JP5751207B2 - Battery DC resistance evaluation device - Google Patents
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- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R31/00—Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
- G01R31/36—Arrangements for testing, measuring or monitoring the electrical condition of accumulators or electric batteries, e.g. capacity or state of charge [SoC]
- G01R31/389—Measuring internal impedance, internal conductance or related variables
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B60—VEHICLES IN GENERAL
- B60L—PROPULSION OF ELECTRICALLY-PROPELLED VEHICLES; SUPPLYING ELECTRIC POWER FOR AUXILIARY EQUIPMENT OF ELECTRICALLY-PROPELLED VEHICLES; ELECTRODYNAMIC BRAKE SYSTEMS FOR VEHICLES IN GENERAL; MAGNETIC SUSPENSION OR LEVITATION FOR VEHICLES; MONITORING OPERATING VARIABLES OF ELECTRICALLY-PROPELLED VEHICLES; ELECTRIC SAFETY DEVICES FOR ELECTRICALLY-PROPELLED VEHICLES
- B60L58/00—Methods or circuit arrangements for monitoring or controlling batteries or fuel cells, specially adapted for electric vehicles
- B60L58/10—Methods or circuit arrangements for monitoring or controlling batteries or fuel cells, specially adapted for electric vehicles for monitoring or controlling batteries
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- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R19/00—Arrangements for measuring currents or voltages or for indicating presence or sign thereof
- G01R19/165—Indicating that current or voltage is either above or below a predetermined value or within or outside a predetermined range of values
- G01R19/16528—Indicating that current or voltage is either above or below a predetermined value or within or outside a predetermined range of values using digital techniques or performing arithmetic operations
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R19/00—Arrangements for measuring currents or voltages or for indicating presence or sign thereof
- G01R19/165—Indicating that current or voltage is either above or below a predetermined value or within or outside a predetermined range of values
- G01R19/16533—Indicating that current or voltage is either above or below a predetermined value or within or outside a predetermined range of values characterised by the application
- G01R19/16538—Indicating that current or voltage is either above or below a predetermined value or within or outside a predetermined range of values characterised by the application in AC or DC supplies
- G01R19/16542—Indicating that current or voltage is either above or below a predetermined value or within or outside a predetermined range of values characterised by the application in AC or DC supplies for batteries
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R27/00—Arrangements for measuring resistance, reactance, impedance, or electric characteristics derived therefrom
- G01R27/02—Measuring real or complex resistance, reactance, impedance, or other two-pole characteristics derived therefrom, e.g. time constant
- G01R27/08—Measuring resistance by measuring both voltage and current
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- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R31/00—Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
- G01R31/36—Arrangements for testing, measuring or monitoring the electrical condition of accumulators or electric batteries, e.g. capacity or state of charge [SoC]
- G01R31/3644—Constructional arrangements
- G01R31/3648—Constructional arrangements comprising digital calculation means, e.g. for performing an algorithm
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- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R31/00—Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
- G01R31/36—Arrangements for testing, measuring or monitoring the electrical condition of accumulators or electric batteries, e.g. capacity or state of charge [SoC]
- G01R31/374—Arrangements for testing, measuring or monitoring the electrical condition of accumulators or electric batteries, e.g. capacity or state of charge [SoC] with means for correcting the measurement for temperature or ageing
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- G—PHYSICS
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- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R31/00—Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
- G01R31/36—Arrangements for testing, measuring or monitoring the electrical condition of accumulators or electric batteries, e.g. capacity or state of charge [SoC]
- G01R31/382—Arrangements for monitoring battery or accumulator variables, e.g. SoC
- G01R31/3842—Arrangements for monitoring battery or accumulator variables, e.g. SoC combining voltage and current measurements
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01M—PROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
- H01M10/00—Secondary cells; Manufacture thereof
- H01M10/42—Methods or arrangements for servicing or maintenance of secondary cells or secondary half-cells
- H01M10/48—Accumulators combined with arrangements for measuring, testing or indicating the condition of cells, e.g. the level or density of the electrolyte
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E60/00—Enabling technologies; Technologies with a potential or indirect contribution to GHG emissions mitigation
- Y02E60/10—Energy storage using batteries
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Description
本発明は、電池直流抵抗評価装置に関し、詳しくは、リチウムイオン電池などの二次電池の内部直流抵抗測定における効率改善に関するものである。 The present invention relates to a battery direct current resistance evaluation apparatus, and more particularly to an improvement in efficiency in measuring internal direct current resistance of a secondary battery such as a lithium ion battery.
ハイブリッド電気自動車などに用いられる二次電池の性能評価指標の一つに、電池内部の直流抵抗(DCR;Direct Current Resistance)があり、このDCRの具体的な試験方法は、たとえば「日本電動車両協会規格JEVS D714 ハイブリッド自動車用密閉形ニッケル・水素電池の直流抵抗算出方法」(非特許文献1)により規定され、公表されている。 One of the performance evaluation indexes of secondary batteries used in hybrid electric vehicles and the like is the direct current resistance (DCR) inside the battery. A specific test method for this DCR is, for example, “Japan Electric Vehicle Association”. Standard JEVS D714 “Method for calculating direct current resistance of sealed nickel-hydrogen battery for hybrid vehicle” (Non-patent Document 1).
図12は、従来のDCR測定系の一例を示すブロック図である。図12において、測定対象の電池1には、電池1に充放電パルスを印加する充放電装置2と、充放電装置2を駆動制御するとともに充放電パルス印加時における電池1の電圧および電流を測定する電圧・電流測定装置3が接続されている。そして、電圧・電流測定装置3には、DCR解析装置4が接続されている。 FIG. 12 is a block diagram showing an example of a conventional DCR measurement system. In FIG. 12, the battery 1 to be measured includes a charge / discharge device 2 that applies a charge / discharge pulse to the battery 1, a drive control of the charge / discharge device 2, and the voltage and current of the battery 1 when the charge / discharge pulse is applied. A voltage / current measuring device 3 is connected. A DCR analyzer 4 is connected to the voltage / current measuring device 3.
このような構成において、DCR測定にあたり、充放電装置2は、電池1に対して、たとえば定格容量が20Ahの場合には、図13に示すようなシーケンスで所定レベルを有する充放電電流パルス波形を印加する。電圧・電流測定装置3は、たとえば図14に示すように、印加された電流パルス波形による放電電流ΔIに対する電池1の応答電圧ΔVを測定する。そして、DCR解析装置4は、これら応答電圧ΔVと放電電流ΔIの商を演算してDCR(=ΔV/ΔI)を算出する。 In such a configuration, in the DCR measurement, the charging / discharging device 2 generates a charging / discharging current pulse waveform having a predetermined level in a sequence as shown in FIG. 13 when the rated capacity is 20 Ah, for example. Apply. For example, as shown in FIG. 14, the voltage / current measuring device 3 measures a response voltage ΔV of the battery 1 with respect to the discharge current ΔI by the applied current pulse waveform. The DCR analyzer 4 calculates DCR (= ΔV / ΔI) by calculating a quotient of the response voltage ΔV and the discharge current ΔI.
図15は、DCR解析装置4の具体的な構成例を示すブロック図である。図15において、入力部41を介してDCR演算部42に測定時刻ポイントを含むDCR測定条件と応答電圧が入力される。DCR演算部42は、前述の演算式DCR(=ΔV/ΔI)に基づいて、DCR測定条件で指定された各測定時刻ポイントにおけるDCRを算出する。ここで、ΔVは応答電圧の降下幅であり、ΔIは電流パルスのレベルである。 FIG. 15 is a block diagram illustrating a specific configuration example of the DCR analysis apparatus 4. In FIG. 15, the DCR measurement condition including the measurement time point and the response voltage are input to the DCR calculation unit 42 via the input unit 41. The DCR calculator 42 calculates the DCR at each measurement time point specified by the DCR measurement condition based on the above-described arithmetic expression DCR (= ΔV / ΔI). Here, ΔV is the drop width of the response voltage, and ΔI is the level of the current pulse.
しかし、上記従来のDCR測定系によれば、電池1に対して比較的大きな充放電パルスを印加することから、電池1の出力に現れる摂動も大きくなってしまう。この結果、以下のような問題が発生することになる。 However, according to the conventional DCR measurement system, since a relatively large charge / discharge pulse is applied to the battery 1, the perturbation that appears in the output of the battery 1 also increases. As a result, the following problems occur.
1)充放電パルス印加後、電池1を安定状態に回復させるためには長い休止時間を取る必要がある。休止時間を設けないと、測定の再現性が確保できない。よって、従来のDCR測定系を用いてたとえば電池の製造ラインでDCR検査を行う場合にはかなりの検査時間がかかることになり、生産性が悪い。 1) It is necessary to take a long rest time in order to restore the battery 1 to a stable state after applying the charge / discharge pulse. Without a downtime, measurement reproducibility cannot be ensured. Therefore, when a conventional DCR measurement system is used, for example, when a DCR inspection is performed in a battery production line, a considerable inspection time is required, and productivity is poor.
2)測定する電池1の容量によっては大容量の電源を必要とする。また、大容量の電源を用いた場合には、これらの機器から発するノイズなどの影響を受けやすく、安定した測定を行うためにはノイズ対策なども必要になる。 2) Depending on the capacity of the battery 1 to be measured, a large capacity power supply is required. In addition, when a large-capacity power supply is used, it is easily affected by noise generated from these devices, and noise countermeasures are necessary to perform stable measurement.
本発明は、これらの問題を解決するものであり、その目的は、大容量の電源を用いることなく、短時間で効率よく測定が行える電池直流抵抗評価装置を提供することにある。 The present invention solves these problems, and an object of the present invention is to provide a battery direct current resistance evaluation apparatus that can perform measurement efficiently in a short time without using a large-capacity power source.
このような課題を達成するために、本発明のうち請求項1記載の発明は、
二次電池の内部直流抵抗を測定する電池直流抵抗評価装置であって、
測定対象電池の交流インピーダンスを測定するインピーダンス測定手段と、
このインピーダンス測定手段の測定結果と選択された等価回路に基づき演算される回路定数と電池直流抵抗測定条件の電流値と開路電圧値(OCV)の変化分に基づき前記測定対象電池の応答電圧を算出するとともに内部直流抵抗値を算出する直流抵抗値解析手段を設け、
前記直流抵抗値解析手段は、電池の充電状態(SOC)を変えながらOCVデータを測定して作成されたSOC-OCVテーブルを用いて前記応答電圧を算出することを特徴とする。
In order to achieve such a problem, the invention according to claim 1 of the present invention is:
A battery DC resistance evaluation device for measuring the internal DC resistance of a secondary battery,
Impedance measuring means for measuring the AC impedance of the battery to be measured;
The response voltage of the battery to be measured is calculated based on the circuit constant calculated based on the measurement result of this impedance measuring means and the selected equivalent circuit, the current value of the battery DC resistance measurement condition, and the change in the open circuit voltage value (OCV). And providing a DC resistance value analyzing means for calculating the internal DC resistance value ,
The DC resistance value analyzing means calculates the response voltage using an SOC-OCV table created by measuring OCV data while changing the state of charge (SOC) of the battery.
請求項2記載の発明は、
二次電池の内部直流抵抗を測定する電池直流抵抗評価装置であって、
測定対象電池の交流インピーダンスを測定するインピーダンス測定手段と、
このインピーダンス測定手段の測定結果と選択された等価回路に基づき演算される回路定数と電池直流抵抗測定条件の電流値と開路電圧値(OCV)の変化分に基づき前記測定対象電池の応答電圧を算出するとともに内部直流抵抗値を算出する直流抵抗値解析手段を設け、
前記直流抵抗値解析手段は、温度を変えながら測定されたOCVデータを用いて前記応答電圧を補正することを特徴とする。
The invention according to claim 2
A battery DC resistance evaluation device for measuring the internal DC resistance of a secondary battery,
Impedance measuring means for measuring the AC impedance of the battery to be measured;
The response voltage of the battery to be measured is calculated based on the circuit constant calculated based on the measurement result of this impedance measuring means and the selected equivalent circuit, the current value of the battery DC resistance measurement condition, and the change in the open circuit voltage value (OCV). And providing a DC resistance value analyzing means for calculating the internal DC resistance value,
The DC resistance value analyzing means corrects the response voltage using OCV data measured while changing the temperature.
請求項3記載の発明は、請求項1または請求項2に記載の電池直流抵抗評価装置において、
前記等価回路として、CPEが直列接続された回路を用いることを特徴とする。
A third aspect of the present invention is the battery direct-current resistance evaluation apparatus according to the first or second aspect ,
As the equivalent circuit, a circuit in which CPEs are connected in series is used .
請求項4記載の発明は、請求項1から請求項3のいずれかに記載の電池直流抵抗評価装置において、
前記等価回路の回路定数は、温度を変えながら測定されたインピーダンスデータを用いて前記回路定数を補正することを特徴とする。
According to a fourth aspect of the present invention, in the battery direct-current resistance evaluation apparatus according to any one of the first to third aspects,
The circuit constant of the equivalent circuit is corrected using impedance data measured while changing the temperature .
本発明の電池直流抵抗評価装置によれば、大容量の電源を用いることなく、短時間で効率よく電池の直流抵抗測定が行える。 According to the battery direct current resistance evaluation apparatus of the present invention, the direct current resistance of a battery can be measured efficiently in a short time without using a large-capacity power source.
以下、本発明について、図面を用いて詳細に説明する。図1は本発明の一実施例を示すブロック図であり、図12と共通する部分には同一の符号を付けている。図1と図12の相違点は、図1には図12の電圧・電流測定装置3に代えてインピーダンス測定装置6が設けられていることである。このインピーダンス測定装置6は、電池1の電気特性としてインピーダンスを測定し、その測定データをDCR解析装置4に入力する。 Hereinafter, the present invention will be described in detail with reference to the drawings. FIG. 1 is a block diagram showing an embodiment of the present invention, and the same reference numerals are given to portions common to FIG. 1 differs from FIG. 12 in that an impedance measuring device 6 is provided in FIG. 1 in place of the voltage / current measuring device 3 of FIG. The impedance measuring device 6 measures impedance as an electrical characteristic of the battery 1 and inputs the measurement data to the DCR analyzing device 4.
図2は図1で用いるDCR解析装置4の具体的な構成例を示すブロック図であり、図15と共通する部分には同一の符号を付けている。図2において、入力部44を介して、インピーダンスデータ、等価回路、SOC-OCVテーブルおよびDCR測定条件の各データが各部に出力される。 FIG. 2 is a block diagram showing a specific configuration example of the DCR analyzer 4 used in FIG. 1, and the same reference numerals are given to the portions common to FIG. In FIG. 2, impedance data, equivalent circuit, SOC-OCV table, and DCR measurement condition data are output to each unit via an input unit 44.
SOC演算部45は、DCR測定条件として規定されている充放電パルス高およびパルス発生時間から充放電量を算出することにより電池1の充電状態SOC(State of Charge)値を算出し、その演算結果をSOC-OCV演算部47に出力する。詳細な計算方法は別途説明する。 The SOC calculation unit 45 calculates the state of charge (SOC) value of the battery 1 by calculating the charge / discharge amount from the charge / discharge pulse height and the pulse generation time defined as the DCR measurement conditions, and the calculation result Is output to the SOC-OCV computing unit 47. A detailed calculation method will be described separately.
回路定数演算部46は、インピーダンス測定装置6により測定されたインピーダンスデータを用いて、等価回路として最適な回路定数を算出する。詳細な計算方法は別途説明する。 The circuit constant calculator 46 uses the impedance data measured by the impedance measuring device 6 to calculate an optimum circuit constant as an equivalent circuit. A detailed calculation method will be described separately.
SOC-OCV演算部47は、SOC-OCVテーブルからSOC値に応じた開路電圧OCV(Open circuit voltage)値を算出する。詳細な計算方法は別途説明する。 The SOC-OCV calculating unit 47 calculates an open circuit voltage OCV (Open circuit voltage) value corresponding to the SOC value from the SOC-OCV table. A detailed calculation method will be described separately.
応答電圧演算部48は、電池1へ電流パルスを印加したときの応答電圧を算出する。具体的には、等価回路、回路定数、DCR測定条件およびOCV値を用いて、電池1の内部インピーダンスに電流パルスを印加した際に発生する電圧変化と内部起電力の和で算出される。詳細な計算方法は別途説明する。 The response voltage calculation unit 48 calculates a response voltage when a current pulse is applied to the battery 1. Specifically, using the equivalent circuit, circuit constant, DCR measurement condition, and OCV value, it is calculated as the sum of the voltage change and the internal electromotive force generated when a current pulse is applied to the internal impedance of the battery 1. A detailed calculation method will be described separately.
それぞれの詳細な計算方法の説明にあたり、各データについて説明する。
図3は、インピーダンス測定装置6により測定された電池1のインピーダンスデータ例図である。特性曲線CHaはインピーダンスの測定結果を示し、特性曲線CHbは位相の測定結果を示している。
In describing each detailed calculation method, each data will be described.
FIG. 3 is an example of impedance data of the battery 1 measured by the impedance measuring device 6. The characteristic curve CHa shows the impedance measurement result, and the characteristic curve CHb shows the phase measurement result.
図4は電池の等価回路の説明図であり、(A)は具体的な等価回路例図、(B)は(A)の回路における各素子の具体的な回路定数例リストである。ここで、(A)の抵抗R1は電池内部の電解液の抵抗を表し、抵抗R2とコンデンサC2の並列回路は電池の一方の電極の抵抗と静電容量を表し、抵抗R3とコンデンサC3の並列回路は電池の他方の電極の抵抗と静電容量を表している。これら3個の抵抗R1〜R3は、特開2001−231179号公報の図3にも記載されているように、周波数帯域によって応答周波数が異なることから、3つに分けて表している。
FIG. 4 is an explanatory diagram of an equivalent circuit of a battery , (A) is a specific equivalent circuit diagram, and (B) is a list of specific circuit constant examples of each element in the circuit (A). Here, the resistor R1 in (A) represents the resistance of the electrolyte inside the battery, the parallel circuit of the resistor R2 and the capacitor C2 represents the resistance and capacitance of one electrode of the battery, and the resistor R3 and the capacitor C3 in parallel. The circuit represents the resistance and capacitance of the other electrode of the battery. These three resistors R1 to R3 are divided into three because the response frequency varies depending on the frequency band as described in FIG. 3 of Japanese Patent Laid-Open No. 2001-231179.
図5は、SOC-OCVテーブルの具体例図である。電池1のSOC値が0〜100%の範囲で10%毎に異なる場合について、各OCV値を測定して作成されたものである。 FIG. 5 is a specific example of the SOC-OCV table. It is created by measuring each OCV value when the SOC value of the battery 1 is different every 10% in the range of 0 to 100%.
SOC値は、SOC演算部45において、所定のDCR測定条件に基づいて演算された各測定時間における演算値である。 The SOC value is a calculated value at each measurement time calculated based on predetermined DCR measurement conditions in the SOC calculation unit 45.
OCV値は、SOC-OCV演算部47により算出された各測定時間における開回路電圧値である。 The OCV value is an open circuit voltage value at each measurement time calculated by the SOC-OCV calculation unit 47.
応答電圧は、応答電圧演算部48で算出された応答電圧である。 The response voltage is a response voltage calculated by the response voltage calculation unit 48.
電池1の電気特性について説明する。
起電力は電池1の起電力であり、OCV値として算出される。
内部インピーダンスは電池1の内部インピーダンスであり、1つあるいは複数の回路素子で構成され、各素子の定数は回路定数演算部46で算出される。
The electrical characteristics of the battery 1 will be described.
The electromotive force is an electromotive force of the battery 1 and is calculated as an OCV value.
The internal impedance is the internal impedance of the battery 1 and is composed of one or a plurality of circuit elements, and the constant of each element is calculated by the circuit constant calculation unit 46.
[応答電圧の算出]
電池1に発生する応答電圧E0は、図6の等価回路に示すように次のE1とE2との和からなる。
a)内部起電力;E1
b)内部インピーダンスによる電圧変化;E2
[Calculation of response voltage]
The response voltage E0 generated in the battery 1 is the sum of the following E1 and E2 as shown in the equivalent circuit of FIG.
a) Internal electromotive force; E1
b) Voltage change due to internal impedance; E2
起電力の電圧E1は、電流の印加状態にはよらない電圧であるが、SOCにより変化する。一般に、放電時には電池1の端子間電圧E0は低下するものとして知られているが、ここではこのような電圧降下は内部インピーダンスによるものである。電流の印加状態にはよらないので、電池1のOCVを測定することで起電力の電圧E1を決定することができる。 The voltage E1 of the electromotive force is a voltage that does not depend on the current application state, but varies depending on the SOC. In general, it is known that the voltage E0 between the terminals of the battery 1 decreases during discharging, but here, such a voltage drop is due to internal impedance. Since it does not depend on the current application state, the voltage E1 of the electromotive force can be determined by measuring the OCV of the battery 1.
内部インピーダンスは、電池1の材質や構造により決定されるインピーダンスである。電流印加時には電圧が発生し、放電時には起電力の電圧とは逆の向きに電圧が発生する。同一規格の電池であっても、内部インピーダンスには個体差があり、これがDCR検査結果の差として現れる。 The internal impedance is an impedance determined by the material and structure of the battery 1. A voltage is generated when a current is applied, and a voltage is generated in a direction opposite to that of the electromotive force during discharge. Even with batteries of the same standard, there are individual differences in internal impedance, and this appears as a difference in DCR test results.
本発明の装置では、電池1の起電力(図6のE1)と、電池1の内部インピーダンスに電流を印加した際に発生する電圧変化(図6のE2)との和を求めて、応答電圧E0とする。 In the apparatus of the present invention, the sum of the electromotive force of the battery 1 (E1 in FIG. 6) and the voltage change (E2 in FIG. 6) generated when a current is applied to the internal impedance of the battery 1 is obtained, and the response voltage Let E0.
[内部インピーダンスによる電圧変化]
時間tにおける電流パルスX(t)に対し、応答電圧e(t)を算出する。
本発明では、電池1の内部インピーダンスを、抵抗と複数のRC並列回路が直列に接続された回路で近似する。つまり、電池1の内部インピーダンスは抵抗と各RC並列回路のインピーダンスの和である。
であり、内部インピーダンスにかかる電圧e(t)は各インピーダンスにかかる電圧の和である。
[Voltage change due to internal impedance]
A response voltage e (t) is calculated for the current pulse X (t) at time t.
In the present invention, the internal impedance of the battery 1 is approximated by a circuit in which a resistor and a plurality of RC parallel circuits are connected in series. That is, the internal impedance of the battery 1 is the sum of the resistance and the impedance of each RC parallel circuit.
The voltage e (t) applied to the internal impedance is the sum of the voltages applied to the respective impedances.
たとえば図7のような直列回路にかかる電圧の和は以下の式で求められる。
e(t)=eA(t)+eB(t)+eC(t)
For example, the sum of the voltages applied to the series circuit as shown in FIG.
e (t) = e A (t) + e B (t) + e C (t)
たとえばeA(t)は、複素数領域sにおける電圧EA(s)の逆ラプラス変換により求める。
ただし、s=jωである(ωは角周波数)。
For example, e A (t) is obtained by inverse Laplace transform of the voltage E A (s) in the complex number region s.
However, s = jω (ω is an angular frequency).
たとえばEA(s)は、次式で求めることができる。
EA(s)=ZA(s)×I(s)
ZA(s) :s領域におけるインピーダンス
I(s) :s領域における電流
For example, E A (s) can be obtained by the following equation.
E A (s) = Z A (s) × I (s)
Z A (s): impedance in the s region I (s): current in the s region
[回路定数の算出]
内部インピーダンスを近似する回路は、電池1のインピーダンス測定と、そのデータを用いた回路中の回路定数の最適化により求める。
最適な回路定数は、y−f(x)の二乗和を最小にする回路定数xであり、最小二乗法により求める。ここではインピーダンスデータをyとし、インピーダンスの計算式には関数f(x)とする。解法のアルゴリズムには、ガウス・ニュートン法やLevenberg-Marquardt法を用いることができる。
[Calculating circuit constants]
A circuit approximating the internal impedance is obtained by measuring the impedance of the battery 1 and optimizing circuit constants in the circuit using the data.
The optimum circuit constant is a circuit constant x that minimizes the sum of squares of y−f (x), and is obtained by the least square method. Here, the impedance data is y, and the impedance calculation formula is a function f (x). As a solution algorithm, Gauss-Newton method or Levenberg-Marquardt method can be used.
[s領域における電流]
DCR評価において、電池1に印加する電流X(t)は、図8に示すような時間を変数とする充放電電流のステップ関数Xk(t)の和である。
[Current in s region]
In the DCR evaluation, the current X (t) applied to the battery 1 is the sum of the step function X k (t) of the charge / discharge current with the time as a variable as shown in FIG.
そして内部インピーダンスにかかる電圧e(t)は、各ステップ関数により発生する応答電圧ek(t)の和である。 The voltage e (t) applied to the internal impedance is the sum of the response voltage e k (t) generated by each step function.
ラプラス変換は線形性があるので、各ステップ関数により発生する応答電圧をs領域で求め、和算して求めることができる。 Since the Laplace transform has linearity, the response voltage generated by each step function can be obtained in the s region and summed.
Ik(s)は、時間領域における電流をラプラス変換して求める。たとえばt=0においてΔIk変化する電流は、ステップ関数で次のように表すことができる。
0 :t<0
ΔIk :t≧0
Ik (s) is obtained by performing Laplace transform on the current in the time domain. For example, a current that changes by ΔI k at t = 0 can be expressed as a step function as follows.
0: t <0
ΔI k : t ≧ 0
これは単位ステップ関数u(t)を用いると次のように表すことができる。
ΔIk×u(t)
つまり、次式のように表すことができる。
Ik(s)=L[ΔIk×u(t)]=ΔIk/s
This can be expressed as follows using the unit step function u (t).
ΔI k × u (t)
That is, it can be expressed as:
I k (s) = L [ΔI k × u (t)] = ΔI k / s
図9は、DCR測定における充放電電流とSOCの変化の関係例図である。図9において、実線は電流パルスを示し、破線はSOCを示している。 FIG. 9 is a diagram illustrating a relationship between the charge / discharge current and the change in SOC in DCR measurement. In FIG. 9, a solid line indicates a current pulse, and a broken line indicates SOC.
[抵抗にかかる電圧]
抵抗の抵抗値がrのとき、電圧er(t)は、次の式により求められる。
er(t)=r×X(t)
[Voltage applied to resistance]
When the resistance value of the resistor is r, the voltage er (t) is obtained by the following equation.
e r (t) = r × X (t)
[RC回路にかかる電圧]
RC回路のインピーダンスがZrc(s)のとき、かかる電圧erc(t)は次の通りである。
[Voltage applied to RC circuit]
When the impedance of the RC circuit is Z rc (s), the voltage e rc (t) is as follows.
Ik(s)がt=tkにおいてΔIk変化する電流のステップ関数であるとき、その応答電圧Yrck(T)は以下のように求める。ただし、T=t-tkとする。 When I k (s) is a step function of current that changes ΔI k at t = t k , the response voltage Y rck (T) is obtained as follows. However, T = t−t k .
RC回路のインピーダンスZrc(s)は抵抗Rと静電容量CのRC並列回路のインピーダンスなので、次のように求まる。 Since the impedance Z rc (s) of the RC circuit is the impedance of the RC parallel circuit of the resistor R and the capacitance C, it is obtained as follows.
このとき、α=1/C、β=−1/RCとすると、Z(s)=α/(s−β)となることから、Erck(s)は以下のように表すことができる。 At this time, if α = 1 / C and β = −1 / RC, then Z (s) = α / (s−β), and thus E rck (s) can be expressed as follows.
は逆ラプラス変換すると、 Is the inverse Laplace transform,
になることから、Yrck(T)は次式のようになる。 Therefore, Y rck (T) becomes as follows.
[内部起電力]
図6に示す電池1の内部起電力E1は、OCV値で決定される。このOCV値は、以下手順にて算出する。
1)DCR充放電パルスによるSOCの変化を算出する。
2)SOCの変化によるOCV値を算出する。
[Internal electromotive force]
The internal electromotive force E1 of the battery 1 shown in FIG. 6 is determined by the OCV value. This OCV value is calculated by the following procedure.
1) The change in SOC due to the DCR charge / discharge pulse is calculated.
2) The OCV value due to the change in SOC is calculated.
[SOC算出]
DCR測定においては、電池1に対して充電あるいは放電パルスを印加するため、図5に示すように測定の進捗に応じて電池1のSOCが変化する。時間tにおけるSOC値は以下の式により算出できる。
[SOC calculation]
In DCR measurement, since a charging or discharging pulse is applied to the battery 1, the SOC of the battery 1 changes according to the progress of the measurement as shown in FIG. The SOC value at time t can be calculated by the following equation.
ここで、S0はSOCの初期値、Cmaxは電池1の最大容量、I(x)は充放電電流である。 Here, S 0 is the initial value of SOC, C max is the maximum capacity of battery 1, and I (x) is the charge / discharge current.
SOCの算出例について説明する。
大容量2400mAh、SOC 50%(1200mAh)の電池1において、2400mAで30秒間の充電パルスを印加した場合、SOCは以下の式で計算される。
{1200mAh+(2400mA*0.0083)}/2400mAh=0.5083
となり、充電パルス印加後のSOCは50.83%となる。
An example of calculating the SOC will be described.
In a battery 1 having a large capacity of 2400 mAh and SOC of 50% (1200 mAh), when a charging pulse of 2400 mA for 30 seconds is applied, the SOC is calculated by the following equation.
{1200 mAh + (2400 mA * 0.0083)} / 2400 mAh = 0.5083
Thus, the SOC after applying the charge pulse is 50.83%.
一方、最大容量2400mAh、SOC50%(1200mAh)の電池1において、2400mAで30秒間の放電パルスを印加した場合、SOCは以下の式で計算される。
{1200mAh+(−2400mA*0.0083)}/2400mAh
=0.4917
となり、放電パルス印加後のSOCは49.17%となる。
On the other hand, in a battery 1 having a maximum capacity of 2400 mAh and SOC of 50% (1200 mAh), when a discharge pulse of 2400 mA for 30 seconds is applied, the SOC is calculated by the following equation.
{1200mAh + (-2400mA * 0.0083)} / 2400mAh
= 0.4917
Thus, the SOC after application of the discharge pulse is 49.17%.
[OCV値算出]
OCVはSOCによって変化する。S(t)におけるOCVを求めるには、電池1の充電状態を変えながらOCVを測定してSOC引きのOCVテーブルを作成し、S(t)に応じて参照するようにする。中間値は、線形補間などの計算法を用いて算出する。
[OCV value calculation]
OCV varies with SOC. In order to obtain the OCV at S (t), the OCV is measured while changing the state of charge of the battery 1 to create an OCV table for SOC pulling, and the OCV table is referred to according to S (t). The intermediate value is calculated using a calculation method such as linear interpolation.
OCVの算出例について以下にて説明する。
時刻t=tkにおけるOCV値e(tk)を次の式を用いて計算する。ただし、SOC値S(tk)=50.83%、OCV1はSOC50%の時のOCV値、OCV2はSOC60%の時のOCV値である。
An example of calculating the OCV will be described below.
The OCV value e (t k ) at time t = t k is calculated using the following equation. However, the SOC value S (t k ) = 50.83%, OCV 1 is the OCV value when the SOC is 50%, and OCV 2 is the OCV value when the SOC is 60%.
この式によるOCV値の演算結果は3.727Vとなる。そして、同じ式によるSOC49.17%のOCV値は3.706Vとなる。 The calculation result of the OCV value according to this equation is 3.727V. And the OCV value of SOC 49.17% by the same formula will be 3.706V.
本発明は、交流インピーダンス測定結果に基づいて電池のDCR測定結果を推定することから、以下の効果が得られる。
1)交流インピーダンス測定は、測定のために印加する交流信号の振幅が小さくとも安定に測定できることから電池1の出力に現れる摂動を小さく抑えることができる。
2)これにより、電池1を元の状態に戻すための待機時間が不要になって測定時間を短縮でき、たとえば製造ラインにおける検査の効率を上げることができる。
Since the present invention estimates the DCR measurement result of the battery based on the AC impedance measurement result, the following effects can be obtained.
1) Since the AC impedance measurement can be stably performed even if the amplitude of the AC signal applied for the measurement is small, the perturbation appearing at the output of the battery 1 can be suppressed to a low level.
2) This eliminates the need for a standby time for returning the battery 1 to its original state, thereby shortening the measurement time and increasing the efficiency of the inspection in the production line, for example.
3)再現性の良い測定が行える。
4)小さな電源容量でも安定した測定が行える。
5)交流インピーダンス測定では、測定結果をFFT処理して解析対象となる周波数のみを用いるためノイズなどの影響を受けにくい。
3) Measurement with good reproducibility can be performed.
4) Stable measurement can be performed even with a small power supply capacity.
5) In the AC impedance measurement, the measurement result is FFT processed and only the frequency to be analyzed is used, so that it is not easily affected by noise or the like.
なお、上記実施例では、OCV算出に用いるパラメータとしてSOCの例について説明したが、SOCに限るものではなく、温度(セル温度、環境温度)を用いてもよい。すなわち、事前に電池1の温度を変えながら測定したOCVデータを用い、温度変化からOCVを算出して応答電圧を補正してもよい。 In the above embodiment, an example of SOC is described as a parameter used for OCV calculation. However, the present invention is not limited to SOC, and temperature (cell temperature, environmental temperature) may be used. That is, the OCV data measured while changing the temperature of the battery 1 in advance may be used to calculate the OCV from the temperature change and correct the response voltage.
また、OCVの算出にあたっては、電池の材料や構造を考慮し、温度テーブルを補正してもよい。 In calculating the OCV, the temperature table may be corrected in consideration of the material and structure of the battery.
また、OCVの算出にあたっては、SOCに温度や他の条件を組み合わせて使用してもよい。 In calculating the OCV, the SOC may be used in combination with temperature and other conditions.
また、等価回路として、CPE(Constant Phase Element)を直列に接続した回路を用いてもよい。CPEは電池内部の物質拡散によるインピーダンスを表すことができる素子であり、インピーダンスZは定数PとTを用い、一般には次のように定義される。 Further, as an equivalent circuit, a circuit in which CPEs (Constant Phase Elements) are connected in series may be used. CPE is an element that can represent the impedance due to material diffusion inside the battery, and the impedance Z is generally defined as follows using constants P and T.
P=0.5のとき、CPEのインピーダンスは、以下の式で表されるワールブルグインピーダンスと等しい。 When P = 0.5, the impedance of the CPE is equal to the Warburg impedance expressed by the following equation.
抵抗やRC並列回路と同様に等価回路中のCPEにかかる電圧を求め、他の部分にかかる電圧と加算することで内部抵抗全体の応答電圧とする。 Similar to the resistor and RC parallel circuit, the voltage applied to the CPE in the equivalent circuit is obtained and added to the voltage applied to other parts to obtain the response voltage of the entire internal resistor.
[CPEにかかる電圧]
CPEのインピーダンスがZcpe(s)のとき、かかる電圧Ecpe(t)は次の通りである。
[Voltage applied to CPE]
When the impedance of CPE is Z cpe (s), the voltage E cpe (t) is as follows.
Ik(s)がt=tkにおいてΔIk変化する電流のステップ関数であるとき、その応答電圧Ecpek(T)は以下のように求める。ただし、T=t-tkとする。 When I k (s) is a step function of current that changes ΔI k at t = t k , the response voltage E cpek (T) is obtained as follows. However, T = t−t k .
CPEのインピーダンスは、定数PとQを用いて次のように定義される。PとQは電池固有の特性であり、回路定数として扱う。 The impedance of CPE is defined as follows using constants P and Q. P and Q are battery specific characteristics and are treated as circuit constants.
よって Therefore
ここで、次の逆ラプラス変換を用いる。 Here, the following inverse Laplace transform is used.
ただし、n>0、Γ(n)はガンマ関数である。これにより、Ecpe(T)は次式のように表せる。 However, n> 0 and Γ (n) is a gamma function. Thereby, E cpe (T) can be expressed as the following equation.
回路定数の決定にあたっては、SOC毎のインピーダンス測定結果(SOC−インピーダンスデータ)を用いてもよい。図10はSOC-インピーダンスデータを用いたDCR解析装置4の具体的な構成例を示すブロック図であり、図2と共通する部分には同一の符号を付けている。SOC-回路定数テーブル演算部49aは、入力部44から入力されるSOC−インピーダンスデータテーブルと等価回路データに基づき、各SOCにおける等価回路に対応した回路定数を求める。 In determining the circuit constant, an impedance measurement result (SOC-impedance data) for each SOC may be used. FIG. 10 is a block diagram illustrating a specific configuration example of the DCR analysis apparatus 4 using SOC-impedance data, and the same reference numerals are given to portions common to FIG. The SOC-circuit constant table calculation unit 49a obtains a circuit constant corresponding to the equivalent circuit in each SOC based on the SOC-impedance data table and the equivalent circuit data input from the input unit 44.
具体的には、たとえば図11に示すように、各回路定数をSOC引きの回路定数としたSOC−回路定数テーブルを作成する。 Specifically, as shown in FIG. 11, for example, an SOC-circuit constant table is created in which each circuit constant is a circuit constant for SOC subtraction.
SOC-回路定数演算部49bは、SOC-回路定数テーブルとSOC演算部45から算出されるSOC値に基づき、SOC値に応じた回路定数を算出する。 The SOC-circuit constant calculation unit 49b calculates a circuit constant corresponding to the SOC value based on the SOC-circuit constant table and the SOC value calculated from the SOC calculation unit 45.
なお、回路定数の演算にあたっては、たとえば各SOCの測定データに基づきパラメータが制限された範囲内に収まるように回路定数の最適化を行うが、特性を変化させる条件はSOCに限るものではなく、温度を条件にしてもよい。 In calculating the circuit constants, for example, the circuit constants are optimized so that the parameters are within a limited range based on the measurement data of each SOC. However, the condition for changing the characteristics is not limited to the SOC. Temperature may be a condition.
以上説明したように、本発明によれば、大容量の電源を用いることなく、短時間で効率よく抵抗測定が行える電池直流抵抗評価装置を提供することができ、電池の製造ラインにおけるDCR検査などに好適である。 As described above, according to the present invention, it is possible to provide a battery direct-current resistance evaluation apparatus capable of measuring resistance efficiently in a short time without using a large-capacity power source, and a DCR inspection in a battery production line. It is suitable for.
1 供試電池
4 DCR解析装置
42 DCR演算部
43 出力部
44 入力部
45 SOC演算部
46 回路定数演算部
47 SOC-OCV演算部
48 応答電圧演算部
49a SOC-回路定数テーブル演算部
49b SOC-回路定数演算部
5 交流電源
6 インピーダンス測定装置
DESCRIPTION OF SYMBOLS 1 Test battery 4 DCR analyzer 42 DCR calculating part 43 Output part 44 Input part 45 SOC calculating part 46 Circuit constant calculating part 47 SOC-OCV calculating part 48 Response voltage calculating part 49a SOC-Circuit constant table calculating part 49b SOC-circuit Constant calculator 5 AC power supply 6 Impedance measuring device
Claims (4)
測定対象電池の交流インピーダンスを測定するインピーダンス測定手段と、
このインピーダンス測定手段の測定結果と選択された等価回路に基づき演算される回路定数と電池直流抵抗測定条件の電流値と開路電圧値(OCV)の変化分に基づき前記測定対象電池の応答電圧を算出するとともに内部直流抵抗値を算出する直流抵抗値解析手段を設け、
前記直流抵抗値解析手段は、電池の充電状態(SOC)を変えながらOCVデータを測定して作成されたSOC-OCVテーブルを用いて前記応答電圧を算出することを特徴とする電池直流抵抗評価装置。 A battery DC resistance evaluation device for measuring the internal DC resistance of a secondary battery,
Impedance measuring means for measuring the AC impedance of the battery to be measured;
The response voltage of the battery to be measured is calculated based on the circuit constant calculated based on the measurement result of this impedance measuring means and the selected equivalent circuit, the current value of the battery DC resistance measurement condition, and the change in the open circuit voltage value (OCV). And providing a DC resistance value analyzing means for calculating the internal DC resistance value,
The DC resistance value analyzing means calculates the response voltage using an SOC-OCV table created by measuring OCV data while changing the state of charge (SOC) of the battery. .
測定対象電池の交流インピーダンスを測定するインピーダンス測定手段と、
このインピーダンス測定手段の測定結果と選択された等価回路に基づき演算される回路定数と電池直流抵抗測定条件の電流値と開路電圧値(OCV)の変化分に基づき前記測定対象電池の応答電圧を算出するとともに内部直流抵抗値を算出する直流抵抗値解析手段を設け、
前記直流抵抗値解析手段は、温度を変えながら測定されたOCVデータを用いて前記応答電圧を補正することを特徴とする電池直流抵抗評価装置。 A battery DC resistance evaluation device for measuring the internal DC resistance of a secondary battery,
Impedance measuring means for measuring the AC impedance of the battery to be measured;
The response voltage of the battery to be measured is calculated based on the circuit constant calculated based on the measurement result of this impedance measuring means and the selected equivalent circuit, the current value of the battery DC resistance measurement condition, and the change in the open circuit voltage value (OCV). And providing a DC resistance value analyzing means for calculating the internal DC resistance value,
The direct current resistance value analyzing means corrects the response voltage using OCV data measured while changing the temperature.
Priority Applications (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2012098622A JP5751207B2 (en) | 2012-04-24 | 2012-04-24 | Battery DC resistance evaluation device |
| KR1020130043546A KR20130119871A (en) | 2012-04-24 | 2013-04-19 | Cell direct-current resistance evaluation system |
| CN201310141489.XA CN103376361B (en) | 2012-04-24 | 2013-04-22 | battery direct current resistance evaluation system |
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| JP2012098622A JP5751207B2 (en) | 2012-04-24 | 2012-04-24 | Battery DC resistance evaluation device |
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| JP2015102444A (en) * | 2013-11-26 | 2015-06-04 | 矢崎総業株式会社 | Battery state detection device and battery state detection method |
| CN104122451A (en) * | 2014-07-08 | 2014-10-29 | 国家电网公司 | Direct-current internal resistance measurement method for storage battery |
| CN105301362B (en) * | 2015-11-02 | 2018-02-09 | 深圳供电局有限公司 | Portable large current dynamic loop resistance detection device |
| CN105938161B (en) * | 2016-07-06 | 2018-09-04 | 惠州亿纬锂能股份有限公司 | A kind of test method and system of the internal resistance of cell |
| WO2018076325A1 (en) * | 2016-10-31 | 2018-05-03 | City University Of Hong Kong | Method and apparatus for use in electric circuit |
| KR102194844B1 (en) | 2017-11-02 | 2020-12-23 | 주식회사 엘지화학 | Method, apparatus and recording medium for estimating parameters of battery equivalent circuit model |
| CN108919127B (en) * | 2018-05-17 | 2020-12-04 | 合肥国轩高科动力能源有限公司 | A method to quickly count the DC internal resistance of secondary batteries at different temperatures and SOCs |
| JP6842212B1 (en) * | 2019-12-26 | 2021-03-17 | 東洋システム株式会社 | Battery performance evaluation method and battery performance evaluation device |
| CN113495221B (en) * | 2020-03-19 | 2023-12-01 | 郑州深澜动力科技有限公司 | Method for testing direct current impedance of battery |
| CN111814297B (en) * | 2020-04-30 | 2024-10-01 | 北京嘀嘀无限科技发展有限公司 | Method for measuring DC internal resistance of electric vehicle battery cell monomer, electronic device and storage medium |
| CN113740751B (en) * | 2020-05-27 | 2024-08-16 | 台达电子企业管理(上海)有限公司 | Battery internal resistance detection device and method |
| CN113866656B (en) * | 2020-06-30 | 2024-11-15 | 宁德时代新能源科技股份有限公司 | DCR calculation method, device, equipment and medium |
| JP7243700B2 (en) * | 2020-10-15 | 2023-03-22 | 株式会社豊田中央研究所 | Resistance measuring device, resistance measuring system, resistance measuring method and its program |
| CN114325431B (en) * | 2021-12-31 | 2024-03-08 | 北京西清能源科技有限公司 | Method and device for measuring and calculating direct current internal resistance of battery |
| KR102900640B1 (en) * | 2022-01-25 | 2025-12-15 | 주식회사 엘지에너지솔루션 | Low-voltate defect inspection method of lithium secondary battery and manufacturing method of lithium secondary battery |
| CN116802507A (en) * | 2022-08-15 | 2023-09-22 | 宁德时代新能源科技股份有限公司 | Battery DC impedance detection method, system, equipment and storage medium |
| US12535529B2 (en) | 2023-07-07 | 2026-01-27 | Ge Aviation Systems Llc | Method and system for a battery monitoring circuit |
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| JP4052418B2 (en) * | 2000-02-15 | 2008-02-27 | 日立マクセル株式会社 | Battery capacity detection method and apparatus, and battery pack |
| JP2004271410A (en) * | 2003-03-11 | 2004-09-30 | Hitachi Ltd | Battery control device for electric car |
| JP4430321B2 (en) * | 2003-03-31 | 2010-03-10 | 古河電池株式会社 | Storage battery state determination device and storage battery state determination method |
| JP4630113B2 (en) * | 2005-04-12 | 2011-02-09 | 古河電気工業株式会社 | Secondary battery deterioration state determination method and secondary battery deterioration state determination device |
| JP2009031220A (en) * | 2007-07-30 | 2009-02-12 | Mitsumi Electric Co Ltd | Battery state detection method and battery state detection device |
| KR20090077657A (en) * | 2008-01-11 | 2009-07-15 | 에스케이에너지 주식회사 | Method and device for measuring SOC of battery in battery management system |
| JP2011122917A (en) * | 2009-12-10 | 2011-06-23 | Yokogawa Electric Corp | Device for evaluating battery characteristics |
| JP5203496B2 (en) * | 2011-11-07 | 2013-06-05 | 古河電気工業株式会社 | Battery state detection method, battery state detection device, and battery power supply system |
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| CN103376361B (en) | 2016-06-01 |
| KR20130119871A (en) | 2013-11-01 |
| CN103376361A (en) | 2013-10-30 |
| JP2013228216A (en) | 2013-11-07 |
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