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THE HISTORY OF SPACE SOLAR CELLS 415<br />

cells providing over 10 kW of power. The 1970s also saw the first use of shallow junction<br />

silicon cells for increased blue response and current output, the use of the back surface<br />

field, the low–high junction theory for increased silicon cell voltage output, and the<br />

development of wraparound contacts for high efficiency silicon (HES) cells to enable<br />

automated array assembly and to reduce costs.<br />

In the 1980s, the gap between theoretical efficiencies and experimental efficiencies<br />

for silicon, gallium arsenide, and indium phosphide became almost nonexistent (see<br />

Figure 10.1) [12]. New thin-film cells of amorphous silicon and CuInGaSe 2 brought the<br />

possibility of higher thin-film efficiencies and flexible, lightweight substrates that excited<br />

the space community. However, silicon still provided the majority of the power for space<br />

and eventually the solar arrays for the International Space Station (ISS) (see Figure 10.2).<br />

35<br />

30<br />

25<br />

20<br />

15<br />

10<br />

Ge<br />

Si<br />

CIGS<br />

CIS<br />

InP<br />

Best confirmed efficiency under AM1.5<br />

standard conditions (T = 25°C)<br />

GaAs<br />

Cu 2 S CuInS 2<br />

CdTe<br />

a-Si:H<br />

CuGaSe 2<br />

Black-body limit<br />

AM0<br />

AM1.5<br />

CdS<br />

5<br />

0.5 1.0 1.5 2.0 2.5<br />

Band gap<br />

[eV]<br />

Figure 10.1 Comparison of measured cell efficiencies to the theoretical limits as a function of<br />

band gap [12]<br />

(a)<br />

(b)<br />

Figure 10.2 (a) Current status of International Space Station (ISS) and (b) planned configuration<br />

of ISS by 2004. (Pictures courtesy of NASA)

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