DSC INTEGRATED GLASSBLOCKS

Page 156

Chapter 4 - Optical performance analysis

In Chart 4.16 the repar33on of the incident radiant flux in total transmi4ance (τ) total reflectance (ρ) together with the rela3ve absorptance of the glassblock (αgb) and the rela3ve absorptance of the DSC (αdsc) are shown in respect of the energy conserva3on law and in dependance of the wavelength. 1,00

ďƐŽƌƉƚĂŶĐĞ͕ ZĞŇĞĐƚĂŶĐĞ͕ dƌĂŶƐŵŝƩĂŶĐĞ

0,90

ʏ

0,80 0,70 0,60

ʌ

0,50 0,40

ɲ dsc

0,30 0,20

ɲ gb

0,10 0,00

400

490

550

670

760

850

940

1030

1120

1210

1300

1400

ǁĂǀĞůĞŶŐƚŚ ;ŶŵͿ Chart 4.16 Hyp. 1a: spectral data

The device behaves as an almost opaque body (with very low transmi4ance in the visible range) showing maximum transmi4ance (about 55%) at 760 nm ca. This result is very much influenced by the DSC type selected. In fact the selected DSC is more designed for high conversion efficiency to the detriment of total transmi4ance: the cell absorbs the most within the visible range, which is also the most energe3c, leading by consequence to a very low transmi4ance in the same range. We want to remember that in this simula3on an improvement in transmi4ance of about 10% can be considered in order to take in account the area not covered by the ac3ve surface in a module, which is not included in the simula3on. 157


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