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Self-Formed Catalysts Using
Electrochemical
(de)Lithiation for Oxygen
Evolution Reaction
Vaidish Sumariaa, Dilip Krishnamurthyb, Venkat Viswanathana,b
aDepartment of Chemical Engineering, Carnegie Mellon University
bDepartment of Mechanical Engineering, Carnegie Mellon University
1
Introduction
• Solar Energy – Inexhaustible Natural resource
• Oxygen evolution reaction – Key process in enabling solar driven water
splitting.
PEMFC
SOFC
2
Current Scenario
IrO2 and RuO2 – among the most active
catalysts
i. Material Scarcity
ii. High cost
Lee Y. et. al. J. Phys. Chem. Lett., 2012, 3 (3), pp Man I.C. et. al. ChemCatChem 2011, 3, 1159 –
Reaction Mechanism for Oxygen Evolution Reaction
2H2O l → O2 g + 4H+
+ 4e−
(ΔGrxn = 4.92 eV)
Associative mechanism
H2O (l) + *  OH* + H+ + e- (Δ𝐺1)
OH*  O* + H+ + e- (Δ𝐺2)
O* + H2O (l)  OOH* + H+ + e- (Δ𝐺3)
OOH*  * + O2 (g) + H+ + e- (Δ𝐺4)
3
Man I.C. et. al. ChemCatChem, 2011, 3, 1159 –
E H+
+ E e−
= −
kT
2
ln 10 × pH + −eU +
1
2
× E H2 g
Calculated using DFT
∆𝐺 = ∆𝐸 − 𝑇∆𝑆 + 𝑍𝑃𝐸
Potential Determining Steps
4
𝐺𝑂𝐸𝑅
= max[ ∆𝐺1
0
, ∆𝐺2
0
, ∆𝐺3
0
, ∆𝐺4
0
]
Potential determining step - last step to become
downhill in free energy as the potential
increased.
Scaling relation : Δ𝐸𝑂𝑂𝐻 = Δ𝐸𝑂𝐻 + 3.2 (𝑒𝑉)
𝐺𝑂𝐸𝑅
= max ∆𝐺2
𝑜
, ∆𝐺3
𝑜
= max[ ∆𝐺2 , 3.2- ∆𝐺2 ]
= max[ ∆𝐺3 , 3.2- ∆𝐺3 ]
Descriptors (∆𝐺2) or (∆𝐺3) can be used as the
single descriptor to predict limiting potential.
Tuning the Adsorption Characteristics
• Strain
5
Strasser P. et. Al., Nature Chemistry, 2010, 2, 454–460
Tuning the Adsorption Characteristics
6
• Changing the Electronic Structure
Stamenkovic V., Angewandte Chemie 118.18 (2006): 2963-2967.
(De)Intercalation –To tune Activity
2D Layered Materials – emerging family of materials with tunable properties
Wang H. et. al. Proc. Natl. Acad. Sci., (2013) 110(49) 19701- 7
(De)Intercalation – Tool to tune Activity
Lu Z. et. al. Nat. Commun., 5 (2014): 8
Criteria For Catalyst selection
“Cathodic materials”
Potentially suitable for Oxygen
Evolution
LCO , LMO , LFP , NMC, NMO, NCA
etc.
“Anodic materials”
Potentially suitable for Oxygen
Reduction
Graphene , MoS2 , h-BN , M-Se2 etc.
Stability
1. ∆𝐺𝑓𝑜𝑟𝑚 < 0
2. At the reaction potential, material
should:
• Not undergo phase transition
• Not undergo decomposition
9
Lattice Optimization
Optimizing the bulk lattice of LiCoO2 and understanding the
effect of (de)litiation on the materials lattice parameters
Lattice Optimization for
LiCoO2
c (DFT)
c
(Experimental)
Li0.25CoO2 14.23 14.2
Li0.50CoO2 14.66 14.4
Li0.75CoO2 14.37 14.3
LiCoO2 14.16 14.07
10
Amatucci, G. G. et. al. , J. Electrochem. Soc., 143.3 (1996): 1114-
Pourbaix Diagram (LiCoO2)
11
The free energy of a given surface
as a function of the potential can be
given as:
𝑈 = 𝑛 ∗ 𝜃 ∗ (Δ𝐺𝑟𝑥𝑛(𝑈 = 0) − 𝑈)
Where:
n = No. of electron involved
𝜃 = Coverage on the surface
Uncertainty Quantification using BEEF-vdW
12
Wellendorff, Jess, et al., Phys. Rev. B 85.23 (2012): 235149.
Probabilistic Pourbaix Diagram
13
Fraction on
Surface (%)
Clean 4.5
½ ML OH* 44.8
½ ML O* 50.7
Surface coverage prediction at
U=0
Activity Volcano
14
Conclusion
• Intercalation materials can be
the new direction to look for
cheaper and high activity
catalysts
• We develop a new
methodology to predict the
surface structure incorporating
the uncertainties obtained
using BEEF-vdW exchange
correlation.
• Develop a thorough
probabilistic Pourbaix
Diagram for the various
phases of LixCoO2 and
understand its effects on
activity.
• Develop a general descriptor
based approach to identify
new for intercalation
materials as catalysts for
various electrochemical
15
Future Work

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Sumaria_ECS_2017.pptx

  • 1. Self-Formed Catalysts Using Electrochemical (de)Lithiation for Oxygen Evolution Reaction Vaidish Sumariaa, Dilip Krishnamurthyb, Venkat Viswanathana,b aDepartment of Chemical Engineering, Carnegie Mellon University bDepartment of Mechanical Engineering, Carnegie Mellon University
  • 2. 1 Introduction • Solar Energy – Inexhaustible Natural resource • Oxygen evolution reaction – Key process in enabling solar driven water splitting. PEMFC SOFC
  • 3. 2 Current Scenario IrO2 and RuO2 – among the most active catalysts i. Material Scarcity ii. High cost Lee Y. et. al. J. Phys. Chem. Lett., 2012, 3 (3), pp Man I.C. et. al. ChemCatChem 2011, 3, 1159 –
  • 4. Reaction Mechanism for Oxygen Evolution Reaction 2H2O l → O2 g + 4H+ + 4e− (ΔGrxn = 4.92 eV) Associative mechanism H2O (l) + *  OH* + H+ + e- (Δ𝐺1) OH*  O* + H+ + e- (Δ𝐺2) O* + H2O (l)  OOH* + H+ + e- (Δ𝐺3) OOH*  * + O2 (g) + H+ + e- (Δ𝐺4) 3 Man I.C. et. al. ChemCatChem, 2011, 3, 1159 – E H+ + E e− = − kT 2 ln 10 × pH + −eU + 1 2 × E H2 g Calculated using DFT ∆𝐺 = ∆𝐸 − 𝑇∆𝑆 + 𝑍𝑃𝐸
  • 5. Potential Determining Steps 4 𝐺𝑂𝐸𝑅 = max[ ∆𝐺1 0 , ∆𝐺2 0 , ∆𝐺3 0 , ∆𝐺4 0 ] Potential determining step - last step to become downhill in free energy as the potential increased. Scaling relation : Δ𝐸𝑂𝑂𝐻 = Δ𝐸𝑂𝐻 + 3.2 (𝑒𝑉) 𝐺𝑂𝐸𝑅 = max ∆𝐺2 𝑜 , ∆𝐺3 𝑜 = max[ ∆𝐺2 , 3.2- ∆𝐺2 ] = max[ ∆𝐺3 , 3.2- ∆𝐺3 ] Descriptors (∆𝐺2) or (∆𝐺3) can be used as the single descriptor to predict limiting potential.
  • 6. Tuning the Adsorption Characteristics • Strain 5 Strasser P. et. Al., Nature Chemistry, 2010, 2, 454–460
  • 7. Tuning the Adsorption Characteristics 6 • Changing the Electronic Structure Stamenkovic V., Angewandte Chemie 118.18 (2006): 2963-2967.
  • 8. (De)Intercalation –To tune Activity 2D Layered Materials – emerging family of materials with tunable properties Wang H. et. al. Proc. Natl. Acad. Sci., (2013) 110(49) 19701- 7
  • 9. (De)Intercalation – Tool to tune Activity Lu Z. et. al. Nat. Commun., 5 (2014): 8
  • 10. Criteria For Catalyst selection “Cathodic materials” Potentially suitable for Oxygen Evolution LCO , LMO , LFP , NMC, NMO, NCA etc. “Anodic materials” Potentially suitable for Oxygen Reduction Graphene , MoS2 , h-BN , M-Se2 etc. Stability 1. ∆𝐺𝑓𝑜𝑟𝑚 < 0 2. At the reaction potential, material should: • Not undergo phase transition • Not undergo decomposition 9
  • 11. Lattice Optimization Optimizing the bulk lattice of LiCoO2 and understanding the effect of (de)litiation on the materials lattice parameters Lattice Optimization for LiCoO2 c (DFT) c (Experimental) Li0.25CoO2 14.23 14.2 Li0.50CoO2 14.66 14.4 Li0.75CoO2 14.37 14.3 LiCoO2 14.16 14.07 10 Amatucci, G. G. et. al. , J. Electrochem. Soc., 143.3 (1996): 1114-
  • 12. Pourbaix Diagram (LiCoO2) 11 The free energy of a given surface as a function of the potential can be given as: 𝑈 = 𝑛 ∗ 𝜃 ∗ (Δ𝐺𝑟𝑥𝑛(𝑈 = 0) − 𝑈) Where: n = No. of electron involved 𝜃 = Coverage on the surface
  • 13. Uncertainty Quantification using BEEF-vdW 12 Wellendorff, Jess, et al., Phys. Rev. B 85.23 (2012): 235149.
  • 14. Probabilistic Pourbaix Diagram 13 Fraction on Surface (%) Clean 4.5 ½ ML OH* 44.8 ½ ML O* 50.7 Surface coverage prediction at U=0
  • 16. Conclusion • Intercalation materials can be the new direction to look for cheaper and high activity catalysts • We develop a new methodology to predict the surface structure incorporating the uncertainties obtained using BEEF-vdW exchange correlation. • Develop a thorough probabilistic Pourbaix Diagram for the various phases of LixCoO2 and understand its effects on activity. • Develop a general descriptor based approach to identify new for intercalation materials as catalysts for various electrochemical 15 Future Work