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Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

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Electrochemical Techniques for Corrosion Measurements
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Page 1: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Electrochemical Techniques for Corrosion Measurements

Page 2: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Assignment

• Present a critical examination of the proposed mechanisms of CO2 and H2S corrosion with particular emphasis on the cathodic (oxidation) reactions.

• Due Date 5 June 2009

Page 3: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

3

Corrosion MeasurementsInvolve the use of a potentiostat for applying a potential (relative to a reference electrode) and measuring the current (flowing from the working electrode to the counter or auxiliary electrode)

*ensure specimen potential (w.r.t. counter) constant … even though solution resistance might alter.

Page 4: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

The Manual PotentiostatVariable High Voltage Source 50-300 V

High Impedance Voltmeter 1012 Ω

Auxiliary Electrode

Working Electrode

Reference Electrode

Ammeter (current)

Page 5: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Electrochemical Impedance Spectroscopy

• Resistance• Ohms Law

• For a resistor, R, it follows Ohm’s Law at all current and voltage levels

• The resistance value is independent of frequency• AC current and voltage signals through a resistor are in phase

with each other

I

ER

Page 6: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Electrochemical Impedance Spectroscopy

• Impedance• Impedance applies to AC voltage and current• Like resistance impedance is a measure of the ability of a

circuit to resist the flow of electrical current• The excitation potential or AC voltage can be expressed as a

function of time

frequency radial the voltage the of amplitude the

t time at potential 0

0

EE

tEE

t

t sin

Page 7: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Electrochemical Impedance Spectroscopy

• The relationship between radial frequency ω (radians s-1) and frequency (f) hertz is:

• The response to the AC voltage is given by:

shift phase the current the of amplitude the

current response 0

0

II

tII

t

t sin

f 2

Page 8: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Electrochemical Impedance Spectroscopy

• Similar to Ohm’s law

• The important point to remember is that when an AC voltage is applied to a pure capacitor the resulting AC current is shifted in phase by 90o

• There is no phase shift for a pure resistor

t

tZ

tI

tE

I

EZ

t

t

sin

sin

sin

sin0

0

0

Page 9: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Electrochemical Impedance SpectroscopyCurrent phase shift due to impedance. Through a capacitor this phase shift is 90o

Applied Voltage

Resulting Current

Page 10: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Electrochemical Impedance Spectroscopy• Randles circuit for a simple corroding system

• Rs = the solution resistance

• Rct = the charger transfer (polarisation resistance)

• Cdl = the double layer capacitance

Page 11: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Electrochemical Impedance Spectroscopy• Nyquist plot for the Randels circuit

Resistance

Capacitance ← Increasing Frequency

Solution Resistance

Charge transfer resistance = Rtotal - Rs

Page 12: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

EIS Nyquist Plots• A Nyquist plot is made up of a series of vectors representing

the total magnitude of the resistance and capacitance components

Phase angle

Non Resistive Component

Page 13: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Electrochemical Impedance Spectroscopy• Bode impedance plot

Impedance

Frequency →

Solution resistance

Rct

Page 14: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Electrochemical Impedance Spectroscopy• Bode Phase plot

Frequency →

Phase angle

Page 15: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

EIS (Summary)

We start here at the high frequency

Page 16: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

EIS

• Diffusion or Mass Transfer controlled process• Nyquist plot - Warburg Impedance

←Frequency

Page 17: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

EIS• Diffusion or Mass Transfer controlled process• Bode Impedance plot

Impedance

Frequency →

Page 18: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

EIS• Diffusion or Mass Transfer controlled process• Bode Phase plot

Phase Angle

Frequency →

Page 19: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

EIS – Mass Transfer Controlled Process (Summary)

NyquistBode Impedance

Bode Phase

Page 20: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

EIS Equivalent Circuit for a Mixed Kinetic and Charge Transfer Controlled Process

Page 21: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

EIS Bode Plots for the Mixed Controlled Reaction

Impedance

Phase

Page 22: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

EIS Equivalent Circuit for a Filmed Corroding Surface (E.g. Failed Coating)

Page 23: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

EIS for a Filmed Corroding Surface (E.g. Failed Coating)

Nyquist

Bode Impedance (Magnitude

Bode Phase Angle

Page 24: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Linear Polarization Method Valid for corrosion under activation control.Involves applying a small perturbation to the potential around Ecorr (i.e., ± ∆E ≈ 10 mV).

Slope of summed curve (measure E vs i for system) is difference between slopes of curves for the coupled reactions: Sa - Sc

N.B. ∆i for summed curve = ia + |∆ic| (∆ia=x)

Page 25: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

The curves are ~linear within ~20mV – Sa and Sc are constant. For ∆E around Ecorr, Sa and Sc are related to icorr (the required quantity): assuming the high-field approximation for the individual reactions

Now:

Polarization Resistance .. .. is measured. The Tafel coefficient ba and bc must be known.

corr

aa

anodic i

bS

di

dE

303.2

corr

cc

redox i

bS

di

dE

303.2

i

E

E

i

bb

bbi

ca

cacorr

303.2

1or

x

ESa

slope slope

xi

ESc

ca

ca

SS

SS

i

E

Page 26: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

26

Remember: during linear polarization measurements we plot E vs i (not log i) around the corrosion potential:

i

E

= polarization resistance

Page 27: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Linear Polarization• This involves the application of low over-potentials and

therefore the currents are relatively very small. This means that the charging current (capacitance current) can make a significant contribution to the noise or background current.

• Use slow scan rates and perform a cyclic scan to check whether you are measuring capacitance.

• The reverse scan should produce an iE curve that retraces over the forward recorded iE curve.

• The iE curve can be curved due to a difference in the anodic and cathodic Tafel slopes.

Page 28: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Linear Polarization• It is important to view the iE curve. If the iE curve is

curved, the polarization resistance can be obtained by drawing a line that is tangential to the curve at Ecorr and at zero current.

• Some portable instruments use a potential-step method. In this case the current, at, for example, -10 mV and +10 mV is measured and Rp is computed from these measurements.

• The advantage of this technique is that the current measurements are made at a constant voltage and therefore the charging current is zero.

• The disadvantage is that no iE curve is recorded and therefore an error can be introduced if there is curvature in the iE graph

Page 29: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Linear Polarization• The portable instruments that use the potential-step

technique, usually apply a high frequency AC signal before the measurement to determine the solution resistance and subtract this value from the measured polarization resistance.

Page 30: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Tafel Extrapolation

Page 31: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Tafel Method We can only measure the net current across the specimen electrode – at the corrosion potential there is no net current (only local anode – cathode currents which constitute the corrosion current). We cannot measure corrosion rate directly, though we need icorr.

Measure potential and current at some distance on either side of Ecorr – extrapolate E - log i curves (in same quadrant) back to Ecorr …

Plot of the total current (iT = io + ic) versus potential showing the extrapolation of the Tafel regions to the corrosion potential, Ecorr, to yield the corrosion current, icorr.

Page 32: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

PassivationUnder certain conditions of potential and pH, some metals form protective films, i.e., they passivate

Pourbaix diagram for the iron/water/dissolved oxygen system showing the effect of potential in moving the system from a corrosive (active) region (point 1) to a passive region (point 2)We can exam the kinetics using a potentiodynamic scan and Evans diagram

Page 33: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

33

The polarization curve for the anodic reaction of a passivating metal drawn for potentials more noble than the equilibrium potential (Ee)a

Oxidative dissolution of oxide (e.g., Cr2O3 CrO4

2-)

(Ee)M/MO is the equilibrium potential for oxide/hydroxide formation

Tafel region(icrit is min. reaction rate required to initiate film growth by precipitation of Mn+)

The region attained by the metal in a given environment depends upon the cathodic reaction i.e., where the cathodic curve cuts the above anodic curve.

“Flade”

Page 34: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Tafel Extrapolation Technique• Involves measurements at high over-potential in

which logi is recorded. • The best method of performing these measurements

is by : • 1) Using two identical electrodes and recording the

anodic curve on one electrode and the cathodic curve on the other electrode. In each case starting at the open circuit potential Eoc (or Ecorr)

• 2) Performing the cathodic curve on one electrode starting the scan from Eoc. Turning off the potentiostat and monitoring Eoc until it returns to its original value. The anodic scan is then recorded again starting at the Eoc.

Page 35: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Tafel Extrapolation Technique• Before commencing a Tafel measurement, it is

generally best to allow your metal electrode to reach a steady state potential. This can be observed by performing a potential time measurement in which Ecorr is monitored with time.

• Scan Rates are normally in the range of 0.1 mV to 5.0 mV per second. The cathodic plot is scanned to an over-potential of about 400 mV.

• Anodic potentials can be scanned much higher depending on what information needs to be obtained.

Page 36: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Cyclic Pitting Scans• The technique is used to evaluate the susceptibility

of metals to pitting corrosion in a particular environment. It is applicable to metals such as stainless steels, high nickel alloys and aluminium, which form a passive protective film.

• With this technique, the potential is scanned to voltages in the transpassive region.

• Exceeding the passive region is indicated by a sudden increase in current. At this stage the voltage scan is reversed, usually when the current reaches a certain current density (0.5 mA cm-2)

Page 37: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Cyclic Pitting Scans• The extent of the hysteresis in the reverse scan is an

indication of the susceptibility to pitting corrosion. • Pitting corrosion is considered to stop at the potential where

the iE curve from the reverse scan crosses the iE curve of the forward scan.

• The sudden increase in current can be due to three processes:• 1) Onset of pitting corrosion • 2) Trans-passive uniform corrosion• 3) The oxygen evolution reaction • In the case of trans-passive corrosion, the slope of the iE

curve is not as steep compared to pitting corrosion and oxygen evolution.

• In the case of oxygen corrosion, the reverse iE curve normally will retrace over the forward iE curve.

Page 38: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Harmonic Analysis• Butler Volmer Equation

• When an electrode is polarized near the corrosion potential by a sinusoidal voltage of frequency ω and amplitude U0, then the current density of the Faradaic process is given by:

Page 39: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Harmonic Analysis• The current densities of the Faradaic process will

have a distorted sinusoidal form due to the non-linear nature of the cathodic and anodic partial processes in a polarization curve.

• The amplitudes of the harmonic components can be obtained by Fourier series expansion of the exponential terms

Page 40: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Harmonic AnalysisThe simplified magnitude of the first three harmonic components are given by:

Page 41: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Harmonic Analysis• The technique has been verified by the work of Will Durnie,

Curtin University. • He compared corrosion rates from HA with those obtained

using linear polarization measurements and Stern Geary equation.

• When the Tafel slopes obtained from HA were placed in the Stern Geary equation an excellent correlation was obtained.

Page 42: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Harmonic Analysis

Durnie, W. H.,Curtin University

Page 43: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Electrochemical Noise (ECN)• ECN measures the current/voltage response between two

(largely) identical electrodes. • The two electrodes are coupled together (short circuited

together) through a zero resistance ammeter (ZRA).• The random fluctuations of current is measure by the ZRA.• At the same time the random fluctuations in voltage noise at

the coupled electrodes is measured with respect to a reference electrode.

Page 44: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Electrochemical Noise Measurement

A

Working Electrode 2Working Electrode 1

Zero Resistance Ammeter

V

Reference Electrode

Page 45: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Rotating dual cylinder electrode (RDCE)

• Standard electrochemical cell with reference, auxiliary and RDCE

• The RDCE is useful for performing ECN Measurements

• ECN uses identical electrodes. In the example shown the electrode areas are not the same since this RDCE was used to investigate preferential weld corrosion

Page 46: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Potential Noise and Current Noise

Page 47: Lecture 10 Electrochemical Techniques for Corrosion Measurements 2

Voltage Noise PSD

1.E-15

1.E-12

1.E-09

1.E-06

1.E-03

1.E-04 1.E-03 1.E-02 1.E-01 1.E+00Frequency/Hz

Vo

lta

ge

PS

D /

V2

/Hz

3.5 days


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