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TUTORIAL ON ELECTROCHEMICAL IMPEDANCE SPECTROSCOPY

David C. Silverman


Table of Contents

Overview of Tutorial
Overview of EIS
Analysis Using Simple Circuits
Constant Phase Element
Corrosion Rate Estimation
        Two Capacitive Relaxation Time Constants
Critical Criteria for Proper Spectra
Diffusion Impedance
Pseudoinductance

Overview of EIS

Electrochemical impedance spectroscopy (EIS) (sometimes also called AC impedance) is an electrochemical technique in which a low amplitude alternating potential (or current) wave is imposed on top of a DC potential (often the corrosion potential and zero imposed current). As such, this technique is in essence built on DC techniques as shown in this figure . In DC technology, a voltage (or current) is imposed on an electrochemical system and the resulting current (or voltage) is measured. The relationship between the voltage and current is used to make a judgment about the corrosion rate and other corrosion characteristics (link to poltutorial).

EIS adds another level to the analysis. A low amplitude repeating wave of varying frequency is imposed on top of the DC input signal. Usually the wave is a sinusoidal voltage wave but other waveforms have been used. Assuming a sinusoidal input, the resulting output signal is of the same frequency but is shifted in time is shown in this figure . But, using sines and cosines to describe the relationship between input and output is cumbersome. Vector analysis provides a more convenient descriptive method. The equations may be written as follows:
                                                                                 (1)

                                                                        (2)

                                                                        (3)

                                                                        (4)

where V and I are the total voltages and the subscripts 'inphase' and 'outofphase' refer to the real or in phase and imaginary or out of phase contributions to the total signal.

The relationship can be seen in the following figure . A sinusoidal current or voltage can be pictured as a rotating vector with a rotation rate equal to ω radians per second. (AC current rotates at 60 Hz or 377 radians per second. The in phase or real component shown defines the observed voltage or current. It becomes the real component of the rotating vector. The out of phase or imaginary component (usually written with a "j" in front) shown defines the non-observed voltage or current.

The voltage and current can be pictured as similar rotating vectors in the following figure. Assuming the voltage is forcing the current, if current is in-phase with voltage, the vectors are coincident and rotate together. When voltage and current are out of phase, they rotate at the same frequency ω but are separated by a constant angle shift θ, the phase angle. In EIS measurements, one vector is viewed using the other as a frame of reference. Thus, the reference point rotates and the time dependence of the signals (ωt) is not viewed. Both the current and voltage vectors are referred to the same reference frame.

The voltage vector is divided by the current vector to yield the impedance voltage divided by current) as shown in this figure. The mathematical convention for separating the real (x) and imaginary (y) components is as follows:

                                                                                 (5)

                                                                                           (6)

                                                                                                (7)

                                                                                                (8)

                                                                                                                (9)

According to ASTM G-15, the definition of "Electrochemical Impedance" is the frequency dependent, complex valued proportionality factor, ΔE/ΔI, between the applied potential (or current) and the response current (or) potential in an electrochemical cell. This factor becomes the impedance when the perturbation and response are related linearly (the factor value is independent of the perturbation magnitude) and the response is caused only by the perturbation. The value may be related to the corrosion rate when the measurement is made at the corrosion potential. The goal of the EIS technique is to measure the impedance as a function of frequency by proper procedures and then analyze the resulting spectrum to estimate corrosion rates and mechanisms the might give rise to the spectra. Further reading is available in D.C.Silverman, "Primer on the AC Impedance Technique", Electrochemical Techniques for Corrosion Engineering (R. Baboian, ed.), p. 73, NACE, 1987 1    (370k)) ,J. R. Macdonald, 'Impedance Spectroscopy', John Wiley & Sons, NY, 1987 and D. C. Silverman and J. E. Carrico, "Electrochemical Impedance Technique - A Practical Tool For Corrosion Prediction", Corrosion, Vol. 44, No. 5, p. 280 (1988) 1    (517k).




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David C. Silverman, Ph.D. - Primary Consultant
E-Mail:     dcsilverman@argentumsolutions.com
Phone:     314-576-3586
Fax:         314-754-9825
Address:   The Argentum House
                14314 Strawbridge Ct.
                Chesterfield, MO 63017