Note that more energy is derived from a collector when the water temperature entering the collector is low. It is important in solar energy system design to only heat the water or heat transfer fluid to the lowest temperature consistent with system output requirements.
The energy balance on a solar collector absorber or receiver can be written as; (5.1) - rate of ‘useful’ energy leaving the absorber (W) - rate of optical (short wavelength) radiation incident on absorber (W) - rate of thermal energy loss from the absorber (W) (5.2) - mass flow rate of heat transfer fluid (kg/s)
The optical efficiency of a solar collector is defined as the rate of optical (short wavelength) energy reaching the absorber or receiver, divided by the appropriate solar resource. Dividing Equation (4.3) by Equation (4.4), we have for optical efficiency; (5.14)
A measurement is made only when the collector is at steady state, which is indicated by a constant rise in heat transfer fluid as it flows through the receiver. In a typical test to determine solar collector efficiency, the collector aperture is aligned as close as possible to normal to the incident direct (beam) solar irradiance.
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