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3.3 Estimation <strong>of</strong> <strong>the</strong>rmal energy gain <strong>and</strong> loss through building fenestration 71<br />

Window Heat Gain <strong>and</strong> Loss Energy [kWh/m 2 ]<br />

1,000<br />

0,800<br />

0,600<br />

0,400<br />

0,200<br />

0,000<br />

‐0,200<br />

‐0,400<br />

12/01<br />

12/03<br />

12/05<br />

12/07<br />

12/09<br />

12/11<br />

12/13<br />

12/15<br />

12/17<br />

12/19<br />

12/21<br />

Fig. 3.20: Energy balance for <strong>the</strong> south window in December (left side <strong>of</strong> fig.) <strong>and</strong> in March (right side <strong>of</strong><br />

fig.).<br />

From <strong>the</strong> above figures, it can clearly be seen that even a window with a view facing south<br />

has a negative balance <strong>of</strong> energy during December. Therefore it is necessary to analyze not<br />

only <strong>the</strong> entire building performance, but each <strong>façade</strong> separately <strong>and</strong> <strong>the</strong>ir influence on <strong>the</strong><br />

total energy consumption. All shading surfaces, attached as well as detached to <strong>the</strong><br />

building structure, are included within <strong>the</strong> energy simulation model in order to create <strong>the</strong><br />

optimal physical reality.<br />

3.3.2 Analysis <strong>of</strong> <strong>the</strong> energy balance for windows<br />

12/23<br />

12/25<br />

12/27<br />

12/29<br />

12/31<br />

Window Heat Gain <strong>and</strong> Loss Energy [kWh/m 2 ]<br />

This part <strong>of</strong> <strong>the</strong> dissertation focuses on <strong>the</strong> relationship between <strong>the</strong> space-heating energy<br />

consumption <strong>and</strong> <strong>the</strong> area <strong>of</strong> <strong>the</strong> <strong>glazing</strong> system. It was decided to change <strong>the</strong> window-towall<br />

ratio (WWR) for <strong>the</strong> whole building to ensure that <strong>the</strong> optimal value <strong>of</strong> WWR exists in<br />

<strong>the</strong> first order. The simulations were done for a heating period <strong>and</strong> <strong>the</strong> results are shown in<br />

Fig. 3.21.<br />

1,800<br />

1,600<br />

1,400<br />

1,200<br />

1,000<br />

0,800<br />

0,600<br />

0,400<br />

0,200<br />

0,000<br />

‐0,200<br />

‐0,400<br />

03/01<br />

03/03<br />

03/05<br />

03/07<br />

03/09<br />

03/11<br />

03/13<br />

03/15<br />

03/17<br />

03/19<br />

03/21<br />

03/23<br />

03/25<br />

03/27<br />

03/29<br />

03/31

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