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Chem 4003

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    1

    Introduction

    Definitions:

    Electrochemistry

    Electrochemical Engineering

    Challenges

    Course Content

    Major Applications

    History

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    2

    Electrochemistry

    Electrochemistry is the branch of chemistryconcerned with the interrelation of electrical andchemical effects

    Deals withThe study of chemical changes caused by the

    passage of a current

    The production of electrical energy by chemicalreactions

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    3

    Electrochemical Engineering

    The use of chemical engineering fundamentalprinciples for the study and analysis of

    electrochemical systemsThermodynamics

    Transport phenomena

    kinetics

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    4

    What is an electrochemicalsystem?

    System characterized by:

    Strong interactions among solute and with the

    solvent (ionic species)Passage of a current

    Potential

    Electrical energy transformed into chemicalenergy or vice versa

    e.g., batteries, fuel cells, etc

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    5

    Challenges

    No much cover on other courses

    Chemistry

    ThermodynamicsPhysical chemistry

    Electrochemical systems are different

    Break any myths about electrochemical systems

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    6

    Course Content

    Basic concepts

    Thermodynamics

    Electrode kinetics Transport mechanisms

    Modeling

    Applications

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    7

    Applications

    Production of Al and Cl

    Corrosion

    Batteries and Fuel Cells Electroplating

    Cathodic protection

    Super capacitors

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    8

    Major Products based onelectrochemical technology

    Process or Product (data from

    National Research Council)

    Annual Market

    ($ billion)

    Aluminium

    Sodium Hydroxide

    ChlorineCopper

    Other metals and chemicals

    Electroplating

    Batteries

    Semiconductor Processing

    4

    3

    22

    2

    10

    4

    1

    Total 28

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    9

    History

    Discoveries started around 1800

    Allesandro Volta (first battery)

    Michael Faraday (Faradays law) David Grove (1839) discovered the fuel cell

    Georges Leclanche (1868) constructed the carbon

    zinc battery

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    10

    History

    Hall-Heroult aluminum process (1886) reduced theprice from $100/lb to $2/lb

    Walter Nernst Julius Tafel

    Great advances in electroplating (1920-1940s)

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    11

    History

    The formal synthesis of electrochemistry andengineering began in 1950s

    Norbert Ibl in SwitzerlandCharles Tobias in US

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    12

    Summary

    Electrochemistry

    Electrochemical Engineering

    What is an electrochemical system? Major applications of electrochemistry

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    1.13

    OutlineChapter 1: Basic Concepts

    Redox reactions Electrochemical Cells-definition Standard electrode Standard cell potential Electrochemical cells

    Representation Galvanic cells Electrolytic cells

    Nernst equation Faradays law Current and voltage efficiency Ion conduction Transfer numbers

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    1.14

    Redox reactions: Oxidation

    Oxidation

    Process by which an element losses electrons

    (increases its oxidation number)The electrode at which oxidation takes place is

    called the anode

    e.g.,

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    1.15

    Redox reactions: Reduction

    ReductionProcess by which an element gains

    electrons (decreases its oxidationnumber)

    The electrode at which reduction takes

    place is called the cathodee.g.,

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    1.16

    Exercise # 1

    Classify the following redox reactions, include theelectrodes name

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    1.17

    Electrochemical Cells

    Consists of:At least two electrodes where reactions occur

    Electrolyte, for conduction of ionsExternal conductor, to guarantee continuity of

    the circuit

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    1.18

    Electrochemical Cells

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    1.19

    Key information

    Electrochemical reactions ALWAYS take place onelectrodes NOT in the bulk

    A potential is always measured respect toANOTHER electrode

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    1.20

    Standard Electrode Potentials

    The universal reference electrode is hydrogen (SHE)

    Standard conditions:

    Temperature 25oC

    Unit activity coefficient of H+ ions

    Reaction

    E: Electrode potential

    0: Standard conditions

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    1.21

    SHE

    Consists of a Pt wire immersed in a solution of 1 MH+

    Hydrogen gas is bubble at 1 atm The Pt wire provides a surface area for the reaction

    to take place

    The gas stream keeps the solution saturated at theelectrode site

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    1.22

    SHE

    It is a theoretical electrode

    It cant be manufactured because it is impossible to

    have hydrogen ion activity of 1.00 M However, hydrogen electrodes can be

    manufactured

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    1.23

    Building a H2 Electrode

    Begin with aPyrex testtube

    Step 1: Usingglassblowingtechniques, add ashort glass tube tothe side of thetube

    Step 2: Spotweld (or silversolder) a 1 cm x1 cm square of

    platinum foil as aPlatinum wire

    Step 3: Again,usingglassblowing,seal the

    platinum wireinto the base ofthe test tube

    Making a simple, standard Hydrogen electrode

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    1.24

    Meaning of Potential

    The potential represents the maximum electricalenergy available from a cell

    Its related to the Gibbs free energy of the cell by:

    n: number of electronsF: Faraday's constant (96485 C/eq)

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    1.25

    Questions?

    What should be the sign of the potential E0 for areaction to be spontaneous?

    Answer: POSITIVEPositive potentials mean that the reaction is

    spontaneous

    Negative potentials mean that the reaction is notspontaneous

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    1.26

    Standard Potentials inElectrochemical Cells

    Appendix B of the book summarizes the standardelectrode potentials

    Standard electrode potentials can be used tocalculate the Standard potential of anelectrochemical cell

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    1.27

    Standard cell potential: Calculations

    1. Choose the electrode reactions from the standard

    electrode potentials table2. Reverse the sense of the reactions according to

    your system

    1. Reverse the sign of your standard potential3. Balance the number of electrons multiplying by a

    positive number

    4. Add the electrode reactions to obtain overallreaction

    5. Add the potentials to obtain the overall potentialof the cell

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    1.28

    Standard Cell potential: Calculations

    You can balance the stoichiometry of the equationby multiplying by any positive constant

    This operation does not alter the potential of thecell (potential is an intensive quantity, unaffected

    by the number of electrons)

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    1.29

    Schematic Representation ofElectrochemical Cells

    Include all the phases involved

    Separate the phases using bars

    Include information about solvent andconcentrations if available

    e.g.:

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    1.30

    Exercise #2

    Calculate the standard potential of the cell

    What is the anode?

    What is the cathode?

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    1.31

    Galvanic Cells

    It is an energy producing cell

    Also known as:

    Driving cellSpontaneous cell

    They are used as batteries (several cells in series)

    The standard potential is the maximum potentialthat can be provided by the cell

    The anode is assigned a negative sign (negativeelectrode)

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    1.32

    Galvanic Cells: continued

    The cathode is assigned a positive sign (positiveelectrode)

    Sign of current:Positive if it leaves the electrode to the

    electrolyte

    Negative if it enters the electrode from theelectrolyte

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    1.33

    Exercise #3

    Write the reactions, identify positive and negativeelectrodes, identify cathode and anodes, identify

    direction of the current, and draw the cell includingexternal circuit and flow of electrons, for thefollowing reaction

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    1.34

    Electrolytic Cells

    It is an energy consumer cell

    Also known as:

    Driven cellNon Spontaneous cell

    Opposite process of a battery (required energy to

    operate) The standard potential is the minimum necessarypotential required for the cell to operate

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    1.35

    Electrolytic Cells: continued

    The cathode is assigned a negative sign (negativeelectrode)

    The anode is assigned a positive sign (positiveelectrode)

    Sign of current:

    Positive if it leaves the electrode to theelectrolyte

    Negative if it enters the electrode from theelectrolyte

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    1.36

    Exercise #4

    Write the reactions, overall reaction, calculate thetotal standard potential of the cell, identify positive

    and negative electrodes, identify cathode and anodes,identify direction of the current, and draw the cellincluding external circuit and flow of electrons, forthe following reaction:

    Cu + Zn 2+ Cu 2+ + Zn

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    1.37

    Hint It is recommended that for every problem that you

    solve you start by:

    Writing reactionsCalculating open circuit potential (identifying type

    of cell)Drawing schematic of cell and identifying:

    Positive and negative electrodes Anode and cathode Direction of the current

    Direction of electrons

    This is important to understand your problem and thedata that you are given

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    1.38

    Electrolysis of Brine

    Membrane: bi-layer membrane made of perfluorocarboxylicand perfluorosulfonic acid-based films

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    1.39

    Summary

    Where do electrochemical reactions take place?

    What is oxidation? What is reduction?

    What is the meaning of potential? Define galvanic and electrolytic cell

    Calculate the standard potential of a cell

    Define +,-, cathode, anode, current sign, flow ofelectrons

    Draw schematic of electrochemical cell

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    1.40

    Nernst Equation

    Express relationship between the potential of thecell and the concentration (no standardconcentration)

    si

    : stoichiometric coefficient of species i

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    1.41

    Nernst Equation

    The electrode reaction is written in simplified form as

    si: positive for products and negative for reactants

    Mi: symbol for the chemical species

    zi: charge number of the chemical species

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    1.42

    Steps to use Nernst Eq.

    Write down electrode reactions

    Determine # of electrons transferred (balance

    equations) Use Eq. 1 accordingly

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    1.43

    Exercise #6

    In a Zn/Cu cell, If the reaction is done in a cell in5.00 M Zn+2 and 0.30 M Cu+2 at 25oC, what is the

    cell voltage?

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    1.44

    Faradays Law

    Relationship between charge passed (Q) andamount of substance oxidized or reduced (m) at anelectrode

    The amount of product formed is directlyproportional to the charge passed

    For a specified quantity of charge passed, themasses of products formed are proportional tothe electrochemical equivalent weights of the

    products

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    1.45

    Faradays Law Eq.

    M: atomic or molecular weightI: current, At: time elapsed, sF: Faradays constant, 96,485 C/equiv or 26.8 Ah/equiv (last

    one is very useful in battery applications)

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    1.46

    Faradays Law Eq.

    The product of: (It) is known as total charge passed(Q)

    If current changes with time, it should be integratedover time to obtain Q

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    1.47

    Deviations from Faradays Law

    Some causes of deviation from Faradays law are:Consumption of some of the charge by parasitic

    processesAll of the reactants are not consumedThe postulated process is not the actual processSome of the material from the sample falls of

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    1.48

    Units and Formula Reminder

    Power is the product of current by voltage:

    P = I V

    (units are Win international system)W = AV

    W = J/s

    A = C/s

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    1.49

    Exercise #7

    Solve Ex. 2 of the book (Ch2, p26), parts a, b, andc.

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    1.50

    Current efficiency

    For electrolytic process

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    1.51

    Current efficiency

    For galvanic process, known as faradays efficiency

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    1.52

    Voltage efficiency

    For electrolytic process:

    For galvanic process:

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    1.53

    Energy efficiency

    Product of the current and voltage efficiencies:

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    1.54

    Exercise #8

    Solve problem 4 of the book (Ch2, p. 27)

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    1.55

    Ion Conduction

    ConductivityThe measure of the materials capability to

    transfer electrical energy

    Electrical conductivity (electronic conductivity)is used in metalsIonic conductivity is used in electrolytes (ions

    transfer the current)

    Conductivity of metals much higher than ionicconductivityUnits: S/cm (Siemens)

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    1.56

    Order of Magnitude ofConductivities

    In an aqueous system at room temperature:

    10-2 S/cm

    Much lower than metals, order of magnitude formetals is:

    105 S/cm

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    1.57

    Ionic Conductivity

    This Equations assumes complete dissociation ofspecies

    ui: ionic mobility, cm2

    -mol/J-szi: charge of species, dimensionless

    Ci: concentration of species, mol/cm3

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    1.58

    Charged particlein electrified model

    Assumes:

    Ions are spheres

    Continuous viscous mediumLow Reynolds numbers

    Uses Stokes law to calculate the drag force

    Uniform electric field

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    1.59

    Charged particle model continued

    r : radius of particle, cm

    Ef: forced field, V/cm. For calculations

    assume 1 V/cme : charge of an electron, 1.6x10-19 C/chg

    : viscosity, g/cm-s

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    1.60

    Units Reminder

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    1.61

    Procedure to use chargeparticle model

    Calculate velocity using Eq. 11. AssumeEf =

    1V/cm

    Check value ofRe number

    d: ion diameter, cm: density, g/cm3

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    1.62

    Procedure continued

    Calculate current density

    Since the field is proportional to the negative of thepotential gradient, the conductivity can becalculated

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    1.63

    Equivalent conductance model

    Equivalent conductance (, cm2/ohm-equiv) doesnot change abruptly with concentration

    Correlated with square root of concentration (Fig.2.4)

    Extrapolating to zero gives the equivalentconductance at dilute conditions ()

    Kohlrausch noticed that the difference between having a common ion was approximately constant

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    1.64

    Equivalent conductance model

    Kohlrausch concluded that the equivalentconductance can be considered the sum of twoionic components acting independently:

    Equivalent conductances are given in Appendix C

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    1.65

    Mobility and diffusivity

    Equivalent ion conductance is related to mobility:

    At dilute conditions Nernst-Einstein equationrelates mobility to diffusivity:

    Di: diffusion coefficient of species i, cm2/s

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    1.66

    Calculation of ionic conductivityusing ion conductance

    Get equivalent conductance (Appendix C, CRC,etc)

    Calculate mobility using Eq. 14 Calculate conductivity using Eq.10

    This procedure is not valid at high concentrations(see Fig. 2.6)

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    1.67

    Exercise #9

    Calculate the ionic conductivity of a 0.1 N KClsolution using two different methods. Compareyour values. The crystal radius of K is 1.33

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    1.68

    Effect of Temperature onionic conductivity

    As a general rule ionic conductivity increases withincreasing temperature

    Rule of thumbs:

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    1.69

    Problem

    What would be the conductivity of KCl at 60 oC?

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    1.70

    Transference number

    Represents the fraction of current carried by aspecified ion in the absence of concentrationgradients

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    1.71

    Useful Expression

    Combining Eqs 18 and 14:

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    1.72

    Transference number

    The fractional current carried by each species mustadd up to the total current, then

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    1.73

    Transference number

    For a binary electrolyte

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    1.74

    Exercise #10

    Solve problem 6 of the book, Ch2 (p. 27). Thetransference number of Cu+2 in a copper sulfatesolution in water is 0.44

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    1.75

    Summary

    Use and understand Nernst equation

    Calculate theoretical amount of reactants and

    products using Faradays law Determine current, voltage and energy efficiency

    Calculate ionic conductivity

    Calculate transference numbers

    Chapter 2:Th d i f l h i l

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    2.76

    Outline

    Cell thermodynamics

    Temperature and Pressure effects

    Nernst Equation Pourbaix Diagram

    Equilibrium constant

    Reversible heat transfer

    Thermodynamics of Electrochemical Systems

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    2.77

    Cell Thermodynamics

    Meaning of potential

    n :number of electrons

    F: Faraday's constant (96485 C/eq)

    Previously we used

    the definition of potential

    0 0G n F E=

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    2.78

    Cell Thermodynamics

    Need to relate thermodynamic (reversible) potentialto state variables

    Electrochemical cells are treated at constant T andP

    Consider closed system (transport of materialbetween system and surrounding is not permitted)at constant T and P to start relationships

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    2.79

    Cell thermodynamics

    Using first law of thermodynamics (closedsystem):

    The work can be associated with

    Mechanical changes

    Other sources: magnetic, surface, or electricwork

    U q w=

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    2.81

    Cell thermodynamics

    For a reversible change at constant temperature, theheat transferred is given by

    S: change in entropy

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    2.82

    Cell thermodynamics

    The canonical state variable for a system operatingat constant T and P is the Gibbs free energy:

    The enthalpy change is given by:

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    2.83

    Cell thermodynamics

    Combining Eqs. 1 to 4:

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    2.84

    Cell thermodynamics

    Substituting Eqs. 6 and 7 into 5 yields:

    Reversible work, therefore it is the maximum workthat can be obtained from the system

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    2.85

    Cell thermodynamics

    The maximum electrical energy available in anexternal circuit is equal to the number of chargesmultiplied by the maximum potential difference

    (reversible work):

    By using: F in C/ eq and E in V, your work will give

    you J

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    2.86

    Cell thermodynamics

    Equating Eqs. 8 and 9:

    Equation 10 demonstrates that we can obtainthermodynamics information from electrochemicalmeasurements, and vice measurements, and vice-

    versa

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    2.87

    Cell thermodynamics

    Because Gibbs free energy is a state function (itdoes not depend on trajectory) we can manipulateequations mathematically to obtain reversible

    potentials, e.g.:

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    2.88

    Cell thermodynamics

    Substituting Eq. 10 into 11:

    Dividing by F and simplifying:

    Eq. 13 is ALWAYS TRUE

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    2.89

    Thought

    We said before:

    You can balance the stoichiometry of the

    equation by multiplying by any positive constantThis operation does not alter the potential of thecell (potential is an intensive quantity,unaffected by the number of electrons)

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    29/04/12 CHEM4003 2.90

    Answer to thought

    Yes it is true because we were multiplying theindividual reactions to eliminate the electrons fromthe total reaction

    However, Eq. 13 is still true

    See demonstration on the board

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    2.91

    Thought

    What happen when the final reaction involveelectrons?

    1. Choose the electrode reactions from thestandard electrode potentials table

    2. Reverse the sense of the reactions according toyour system

    3. Reverse the sign of your standard potentials4. Add the potentials using Eq. 13 to obtain the

    potential of the total reaction

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    2.92

    Cell thermodynamics:conclusions

    Eq. 13 is always valid

    If your overall reaction does not involve electrons

    you dont need to correct the potentials (useprocedure explain before)

    If your final reaction has electrons involved youneed to strictly use Eq. 13.

    Standard Potentialand Gibbs free energy

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    2.93

    and Gibbs free energy

    According to Eq. 10 the standard potential of the

    cell can be calculated from the Gibbs free energy Gibbs Free energy for a reaction:

    Where:

    s: stoichiometric coefficient (positive for products and

    negative for reactantsG: free energy of formation. Information tabulated

    see Thermo chemical data handout

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    29/04/12 CHEM4003 2.94

    Exercise 1

    Solve Problem 2 of the book

    (Ch 3,p. 46)

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    29/04/12 CHEM4003 2.95

    Temperature Effect

    We can calculate the reversible electrode potentialat other temperature by calculating the Gibbs freeenergy at a specified T and Using Eq. 10

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    2.96

    Temperature Effect

    Consider a reversible process were only mechanicalwork is permitted, then the first law is

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    2.97

    Temperature Effect

    The enthalpy is defined by

    A differential change in enthalpy is given by

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    2.98

    Temperature Effect

    The Gibbs free energy is defined by

    A differential change in Gibbs free energy is givenby

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    2.99

    Temperature Effect

    Combining Eqs. 14, 16, and 18

    Consider a process from state 1 to state 2, we canwrite Eq. 19 for each state as:

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    2.100

    Temperature Effect

    At constant pressure Eq. 19 becomes:

    Substituting Eq. 10 into Eq. 21 yields:

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    2.101

    Temperature Effect

    Using Eq. 22 we can calculate the effect oftemperature on the reversible potential.

    Over a small temperature range a constant entropychange of reaction is usually justifiable, thenintegrating Eq. 22:

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    2.102

    From thermodynamics

    The enthalpy, entropy, or Gibbs free energy of areaction is given by:

    Where:

    M: property (H, S or G)

    s: stoichiometry coefficient (positive for

    products and negative for reactants)

    ff

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    2.103

    Temperature Effect:Important considerations

    It is very important to include the phases in thecalculation, that is, make sure that you read the

    properties of the compounds at the T physical stage

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    2.104

    Exercise 2

    In a fuel cell the overall reaction is given by:

    Write the electrode reactions Estimate the standard cell potential Calculate the change in reversible potential with

    temperature (mV/K) near room temperature What is the reversible potential of the cell at 35 oC.

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    2.105

    Pressure Effect

    The change in the reversible potential with pressurecan also be calculated from Eq. 19 by taking itsderivate at constant temperature:

    Change of volume in the reaction

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    2.106

    Pressure Effect

    Substituting Eq. 10 into Eq. 24 yields:

    At low pressure the ideal gas assumption is valid,then:

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    2.107

    Pressure Effect

    Substituting Eq. 26 into Eq. 25 and integrating:

    Eq. 27 can be used at low pressures where the idealgas assumption is valid

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    2.108

    Exercise 3

    Calculate the reversible potential of the celldescribed in Exercise 2 at 3 atm

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    2.109

    Thermodynamics Properties

    Thermodynamics properties can be obtained bymeasuring electrochemical potential, e.g., enthalpycan be calculated by

    Entropy change of a reaction can be calculated byusing Eq. 22

    Nernst Equation

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    2.110

    Nernst Equation

    Walther Nernstdeveloped an equation thatcorrelates the voltage of the cell with its properties

    To calculate the reversible potential at conditions

    different to standard we can use the Eq:

    Where a is the activity coefficient of species i

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    2.111

    Nernst Equation

    As an approximation, we can ignore activitycoefficient corrections and use concentrations in

    place of activities:

    Ass mptions

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    Assumptionswhen using Nernst Equation

    Neglects:

    Activity coefficients

    Potential that arise from bringing two differentliquid phases into contact

    Nernst Equation:

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    2.113

    Nernst Equation:Important considerations

    It cant be used to make T and concentrationcorrections simultaneously.

    In such a case:

    Use Eq. 22 or Eq. 25 to make T and Pcorrections, respectively

    Applied Nernst Eq. at the new T or P.

    Nernst Equation:

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    2.114

    Nernst Equation:Conventions to activity coefficients

    Assume activity coefficient of 1 for the followingcases:

    Substances in excess (e.g., solvents)

    solids

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    2.115

    Pourbaix Diagram

    Consists of plotting the potential vspH

    This type of diagram is useful because it allowsidentifying phases in equilibrium providing criticalinformation on the behavior of the system

    It was proposed by Marcel Pourbaix

    Procedure to buildPourbaix Diagram

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    2.116

    Pourbaix Diagram

    Write down all the equations involved in the system Use Nernst equation Express all reactions as a function of potential, pH, or

    both

    Plot Potential vs. pHEqs. independent of pH are plotted as a horizontal

    lineEqs. independent of potential are plotted as a

    vertical lineEqs. dependent on both (pH & potential) are plotted

    as an oblique line

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    2.117

    Pourbaix diagram other assumptions

    Typical assumptions

    Concentrations of ions 10-6 M

    Gases at 1 atm

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    2.118

    Exercise 4

    Build the Pourbaix diagram for the lead-watersystem (also known as le Plant battery). Take intoconsideration the following reactions

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    2.119

    Equilibrium Constant

    When the reversible potential equals zero, meansthat the driving force for the electrochemicalreaction is zero, which represents the stable

    equilibrium state for the cell

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    2.120

    Equilibrium Constant

    Since the potential is zero at equilibrium, we candetermine the equilibrium constant from thestandard open circuit potential:

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    2.121

    Exercise 5

    Calculate the equilibrium constant for theDaniellCell

    Zn/Zn+2 /Cu+2 /Cu

    Heat Transfer

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    2.122

    Because the system works at constant T and

    Pressure, we expect to see some transfer of heat tothe medium

    Heat transfer includes: reversible and irreversible

    heat (always negative, loss to ambient) The reversible heat is given by

    IfS>0 the process is endothermic

    IfS

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    2.123

    For a reversible process in an open system, the energy

    balance is given by:

    :partial molar quatity (includes mixing energy)

    Most of the time mixing energy is low compared toenergy of reaction, then the change can be calculated

    based on pure components

    S

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    2.124

    Summary

    Meaning of potential (related to Gibbs free energy)

    For temperature effects use the entropy change (becareful with the physical change stage of thereactants and products)

    For pressure change use the volume change(include only gases in the change calculation)

    Use assumptions in Nernst Equation

    S

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    2.125

    Summary

    You cant correct for T, P and concentration effectssimultaneously Correct for T and P Correct for concentration effect

    Know how to build and interpret Pourbaix diagram Calculate equilibrium constants Calculate heat transfer in open systems

    Whats the meaning of a positive and negativeentropy change?

    Chapter 3: Electrode Kinetics

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    3.126

    Outline

    Interface Role

    Electric Double Layer

    Helmholtz model Electrode Kinetics Models

    Butler-Volmer Equation

    Tafel Equation

    Reference Electrodes

    f l

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    3.127

    Interface Role

    Electrode kinetics are governed by the potentialdifference across a thin (order 10 A) layer adjacentto the electrode surface

    This layer is called the double-layer

    Potential difference across the thin layer is about0.1 V

    Large magnitude of electric field (106 V/cm)

    f l

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    Interface Role

    Large driving force for the electrode reaction

    Because of the large electric field we will havecharge separation in the double layer

    Electroneutrality condition does not apply in thedouble layer region

    I f R l

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    Interface Role

    At equilibrium (thermodynamics relationships areused) theres no current applied

    When current is applied the potential will deviatefrom equilibrium

    The difference between the potential and theequilibrium potential is called the overpotential (or

    surface overpotential)

    I f R l

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    3.130

    Interface Role

    The surface overpotential is given by:

    I ith El t d Ki ti

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    3.131

    Issues with Electrode Kinetics

    Electrode reactions are heterogeneous. This impliesthat a conductive surface must be in contact withthe electrolyte

    This arrangement produces a number of issues (weneed a clean surface to evaluate pure kinetics):Film formationChanges in electrode microstructure

    Electrolyte contaminationAll of them cause variations in current-potentialmeasurements

    E i t l S l ti

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    Experimental Solutions

    Careful electrode surface preparation (e.g., polishthe surface, in corrosion we need a rough surfaceinstead)

    Electrolyte purification (e.g., deoxygenation of theelectrolyte)

    Control of mass transport to the electrode surface

    (mixing)

    Typical KineticsE i t l S t

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    3.133

    Experimental Set-ups

    1-reference electrode

    2-gas in

    3-gas out4-Luggin capillary

    5-platinum counter electrode

    6-rotating electrode

    7-temperature probe

    8-pH electrode

    9-working electrode.

    Typical Kinetics

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    3.134

    ypExperimental Set-ups

    The electrode rotates to have control of the masstransfer limitations

    The flow profile is known in this type of systems

    Classical arrangements:

    Rotating disk electrode (use for laminar flows)

    Rotating cylinder electrode (use for turbulent

    flows)

    More Issues with

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    Electrode Kinetics

    Accurate measurement of the potential is difficult Because we cant measure an absolute value for the

    potential, we are forced to use a reference electrode

    Reference electrodes are chosen based on:reversibility, stability, and convenience (cost) Suitable placement of the reference electrode is

    another issue (need to correct for ohmicdifferences)

    El t i D bl L

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    3.136

    Electric Double Layer

    When we apply a potential to an electrode thecharges that accumulate at the surface of theelectrode attract opposite charges from the

    electrolyte We expect to have a distribution of charges in order

    to balance the charges at the surface with the

    charges from the electrolyte

    Electric Double Layer

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    Electric Double Layer

    There are different models to determine the effect(or to simulate the effect) of the double layer:

    Helmholtz model

    Gouy and Chapman model

    Stern model

    Helmholtz Model

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    3.138

    Helmholtz Model

    It was developed in 1879 Its the simplest model for

    double layer

    Two parallel layers ofcharges are separated bysolvent molecules

    The distance (d) representsthe outer Helmholtz plane

    Fixed distribution of layer(charges)

    Helmholtz Model

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    3.139

    Helmholtz Model

    Double layer model as a simple parallel platecapacitor

    C: capacitance per unit area (F/m2 or mF/cm2)

    D: dielectric constant (or relative permittivity)

    d: Separation between charges, cm

    0: Permittivity of free space, 8.8542x10-14 F/cm

    Helmholtz Model

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    Helmholtz Model

    The potential distribution is a linear functionbetween the two layers of charge

    Because the distribution of the charges does notchange the potential is constant, also C is constant

    Helmholtz Model

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    3.141

    Helmholtz Model

    For water D10, d10 A, then:

    Helmholtz Model

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    3.142

    Experimentalmeasurements use a NaFsolution in a mercuryelectrode

    Mercury offers a uniform

    surface and NaF is notadsorbed Capacitance in the right

    order of magnitude but itis not constant

    Only for highconcentrations thecapacitance tends to beconstant

    Fig. Capacitance vs. potential

    relative to the point of zero chargefor a NaF solution on a mercuryelectrode at 25oC (experimentaldata)

    Gouy-Chapman Model

    It d l d i 1910

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    3.143

    It was developed in 1910 Its analogous to the Debye-

    Hckel theory The thickness of the double layer

    represents a compromise betweenelectrical forces (tending to

    maintain the ordering) andthermal forces (tending to makethe arrangement random)

    No fixed charges

    Significant deviation fromelectroneutrality occurs on theDebye length

    Gouy Chapman Model

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    3.144

    Gouy-Chapman Model

    The capacitance is given by

    Gouy-Chapman Model

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    3.145

    Its good at potentials near the zero charge region Atpotentials ore than 0.5 V in either direction the observedflattering of the capacitance is not predicted

    Fig. Capacitance vs. potential relative to

    the point of zero charge for a NaF solution,calculated using Gouy-Chapmanmodel (Eq. 3)

    Fig. 5.2 Capacitance vs. potential relativeto the point of zero charge for a NaFsolution on a mercury electrode at 25oC(experimental data)

    Stern Model

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    3.146

    Combines the Helmholtz model

    and the Gouy-Chapman model Some of the charge is fixed (d

    region) and some of the charge isdiffuse or spread out

    The total length of the boundarylayer is given by the fixed region

    plus the diffuse region

    Stern Model

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    3.147

    Stern Model

    Because the capacitances are in series thecapacitance of the double layer is given by:

    Stern Model

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    3.148

    Stern Model

    The smallest capacitance is the one that governs thebehavior of the system:

    If CH CG-C then CSCG-C

    If CH

    CG-C

    then CS

    CH

    Eq. 5

    Stern Model

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    3.149

    Stern Model

    Assuming that CH is

    constant

    The Stern model predictsthe experimental datavery well

    Fig. Capacitance of 0.001 M NaF vs. potential relative to

    the point of zero charge at 25oC. The experimental data(circles) agrees very well with the model (Stern Model, Eq.4)

    Consequences

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    3.150

    of the Double-Layer

    Species outside the Helmholtz region are toodistant to react

    The driving force for the reaction is the potential

    drop across the Helmholtz region rather than thepotential drop across the whole double layer

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    Electrode Kinetics

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    3.152

    Electrode Kinetics

    In ordinary kinetics weexpress the progress of areaction by plotting the

    reaction coordinate vs. theenergy of the species(assuming transition statetheory)

    Electrode Kinetics

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    3.153

    Electrode Kinetics

    Let us consider one elementary stepelectrochemical reaction:

    WhereO+: oxidized species

    R: reduced specieskc: cathodic reaction rate constant

    ka: anodic reaction rate constant

    Electrode Kinetics

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    3.154

    A more negative potential (morepositive energy) tends to promotereduction

    At progressively more negativepotential, the energy of the oxidized

    species is increased

    3: reduction is favored

    1

    : oxidation is favored

    2: equilibrium potential, no netreaction takes place

    Electrode Kinetics

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    3.155

    Electrode Kinetics

    Consider the case where we start an experiment atthe potential 1 and we reduce it to 2

    The activation energy for the first process (Eac1) is

    higher than for the second process (Eac2)

    Electrode Kinetics

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    3.156

    We can express the activation energy for the secondprocess as a function of the first process by:

    Where

    is the symmetry factor (transfer coefficient)

    represents the fraction of energy that has been usedto reduce the activation energy of the reaction

    Electrode Kinetics

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    3.157

    Similarly the activation energy for the anodicprocess (which increases) can be expressed by:

    n: is the number of electrons transferred in thereaction. For elementary steps n is most of the time1, it is unusual to have more than1 electron

    involved in an elementary step

    Electrode Kinetics

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    3.158

    The form of our kinetic expression is the same asthat for chemical reactions (using an Arrheniusdependence of temperature):

    Where

    k: is the a constant, cm/s G: is the free energy of activation

    Electrode Kinetics

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    3.159

    The rate of electrochemical reaction is directlyproportional to the current density:

    Wherer: reaction rate, mol/s cm2

    i: current density, A/cm2 (the area is the electrode surface area)c: is the reactant concentration (mol/cm3)

    Electrode Kinetics

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    3.160

    For the general anodic reaction given in Eq.6 (firstorder reaction), we substitute Eq. 8 into Eq. 10

    We have assumed a reference potential, therefore thesubscripts 1 and 2 have been dropped

    Electrode Kinetics

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    3.161

    We can redefine the reaction constant including theactivation energy at our reference potential:

    Electrode Kinetics

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    3.162

    Similarly for the cathodic reaction:

    The net current density (i=ia-ic) is the difference

    between the anodic and cathodic current densities(Eq. 12-Eq. 13)

    Electrode Kinetics

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    3.163

    At equilibrium the net current density is zero, butthe rates of the anodic and cathodic reaction are notzero. The magnitude of both (ia and ic) are the same

    and this is called exchange current density (i0)

    Electrode Kinetics

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    3.164

    If we designate the equilibrium potential as 0

    Taking the logarithm of Eq. 15 and rearranging:

    Electrode Kinetics

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    3.165

    Substituting Eq. 16 into Eq. 14 and using thedefinition of overpotential:

    Electrode Kinetics

    Rearranging Eq. 17:

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    3.166

    Eq. 18 is a general kinetics expression for the first orderelementary step given in Eq. 6

    The concentration of the reactants are at the surface of theelectrode The cathodic and anodic kinetic constants can be

    evaluated at equilibrium from the exchange current

    density:

    Where the superscript 0 represents equilibrium conditions

    Eq.18

    Electrode Kinetics

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    3.167

    Substituting the kinetic constants into Eq. 18 weobtain:

    Butler-Volmer Equation

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    3.168

    Redefining the transfer coefficients for the anodic and

    cathodic components as:

    And assuming the concentration at the surface is equal tothe concentration at the bulk which will be the case ofequilibrium condition, then Eq. 19 becomes:

    Eq. 20 is known as theButler-VolmerEquation

    Butler-Volmer Equation

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    3.169

    Three variables a, c, and i0 need to be determined to useButler-Volmer Equation

    Butler-Volmer equations gives a good representation of

    experimental data for many systems The exchange current density is a strong function of

    temperature When the exchange current density is very large, the

    reactions is said to be reversible

    Butler-Volmer Equation

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    3.170

    When two reactions take place simultaneously, onthe same electrode surface, we can use the Butler-Volmer equation for each of them

    We will have to determine the individualparameters for both reactions

    Linear form ofButler-Volmer Equations

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    Butler-Volmer Equations

    One of the disadvantages of the Butler Volmerequation is that the overpotential cant be expressedimplicitly

    To confront this several approximations have beenmadeSmall surface overpotentialLarge surface overpotential

    Linear form ofButler-Volmer Equations

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    3.172

    Butler-Volmer Equations

    When the overpotential is very small, theexponential term in Eq.20 can be expanded usingMaclaurin series, neglecting some of the terms in

    the series:

    Linear form ofButler-Volmer Equations

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    3.173

    Eq. 21 is the linear form of the Butler-VolmerEquation

    The current density is a function of only oneparameter (i0 and the transfer coefficients can bedefined as one constant)

    It is used to model systems operating at low currentdensities

    Its often used when the overpotential is 10mV orless

    If the current density does not vary widely (30%),the linear expression can be used even in the highcurrent density

    Tafel Equation

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    3.174

    If the overpotential is large and positive, the secondterm in Eq. 20 can be neglected:

    If the overpotential is large and negative, the firstterm in Eq. 20 can be neglected:

    Tafel Equation

    Eqs. 22 and 23 are known as Tafelti

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    3.175

    equations

    Taking the logarithm of Eq.22 andrearranging:

    The constantB is called the Tafel Slope Use of the Tafel approximation depends on the error thatcan be tolerated

    It is general used when the overpotential is at least 50 to100 mV

    Th T f l l i b t 30 t 300 V/d d

    andWhere

    Tafel Equation

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    3.176

    Values of the exchange current density and thetransfer coefficient are obtained experimentally

    Plot overpotential vs. log(i). The slope of the linewill give the transfer coefficient, and the interceptwill give the exchange current density

    Example 1

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    3.177

    Solve problem 3 of chapter 5 in your text book

    Example 2

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    3.178

    Solve problem 2 of chapter 5 in your text book

    Reference Electrodes

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    3.179

    So far we have learned how to estimate kineticexpressions as a function of the overpotential

    We have also learned that the overpotential is givenby:

    Reference Electrodes

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    3.180

    When using the overpotential equation, we need tomake sure that the potential that we measure is onlydue to the electrochemical reaction

    One of the ways to accomplish that is by usingreference electrodes Before discussing more details about reference

    electrodes, we will present a discussion in the

    factors that affect the potential

    Contributions tothe Potential in Galvanic Cells

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    3.181

    The maximum potential that we can measure in agalvanic cell is the equilibrium potential.

    The equilibrium potential is only obtained when

    no current (or very small current) flows throughthe circuit

    When a current flows through the circuit the

    potential measure will always be smaller than theequilibrium potential

    Contributions tothe Potential in Galvanic Cells

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    3.182

    The decrease in the potential of the cell is due toseveral limitations, and this is often calledPotential loss, Eloss

    Therefore, the potential of a cell is defined as:

    Where

    E: equilibrium potential : potential of the cell

    Contributions tothe Potential in Galvanic Cells

    Th t ti l li it ti i l d

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    3.183

    The potential limitations include:

    Surface overpotential limitations, due to kineticslimitations

    Concentration overpotential, due to diffusion andconvection limitations in the electrolyte (also knownas liquid-junction potential)

    Ohmic drop, due to the mobility limitations (ioninteractions)

    Solid diffusion limitations, due to diffusionlimitations in porous electrodes, e.g., electrodes thatthe ones used in lithium ion batteries

    Contributions tothe Potential in Galvanic Cells

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    3.184

    Accounting for all the limitations the potential lossis given by:

    Where:

    Contributions tothe Potential in Galvanic Cells

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    3.185

    In an electrolytic cell the minimum potential thatwe need to apply for the reaction to take place isthe equilibrium potential

    Therefore the potential in an electrolytic cell isgiven by:

    The potential loss is calculated using Eq. 25.

    Reasons for UsingReference Electrodes

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    3.186

    Measurement of the potential at equilibriumconditions is relatively easy. All we need to makesure is that the current that flows through the circuit

    is very small Such determination depends on the use of a

    counter-electrode having a known reversiblepotential

    Reasons for UsingReference Electrodes

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    3.187

    Under load the measurement of the potentialrespect to a reference electrode becomes morecomplicated (due to theEloss). In addition we will

    have significant reactions at both electrodes Then a simple two electrode approach is not longersatisfactory for making accurate measurements

    A technique to overcome this problem is to use a

    third electrode into the electrolyte

    Reasons for UsingReference Electrodes

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    3.188

    The reference electrode should beplace very close to the workingelectrode

    In theory it should be placed justoutside the electrical double layer

    However, the electrical field of theelectrode can affect themeasurement of the overpotential

    A rule of thumbs suggest to place

    the reference electrode at least4diameters (of the referenceelectrode) away from the workingelectrode

    Reasons for UsingReference Electrodes

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    3.189

    An approach to avoid theeffect of the referenceelectrode field on the

    working electrode is to usea luggin capillary Ohmic drop in the capillary

    tube is small because the

    current that flows through itis very small

    Reasons for UsingReference Electrodes

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    3.190

    Sometimes a second reference electrode is added tomeasure the ohmic drop between two points in thesolution. This approach is known as the four

    electrode arrangement Another use of reference electrodes is to measure

    current distributions in a cell having a non uniformcurrent distribution

    Reasons for UsingReference Electrodes

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    3.191

    Summarizing the reasons for using referenceelectrodes are:

    Accurate measurement of surface overpotentials

    Measurement of ohmic drops in solutionMeasurement of current distribution

    Types of ReferenceElectrodes

    When choosing a reference electrode we have the followingi i

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    3.192

    criteriaReproducibilityStabilitySmall temperature sensitivity

    Sometimes a reference electrode of the same type as theworking electrode is chosen, this is known as a pseudoreference electrode:Avoids:

    Contamination problems Liquid junction potential problems

    The problem with doing this is that sometimes the resultsare not reproducible and they are more difficult togeneralize

    Types of ReferenceElectrodes

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    3.193

    Generally the reference electrode should be chosenthat is reversible to one of the ions in solution.However, this is difficult to accomplish all the time

    The practical approach is to choose a referenceelectrode that is standard built for some electrolyteconditions

    Types of ReferenceElectrodes

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    3.194

    Typical reference electrodes

    Hydrogen electrode

    Calomel electrode (SCE)

    Mercury-Mercuric oxide electrode

    Mercury-mercurous sulfate electrode

    Silver-Silver Chloride electrode

    Calomel Electrode

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    3.195

    It is constructed by covering a pool of mercury withmercurous chloride (calomel)

    Potassium chloride is the electrolyte for the

    following reaction:

    Calomel Electrode

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    3.196

    The equilibrium potential is given by:

    Commercial electrodes are commonly preparedwith three concentrations of KCl: 0.1 N, 1 N andsaturated

    The calomel electrode is best used in acid solutions Reproducibility is about 2 mV

    Ag/AgCl Electrode

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    3.197

    It is used when mercury contamination is notallowed

    KCl is used as the electrolyte. The most common

    concentration is 4M It is also used in acidic solutions

    The reaction involved is:

    The equilibrium potential is given by:

    Mercury/Mercurous electrode

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    3.198

    It is used in acid solution

    When chloride contamination is not allowed

    The reactions if given by:

    Mercury/Mercuric oxideelectrode

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    3.199

    It is used in basic solutions

    It uses KOH as the electrolyte

    The reaction is given by:

    Calculation of overpotentials

    For the calculation of overpotential we need to use Eq.

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    3.200

    For the calculation of overpotential we need to use Eq.

    Because the applied potential is measured respect to a

    reference electrode, the Equilibrium potential for thereaction needs to be expressed respect to the referenceelectrode:

    Ew: equilibrium potential of the working electrodeEref: equilibrium potential of the reference electrode

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    Summary

    At the end of this chapter you must be able to:

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    3.202

    p y

    Use and understand the different expression to expresselectrode kinetic rates

    Calculate over potentials

    Correct surface overpotentials from other loss effectsKnow the uses and applications of reference electrodesUnderstand the effect of the double layer on the

    electrode kinetics (e.g., what do you do experimentally

    do reduce this effect?)

    Outline

    Chapter 4: Mass Transport

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    4.203

    Fundamental relationships

    Mass transport boundary layer

    Concentration Overpotential

    Limiting Current Density

    Fundamental Relationships

    A general description of an electrochemical system

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    4.204

    A general description of an electrochemical systemtakes into account:Species fluxes

    Material conservation (material balance)

    Current flowElectroneutrality

    Electro-kinetics

    Global reactionsHydrodynamics

    Species Flux

    Using dilute concentration theory (considers only

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    4.205

    Using dilute concentration theory (considers only

    interactions between solute-solvent), the flux ofspecies is given by:

    Comparing to general chemical engineering systems

    the difference in the flux is given by the migrationterm (potential generated due to the ion interactions)

    Species Flux

    Where:

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    4.206

    Where:

    Ni: flux of species, mol/cm2 s

    zi: charge number of species i, eq/mol

    ui: mobility of species i, cm2-mol/Jsci: concentration of species i, mol/cm3

    : electrostatic potential, V

    Di: diffusion coefficient of species i, cm2/s

    v: fluid velocity, cm/s

    The flux is perpendicular to the surface area (as usual)

    Current Flow

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    4.207

    Current will arise from the motion of the chargesand is given by:

    Material Balance

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    4.208

    The material balance is given by:

    Where Ri represents a chemical reaction ccurring insolution (mol/cm3).

    Eq. 3 assumes constant volume

    Electroneutrality Equation

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    4.209

    Because the electrical forces between chargedspecies are so large, significant charge separationcannot occur. Therefore, in the bulk the

    electroneutrality assumption is valid:

    Simulations

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    4.210

    To carry out a simulation of the performance on anelectrochemical system, Eqs. 1-4 need to be solvedsimultaneously

    We need a description of the flow pattern toaccount for v in Eq. 1

    Eqs. 1 to 4 apply at the bulk, the electrode kineticsis used as boundary conditions for the solution ofthe differential equations

    Common simplifications

    If bulk concentrations can be ignored we can demonstrate

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    4.211

    bu co ce t at o s ca be g o ed we ca de o st ate

    that the gradient of the current is given by:

    When concentration variations can be neglected weobtained ohms law instead of Eq. 2:

    Where k (conductivity) is given by:

    This Eq. is known as conservation of charge

    Common simplifications

    Another important definition is the transport

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    4.212

    Another important definition is the transport

    number:

    When concentration variations are important,ohms law becomes modified ohms law:

    Common Simplifications

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    4.213

    When migration is negligible (in excess of a supportingelectrolyte), the coefficient of the potential gradient inEq. 1 is large, then the potential gradient must be small

    The material balance can be obtained from substitutingsimplified Eq. 1 into Eq. 3

    Common simplifications(supporting electrolyte)

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    4.214

    This equation is known as the convective diffusionequation:

    The potential distribution can still be obtained by

    solving the modified ohms law equation

    Mass transport boundary layer

    For systems where the concentration gradient issignificant, one common simplification is to treat

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    4.215

    g , p

    the boundary layer region as a region with a linearconcentration gradient

    This is known as Nernst diffusion layer

    Mass transport boundarylayer

    Nernst approximation for the concentration gradient is

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    4.216

    expressed as:

    Where:

    c: concentration at the bulk

    c0: concentration at the surface: thickness of the boundary layer.The thickness of this layer is between 0.05-0.001 cm

    Example 1

    Use the transport equations to derive an expression

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    4.217

    p q p

    for the current for a copper deposition reaction as afunction of the surface and bulk concentration. Theelectrolyte is composed of copper, water and H2SO4

    (added to increase conductivity)

    Write down expressions for your transportproperties

    Consequences of addingsupporting electrolytes

    Reduces ohmic losses

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    4.218

    Reduces limiting current density

    Increases the viscosity of the solution and thereforedecreases the maximum velocity

    Reduces the magnitude of the electric field

    Concentration Overpotential

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    4.219

    Concentration overpotential is associated with themass transport limitations

    It results from:

    The concentration difference between bulk and

    electrode surfaceFrom the potential gradient (see modified Ohms

    law, second term)

    Concentration Overpotential

    Assuming that the variations in the ionic

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    4.220

    conductivity are small (small current densities or asupporting electrolyte is used). The concentrationoverpotential can be obtained by:

    Concentration Overpotential

    When the conductivity is large the equation can be

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    4.221

    approximated with:

    This is the concentration overpotential for a cathodicreaction. The concentration overpotential for acathodic reaction is negative (as well as its surfaceoverpotential)

    Concentration Overpotential

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    4.222

    For an anodic reaction, the concentrationoverpotential is positive and can be estimated (forlarge conductivities) by:

    Limiting current

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    4.223

    When the current at the surface is equal to zero, thecurrent measured is known as the limiting current

    For the boundary layer assumption, the current is

    defined as (we demonstrated this in Example 1):

    Limiting current

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    4.224

    Then the limiting current for the Nernst diffusionlayer is given as:

    The limiting current density is a function of the

    flow pattern. It is up to 100 order of magnitudelarger in stirred solutions

    Limiting current

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    4.225

    The overpotential can be expressed as a function ofthe limiting current, for example for highconductivities the cathodic concentration

    overpotential is given by Eq. 6, which can beexpressed as:

    Limiting current

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    4.226

    At currents higher than the limiting currentadditional reactions takes place

    After the limiting current the two reactions take

    place in parallel with the secondary reaction takingover the primary reaction

    Limiting current

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    4.227

    Supporting electrolytes reduce ohmic losses buttend to reduce the limiting current

    Supporting electrolytes increase the viscosity of the

    solution and decreases the mobility of the ions

    Diffusion coefficient

    The transport equations require the use of thediffusion coefficient.

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    4.228

    diffusion coefficient.

    The diffusion coefficient for ionic species can becalculate by using the Nernst-Einstein equation:

    For a binary electrolyte the diffusion coefficient

    becomes:

    Diffusion coefficient

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    4.229

    Because the ionic diffusion coefficient is related tothe mobility, it can be calculated using theequivalent conductances:

    Values of diffusion coefficients of selected ions at infinitedilution in water at 25oC p284

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    4.230

    Estimation of limiting current

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    4.231

    The limiting current can be estimated from themass transfer correlations

    Usually mass transfer limitations are expressed as:

    Where km is the mass transfer coefficient (cm/s)

    Estimation of limiting current

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    4.232

    At the limiting current the surface concentration iszero, therefore, the limiting current is related to themass transfer coefficient:

    The mass transfer coefficient is related to theSherwood number (Sh) which is a function of theReynolds (Re) and the Schmidt (Sc) numbers

    Estimation of limiting current

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    4.233

    The following correlations are used

    WhereL is the characteristic length, v is the velocity of thefluid, and v is the kinematic viscosity (cm2/s) (v = /)

    Estimation of limiting current

    Some correlations require the use of the Grashof

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    4.234

    number (Gr). This number is used when the mass transport is

    affected by density differences

    Where:g: acceleration due to gravity

    : bulk density0: surface density, equal to the solvent density

    Estimation of limiting current

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    4.235

    Correlations for the Sherwood number has beendetermine for specific geometries where the flow

    pattern is well known

    The correlations are summarized in appendix E ofthe book

    Example 2

    For the cathodic deposition of copper from 0.5 M CuSO4and 0.5 M H2SO4 electrolyte, the kinetic parameters are

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    4.236

    c=0.5 and i0=1 mA/cm2. If the applied potential is 100mV respect to a SCE. Calculate:

    A. The current density for copper deposition expected ifonly kinetics limitations are involved

    B. The limiting current density if two plane parallelcopper electrodes, 2 cm long are used in a beaker ofunstirred electrolyte

    C. Estimate the thickness of the Nernst diffusion layer

    Summary

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    4.237

    At the end of this chapter you should be able to:

    Calculate diffusion coefficients for ionic species

    Determine limiting current for different geometries

    Calculate currents when kinetics and mass transportlimitations are involved

    Write down the fundamental equations to model an

    electrochemical system assuming dilute solutiontheory

    Outline

    Chapter 5:Industrial applications of Electrochemical Engineering

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    Batteries and Fuel cells:Working Principle, types, applications and

    design aspects

    Production and refining of metals : Applications in chemical industries Corrosion Prevention

    Fuel cells-An introduction

    Output of conventional batteries are limited.

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    They are polluting. Continuous operation results in fall in efficiency. Output not stable under long durations of operations.

    Fuel cellAn Electrochemical energy conversion deviceProduces electricity from external fuel and oxidant.Can operate virtually continuously as long as the

    necessary flows are maintained.

    Basic Fuel Cell Concept

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    Fuel cells-Working principle

    A fuel cell is an electrochemical device that converts the

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    chemical energy in fuels (e.g. hydrogen, methane, butane oreven gasoline and diesel) into electrical energy. It exploits the natural tendency of oxygen and hydrogen to

    react to form water.

    The direct reaction is prevented by the electrolyte, whichseparates the two reactants.

    Therefore two half-reactions occur at the electrodes:

    Anode: Fuel (e.g. H2, CO, CH4) is oxidized

    Cathode: Oxygen is reduced

    The ions are transported to the other electrodethrough the electrolyte.

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    The fuel cell contains no moving parts and onlyfour active elements:cathode,anode,

    electrolyte and interconnect;

    It is a simple and robust system.

    A fuel cell uses a chemical reaction to provide anexternal voltage, as does a battery, but differs froma battery in that the fuel is continually supplied in

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    the form of hydrogen and oxygen gas.

    It can produce electrical energy at a higherefficiency than just burning the hydrogen to

    produce heat to drive a generator

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    Types of Fuels cells

    The general design of most fuel cells is similar

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    except for the electrolyte. The six main types of fuel cells, as defined by theirelectrolyte, areAlkaline Fuel Cells,

    Proton Exchange Membrane Fuel Cells,Phosphoric Acid Fuel Cells,Molten Carbonate Fuel Cells,Direct Methanol Fuel Cells,

    Solid Oxide Fuel Cells.

    Alkaline Fuel Cell

    Electrolyte is a porous matrix

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    saturated with aqueousalkaline solution (normallyKOH)

    Provides heat, electricity andpotable water as outputs.

    Used in Apollo Mission tomoon. 1: Hydrogen 2:Electron flow

    3:Charge4:Oxygen 5:Cathode

    6:Electrolyte

    7:Anode 8:Water 9:Hydroxyl

    Ions

    Chemical reaction

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    The chemical reaction that occurs at the anode is:2H2 + 4OH 4H2O + 4 e-

    The reaction at the cathode occurs when theelectrons pass around an external circuit and reactto form hydroxide ions, OH :

    O2 + 4e + 2H2O4OH

    Types of alkaline Fuel cell

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    Mobile Electrolyte-eg. Pure H2 Fuel-Electrolyte pumped

    through a circuit

    Static Electrolyte- eg. Pure H2 Fuel-But electrolyte is held

    in a matrix material

    Dissolved Fuel Electrolyte-eg. Hydrazine Fuel

    Fuels used in Alkaline Fuel Cells

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    Metal HydrideAbility to be recharged with electrical energyLow operating temperatures (down to -20C);

    Fast kinetics;Extended shelf life;Absorbs and stores hydrogen within the cell.

    Fuels used in Alkaline Fuel Cells

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    Direct borohydride cell

    A solution of sodium borohydride is used as thefuel.

    Prevents the conversion of KOH to K2CO3Cheaper than traditional fuel cells as it does not

    need platinum electrodes.

    Advantages

    Features of Alkaline fuel cell

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    Cathode reaction faster in alkaline electrolyte,higher performance

    Byproduct is pure water, can be used for other

    purposes.Gives out heat which can be used for heating

    purposes.

    Disadvantages

    Expensive removal of CO2 from the cell

    required.

    lk li f l ll d bl

    Features of Alkaline fuel cell

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    Alkaline fuel cells encountered many problemsincluding cost, reliability, ease of use, durability,and safety which were not easily solved.

    Attempts at solving these problems proved to beuneconomical given the other sources of energy atthe time.

    Th t h b ( k

    PEMFC-Proton Exchange Membrane Fuel Cell

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    The proton exchange membrane (a.k.a.Polymer Electrolyte membrane) fuel cell uses a

    polymeric electrolyte.

    This proton-conducting polymer forms the heart ofeach cell and electrodes (usually made of porouscarbon with catalytic platinum incorporated intothem) are bonded to either side of it to form a one-

    piece membrane-electrode assembly (MEA).

    Advantages

    A i k i f k d h

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    A quick overview of some key advantages thatmake PEMs such a promising technology for theautomotive markets:Low temperature operation, and henceQuick start upNo corrosive liquids involvedWill work in any orientation (or zero g for that

    matter)Thin Membrane-electrode assemblies allow

    compact cells

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    Reactions in PEMFC

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    Molten Carbonate Fuel Cells

    O hi h

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    Operates at hightemperature

    Molten carbonate is

    used as electrolyte. Produces water and

    CO2 as byproducts.

    Delivers high power,of the order 100 MW

    Features of MCFC

    Ad t

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    AdvantagesHigh efficiencyFuel flexibility

    Can use a variety of catalystsSuitable for CHP Disadvantages

    High temperature speeds corrosion andbreakdown of cell components

    Complex electrolyte managementSlow start-up

    PAFCPhosphoric Acid Fuel Cell

    El t l t d i Ph h i A id

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    Electrolyte used is Phosphoric Acid Not affected by CO in the hydrogen stream

    Works above a temperature of 400C.

    If working at 150 to 200 C, expelled water can beconverted to steam and used for heating. Combinedheat and power efficiency of 80 %.

    Large weight and size

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    SOFCSolid oxide fuel cells

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    Solid oxide fuel cells (SOFCs) use a hard, non-

    porous ceramic compound as the electrolyte.

    Because the electrolyte is a solid, the cells do not

    have to be constructed in the plate-like

    configuration typical of other fuel cell types.

    SOFCs are expected to be around 50%60%

    efficient at converting fuel to electricity

    SOFCSolid oxide fuel cells

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    Solid oxide fuel cells operate at very high temperatures

    d 1 000C (1 830F)

    Solid oxide fuel cells (SOFCs)

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    around 1,000C (1,830F). High-temperature operation removes the need for

    precious-metal catalyst, thereby reducing cost. It also allows SOFCs to reform fuels internally, which

    enables the use of a variety of fuels and reduces the costassociated with adding a reformer to the system. SOFCsare also the most sulfur-resistant fuel cell type; they can

    tolerate several orders of magnitude more of sulfur thanother cell types.

    In addition the are not poisoned b carbonid (CO) hi h b d f l

    Solid oxide fuel cells (SOFCs)

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    In addition, they are not poisoned by carbonmonoxide (CO), which can even be used as fuel.This property allows SOFCs to use gases madefrom coal.

    have the distinct advantage of being able to run onbiogas (which delivers the most energy per hectareof crops), natural gas, propane, ethanol, diesel or

    biodiesel and don't require hydrogen,

    http://www.fz-juelich.de/ief/ief-3/datapool/page/179/bild4_b-e.gif
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    http://www.fz-juelich.de/ief/ief-3/datapool/page/179/bild4_b-e.gif
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    Fuel Cel l Type OperatingTemperature Sys tem Output ApplicationsPEM Fuel Cell 50 - 100C

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    Small distributedgenerationTransportation

    Solid Oxide FC 650 - 1000C 5kW 3MW Auxiliary powerElectric utility

    Large distributedgeneration

    Alkaline Fuel Cell 90 - 100C 10kW 100kW MilitarySpace

    Phosphoric Acid FC 150 - 200C 50kW 1MW Distributed

    generationMolten Carbonate FC 600 - 700C

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    dDcCbBaA ++

    bpapdpcpRTGG

    ba

    dco

    .

    .ln+=

    1.The maximum energy output from a fuel cell isequal to its Gibbs energy (at Standard

    conditions)

    Emax

    =GO=H

    f- TS= H

    f- E

    loss

    Correction due to variation in Standard conditions:

    Where pi

    is the partial pressure of the reactants

    and products.

    From Nernst Equation,

    2.The Electric potential can be calculated from the

    equationG = n F E

    cell

    bpap

    dpcpRTEE

    ba

    dcocell

    .

    .ln+=

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    3.The theoretical efficiency of the Fuel cell,max.

    fff

    lossf

    H

    nFE

    H

    G

    H

    EH

    =

    =

    =

    max

    f

    Ivf ..max=

    4.The practical fuel cell efficiency,

    is the practical fuel cell efficiency

    v is the voltage efficiencyIis the current efficiency

    CRfO ..=

    5.The Overall system efficiency,

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    CRfO

    R

    C

    is the Reformer efficiency

    is the DC/AC converter efficiency

    Batteries-Electrochemical cells

    What is a battery?

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    What is a battery? A battery is an electrochemical cell that converts

    chemical energy into electrical energy. It comprises of two electrodes: an anode (the

    positive electrode) and a cathode (the negativeelectrode), with an electrolyte between them. At each electrode a half-cell electrochemical

    reaction takes place.

    Basic principles-The Electrochemical series

    Different metals (and their compounds) have

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    Different metals (and their compounds) havedifferent affinities for electrons.

    When two dissimilar metals (or their compounds)are put in contact through an electrolyte, there is a

    tendency for electrons to pass from one material toanother.

    The metal with the smaller affinity for electronsloses electrons to the material with the greateraffinity, becoming positively charged.

    The metal with the greater affinity becomesnegatively charged.

    The ElectrochemicalSeries

    Most wants to reduce (gainelectrons)

    Gold

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    Gold Mercury

    Silver

    Copper

    Lead

    Nickel

    Cadmium

    Iron

    Zinc

    Aluminum Magnesium

    Sodium

    Potassium

    LithiumMost wants to

    oxidize (loseelectrons)

    Types of Batteries

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    Primary (Nonrechargeable) Batteries

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    Secondary (Rechargeable) Batteries

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    Battery Reactions and Chemistry

    Discharge

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    g Electrode 1 is an anode: the electrode is oxidised, producing

    electrons. Electrode 2 is a cathode: the electrode is reduced, consuming

    electrons.

    In the fully charged state, there is a surplus of electrons on theanode (thus making it negative) and a deficit on the cathode (thusmaking it positive).

    During discharge, electrons therefore flow from the anode to thecathode in the external circuit and a current is produced.

    Therefore in simple terms batteries work as electron pumps in theexternal circuit, preferably with only ionic current flowing throughthe electrolyte.

    If the anode were zinc and the cathode were copper the half

    reactions would proceed as follows:

    At the anode: Zn Zn2+(aq) + 2e Eo = 0.76V

    At the cathode: Cu2+(aq) + 2e Cu Eo = 0.34V

    Thus the total potential for this cell is 1.10 V.

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    us e o a po e a o s ce s 0

    During use as a battery, discharge leads todissolution of Zn at the anode and the

    deposition of Cu at the cathode. Such a cell is embodied in the Daniell Cellintroduced in 1836. As a practical cell thisrequired two electrolytes (typically zinc

    sulphate and copper sulphate aqueoussolutions) to avoid polarisation.The electrolytes are separated from each otherb a salt brid e or a orous membrane which

    ChargeWhen the cell potential is depleted the battery can be recharged.

    When a current is applied to the cell in the opposite direction the

    anode becomes the cathode, and vice versa.Thus electrode 2 that was oxidised upon discharge is now reduced

    and the electrode 1 that was reduced is now oxidised so the

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    electrodes are returned to their former state, ready to be discharged

    again.

    This time the anode would be copper and the cathode would be

    zinc, and the half reactions would proceed as follows:At the anode: Zn2+(aq) + 2e Zn Eo = -0.76VAt the cathode: Cu Cu2+(aq) + 2e Eo = -0.34VThe minimum potential required for charging will be 1.10 V, as this

    is the potential of the cell. In reality much higher potentials will be

    required to overcome the polarisation.

    Lead Acid Battery-An automobile industryapplication

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    In the charged state, each cell contains electrodes of elemental lead (Pb)and Lead (IV) Oxide (PbO

    2) in an electrolyte of approximately 33.5% v/v (4.2

    Molar) sulfuric acid (H2SO

    4).

    In the discharged state both electrodes turn into lead(II) sulfate (PbSO4) and

    the electrolyte loses its dissolved sulfuric acid and becomes primarily water.Due to the freezing point depression of water as the battery discharges

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    Due to the freezing-point depression of water, as the battery dischargesand the concentration of sulfuric acid decreases, the electrolyte is more likely

    to freeze during winter weather.

    The chemical reactions are (discharged to charged):

    Anode (oxidation):

    Cathode (reduction):

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    Electrorefining

    Electro refining of a metal by electrolysis is a wayf ifi ti f t l i l t t d b

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    Electro refining of a metal by electrolysis is a wayof purification of a metal previously extracted byclassical metallurgical or electrochemical processes

    In electro refining, the anodes consist of unrefinedimpure metal, and as the current passes through theacidic electrolyte the anodes are corroded into thesolution so that the electroplating process depositsrefined pure metal onto the cathodes.

    Electrorefining

    In the case of electrorefining of copper, the anode is

    made of impure copper, while cathode is made of a

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    made of impure copper, while cathode is made of athin sheet of pure copper. The electrolyte is an

    aqueous solution of copper sulphate acidified with

    sulphuric acid. The reactions taking place during

    electrolysis are,

    Anode - oxidation: Cu metal (impure)---> Cu+2 + 2 electronsCathode - reduction: Cu+2 + 2 electrons ---> Cu metal (pure)

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    Steps in Electro refining

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    Steps in Electro refining

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    Industrial Applications-Copperrefining

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    Electrorefining of copper

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    Extraction of Aluminium from bauxite-Three stageprocess

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    Refining of aluminium(Hoopes process)

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    Refining of aluminium(Hoopes process)

    The cell consists of an iron tank lined with carbon at thebottom.

    A molten alloy of copper, crude aluminium and silicon is

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    y pp ,used as the anode. It forms the lower most layer in the cell.

    The middle layer consists of molten mixture of fluorides, ofsodium aluminium and barium (cryolite + BaF2).

    The upper most layer consists of molten aluminium. A set of graphite rods dipping in molten aluminium serve as

    cathode. On passing current aluminium ions from the fused electrolyte

    are discharged at cathode and pure aluminium collects as thetop layer. Meanwhile, an equivalent quantity of aluminium from crude

    alloy at the bottom goes into electrolyte in the middle layer.

    Performance evaluation inElectrorefining

    The amount of metal deposited was determined bythe weight change (W) observed in the cathode

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    p ythe weight change (W) observed in the cathodebefore and after electrolysis. The theoreticalamount of metal that can be deposited for the

    quantity of electricity passed during the experimentwas determined

    Using the Faraday's law: whereWm is the theoretical amount of metal deposited,

    the termI t(current time) is the quantity ofelectricity supplied,

    n is the number of electrons transferred in theelementary act of the electrode reaction,

    Am is the atomic weight of the metal and

    Fisthe Faraday constant (96485 Coulombs).

    Current efficiency (eff), which is defined as the

    ratio of the actual amount of metal deposited to thatexpected theoretically , was calculate


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