This page provides some data from tests of glazing materials done by Alan Rushforth.
Alan is working on developing an inexpensive, long life, low maintenance solar water heating collector for commercial buildings (e.g. apartment buildings). He is looking for a glazing material that offers high collection performance at a low price, and for a a cost effective way to transfer heat from the collector absorber to the working fluid (water).
I think that he has developed a really simple way to compare the collection efficiency of glazing materials.
In this stagnation test, Alan made several identical solar collector boxes. Each box is made from 1 inch thick rigid foam board, and is painted flat black inside. The collectors boxes are about 8 by 10 inches, and about 1 inch deep. Each is glazed with a different material (glass, polycarbonate, Teflon, ...). The glazing material is sealed to the collector box in such a way that there is no air leakage. The collector boxes are mounted on a rack such that they all see the same sun conditions. The boxes are exposed to sunlight which is nearly normal to the glazing surface, and the stagnation temperature in each collector box is measured.
Five identical collector boxes with different types of glazing installed.
The idea is that the the stagnation temperature depends on 1) how much sun is transmitted by the glazing, and 2) how much heat is lost through the glazing. The stagnation temperature also depends on the losses from the sides and back of the collector box (but this is the same for all the boxes), and on the ambient temperature. So, the test determines the highest performing glazing for the ambient temperature at which the test was run -- the results will be different for other outside temperatures.
The glazing material that produces the highest stagnation temperature has the highest thermal performance at this ambient temperature.
It appears to me that this simple test quickly and easily determines the comparative performance of the glazing tested, including the combined effect of:
Solar transmittance into the collector box
Glazing losses due to radiation, conduction and convection
Does anyone see anything wrong with this logic?
Here are Alan's results to date:
Time |
Ambient Temp. |
Window glass |
Tefzel 200 LZ (2 mil) |
Teflon FEP500C (2 mil) |
Corrugated polycarbon-ate |
8 mm twinwall polycarb. |
2/5/07 - 9:55AM just before test went outdoors |
68F |
67F |
70F |
70F |
67F |
67F |
10:00 sun |
24 |
114 |
95 |
85 |
114 |
114 |
10:05 |
24 |
128 |
103 |
91 |
131 |
141 |
10:10 |
25 |
110 |
102 |
96 |
148 |
155 |
10:16 light cloud |
25 |
99 |
85 |
85 |
123 |
146 |
10:34 |
26 |
90 |
78 |
70 |
101 |
116 |
11:28 sun |
28 |
145 |
122 |
106 |
163 |
194 |
12:48 cloud |
28 |
81 |
78 |
71 |
103 |
118 |
1:14 |
28 |
95 |
100 |
82 |
111 |
109 |
1:20 |
29 |
105 |
107 |
92 |
127 |
134 |
1:40 |
30 |
114 |
113 |
98 |
132 |
144 |
2:04 |
30 |
60 |
64 |
54 |
67 |
96 |
3:00 |
29 |
105 |
113 |
90 |
105 |
125 |
3:25 |
29 |
95 |
99 |
89 |
106 |
136 |
4:30 (low sun behind trees) |
28 |
34 |
37 |
34 |
37 |
41 |
2/6/07 -9:55 AM |
16 |
|
105/83 |
72 |
112 |
112 |
10:00 full sun all day |
17 |
|
105/80 |
67 |
111 |
122 |
|
17 |
|
138/101 |
95 |
158 |
188 |
100:00w/ reflector added |
17 |
|
221/hi |
143 |
228 |
250 |
“ |
17 |
|
229/hi |
146 |
237 |
263 |
“ |
17 |
|
238/hi |
152 |
247 |
280 |
“ |
17 |
|
246/hi |
hi |
255 |
287 |
12:00 w/o reflector |
17 |
|
207/hi |
134 |
212 |
252 |
“ |
17 |
|
207/hi |
134 |
212 |
252 |
“ |
17 |
|
208/hi |
142 |
216 |
248 |
1:05 with reflector |
17 |
|
239/hi |
hi |
246 |
281 |
1:15 with reflector |
17 |
|
237/hi |
hi |
241 |
281 |
Notes:
1) On 2/5/07 the collectors were in a location with some light twig shading plus there was an occasional light cloud. On 2/6/07 the collectors were in full sun with zero clouds.
2) Gray numbers were from non-oven type thermometers that have a 158 limit and were reading lower than the oven thermometers. Dark numbers are all from oven thermometers.
Alan has been working on finding a way to make water spread out between a substrate and an overlying layer of film. The idea being that if this could be accomplished, the thin film of water would efficiently collect heat from the absorber, and also be inexpensive.
The early tests with commonly available films resulted in the water not spreading out uniformly, but instead concentrating into rivulets. Alan then tried the same test on small samples of Teflon and Tefzel film from DuPont -- these are the initial results:
2/8/07