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In contrast, Figure 10 shows an increased impact of Rscr with cell length, as
in thiscase, the longercell length increases thecurrentdensity,but theTCOmetal
contactarea(busbaronly)remains thesame. Forall cellswithametallic interconnect,
thecellswithametallicgridshowahighercell efficiency(Figure11)comparedto
thecellswithonlyaTCOasthe frontcontact forsimilarRscr (Figure10).
2.5. Influenceof IlluminationPower
Solarpanelsandsolarcellsare testedandcertifiedatan illuminationpowerof
1000 W/m2 (also denoted as onesun). Therefore, the panelconfiguration is usually
optimized for this high intensity. However, in northwest Europe, this high power is
seldom reached. In real life, much of the power generated by solar panels is actually
around an illumination power of 500 W/m2. For cells without a metallic grid, the
influenceof the illuminationpowerwasinvestigatedwithvariationof thecell length,
as shown in Figure 12a. Seemingly, as the illumination power decreases, the impact
of the cell length drops. However, when these data are normalized, as shown in
Figure 12b, it is seen that the relative power is merely shifted toward somewhat
highercell lengthsandthe impact is reducedfor longercells. Nevertheless,down
to an illumination power of 0.5 suns, the cell length remains a critical part of the
configurationoptimization.
Materials
2016,
9,
96
the relative power is merely shifted toward somewhat higher cell lengths and the impact is reduced
for longer cells. Nevertheless, down to an illumination power of 0.5 suns, the ell length remains a
critical part of the configuration optimization.
Figure 12. Efficiency as function of the cell length for different light intensities (see legend in sun units,
whereby one sun is 1000 W/m2): (a)
calculated values; (b)
normalized values.
For cells with a finger grid, the cell efficiency seems to become less affected by the cell length,
as shown in Figure 13, which shows efficiency as function of the cell length for illumination powers
from
0.2
to
1
sun
in
Figure
13a–d.
Note
that
for
each
graph,
the
minimum
value
on
the
x‐axis
is
about
half of the maximum value
to facilitate comparison with Figure 12b.
Figure 12. Efficiency as function of the cell length for different light intensities (see
legend in sun units, whereby one sun is 1000 W/m2): (a) calculated values; (b)
normalizedvalues.
For cells with finger grid, the cell efficiency seems to become less affected
bythecell length,asshowninFigure13,whichshowsefficiencyas functionof the
cell lengthfor illuminationpowers from0.2 to1suninFigure13a–d. Note that for
each graph, the minimum value on the x-axis is about half of the maximum value to
facilitatecomparisonwithFigure12b.
125
Photovoltaic Materials and Electronic Devices
- Title
- Photovoltaic Materials and Electronic Devices
- Author
- Joshua M. Pearce
- Editor
- MDPI
- Location
- Basel
- Date
- 2016
- Language
- English
- License
- CC BY-NC-ND 4.0
- ISBN
- 978-3-03842-217-4
- Size
- 17.0 x 24.4 cm
- Pages
- 216
- Keywords
- Perovskite, Plasmonics, Nanostructured Materials, Anti-Reflection Coatings, Transparent Conductive Oxides, Amorphous Silicon, Dye-sensitized Solar Cells (DSSCs) Materials, Organic Photovoltaic Materials, Solar Energy Materials
- Categories
- Naturwissenschaften Physik
- Technik