IntroductionExperimental (Davis and Bartera, 1975;Lavan and Thompson, 1977;Fanney and Klein, 1988) and analytical (Sharp and Loehrke, 1979;Wuestling, 1983 ;Jesch and Braun, 1984;Wuestling et al., 1985) investigations show that thermal stratification of the solar storage tank enhances the performance of solar domestic hot water (SDHW) systems . Maximum possible thermal performance is obtained when no mixing occurs in the solar storage tank. In this case, the coldest stored fluid is circulated through the collector(s). Heated water is then returned to the tank without inducing mixing of fluid layers with different temperatures. During water draws to the load, the hottest water in the tank is withdrawn from the tank and replaced (again without mixing) with cold water from the mains water supply. Minimum performance is obtained when fluid streams entering the storage tank mix completely (and instantaneously) with water in the tank . In this case, water circulated to the collector is at the same temperature as that supplied to the load.Loss of stratification of the thermal storage tank results from convective mixing, both forced and natural , and, to a lesser extent, from conduction between hot and cold fluid layers. Maintaining thermal stratification requires inhibition of mixing in the tank. Mixing depends on the design of the tank and the operating conditions (flow rate and temperature of incoming fluid streams and the temperature distribution in the tank). Forced convection mixing is due to the momentum of the fluid streams entering the storage tank and depends on the flow rate of the entering stream and the design of the inlet. Momentum diffusers have been employed to reduce mixing due to jet entrainment.