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1
Introduction
Definitions:
Electrochemistry
Electrochemical Engineering
Challenges
Course Content
Major Applications
History
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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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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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Challenges
No much cover on other courses
Chemistry
ThermodynamicsPhysical chemistry
Electrochemical systems are different
Break any myths about electrochemical systems
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Course Content
Basic concepts
Thermodynamics
Electrode kinetics Transport mechanisms
Modeling
Applications
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Applications
Production of Al and Cl
Corrosion
Batteries and Fuel Cells Electroplating
Cathodic protection
Super capacitors
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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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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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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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History
The formal synthesis of electrochemistry andengineering began in 1950s
Norbert Ibl in SwitzerlandCharles Tobias in US
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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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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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Electrochemical Cells
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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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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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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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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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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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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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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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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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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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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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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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Current efficiency
For electrolytic process
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Current efficiency
For galvanic process, known as faradays efficiency
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Voltage efficiency
For electrolytic process:
For galvanic process:
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Energy efficiency
Product of the current and voltage efficiencies:
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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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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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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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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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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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Units Reminder
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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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Procedure continued
Calculate current density
Since the field is proportional to the negative of thepotential gradient, the conductivity can becalculated
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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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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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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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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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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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Effect of Temperature onionic conductivity
As a general rule ionic conductivity increases withincreasing temperature
Rule of thumbs:
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Problem
What would be the conductivity of KCl at 60 oC?
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Transference number
Represents the fraction of current carried by aspecified ion in the absence of concentrationgradients
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Useful Expression
Combining Eqs 18 and 14:
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Transference number
The fractional current carried by each species mustadd up to the total current, then
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Transference number
For a binary electrolyte
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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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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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Outline
Cell thermodynamics
Temperature and Pressure effects
Nernst Equation Pourbaix Diagram
Equilibrium constant
Reversible heat transfer
Thermodynamics of Electrochemical Systems
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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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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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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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Cell thermodynamics
For a reversible change at constant temperature, theheat transferred is given by
S: change in entropy
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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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Cell thermodynamics
Combining Eqs. 1 to 4:
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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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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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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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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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Cell thermodynamics
Substituting Eq. 10 into 11:
Dividing by F and simplifying:
Eq. 13 is ALWAYS TRUE
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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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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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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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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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Temperature Effect
Consider a reversible process were only mechanicalwork is permitted, then the first law is
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Temperature Effect
The enthalpy is defined by
A differential change in enthalpy is given by
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Temperature Effect
The Gibbs free energy is defined by
A differential change in Gibbs free energy is givenby
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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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Temperature Effect
At constant pressure Eq. 19 becomes:
Substituting Eq. 10 into Eq. 21 yields:
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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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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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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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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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Pressure Effect
Substituting Eq. 10 into Eq. 24 yields:
At low pressure the ideal gas assumption is valid,then:
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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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Exercise 3
Calculate the reversible potential of the celldescribed in Exercise 2 at 3 atm
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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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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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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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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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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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Pourbaix diagram other assumptions
Typical assumptions
Concentrations of ions 10-6 M
Gases at 1 atm
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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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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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Equilibrium Constant
Since the potential is zero at equilibrium, we candetermine the equilibrium constant from thestandard open circuit potential:
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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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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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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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Outline
Interface Role
Electric Double Layer
Helmholtz model Electrode Kinetics Models
Butler-Volmer Equation
Tafel Equation
Reference Electrodes
f l
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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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Interface Role
The surface overpotential is given by:
I ith El t d Ki ti
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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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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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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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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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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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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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Helmholtz Model
For water D10, d10 A, then:
Helmholtz Model
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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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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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Gouy-Chapman Model
The capacitance is given by
Gouy-Chapman Model
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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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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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Stern Model
Because the capacitances are in series thecapacitance of the double layer is given by:
Stern Model
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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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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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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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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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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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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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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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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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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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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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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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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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We can redefine the reaction constant including theactivation energy at our reference potential:
Electrode Kinetics
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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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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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If we designate the equilibrium potential as 0
Taking the logarithm of Eq. 15 and rearranging:
Electrode Kinetics
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Substituting Eq. 16 into Eq. 14 and using thedefinition of overpotential:
Electrode Kinetics
Rearranging Eq. 17:
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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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Substituting the kinetic constants into Eq. 18 weobtain:
Butler-Volmer Equation
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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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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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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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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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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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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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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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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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Solve problem 3 of chapter 5 in your text book
Example 2
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Solve problem 2 of chapter 5 in your text book
Reference Electrodes
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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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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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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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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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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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Accounting for all the limitations the potential lossis given by:
Where:
Contributions tothe Potential in Galvanic Cells
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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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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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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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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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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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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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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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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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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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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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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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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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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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It is used in acid solution
When chloride contamination is not allowed
The reactions if given by:
Mercury/Mercuric oxideelectrode
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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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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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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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Fundamental relationships
Mass transport boundary layer
Concentration Overpotential
Limiting Current Density
Fundamental Relationships
A general description of an electrochemical system
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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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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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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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Current will arise from the motion of the chargesand is given by:
Material Balance
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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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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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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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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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Another important definition is the transport
number:
When concentration variations are important,ohms law becomes modified ohms law:
Common Simplifications
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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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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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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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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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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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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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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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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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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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For an anodic reaction, the concentrationoverpotential is positive and can be estimated (forlarge conductivities) by:
Limiting current
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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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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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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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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,
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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