electrochemical noise intro
TRANSCRIPT
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Electrochemical Noise
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Electrochemical Noise Measurement
-0.3644
-0.3642
-0.364
-0.3638-0.3636
-0.3634
-0.3632
-0.363
-0.3628
P
o
te
n
tia
l
(V
/S
0
5E-08
1E-07
1.5E-07
2E-07
2.5E-07
C
u
rre
n
t
(A
)
0 400 800 1200Time (secs)
Potential
Current
Steel in 0.05M Ca(OH)2 + 0.1M NaCl
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Potential Noise
Measured as potential difference between twonominally identical electrodes, or relative to areference electrode (usually assumed to be
noiseless).
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Measurement Methods
1 - Potential Noise
V
Reference
ElectrodeWorking
Electrode
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Terminology - Potential Noise
Instantaneous noise potential,
Potential noise power (= variance of signal)
Potential noise standard deviation
E E En2
2
E E En
E E En22
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Potential Noise
First shown to be related to corrosion rate byIverson in 1968.
Recent theoretical work suggests that the potential
noise is larger for less frequent, and hence morelocalized events, such as metastable pittingcorrosion
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Current Noise
Usually measured as galvanic current flowingbetween two nominally identical electrodes,although potentiostatic measurements can be
made.
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Measurement Methods2 - Current Noise
A
Working
Electrode 2Working
Electrode 1
Zero Resistance
Ammeter
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Terminology - Current Noise
Instantaneous noise current,
Current noise power (= variance of signal)
Current noise standard deviation
I I In
2 2 ( )
I I In
I I In22
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Current Noise
Standard deviation of current is usually found toincrease as corrosion rate increases.
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Noise Resistance
Obtained by dividing standard deviation of potentialnoise by standard deviation of current noise,measured at the same time, to produce Rn.
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Measurement Methods3 - Noise Resistance
A
Working
Electrode 2
Working
Electrode 1
Zero Resistance
Ammeter
V
Reference
Electrode
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Noise Resistance
Rn is expected to be equivalent to the linearpolarization resistance, Rp.
Hence often gives good quantitative estimate of
corrosion rate using the Stern-Geary equation.There are questions about the effective
measurement frequency.
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Sources of Noise
Active dissolution (or other electrochemicalreaction)
Pit nucleation, propagation and death
Hydrogen bubble evolution
Mass transport fluctuations
Mains frequency interference
Electronic noise
Vibration
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Crevice Corrosion
-0.3644
-0.3642
-0.364
-0.3638
-0.3636
-0.3634
-0.3632
-0.363
-0.3628
P
o
ten
tia
l
(V
/S
0
5E-08
1E-07
1.5E-07
2E-07
2.5E-07
C
ur
re
n
t
(A
)
0 400 800 1200Time (secs)
Potential
Current
Mild steel in 0.05 M Ca(OH)2 + 0.1 M NaCl
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Pitting Corrosion
-0.276
-0.2755
-0.275
-0.2745
-0.274
-0.2735
-0.273
-0.2725
-0.272
P
o
ten
tia
l
(V
/S
C
3E-08
4E-08
5E-08
6E-08
7E-08
8E-08
9E-08
C
ur
re
n
t
(A
)
0 200 400 600 800 1000 1200Time (secs)
Potential
Current
mild steel in 0.05 M Ca(OH)2 + 0.025 M NaCl
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Correlation of E and I
-0.3643
-0.3642
-0.3641-0.364
-0.3639
-0.3638
-0.3637
-0.3636
-0.3635
P
otential(V
/S
C
E
)
5E-08
1E-07
1.5E-07
2E-07
2.5E-07
Cu
rrent(A
)
0 10 20 30 40 50 60
Time (s)
Vol tage Current
-0.276
-0.2755
-0.275
-0.2745
-0.274
-0.2735
P
otential(V
/S
C
E
)
3E-08
4E-08
5E-08
6E-08
7E-08
8E-08
Cu
rrent(A
)
100 110 120 130 140 150 160
Time (s)
Potential Current
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Bidirectional Transients in Pitting
-0.388
-0.386
-0.384
-0.382
-0.38
-0.378
P
o
te
n
tia
l
(V
/S
2E-07
3E-07
4E-07
5E-07
6E-07
7E-07
8E-07
C
u
rr
e
n
t
(A
)
0 200 400 600 800 1000 1200Time (secs)
Potential
Current
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Pitting Corrosion
-0.04
-0.035
-0.03
-0.025
-0.02
-0.015
P
o
te
n
ti
a
l
(V
/S
-1.8E-06
-1.6E-06
-1.4E-06
-1.2E-06
-1E-06
C
u
rre
n
t
(A
)
0 200 400 600 800 1000 1200
Time (s)
Voltage
Current
Mild steel in 0.01 M NaNO2 + 0.05 M NaCl
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Shot Noise Analysis
Noise results from random variation in number ofpulses arriving within each sample interval
Current noise has constant power per unit of
bandwidth (white noise)
tmeasuremenofbandwidth=current=
pulseincharge=where
2= 2
bI
q
qIbIn
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Shot Noise Analysis
We can estimate the charge in each event from
Similarly we can estimate the frequency of eventsfrom
B
b
qEI
=
2
2
==E
corr
nb
B
q
If