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Chapter 21 • (EROI) and (EPBT) for PVs 421
quality correction and harmonizing for large battery systems. Koppelaar also examined
the age of systems being analyzed compared with publication dates and found that some
authors were using systems that were 6 years, in an extreme case 18 years old. This had a
serious impact on values for both EpBT and EROI of the pv modules and systems studied.
Five popular types of pv modules often analyzed are monocrystalline (monoSi), mul
ticrystalline, or polycrystalline (multiSi or polySi), amorphous silicon (aSi), CdTe thin
film (CdTe), and CIS thinfilm (CIS). Kumar et al. [20] studied these five types of modules
in varying environments and systems. As can be expected, they found that EpBT varied
greatly from case to case and also that Si volume and methods of production were large
factors in determining CED, which along with efficiency were the largest factors for EpBT.
Overall they found monoSi to have the highest lifecycle energy demand and a large range
in EpBT due to estimations of silicon purification and crystallization processing. polySi
had a much lower EpBT and the thinfilm systems (aSi, CdTe, and CIS) had the lowest
EpBTs. Among the thinfilms, CIS consumed the most primary energy and the aSi had the
longest EpBT due to lower conversion efficiency. CdTe held the lowest EpBT across sys
tems analyzed. Bhandari et al. [38] found similar results when they examined several LCAs
for EpBT and CED. After harmonizing the variables for output, they calculated mean EpBT
varying from 1.0 to 4.1 years. CdTe modules ranked lowest, followed by copper indium
gallium diselenide, aSi, polySi, and monoSi with the highest EpBT. They also found that
across different types of pv, variation in CED was greater than that in efficiency and perfor
mance ratio, concluding that CED, not efficiency, has greater influence on EpBT.
If a low CED is the important factor for a low EpBT, we can assume that new manufac
turing technologies and application methods, such as advanced production processes and
reducing raw material consumption, especially silicon, would show a reduction in EpBTs
over time. Wong et al. [39] studied the difference in monoSi versus polySi pv process
ing and found that the former had a larger CED due to an additional Czochralski process,
which has a significant energy requirement. Although this results in greater conversion
efficiency for monoSi, it is insufficient to lower the EpBT below that of polySi. Wong et al.
describe another approach to manufacturing a combination of monoSi and polySi into
a hybrid cSi, which eliminates the need for the extra Czochralski process and produces
a pv module with greater efficiencies than polySi but lower energy costs than monoSi.
They also note that wafer thickness has been greatly reduced without losing efficiency by
the use of reflective backcoatings, which increase chances of photon capture.
In the few studies that have applied harmonization to NEA, EpBT, and EROI analyses,
a reduction in CED across the industry was found. Gorig and Breyer [40] calculated and
compared the CED of different modules and systems over time using LCAs. They employed
financial learning curve concepts to determine the energy demand for major pv systems.
They weighted both module and system energy demand according to their share in the
pv market at the time and found that the CED for all modules and systems, for which
there was adequate marketing data, had decreased over time. The modules and systems
with higher amounts of Si decreased at faster rates. They showed that energy consumption
in pv manufacturing followed the loglinear learning curve and BOS, such as aluminum