Galvanostatic EIS (GEIS)
Electrochemical Impedance Spectroscopy (EIS) is an electrochemical technique that measures the impedance of a system as a function of AC current frequency. EIS enables the separation of different component influences, including contributions from electron transfer resistance, double layer capacitance, and other electrochemical processes.
GEIS applies a galvanostatic sinusoidal excitation signal and analyzes the resulting potential response from the device under test (DUT). The density parameter determines the number of measurement points within a specified frequency range. Averaging multiple sine waves reduces noise and non-systematic interference, although this increases the total measurement time.
Galvanostatic EIS is ideal for devices under test (DUT) with low impedances, such as fuel cells, electrolysis cells, batteries, and supercapacitors. High capacitance devices exhibit very long relaxation times. A drifting open circuit voltage (OCV) can cause very high equalizing currents in low impedance devices.
Parameter Description
Parameter |
Name |
Description |
Unit |
|---|---|---|---|
I dc bias |
DC bias current |
DC bias current for defining the operating point of the object |
A |
I amplitude |
amplitude |
AC current peak amplitude |
A |
f start |
start frequency |
starting frequency of the impedance spectrum |
Hz |
f max |
maximum frequency |
upper frequency limit of the impedance spectrum |
Hz |
f min |
minimum frequency |
lower frequency limit of the impedance spectrum |
Hz |
t meas |
minimum measurement time |
minimum recording time for each frequency step |
s |
N waves |
minimum averages |
minimum number of sine waves for each frequency step |
|
Density >66Hz |
density above 66 Hz |
number of frequency steps per decade between 66 Hz and f max |
|
Density at f min |
density at f min |
number of frequency steps per decade at f min |
A Start Phase Galvanostatic can be enabled or disabled before the method is executed.
Measurement Result
The measurement results can be displayed as either Nyquist or Bode plots. To evaluate the spectra, the measurement data is fitted to a representative equivalent circuit model of the DUT. This approach enables the determination of detailed individual parameters for each equivalent circuit element.
Custom Experiment Builder
This experiment is a combination of the following blocks: