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IEA Solar Heating and Cooling Programm - NachhaltigWirtschaften.at

IEA Solar Heating and Cooling Programm - NachhaltigWirtschaften.at

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<strong>IEA</strong> SHC Task 38 <strong>Solar</strong> Air Conditioning <strong>and</strong> Refriger<strong>at</strong>ion Subtask A Report, November 2009<br />

Serial flow, "Low Flow"<br />

∆M ges = 10 - 15 l/m 2 h rel<strong>at</strong>ed to<br />

collector area<br />

Parallel flow, "High Flow"<br />

∆M ges= 50 l/m 2 h rel<strong>at</strong>ed to<br />

collector area<br />

∆M ges = ∆M col = 10 - 15 l/m 2 h ∆M ges = 4 * ∆M col = 50 l/m 2 h<br />

∆p ges = 4 * ∆p col<br />

∆p ges = ∆p col<br />

∆T ges = 4 * ∆T col = 40 °C ∆T ges = ∆T col = 10 °C<br />

∆M col<br />

∆Τ<br />

∆p<br />

∆M col<br />

∆Τ<br />

∆p<br />

∆M col<br />

∆Τ<br />

∆p<br />

∆M col<br />

∆Τ<br />

∆p<br />

∆M col<br />

∆Τ<br />

∆p<br />

∆M col<br />

∆Τ<br />

∆p<br />

∆M col<br />

∆Τ<br />

∆p<br />

∆M col<br />

∆Τ<br />

∆p<br />

∆M ges<br />

∆M ges<br />

Fig. 7: Hydraulics for the collector field for low flow serial (left) <strong>and</strong> high flow parallel (right)<br />

systems. In all cases care has to be taken to maintain an equal resistance in all parallel<br />

lines. This can be partly achieved by a “Tichelmann” arrangement where the added length of<br />

the inlet <strong>and</strong> outlet pipes is the same for all parallel collectors (Streicher 2008).<br />

Many existing solar combisystems (without cooling function) work with the low-flow principle<br />

in the collector loop. The advantage is th<strong>at</strong> the necessary temper<strong>at</strong>ure lift for domestic hot<br />

w<strong>at</strong>er prepar<strong>at</strong>ion <strong>and</strong> space he<strong>at</strong>ing can be reached in one step in the solar collector if the<br />

solar radi<strong>at</strong>ion is high enough. Therefore, the auxiliary he<strong>at</strong>er has to be oper<strong>at</strong>ed less<br />

frequently.<br />

When connecting such a system to a thermally driven chiller, this can be a problem because<br />

the temper<strong>at</strong>ure difference between flow <strong>and</strong> return of the hot side of the chiller is typically<br />

small (~ 6 K). Therefore it would make more sense to oper<strong>at</strong>e the collector loop (<strong>at</strong> least for<br />

the cooling mode) <strong>at</strong> this small temper<strong>at</strong>ure difference r<strong>at</strong>her than the roughly 30-40 K th<strong>at</strong><br />

are typical for low-flow solar combisystems due to the domestic hot w<strong>at</strong>er (DHW) dem<strong>and</strong>.<br />

During the summer high flow oper<strong>at</strong>ion would be favourable for solar cooling but low flow<br />

oper<strong>at</strong>ion would be favourable for DHW production.<br />

One option to overcome this dilemma is to switch the collector loop <strong>at</strong> least between low-flow<br />

oper<strong>at</strong>ion in winter to high-flow oper<strong>at</strong>ion in summer. However, care has to be taken to<br />

ensure proper turbulent flow <strong>and</strong> acceptable pressure drops in the collector circuit as well as<br />

on the balanced flow through all parallel collector tubes.<br />

There are in principle four options:<br />

• The collector hydraulics stay the same in summer <strong>and</strong> winter but the mass flow<br />

through the collector varies by switching the pump speed or the type of pump. In this<br />

page 14

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