karsten reuter · 2019-09-06 · energy return on investment decentralized earth abundance...
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Technische Universität München
Multiscale Theory of Operando Energy Conversion Systems
Karsten Reuter Chemistry Department and Catalysis Research Center
Technische Universität München
Sustainable Energy Conversion: The Engine of our Society
Sustainable Energy Conversion Strategies
Diversified Solutions
HumanEnergyDemands
Diversified Energy Research
Energy securityAdaptability
Scalability
energy return on investment
earth
abu
ndan
ce
decentralized
intermittenttra
nspa
rent
large-scale
continuous
efficiencystationary
out-doors
stability
high capacity
in-d
oors fle
xibl
e
cycling
mobile
high
pow
er
to global demand
through complementarity
to application requirement
e-conversion: DFG Cluster of Excellence, 2019-2025
computationalscreening
Common Challenges
Views of Heterogeneous Catalysis
© R. Schlögl, 20 nm Cu in10:1 H2 + O2 at 200 mbar and 523 KK. Reuter, Catal. Lett. 146, 541 (2016)
Working Interfaces: Generated by the Functionality They Aim to Drive
K.F. Kalz et al., Chem. Cat. Chem. 9, 17 (2017)DFG SPP2080, 2018-2021
- Operando studies
- Microscopic processes and macroscopic environment
Multiphysics – Multiscale Modeling
i) Oxide Formation in Oxidation Catalysis:Hierarchical multiscale modeling from electrons to the reactor
ii) On the Way to Adaptive Multiscale Modeling:Machine learning as gateway to structural complexity
Agenda
Operando Studies of Model Catalysts
A. Stierle and A.M. Molenbroek (Eds.), MRS Bull. 32 (2007)
P.B. Rasmussen et al., Rev. Sci. Instrum. 69, 3879 (1998)
Reactor STM
S. Yamamoto et al., J. Phys. CM 20, 184025 (2008)
in situ XPS
0.89 eV
DFT-PES for CO(cus) + O(cus)Elementaryprocesses
Red: adsorbed O Blue: adsorbed CO
Microkinetic model
Site
occ
upat
ion
(%)x
xx x
xx x x xxx
x
x
xxx
xx x
2
po2= 10-10 atm
pCO (10-9 atm)
exp.
theory
0.0 1.0 2.0 3.0
Intrinsic catalyticactivity
Heat and masstransport
From Electrons to the Reactor
A. Bruix, J.T. Margraf, M. Andersen and K. Reuter, Nature Catal. 2, 659 (2019)
Electronic Regime: Energetics of Elementary Processes
Active site model„Level of theory“
M. Sabbe, M.F. Reyniers, and K. Reuter, Catal. Sci. Technol. 2, 2010 (2012)
COcus + Ocus → CO2
0.9 eV
A
B
MolecularDynamics
TS
kA→B
kB→A
kineticMonte Carlo
N
t
B
A
∑∑ →→ +−=j
jijj
ijii tPktPkdt
tdP )()()(
ΔEA→B ΔEB→A
∆−Γ=
=
→
→→
TkEZ
ZhTkk
ji
i
jiji
B
)(TSB
exp
Transition State Theory
Tackling Rare-Event Time Scales
First-principles kinetic Monte Carlo simulations for heterogeneous catalysis: Concepts, status and frontiers, K. Reuter, in “Modeling Heterogeneous Catalytic Reactions: From the Molecular Process to the Technical System”, (Ed.) O. Deutschmann, Wiley-VCH, Weinheim (2011)
kmos: A Lattice kMC Framework
M.J. Hoffmann, S. Matera and K. Reuter,Comp. Phys. Commun. 185, 2138 (2014)
Heat and Mass Transfer Effects
T, pCO, pO2
T
S. Matera and K. Reuter, Catal. Lett. 133, 156 (2009)
e.g. CO oxidation
pCO2
p
pO2
pCO
Computational Fluid Dynamics: Accounting for the Flow Field
Computational Fluid Dynamicswith chemical source terms
from 1p-kMC
( ) 2
B
ucad
TmkpATSkπ
=S. Matera and K. Reuter,
Phys. Rev. B 82, 085446 (2010)
Predictive Surface Reaction Chemistry in Real Reactor Models
S. Matera, M. Maestri, A. Cuoci, and K. Reuter,ACS Catal. 4, 4081 (2014)
withM. Maestri and A. Cuoci
(Politecnico Milan)
Laser-Induced Fluorescence (LIF)
Stimulation ofknown excitation
(here: CO2 vibration)
→ 2D concentration profile above catalyst
Y. Zetterberg et al., Rev. Sci. Instrum. 83, 053104 (2012)
12
6
0y-di
rect
ion
[mm
]
400
300
200
100
0 CO
2LI
F si
gnal
[a.u
.]
-4 -2 0 2 4x-direction [mm]
E. Lundgren, J. Gustafson et al. (Lund University) CO oxidation at Pd(100)
CO2
-4 -2 0 2 4x-direction [mm]
1p-kMC/CFD simulation vs. in situ LIF measurementsof near-ambient CO oxidation at Pd(100)
CO : O2 = 1 : 4, ptot = 0.18 atm, T = 600 K, 72 mln/min, 50% Ar
400
300
200
100
0 CO
2LI
F si
gnal
[a.u
.]CO2
CO
Product Boundary Layer as a Non-Invasive Probe
CO2
S. Matera, M. Maestri, A. Cuoci, and K. Reuter,ACS Catal. 4, 4081 (2014)
ptot = 0.18 atm72 mln/min, 50% Ar
Active Pd(100) as a minority phase
on the surface?!
S. Matera, S. Blomberg et al., ACS Catal. 5, 4514 (2015)
Identification of the Active Phase
with E. Lundgren, J. Gustafson et al. (Lund University)
Exp.
PdO(√5x√5)R27°
Pd(100)
i) Oxide Formation in Oxidation Catalysis:Hierarchical multiscale modeling from electrons to the reactor
ii) On the Way to Adaptive Multiscale Modeling:Machine learning as gateway to structural complexity
Agenda
From Static to Adaptive Multiscale Modeling
?
• Generic active siteindependent of operation conditionsdominant over other sites(one site model)
• Atomistic active site model- every atom counts- generally insufficient experimental characterization
- might change drastically operando
Active Sites: The Effective to Atomistic Gap
K. Reuter, C.P. Plaisance, H. Oberhofer, and M. Andersen, J. Chem. Phys. 146, 040901 (2017)
The Active Site in OER at Co3O4
Active site changes withapplied potential
C.P. Plaisance et al., J. Am. Chem. Soc. 137, 14660 (2015);
C.P. Plaisance, K. Reuter, and R.A. van Santen,Faraday Disc. 188, 199 (2016)
Operando Particle Shape Changes in OER at IrO2
Stabilization of {111} facets at operating potentials
D. Opalka, C. Scheurer and K. Reuter, ACS Catal. 9, 4944 (2019)
Ab initio thermodynamics
Computing Approaches to Adsorption Energies
90s 00s 10s
GGA functionals
Rh
Scaling relations Machine learning
- Present set of computational tools well developed to tackle „static“ catalytic problems (→ computational screening)
- Addressing near-ambient in situ studies requires multiscale modelingfrom electrons to the reactor
- Present microkinetic approaches fall short in scrutinizing potentiallycrucial dynamical transformations of the active surface.A self-fulfilling prophecy?!
- Machine learning approaches likely the game changerto tackle the real complexity of working catalysts
We‘ve come a long way to reach half way…
A. Bruix, J.T. Margraf, M. Andersen and K. Reuter, Nature Catal. 2, 659 (2019)
Technische Universität München
THANK YOU!
Mie AndersenAlbert BruixJohannes MargrafHarald Oberhofer
Daniel OpalkaMatteo Maestri (→Polimi)Sebastian Matera (→FU Berlin)Craig Plaisance (→LSU)
J. Gustafson, E. Lundgren (U Lund)A.J. Medford, J. K. Nørskov (DTU)S.V. Levchenko, M. Scheffler (FHI Berlin)