DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities •...

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ElectroCat Workshop – Argonne National Laboratory, July 26 th , 2016 Slide 1 DFT Modeling of PGM-free Catalyst Activity and Durability Edward (Ted) F. Holby, Sigma Division, Los Alamos National Laboratory U =0 V U L = 0.80V LA-UR-16-25411

Transcript of DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities •...

Page 1: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 1

DFT Modeling of PGM-free Catalyst Activity and Durability

Edward (Ted) F. Holby, Sigma Division, Los Alamos National Laboratory

U =0 V UL = 0.80V

LA-UR-16-25411

Page 2: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 2

Summary

• Modeling Goals • Overview of LANL Modeling

Capabilities • Which Structures? • Activity Approach

• Computational Hydrogen Electrode

• Durability Approach • First-principles Molecular

Dynamics • Vibrational Signatures

• Linking Structure to Signature

• Paths Forward • Replacing Fe • Ligand Modification • Strain Engineering

Page 3: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 3

Modeling Goals

• Use modeling approaches to: • Guide synthesis of improved PGM-free electrocatalysts • Aid characterization of synthesized materials by linking atomic scale structure to

experimental spectroscopic signatures and observed properties

• Utilize automation to speed throughput of calculations • Leverage software developed as part of the Materials Genome Initiative (MGI)

Generate structure:property library accessible via web portal

Reaction Coordinate0 1 2 3 4 5 6 7

Free

Ene

rgy

(eV)

0

1

2

3

4

5

IdealFeN4

FeN4(*OH)

U = 0 V Ul = 0.22 V Ul = 0.66 V

Activity Descriptor

Durability Descriptor

Vibrational Signatures

Knock on displacement

threshold energy (?)

Page 4: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 4

LANL Modeling Capabilities

• Combination of computing facilities and theory expertise for materials modeling • Utilized codes:

• Vienna ab initio Simulation Package (VASP) • Amsterdam Density Function Suite (ADF) • Gaussian09 • Large-scale Atomic/Molecular Massively Parallel Simulator (LAMMPS)

• Computing Resources: • LANL IC Wolf Cluster – 9856 Intel Xeon cores, 205 Tflops/s (peak) • LANL IC Moonlight Cluster – 4928 Intel Xeon cores + 616 GPUs, 488 Tflops/s

(peak) • LANL IC Pinto Cluster – 2464 Intel Xeon cores, 51 Tflops/s (peak) • Dedicated 1000 core (extendable) in-house cluster

Page 5: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 5

Active Site Structures

• Which structures to consider? • Guided by relative thermodynamic stability determined via Metropolis Monte

Carlo search and DFT studies • N-coordinates metal • N-metal complexes have lower formation energies at edges • Edge-N-metal complexes thermodynamics driven to form small clusters

• Previously proposed structures • Bio-mimetic guidance • Combinations and permutations of above based on modeling insight

• Spontaneous ligands

Holby and Taylor, App. Phys. Lett., 101, 0641012, 2012; Holby, Wu, Zelenay, and Taylor, ECS Trans. 50, 1839, 2013; Holby, Wu, Zelenay, and Taylor, J. Phys. Chem. C, 118, 14388, 2014; Holby and Taylor, Sci. Rep. 5, 9286, 2015; Holby and Zelenay, Nano Energy, in Press (2016).

-10

-5

0

5

10

15

-2 -1.5 -1 -0.5 0 0.5 1

Form

atio

n En

ergy

(e

V)

N Chemical Potential (eV)

Bulk FeN4Bulk Fe2N6Zig-Zag Fe2N6

Page 6: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 6

Activity Approach: Calculation of PGM-free ORR Activity via DFT

Nørskov et al., J. Phys. Chem. B, 108, 17886, 2004; Anderson, Phys. Chem. Chem. Phys, 14, 1330, 2012; Studt, Catal. Lett., 143, 58, 2013.

0

1

2

3

4

5

6

0 1 2 3 4 5 6 7

Free

Ene

rgy

(eV)

Reaction Coordinate

U = 1.23 V

U = 0 V vs. CHE *OO + 4H+ / *O + *O + 4H+

* + 2H2O

*OH + H+ + H2O

* + 4H+ + O2

*OOH + 3H+ / *OH + *O + 3H+

*O + 2H+ + H2O / *OH + *OH + 2H+

+4e- +4e-

+3e-

+2e-

+e-

O2H4e4HO 22 →++ −+ V1.23potential reversibleUrev ==

Calculation of maximum exergonic potential, Ul, as ORR activity descriptor; computational hydrogen electrode (CHE); DFT of ORR intermediate binding energies

Page 7: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 7

Activity of Predicted Stable Structures – FeCoN5(*OH)

0

1

2

3

4

5

6

0 1 2 3 4 5 6 7

Free

Ene

rgy

(eV)

Reaction Coordinate

IdealFeCoN5(*OH)Ideal FeCoN5(*OH)

U = 0 V

Ul = 0.80 V

• 2 FeCoN5(*OH) defects more thermodynamically stable than Fe2N5(*OH) + Co2N5(*OH)

• FeCoN5(*OH) + *OO → *OOH is potential determining step

Holby and Taylor, Sci. Rep., 5, 9286, 2015.

Page 8: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 8

Durability Approach: First-Principles Molecular Dynamics • Need computational descriptor of durability for application of high-throughput modeling

• Complex corrosion or poisoning phenomenon: includes kinetic barriers, defects, adsorbates, etc.

– How to best simplify? Can simplified model capture complex behavior?

• Tested beam damage model (knock on displacement threshold energy, EKODTE ) for C neighboring defects and adsorbates as initial test of durability descriptor

• Further testing / validation required (ENABLE synthesis / modeling comparisons and Mn/Fe/Co test)

• Plausible durability descriptor hypothesized and initial simulations prove computational accessibility in high-throughput environment

EKODTE = 185 kV EKODTE = 135 kV EKODTE = 155 kV EKODTE = 170 kV

EKODTE = 160 kV

Graphene Monovacancy Divacancy Epoxide Hydroxide

Holby, Fuel Cells, in press.

Page 9: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 9

Durability Approach: First-Principles Molecular Dynamics

• Simulation of e- hitting edge N of an FeN4 edge structure, displacing edge NH structure • N atom most susceptible to removal for both FeN4 edge (124 kV) and bulk (150 kV)

Page 10: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 10

Vibrational Signatures

• Finite-difference method after relaxation with stricter convergence criteria (6N single point DFT calculations required)

• Gives zero point energy (ZPE), vibrational entropy, and vibrational normal modes • Normal modes with and without probe molecule can be used for comparison to experimental

techniques (e.g., Nuclear Resonance Vibrational Spectroscopy, NRVS)

As Prepared Reduced NO(g) treated

Fe2N5 active site model (presumably reduced from Fe2N5(*OH) ) predicts

both NO dissociation as well as relevant NRVS peaks… do other structures?

Page 11: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 11

Paths Forward: Replacing Fe

• Do otherstructures spontaneously form an *OH ligand and does it affect ORR activity? – Use Me-N4 edge structure from stability study

• What role does Me species (Me = Mn, Fe, Co, Ni) play in activity and reaction pathway?

Calculated via Vienna ab initio Simulation Package (VASP) on 5×8 C pair ZZ edge graphene nanoribbons, PBE-GGA with Grimme dispersion correction and 15 Å vacuum with 5×1×1 K-pt mesh and 400 eV plane-wave energy cutoff

MnN4 – ZZ

FeN4 – ZZ

CoN4 – ZZ

MnN4(*OH) – ZZ

FeN4(*OH) – ZZ

CoN4(*OH) – ZZ

NiN4 – ZZ NiN4(*OH) – ZZ

Considered Active-Site Structures

Mn2N5 – ZZ

Fe2N5 – ZZ

Co2N5 – ZZ

Mn2N5(*OH) – ZZ

Fe2N5(*OH) – ZZ

Co2N5(*OH) – ZZ

Page 12: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 12

Theoretical Modeling of Fe-free ORR Potential Energy Surfaces

Reaction Coordinate0 1 2 3 4 5 6 7

Free

Ene

rgy

(eV)

0

1

2

3

4

5

IdealNiN4

NiN4(*OH)

U = 0 V

Ul = 0.35 V Ul = 0.28 V

Reaction Coordinate0 1 2 3 4 5 6 7

Free

Ene

rgy

(eV)

0

1

2

3

4

5

IdealMnN4

MnN4(*OH)

U = 0 V

Ul = 0.08 V Ul = 0.63 V

Reaction Coordinate0 1 2 3 4 5 6 7

Free

Ene

rgy

(eV)

0

1

2

3

4

5

IdealFeN4

FeN4(*OH)

U = 0 V

Ul = 0.22 V Ul = 0.66 V

Reaction Coordinate0 1 2 3 4 5 6 7

Free

Ene

rgy

(eV)

0

1

2

3

4

5

IdealCoN4

CoN4(*OH)

U = 0 V

Ul = 0.62 V Ul = 0.75 V

• Calculation of ORR pathway → persistent *OH for edge MnN4 and FeN4 (but not CoN4 or NiN4) • Activity descriptor, Ul, prediction without *OH modification: Ul,Co > Ul,Fe > Ul,Mn > Ul,Ni • With *OH modification of Mn and Fe: Ul,Fe > Ul,Mn ≈ Ul,Co > Ul,Ni

Page 13: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 13

Fe-free ORR Catalysts—Experiment and Theory

Calculated Ul using computational hydrogen electrode (CHE) formalism and DFT (GGA)

ORR: 0.6 mg/cm2; 0.5 M H2SO4; 900 rpm; 25ºC; Ag/AgCl (3.0 M KCl) reference electrode; graphite counter electrode; steady-

state potential program: 30 mV steps, 30 s/step

Mn Fe Co Ni

0.4

0.5

0.6

0.7

Mn Fe Co Ni0.7

0.8

0.9

Me2N5

MeN4

Experimental

Ul (

V vs

. CH

E) Theoretical

E1/2

E (V

vs.

RH

E) Eonset

0.2 0.4 0.6 0.8 1.0

-3.0

-2.5

-2.0

-1.5

-1.0

-0.5

0.0

Cur

rent

Den

sity

(mA

/cm

2 )

Potential (V vs. RHE)

(CM+PANI)-Ni-C (CM+PANI)-Mn-C (CM+PANI)-Co-C (CM+PANI)-Fe-C

*OH modification determined to occur for MnN4, FeN4 and Me2N5 No *OH modification determined to occur for CoN4 and NiN4 Theoretical prediction of spontaneous *OH ligand modification of active

site structures explains shift in activity trend with Me-N-C catalysts

Ul,Fe > Ul,Co ≥ Ul,Mn > Ul,Ni

Page 14: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 14

ORR Activity of (CM+PANI)-Me-C Catalysts: RDE and Fuel Cell

ORR: 0.6 mg/cm2; 0.5 M H2SO4; 900 rpm; 25ºC; Ag/AgCl (3 M KCl) reference electrode; graphite counter electrode;

steady-state potential program: 30 mV steps, 30 s/step

Anode: 0.2 mgPt cm-2 Pt/C H2,1.0 bar H2 partial pressure; Cathode: ca. 4.0 mg cm-2 (CM+PANI)-Me-C, 1.0 bar air partial

pressure; Membrane: Nafion,211; Cell size: 5 cm2

Current density (A cm-2)

0.0 0.2 0.4 0.6 0.8

Volta

ge (V

)

0.0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9 (CM+PANI)-Fe-C(CM+PANI)-Co-C(CM+PANI)-Mn-C(CM+PANI)-Ni-C

0.2 0.4 0.6 0.8 1.0

-3.0

-2.5

-2.0

-1.5

-1.0

-0.5

0.0

Cur

rent

Den

sity

(mA

/cm

2 )

Potential (V vs. RHE)

(CM+PANI)-Ni-C (CM+PANI)-Mn-C (CM+PANI)-Co-C (CM+PANI)-Fe-C

Promising activity observed from Mn- and Co-based catalysts as alternative to Fe-free ORR catalysts, but further development in MEA fabrication and

catalyst design necessary to approach activity of Fe-based catalysts

Page 15: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 15

Paths Forward: Ligand Modification

• Ligands (spontaneously formed or otherwise) have been shown to be one path forward to improve electrocatalytic activity

• What persistent ligand might be added via synthesis to improve material performance? – OH and NHx suggested in literature

Jia, et al., ACS Nano 9, 12496, 2015. Busch, et al., Nano Energy, in Press. 2016.

Page 16: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 16

Paths Forward: Strain Engineering

• Strain modification of electrocatalyst sites proposed for a variety of other systems, including metal-free ORR catalysts and PGM

Chai, et al., JACS 136, 13629, 2014.

CNT Curvature Effect

Strasser et al., Nature Chemistry, 2, 454, 2010.

Cu Induced Lattice Strain of Pt Core Shell Nanoparticles

“Moderate compressive lattice strain is predicted to enhance the rate of ORR catalysis.”

“The ORR activity of this structure can be tuned by the curvature around the active site.”

Page 17: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 17

Paths Forward: Strain Engineering

• MnCoN5(*OH) has the highest Fe-free Ul value calculated so far (Ul = 0.67 V) • Compressive uniaxial strain of zig-zag nanoribbon leads to less strongly bound *O and *OH • Variability of activity due to strain – suggests possible long-range structural effects on activity

1% compressive uniaxial strain of MnCoN5(*OH) structure increases calculated Ul to 0.70 V and 2% compressive uniaxial strain increases calculated Ul to 0.71 V

C N

Co

O H Mn

Strain Engineering of MnCoN5(*OH)

Page 18: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

229th ECS Meeting – San Diego, California – May 31st, 2016 Slide 18

Acknowledgements

U.S. Department of Energy for funding of “Advanced Cathode Catalysts” project through Office of Fuel Cell Technologies (EERE)

Los Alamos National Laboratory Institutional Computing Program for computational support.

Page 19: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 19

Backup Slides

Page 20: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 20

-1

0

1

2

3

4

5

6

0 1 2 3 4 5 6 7

Free

Ene

rgy

(eV)

Reaction Coordinate

Ideal Fe2N5

Activity of Predicted Stable Structures

U = 0 V

Ul= -0.15 V

Holby and Taylor, Sci. Rep., 5, 9286, 2015.

• Fe2N5(*OH) + *OH → H2O is potential determining step

Page 21: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 21

-1

0

1

2

3

4

5

6

0 1 2 3 4 5 6 7

Free

Ene

rgy

(eV)

Reaction Coordinate

Ideal Fe2N5

Activity of Predicted Stable Structures

• Poor activity from Fe2N5 structure due to OH “overbinding”

U = 0 V

Ul= -0.15 V

Holby and Taylor, Sci. Rep., 5, 9286, 2015.

Page 22: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 22

Activity of Predicted Stable Structures – Fe2N5(*OH)

-1

0

1

2

3

4

5

6

0 1 2 3 4 5 6 7

Free

Ene

rgy

(eV)

Reaction Coordinate

IdealFe2N5Fe2N5(OH)

Ideal Fe2N5 Fe2N5(*OH)

U = 0 V

Ul = 0.72 V

• Fe2N5(*OH) + *OH → H2O is potential determining step

Holby and Taylor, Sci. Rep., 5, 9286, 2015.

Page 23: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 23

Active Site Structures

• M-N3, M-N4, M2-N5, M2-N6 (M = Mn, Fe, Co, Ni) in bulk, zig-zag edge, and arm-chair edge with and without ligands are main focus

Holby and Taylor, App. Phys. Lett., 101, 0641012, 2012; Holby, Wu, Zelenay, and Taylor, ECS Trans. 50, 1839, 2013; Holby, Wu, Zelenay, and Taylor, J. Phys. Chem. C, 118, 14388, 2014; Holby and Taylor, Sci. Rep. 5, 9286, 2015; Holby and Zelenay, Nano Energy, in Press (2016).

Page 24: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 24

Synthesis of CM+PANI Systems

Polyaniline Cyanamide

First heat treatment at 900oC in inert atmosphere

ORR performance evaluation; characterization

0.5 M H2SO4 leach at 80-90oC

NC

H

H

N

Second heat treatment at 900ºC in inert atmosphere

Carbon support (Co, Mn, Ni) chlorides

Page 25: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 25

Molecular Comparison – “FeN4C10” vs. “FeN4C12” Sites

Zitolo et al., Nat. Mat., 14, 937942-, 2015.

U*OH = -0.031 V

U*OH = 0.536 V

“FeN4C10” “FeN4C12”

U*OH = 0.266 V

U*OH = 0.424 V

Calculated via Amsterdam Density Functional (ADF) Suite, Dispersion Corrected PBE-GGA, TZP basis set with no frozen core

Page 26: DFT Modeling of PGM‐Free Catalyst Activity and Durability · LANL Modeling Capabilities • Combination of computing facilities and theory expertise for materials modeling • Utilized

ElectroCat Workshop – Argonne National Laboratory, July 26th, 2016 Slide 26

Stability of (CM+PANI)-Me-C Catalysts after 10,000 Cycles

Potential (V vs. RHE)0.0 0.2 0.4 0.6 0.8 1.0

Cur

rent

den

sity

(mA

cm-2

)

-3

-2

-1

0(CM-PAN)-Fe-C

Highlight: Although slightly lower activity, better stability observed with Co and Mn catalysts

ORR: 0.60 mg/cm2; 0.5 M H2SO4; 900 rpm; 25ºC; Ag/AgCl (3 M KCl) reference electrode; graphite counter electrode; steady-state potential program: 30 mV steps, 30 s/step; Durability cycling: 0.6 - 1.0 V; N2 saturation; 100 mV/s.

Potential (V vs. RHE)0.0 0.2 0.4 0.6 0.8 1.0

Cur

rent

den

sity

(mA

cm-2

)

-3

-2

-1

0(CM+PANI)-Co-C

30 mV drop

10 mV drop

Potential (V vs. RHE)0.0 0.2 0.4 0.6 0.8 1.0

Cur

rent

den

sity

(mA

cm-2

)

-3

-2

-1

0(CM+PANI)-Mn-C

11 mV drop