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@PHDTHESIS{Rauls:1040585,
author = {Rauls, Edward},
title = {{D}ynamischer {B}etrieb von
{P}olymer-{E}lektrolyt-{M}embran {W}asserelektrolyseuren},
volume = {658},
school = {RWTH Aachen University},
type = {Dissertation},
address = {Jülich},
publisher = {Forschungszentrum Jülich GmbH Zentralbibliothek, Verlag},
reportid = {FZJ-2025-01945},
isbn = {978-3-95806-811-7},
series = {Schriften des Forschungszentrums Jülich Reihe Energie $\&$
Umwelt / Energy $\&$ Environment},
pages = {XIV, 239},
year = {2025},
note = {Dissertation, RWTH Aachen University, 2024},
abstract = {Dynamically operated water electrolyzers can provide
security of supply and power system stability in energy
systems with a high proportion of fluctuating renewable
energy sources such as wind power or photovoltaics. Polymer
Electrolyte Membrane (PEM) electrolyzers are particularly
suitable for these operating scenarios due to their ability
to handle highly dynamic load changes. This work addresses
the impact of dynamic operation of PEM electrolyzers on
efficiency and potential operating scenarios in future
energy systems. For this purpose, a dynamic simulation model
for PEM electrolyzers is developed, parameterized, and
validated on a 100 kWel electrolyzer. This model is scaled
up to the megawatt range and dynamic aspects are
investigated on different scales. The heat-up process of
electrolyzers has the highest average efficiency of 74.1
$\%LHV$ when part-load operation is directly entered at
moderate cell voltages around 1.80 V. Heat-up with auxiliary
electric heaters has a maximum efficiency of 60.0 $\%LHV$
and is therefore less efficient than heatup under partial
load but it qualifies electrolyzers as flexible power sinks.
Standby modes allow reduced start-up times of nominal power
but require electrical power to maintain operating
conditions. Electrolyzers of 400 kWel and larger require
about 2 $\%$ of their rated power in warm standby mode and
between 7 and 9 $\%$ of their rated power under minimum
load. For a 1 MWel electrolyzer, it can be energetically
beneficia to stay in warm standby mode for more than 24
hours, which shortens the return to the nominal operating
point from 37 minutes to a few seconds. During dynamic
operation, short-term fluctuations in operating temperature
of less than 5 K around the set point are observed,
affecting system efficiency by less than ± 0.5 $\%LHV.$
With 50 μm membranes, average cell efficiencies of more
than 73 $\%LHV$ and system efficiencies of more than 67
$\%LHV$ are possible, regardless of the nominal system
power. Oversizing the auxiliary heating from 2.5 to 10 $\%$
of the nominal electrolyzer power of a 1 MWel electrolyzer
does not improve the cell efficiency but worsens the average
system efficiency from 59.7 $\%LHV$ to 53.5 $\%LHV.$
Completely eliminating auxiliary electrical heating improves
the efficiency and part-load capability of electrolyzers.
For example, for a 400 kWel electrolyzer coupled to a
photovoltaic system, simulations demonstrated that the
average system efficiency over one day in increases from
68.7 $\%LHV$ when using auxiliary heating to 70.2 $\%LHV$ in
autothermal operation. The results of the present work can
be used for the development and optimized operation of
electrolysis systems. For energy system analyses, the
consideration of the transient operating conditions of
electrolyzers offers a complementary contribution towards a
better understanding of the effects of fluctuating energy
sources on grid stability provision services.},
cin = {IET-4},
cid = {I:(DE-Juel1)IET-4-20191129},
pnm = {1231 - Electrochemistry for Hydrogen (POF4-123)},
pid = {G:(DE-HGF)POF4-1231},
typ = {PUB:(DE-HGF)3 / PUB:(DE-HGF)11},
urn = {urn:nbn:de:0001-2504140913116.459385823088},
doi = {10.34734/FZJ-2025-01945},
url = {https://juser.fz-juelich.de/record/1040585},
}