Method and apparatus for determining Characteristic parameters of a charge storage device

• US 6,160,382 A
• Filed: 07/21/1999
• Issued: 12/12/2000
• Est. Priority Date: 11/19/1998
• Status: Expired due to Term

• Current Assignee: Korea Kumho Petrochemical Co Limited (Korea Kumho Petrochemical)
• Original Assignee: Korea Kumho Petrochemical Co Limited (Korea Kumho Petrochemical)
• Inventors: Kim, Jong Hyun, Barsukov, Yevgen, Yoon, Chul Oh
• Primary Examiner(s): Tso, Edward H.
• Assistant Examiner(s): TOATLEY, GREGORY J
• Application Number:
  US09/358,264
• Time in Patent Office: 510 Days
• Field of Search: 320/134, 320/136, 320/106, 395/500.35, 702/65, 324/426
• US Class Current: 320/136
• CPC Class Codes: G01R 31/367 Software therefor, e.g. for battery testing using modelling or look-up tables
• CPC Class Codes: G01R 31/389 Measuring internal impedance, internal conductance or related variables

Abstract

A method and an apparatus for determining characteristic parameters of a charge storage device based on a wide frequency range of impedance measurement and a non-linear equivalent circuit model by which the parameters of the non-linear equivalent circuit model indicative of the characteristics of various charge storage devices such as a primary battery, secondary battery, capacitor, supercapacitor and fuel cell are determined, the method comprising the steps of: (1) measuring voltage and current characteristics in a process of charging/discharging of the charge storage device by applying a voltage/current at a predetermined discharge rate; (2) measuring impedance spectra at a predetermined range of frequency by measuring the current and voltage from both terminals of the charge storage device or from an electrical load directly connected to the charge storage device at a plurality of states of charge within the entire charge/discharge interval; and (3) obtaining the parameters of the non-linear equivalent circuit of the charge storage device from the charge or discharge characteristics measured in step (1) and the characteristic impedance spectrum in the predetermined range of frequency measured in step (2).

Claims

1. A method of determining characteristic parameters of a charge storage device, based on a wide frequency range of impedance measurements and a non-linear equivalent circuit model, which is used to obtain the parameters of the charge storage device such as a primary battery, secondary battery, capacitor, supercapicitor and fuel cell, the method comprising the steps of:

(1) measuring voltage and current characteristics in a process of charging/discharging of charge storage device by applying a voltage/current at a predetermined discharge rate;

(2) measuring impedance spectra at a predetermined range of frequency by measuring the current and voltage from both terminals of the charge storage device or from an electrical load directly connected to the charge storage device at a plurality of states of charge within the entire charge/discharge interval; and

(3) obtaining the parameters of the non-linear equivalent circuit of the charge storage device from the charge or discharge characteristics measured in step (1) and the characteristic impedance spectrum in the predetermined range of frequency measured in step (2).

2. The method as claimed in claim 1, wherein step (1) of measuring the voltage and current characteristics comprises measuring voltage at both terminals of the charge storage device when an input current having a predetermined discharge rate is applied to the charge storage device;

and calculating an instantaneous change of the discharge voltage and storing data at each state of charge.

3. The method as claimed in claim 1, wherein in step (1), the input current having the predetermined discharge rate is sufficiently low enough to maintain steady-state for the instantaneous change (dE/dq) of the voltage (E) with respect to a discharge capacity (q) when it is applied to the charge storage device, the input current being expressed in mA less than a value obtained by dividing a nominal capacity expressed in mAh by one or more hrs.

4. The method as claimed in claim 1, wherein in step (2), the characteristic impedance spectrum is measured by a frequency scan method in which a series of sine waves having selected frequencies in a predetermined range of frequency are applied to the charge storage device as an input signal, and current and voltage signals measured at both terminals of the charge storage device are analyzed.

5. The method as claimed in claim 1, wherein in step (2), the characteristic impedance spectrum is measured by a Fourier transform method in which an input current or voltage composed by superposing multiple waves at selected non-overlapping frequencies in a predetermined range of frequency is applied to both terminals of the charge storage device and the current and voltage obtained are Fourier transformed to obtain the characteristic impedance spectrum.

6. The method as claimed in claim 1, wherein in step (2), the characteristic impedance spectrum is measured by a Laplace transform method in which voltage and current are measured by applying a current or voltage having a specified waveform in a predetermined range of frequency to said both terminals of the charge storage device or connecting an electrical load to the charge storage device which is Laplace transformed through a numerical analysis to obtain the impedance spectrum.

7. The method as claimed in claim 1, wherein in step (2), the characteristic impedance spectrum is measured by at least two methods selected from a frequency scan method in which a series of sine waves having selected frequencies in a predetermined range of frequency are applied to the charge storage device as an input signal, and current and voltage signals measured at both terminals of the charge storage device are analyzed;

a Fourier transform method in which an input current or voltage composed by superposing multiple waves at selected non-overlapping frequencies is applied to said both terminals of the charge storage device and the current and voltage obtained are Fourier transformed; and

a Laplace transform method in which voltage and current measured by applying a current or voltage having a specified waveform in a predetermined range of frequency to said both terminals of the charge storage device or by connecting an electrical load to the charge storage device is Laplace transformed by a numerical analysis.

8. The method as claimed in any one of claims 1 or 4 to 7, wherein the predetermined range of frequency is selected to have the ratio of the maximum frequency to the minimum frequency greater than 100.

9. The method as claimed in claim 1, wherein the non-linear equivalent circuit of the charge storage device in step (3) includes at least two elements selected from a resistor, capacitor, inductor, transmission line or a finite number of ladder-type two-terminals in place of the transmission lines.

10. The method as claimed in claim 1, wherein the non-linear equivalent circuit of the charge storage device in step (3) includes at least two elements selected from a resistor, capacitor, inductor, transmission line or a finite number of ladder-type two terminals in place of the transmission lines.

11. The method as claimed in claim 9 or 10, wherein the ladder-type two-terminals have a predetermined number of two-terminal circuits in the range of 20 μ

sec to 2,000 sec of time constant connected in parallel.

12. The method as claimed in claim 1, wherein the parameters in step (3) are components constituting the non-linear equivalent circuit of the charge storage device and include at least two elements selected from a serial resistance, macroscopic distributed resistance, charge transfer resistance, double layer capacitance, charge storage capacitance, pseudocapacitance, diffusion coefficient, open circuit voltage and instantaneous charge rate of voltage.

13. The method as claimed in claim 1, wherein the parameters in step (3) are determined from a complex impedance spectra by a non-linear least square fitting.

14. The method as claimed in claim 1, wherein the parameters in step (3) are determined from a slope of voltage characteristics vs. discharge capacity.

37. The method as claimed in claim 10, wherein the ladder type two-terminals have a predetermined number of two-terminal circuits in the range of 20 μ

sec to 2,000 sec of time constant connected in parallel.

15. A method of determining characteristic parameters of a charge storage device, based on a wide frequency range of impedance measurements and a non-linear equivalent circuit model, which is used to obtain the parameters of the charge storage device such as a primary battery, secondary battery, capacitor, supercapacitor and fuel cell in a certain state of charge, the method comprising the steps of:

(1) measuring a impedance spectrum in a predetermined range of frequency from voltage and current applied to both terminals of the charge storage device in the corresponding state of charge; and

(2) determining parameters of the non-linear equivalent circuit of the charge storage device in the corresponding state of charge from the measured impedance spectrum in the predetermined range of frequency.

16. The method as claimed in claim 15, wherein in step (1), the impedance spectrum is measured by a frequency scan method in which a series of sine waves having selected frequencies in a predetermined range of frequency are applied to the charge storage device as an input signal and current;

and voltage signals measured at said both terminals of the charge storage device are analyzed.

17. The method as claimed in claim 15, wherein in step (1), the impedance spectrum is measured by a Fourier transform method in which an input current or voltage composed of superposing multiple waves at selected non-overlapping frequencies in a predetermined range of frequency is applied to said both terminals of the charge storage device and the current and voltage obtained are Fourier transformed to measure the impedance spectrum.

18. The method as claimed in claim 15, wherein in step (1), the impedance spectrum is measured by a Laplace transform method in which voltage and current measured by applying a current or voltage having a specified waveform in a predetermined range of frequency to said both terminals of the charge storage device or by connecting an electrical load to the charge storage device is Laplace transformed by a numerical analysis to obtain the impedance spectrum.

19. The method as claimed in claim 15, wherein in step (1), the impedance spectrum is measured by at least two methods selected from a frequency scan method in which a series of sine waves having selected frequencies in a predetermined range of frequency are applied to the charge storage device as an input signal and the current and voltage signals measured at said both terminals of the charge storage device are analyzed;

a Fourier transform method in which, an input current or voltage composed of superposing multiple waves at selected non-overlapping frequencies in a predetermined range of frequency is applied to said both terminals of the charge storage device and the current and voltage obtained are Fourier transformed; and

a Laplace transform method in which the voltage and current measured by applying a current or voltage having a specified waveform in a predetermined range of frequency to said both terminals of the charge storage device or by connecting an electrical load to the charge storage device is Laplace transformed by a numerical analysis.

20. The method as in one of claims claims 15-19, wherein the predetermined range of frequency is selected to have a ratio in which the maximum frequency to the minimum frequency is greater than 100.

21. The method as claimed in claim 15, wherein the non-linear equivalent of the charge storage device in step (2) includes at least two elements selected from a resistor, capacitor, inductor, transmission line or a finite number of ladder-type two terminals in place of the transmissions lines.

22. The method as claimed in claim 15, wherein the non-linear equivalent circuit of the charge storage device in step (2) includes at least two elements selected from a constant current source, constant voltage source, non-linear resistor, non-linear capacitor, non-linear inductor, non-linear transmission line or a finite number of ladder-type non-linear two-terminals in place of the transmission lines.

23. The method as claimed in claim 21 or 22, wherein the ladder type two-terminals have a predetermined number of two-terminal circuits in the range of °

μ

sec to 2,000 sec of time constant connected in parallel.

24. The method as claimed in claim 15, wherein the parameters in step (2) are components constituting the non-linear equivalent circuit of the charge storage device and include at least two elements selected from a serial resistance, macroscopic distributed resistance, charge transfer resistance, double layer capacitance, charge storage capacitance, pseudocapacitance, diffusion coefficient, open circuit voltage and instantaneous change rate of voltage.

25. The method as claimed in claim 15, wherein the parameters in step (2) are determined from a complex impedance spectra by a non-linear least square fitting.

26. The method as claimed in claim 15 or 24, wherein the parameters in step (2) are determined from a slope of voltage characteristics vs. discharge capacity.

27. The method as claimed in claim 15, wherein the parameters of the non-linear equivalent circuit of the charge storage device are obtained, and an open circuit voltage of the charge storage device in a predetermined state of charge is also measured at the same time.

38. The method as claimed in claim 22, wherein the ladder type two-terminals have a predetermined number of two-terminal circuits in the range of 20 μ

sec to 2,000 sec of time constant connected in parallel.

28. An apparatus for determining parameters of a charge storage device by a wide frequency range of impedance measurements and a non-linear equivalent circuit model comprising:

a control means for determining parameters of the charge storage device and simulating various operational characteristics of a circuit including a charge storage device using the determined parameters;

a digital-to-analog converter for converting a predetermined voltage and current data output from the control means to an analog signal;

a potentiostat and/or galvanostat for applying the output signal of the digital-to-analog converter to the charge storage device to output the voltage and current of the capacitor;

an analog-to-digital converter for converting a voltage based on the voltage and current of the charge storage device output from the potentiostat and/or galvanostat and feeding them into the control means; and

a circuit simulator for simulating various operational characteristics of a charge storage device based on the parameters obtained from the control means for a predetermined equivalent circuit including the charge storage device.

29. The apparatus as claimed in claim 28, wherein the control means comprises:

an I/O interface unit for interfacing the capacitor and a predetermined data;

a central processing unit for controlling an operation for measuring voltage, current and impedance spectra of the charge storage device;

means for measuring the voltage/current characteristic of the charge storage device under the control of the central processing unit;

means for measuring the impedance spectra of the charge storage device under the control of the central processing unit; and

means for determining the non-linear parameters by differentiating the measured values from the voltage/current measuring means and the impedance spectra as a function of charge capacity and performing a non-linear least square fitting from the differentiated values.

30. The apparatus as claimed in claim 29, wherein the impedance spectra measuring means measures the impedance spectra by detecting the voltage and current of the charge storage device while it outputs digital data of the voltage and current based on a plurality of predetermined frequencies sequentially;

and performs a calculation on the detected voltage and current of the charge storage device.

31. The apparatus according to claim 30, wherein the detected voltage and current of the charge storage device are calculated by a amplitude/phase shift or Fourier transform method.

32. The apparatus as claimed in claim 29, wherein the impedance spectra measuring means measures the impedance spectra by measuring voltage and current while it applies superposed multiple wave signals selected at predetermined non-overlapping frequencies to the charge storage device, performing the Fourier transform of the measured voltage and current, and performing a calculation on a power spectrum.

33. The apparatus as claimed in claim 29, wherein the impedance spectra measuring means measures the impedance spectra by measuring voltage and current while it outputs voltage and current data having a specified waveform and applies them to the charge storage device, performing a linear regression of the measured voltage and current to calculate the impedance spectra, and performing a calculation on an error function of the impedance.

34. The apparatus as claimed in claim 28, further comprising a separate voltage/current generator for generating a voltage/current based on the digital data output from the control means and applying it to the charge storage device.

35. The apparatus as claimed in claim 28, wherein the galvanostat comprises:

an inversion amplifier for inversion amplifying the output signal of the digital-to-analog converter and applying it to the (-) terminal of the charge storage device;

a buffer for outputting voltages at said both terminals of the charge storage device; and

a current-detecting resistance connected in series with the charge storage device for detecting the current of the charge storage device.

36. The apparatus as claimed in claim 28, further comprising first and second filter/amplifiers between the galvanostat and the analog-to-digital converter for filtering the voltage and current of the charge storage device detected by the galvanostat for removing noises and amplifying the voltage and current.