21
1 Electro-Analytical Techniques Dynamic Review: Potentiometric methods measure the potentials at electrodes by a suitable coupling with a reference electrode; as a potential difference E (E cell ). At the electrode the redox reaction has reached equilibrium. Under such a situation there is no net transfer of charge (current) across the electrode interface. Thus as the measurement is made very little or no current drawn by the measuring device (potentiometer). Example (electrode): Pt/Sn +2 (a Sn+2+, ), Sn +4 (a Sn+4+ ) E el Sn +4 + 2e = Sn +2 The concentrations at the electrode surface are nearly the same as that in the bulk solution. Electrochemistry in Stirred Solutions Disturbing the equilibrium (drives a reaction): Pt/Sn +2 (a Sn+2+, ), Sn +4 (a Sn+4+ ) E <E el (E sufficiently negative) Sn +4 + 2e Sn +2 The concentrations at the electrode surface are different from that in the bulk solution – polarization. Working electrode (WE) Electrode at which reaction of interest occur. Metal electrodes are generally polarizable. To make them non-polarized, stir the solution so that the concentration at the surface is the same as in the bulk. Reference electrodes are generally non-polarizable. Current is a measure of the reaction rate at the electrode(s). Charge is a measure of the extent of the reaction occurred at the electrode(s).

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Electro-Analytical Techniques

Dynamic

Review:

Potentiometric methods measure the potentials atelectrodes by a suitable coupling with a referenceelectrode; as a potential difference E (Ecell).

At the electrode the redox reaction has reached equilibrium. Under such a situation there is no net transfer of charge (current) across the electrode interface.

Thus as the measurement is made very little or no current drawn by the measuring device (potentiometer).

Example (electrode):

Pt/Sn+2(aSn+2+,), Sn+4(aSn+4+) Eel

Sn+4 + 2e = Sn+2

The concentrations at theelectrode surface are nearlythe same as that in thebulk solution.

Electrochemistry in Stirred Solutions

Disturbing the equilibrium (drives a reaction):

Pt/Sn+2(aSn+2+,), Sn+4(aSn+4+) E <Eel (E sufficientlynegative)

Sn+4 + 2e → Sn+2

The concentrations at theelectrode surface are different from that in thebulk solution – polarization.

Working electrode (WE)Electrode at which reaction ofinterest occur.

Metal electrodes are generally polarizable.

To make them non-polarized, stir the solution so that the concentration at the surface is the same as in the bulk.

Reference electrodes are generally non-polarizable.

Current is a measure of the reaction rate at the electrode(s).

Charge is a measure of the extent of the reactionoccurred at the electrode(s).

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Application of a potential sufficiently different from theequilibrium potential would drive the half reactionin one direction. This would lead to a flow of charge (electrons) i.e. a current, i.

And quantity of charge q = it; t = time; i is held constant;

More precisely;0

t

q idt

Moles of material electro-generated; 0

t

idtq

nF nF

dqi =

dt

0

t

q idt Cur

rent

, I.a

mp

However, potential at a single electrode cannotbe changed solitarily, two electrodes are required.

The second electrode –Auxiliary (or counter) electrode.

A redox reaction (complementary) would occur at thecounter electrode simultaneously.

power source

Cu = Cu+2 + 2e½ O2 + 2H+ + 2e = H2O

The spontaneousreaction propensity is measured by Ecell;

Electro-deposition of Copper.

Non-spontaneous process.

The energy required toeffect the reactionis drawn from the external power source.

power source

Vapp

i

Cu+2 + 2e → Cu H2O →½ O2 + 2H+ + 2e

ElectrolysisNote: electrolysis is not an equilibrium situation.

1. Redox reaction occur at the electrode interfaces,interchange of electrons occur. The reaction is ‘forced’; it is a energetically uphill, non-spontaneousprocess.

2. Oxidation reaction occur at the anode,

3. Reduction reaction occur at the cathode,

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Minimal applied potential (difference) requiredto effect Electrolysis.

a. Reduction; Cu+2 + 2e → Cu

Cu

Cu+2+2e

Overcoming activation energy requires input of energy.Achieved by increasing the negativeness of the cathode. i.e. Eapp,cathode < Eeq.cathode

Cu

Cu+2+2e

b. Oxidation; H2O →½ O2 + 2H+ + 2e

½O2+2H++2e

H2O

To overcome the activation energy required an input of energy, increasing the positivity of the anode. Eapp,anode > Eeq.anode

H2O

½ O2+2H++2e

Vapp= Eapp,anode – Eapp,cathode > Ecell just to start electrolysis

Vapp – Ecell = Cell overvoltage

In addition, to drive a current the resistance of the cell must be overcome as well; IR drop,Ohmic potential.

Further, the depletion of material at the electrodeswould require the movement of material from thebulk of the solution (diffusion – if solution is unstirred) and that involves some energy as well -concentration overpotential.

Vapp = Ecathode – Eanode + overpotentials + iR Equilibrium potential

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Totalcurrent

Faradaic Current(difference)

Equilibrium potential

overpotentials

iR

i –V Plot, stirred solutions Eapp = Ecathode – Eanode + overpotentials + iR

cath

od

ica

no

dic

E0

Eapp

(-)

Cat

hodi

c cu

rren

t

Anodic current

E0

Neg

ativ

e po

tent

ial i

ncre

asin

g

Ele

ctro

n E

nerg

y in

crea

sing

LUMOHOMOo o

e-

orM+ MM M+

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How the applied potential difference distributes itselfbetween the two electrodes is harder to decipher.

Often it is necessary to find the actual potentialon the working electrode.

The working electrode is the electrode in an electrochemical system on which the reaction of interest is occurring.

Strategy – three electrode cell.

Controlled potential analysis

Three electrode cell

workingelectrode

Very small gap, low resistance

Electrogravimetric Analysis

This method employs an electric current to deposit a solid on an electrode from a solution.

Two or three electrode circuitused, either a constant current or a constant potential is applied to the pre-weighed working electrode

Basis: Faraday’s Laws of electrolysis.

mass deposited

Molar massmoles

begining

end

Coulometry:

Coulometry determines the unknown concentration of an analyte in solution by completely converting the analyte from one oxidation state to another.

Coulometry is an absolute measurement similar to gravimetry or titrimetry and requires no chemical standards or calibration.

Useful for determining absolute concentration of standards.

Basis: Faraday’s Laws of electrolysis.

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Coulometry

0

t

idtq

nF nF

Coulombs ofcharge measured

dqi =

dt

Amperometry: Constant potential mode

In amperometric experiments the potential of the indicator electrode(s) is adjusted to a value so that redox processes could occur (stirred solutions).

The current flowing between the indicator electrode and a second electrode in the solution is measured.

There is a minimum potential required to initiate anoxidation or reduction reaction at an electrode.

To effect a net Faradaic process the magnitude of the applied potential must be sufficiently higher in magnitude than the minimum equilibrium potential.

Faradaic current proportional to the concentrationof the species undergoing transformation (redox).

+O

OH

HH

OH

H

OH

H OH

H

OH

Fe

1

+O

HH

OH

HOH

H OH

OH

O Fe

1

+ 2H+

+

2 2glucose oxidase

H2O2

Fe

1

Fe

1

+

+

eAt WE:

mediator

A standard curve of current as a function of concentration of a series of standard solutions is prepared, and the concentration of the analyte is determined from the curve.

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Amperometry is also used to locate the end point in amperometric titration curves; a plot of current as a function of titrant volume.

The shape of the curve varies depending on the chemical species (titrant, analyte, products) that are electroactive and the reversibility of the redox couple.

The plot consists of linear and nonlinear regions before and after the end point and are extrapolated to intersect at the end point.

Some information from unstirred solutionsmay be used to design amperometricexperiments.

Convention (i – V plots) (polarographic):

Y- axis: Cathodic currents positive direction (up)X- axis: Negative potential increases to the right

(-)(+)Stronger oxidant Stronger reductant

Eapp vs Eref

i cath

odic

i ano

dic

i-V plots for unstirred solutions are generally plottedfor analytes. Such plots contains the unique redox characteristic (potential) of the redox couple; i = steadycurrent and every point here is from a ‘new experiment’.

diffusion current

E1/2

For stirred solutions the current is directly related to the concentration. i

Vtit

T + X →T’ + X’i

Vtit

i

Vtit

i

Vtit

Amperometric Titrations;single polarizableelectrode – RE;combination.

E

E

id

E

id

E

id

id

X*

X*

T*

T*

T*

0 T

T

X

X

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i

Vtit

i

VtitT + X →T’ + X’

Amperometric Titrations;dual polarizableelectrodes

i

Vtit

X *, X’ *

X *, X’ *

T *, T’ *

T *, T’ *

Reversibleelectroactive

Coulometry

q = i t

Coulometric determination with amperometric detection.

Constant current mode.

Amperometric detection.

Detector circuit

Coulometry: Determine

Br2

Br

Br

→+

2Br- → Br2 +2e

2_2

itmoles Br

F

Reagent electrolytically generated,q for reagent generation measured. CV

Detector circuit

Coulometry:Constant current amperometric detection mode

Eg. Ascorbic acid + I2

Electrochemicallygenerated or added I2 in solution.

Monitor voltage required to maintain a constant current. Voltage drops once unreacted I2 start accumulating in solution.

Volume, std I2

CCDetector circuit

Analysis of water is based on the quantitative reactionB = base;

2B + I2 +B•SO2 + H2O 2BH+I- + BSO3

BSO3 + ROH BH+ R-OSO3-

Karl Fisher Titration; water determination

I2 generated electrochemically via (i); 2I- I2 + 2e

2 2

2

1 1 2

moles 2

mol I mol H O F

itH O

F

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B, ROH, SO2,solvent, KI

i

2I- I2 + 2eI2 + 2e 2I-

2I- I2 + 2e

AUX

WE

Detector circuit

CH3OH +SO2 + RN [RNH]+[SO3CH3]-

2RN + I2+ [RNH]+[SO3CH3]- + H2O 2[RNH+]I-+ [RNH]+[SO4CH3]-

Bases: imidazole, diethanolamine

Alcohols: methanol, diethylene glycol monomethyl ether

Organic solvent: chloroform, methanol, carbon tetrachloride, formamide, ..

Rotating Electrode:

Electrode reactions performed at electrodes in stirred solutions can be driven to completion. The total charge involved in such work is related to the amount of electro-active materials oxidized or reduced. The process requires a considerable time.(coulometry).

If the current is not maintained for a considerable time and/or the current is very small the change in concentration due to electrode reaction is negligible. At such situations the instantaneous current is proportional to the concentration of the material undergoing the transformation (amperometry).

Voltammetry

In voltammetry the current is measured as a function of a varying applied potential at an electrode.

There is a minimum potential required to initiate anoxidation or reduction reaction at an electrode.

Voltammetry is carried out in three electrodesystems so that the potential applied to theworking electrode can be accurately measured.

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Three electrode cell

Background current (Ohms Law)or Residual current

Faradaic currentCharging current

Unstirred solutions

The structure of the electrode solution interface:Concentration profile (in solution)

voltage-ve

time

V2

V1

(-)

Con

cent

ratio

n

x

A + ne → R

Application of a sufficiently negative potential initiates a reduction reaction at the surface.

Oxidized material [A] is removed by the reaction thus it’s concentration near the surface drops.

Further, a more negative the potential depletion rateis higher further decreasing the concentration at the surface in a shorter time.

Concentration gradients are created and at a certain of the applied potential and beyond the concentration at the surface will be almost zero –steady state.

Concentration profile

highestconcentration gradient

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Concentration profile (in solution)

Con

cent

ratio

n

steady state

time

t=0

voltage-ve

time

V2

V1

Electron transfer reaction rate at surface imeasured.

Reaction rate at the interface is directly related to thefaradaic current, i.

A+(surface) + e → A Faradaic current***

The overall electrode reaction rate at steady state;

A+(bulk) → A+(surface) → Aslow fast

i ~ rate determining slow step (diffusion rate)

In general i increases with the magnitude of the applied potential, maximum i is a limiting value !!

+ediffusion

Slow step (mass transfer step):

1. *MigrationMovement of ions in an electric field. Contributionto migration by analyte of interest, minimized by adding a supporting electrolyte to the test solution.

2. *ConvectionMovement of bulk solution to the surface due to thermal motion and stirring; is eliminated by using quiescent conditions (no stirring during measurement and constant temperature)

3. DiffusionMovement of analyte due to the concentration gradient in the solution.

* Not uniform – can be made to disappear functionally.

0A A A

d A A

C C Ci i nFAD nFAD

x

Highest at the limiting current (diffusion current, id).

Any further increase of potential (negatively) does not increase diffusion current.

Convention: Cathodic currents positive

0

A AC C

Voltammogram

V (-)

t

id

curr

ent

Linear sweep voltammetry

electrochemical reaction

Background – Ohm’s Law

The diffusion current is found by the difference between the current plateau (average) and a linear extension of the low potential response.

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00

0

Diffusion Current,

( )

at steady state because 0 at the diffusion limit.

d

A Ad A A A A A A

A

i

C Ci nFAD k C C k C

C

Note: backgroundneglected.

Characteristic ofhalf reaction;Half wave potential Eo

Heyrovsky-Ilkovic Equation

i

id

Heyrovsky-Ilkovic Equation

dappl 1/2

i iRTE E ln

nF i

Upon rearrangement;

1/2

1/

dp

2

ap l

allows determination of

nF nF

n experimentally for

reversible sy

iE

RT RT

i

iln

i

nterceptE

slop

stems!!!

E

e

0<α<1 and α=1, for reversible redox system

Sigmoid !

Note: oxidation reaction!!

IUPAC convention

+2

Electrochemical reaction at the surfaces is an interfacial phenomenon. It’s highly dependent of the surface characteristics of the surfaces involved.

Any changes at the surface changes the i vs V curves.

The surface needs refreshing frequently.

It is achieved by employing the dropping Hg electrode.

A new Hg drop is created periodically and the reaction done on a fresh surface (Polarography).and high over-potential of Hg allows use of larger negative limit of applied potential.

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Polarography

http://www.youtube.com/watch?v=C8CM7d5e5Vg

Complications:Spiky nature of the signal ~ noise.Restructuring of charged species and moleculesat the interface, each time a new surface is created.

Ilkovic Equation

1/ 2 2/3 1/ 6706d A Ai nD m t C

Ilkovic Equation

n = number of electrons DA = Diffusion coefficient cm2/s m = flow rate of mercury mg/s CA = conc. mM t = time

Polarogram (voltammogram - dropping Hg electrode)

noisy signal

A single voltammogram can quantify many species if sufficient separation between waves.

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Polarographic experiments on a given surfacecan be done only within a potential range.

At positive limit, oxidation of water2H2O→4H+ +O2(g) + 4e-

At negative limit, reduction of water2H2O+ 2e- →H2 + 2OH-

Problems with dissolved O2 - must purge solutionsof dissolved O2.

Useful media/voltage ranges

imeasured = ifaradaic + icharging

useful analytical component

Useless, contributesto the background.

Minimize as much aspossible.

Advantages of DME(as opposed to stationary electrodes):

a. clean surface generatedb. rapid constant current achievement at drop growthc. remixing of solution when drop fallsd. high Hg overvoltage means even metals with high

-ve E0 systems can be studied without H2 formatione. amalgam formation more favorable vs. metal (s)

http://www.youtube.com/watch?v=C8CM7d5e5Vg

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Disadvantages of DME

a. Hg easily oxidized, limited use as an anode (E = 0.25V vs SCE)

2Hg + 2Cl- →Hg2Cl4-2+ 2e-

b. non-faradaic residual currents limit detection >10-5 Mc. cumbersome to use (toxic mercury)d. sometimes produce a current maxima for unclear

reasons (use maxima suppressor)

Sampled current polarography:

1. Unstirred solutions2. Create a drop (r = constant const. elect. area)3. Apply a ‘new’ potential (E ) (i = ifaradaic + icharging)4. Delay for a time5. Measure current (i = ifaradaic)6. Release the drop7. Repeat 2-6.

Current vs time

Con

cent

ratio

n

steady state

time

t=0

voltage-ve

time

V2

V1

time

‘i’Faradaic, iF

Charging, iC

E

itotal= iF+iC

iD

Faradaic Current vs. time

Cottrell Equation

| |

bulk

bulk

nFA Di C

C Concentration of ion in solution

A electrode area (not time varying)

t

drops faster with time!!!Note the absence of noisy character of the signal.

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Pulsed Voltammetric Techniques:

Pulsed techniques takes advantage of the difference in the rate of the decay of the charging and the Faradaic currents following a potential step (pulse).

The charging current decays exponentially, whereas the Faradaic current (for a diffusion-controlled current) decays as a function of 1/t.

The charging current is negligible with 5 times the time constant of decay. The measured current is predominantly Faradaic current.

Normal Pulse Voltammetry:

The potential wave form; a series of pulses of increasing amplitude, potential returning to the initial value after each pulse (unstirred).

Excitation Potential

Excitation Potential

Re-dox processes with E1/2 difference of ~0.2V resolvable.

Differential Pulse Voltammetry:

Excitation Potential

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Differential Pulse Voltammetry:

The potential wave form; small pulses (constant amplitude) superimposed upon a staircase wave. Current is sampled twice in each pulse period; before the pulse, and at the end of the pulse. The difference between these two current values is recorded and displayed.

Detection Limit: 10-7 – 10-8M.

Excitation Potential

ip

ip C

E1/2

Square-Wave Voltammetry:

if

ir

≥5msExcitation Potential

cathodic

anodic

if

ir

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Square-Wave Voltammetry:

The potential wave form; a square wave of constant amplitude superimposed on a staircase wave form.

The current is measured at the end of each half-cycle. The current measured on the reverse half-cycle (ir)and subtracted from the current measured on the forward half-cycle (if).

This difference current (if - ir) is displayed as a function of the applied potential. Same drop.

For a reduction process, with potential well positive of the redox potential, both the forward and reverse currents are zero, so the difference current is also zero.

At potentials well negative of the redox potential, the current is diffusion-controlled, and the potential pulse has no effect; hence, the forward and reverse currents are equal, and the difference current is again zero.

The largest difference between the forward and reverse currents (and hence the largest current response) is at the redox potential.

Advantages to measuring the difference current.

1. Increase of the discrimination of the charging current, since any residual charging current is subtracted out.

2. The output of the current response is a symmetric peak, rather than the sigmoidal curve typically found for normal pulse voltammetry.

3. Easy resolution of peaks; E1/2 difference of ~0.05Vresolvable.

Anodic Stripping Voltammetry

In ASV, a mercury electrode is held at a sufficientlynegative potential to reduce metal ions in solution and form an amalgam with the electrode.

The solution is stirred to during deposition of the analytes (metal) referred to as pre- concentration step.The reduced metals form amalgam with mercury.

After reducing and accumulating the analyte for some period of time, td, allow a quiescence time and change the potential on the electrode (increase) to re-oxidizethe analyte and generate a current signal; in NPV,DPV or SWV ramps.

l dA

Hg

i tC

nFV

CA = concentration of analyte on ‘deposit’il = limiting current at depositiontd = time of depositionn =number of electrons for reductionF = Faraday constantVHg = volume of mercury (in the electrode)

The re-oxidizing (stripping) current CA CA,solution

Primary advantage of ASV is the pre-concentrationstep of the analyte which allows to enhance output signal (Detection limit 10-10 M).

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Cyclic Voltammetry:

A triangular waveform applied to the WE.

Linear wave forms used are increased and decreasedin either anodic or cathodic fashion.

Eg.

foward

reverse

foward

reverse

Excitation Potential

Excitation Potential Current – Potential Response

reduction

-ve

drop – due to depletion of analytediffusion too slow

Di nFAc ; Cottrell Equation

t

cpE

, t

oxidation

8 3/ 2 1/ 2 1/ 22.69 10pci n ACD

ipc = peak limiting current AA = area of electrode m2

n =number of electrons for reductionC = concentration of analyte mol/LD= Diffusion coefficient m2/s = sweep rate V/s

Cyclic Voltammogram ofa reversible redox system.

Epa

Epc

59.0pa pc

RT mVE E

nF n

A ne B

1pc

pa

i

i

1/2 2pa pcE E

E

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reversible

Irreversible(not totally)

http://www.ovguide.com/fullerene-9202a8c04000641f8000000000016cb8

Electrochemical detectors

The mobile phase is flowing past the electrodes, the solvent will be continuously replaced as the peak passes through the detector.

The electrochemical detector responds to substances that are either oxidizable or reducible. The detector normally has three electrodes, the working electrode (oxidation/reduction occur), the auxiliary electrode and the reference electrode). The electrical output results from an electron flow caused by the chemical reaction that takes place at the surface of the electrodes.

Reference electrode downstream

There are two modes of operation in electrochemical detection;coulometric detection and amperometric detection.

Coulometric detection: If the reaction at the electrode surface exhausts all the reactant and the current becomes zero, the total charge that passes will be proportional to the mass of solute detected.

Amperometric detection: While there is solute present between the electrodes, a current will be maintained (albeit varying in magnitude).

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Derivatizing of samples has become vitally important in making the analytes conducive for detection.

Derivatization of reactive analytes with redox functional groups for HPLC shows following advantages:

increases analyte stability higher selectivity and sensitivity

Additionally the altered polarity from the functional group may lead to better chromatographic separation.