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        ![]() MIL-HDBK-1003/13A 
b. 
Air systems*.  Since rock has a specific heat of 0.21 Btu/lb-deg. 
F, and rock densities (170 lb/ft3) typically contain 20%-40% 
voids, then the optimum storage size is 0.8 ft3 per square foot 
of collector (range 0.5 to 1.15 ft3 per square foot of 
collector).  The range in SI units is 0.15 to 0.35 m3/m2. 
* 
Storage volumes in this range will store the equivalent of overnight to 
one full day of heating. 
In general, for equal storage capacity, the rock pebble bed would have to 
occupy a volume 2-1/2 to 3 times larger than a water tank.  Rock storage bins 
have higher structural requirements, and tend to lose more heat due to their 
greater surface area.  Rock bins generally provide good temperature strati- 
fication; contrary to practice in conventional DHW systems, stratification is 
desirable in both water and air solar systems.  NCEL has done studies to show 
that good stratification can add 5%-10% to overall system performances (Sharp 
and Loehrke, 1978).  To achieve this, baffles or modified inlets to the tanks 
are used.  However, specially designed tanks with baffles or diffusers are 
expensive and not readily available.  To suppress convection warm water 
enters and leaves the top of the tank, and cold water, the bottom.  In this 
way the hottest water goes to the load and the coldest to the collectors. 
A typical DHW system is shown in Figure 2-10.  Use of two tanks insures that 
when hot water from the first (tempering) tank is available, the auxiliary 
heat will not come on; also less total fuel will be used to bring the smaller 
second tank up to temperature.  Single tank arrangements, while possible and 
economical, are not recommended due to the fact that they tend to activate 
the heating element every time there is a draw of water rather than wait for 
the solar collectors to provide additional heated water.  Research is being 
done and new tanks designed to overcome this deficiency.  The two-tank 
arrangement avoids this control problem.  Two-tank arrangements are suited to 
retrofits since the second tank (the water heater) is already there.  A 
variation would be to use a heat exchanger (copper coil) in the tempering 
tank collector loop for freeze protection.  The tempering tank could then be 
an inexpensive unpressurized tank. 
Another method of heat storage in air systems that is currently being 
investigated is latent heat storage.  Latent heat is stored in a material as 
it changes phase from a solid to a liquid.  Materials which have melting 
points near the temperatures supplied by solar collectors store heat as they 
melt and release it as they resolidify.  The two materials which have 
received the most attention are salt hydrates and paraffins. 
The advantage of latent heat storage is that it can store very large 
quantities of heat per pound of storage material.  Therefore, less volume 
should be required for latent heat storage than for heat storage in rock 
beds.  However, problems of slow solidification and low heat conductivity 
retards effective heat transfer to and from the material.  As a result, a 
large surface area-to-volume ratio is required, which significantly increases 
the effective volume of latent storage. 
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