Highly time resolved impedance spectroscopy

• US 6,556,001 B1
• Filed: 09/29/2000
• Issued: 04/29/2003
• Est. Priority Date: 10/12/1999
• Status: Expired due to Fees

• Current Assignee: Erich Sackman, Gerald Wiegand
• Original Assignee: Erich Sackman, Gerald Wiegand
• Inventors: Sackman, Erich, Wiegand, Gerald
• Primary Examiner(s): Le, N.
• Assistant Examiner(s): Nguyen, Vincent Q.
• Application Number:
  US09/675,705
• Time in Patent Office: 942 Days
• Field of Search: 324/76.21, 324/718, 324/551, 324/71.1, 324/76.22, 324/71.2, 738/08, 738/66, 204/196.06, 204/196.36, 204/404
• US Class Current: 324/76.21
• CPC Class Codes: G01N 27/026 Dielectric impedance spectroscopy electrochemical impedance spectroscopy for measuring corrosion G01N17/02
• CPC Class Codes: G01R 23/16 Spectrum analysis; Fourier analysis
• CPC Class Codes: G01R 27/02 Measuring real or complex resistance, reactance, impedance, or other two-pole characteristics derived therefrom, e.g. time constant by measuring phase angle only G01R25/00

Abstract

A highly time resolved impedance spectroscopy that enhances the measurement of the dynamics of non-stationary systems with enhanced time resolution. The highly time resolved impedance spectroscopy includes an optimized, frequency rich a.c., or transient, voltage signal is used as the perturbation signal, non-stationary time to frequency transformation algorithms are used when processing the measured time signals of the voltage and current to determine impedance spectra which are localized in time; and the system-characterizing quantities are determined from the impedance spectra using equivalent circuit fitting in a time-resolution-optimized form.

Claims

1. A method of highly time resolved impedance spectroscopy comprising:

generating an a.c. voltage perturbation signal and applying it to a system;

recording the a.c. voltage perturbation signal and a current signal produced in response to the perturbation signal; and

processing the recorded signals using a non-stationary time to frequency transformation.

2. A method as defined in claim 1, wherein the non-stationary time to frequency transformation is a short time Fourier transform.

3. A method as defined in claim 1, wherein the non-stationary time to frequency transformation is a wavelet transformation.

4. A method as defined in claim 1, wherein the non-stationary time to frequency transformation is a Wigner distribution.

5. A method as defined in claim 1, wherein the recording of the a.c. perturbation signal is continuous.

6. A method as defined in claim 1, wherein the recording of the a.c. perturbation signal is partly continuously recorded.

7. A method as defined in claim 1, wherein the a.c. perturbation signal is structured noise.

8. A method as defined in claim 1, further comprising using a high-performance signal amplifier.

9. A method as defined in claim 1, further comprising a analog-digital conversion of the measuring signals.

10. A method as defined in claim 1, further comprising data processing hardware and software for real-time analysis of the impedance spectra.

11. A method as defined in claim 1, further comprising detection of the conductivity of natural or artificial freely-suspended or substrate-supported lipid membranes with and without ion channels.

12. A method as defined in claim 1, further comprising the use of a frequency range of about 100 Hz to 100 kHz and the logarithmic analysis of the real and imaginary part of the impedance.

13. A method as defined in claim 1, further comprising detection of compounds in solutions with a conductivity changing effect in regard to biomembranes.

14. A method as defined in claim 1, further comprising using a measuring chambers with temperature control and liquid handling.

15. A method as defined in claim 1, further comprising use of a complex nonlinear least square method to fit parameters of an equivalent circuit to the measured impedance spectra.

16. A method as defined in claim 1, further comprising the use of automatic liquid handling systems.

17. A method as defined in claim 1, further comprising the use of multielectrode arrangements.

18. A method as defined in claim 17, further comprising the use of multiple measuring chamber systems with parallel data acquisition and analysis.

19. A method as defined in claim 17, further comprising the use of multiple measuring chamber systems with sequential data acquisition and analysis.

20. A method as defined in claim 1 further comprising the integration in automated production and process flow.

21. An apparatus for measuring impedance spectra with high time resolution, the apparatus comprising:

a memory device configured to store an algorithm for generation of a voltage perturbation signal and instructions to process and evaluate measured data;

at least one analog to digital converter configured to receive a signal representing the voltage perturbation signal and to output a digital value representing the perturbation signal, and to receive an electrical current signal representing a system response to the perturbation signal and to output a digital value representing the system response; and

a processor configured to receive the digital values output by the at least one analog to digital converters, and to receive the algorithm and instructions to process and evaluate measured data from the memory device, and to output a perturbation signal and an impedance spectra, wherein the instructions to process and evaluate measured data comprise a non-stationary time to frequency transformation.

22. The apparatus as defined in claim 21, wherein the non-stationary time to frequency transformation is a short time Fourier transform.

23. The apparatus as defined in claim 21, wherein the non-stationary time to frequency transformation is a wavelet transform.

24. The apparatus as defined in claim 21, wherein the non-stationary time to frequency transformation is a Wigner distribution.

25. The apparatus as defined in claim 21, wherein the perturbation signal is continuously recorded.

26. The apparatus as defined in claim 21, wherein the perturbation signal is partly continuously recorded.

27. The apparatus as defined in claim 21, wherein the perturbation signal is structured noise.

28. The apparatus as defined in claim 21, further comprising use of a complex nonlinear least square method to fit parameters of an equivalent circuit to the impedance spectra.

29. The apparatus as defined in claim 21, further comprising the use of multielectrode arrangements.

30. The apparatus as defined in claim 21, further comprising use of automatic liquid handling systems.

31. The apparatus as defined in claim 21, further comprising use of a multiple measuring chamber systems with parallel data acquisition and analysis.

32. The apparatus as defined in claim 21, further comprising use of a multiple measuring chamber systems with sequential data acquisition and analysis.

33. The apparatus as defined in claim 21, further comprising a measuring cell or chamber for detection of the conductivity of natural or artificial freely-suspended or substrate-suspended lipid membranes with or without ion channels.

34. The apparatus as defined in claim 21, further comprising a measuring cell or chamber for detection of compounds in solutions with a conductivity changing effect in regard to biomembranes.

35. The apparatus as defined in claim 21, further comprising the use of a measuring cell or chamber with temperature control and liquid handling.