-concentrator-area ratio of A0 0.0035 was found for a concentrator with 45 rim angle,
10 mrad optical error and 1 tracking error. A method to determine the temperature profile and net heat
transfer rate along the length of the receiver tube is presented. Receiver efficiencies are shown in terms of
mass flow rate, receiver tube diameter, pressure drop, maximum receiver surface temperature and inlet
temperature of the working fluid. For a 4.8 m diameter parabolic dish, the larger the receiver tube diameter
and the smaller the mass flow rate through the receiver, the higher the receiver surface temperature
and the less efficient the collector becomes. However, the smaller the receiver tube diameter, the higher
the pressure drop through the tube and the smaller the second law efficiency. It was found that the receiver
with larger tube diameter would perform better in a solar thermal Brayton cycle. An overall solar-toheat
efficiency of between 45% and 70% is attainable for the solar collector using the open-cavity receiver.
