Cli-mate CLI-AP30 Spezifikationen Seite 18

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the heated fluid can reach the
tank. The hot fluid sits in the
return line and loses heat until
the next ON cycle, before it
finally is delivered back to the
tank. This is especially true
when high flow rates are used
and when there is a long pipe
run. A variable speed control
helps to prevent this from
happening by sending the heat
back into the tank as it is
produced and results in higher
overall system efficiency and
heat output.
f) Direct Flow - Flow Rate: A
high flow rate in a direct flow
system may cause turbulence in
the solar storage tank and
disturb stratification, which can
lower the entire tank temp during
low solar production periods. A
variable speed pump control will ensure that the flow rate matches the heat output and limit tank de-
stratification.
g) Correct Pump Choice: Any pump used for solar loop circulation must be able to handle continuous use
to at 232
°
F (110
°
C) and higher, if required by system design. The solar pump should always be installed on
the Supply (aka Flow) Line (i.e. pumping to the collector and away from the heat exchanger or tank) thus
limiting exposure to high temperatures. In addition, a check valve should always be installed after the pump
to prevent back flow, and nighttime thermo-siphoning, UNLESS the system is a drain-back, which should
never have a check valve installed in the solar loop. See Apricus OG-300 Schematics and Parts List
system diagrams for reference. The Apricus pump stations incorporate a flow meter, pump and check
valve. Refer to Closed Loop and Direct Flow Pump Station Installation instructions in this manual for more
details on pump station operation.
h) Flow Rate: The flow rate through the collectors should be determined under the following considerations:
i) Turbulent flow through the header is necessary for optimal heat transfer during high solar output and
is achieved at flow rates of 0.8 gpm (3 Lpm) and greater. In a single collector installation, this flow rate
will generally only be achieved during summer. Running a high flow rate during the winter to achieve
turbulent flow is NOT recommended or required as the heat output is not as high, and excessive ON/
OFF cycling of the pump will occur which can cause premature pump failure.
ii) Temperature rise of the heat transfer fluid during each pass through the collector manifold(s) can be
adjusted by changing the flow rate. Reducing the flow rate by half will double the temperature rise per
pass. Normally, a temperature rise of 10-30°F is an acceptable range. Lower delta-t levels
(temperature rise) attained at higher flow rates may cause the pump to turn ON/OFF too often.
Extremely high delta-t levels produced by low flow rates will decrease collector efficiency. This
decrease is far less acute with evacuated tubes than that experienced with a flat plate collector and
may be acceptable, especially if pressure drop is an issue.
A suitable flow rate range for each 30 tube collector is a 0.4-0.8 gpm (1.5-3 Lpm).
iii) The following table provides estimated temperature rise at various flow rates:
Flow Rate per 30 tubes
Temp Rise @ 150Btu/ft
2
(Clear Winter Day)
Temp Rise @ 320Btu/ft
2
(Clear Summer Day)
0.2 gpm (0.75 Lpm)
30
°
F (16.4
°
C)
85
°
F (35
°
C)
0.4 gpm (1.5 Lpm)
15
°
F (8.2
°
C)
42
°
F (17.5
°
C)
0.6 gpm (2.3 Lpm)
10
°
F (5.5
°
C)
28
°
F (11.7
°
C)
0.8 gpm (3 Lpm)
7
°
F (4.1
°
C)
21
°
F (8.7
°
C)
Apricus Solar Collector Installation & Operation Manual - USA
Copyright © 2011 – Apricus Inc Doc: A7-05.4.12-PB Page 15 of 129
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