electrochemical impedance spectroscopy - zivelab started with eis.pdf · may 2012 electrochemical...
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May 2012
Electrochemical Impedance Spectroscopy
Designing the Solution for ElectrochemistryPotentiostat/Galvanostat І Battery Cycler І Fuel Cell Test Station+82-2-578-6516 І [email protected] І www.zivelab.com І www.fctest.com
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• Electrochemical?– In electrochemistry, everything of interest takes place at the interface
between electrode & electrolyte!– Controlling REDOX by Potentiostat/galvanostat
• Impedance?– AC circuit theory describes the response of a circuit to an alternating current
or voltage as a function of frequency– Impedance is a totally complex resistance encountered when a current flows
through a circuit made of resistors, capacitors, or inductors, or any combination of these
– Ohm’s Law, V = R I → V = Z I (complex number Z)
• Spectroscopy?– No Quantum Process– Small Perturbation → Response
Nomenclature : EIS
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Excitations used in E’chem Techniques
1. DC
2. Sweep
3. Pulse
4. Sine
Potentiostatic
CA, CC, CP
LSV, Tafel, PD, LPR CV Cyclic Polarization
PEIS, GEIS
DPV NPVRNPV SWV
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Electrochemical Interfaceand Electrochemical Process
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• Everything happens at the
interface
• Charge Transfer Rct
– Rct~ 1/ i0– Butler‐Volmer Equation
• Diffusion Layer W
• Bulk Electrolyte Rser, RΩ• Double Layer Cdl
– Non‐Faradaic Process
Electrochemical Interface
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Randles’ Circuit
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Process of Energy Storage in Electrochemical System
• Ionic charge conductionthrough electrolyte in pores of active layer
• Electronic charge conduction through conductive part of active layer
• Electrochemical reactionon the interface of active material particles including electron transfer
• Diffusion of ions or neutral species into or out of electrochemical reaction zone.
EISZ(SOC,SOH,T;ω)
Performance Simulation•Arbitrary Load•DC/AC/Transient•Power/Energy
•Discharge Process•Polarization Curve•CV
Evaluation & Diagnosis•CO poisoning •Water flooding in FC
Study of Mechanism
Ex) Rs, Rct, Cdl, W …
Common Steps
)TSOH,SOC,(P
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Impedance Spectra of a Li‐ion battery
Nyquist Plotvs. level of discharge
Effect of temperatureCF)Discharge curveupon cycling
Impedance Spectraupon cycling
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PEMFC
A. PEMFC Under Dead End
( H2O outlet in cathode closed)
B. PEMFC Under CO Poisoning
(H2 + 100ppm CO as fuel gas)
Ref. Zahner elektrik‐Kronach Impedance Day 2012
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Circuit Elements (1)
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Basic Circuit Elements
Resistor→
Inductor→
Capacitor→
RIE
IdtCC
QE 1
dtdILE
RZ
Cj
CjZ
11
LjZ
tjeItI 0)(
tjeItI 0)(
tjeItI 0)(
IZE
IZE
IZE
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AC Current, Voltage, and Impedance
"')sin(cos
/,)()()()(Impedance
)cos()(Current2 & 1where,
)cos()(Voltage
)(
)(
jZZjZ
IEZwhereeZIEZ
eI
tIIfjeE
tEE
o
oooj
o
tjo
o
tjo
o
→ Modulus & Phase(Bode Plot)
→ Real & Imaginary part (Nyquist Plot)
← Ohm’s Law
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• Nyquist Plot– Vectors of length |Z|– Individual charge transfer
processes are resolvable.– Frequency is not shown.– Small Z can be hidden by large Z.
• Bode Plot– C may be determined graphically.– Small Zs in presence of large Zs
are usually easy to identify.
Presentation of Impedance SpectrumIm
aginary, ‐Zʺ
Real, Zʹ
|| Z 0
log
log
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Basic Circuit Elements
Resistor→
Inductor→
Capacitor→
RZ
Cj
CjZ
11
LjZ
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• Serial Combination • Parallel Combination
Combinations of Elements
21 ZZZ 21
111ZZZ
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Combinations of Circuit Elements
R‐C→
R|C→
R‐R|C→
CjRZ
1
CjRZ
11
CjR
RZ S
1
1
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Rs‐R|C
"'
1111
222222
jZZ
CRRCRj
CRRRs
CjR
RZ S
minmaxmax
222max
max
22
2
222222
phase,""1212
'4.
2")
2('
1",
1'3.
,2.,01.
ZZRC
RCR
RCRRRZ
RZRRZCR
RCRZCR
RRZ
RZRRZ
s
SS
s
s
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Rs‐R|C
Rs RS+R
R
ωmax = 2fmax = 1 / RC
Z’
‐Z”
ωω 0
logω
Phase ϕ
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• Ideal Coating • Imperfect Coating
Coating Capacitance
dACcoat
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• There is not a unique equivalent circuit that describes a spectrum.
• Measuring Z is simple and easy, but analyzing it is difficult.
• Physically relevant model is important.– It can be tested by altering
physical parameters.• Be cautious in handling empirical
models even if you get a good looking fit.– Use the fewest elements– Test it by T‐test
Uniqueness of Models
Same Impedance Spectrum
Z’
‐Z”
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• Ambiguities in interpretation
– All cells have intrinsically distributed properties
– Ideal circuit elements may be inadequate to describe real
electrical response
– Use of distributed elements (e.g. CPE)
• There is not a unique equivalent circuit describes
measured impedance spectrum
Disadvantages of EIS
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• Relatively simple electrical measurement
• But analysis of complex material variables: mass transport, rates of chemical reactions, corrosion….
• Predictable aspects of the performance of chemical sensors and fuel cells
• Providing empirical quality control procedure
Advantages of EIS
Modified figure shown in page 10, IS(2nd ed.)
ElectrochemicalSystem
EIS ExperimentZe(ω)Theory
Physically Relevant Model
Mathematical Model
Ztheory(ω)
Empirical CircuitZem(ω)
Curve Fitting
SystemCharacterization
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Circuit Elements and Electrochemical Meanings
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• Electrolyte Resistance
– 3 electrode: between WE and RE
– 2 electrode: all series R in the cell are measured incld. R of
contacts, electrodes, solution, and battery separators
– Depends on ionic concentration, type of ions,
temperature, and geometry
Physical Electrochemistry & Equivalent Circuit Elements
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• Charge Transfer Resistance– Echem charge transfer reactions are generally modeled as
resistances.– When an EIS spectrum is measured on a corrosion cell at Ecorr,
the resistance at low‐frequency is identical to the polarization resistance.
Physical Electrochemistry & Equivalent Circuit Elements
0
),0(),,0(
nFiRT
iER
tCtCct
RO
oR
R
O
O
ii
CtC
CtC
nFRT
**
),0(),0(
For a one step, multi‐electron process, O + ne Rsmall overpotential is given by
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• Double Layer Capacitance– A electrical double layer forms as
ions from the solution “stick on” the electrode. There is an Å‐wide separation between charge in the electrode and ionic charges in the solution.
– Charges separated by an insulator form a capacity. On a bare metal, estimate 20 to 40 μF of C for every cm2 of electrode area.
– Depends on electrode potential, temperature, ionic concentrations, types of ions, oxide layers, electrode roughness, impurity adsorption, etc
Physical Electrochemistry & Equivalent Circuit Elements
From A. J. Bard & L. R. Faulkner, “Electrochemical Methods”
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• Constant Phase Element (CPE)
– The CPE is basically an imperfect capacitor.
– It’s phase shift is less than 90.
– Unlike C, a CPE has 2 parameters• α is generally between 0.9 and 1.0
• A is similar to C
– Possible Explanations • Surface roughness Fractal Dimension, D=1+1/α
• Distribution of reaction rates on a surface
• Varying thickness or composition of a coating
Physical Electrochemistry & Equivalent Circuit Elements
)(1jA
ZCPE
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• Diffusion– Diffusion processes can create an impedance, which is
small at high frequency and increases as frequency decreases.
– Warburg Impedance• Warburg looks like a special CPE with A=1/s and α=1/2.• However, remember that Warburg is derived from electrochemical kinetics. Parameters you obtain with Warburg have physical meanings. It is only partly true for CPE.
• You can get a good fit, but how to interpret the resulting parameters?
Physical Electrochemistry & Equivalent Circuit Elements
2/14
)()1(
jejZ
j
W
*2/1*2/122
112 RROO CDCDAFn
RT
For a one‐step, multi‐electron process
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• Diffusion– Nernstian & Finite Diffusion Impedance
– Homogeneous reaction(Gerischer)
– Spherical Diffusion
Physical Electrochemistry & Equivalent Circuit Elements
jBAZ
1
jBAZ
11
)tanh()1( DjjZ
)coth()1( DjjZ
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• Diffusion Transmission Line Model
Physical Electrochemistry & Equivalent Circuit Elements
)1( jZ
)tanh()1( DjjZ
)coth()1( DjjZ
Warburg
Nernstian Impedance: Diffusion by Constant Concentration
Finite Diffusion Impedance: Diffusion by Phase Boundary
T Element
O Element
W Element
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Nernstian Impedance
R: 100ΩC: 0.001F
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Nernstian Impedance
R: 100ΩC: 0.001F
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Finite Diffusion Impedance
R: 100ΩC: 0.001F
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Finite Diffusion Impedance
R: 100ΩC: 0.001F
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Validation of Impedance DataKramers‐Kronig Relation
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• Ideal impedance data must fulfill:– Causality: The output must be exclusively a result of the input– Linearity: The response must be a linear fn. of the perturbation– Stability: The system must not be changing during measurement
→ a serious problem for corroding systems– Finite‐Valued: Impedance must be finite value at any frequency
• Kramers‐Kronig Relation: – Validation Test– Low Frequency Extrapolation
– The integration range includesthe frequencies zero and infinity
– Note pure capacitor cannot be calculated
Validation of Impedance Data
dxx
ZxZZ
dxx
ZxxZZZ
022
022
)(')('2)("
Z" Z'b.
)(")("2)(')('
Z' Z"a.
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• Circuit theory is simplified when the system is “linear”.
• Z in a linear system is independent of excitation amplitude. The response of a linear system is always at the excitation frequency (no harmonics are generated).
• Look at a small enough region of a current versus voltage curve and it becomes linear.
• If the excitation is too big, harmonics are generated and EIS modeling does not work.
Electrochemistry: A Linear System?
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• Measuring EIS spectrum takes time (often many hours).
• The sample can change during the time the spectrum is
recorded.
• If this happens, modeling results may be wildly
inaccurate.
• To shorten the measuring time of impedance spectrum,
use FFT EIS method.
E’chem: A Stationary System?
Non‐Stationary Conditions result in non‐stationary spectra !
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K‐K Relation
Ref. Scribner Associates Inc. – ZView K‐K Transform Tutorial
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Validation of Impedance Data Z‐HIT
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Limitation of K‐K Relation• The integration range includes the frequencies zero and infinity• |Z| and Phase are measured independently with different accuracy and
sensitivity, but in theory, they are correlated with each other.
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Heating NTC, PTC
1 2 3 4 53,4
3,5
3,6
3,7
3,8
3,9
4,0
0
15
30
45
60
75
90
KTY 10k (NTC)
LOG
Impe
danc
e /
LOG frequency / Hz
|Phase| / °
0 1 2 3 4 5
3,05
3,10
3,15
0
15
30
45
60
75
90Pt 1000 (PTC)
LOG
Impe
danc
e /
LOG frequency / Hz
|Phase| / °
Ref. Zahner elektrik‐Kronach Impedance Day 2012
Phase is more stable than |Z|!
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Z‐HIT Approximation
Ref. Kronach Impedance Day 2012
ln)(
ln)( 2 + onst. )(ln0
0 dd
dcZ O
S
Local relationship between impedance and phase
=> Not affected by the limited bandwidth problem
=> Reliable detection of artifacts and instationarities (drift)
=> Reconstruction (!!) of causal spectra
=> Reliable interpretation of spectra
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Ex. Spectrum of a fuel cell under load
10m 100m 1 3 10 100 1K 10K 100K
10
20
15
30
25
|Z| / m
-30
0
30
60
phase / o
frequency / Hz
1. Z-HIT
2. FIT10m 100m 1 3 10 100 1K 10K 100K
10
20
15
30
25
|Z| / m
-30
0
30
60
phase / o
frequency / Hz
Ref. Kronach Impedance Day 2012
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Ex. Fuel cell under CO poisoning
Ref. Zahner elektrik‐ Kronach Impedance Day 2012
0,0 0,1 0,2 0,3 0,4 0,5
-0,2
-0,1
0,0
0,10.1 Hz
2 Hz
3 Hz
10K
DATA FIT
imag
inar
y pa
rt /
real part / 0,0 0,1 0,2 0,3 0,4 0,5
-0,2
-0,1
0,0
0,1
0.1 Hz
2 Hz
3 Hz
10 KHz
DATA FIT
imag
inar
y pa
rt /
real part /
Raw data Refined data
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Other Methods to Measure EIS
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Multi‐Sine Wave Method
Single Sine Method
Multi‐Sine Method
In Galvanostatic EIS, Freq |Z| |V| : Linear Region?
“Pseudo‐Galvanostatic EIS”
Time
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Time Resolved EIS
10m 50m
real part / Ohm
-10m
10m
0
imag
. par
t / O
hm
10m 50m
real part / Ohm
-10m
10m
0
imag
. par
t / O
hm
10m 50m
real part / Ohm
-10m
10m
0
imag
. par
t / O
hm
1. Real Time‐Drift Compensation
impe
danc
e
time
frequency
drift affected data
time course of theinterpolated data
impedance atsingle frequencies
3. Z‐HIT Refinement
2. Time‐Course Interpolation
An EIS recorded at the PEMFC with flooded cathode, after 4450s of “dead end” operation at 2A. After pp501‐505, IS (2nd ed.) & Schiller
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Artifacts
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• The effects of inductances are often seen at the high frequencies
• The value of inductor is very small, however, this can be important if the electrode impedance is low.
• Possible Causes– Actual physical inductance of loop or
coil of wire between electrode and potentiostat
– Self inductance of the electrode itself: even a straight piece of rod has some self inductance ~ several nH
– Some cylinder‐type batteries also shows this effect ~ uH
– Instrumental artifacts, notably capacitance associated with the current measuring resistor, however.potentiostat manufacturers may
have already made corrections for this effect
Inductive Loop at High Frequency
LjZL dtdILE
‐Zʺ
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Mutual Induction ‐ Twisting Cables
Ref. Zahner elektrik‐Kronach Impedance Day 2012
A B C D
Arbitrary CE/RE & WE/WS CE/WS & WE/RE CE/WE & RE/WS
Cell: 20 mΩ planar resistor
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Others
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• Potentiostatic Mode– Vac is 1 mV Minimum !– 1 mVrms = 1.414 Arms X Z– Zmin = 707 uΩ– These are Absolute Minimum Z Values !
• Limitation is APPLIED E• Measured E is still Accurate!
• Galvanostatic Mode– Can Measure Smaller E Values ! ~Microvolts– CMR of electrometer may limit the absolute minimum Z
Values! ‐> 5 uΩ– Refer to “Shorted Lead Test”
Galvanostatic EIS is Better for Low Z
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• Building equivalent circuit model– Physically relevant model
• Each component is postulated to come from a physical process in the EChem cell based on knowledge of the cell’s physical characteristics.
– Empirical model
• Complex Nonlinear Least Square (CNLS) Fitting Algorithm– is used to find the model parameters that cause the best agreement between
a model’s impedance spectrum and a measured spectrum.– starts with initial estimates of model parameters. – Iterations continue until the goodness of fit exceeds an acceptance criterion,
or until the number of iterations reaches a limit. – Please check the change of χ2after each iteration.– Sometimes, CNLS algorithm cannot converge on a useful fit because of
• An incorrect model• Poor estimates for the initial values• Noise and etc.
– Don’t care if the fit looks poor over a small section of the spectrum.
How to Extract Model Parameters