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    Summary

    The Basic Electrochem istry

    Lecture1

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    Summary: Faradic process

    The current flow to and from electrodes is the results of

    Faradaic and Non-Faradaic processes. These processes

    can occur alone or simultaneously.

    A Faradaic process involves the transfer of electrons

    across the electrode-electrolyte interface.

    A Non-Faradaic process involves charging of the interface

    (double layer), much like that of capacitor, without the

    transfer of electrons.

    Basic Electrochemistry: Lecture 1 Summary Vojtech Svoboda, January 2010

    CPE690: Power Sources for Portable, Automotive, and Renewable Energy Systems

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    Summary: Faradic process

    Charge Transfer Electrodes: electrodes at which Faradaic

    process occur. Electrons are either gained or given up

    depending on their energy.

    By driving the potential of the electrode more negative, the energy of

    the electrons in the electrode increases thereby given the electrons

    sufficient energy to occupy vacant states on the species in the

    electrolyte.

    By driving the potential more positive, the electrons in the electrode

    loose energy, thereby making it possible for electrons from species in

    the electrolyte to lower their energy by transferring to the electrode.

    Basic Electrochemistry: Lecture 1 Summary Vojtech Svoboda, January 2010

    CPE690: Power Sources for Portable, Automotive, and Renewable Energy Systems

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    Summary: Faradays Law of Electrolysis

    Faradays Law of Electrolysis: The extent of the electroc hemical

    react ion is p roport ional to the charge passed to the electrode.

    This can be demonstrated by the dissolution of metal: M Mn+ + ne-

    The charge Q(in coulombs) passed to the electrode is represented as:I= current (amps) to the electrode

    t= duration (seconds) of the current

    Moles of electrons passed are obtained by dividing Qby

    Faraday constant: F= 96487 C/mol e

    Mols of metal dissolved are obtained by dividing the mols of electron by n:

    (mol) Then mass: (g) AW = atomic weight (g)

    t

    IdtQ0

    Fn

    tIM

    *

    * AW

    Fn

    tIM *

    *

    *

    Basic Electrochemistry: Lecture 1 Summary Vojtech Svoboda, January 2010

    CPE690: Power Sources for Portable, Automotive, and Renewable Energy Systems

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    Summary: Faradays Law of Electrolysis

    Electrolysis is a Faradaic process where electrons are

    transferred across the electrode-electrolyte interface

    resulting in transformation of chemical spices.

    Water electrolysis is electrochemical water splitting, where

    Reduction reaction proceeds on Cathode, in which

    electrons are consumed: 4H+ + 4e 2H2

    Oxidation reaction proceeds on Anode, in which electronsare given: 2H2O O2 + 4H

    + + 4e

    Overall reaction: 2H2O O2 + 2H

    Basic Electrochemistry: Lecture 1 Summary Vojtech Svoboda, January 2010

    CPE690: Power Sources for Portable, Automotive, and Renewable Energy Systems

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    Summary: Galvanic & Electrolytic Cell

    Galvanic cell: Reactions occur spontaneously, chemical

    energy can be converted into electrical energy.

    Examples: Discharging batteries.

    Electrolytic cell: Reactions driven by external power

    source. A sufficient potential is applied across the two

    electrodes to induce the electrochemical reactions.

    Cathode potential is more negative than anode potential.

    Examples: Charging batteries, electrolysis, electroplating.

    Basic Electrochemistry: Lecture 1 Summary Vojtech Svoboda, January 2010

    CPE690: Power Sources for Portable, Automotive, and Renewable Energy Systems

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    Summary: Non-Faradaic process & Double Layer

    In some cases, it might be thermodynamically or kinetically

    unfavorable for Faradaic charge transfer processes to

    occur even if electrode is polarized through a range of

    potentials. Current, however may still flow to the electrode.

    Non-Faradaic Current - Double Layer Charging

    The current originates from charging of the electrode,

    which is analogous to charging of a capacitor. During

    charging, species in the electrolyte may absorb or desorbfrom the interface, and therefore, the structure of the

    interface may change.

    Basic Electrochemistry: Lecture 1 Summary Vojtech Svoboda, January 2010

    CPE690: Power Sources for Portable, Automotive, and Renewable Energy Systems

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    Summary: Double Layer

    Interphase region: The transitional region going from the

    electrode phase to the electrolyte phase. The interphase

    region is also called the electric double layerdue to the

    two layers of excess charge.

    Double layerrepresents a capacitor is describes by

    capacitance Cdranging from 10 to 40 mF/cm2. However,

    since the capacitance is a function of potential, the doublelayer does not behave as an ideal capacitor.

    Basic Electrochemistry: Lecture 1 Summary Vojtech Svoboda, January 2010

    CPE690: Power Sources for Portable, Automotive, and Renewable Energy Systems

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    Summary: Double LayerDouble layer models:

    Helmholtz model

    Helmholtz proposed there is one layer of excesscharge in the electrode and another layer of excess

    charge in the electrolyte separated by a fixed

    distance to give a linear potential profile.

    Goy-Chapman model

    Stern model: Stern proposed a hybrid ofHelmholtz and Goy-Chapman models.

    Hamann, C. et al.: Electrochemistry,

    Wiley-VCH Verlag, 2007, page 117

    Basic Electrochemistry: Lecture 1 Summary Vojtech Svoboda, January 2010

    CPE690: Power Sources for Portable, Automotive, and Renewable Energy Systems