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PEC Presentation Sample

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    Photo Electrochemical Water

    Splitting for Hydrogen Production

    -

    Basics

    Presented by ANAMIKA BANERJEE

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    It is estimated that the global energy consumption will increase from

    13.5 TW (in 2001) to 27- 41 TW (by 2050).

    MAJOR SOURCES OF ENERGY

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    HYDROGEN 

    1. Combustion

    generates only

    steam & water.

    2.Heat of

    combustion is

    34.18 kcal/g.

    3.High energy

    storage capacity

    i.e. 119 kJ/g.

    4.Easily

    assimilated

    into the

    biosphere.

    5. It is non toxic.

    6. Can be used in

    the chemical

    industry, for the

    production of

    chemicals &

    conventional

    petrochemicals.

    7.Suitable fuel

    for use in fuel

    cells.

    8.Transmission

    of energy in the

    form of

    Hydrogen

    is economical.

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    PHOTOELECTROCHEMICAL

    CELLS

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    PEC technology is based on solar energy, which is a

    perpetual source of energy and water, which is a

    renewable source.

    PEC technology is environmentally safe, with no

    undesirable byproducts.

    PEC technology may be used on both large and small

    scales.

    PEC technology is relatively uncomplicated.

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    PHOTO- ELECTROCHEMISTRY OF WATER

    DECOMPOSITION

    The principle of photoelectrochemical water decomposition is based

    on the conversion of light energy into electricity within a cell

    involving two electrodes(or three), immersed in an aqueous

    electrolyte, of which at least one is made of a semiconductor

    exposed to light & able to absorb light. This electricity is then used

    for water electrolysis.

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    The performance of PECs is considered in terms of:

    Excitation of electron

    hole pairs in

    photo

    electrodes.

    Charge separation in photo electrodes.

    Electrode processes & related

    charge transfer within PECs

    Generation of PEC voltage

    required for water decomposition

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    SCHEMATIC REPRESENTATION OF 3 ELECTRODE

    SYSTEM

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    SEMICONDUCTOR

    PROPERTIES

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    ENERGY BAND IN SEMICONDUCTOR

    Consist of a large number of closely spaced energy levels.

    Bands are made up large number of atomic orbitals and the

    difference in energy between adjacent orbitals within a given

    energy band is so small so that band can be considered a

    continuum of energy levels

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    VALENCE BAND CONDUCTION BAND

    Energy band: highest occupied energy level is called the

    valence band and the lowest unoccupied energy level is

    called the conduction band.

    Conduction Band

    Valence Band

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    •The band gap, Eg

    , is the smallest energy difference between

    the top of the valence band and the bottom of the conduction

    band

    •The required band gap of the semiconductor for water splitting

    should be 1.8 – 2.2 eV.

    •Large band gap semiconducting oxides are stable in aqueous

    electrolyte but absorb in UV region which is only about 4 of

    the solar spectrum, whereas small band gap semiconductor &

    optimum band gap semiconductor have the potential to absorb

    visible part of solar spectra but corrode when dipped in

    electrolyte.

    E

    g

    Valence Band

    Conduction Band

    BAND GAP (Eg

    )

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    BAND EDGES

    A semiconductor capable of spontaneous water splitting must have

    conduction band energy (E

    C

    ) higher and valence band energy (E

    V

    ) lower

    than that of reduction potential E

    red

    (H

    2

    /H

    +

    ) & oxidation potential E

    ox

    (OH

    -

    /O

    2

    ) of water respectively.

    0.0

    1.23

    H

    +

    /H

    2

    O

    2

    / H

    2

    O

    E

    C

    E

    V

    h

    +

    e

    -

    E

    g

    ≥ eV

    V vs NHE

    Ideal straddling condition of Conduction & valence band edges of a

    semiconductor

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    Energy level Diagram

    (pH 1)

    Band positions of several semiconductor materials in contact

    with aqueous electrolyte at pH 1

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    .

     It is imp. because when a reference electrode is used to make

    measurements, it compares E

    f

    of semiconductor with its own

    unchanging Fermi level.

    E

    C

    E

    F

    E

    V

    Intrinsic

    FERMI ENERGY (E

    F

    )

    In an extrinsic semiconductor:

    E

    C

    E

    F

    E

    V

    n – type

    E

    C

    E

    F

    E

    V

    p – type

    In an intrinsic semiconductor:

    It is the energy level where probability of occurrence of an electron is half.

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    +

    +

    +

    +

    +

    +

    +

    +

    -

    -

    -

    -

    -

    -

    -

    -

    E

    REDOX

    E

    REDOX

    E

    F

    E

    F

    n

    type p

    type

    BAND BENDING :-

    E

    F

    > E

    redox

    - e

    -

    will be transferred from

    electrode into the solution and the there

    is a positive charge associated with the

    space charge region.

    E

    F

    < E

    redox

      e

    -

    must transfer from the

    solution to the electrode to attain

    equilibrium and generates a negative

    charge in the space charge region .

    It is the difference between the potential at the surface and potential in thebulk of the semiconductor.

    The electric field that is formed in space charge region results in bending of

    bands.

    Band bending acts as a barrier for the recombination of charge carriers.

    Band bending becomes zero only at flat band potential(Vfb

    )

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     Also called asdepletion region.

     An insulating region within a

    conductive, doped semiconductor

    material where the charge carriers are

    diffused or forced away by an electric

    field.

     It is called so because it is formed

    from a conducting region by removal

    of all charge carriers leaving none to

    carry a current.

    E

    F

    E

    F

    E

    C

    E

    C

    E

    V

    E

    V

    Space charge

    (depletion)

    Space charge

    (depletion)

    n – type

    p – type

    SPACE CHARGE REGION :-

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    The flat band potential corresponds to the externally applied potential

    for which there is no band bending at the semiconductor surface.

    This potential is equal to the curvature of the bands in the absence of

    any potential applied to the interface.

    Photo-cells equipped with a photo-anode made of materials with

    negative flat-band potentials (relative to the redox potential of the

    H

    +

    /H

    2

    couple, which depends on the pH) can split the water molecule

    without the imposition of a bias.

    If V

    fb

    is positive, then more electrons are attracted towards space

    charge region, hence this region decreases and it leads to increase in

    the recombination of charge carriers.

    If Vfb

    is negative, then space charge region becomes broadened as a

    result there is decrease in recombination of charge carriers.

    FLAT BAND POTENTIAL :-

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    STRATEGIES FOR THE IMPROVEMENT OF

    SEMICONDUCTOR

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    DOPING:

    •Extends absorption in

    visible region.

    • Increases the lifetime

    of photo generated

    carriers.

    •Improves electrical

    conduction

    DYE SENSITIZATION

    •Use of

    sensitizer/catalyst/dyes

    • Improvement in

    absorption of solar

    energy

    •Enhanced photo -

    response with dyes

    ION IMPLANTATION

    • Modify electronic

    structures of

    semiconductor to

    improve visible light

    response.

    •Referred as ‘second

    generation photo

    catalyst’

    .

    SWIFT HEAVY ION

    IRRADIATION

    •For modification in

    surface properties of

    material through

    electronic excitations

    resulting in alteration

    in the photo response of

    the material in PEC cell.

    BILAYERED SYSTEMS

    • Broad absorption

    •  Good charge transportation

    •  Reduced recombination rate

    •   Inbuilt electric field at the

    heterojunction

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    CHARACTERIZATION METHODS

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    X- Ray Diffractometer

    • For measurement of Phase & Particle size

    • Scherrer’s Equation (for crystallite size): 0.9λ /β cosθ

    UV Vis Spectrophotometer

    •   For the measurement of band gap.

    •   For direct- indirect, allowed or forbidden transition.

    Atomic Force Microscope (AFM )

    • To determine surface morphology of hetero- junction

    thin film.

    Potentiostat – For PEC study.

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    SEM

    (Scanning Electron M icroscope)

    Scans the surface of the sample by releasing electrons and making

    the electrons bounce or scatter upon impact. The machine collects the

    scattered electrons and produces an image.

    Information on the

    sample’s surface and its

    composition

    Shows the sample bit by

    bit as area where the

    sample is placed can be

    rotated in different

    angles.

    3D image Resolution-0.4nm

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    PHOTOCURRENT VOLTAGE CHARACTERISTICS

    •  They are the useful tool in determining the operating characteristics

    of a device by showing its possible combinations of current &

    voltage. As a graphical aid visually understand better what is

    happening.

    •  These curves show the relationship between the current flowing

    through an electrical or electronic device & the applied voltage across

    its terminals.

    P

    o

    u

    n

     

    e

    n

    s

    t

    y

    Potential

    V < 0, Cathodic current in forward bias

    region.

    V > 0, Anodic current in reverse bias

    region.

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    PARAMETERS OBTAINED FROM THE I-V PLOT :

    1. Photocurrent Density: Difference of light current- dark current/area of

    semiconductor.

      More photocurrent density, more is hydrogen production.

    2. Open Circuit Voltage (V

    oc

    ): The voltage between the terminals when no

    current is drawn (infinite load resistance)

      In Electron recombination kinetics, high Voc

    - low recombination rate

    and high photocurrent density.

    3. Short circuit current (I

    sc

    ) : The current when the terminals are connected

    to each other (zero load resistance)

      Isc

    increases with light intensity, as higher intensity means more

    photons, which in turn means more electrons

    MOTT

    SCHOTTKY

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    MOTT - SCHOTTKY

    MEASUREMENTS 

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    EFFICIENCY

    MEASUREMENTS

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    They are split into two main categories:

    (i) Benchmark efficiency

    (a) solar-to-hydrogen conversion efficiency (STH)

    (ii) Diagnostic efficiencies (to understand material performance)

    (a) applied bias photon-to-current efficiency (ABPE)

    (b) external quantum efficiency (EQE) = incident photon-to-

    current efficiency (IPCE)

    (c) internal quantum efficiency (IQE) = absorbed photon-to-

    current efficiency (APCE)

    ABPE = J

    ph

    (mA/cm

    2

    ) X [1.23 – V

    b

    (V)]/P (mW/cm

    2)

    APCE = J

    ph

    (mA/cm

    2

    )X[1.23 – V

    b

    (V)]/P mono(mW/cm

    2

    ) X λ (nm)(1-10-A)

    STH = [|j

    sc

    (mA/cm

    2

    )| X(1.23V) X ηF]/P (mw/cm2)

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    IPCE

    IPCE describes the maximum possible efficiency with which

    incoming radiations can produce hydrogen from water.

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