Eirelec 2011- Oxygen Evolution at Oxidized Metal and Metal Oxide Electrodes - Iron in Base

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    Mike LyonsSchool of Chemistry

    Trinity College Dublin 2

    [email protected]

    Eirelec 11: Electrochemistry-The Future?Dun Raven Arms, Adare, Limerick, 17 May 2011

    Plus a change, plus c'est la mme chose.Alphonse KARR, Les Gupes 1849.(The more things change, the more they remain the

    same. ...)

    mailto:[email protected]:[email protected]
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    Hydrogen Economy Transition Metal Oxides: compact and hydrous. Preparation of Hydrous Oxide modified Fe

    electrodes via Repetive Potential Cycling Method

    (RPCM) Duplex layer model of oxide/solution interface. Acid/base behaviour of hydrous oxide film :

    interconnected anionic surfaquo groups.

    Redox switching behaviour of hydrous oxide film. OER kinetics and mechanism of oxide modified Fe

    electrodes in aqueous base. Concluding comments.

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    The Hydrogen Economy:Hydrogen as an energy carrier.

    G.W. Crabtree, M.S. Dresselhaus, M.V.

    Buchanan, The hydrogen Economy PhysicsToday, Dec.2004, pp.39-45.U. Bossel, Does a hydrogen economy makesense? Proc. IEEE, 94 (10)(2006), pp.1826-1836.

    P.P. Edwards, V.L. Kuznetsov, W.I.F. David,N. Brandon. Energy Policy 36(2008) 4356-4362.

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    2 types: Compact anhydrous oxides,

    e.g.

    rutile, perovskite, spinel. Oxygen present only as bridging

    species between two metalcations and ideal crystalsconstitute tightly packed giant

    molecules. Prepared via thermal techniques,e.g decomposition of unstablesalt

    Micro-dispersed hydrousoxide

    s Oxygen is present not just as a

    bridging species between metalions, but also as O-, OH and OH2species in coordinated terminalgroup form.

    Hydrous oxides in contact withaqueous media contain largequantities of loosely bound andtrapped water plus electrolytespecies.

    Prepared via base precipitation,electrochemical techniques.

    Materials are prepared inkinetically most accessiblerather than thermodynamicallymost stable form.

    Are often amorphous or onlypoorly crystalline and prone torearrangement.

    L. D. Burke, M.E.G. Lyons,

    Modern Aspects Electrochemistry, 18 (1986)169-248.

    Geothite

    FeOOH

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    Cathodic Hydrogen Evolution Reaction (HER)

    Acid: 2H3O+ + 2e- H2(g) +2 H2OBase: 2H2O + 2e- H2(g) + 2 OH-

    Simplest (therefore most studied) representative electro-catalytic reaction.Multistep process involving adsorbed intermediates.

    Classical analysis assumes HEROccurs on oxide free metal surface.

    Volmer (V) : hydrogen adsorption or discharge step.H3O+ + M + e- MHads + H2O

    H2O + M + e- MHads + OH-

    Heyrovsky (H): Electrochemical Desorption step.MHads + H3O+ + e- H2(g) + M + H2OMHads + H2O + e- H2(g) + M + OH-

    Tafel (T) : Chemical Desorption step.MHads + MHads H2(g) + 2M

    2 main mechanisms : Volmer-Heyrovsky (VH) Volmer-Tafel (VT).

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    Kinetically limiting step in waterelectrolysis cells and PEM fuel cell.

    Multistep multi-electron transfer reaction

    involving adsorbed intermediates. Overall reaction (alkaline medium)

    O2 + 2H2O + 4e- 4OH-

    E0 = 0.303 V (vs. Hg/HgO)

    Krasilshchikov (1963)

    S + OH-

    SOHad + e-

    SOHad + OH- SO-ad + H2O

    SO-ad SOad + e-

    2SOad 2S + O2

    Bockris Electrochemical Oxide (1956)

    S + OH-

    SOHad + e-

    SOHad + OH- SO + H2O + e

    -

    SO + SO 2S + O2

    Krasilshchikov/modification thereof, ispathway most often proposed for OER onmetal / metal-oxide electrodes in alkalinesolution.

    Depending on RDS can explain a variety ofTafel slopes.

    Modification permits concept of

    formation/decomposition of higher oxide e.g.for Ni

    OH- OHad+ e-

    OHad+ OH- O-ad+ H2O

    2 -NiOOH + O-ad 2NiO2+ H2O + e-

    2NiO2 + H2O 2 -NiOOH + Oad

    Oad+ Oad O2

    OER at oxidized metal and metal oxideelectrodes involves active participation ofoxide.

    Acid/base behaviour of oxide importantconsideration .

    Concept of active surface or surfaquo groupsimportant.

    Anodic Oxygen Evolution Reaction (OER)

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    L.D. Burke, E.J.M. OSullivan J. Electroanal. Chem., 93 (1978) 11.

    Rhodium redox chemistry: alkaline solution

    L.D. Burke, E.J.M. OSullivan, J. Electroanal. Chem., 117(1981) 155.

    Microdispersed hydrous oxide formedvia potential cycling technique (similar

    to poly(aniline) deposition to form PME).

    Duplex layer model: oxide/solution

    interface.

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    OSullivan & Burke,

    J. Electrochem. Soc.,137 (1990) 466.

    OER activity & mechanism(shift in OER potential anddecrease in Tafel slope)

    depends on charge capacity(thickness) of hydrousoxide layer.

    Increasing oxidethickness

    OER atmulticycledhydrous rhodiumoxide modified

    electrodes.

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    Fe + OH- FeOH(ads.) + 2e-

    FeH(ads.) Fe + H+ + e-

    A1

    FeOH(ads.) + OH- Fe(OH)2 + e-

    FeOH(ads.) + OH- FeO + H2O + e-

    A2

    [Fe2(OH)63H2O]2- + 3OH- [Fe2(OH)9]3- +3H2O + 2e-

    A3/C2

    [Fe(OH)3.5

    nH2O]0.5-(Na+)

    0.5+ e- Fe(OH)

    2n H

    2O + 0.5Na+ + 1.5OH-

    FeO.FeOOH + H2O + 3e- Fe + FeO22- + H2O + OH-

    C1

    A0: OER

    C0: HER

    Surface redox chemistry: Bright Fe electrode

    3Fe(OH)2 + 2OH- Fe3O4 + 4H2O + 2e

    -

    3FeO + 2OH- Fe3O4 + H2O + 2e-

    A4

    In situ Raman

    EQCMRRDE

    Greater fine structureobserved at low sweeprate.

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    Hydrous Oxide Growth via Cyclic Potential Multicycling (CPM)Procedure of Fe electrode in aqueous alkaline solution.

    Layer growth parameters: Upper, lower potential

    sweep limits. Solution temperature. Solution pH. Potential sweep rate. Base concentration. N

    A3

    C2 0.5 M NaOH

    Lyons, Burke, J. Electroanal. Chem., 170 (1984) 377-381

    Lyons, Burke, J. Electroanal. Chem., 198 (1986) 347-368

    Lyons, Brandon Phys. Chem. Chem. Phys., 11 (2009) 2203-2217

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    N

    0 200 400 600

    Q/mC

    cm-

    2

    0

    20

    40

    60

    80

    100

    120

    Q=a(1-exp(-bN))

    R=0.9947, R2 = 0.9895a = 103.94 6.05 mC/cm2

    b = 0.0044 0.0006 cycle-1

    Hydrous oxide growth kinetics

    Number of Growth Cycles

    0 100 200 300 400 500

    Charge/C

    0.000

    0.002

    0.004

    0.006

    0.008

    0.010

    0.012

    0.014

    0.016

    Murphy Ph.D Thesis UCC 1981

    Fe wire electrode, 1.0 M NaOH Inlaid Fe foil electrode, 0.5 M NaOH

    Doyle, unpublished work, TCD 2011

    RPS Methodology reproducible across space and time.

    R = 0.9935, R2 = 0.9870a = 0.0136 0.0003 Cb = 0.0156 0.0011 cycle-1

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    Hydrous oxide film regarded as a surfacebonded polynuclear species. Metal cations

    in polymeric network held together bysequence of oxy and hydroxy bridges.Mixed conduction (electronic, ionic) behavioursimilar to that exhibited byPolymer Modified Electrodes.Can regard microdispersed hydrous oxide layer asopen porous mesh of interconnected surfaquometal oxy groups.

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    Elow er

    / V (vs Hg/HgO)

    -1.7 -1.6 -1.5 -1.4 -1.3 -1.2 -1.1 -1.0 -0.9

    Q

    /mC

    0

    10

    20

    30

    40

    50

    60

    70

    80

    Upper Limit E = 0.324 V

    Effect of lower potential limit ELL of growth sweep on development of hydrousoxide charge capacity.

    Q (proportional to oxidelayer thickness) identified asanodic chargecapacity measured between-1.226 and 0.324 V, at33 mV/s after repetitivetriangularsweep at 3.3 V/s for 5 min

    between fixed UPL = 0.324Vand variable LPL as indicated.

    ELL, optimum

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    Eupper

    / V (vs Hg/HgO)

    -1.0 -0.8 -0.6 -0.4 -0.2 0.0 0.2 0.4 0.6 0.8 1.0 1.2

    Q

    /mC

    0

    10

    20

    30

    40

    50

    60

    70

    80

    Lower limit E = - 1.426 V

    Effect of upper limit EUL of growth sweep on development of hydrousoxide charge capacity.

    Q (proportional to oxidelayer thickness) identified asanodic chargecapacity measured between-1.226 and 0.324 V, at33 mV/s after repetitivetriangularsweep at 3.3 V/s for 5 min

    between fixed LPL = -1.426Vand variable UPL as indicated.

    EUL, optimum

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    Hydration process promoted by increasingadsorption of OH- ions as pH increases.Hence adsorbed OH- species repel each otherand attract hydrated positive counter ions intooxide matrix hence encouraging hydroxylation

    processes.

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    [Fe2(OH)6(OH2)3]2-

    2Fe(OH)2 + 3H2O

    2Fe(OH)2 2FeO + 2H2O

    Increased instability of hydrouslayer and more effectivepassivation as solutiontemperature increases.

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    A4

    A3

    C2

    EP

    A2

    C1

    A1: not determined. Peak ill-defined in pH rangeStudied.A2: Regular Nernstian shift. -0.06 V/dec (wrt SCE)-2.303RT/F V/dec; zero shift wrt RHE.A3: Super-Nernstian shift. 0.087 V/dec (wrt SCE) or-0.028 V/dec (wrt RHE), i.e. - 3/2(2.303RT/F) V/decC

    2

    : Super-Nernstian shift. -0.092 V/dec (wrt SCE) or 0.033V/dec (wrt RHE), i.e. -3/2 (2.303RT/F) V/dec.A4: Regular Nernstian shift. . -0.06 V/dec (wrt SCE)-2.303RT/F V/dec; zero shift wrt RHE.C1: + 0.044 V/dec (wrt RHE) or + 0.044 0.059 = -0.015 V/decwrt SCE.EP passivation peak shows regular Nernstian behaviour.

    A1

    Voltammetric response as function of solution pH

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    [Fe2(OH)6(OH2)3]2- + 3OH-

    [Fe2O3(OH)3(OH2)3]3- + 3H2O + 2e-

    [M2O3 (OH)3 (OH2)3]n 3- + 3nOH- [MO2(OH)2(OH2)2]2n2- + 3nH2O + 2ne-

    M(IV)

    M(III)

    Fe(II)

    Fe(III)

    Redox switching involves topotactic chargestorage reactions in open hydrous oxide layer whichBehaves as ion exchange membrane.Hydrated counter/co-ions (M+, H+, OH- assumedpresent in pores and channels of film to balance

    negative charge on polymer chain.Equivalent circuit model: dual/multi- railTransmission Line as done for ECP films..

    Super-Nernstian Redox Potentialvs pH shift related to hydrolysiseffects in hydrous layer yieldinganionic oxide structures.

    L.D. Burke, M.E.G. Lyons, E.J.M.OSullivan,D.P. Whelan J. Electroanal. Chem.,122 (1981) 403.

    M = Ir, Rh

    dE/dpH = -3r/2

    r= 2.303RT/Fr= -88.5 mV/decT = 298K

    Rhodium oxide

    Iron oxide

    Redox switching chemistry: hydrous oxideLayer, Mixed conduction mechanism:ion/electron transfer.

    Fe(III) Oxidized form yellow-green

    Fe(II) Reduced form transparent

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    A

    B A

    B A

    B A

    B

    Elec

    trode

    ne-

    Polymer layer Solution

    Charge ejection/injection:

    potential gradient drivenCharge ejection/injection:

    potential gradient driven

    Charge propagation:

    concentration gradient drivenCharge propagation:

    concentration gradient driven

    DE ckD 2exE

    Mixed conductivity:Electron hopping coupledwith counter ion transport.

    Microdispersed hydrousOxide has many physicalcharacteristics similar tothose of electroactivepolymer material.

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    22

    Migration/diffusion model for electron hopping.

    xc

    ab

    x

    b

    xD

    t

    bE

    x

    f

    t

    b

    t

    a E

    xc

    ab

    x

    bDf EE

    D-term M- term

    Eqn. Of continuity Steady state D/M flux

    A

    B A

    B A

    B A

    B

    E

    lectrode

    ne-

    Polymer layer Solution

    Charge ejection/injection:

    potential gradient drivenCharge ejection/injection:

    potential gradient driven

    Charge propagation:

    concentration gradient drivenCharge propagation:concentration gradient driven

    DE

    xxx fkexpkk xx 1f

    2

    2

    2

    2

    Exc

    ba

    xx

    b

    c

    ba

    x

    bD

    t

    b

    RT

    FE

    Potential gradient

    between sites

    Nernst-Planck

    equation.

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    macroscopic charge propagation through polymer

    can be represented in terms of a diffusion-migration process rate of electron hopping quantified via electron exchangerate constant kex or electron hopping diffusion coefficient DE

    local potential gradients between redox sites producea migration term in description of electron hopping flux

    DE predicted to vary linearly with redox site concentration

    electron hopping can be further described using theMarcus theory of ET

    mechanism of electron hopping dependent on degree of localmobility of redox groups ; physical diffusion of redox groups alsomay be important

    electron hopping diffusion coefficients can be evaluated usingtransient or steady state electrochemical techniques

    Features of Redox Conduction.

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    Scan Rate / V s-1

    0.0 0.1 0.2 0.3 0.4 0.5

    Charge/C

    0.000

    0.005

    0.010

    0.015

    0.020

    1 cycle

    30 cycles

    120 cycles

    Variation of integrated voltammetric charge withSweep rate. Multicycled hydrous oxide coated Feelectrodes, 0.5 M NaOH

    More deeply buried Fesites accessed by ECdriving force at longer

    Timescales.

    Finite rate of electron

    self exchange kinetics.

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    Thin films, 30 cycles Thick films 240 cycles

    Laviron Analysis

    DCT,ox = 1.88 x10-10 cm2s-1

    DCT,red =3.77 x10-10 cm2s-1

    c = r/M ; n = 2Fe(II):[Fe2(OH)6(OH2)3]

    2-

    M = 267 g mol-1

    r (Fe(OH)2=3.4 gcm-3

    Fe(III):[Fe2O3(OH)3(OH2)3]

    3-

    M = 265 g mol-1

    r(Fe2O3.nH2O) 3 gcm-3

    Macroscopic average value.Rate controlling transportprocess during redox switchingprobably ion diffusion.Need EQCM analysis forfurther confirmation.

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    26

    Z

    Y

    X

    Polymerstrand

    Polymer strand/pore solution

    interface

    PoreelectrolyteSupport

    electrode

    Bulk electrolytesolution

    Z

    Y

    X

    Polymerstrand

    Polymer strand/pore solution

    interface

    PoreelectrolyteSupport

    electrode

    Bulk electrolytesolution

    General dual rail transmission linemodel is used to reflect the coupledprocesses of electronic and ionic

    transport within a conductingPolymer/metal oxide thin film.

    Dual Rail Transmission Line Modelfor Redox Switching in ECP/metal oxide films.

    Two main approaches to TL analysis: Assume ECP film is highly porous matrix.

    Use porous electrode models(de Levie, Bisquert, Paasch) to analyseelectrochemical response.

    Polymer film assumed homogeneous

    (Vorotyntsev, Buck, Albery).Model diffusive (ambipolar) transport ofPolarons and counterions in terms ofcharacteristic resistances andNernst-Planck equations. Porosityaccounted for by associated distributedcapacitance.

    Circuit Details.

    .

    Bisquert et al. J. Electroanal. Chem.

    508 (2001) 59-69

    The TL circuit consists of distributedimpedances corresponding to chargetransport along the polymerstrand (Z), ion transport withinthe pore electrolyte (X) and animpedance representing the interfacebetween the strand and the pore (Y).At the simplest level Z correspondsto the electronic resistance RE,

    X to the ionic resistance RI, andY to a distributed capacitance CS .

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    Doyle, 2011, unpublished work

    Hydrous Fe oxideLayer,30 cycles

    Un-cycled Fe electrode

    (vs Hg/HgO)

    Layer growth parameters: Upper, lower potentialsweep limits.

    Solution temperature Solution pH Potential sweep rate. Base concentration.

    Hydrous Oxide Growth via potential multicyclingprocedure in aqueous alkaline solution.

    Lyons, Burke, J. Electroanal. Chem., 170 (1984) 377-381

    Lyons, Burke, J. Electroanal. Chem., 198 (1986) 347-368

    Lyons, Brandon Phys. Chem. Chem. Phys., 11 (2009) 2203-2217

    Tafel slope= 50 mV/dec

    Tafel Slope= 40 mV/dec

    Tafel slope uncycled electrode = 50 mV/decTafel slope for HO coated electrode ca. 40-45 mV/decindependent of HO thickness.

    Note: experiments performed in 0.5 MNaOH on aged Fe electrodes.

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    Potential / V vs. Hg/HgO

    0.6 0.7 0.8 0.9 1.0 1.1

    Log(Current/A)

    -5.5

    -5.0

    -4.5

    -4.0

    -3.5

    -3.0

    -2.5

    -2.0

    -1.5

    bare

    30 cycles

    60 cycles

    120 cycles

    180 cycles240 cycles

    300 cycles

    Effect of potential cycling on Tafel Plot behaviour (iRu corrected)recorded for hydrous oxide coated Fe electrodes in 0.5 M NaOH.

    Potential span of Low Tafel Sloperegion less for multi-cycled oxidecoated electrodes than foruncycled electrode.Tafel slope at low potentialindependent of hydrous oxidethickness once multicycling protocolhas begun (unlike rhodium oxide).Tafel slope (iR corrected) forHydrous oxide coated Fe electrode

    less than that recorded foruncoated electrode.

    Q /C

    0.004 0.006 0.008 0.010 0.012 0.014 0.016 0.018 0.020 0.022

    b/mVdec

    -1

    38

    40

    42

    44

    46

    48

    50

    Tafel Slopes vary from ca. 50 mV/decfor un-cycled Fe electrode to ca. 40 mV/decfor Fe electrodes coated with thickHydrous oxide layers (0.1 M NaOH).

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    Hydrous Oxide: OER Kinetic parametersLow overpotentialsb = 60 mV dec-1 = 2.303(RT/F)mOH- = 3/2High overpotentials

    b = 120 mV dec-1 = 2.303(2RT/F)mOH- = 1.0

    Dual Tafel Slope behaviour not due tochange in RDS but arises due to potentialdependence of total fractional coverage Sof electrosorbed reaction intermediates.

    P d E 1 30V f 15 f ll d b 1 l b 1 1 5

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    Aged passive oxideCoated Fe electrode

    Aged electrode, severe cathodicpre-treatment: OER Kinetic parameters

    Low overpotentialsb = 60 mV dec-1 = 2.303(RT/F)mOH- = 3/2High overpotentialsb = 120 mV dec-1 = 2.303(2RT/F)mOH- = 1.0

    Pre-reduction at E = - 1.30V for t = 15 min, followed by 1 cycle between 1.175And 0.625 V in 1.0 M NaOH at 40 mV/s.

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    S + OH- SOH + e- (AI)SOH + OH- SO - + H2O (AII)SO - + OH- SO2H- + e- (AIII)SO2H- + OH- S + H2O + O2 + 2e- (AIV)

    S = electrocatalytically active ironsurfaquo group = stabilized Fe(VI) moeity

    QSSA, Langmuir Adsorption conditions:

    OHOHS

    akRTFk

    RTFaakFk

    i2

    01

    2

    2

    0

    1

    )1(exp

    exp4

    RTFkkaaFki OHS exp4 010122

    Step (AII) RDSLow overpotential

    RTFaaFki OHS exp40

    1

    Step (AI)RDSHigh overpotential

    Simple Kinetic analysis (Lyons 1984) predictsCorrect Tafel slopes over entire range, but predicts a reaction order mOH-

    of 2 at low (instead of 3/2) and 1 at high .

    OER Kinetic Analysis:Model ALyons 1984

    Dual Tafel Slope behaviour attributedto change in RDS as potential increases.

    OH OH (BI)

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    S + OH- S-OH + e- (BI)S-OH + OH- S-H2O2 + e- (BII)S-H2O2 + OH- S-OH2- + H2O (BIII)S-H2O2 + S-HO2- O2 + H2O + OH- (BIV)

    S-H2O2 = physisorbed hydrogen peroxide

    Assume intermediate surface coverage of S-OH species.Pseudo equilibrium condition & Temkin adsorption isotherm(interaction parameter gj) assumed.

    OER Kinetic Analysis:Model BLyons & Brandon 2009

    Assume at low step (BII) is rate limiting.

    SS

    S RT

    F

    RT

    gg

    akf

    OSHSOH

    SOHOH

    exp

    1

    exp220

    2

    2/1110

    8.00

    S

    SS

    RT

    F

    RT

    gakf SOHSOHOH

    exp

    1exp02

    22OSHSOHgg

    Assume step (BI) is in pseudo-equilibrium.

    FKaRTg

    RT

    FKa

    RT

    Fa

    k

    k

    RT

    g

    RT

    g

    RT

    F

    RT

    gkf

    RT

    F

    RT

    gakf

    ff

    OHSOH

    OHOHSOHSOH

    SOH

    SOH

    SOHSOH

    SOHSOHOH

    S

    SS

    S

    S

    ln

    expexpexpexp1

    1exp

    1exp

    expexp1

    0

    1

    0

    1

    0

    11

    0

    11

    11

    SRT

    FaKkff OHSOH

    1exp21022

    2/32ln

    ln

    303.21

    303.2log

    2/1

    2/1

    S

    S

    OH

    OH

    a

    a

    fm

    FRT

    FRT

    fb

    OH

    At high surface coverage conditions

    change to where SOH = S

    1. Step (BII)still rate determining.Langmuir adsorption pertains. Also gSOH 0.

    SRT

    Fakff OH

    exp022

    0.1

    2303.2

    OHm

    F

    RTb

    OER Ki ti A d (EC l i ti t ) d d F

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    Overpotential / V0.2 0.3 0.4 0.5 0.6 0.7

    LogCurrentDensityi/Acm

    -2

    -6

    -5

    -4

    -3

    -2

    -1

    0

    FreshAged

    b = 39.5 mVdec-1

    b = 44 mVdec-1

    OER Kinetics: Aged (EC polarization measurements) pre-reduced Feelectrodes (not multicycled).

    Overpotential / V (Hg/HgO, 1 M)0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7

    LogCurrentDensityi/Acm

    -2

    -8

    -7

    -6

    -5

    -4

    -3

    -2

    -1

    0

    1st forward

    reverse2nd forward

    Slope of 40 mVdec-1

    Potential E / V (Hg/HgO, 1 M)

    -1.4 -1.2 -1.0 -0.8 -0.6 -0.4 -0.2 0.0 0.2 0.4 0.6 0.8

    CurrentDensityi/Acm-2

    -0.002

    -0.001

    0.000

    0.001

    LESS AGEDMORE AGED

    Peak A4 becomes more enhanced on aging.Compact anhydrous oxide chemistryDominates interfacial EC behaviour.Is associated with increase in low overpotentialTafel slope from ca. 40 mV to ca. 45-47 mV.

    Pre-treatment: cathodic polarization at E = - 1.10VIn 1.0 M NaOH, t = 5 min, followed by singleCycle at 40 mV/s between limits 1.175 to 0.625 V.

    OER Ki ti A d d d F

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    Cyclic voltammograms (1.0 M NaOH, scan rate = 40mV s-1) characterising an Fe electrode prior to its 1st,5th and 16th utilisation in OER polarisationexperiments.

    OER steady state polarisation curves for a pre-reducedFe electrode in various NaOH solutions. The tracedenoted as fresher 1.0 M was recorded for the sameelectrode in an earlier experiment, before satisfactoryreproducibility with respect to Tafel slope had becomeestablished.Inset Reaction order plots constructed from thereproducible polarisation data at a potential of E= 0.7V.

    [Fe(VI)Om(OH)n]p- + OH-

    [Fe(VI)Om+1(OH)n-1]p- + H2O + e

    -

    [Fe(VI)Om+1(OH)n-1]p- + OH-

    [Fe(VI)Om OOH(OH)n-1]p- + e- RDS

    [Fe(VI)Om OOH(OH)n-1]p- + OH-

    [Fe(VI)Om OO(OH)n-1]p- + H2O + e-[Fe(VI)Om OO(OH)n-1]

    p-+ OH-

    [Fe(VI)Om(OH)n]p- + O2 + e

    -

    p = 2m+n-6

    Effect of oxide on OER Kinetics at oxidized aged Fe explainedin terms of Conway-Meyer dual barrier model.

    b 2.3034RT/5FmOH 1

    Physisorbed peroxide intermediate model assumed.

    OER Kinetics: Aged pre-reduced Feelectrodes (not multicycled).

    Low overpotential

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    Conway-Meyer Dual Barrier Model

    VM

    VF

    VS

    Barrier Oxide Film

    Compact EDL

    Solution

    F

    S

    si

    FS

    Feffi

    SF

    SF

    a

    eff

    i

    m

    is

    mm

    F

    RT

    F

    RT

    ib

    RT

    Fakf

    S

    SF

    F

    is

    ,,

    )(303.2303.2

    log

    exp)(

    S

    SS

    J.J. MacDonald, B.E. Conway,Proc. Roy. Soc., Ser.A, 269 (1962) 419-440.

    R.E. Meyer, J. Electrochem. Soc.,107 (1960) 847-853.

    Reaction order in absence of barrier

    Effective reaction order

    Effective symmetryFactor S = (F/(F+S))S

    Potential dependent field assisted chargeTransfer across a barrier oxide film(process F) in series with interfacialcharge transfer reaction (process S).Effective Symmetry factor (and henceTafel slope) and reaction order issome fraction F() =F/(F + S)of the true values.

    SiSF

    FSieffi

    Seff

    S

    SF

    FS

    mmFm

    bFb

    F

    ,,,

    1

    S

    S OH S OH (BI)

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    S + OH- S-OH + e- (BI)S-OH + OH- S-H2O2 + e- (BII)S-H2O2 + OH- S-OH2- + H2O (BIII)S-H2O2 + S-HO2- O2 + H2O + OH- (BIV)

    Assume step (BII) is rate determining (low values), and thatdual barrier model pertains.Analysis of barrier free situation suggests that bS = 40 mV/dec(2.303(3RT/2F) and mOH = 2.

    SS

    RT

    FKaf SF

    F

    OH

    1exp

    2

    12

    )(

    /047.05

    4

    303.21

    303.21303.2log

    2/1

    ,

    2/1

    S

    SF

    SF

    OH

    SF

    FOH

    SF

    FeffOH

    SF

    SFa

    eff

    mm

    decVF

    RT

    F

    RT

    F

    RT

    ib

    21

    /235.04

    303.2303.2303.2

    exp

    2/1,1

    ,

    2/1

    S

    SS

    SFOH

    SF

    SF

    F

    m

    OH

    SF

    F

    effOH

    S

    F

    SF

    SF

    SFeff

    OH

    mm

    decVF

    RTb

    F

    RT

    F

    RTb

    RT

    FKaf

    Low overpotentials

    Assume step (BI) is rate determining (high values), and that dual barrier model pertains.Analysis of barrier free situation suggests bS = 0.120V /dec (2.303(2RT/F) and mOH = 1.0.

    Aged pre-reduced FeelectrodesOER Kinetic analysisIncorporating DBM.

    High overpotentials

    Not easy to check this prediction at high .

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    Bockris, Otagawa, J. Phys. Chem.,87 (1983 )2960

    Bockris, Otagawa, J. Electrochem. Soc., 131 (1984) 290.

    Hydrous OxideLayer

    Compact OxideLayer

    Lyons BrandonPhysisorbed peroxideOER model incorporatingDual Barrier concept.

    Interlinked surfaquogroups

    OER Kinetics: Oxidized metal electrodes: Passive oxide films

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    Electrode Experiment, b, mOH- Dual

    barrier

    b, mOH

    for

    analysis

    Isotherm

    L or T

    Path-

    wayNi no-pre-treat 2RT/3F order not

    measurableNo As listed left L, 0 C

    Ni pre-reduced 2RT/3F, 1 No As listed left L, 0 C

    Ni pre-oxidised 2RT/3F, 1 No As listed left L, 0 C

    Co no-pre-treat 2RT/3F(5M)4RT/5F(1M) low [OH-

    ] ----- ----- -----Co pre-reduced 4RT/5F, 1 Yes 2RT/3F, 2 L, 0 E

    Co aged low RT/F, 3/2 No As listed left T, rI

    >> rII

    E

    Co aged high 2RT/F, 1 No As listed left L, 1 E

    Fe no-pre-treat 2RT/3F(1M)4RT/5F(5M) high [OH-] ----- ----- -----

    Fe pre-reduced(fresh)

    2RT/3F order notmeasurable

    No ----- ----- -----

    Fe pre-reduced(aged)

    4RT/5F, 1 Yes 2RT/3F, 2 L, 0 E

    Fe aged low RT/F, 3/2 No As listed left T, rI

    >> rII

    E

    Fe aged high 2RT/F, 1 No As listed left L,

    1 E

    OER Kinetics: Oxidized metal electrodes: Passive oxide films

    M. Brandon, Ph.D Thesis University of Dublin, 2008

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    Hydrous microdispersed oxides readily prepared via repetitive cyclic potential sweep method

    of parent metal (Fe, Co, Ni, Mn, Rh, Ir, Au, Pt, Pd) in aqueous alkaline solution. Method similarto electropolymerization of ECP films.

    Charge storage/charge percolation properties of hydrous oxide depend on electrochemicaland environmental variables such as: lower and upper potential sweep limits, potential sweeprate, base concentration, solution temperature, solution pH.

    Acid base behaviour of anodically formed transition metal oxides important when consideringmechanism of both redox switching & oxygen evolution

    Hydrous oxide material is catalytically active wrt OER.

    Hydrous oxides more difficult to reduce than less hydrated compact materials. General mechanistic ideas : hydrous oxide akin to electroactive polymer . Hydrous oxide is

    mixed ionic and electronic conductor. Hydrous oxide consists of an open structure derivedfrom extended linkages of active surfaquo groups which are involved in anodic OER process.

    Full understanding of OER mechanism on passive oxide coated Fe and hydrous oxide coated Feelectrodes in aqueous alkaline solution now obtained via SS Tafel Plot, open circuit potentialdecay, complex impedance spectroscopy and reaction order measurements.

    Main ideas developed in:

    M.E.G. Lyons, M.P. Brandon, Phys. Chem. Chem. Phys., 11 (2009) 2203-2217.

    M.E.G. Lyons, M.P. Brandon, J. Electroanal. Chem., 631 (2009) 62.

    M.E.G. Lyons, M.P. Brandon, J. Electroanal. Chem., 641 (2010) 119.

    M.E.G. Lyons, M.P. Brandon, Int. J. Electrochem. Sci., 3 (2008) 1463-1503.

    M.E.G. Lyons, L.D. Burke, J. Electroanal. Chem., 198 (1986) 347-368.

    M.E.G. Lyons, L.D. Burke, J. Electroanal. Chem., 170 (1984) 377-381

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    Dr Richard Doyle, TCD

    Dr Michael Brandon, TCDProf. Declan Burke UCC

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    Acknowledgements: Funding Science Foundation Ireland (SFI) Principal

    Investigator Programme Grant Number SFI/10/IN.1/I2969.

    DuPont (Geneva)

    Enterprise Ireland

    IRCSET

    Trinity College Dublin

    EU ALFA Programme.MEDIS

    EU/LAALFA

    http://www.tcd.ie/