co and no-induced disintegration of rh, pd, and pt...
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CO and NO-induced disintegration of Rh, Pd, and Pt nanoparticles on TiO2(110): A first principles study Bryan Goldsmith,1 Evan Sanderson,2 Runhai Ouyang,3 Wei-Xue Li3
1. Department of Chemical Engineering, University of California, Santa Barbara, CA, 93106-5080 2. Department of Chemistry & Biochemistry, University of California, Santa Barbara, CA 93106-9510
3. State Key Laboratory of Catalysis, Dalian Institute of Chemical Physics, Chinese Academy of Sciences, Dalian 116023, China
Introduction
Free energy of reactant-induced NP disintegration
Computational Methodology
Adatom complex formation and particle energetics
adatom/support support bulkformationE E E E= − −
NP disintegration in the presence of reactants is common
e.g. Rh/TiO2, Rh/Al2O3, Pd/Fe2O3, Pt/SiO2, Ir/Al2O3, Ni/TiO2, Ru/TiO2
Most stable adatom positions on TiO2(110), corresponding to formation energies of 2.88, 2.01 and 3.12 eV for Rh, Pd, and Pt, respectively.
If ΔGdisintegration is negative, then the NP should be expected to disintegrate under equilibrium conditions.
Disintegration of supported nanoparticles (NPs) in the presence of reactants can lead to catalyst deactivation or be exploited to redisperse sintered catalysts.
Nanoparticle disintegration can cause catalyst deactivation
Rh/SiO2
Disintegration
Most active size
Density Functional Theory modeling using Vienna Ab-initio Simulation Package
Projector Augmented Wave method RPBE Functional + Spin polarization Plane wave kinetic energy cutoff = 400 eV Forces converged to 0.03 eV/Å via conjugate gradient
Vacuum layer thickness of 15 Å Bottom two tri-layers are fixed in positions.
(4x2) Rutile TiO2(110)
Periodic model
00
0
3( , , ) ( , ) xf x B
pG R T p E n T p k TLn TSR p
µ Ω
∆ = − − + −
medisintegration
γ
Formation energy of adatom complex
Standard gas phase chemical potential
Configurational entropy of complexes
Nanoparticle energy
0G∆ <disintegration
Disintegration can be modeled by the Gibbs Free Energy
An exothermic adatom complex formation energy and a small particle radius will promote NP disintegration. Increasing the reactant species chemical potential, by raising pressure or lowering temperature, will also enhance disintegration.
We address the following questions: Between supported Rh, Pd and Pt catalysts, which one is more susceptible to the disintegration. Among NO and CO, which one is more efficient for the
redispersion of the low surface area catalyst. How sensitive do these results depend on the particle size,
temperature and partial pressure.
Density functional theory allows the rapid calculation of the effects of reactant partial pressure (p), temperature (T), NP radius (R), as well as particle morphology on the stability of supported NPs toward disintegration into adatom complexes.
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Rh(CO)2 and Rh(NO)2 have more favorable formation energies than Rh(CO) and Rh(NO)
Formation energy = 0.75 eV -1.35 eV
-0.02 eV -1.58 eV
C O
Rh
N
Rh(CO)2
Rh(NO)2
Rh(CO)
Rh(NO)
Rh Pt
Pd
NO binding on (111) facet
NO chemical potential (eV)
Acknowledgments References
Pt, Pd, Rh NP/TiO2(110) disintegration
Conclusions The interaction between CO and NO with the Rh adatom is
greater than for the Pd and Pt adatoms. The Rh/TiO2(110) NPs are less resistant to CO and NO-induced
disintegration than the Pd/TiO2(110) and Pt/TiO2(110) NPs NO is a more efficient reactant for particle redispersion than CO
Influence of CO and NO adsorption on Pt, Pd, or Rh nanoparticle surface energetics 𝜸𝒎𝒎
Reactant environment and particle size effects on supported nanoparticle energy
Rh NPs are more susceptible to CO and NO-induced disintegration compared to both Pd and Pt NPs, and NO is a greater promoter of NP disintegration than CO. The facile disintegration of Rh NPs is due to the large and exothermic formation energy of the Rh adatom complexes. These findings provide insights for how to either prevent or promote reactant-induced NP disintegration.
[1] McClure, S. M.; Lundwall, M. J.; Goodman, D. W. Proc. Natl. Acad. Sci. 2011, 108, 931 [2] Ouyang, R.; Liu, J.-X.; Li, W.-X. J. Am. Chem. Soc. 2012, 135, 1760
The interaction of CO and NO with Rh adatom is greater than for Pd and Pt adatoms
Formation energy
Rh Pd Pt
Metal(CO) 0.75 0.26 0.09 Metal(CO)2 -1.35 -0.54 -0.69 Metal(NO) -0.02 -0.05 -0.10 Metal(NO)2 -1.58 -0.67 -0.68 Energies are in eV.
Exothermic formation energy promotes particle disintegration
CO and NO bind strongest to Rh metal compared to Pd and Pt metals
111 111( , ) [ ( , )] ( , )me i i i mei
meT P f T PT Pγ γ γ γ γ∆= + ∆ ≈ +∑
Rh Pt Pd
CO binding on (111) facet
CO chemical potential (eV)
Redu
ctio
n in
su
rfac
e en
ergy
(eV/
Å2 )
Temperature ↓, Pressure ↑, Coverage ↑
Redu
ctio
n in
su
rfac
e en
ergy
(eV/
Å2 )
NPE∆
LESS STABLE MO
RE S
TABL
E
(111)NP
3 γΔE =
RΩ
NPE∆
contours (Ω is molar volume)
In the presence of CO In the presence of NO
eV
eV
This work was funded by the NSFC (21173210, 21225315), the 973 Program (2013CB834603), and the NSF-OISE 0530268. B.R.G. acknowledges the PIRE-ECCI program for a graduate fellowship. E.D.S. thanks IRES-ECCI for an undergraduate summer research fellowship.
These trends, which are manifested by the interplay between coverage dependent adsorption energies, reactant-induced surface stabilization, and NP size, give insight into the variability of particle stability over a broad range of reaction conditions.
diameter = 20 Å
In agreement with experiment, Rh(CO)2 predicted to form but not Rh(CO)
Rh(CO)2 Exp.
Detected
not detected
Pd and Pt not predicted to form adatom complexes
In the presence of CO
CO chemical potential (eV)
Gibb
s fre
e en
ergy
of
disi
nteg
ratio
n (e
V)
Exp. Suggested
In agreement with experimental suggestions, Rh(NO)2 predicted to form
Pd and Pt not predicted to form adatom complexes (Under typical conditions)
In the presence of NO
Gibb
s fre
e en
ergy
of
disi
nteg
ratio
n (e
V)
NO chemical potential (eV)
diameter = 20 Å
Include gas phase disintegration Consider adatom translation Particle size-dependent binding
energies
Future work
Reduction in surface energy due to reactant binding
At a specified gas phase chemical potential, the adatom complex that is most likely to form has the most negative disintegration free energy.
Pd(CO)2 (g)