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How Cabling and Signal Amplitudes Affect EIS Results

Accurate EIS

Gamry Instruments prides itself on performing accurate EIS. We publish an Accuracy Contour Plot (ACP) for every instrument we sell. ACPs describe a region of accuracy over a given range of impedances and frequencies under a defined set of conditions.

Why Generate ACPs?

Why do we do this? Two main reasons:

  1. So that you understand the ranges and limitations of our instruments when performing EIS under typical conditions
  2. ACPs can change depending on cable length and signal amplitude

Generating an ACP typically starts with examining the open lead curve and the shorted lead curve. The open lead curve is meant to describe the absolute capacitive limits of the entire potentiostat and cable under a stated amplitude. Any result that you get from an EIS experiment that is at or above open lead curve should be thrown out no matter how nice the data appear. You are measuring the capacitance of your measurement system and not your sample. Extremely well insulating coatings can be one example.

Potentiostatic experiments are typically performed at 10 mV rms or smaller in order to maintain a linear response. Remember that in order for EIS results to be valid, your system needs to be linear, stable, and casual. Linearity, stability, and causality can assessed using Gamry’s built-in Kramers-Kronig function found in our analysis software. Galvanostatic experiments are a little bit different in that the current amplitudes can get larger as long as the voltage response maintains linearity – i.e. passes the Kramers-Kronig test.

ACPs of the Interface 1010

ACPs are only valid under the specified conditions.  For example, the ACP for the Interface 1010 as seen below shows that you can measure impedances from 3 GΩ down to less than 1 mΩ at greater than 99% accuracy. The lower impedance limit is useful to know when examining energy storage and conversion devices while the upper impedance limit is useful for corrosion-resistant materials and well-coated samples. It is also helpful to know the capacitive limit, seen as an increasing line as frequency decreases, for well-coated samples.  

IFC 1010 ACP Full sizeFigure 1. Accuracy Contour Plot for an Interface 1010 with a 60 cm cell cable
and ≤ 10 mV rms signal amplitude.

Uncompromised EIS performance

Our accuracy contour plots have always been transparent and easy to reproduce. The figure below shows EIS results taken on an Interface 1010E potentiostat for four capacitors, ranging from pF- to F-level capacitance. These are overlaid onto the Interface 1010E ACP and behave exactly as expected:

    1. Ceramic and Mylar capacitors exhibit linear response on a log-log Bode plot (pF- to nF-level), increasing in magnitude as frequency decreases.
    2. Electrolytic capacitors and supercapacitors exhibit an initially flat frequency response tied to real electrochemical processes but eventually reach the linear response expected for capacitors (µF- to F-level).
    3. High frequency artifacts present at lower impedances are tied to mutual inductance (L) along the potentiostat cell cable. Mutual inductance bounds the accuracy of low impedance, high frequency systems.
    4. A special case of resonance is observed for the 100 nF capacitor. After all, the resonant frequency for the RLC couple (100 nF and ~200 nH) is a little over 1 MHz. At resonance, imaginary impedance (Zimag) goes to zero and Zmod trends downwards towards a lower limit of the series resistance (R), usually tied to contact resistances for Mylar capacitors. 

 a. If you study systems within ~nF capacitance, look out for this type of high frequency behavior.

Notice for the 3F capacitor that we had to go to lower frequencies to better resolve the capacitive impedance response. For larger capacitance and other high capacity energy storage devices, low frequency systematic drift can become an issue as potentiostatic EIS is no longer practical. We have a solution for this in the form of drift correction for galvanostatic EIS (software version 7.8.4 and higher). 

accuracy contour plot of EIS performance

Figure 2. Four different capacitors as measured by an Interface 1010E.  

Cable lengths and signal amplitudes

Gamry’s standard cell cable is 60 cm but we also have 1.5, 3, and 10 m cables available as options.  Since the open lead curve is the measure of the instruments capacitive limit for a measurement, we measured the open lead curve for the 3 and 10 m cables also.  Additionally, we measured the open lead curve without a cable.  As shown in Figure 3, the maximum applied frequency decreases as a function of cable length.  The capacitive region of the ACP decreases slightly as the cable length is increased.  The No Cable line falls in the middle due to the unshielded shunts we used to short the pins on our cell cable connector. Notice too that the maximum impedance limit decreases as a function of cable length due to the increased R of the cable.  If you were to use a longer cable you would expect a decrease in bandwidth due to the added R and C.

OLC Diff cables

Figure 3. Open Lead Curve for an Interface 1000 with a 10mV rms amplitude and different cable lengths. Orange curve – no cable;
Black curve – 60 cm; blue curve – 3 m; Red curve – 10 m.

Changing the signal amplitude also has an effect on the ACP.  An increase in amplitude increases signal to noise, pushing the capacitive limit higher as shown in Figure 4.  Signal amplitudes of 1, 10, 100, and 707 mV rms were used to generate the four open lead curves. A 60 cm cell cable was used.  Though it seems logical to use larger amplitudes, in reality, the larger amplitude likely invalidates the linearity criterion of EIS.   

OLD diff amplitudes2

Figure 4. Open Lead Curve for an Interface 1000 using a 60 cm cell cable with different signal amplitudes. Blue diamonds – 1 mV rms; Red squares – 10 mV rms; Green dots – 100 mV rms; Purple triangles – 707 mV rms.

Consider the potentiodynamic scan shown in Figure 5.  The response is linear around the open circuit potential but moving away from open circuit creates a non-linear response.

Potentiodynamic 430SS

Figure 5. Potentiodynamic scan on 430 SS in 1 M H2SO4. 0.167 mV/s.

Hence, in an EIS experiment, you need to use small amplitudes such as 10 mV.  As can be seen in the ACPs shown in Figure 4, the capacitive limit increases when you use larger signals but as was just mentioned you cannot use larger signals without risk of damaging the sample.  These are the changes that affect the capacitive region of the ACPs.  The second important region is the lower impedance limits and bandwidth.

The lower impedance limits are typically determined by the maximum current of the instrument along with instrument design.  Separation of the current carrying leads from the sense leads increases the bandwidth for the inductive region. Note that the 1.5 m Low Z cable has separated current carrying and sense leads thereby increasing the bandwidth as shown in Figure 6.  The plots shown here are for an uncalibrated 0.500 mΩ shunt whose actual bandwidth is unknown.  The illustration of the plot is to show the effect of increased cable length on bandwidth.

LowZ diff cables

Figure 6. ACP showing lower impedance limits for three different cable on an Interface 1000 using a signal amplitude of 100 mA rms.
Blue - 60 cm, green - 1.5 m, purple - Low Z cable.

What is the point of all this?

Lots of instrument manufacturers don't publish ACPs and of those that do they don't provide you with realistic or even any conditions related to how those ACPs were generated.  Be sure you understand the limits of any instrument before making your purchase.

The purpose of this technical note is to describe the effect of signal amplitudes and cable lengths on accuracy contour plots.  Gamry prides itself on providing accurate ACPs generated using real-world signal amplitudes and actual cell cables. 

If you wish to generate your own Accuracy Contour Plot or at least check your system's performance, you can use our Quick Check of EIS System Performance