November 2008, 1 Potentiostats Principles of operation.
-
Upload
alana-kille -
Category
Documents
-
view
214 -
download
0
Transcript of November 2008, 1 Potentiostats Principles of operation.
November 2008, 1
PotentiostatsPrinciples of operation
November 2008, 2
Overview
• The potentiostat – a black box ?• Potentiostat (role)• The operational amplifier
– Voltage follower – Current follower– Scaler & Adder– Control amplifier
• Basic potentiostat construction• How to make the most of your potentiostat
November 2008, 3
Overview
• A. Bard & L. Faulkner, Electrochemical Methods – Fundamentals and Applications, 2nd edition, John Wiley & Sons
• H. Girault, Analytical and Physical Electrochemistry, EPFL Press, Marcel Dekker
• C. Brett, A. M. Brett, Electrochemistry – Principles, Methods and Applications, Oxford University Press
• D. Pletcher, R. Greef, R. Peat, L. Peter, J. Robinson, Instrumental Methods in Electrochemistry, Horwood Publishing
• R. E. Simpson, Introductory Electronics – For Scientists and Engineers, Allyn and Bacon
November 2008, 4
The potentiostat – a black box ?
November 2008, 5
Difficulties of potential control
• It is not possible to measure the potential of the working electrode potential difference w.r.t. reference electrode
• Reference electrode is always required• Controlling potential is a lot more difficult than
controlling current• This increases the probability of an experiment
going wrong
November 2008, 6
The role of the potentiostat – facts…
• The potentiostat controls the potential of the working electrode (relative to the reference electrode)
• The potentiostat controls the potential of the working electrode regardless of the characteristics of the cell
• The counter electrode is required for measuring the current only
November 2008, 7
…or fiction
• The potentiostat controls the potential of the working electrode (relative to the reference electrode) : false
• The potentiostat controls the potential of the working electrode regardless of the characteristics of the cell : false
• The counter electrode is required for measuring the current only : false
November 2008, 8
Is it important to know how it works ?
• Probably not but… • Important for troubleshooting
– Example #1 – VOVL warning at potentials well below the maximum value ?common problem with fast kinetics in resistive environments
– Example #2 – Small counter electrode / QCM crystalproblems occurring during dissolution of deposited metallic adlayer short-circuit in the cell
November 2008, 9
The role of the potentiostat
• The default role of a potentiostat is to control/measure a potential difference (involves feedback mechanism)
• The instrument applies and maintains a given setpoint, regardless of the characteristics of the cell
• If the cell changes during time, the potentiostat changes its output in order to maintain the setpoint
At all times, the potential difference between the working electrode and the reference electrode must be controlled!
November 2008, 10
Understanding the potentiostat
• Core element of a modern potentiostat The operational amplifier (op amp)
-
+
VS-
VS+
VoutV-
V+
Inverting input
Non inverting input
November 2008, 11
The operation amplifier
• Role of the op amp Amplify the voltage difference between the 2
inputs by a factor G
G = Open loop gain
Vs = voltage of inverting input with respect to the non-inverting input
-
+
VS-
VS+
VoutV-
V+
VS out SV (V V ) G V G -
+
VoutV-
V+
VS
November 2008, 12
The operation amplifier
• The ideal op amp: interesting properties– Infinite open gain loop (G = )
• Slightest input voltage difference Vs drives the output to infinity
– Infinite input impedance (input i = 0)– Zero output impedance (output i = )
November 2008, 13
The operation amplifier
• The ideal op amp: interesting properties– Infinite open gain loop (G = )
• Slightest input voltage difference Vs drives the output to infinity
• If op amp is used in any circuitry, then the 2 inputs must be (by design) at the same voltage !
• The amplifier must be stabilized by feeding back part of its output to its input
November 2008, 14
Building block # 1 - Voltage follower
-
+Vout
Vin
VS
• Based on voltage feedback
out SV V G
S out inV V V
out out in out in
1V V V G V 1 V
G
o ouG t it nu
1lim V 1
GV V
November 2008, 15
Building block # 1 - Voltage follower
-
+Vout
Vin
• Based on voltage feedback
out inV V
Output of the voltage follower is always equal to the input voltage! Useless ? Input impedance =
Vin
Vin
Vin
November 2008, 16
Building block # 2 - Current Follower
• Based on current feedback
-
+Voutiin
Rf
if
S
@ S : i 0f ini i
out Sin
f
V Vi
R
And out SV V G
outout
in out in ff
VV 1G i V 1 i R
R G
out out in fG
1lim V 1
GV i R
November 2008, 17
Building block # 2 - Current Follower
• Based on current feedback
-
+Voutiin
Rf
if
S
Vout -iin Rf
CF is a current-to-voltage converter
Constitutes the basic element of a zero-resistance amperometer (ZRA) – no shunt resistance
Voltage @ summing point S
VS = - Vout / G 0 V
S is a virtual ground!
November 2008, 18
Building block # 2 - Current Follower
• Based on current feedback
-
+Voutiin
Rf
if
S
Vout -iin Rf
Output of the CF must match the input current (x Rf) at all times !
November 2008, 19
Building block # 2 - Current Follower
• Based on current feedback
-
+Voutiin
Rf3
S
Rf2
Rf1
Automatic current ranging in the potentiostat
November 2008, 20
Automatic current ranging issues
• Relay settling time problem prevents ACR @ high sampling rate
1000 V/s linear scan100 uA current range
alkanethiol SAM on gold composed of a 10 bond ferrocenederived alkanethiol with 8-mercaptooctanol in a 1:20 ratio
November 2008, 21
Automatic current ranging issues
• Relay settling time problem prevents ACR @ high sampling rate
1000 V/s linear scan10 mA current range
alkanethiol SAM on gold composed of a 10 bond ferrocenederived alkanethiol with 8-mercaptooctanol
November 2008, 22
Building block # 3 - Scaler
-
+Vout
Rf
if
S
Rin
Vin
iin
Vout = -iin
Rf
fou
inin t in
inin
Vi
R
RV V
R
• Based on current feedback
Scaling factor
November 2008, 23
Building block # 3 - Scaler
-
+Vout
Rf
if
S
Rin
Vin
iin
• Based on current feedback
fout in
in
RV V
R
Output of the scaler is always equal to the inverted input multiplied by the scaling factor !
November 2008, 24
Building block # 4 - Adder
-
+Vout
Rf
if
S
R1
R2
R3
V1
V2
V3
i1
i2
i3Vout = -iin
Rf
f f fout 1 2 3
1 2
31 2in 1 2 3
1 32 3
VV Vi i i i
R R
R R RV V V V
R R RR
• Combination of scalers
November 2008, 25
Building block # 4 - Adder
-
+Vout
Rf
if
S
R1
R2
R3
V1
V2
V3
i1
i2
i3f f f
out 1 2 31 2 3
R R RV V V V
R R R
• Combination of scalers
Output of the adder is always equal to the inverted sum of the independently scaled input voltages!
November 2008, 26
Building block # 5 - The control amplifier
Vout
VA = -Vin
-
+
R1
R2
A
i0
i0
R
R
i
i
SVin
-Vin
Condition must be true at all times
21
out0 RR
Vi
2
in0 R
Vi
2
21inout R
RRVV
November 2008, 27
Building block # 5 - The control amplifier
Vout
VA = -Vin
-
+
R1
R2
A
i0
i0
R
R
i
i
SVin
-Vin
2
21inout R
RRVV
Output of the control amplifier is set so that the potential of A is at – Vin w.r.t. ground at all times: potentiostat
November 2008, 28
Building block # 5 - The control amplifier
Vout
VA = -Vin
-
+
R1
R2
A
i0
i0
R
R
i
i
SVin
-Vin
2
21inout R
RRVV
Vin (V) 1 1 1
VA (V) -1 -1 -1
R1 (Ohm) 100 100 10000
R2 (Ohm) 1000 1000000 1000
Vout (V) -1.1 -1.0001 -11 !! Max Vout = Compliance voltage
November 2008, 29
0.1 0.2 0.3 0.4 0.5
-8.0x10-5
-6.0x10-5
-4.0x10-5
-2.0x10-5
0.0
2.0x10-5
4.0x10-5
6.0x10-5
8.0x10-5
250 mV/s 100 50 25 10 5
I /A
E /V
4.8mM ferrocene, 0.1M [NEt4][BF
4], MeCN
flow rate = 1ml/hr
Compliance voltage problems
November 2008, 30
Compliance voltage problems
-0.1 0.0 0.1 0.2 0.3 0.4
-1.0x10-4
-5.0x10-5
0.0
5.0x10-5
1.0x10-4
1.5x10-4
I /A
E /V
1000 mV/s
-0.1 0.0 0.1 0.2 0.3 0.4-0.1
0.0
0.1
0.2
0.3
0.4
2nd
sign
al E
/V
E /V
November 2008, 31
Basic potentiostat/e-cell
-
+
R
R
i
i
SVin
icell
Vout
ce
we
re-Vin
ce
we
reR
wece re
Rp
Cd
Vref = -Vin
pout in
p
R RV V
R
November 2008, 32
Basic potentiostat/e-cell
• The potentiostat controls the potential of the working electrode (relative to the reference electrode)
• The potentiostat controls the potential of the working electrode regardless of the characteristics of the cell
• The counter electrode is required for measuring the current only
November 2008, 33
Basic potentiostat/e-cell
-
+
R
R
i
i
SVin
icell
Vout
ce
we
re-Vin Vref = -
Vin
pout in
p
R RV V
R
Problems of this potentiostat concept:
-Current flowing through the reference electrode
-No current measurement
November 2008, 34
-
+
S
icell
Vout
ce
we
re
Vin
-
+
-Vin
Basic potentiostat/e-cellp
out inp
R RV V
R
Voltage follower
Control amplifier
November 2008, 35
-
+
S
icell
Vout
ce
we
re
Vin
-
+
-
+
VcurrentS’
-Vin
Basic potentiostat/e-cellp
out inp
R RV V
R
current cell fV i R
Current follower
Voltage follower
Control amplifier
November 2008, 36
-
+
S
icell
Vout
ce
we
re
V1
V2
V3
-
+
-
+
VcurrentS’
-Vin
Basic potentiostat/e-cellp
out inp
R RV V
R
current cell fV i R
Current follower
Voltage follower
Control amplifier
Adder
November 2008, 37
Summary
• The potentiostat does not control the potential of the working electrode!
• The potentiostat controls the potential of the counter electrode only (relative to the working electrode)
• The counter electrode is the most important electrode (followed by the reference electrode – the working electrode is never a problem)
• Compliance voltage limits are very important in the choice of the potentiostat / application
• With a few components you can build your own potentiostat
November 2008, 38
Good enough for a homemade potentiostat?
November 2008, 39
Difficulties with potential control
• Interfacial capacitance and solution resistance– High solution resistance has high impact
on potential control, especially for large currents
– Potentiostat must have enough power reserve to supply the necessary current
– Ex: 1 V step in 1 µs on a 2 µF interfacial capacitance – imean = 2 µC/1 µs = 2 Apeak current can be higher !
November 2008, 40
Difficulties with potential control
• Solution resistance – high current measurements
Ru is the uncompensated resistance
Compensated resistance (control amplifier)
November 2008, 41
Difficulties with potential control
• Solution resistance – high current measurements
wk
ce
iRsol
Ref
iRu
Ru is the uncompensated resistance
Rsol = R + Ru
For high currents, the voltage drop across the solution can reach ~ 100 V
- The potentiostat must be able to supply enough power ( the compliance voltage must be high enough)!
November 2008, 42
Difficulties with potential control
• How to reduce Ru
– Reduce total resistance (R + Ru)•
Increase the conductivity (supporting electrolyte, polar solvent)
• Reduce the viscosity• Increase the temperature
– Reduce the size of the we
– Move the re as close as possible to the we• Use a Luggin capillary
November 2008, 43
-
+
S
icell
Vout
ce
we
re
V1
V2
V3
-
+
-
+
Vcurrent = -iRfS’
-Vin
Electronic IRu compensation – positive feedback
November 2008, 44
-
+
S
V1
V2
V3
-
+
Vcurrent = -iRfS’
-Vin
Automatic compensation of the iRu drop can be attempted by feeding back a correction voltage proportional to the current flow to the input of the potentiostatThe variable resistance can be trimmed to be set to a fraction f of the feedback resistance (Rf)
feedback voltage is –ifRf
etrue (vs re) = e1 + e2 + e3 – ifRf + iRu
Electronic IRu compensation – positive feedback
November 2008, 45
Computer controlled potentiostat• Computer use digital signals (0 & 1) instead of
analog signals (0-10 V) • Interfacing a potentiostat with a computer
requires translation back and forth• Modern potentiostats have on-board DAC
(digital to analog converters) and ADC (analog to digital converters)
November 2008, 46
Computer controlled potentiostat
01001010…
10010100…
DAC
ADC
0-10 V
0-10 V
P-stat
External (RDE, strirrer, T, …)
External (QCM, spectro, pH, …)
November 2008, 47
Computer controlled potentiostat
DAC Digital to analog converter
- Resolution in bits: 16 bits – 216 = 65536 digital words- 10 V range/65536 = 150 V resolution
- Defines the smallest possible step
- Multiple channels working as indipendent function generators
November 2008, 48
Computer controlled potentiostat
ADC Analog to digital converter
- Resolution in bits: 16 bits – 216 = 65536 digital words- 10 V range/65536 = 150 V resolution
- ADC is a digital filter
Multi-channel ADC to convert several analog signals into digital
November 2008, 49
Autolab potentiostat
November 2008, 50
Autolab potentiostat
01001010…
10010100…
DAC
ADC
0-10 V
0-10 V
P-stat
External (RDE, strirrer, T, …)
External (QCM, spectro, pH, …)
MODULE
01001010…
0-10 V
November 2008, 51
Autolab potentiostat other D/A modules• Scangen module: true linear scan
generator– Generates an analog scan (no staircase)
with scan rates up to 250,000 V/s
• FRA module: frequency response analyzer– Digital to analog sine wave generator
• Both modules are fed into the Adder circuit of the Autolab