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4/30/2012
Voltammetry6, 2004
Lecture Date: April 28th, 2008
Reading Material
● Skoog, Holler and Crouch: Ch. 25
● Cazes: Chapter 17
● For those using electroanalyticalchemistry in their work, see:
A. J. Bard and L. R. Faulkner, “ElectrochemicalMethods”, 2nd Ed., Wiley,2001.
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Voltammetry
Voltammetry techniques measure current as a function of applied potential under conditions that promote polarization of a working electrode
Polarography: Invented by J. Heyrovsky (Nobel Prize 1959). Differs from voltammetry in that it employs a dropping mercury electrode (DME) to continuously renew the electrode surface.
Amperometry: current proportional to analyte concentration is monitored at a fixed potential
Polarization
Some electrochemical cells have significant currents.
– Electricity within a cell is carried by ion motion – Whensmall currents are involved,E = IR holds
– R depends on the nature of the solution (next slide) When current in a cell is large, the actual potential usually differs from that calculated at equilibrium
using the Nernst equation
– This difference arises from polarizationeffects
– The difference usually reduces the voltage of a galvanic cell or increases the voltage consumed by an electrolytic cell
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Ohmic Potential and the IR Drop
To create current in a cell, a driving voltage is needed to overcome the resistance of ions to move towards the anode and cathode
This force follows Ohm’s law, and is governed by the resistance of the cell:
Ecell = Eright − Eleft − IR
IR Drop
Electrodes
More on Polarization
Electrodes in cells are polarized over certain current/voltage ranges
“Ideal” polarized electrode: current does not vary with potential
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Overvoltage and Polarization Sources
Overvoltage: the difference between the equilibrium potential and the actual potential
Sources of polarization in cells:
– Concentration polarization: rate of transport to electrode is insufficient to maintain current
– Charge-transfer (kinetic) polarization: magnitude of current is limited by the rate of the electrode reaction(s) (the rate of electron transfer between the reactants and the electrodes)
– Other effects (e.g. adsorption/desorption)
DC Polarography
The first voltammetric technique (first instrument built in 1925)
DCP measures current flowing throughthe dropping mercury electrode (DME) as a function of applied potential
Under the influence of gravity (or otherforces), mercury drops grow from the end of a fine glass capillary until they detach
If an electroactive species is www.drhuang.com/.../polar.doc_files/image008.gif capableof undergoing a redox
process at the DME, then an S-shapedcurrent-potentialtrace (a polarographic wave) is usually observed
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Voltage-Time Signals in Voltammetry
A variable potential excitation signal is applied to the working electrode
Different voltammetric techniques use different waveforms
Many other waveforms are available (even FT techniques are in use)
Linear Sweep Voltammetry
Linear sweep voltammetry (LSV) is performed by applying a linearpotential ramp in the same manner as DCP.
However, with LSV the potential scan rate is usually much faster than with DCP.
Whenthe reduction potential of the analyte is approached, the current begins to flow.
– The current increases in response to the increasing potential.
– However, as the reduction proceeds, a diffusion layer is formed and the rate of the electrode reduction becomes diffusionlimited. At this point the current slowly declines.
The result is the asymmetric peak-shaped I-E curve
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