KTB Nr. 2006-35-kj-en Collector test according to EN 12975-1,2:2006
KTB Nr. 2006-35-kj-en Collector test according to EN 12975-1,2:2006
KTB Nr. 2006-35-kj-en Collector test according to EN 12975-1,2:2006
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The power output per collec<strong>to</strong>r unit can be calculated for other collec<strong>to</strong>rs of<br />
this series <strong>according</strong> <strong>to</strong> the follwoing procedure:<br />
with:<br />
P<br />
P ref<br />
A a<br />
A a,ref<br />
P = P ref ∗<br />
Aa<br />
A a,ref<br />
= <strong>Collec<strong>to</strong>r</strong> output for a differ<strong>en</strong>t collec<strong>to</strong>r of the series<br />
= <strong>Collec<strong>to</strong>r</strong> output for collec<strong>to</strong>r Collet<strong>to</strong>re Solare Piano CP4M , (values see table)<br />
= Aperture area of a differ<strong>en</strong>t collec<strong>to</strong>r of the series<br />
= Aperture area of collec<strong>to</strong>r Collet<strong>to</strong>re Solare Piano CP4M<br />
7 Incid<strong>en</strong>ce angle modifier IAM<br />
The IAM (= Incid<strong>en</strong>ce Angle Modifier) is a correction fac<strong>to</strong>r repres<strong>en</strong>ting how the<br />
angle of incid<strong>en</strong>t radiation affects the performance of a collec<strong>to</strong>r.<br />
The IAM of flat plate collec<strong>to</strong>r is assumed as rotation-symmetric. Therefor the<br />
thermal performance of the collec<strong>to</strong>r is only dep<strong>en</strong>ding on the angle betwe<strong>en</strong> the<br />
incid<strong>en</strong>t radiation and the normal of the collec<strong>to</strong>r plane.<br />
θ: 0 ◦ 10 ◦ 20 ◦ 30 ◦ 40 ◦ 50 ◦ 60 ◦ 70 ◦ 80 ◦ 90 ◦<br />
K θ : 1.00 1.00 1.00 0.99 0.98 0.95 0.89 0.76 0.50 0.00<br />
Table 2: Measured (bold) and calculated IAM data for Collet<strong>to</strong>re Solare Piano CP4M<br />
The IAM was measured for one angle (θ = 50 ◦ ). All other angles for the<br />
IAM in table 2 were calculated <strong>according</strong> <strong>to</strong> Ambrosetti 1 (equation 7).<br />
K θ = 1 − [tan θ 2 ] 1 r (3)<br />
1 P.Ambrosetti. Das neue Brut<strong>to</strong>wärmeertragsmodell für verglaste Sonn<strong>en</strong>kollek<strong>to</strong>r<strong>en</strong>, Teil<br />
1 Grundlag<strong>en</strong>. EIR, Wur<strong>en</strong>ling<strong>en</strong> 1983<br />
<strong>KTB</strong> <strong>Nr</strong>. <strong>2006</strong>-<strong>35</strong>-k-j-<strong>en</strong> : <strong>Collec<strong>to</strong>r</strong> <strong>test</strong> <strong>according</strong> <strong>to</strong> <strong>EN</strong> <strong>12975</strong>-1,2:<strong>2006</strong><br />
IMMERGAS S.p.A. , Series Collet<strong>to</strong>re Solare Piano CP4M and Collet<strong>to</strong>re Solare Piano CP2M<br />
04.07.2007, Fraunhofer-ISE, Heid<strong>en</strong>hofstraße 2, D-79110 Freiburg<br />
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