JP7671673B2 - Method for determining abnormality in lithium-ion secondary batteries - Google Patents
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Description
本発明は、リチウムイオン二次電池の異常判定方法に係り、詳しくは、電極条件のばらつきを反映したリチウムイオン二次電池の異常判定方法に関する。 The present invention relates to a method for determining an abnormality in a lithium-ion secondary battery, and more specifically, to a method for determining an abnormality in a lithium-ion secondary battery that reflects variations in electrode conditions.
リチウムイオン二次電池は、例えば、電気自動車などの駆動電源として広く用いられている。このようなリチウムイオン二次電池では、過酷な条件で使用されるため、製造したリチウムイオン二次電池に対して、出荷前に予めその品質の良否を正確に判定することが望まれる。 Lithium ion secondary batteries are widely used, for example, as power sources for electric vehicles and the like. Because such lithium ion secondary batteries are used under harsh conditions, it is desirable to accurately determine the quality of manufactured lithium ion secondary batteries before shipping.
特に電極における金属リチウムの析出は、電池寿命などにも影響が大きいため、出荷前にリチウム析出耐性の良否を正確に判断することが望まれる。
そこで、特許文献1に記載された発明では、あらかじめ用意した抵抗値と容量の相関関係と、対象とする二次電池の温度頻度分布に基づいて推定される容量を利用して、抵抗値を推定する。推定した抵抗値と閾値に乖離がある場合、異常と判定する。
In particular, since the deposition of metallic lithium in the electrodes has a large effect on battery life, it is desirable to accurately determine whether the lithium deposition resistance is good or not before shipping.
In the invention described in Patent Document 1, the resistance value is estimated using a correlation between the resistance value and the capacity prepared in advance and a capacity estimated based on the temperature frequency distribution of the target secondary battery. If there is a deviation between the estimated resistance value and a threshold value, it is determined that an abnormality has occurred.
また、特許文献2に記載された発明では、析出反応および溶解反応における、過電圧と交換電流密度を用いて、反応電流を算出し、リチウム析出量を推定する。その際、反応抵抗変化率で補正した交換電流密度を用いることで、反応抵抗に依存したリチウム析出量を算出している。 In addition, in the invention described in Patent Document 2, the reaction current is calculated using the overpotential and exchange current density in the precipitation reaction and dissolution reaction, and the amount of lithium precipitation is estimated. In this case, the amount of lithium precipitation that depends on the reaction resistance is calculated by using the exchange current density corrected by the rate of change of reaction resistance.
特許文献1に記載した発明によれば、電池性能として重要な抵抗値を推定できる。さらに特許文献2に記載した発明では、反応抵抗に依存したリチウム析出量を推定できる。 The invention described in Patent Document 1 makes it possible to estimate the resistance value, which is important for battery performance. Furthermore, the invention described in Patent Document 2 makes it possible to estimate the amount of lithium deposition that depends on the reaction resistance.
しかしながら、特許文献1に記載された発明では、製造のばらつきによる抵抗値-容量の相関関係の変化は想定されておらず、異常と誤判定する可能性ある。また、抵抗値とリチウム析出耐性との関係は想定されていない。 However, the invention described in Patent Document 1 does not take into account changes in the correlation between resistance value and capacity due to manufacturing variability, which may lead to erroneous determination of an abnormality. In addition, the relationship between resistance value and lithium precipitation resistance is not taken into account.
また、特許文献2に記載された発明でも、リチウム析出量が推定できるが、製造のばらつきによる反応電流と抵抗値の相関関係の変化は想定されておらず、リチウム析出量の推定精度が低下している可能性がある。 In addition, the invention described in Patent Document 2 can also estimate the amount of lithium precipitation, but does not take into account changes in the correlation between the reaction current and the resistance value due to manufacturing variations, and this may result in reduced accuracy in estimating the amount of lithium precipitation.
本発明のリチウムイオン二次電池の異常判定方法が解決しようとする課題は、リチウムイオン二次電池の製造にばらつきがあった場合でも、電極条件を反映してリチウム析出耐性の異常を正確に判定することである。 The problem that the lithium ion secondary battery anomaly determination method of the present invention aims to solve is to accurately determine anomalies in lithium precipitation resistance by reflecting electrode conditions, even when there is variation in the manufacturing of lithium ion secondary batteries.
上記課題を解決するため本発明のリチウムイオン二次電池の異常判定方法は、設定した電極条件におけるリチウムイオン二次電池の析出電流値と反応抵抗の基準となる基準相関関係を取得する基準相関関係取得のステップと、判定対象となるリチウムイオン二次電池の反応抵抗を取得する反応抵抗取得のステップと、前記判定対象となるリチウムイオン二次電池の析出電流値を取得する析出電流値取得のステップと、前記判定対象となるリチウムイオン二次電池の電極条件に基づいて、前記基準相関関係を補正し補正相関関係を取得するとともに、当該補正相関関係に基づいて正常範囲を規定する正常範囲規定のステップと、前記反応抵抗取得のステップで取得した反応抵抗と、前記析出電流値取得のステップで取得した析出電流値との関係が、前記正常範囲を外れた場合に、当該判定対象となるリチウムイオン二次電池が異常であると判定する異常判定のステップとを備えたことを特徴とする。 In order to solve the above problem, the method for determining an abnormality of a lithium-ion secondary battery of the present invention includes a step of acquiring a reference correlation that is a reference for the deposition current value and reaction resistance of a lithium-ion secondary battery under set electrode conditions, a step of acquiring a reaction resistance of the lithium-ion secondary battery to be determined, a step of acquiring a deposition current value of the lithium-ion secondary battery to be determined, a step of correcting the reference correlation to obtain a corrected correlation based on the electrode conditions of the lithium-ion secondary battery to be determined, and a step of determining a normal range based on the corrected correlation, and an abnormality determination step of determining that the lithium-ion secondary battery to be determined is abnormal if the relationship between the reaction resistance obtained in the step of acquiring the reaction resistance and the deposition current value obtained in the step of acquiring the deposition current value falls outside the normal range.
前記電極条件は、電極対向部面積、負極密度、正極目付、負極目付のうち、少なくとも一つを含むようにすることができる。
前記基準相関関係は、反応抵抗に対する析出電流値の一次関数として取得され、前記正常範囲規定のステップにおいて、前記判定対象の電極条件に基づいて前記一次関数の傾きをそのままに、切片を調整することで前記補正相関関係を取得するようにしてもよい。
The electrode conditions may include at least one of an electrode opposing portion area, a negative electrode density, a positive electrode basis weight, and a negative electrode basis weight.
The reference correlation may be obtained as a linear function of deposition current value against reaction resistance, and in the step of defining the normal range, the corrected correlation may be obtained by adjusting the intercept while keeping the slope of the linear function unchanged based on the electrode conditions to be determined.
前記切片の調整は、各電極条件の値にそれぞれ設定した定数を乗じて積算することで切片の補正量を算出するようにすることもできる。
前記判定対象は、予め前記電極条件の設計の公差範囲にある良品から選択されるようにしてもよい。
The intercept can also be adjusted by multiplying the value of each electrode condition by a constant set for each electrode condition and integrating the result to calculate the correction amount for the intercept.
The object to be judged may be selected in advance from among non-defective products that fall within a tolerance range of the design of the electrode conditions.
前記析出電流値は、低温サイクル試験により取得することができる。
前記反応抵抗は交流インピーダンス測定により取得することができる。
The deposition current value can be obtained by a low-temperature cycle test.
The reaction resistance can be obtained by AC impedance measurement.
本発明のリチウムイオン二次電池の異常判定方法は、リチウムイオン二次電池の製造にばらつきがあった場合でも、電極条件を反映してリチウム析出耐性の異常を正確に判定することができる。 The method for determining anomalies in lithium ion secondary batteries of the present invention can accurately determine anomalies in lithium precipitation resistance by reflecting electrode conditions, even when there is variation in the manufacturing of lithium ion secondary batteries.
(本実施形態の構成)
以下、本発明のリチウムイオン二次電池の異常判定方法の一実施形態を図1~12を参照して説明する。
(Configuration of this embodiment)
Hereinafter, one embodiment of the method for determining an abnormality in a lithium ion secondary battery of the present invention will be described with reference to FIGS.
<本実施形態の原理>
リチウムイオン二次電池において、金属リチウム(以下「Li」と略記する場合がある。)の析出は、極板間の短絡の原因になるなどするため、いわゆるリチウム析出耐性が低い(金属Liが低電流で析出しやすい)電池は、望ましくない。そこで、リチウムイオン二次電池においては、電極対向部面積[cm2]、負極密度[mg/cm3]、正極目付[mg/cm2]、負極目付[mg/cm2]などの電極条件について検査する。そして、設計値に対して一定の公差範囲のもののみを所定のリチウム析出耐性を有する良品として、それ以外の電池は不良品として、良品のみを製品として出荷する。
<Principle of this embodiment>
In lithium ion secondary batteries, the deposition of metallic lithium (hereinafter sometimes abbreviated as "Li") can cause short circuits between plates, and so-called batteries with low lithium deposition resistance (metallic Li is easily deposited at low current) are undesirable. Therefore, in lithium ion secondary batteries, electrode conditions such as the electrode facing area [ cm2 ], negative electrode density [mg/ cm3 ], positive electrode weight [mg/ cm2 ], and negative electrode weight [mg/ cm2 ] are inspected. Then, only those batteries that are within a certain tolerance range from the design value are deemed to be good products having a specified lithium deposition resistance, and other batteries are deemed to be defective products, and only the good products are shipped as products.
図1は、電極条件の設計中央値に対する反応抵抗[mΩ]に対する析出電流[A](金属リチウムが析出する最小電流値)との相関関係を示す「基準相関線L0」のグラフである。ここで、図1に示す基準相関関係を示すグラフの傾きaの一時関数の直線を「基準相関線L0」という。切片はb0である。このように、製造した電極条件の設計中央値である良品のリチウムイオン二次電池のみである場合には、反応抵抗[mΩ]に対する析出電流[A]との相関関係は、一定の関係を示す。よって、製造したリチウムイオン二次電池の反応抵抗[mΩ]に対する析出電流[A]との相関関係が、図1に示すような関係であれば、正常の良品のリチウムイオン二次電池であると判断できる。 FIG. 1 is a graph of the "reference correlation line L 0 " showing the correlation between the reaction resistance [mΩ] and the deposition current [A] (the minimum current value at which metallic lithium is deposited) for the design median of the electrode conditions. Here, the straight line of the one-time function of the slope a of the graph showing the reference correlation shown in FIG. 1 is called the "reference correlation line L 0 ". The intercept is b 0. In this way, in the case of only a good lithium ion secondary battery that is the design median of the manufactured electrode conditions, the correlation between the reaction resistance [mΩ] and the deposition current [A] shows a constant relationship. Therefore, if the correlation between the reaction resistance [mΩ] and the deposition current [A] of the manufactured lithium ion secondary battery is as shown in FIG. 1, it can be determined that it is a normal good lithium ion secondary battery.
しかしながら、実際には電極条件の設計値中央値に対して製造のばらつきがあり、ばらつきによっては、良品や不良品とする判定基準が異なってくる。
図2は、電極条件によって、反応抵抗[mΩ]に対する析出電流[A]との相関関係が変化することを示す「補正相関線L1~L3」のグラフである。
However, in reality, there is manufacturing variation from the median design value of the electrode conditions, and the criteria for determining whether a product is good or bad vary depending on the variation.
FIG. 2 is a graph of "corrected correlation lines L 1 to L 3 " which show that the correlation between the deposition current [A] and the reaction resistance [mΩ] changes depending on the electrode conditions.
電極条件が異なると、電極条件の設計中央値に対する反応抵抗[mΩ]に対する析出電流[A]との相関関係が変化する。例えば、図2のグラフに丸で示した電極条件の設計中央値の相関関係を示すグラフである基準相関線L0は、例えば、四角で示すグラフである補正相関線L1のように変化する。このとき基準相関線L0の傾きaは変化せずに、下方に平行移動する。さらに、電極条件が大きく変化すると、三角で示すグラフである補正相関線L2のように変化し、さらに電極条件が変化するとひし形で示すグラフである補正相関線L3のように変化する。このように、電極条件が、設計中央値から変化すると、反応抵抗[mΩ]に対する析出電流[A]との相関関係が変化する。つまり、異常判定の基準となる中心がずれてしまうことになる。 When the electrode conditions are different, the correlation between the reaction resistance [mΩ] and the deposition current [A] for the design median of the electrode conditions changes. For example, the reference correlation line L0 , which is a graph showing the correlation of the design median of the electrode conditions shown by a circle in the graph of FIG. 2, changes to, for example, the corrected correlation line L1 , which is a graph shown by a square. At this time, the slope a of the reference correlation line L0 does not change, but moves downward in parallel. Furthermore, when the electrode conditions change significantly, it changes to the corrected correlation line L2 , which is a graph shown by a triangle, and when the electrode conditions change further, it changes to the corrected correlation line L3 , which is a graph shown by a diamond. In this way, when the electrode conditions change from the design median, the correlation between the reaction resistance [mΩ] and the deposition current [A] changes. In other words, the center, which is the standard for abnormality judgment, is shifted.
そうすると本来正常である電池を異常と誤判定したり、本来不良である電池を正常と誤判定したりする場合がありうる。そのため判定の精度が低下していたという問題があった。 This can lead to a battery that is actually normal being erroneously determined to be abnormal, or a battery that is actually defective being erroneously determined to be normal. This can lead to a problem of reduced accuracy in the determination.
そこで、本発明では予め、リチウム析出耐性に密接な電極対向部面積[cm2]、負極密度[mg/cm3]、正極目付[mg/cm2]、負極目付[mg/cm2]に関して製造ばらつきを考慮した析出耐性の析出電流値[A]と反応抵抗[mΩ]の相関関係を取得する。 Therefore, in the present invention, the correlation between the deposition current value [ A ] and the reaction resistance [mΩ] of the deposition resistance is obtained in advance, taking into account manufacturing variations in the electrode opposing area [cm2], negative electrode density [mg/ cm3 ], positive electrode basis weight [mg/ cm2 ], and negative electrode basis weight [mg/ cm2 ], which are closely related to lithium deposition resistance.
ここで、電極対向部面積[cm2]、負極密度[mg/cm3]、正極目付[mg/cm2]、負極目付[mg/cm2]が公差を外れているような場合は、そのリチウムイオン二次電池は設計値から外れた不良品として出荷することができない。 If the electrode opposing area [ cm2 ], negative electrode density [mg/ cm3 ], positive electrode basis weight [mg/ cm2 ], or negative electrode basis weight [mg/ cm2 ] is outside the tolerances, the lithium-ion secondary battery is deemed a defective product that does not meet the design values and cannot be shipped.
一方、一定範囲の公差内の正常な電極対向部面積[cm2]、負極密度[mg/cm3]、正極目付[mg/cm2]、負極目付[mg/cm2]を備えたリチウムイオン二次電池は良品である。このような正常な良品のロットから抜き取り検査を行う。そして、抜き取った複数の製品サンプルの析出電流値(金属リチウムが析出する最小電流値)[A]と反応抵抗[mΩ]を測定する。 On the other hand, lithium ion secondary batteries having normal electrode facing area [ cm2 ], negative electrode density [mg/ cm3 ], positive electrode weight [mg/ cm2 ], and negative electrode weight [mg/ cm2 ] within a certain range of tolerance are considered to be good products. Random inspection is performed from such a lot of good products. Then, the deposition current value (the minimum current value at which metallic lithium is deposited) [A] and reaction resistance [mΩ] of the multiple product samples taken are measured.
図1に示すような設計値中央値での析出電流値[A]と反応抵抗[mΩ]の相関関係を「基準相関関係」といい、このグラフを基準相関線L0という。この「基準相関線L0」に基づいて、予め電極条件の製造ばらつきを考慮して補正した析出電流値[A]と反応抵抗[mΩ]の相関関係である「補正相関関係」を求めておく。 The correlation between the deposition current value [A] and the reaction resistance [mΩ] at the median design value as shown in Figure 1 is called the "reference correlation", and this graph is called the reference correlation line L 0. Based on this "reference correlation line L 0 ", a "corrected correlation" is calculated in advance, which is the correlation between the deposition current value [A] and the reaction resistance [mΩ] corrected in advance to take into account the manufacturing variations in the electrode conditions.
図3は、製造するリチウムイオン二次電池の電極条件に合致する「補正相関線L1」に基づいて、規定した「正常範囲SZ」を示すグラフである。図3に示すように、製造するリチウムイオン二次電池の電極条件に合致する「補正相関線L1」に基づいて、許容できる公差範囲を「正常範囲」と規定する。 3 is a graph showing a "normal range SZ" defined based on the "corrected correlation line L 1 " that matches the electrode conditions of the lithium ion secondary battery to be manufactured. As shown in FIG. 3, an allowable tolerance range is defined as a "normal range" based on the "corrected correlation line L 1 " that matches the electrode conditions of the lithium ion secondary battery to be manufactured.
そして、抜き取ったリチウムイオン二次電池の反応抵抗値[mΩ]と金属リチウムの析出電流値[A]を判定する。抜き取ったリチウムイオン二次電池を図3に示すリチウムイオン二次電池の正常範囲と比較する。この比較で反応抵抗値[mΩ]に対して正常な析出電流値[A]の正常範囲にあるか否かで、抜き取ったリチウムイオン二次電池が正常であるか異常であるかを判定する。 Then, the reaction resistance value [mΩ] and the deposition current value [A] of metallic lithium of the removed lithium ion secondary battery are determined. The removed lithium ion secondary battery is compared with the normal range of lithium ion secondary batteries shown in Figure 3. This comparison determines whether the reaction resistance value [mΩ] is within the normal range of the normal deposition current value [A], and whether the removed lithium ion secondary battery is normal or abnormal.
このような判定を行うことで、電極の製造にばらつきがあって電極条件が異なっても、より精度の高いリチウムイオン二次電池の異常判定方法とすることができた。
以下、本実施形態のリチウムイオン二次電池の異常判定方法を詳細に説明する。
By carrying out such a judgment, it is possible to provide a method for judging an abnormality in a lithium ion secondary battery with higher accuracy even if the electrode conditions differ due to variations in electrode manufacturing.
The method for determining an abnormality in a lithium ion secondary battery according to this embodiment will be described in detail below.
<本実施形態のリチウムイオン二次電池の異常判定方法の概要>
図4は、本実施形態のリチウムイオン二次電池の異常判定方法の手順を示すフローチャートである。図4を参照して、まず本実施形態のリチウムイオン二次電池の異常判定方法の手順の概略を説明する。
<Overview of the method for determining abnormality in a lithium-ion secondary battery according to the present embodiment>
4 is a flow chart showing the procedure of the method for determining an abnormality in a lithium ion secondary battery according to the present embodiment. First, an outline of the procedure of the method for determining an abnormality in a lithium ion secondary battery according to the present embodiment will be described with reference to FIG.
本実施形態のリチウムイオン二次電池の異常判定方法では、まず、準備段階として、基準相関関係取得のステップ(S1)を実施する。「基準相関関係」とは、設計中央値で設定した電極条件におけるリチウムイオン二次電池の析出電流値[A]と反応抵抗[mΩ]の基準となる基準相関関係を取得する。 In the method for determining an anomaly in a lithium ion secondary battery according to this embodiment, first, as a preparation step, a step (S1) of acquiring a reference correlation is carried out. The "reference correlation" is a reference correlation that is a standard between the deposition current value [A] and the reaction resistance [mΩ] of a lithium ion secondary battery under electrode conditions set at the design median.
続いて、正常範囲規定のステップ(S2)では、予め製造するリチウムイオン二次電池の電極条件に基づいて、基準相関関係取得のステップ(S1)で取得した基準相関関係を補正して補正相関関係を取得する。「補正相関関係」とは、基準相関関係取得のステップ(S1)で取得した基準相関関係を、判定対象となるリチウムイオン二次電池の電極条件に適合するように補正した相関関係である。判定対象となるリチウムイオン二次電池は、源泉工程及び電極体が製造された時点でリチウムイオン二次電池の電極条件が測定される。すなわち、電極対向部面積[cm2]、負極密度[mg/cm3]、正極目付[mg/cm2]、負極目付[mg/cm2]が測定される。これらの電極条件に基づいて図3に示すような補正相関関係が求められる。 Next, in the step (S2) of defining the normal range, the reference correlation acquired in the step (S1) of acquiring the reference correlation is corrected based on the electrode conditions of the lithium ion secondary battery to be manufactured in advance to acquire a corrected correlation. The "corrected correlation" is a correlation obtained by correcting the reference correlation acquired in the step (S1) of acquiring the reference correlation so as to conform to the electrode conditions of the lithium ion secondary battery to be judged. The electrode conditions of the lithium ion secondary battery to be judged are measured at the time of the source process and the manufacture of the electrode body. That is, the electrode facing area [cm 2 ], the negative electrode density [mg/cm 3 ], the positive electrode basis weight [mg/cm 2 ], and the negative electrode basis weight [mg/cm 2 ] are measured. Based on these electrode conditions, the corrected correlation as shown in FIG. 3 is obtained.
図3に示すように、補正相関関係を取得したら、この補正相関関係に基づいて正常範囲を規定する。
次に、リチウムイオン二次電池製造のステップ(S3)を行う。ここでは、検査の対象となるリチウムイオン二次電池を通常の方法でロット単位で製造する。同じロットでは、リチウムイオン二次電池の電極条件、すなわち電極対向部面積[cm2]、負極密度[mg/cm3]、正極目付[mg/cm2]、負極目付[mg/cm2]は、許容された公差の範囲内で、均一である。なお、電極条件が公差から外れる場合は、そのロットのリチウムイオン二次電池は、不良品として処理される。
As shown in FIG. 3, once the corrected correlation is obtained, a normal range is defined based on the corrected correlation.
Next, a step (S3) of manufacturing the lithium ion secondary battery is performed. Here, the lithium ion secondary battery to be inspected is manufactured in a lot unit by a normal method. In the same lot, the electrode conditions of the lithium ion secondary battery, i.e., the electrode facing area [cm 2 ], the negative electrode density [mg/cm 3 ], the positive electrode basis weight [mg/cm 2 ], and the negative electrode basis weight [mg/cm 2 ], are uniform within the range of the allowable tolerance. If the electrode conditions are out of the tolerance, the lithium ion secondary battery of that lot is treated as a defective product.
続いて、良品抜き取りのステップ(S4)で、同じ生産ロットのリチウムイオン二次電池から、判定対象となるリチウムイオン二次電池を抜き出す。抜き取り検査としたのは、低温サイクル試験による析出電流値取得のステップ(S6)を行った場合、そのリチウムイオン二次電池は劣化してしまうため、全数検査は行い得ないためである。 Next, in the step of sampling good products (S4), lithium ion secondary batteries to be judged are sampled from the lithium ion secondary batteries in the same production lot. Sampling inspection is performed because the lithium ion secondary batteries will deteriorate if the step of obtaining the deposition current value by low-temperature cycle testing (S6) is performed, and 100% inspection cannot be performed.
抜き取ったリチウムイオン二次電池は、反応抵抗取得のステップ(S5)において、反応抵抗[mΩ]が測定される。
その後、析出電流値取得のステップ(S6)により、抜き取ったリチウムイオン二次電池の析出電流値[A]を取得する。
The reaction resistance [mΩ] of the removed lithium ion secondary battery is measured in a reaction resistance acquisition step (S5).
Thereafter, in a deposition current value acquisition step (S6), the deposition current value [A] of the extracted lithium ion secondary battery is acquired.
異常判定のステップ(S7)では、反応抵抗取得のステップ(S5)で取得した反応抵抗[mΩ]と、析出電流値取得のステップ(S6)で取得した析出電流値[A]との関係を判断する。ここでは正常範囲規定のステップ(S2)で規定した正常範囲SZ内か、正常範囲SZを外れるかを判断する。 In the step of determining anomaly (S7), the relationship between the reaction resistance [mΩ] obtained in the step of obtaining the reaction resistance (S5) and the deposition current value [A] obtained in the step of obtaining the deposition current value (S6) is determined. Here, it is determined whether the value is within the normal range SZ defined in the step of defining the normal range (S2) or outside the normal range SZ.
ステップS8では、反応抵抗取得のステップ(S5)で取得した反応抵抗[mΩ]と、析出電流値取得のステップ(S6)で取得した析出電流値[A]との関係が、正常範囲規定のステップ(S2)で規定した正常範囲SZ内か判断する。正常範囲SZ内と判断した場合は(S8:YES)、正常と判定し(S9)、そのロットのリチウムイオン二次電池全品が正常な良品と判断して、製品として出荷する。 In step S8, it is determined whether the relationship between the reaction resistance [mΩ] obtained in the reaction resistance acquisition step (S5) and the deposition current value [A] obtained in the deposition current value acquisition step (S6) is within the normal range SZ specified in the normal range definition step (S2). If it is determined to be within the normal range SZ (S8: YES), it is determined to be normal (S9), and all lithium ion secondary batteries in that lot are determined to be normal, non-defective products, and are shipped as products.
一方、反応抵抗取得のステップ(S5)で取得した反応抵抗[mΩ]と、析出電流値取得のステップ(S6)で取得した析出電流値[A]との関係を判断する。反応抵抗[mΩ]と、析出電流値[A]との関係が正常範囲規定のステップ(S2)で規定した正常範囲SZ外と判断した場合は(S8:NO)、異常と判定する(S10)。そして、そのロット全体のリチウムイオン二次電池が異常な不良品と判断して、製品としての出荷を停止する。 On the other hand, the relationship between the reaction resistance [mΩ] acquired in the reaction resistance acquisition step (S5) and the deposition current value [A] acquired in the deposition current value acquisition step (S6) is determined. If it is determined that the relationship between the reaction resistance [mΩ] and the deposition current value [A] is outside the normal range SZ defined in the normal range definition step (S2) (S8: NO), it is determined that there is an abnormality (S10). Then, the entire lot of lithium ion secondary batteries is determined to be defective and shipment as products is halted.
以上で、本実施形態のリチウムイオン二次電池の異常判定方法の手順を終了する。以下、各ステップを詳細に説明する。
<基準相関関係取得のステップ(S1)>
本実施形態のリチウムイオン二次電池の異常判定方法では、まず、準備段階として、基準相関関係取得のステップ(S1)を実施する。ここでは設定した電極条件におけるリチウムイオン二次電池の析出電流値[A]と反応抵抗[mΩ]の基準となる基準相関関係を取得する。
This completes the procedure for the method for determining an abnormality in a lithium ion secondary battery according to the present embodiment. Each step will now be described in detail.
<Step of acquiring reference correlation (S1)>
In the method for determining an abnormality in a lithium ion secondary battery according to the present embodiment, first, as a preparation step, a step (S1) of acquiring a reference correlation is performed. In this step, a reference correlation serving as a reference between the deposition current value [A] and the reaction resistance [mΩ] of the lithium ion secondary battery under the set electrode conditions is acquired.
ここでは、設計値中央の電極条件を有したリチウムイオン二次電池を、実際に反応抵抗[mΩ]と、そのときの析出電流値[A]を実際に測定する。異なった反応抵抗[mΩ]のリチウムイオン二次電池を複数準備し、それらの析出電流値[A]の結果をプロットして平均二乗法などで直線を求める。なお、実際の測定値に対して、電極条件の誤差に対応して、理論的な数値の修正をすることもできる。 Here, the reaction resistance [mΩ] and the deposition current value [A] at that time are actually measured for a lithium-ion secondary battery with electrode conditions in the middle of the design values. Several lithium-ion secondary batteries with different reaction resistances [mΩ] are prepared, and the results of the deposition current values [A] are plotted to obtain a straight line using the mean square method or similar. Note that it is also possible to correct the theoretical values for the actual measured values in response to errors in the electrode conditions.
<反応抵抗[mΩ]の測定>
ここで、本実施形態における反応抵抗[mΩ]の求め方について説明する。反応抵抗[mΩ]は、交流インピーダンス測定により測定している。
<Measurement of reaction resistance [mΩ]>
Here, a method for determining the reaction resistance [mΩ] in this embodiment will be described. The reaction resistance [mΩ] is measured by AC impedance measurement.
<リチウムイオン二次電池1の等価回路>
図5は、リチウムイオン二次電池の等価回路を概略的に示す回路図である。リチウムイオン二次電池は、図5に示すような等価回路で表すことができる。すなわち、溶液抵抗Rsolと、ここに直列につながれた電荷移動抵抗Rctと電気二重層Cdlの並列回路として表現できる。電極間に電解液を有した構成は電気二重層Cdlと観念され、コンデンサとして機能する。このため、電気二重層Cdlの交流抵抗は低周波領域では誘電体の分極の遅延による誘電損失に相当する抵抗成分となり、高周波領域では、電極の表皮効果や近接効果に相当する抵抗成分となる。このようにインピーダンスは周波数によって変わる。理論的には直流では電気二重層Cdlは電気を通さず、交流電圧の周波数が高くなるにつれて抵抗値がゼロになる。したがって、周波数が高周波(例えば100Hz以上)では、回路の合成抵抗は、溶液抵抗Rsolと等しくなる。周波数が高くなるにつれて(100Hz~100mHz)では、溶液抵抗Rsolに加えて、電荷移動抵抗Rctと電気二重層Cdlと合成抵抗となる。そして、低周波(100mHz未満)では、回路の合成抵抗は、溶液抵抗Rsolに加えて電荷移動抵抗Rctとの和になる。
<Equivalent circuit of lithium ion secondary battery 1>
FIG. 5 is a circuit diagram showing a schematic equivalent circuit of a lithium ion secondary battery. A lithium ion secondary battery can be represented by an equivalent circuit as shown in FIG. 5. That is, it can be represented as a parallel circuit of a solution resistance Rsol, a charge transfer resistance Rct, and an electric double layer Cdl connected in series thereto. A configuration having an electrolyte between electrodes is considered as an electric double layer Cdl, and functions as a capacitor. For this reason, the AC resistance of the electric double layer Cdl becomes a resistance component equivalent to a dielectric loss due to a delay in the polarization of the dielectric in the low frequency region, and becomes a resistance component equivalent to the skin effect and proximity effect of the electrodes in the high frequency region. In this way, the impedance changes depending on the frequency. Theoretically, the electric double layer Cdl does not conduct electricity in direct current, and the resistance value becomes zero as the frequency of the AC voltage increases. Therefore, at high frequencies (for example, 100 Hz or higher), the combined resistance of the circuit becomes equal to the solution resistance Rsol. As the frequency increases (100 Hz to 100 mHz), in addition to the solution resistance Rsol, the combined resistance becomes the charge transfer resistance Rct and the electric double layer Cdl. At low frequencies (less than 100 mHz), the total resistance of the circuit is the sum of the solution resistance Rsol and the charge transfer resistance Rct.
すなわち、金属リチウム析出に密接な関係のある正極と負極の間に流れる電流は、この反応抵抗Rct[mΩ]に依存する。
<交流インピーダンス法>
リチウムイオン二次電池は、以上のような性質を有するため交流インピーダンス法により、その特性が測定される。交流インピーダンス法とは、微小振幅で、段階的に周波数を変えて電圧又は電流をリチウムイオン二次電池の電極系に印加して掃引することにより、インピーダンススペクトルを観察する方法である。
In other words, the current flowing between the positive electrode and the negative electrode, which is closely related to the deposition of metallic lithium, depends on this reaction resistance Rct [mΩ].
<AC impedance method>
Because of the above-mentioned properties of lithium-ion secondary batteries, their characteristics are measured by the AC impedance method, which is a method for observing the impedance spectrum by applying and sweeping a voltage or current with a small amplitude and stepwise changing frequency to the electrode system of the lithium-ion secondary battery.
ここで「交流(AC:alternating current)」とは、時間とともに周期的にプラスマイナスが変化する電流(交流電流)を示す言葉であり、「交番電流」の略である。本実施形態では、交流は正弦波であるが、周期的に大きさと向きが変化するものであれば正弦波に限らない波形のものも含む。正弦波以外の交流は非正弦波交流(non-sinusoidal alternating current)といい、矩形波交流や三角波交流や鋸歯状波などを含む。さらに、交流に替えて、一定の周期を有する矩形波、三角波、鋸状波などの直流のパルス波によって周波数を変化させながら測定してもよい。 The term "alternating current (AC)" refers to a current whose plus and minus values change periodically over time (alternating current), and is an abbreviation of "alternating current." In this embodiment, the AC is a sine wave, but it also includes waveforms other than sine waves as long as the magnitude and direction change periodically. AC other than a sine wave is called non-sinusoidal alternating current, and includes square wave AC, triangular wave AC, sawtooth wave, and the like. Furthermore, instead of AC, measurements may be made while changing the frequency using a DC pulse wave such as a square wave, triangular wave, or sawtooth wave with a fixed period.
<ナイキストプロット>
図6は、交流インピーダンス法によるナイキストプロットと、各抵抗成分との関係を示すグラフである。
<Nyquist plot>
FIG. 6 is a graph showing the relationship between the Nyquist plot by the AC impedance method and each resistance component.
交流インピーダンス法によるリチウムイオン二次電池の解析結果は、例えば、ナイキストプロット(Nyquist plots)として出力する。ナイキストプロットによれば、インピーダンスと位相差から、二次電池の電極反応速度,電解質の電気伝導率,電気二重層容量などの特性が測定できる。 The results of the analysis of lithium-ion secondary batteries using the AC impedance method are output as Nyquist plots, for example. From the impedance and phase difference, Nyquist plots allow the measurement of characteristics such as the electrode reaction rate of the secondary battery, the electrical conductivity of the electrolyte, and the electric double layer capacity.
ナイキストプロットは、縦軸に抵抗の虚数値Zimg[Ω]、横軸にZreal[Ω]をとり、高周波から微小振幅で、段階的に周波数を変えて電圧又は電流をリチウムイオン二次電池の電極系に印加する。これにより左下の原点Poから横軸に沿って右側にシフトした位置のゼロクロスPxから、中心を横軸上に有する円弧状のグラフが上方に延びる。そして、右上の所定の点から半径方向外側に直線状のグラフが延びる。 In a Nyquist plot, the vertical axis represents the imaginary value of resistance Zimg [Ω] and the horizontal axis represents Zreal [Ω], and voltage or current is applied to the electrode system of a lithium-ion secondary battery at a stepwise changing frequency, from high frequency to minute amplitude. This results in an arc-shaped graph with its center on the horizontal axis extending upward from the zero cross Px, which is shifted to the right along the horizontal axis from the origin Po at the bottom left. Then, a linear graph extends radially outward from a specified point at the top right.
<電子移動抵抗Rs>
本実施形態の例では、電子移動抵抗Rsは、原点PoからゼロクロスPxまでの距離で表わせられる。つまりゼロクロスPxの抵抗の実数値Zreal[Ω]で表され、例えば100Hz以上の高周波数での電解液や極柱、集電板などの電子が移動する際の抵抗を解析することができる。
<Electron transfer resistance Rs>
In this embodiment, the electron transfer resistance Rs is expressed as the distance from the origin Po to the zero cross Px. In other words, it is expressed as the real value Zreal [Ω] of the resistance at the zero cross Px, and it is possible to analyze the resistance when electrons move in the electrolyte, the pole, the current collector, etc. at a high frequency of, for example, 100 Hz or more.
<反応抵抗Rct>
本実施形態の例では、中間の周波数(100Hzから0.1Hz)では、電極での化学反応で、電荷(イオン)移動が生じる際の抵抗である「反応抵抗Rct」を解析することができる。ゼロクロスPxから、横軸上に中心を有する円弧状のグラフで表され、電極性能が劣化すると半径が大きな弧となる。
<Reaction resistance Rct>
In the example of this embodiment, at intermediate frequencies (100 Hz to 0.1 Hz), the "reaction resistance Rct" which is the resistance when charge (ion) transfer occurs in a chemical reaction at the electrode can be analyzed. It is expressed as an arc-shaped graph with its center on the horizontal axis from the zero cross Px, and the arc becomes larger in radius when the electrode performance deteriorates.
<拡散抵抗Zw>
0.1Hz未満の低周波では、活物質内の電荷が拡散していく際の抵抗である「拡散抵抗Zw」を観察することができる。
<Diffusion resistance Zw>
At low frequencies below 0.1 Hz, it is possible to observe the "diffusion resistance Zw," which is the resistance when the charge in the active material diffuses.
<ナイキストプロットでの解析>
図7は、リチウムイオン二次電池の劣化と、ナイキストプロットとの関係を示すグラフである。実線で示すグラフが、劣化していない初期状態のリチウムイオン二次電池のナイキストプロットを示す。電解液や極柱、集電板などの電子が移動する際の抵抗が大きくなると、ゼロクロスPxが、横軸に沿って右側にシフトする位置のゼロクロスPx´に移動する。これに伴い円弧の部分も右側にシフトして一点鎖線で示すような位置にずれる。すなわち、電子移動抵抗Rsの抵抗の実数値Zrealが大きくなる。
<Analysis using Nyquist plot>
7 is a graph showing the relationship between the degradation of a lithium ion secondary battery and the Nyquist plot. The solid line graph shows the Nyquist plot of a lithium ion secondary battery in an initial state without degradation. When the resistance of the electrolyte, the poles, the current collector, etc. when electrons move increases, the zero cross Px moves to a zero cross Px', which is a position shifted to the right along the horizontal axis. Accordingly, the arc portion also shifts to the right and shifts to the position shown by the dashed line. In other words, the real value Zreal of the resistance of the electron transfer resistance Rs increases.
なお、電解質性能が劣化すると、劣化していない初期状態のリチウムイオン二次電池のナイキストプロット円弧の部分の半径が大きくなり、一点鎖線で示すようなグラフとなる。 When the electrolyte performance deteriorates, the radius of the Nyquist plot arc of a lithium-ion secondary battery in its initial, undegraded state increases, resulting in a graph like that shown by the dashed dotted line.
以上のように本実施形態では、交流インピーダンス法により反応抵抗Rct[mΩ]を測定できる。反応抵抗Rct[mΩ]を正確に測定することで、正極と負極の間に流れる金属リチウム析出に密接な関係のある電流との関係を明らかにすることができる。 As described above, in this embodiment, the reaction resistance Rct [mΩ] can be measured by the AC impedance method. By accurately measuring the reaction resistance Rct [mΩ], it is possible to clarify the relationship with the current that flows between the positive electrode and the negative electrode and is closely related to the deposition of metallic lithium.
<析出電流値[A]の測定>
低温サイクル試験は、温度-6.7~-40°Cで、数10~数100Aの電流を数秒~数10秒間印加し、その1/10程度の電流を逆向きに同容量印加を繰り返す試験である。このような繰り返しで、低温時の過充電や過放電による金属リチウムの析出しやすい環境を再現して行う試験である。
<Measurement of deposition current value [A]>
The low-temperature cycle test involves applying a current of several tens to several hundreds of A for several to several tens of seconds at temperatures between -6.7 and -40°C, and then repeatedly applying a current of about 1/10 of that amount in the opposite direction with the same capacity. This test is carried out by repeating this process to recreate an environment in which metallic lithium is likely to precipitate due to overcharging and overdischarging at low temperatures.
本実施形態では、例えば複数のリチウムイオン二次電池に対して、電池温度-6.7°Cで、それぞれサンプルごとに電流を変えて100~200Aで5秒充電し、その1/10の電流で50秒放電する。このサイクルを1000サイクル繰り返した。 In this embodiment, for example, multiple lithium-ion secondary batteries were charged at a battery temperature of -6.7°C for 5 seconds at 100 to 200 A, with the current changed for each sample, and then discharged for 50 seconds at 1/10 of that current. This cycle was repeated 1,000 times.
そして1000サイクル終了後の電流が異なるそれぞれのリチウムイオン二次電池の電極における金属リチウムの析出の有無を確認した。そして、析出があった電流値と析出がなかった電流値の境界を取得し、そのリチウムイオン二次電池の金属リチウムの析出電流値[A]とした。 Then, the presence or absence of metallic lithium deposition in the electrodes of each lithium-ion secondary battery with different currents after 1000 cycles was confirmed. The boundary between the current value where deposition occurred and the current value where deposition did not occur was obtained, and this was designated as the metallic lithium deposition current value [A] of that lithium-ion secondary battery.
<基準相関関係の取得>
以上のように測定した反応抵抗[mΩ]に対する析出電流値[A]を複数点グラフ上でプロットして、最小二乗法などでこれらを通る直線を求める。設計中央値で設定した電極条件におけるリチウムイオン二次電池の析出電流値[A]と反応抵抗[mΩ]の基準となる基準相関関係を取得する。
Obtaining baseline correlations
The deposition current value [A] versus reaction resistance [mΩ] measured as described above is plotted on a multi-point graph, and a straight line passing through these values is obtained using the least squares method, etc. A reference correlation is obtained between the deposition current value [A] and reaction resistance [mΩ] of a lithium-ion secondary battery under electrode conditions set at the design median value.
このとき、基準相関関係を表す直線「基準相関線L0」は、
「析出電流値[A]=a×反応抵抗[mΩ]+b0[A]」
という一次関数で表すことができる。
In this case, the straight line "reference correlation line L 0 " representing the reference correlation is
"Deposition current value [A] = a x reaction resistance [mΩ] + b 0 [A]"
This can be expressed by a linear function.
<正常範囲規定のステップ(S2)>
正常範囲規定のステップ(S2)では、製造するリチウムイオン二次電池の電極条件に基づいて、基準相関関係取得のステップ(S1)で取得した基準相関関係を補正して補正相関関係を取得する。判定対象となるリチウムイオン二次電池は、源泉工程及び電極体が製造された時点でリチウムイオン二次電池の電極条件が測定される。すなわち電極対向部面積[cm2]、負極密度[mg/cm3]、正極目付[mg/cm2]、負極目付[mg/cm2]が測定される。これらの電極条件に基づいて図3に示すような補正相関関係が求められる。
<Step of defining normal range (S2)>
In the step (S2) of defining the normal range, the reference correlation obtained in the step (S1) of obtaining the reference correlation is corrected based on the electrode conditions of the lithium ion secondary battery to be manufactured to obtain a corrected correlation. The electrode conditions of the lithium ion secondary battery to be judged are measured at the time of the source process and the manufacture of the electrode body. That is, the electrode facing area [ cm2 ], the negative electrode density [mg/ cm3 ], the positive electrode basis weight [mg/ cm2 ], and the negative electrode basis weight [mg/ cm2 ] are measured. Based on these electrode conditions, the corrected correlation as shown in FIG. 3 is obtained.
補正相関関係を取得したら、この補正相関関係に基づいて正常範囲を規定する。ここで、図1に示す「基準相関線L0」は、リチウムイオン二次電池の電極条件により変化することがわかっている。その変化は、図2に示す「補正相関線L1~L3」のグラフのように基準相関線L0の傾きaをそのままに平行移動し、切片b0のみが変化する。この切片の変化は、電極対向部面積[cm2]、負極密度[mg/cm3]、正極目付[mg/cm2]、負極目付[mg/cm2]のそれぞれの電極条件に依存する。以下、それぞれの電極条件による補正について、分けて説明する。 Once the corrected correlation is obtained, the normal range is defined based on this corrected correlation. Here, it is known that the "reference correlation line L 0 " shown in FIG. 1 changes depending on the electrode conditions of the lithium ion secondary battery. The change is a parallel shift of the slope a of the reference correlation line L 0 as shown in the graph of the "corrected correlation lines L 1 to L 3 " shown in FIG. 2, and only the intercept b 0 changes. The change of this intercept depends on each of the electrode conditions, namely the electrode facing area [cm 2 ], the negative electrode density [mg/cm 3 ], the positive electrode basis weight [mg/cm 2 ], and the negative electrode basis weight [mg/cm 2 ]. Hereinafter, the correction according to each electrode condition will be explained separately.
<電極対向部面積低下率[%]と基準相関線L0の切片b0との関係>
図8は、電極対向部面積低下率[%]と基準相関線L0の切片b0の変化との関係を示すグラフである。電極対向部面積[cm2]が設計中央値より大きくなると、電流密度[A/cm2]が小さくなり、リチウム析出耐性が良化する。電極対向部面積[cm2]が小さくなると、電流密度[A/cm2]が大きくなり、リチウム析出耐性が悪化する。すなわち、図8に示すように、設計中央値の電極対向部面積[cm2]が電極対向部面積低下率[%]の低下に応じて、基準相関線L0の切片b0が、下方にシフトする。
<Relationship between electrode facing area reduction rate [%] and intercept b0 of reference correlation line L0 >
8 is a graph showing the relationship between the electrode opposing area reduction rate [%] and the change in the intercept b0 of the reference correlation line L0 . When the electrode opposing area [ cm2 ] is larger than the design median, the current density [A/ cm2 ] is reduced, and the lithium precipitation resistance is improved. When the electrode opposing area [ cm2 ] is reduced, the current density [A/ cm2 ] is increased, and the lithium precipitation resistance is deteriorated. That is, as shown in FIG. 8, the intercept b0 of the reference correlation line L0 shifts downward as the design median electrode opposing area [ cm2 ] decreases in accordance with the decrease in the electrode opposing area reduction rate [%].
<負極密度[mg/cm3]と基準相関線L0の切片b0との関係>
図9は、負極密度[mg/cm3]と基準相関線L0の切片b0の変化との関係を示すグラフである。負極密度[mg/cm3]が設計中央値より大きくなると、Li+拡散性が低下し、析出耐性が悪化する。すなわち、負極密度[mg/cm3]が、設計中央値より大きくなると、基準相関線L0の切片b0が、下方にシフトする。
<Relationship between negative electrode density [mg/cm 3 ] and intercept b 0 of reference correlation line L 0 >
9 is a graph showing the relationship between the negative electrode density [mg/cm 3 ] and the change in the intercept b 0 of the reference correlation line L 0. When the negative electrode density [mg/cm 3 ] is greater than the design median, the Li + diffusivity decreases and the precipitation resistance deteriorates. That is, when the negative electrode density [mg/cm 3 ] is greater than the design median, the intercept b 0 of the reference correlation line L 0 shifts downward.
<正極目付[mg/cm2]と基準相関線L0の切片b0との関係>
図10は、正極目付[mg/cm2]と基線準相関線L0の切片b0の変化との関係を示すグラフである。正極目付[mg/cm2]が設計中央値より大きくなると、電流密度[A/cm2]が大きくなり、析出耐性が悪化する。すなわち正極目付[mg/cm2]が設計中央値より大きくなると、基準相関線L0の切片b0が、下方にシフトする。
<Relationship between positive electrode weight [mg/cm 2 ] and intercept b 0 of reference correlation line L 0 >
10 is a graph showing the relationship between the positive electrode basis weight [mg/ cm2 ] and the change in the intercept b0 of the baseline correlation line L0 . When the positive electrode basis weight [mg/ cm2 ] is greater than the design median, the current density [A/ cm2 ] increases and the precipitation resistance deteriorates. In other words, when the positive electrode basis weight [mg/ cm2 ] is greater than the design median, the intercept b0 of the baseline correlation line L0 shifts downward.
<負極目付[mg/cm2]と基準相関線L0の切片b0との関係>
図11は、負極目付[mg/cm2]と基準相関線L0の切片b0の変化との関係を示すグラフである。負極目付[mg/cm2]が設計中央値より大きくなると、単位面積あたりのLi+受け入れ性が良化し、析出耐性が良化する。すなわち、この場合は、負極目付[mg/cm2]が設計中央値より大きくなると、基準相関線L0の切片b0が、逆に上方にシフトする。
<Relationship between negative electrode weight [mg/cm 2 ] and intercept b 0 of reference correlation line L 0 >
11 is a graph showing the relationship between the negative electrode basis weight [mg/ cm2 ] and the change in the intercept b0 of the reference correlation line L0 . When the negative electrode basis weight [mg/ cm2 ] is greater than the design median, the Li + acceptability per unit area improves and the precipitation resistance improves. That is, in this case, when the negative electrode basis weight [mg/ cm2 ] is greater than the design median, the intercept b0 of the reference correlation line L0 shifts upward instead.
<電極条件と基準相関線L0の切片b0との関係>
図12は、基準相関線L0を、判定対象の電極条件を反映して切片b0を補正した補正相関線L1~L2のグラフである。
<Relationship between electrode conditions and intercept b0 of reference correlation line L0 >
FIG. 12 is a graph of corrected correlation lines L 1 to L 2 obtained by correcting the intercept b 0 of the reference
以上説明したように電極対向部面積[cm2]、負極密度[mg/cm3]、正極目付[mg/cm2]、負極目付[mg/cm2]が、設計中央値より変化すると、それぞれ基準相関線L0の切片b0を変化させる。それぞれの変化に対する切片b0の変化は、さまざまである。そこで、切片b0の調整は、それぞれの電極条件変化の値にそれぞれ設定した定数を乗じて切片b0に換算する。そして、これらの切片のシフト量Δb[A]を積算することで切片b0の補正量を算出することができる。 As described above, when the electrode opposing area [cm 2 ], negative electrode density [mg/cm 3 ], positive electrode basis weight [mg/cm 2 ], and negative electrode basis weight [mg/cm 2 ] change from their design median values, the intercept b 0 of the reference correlation line L 0 is changed. The change in intercept b 0 for each change varies. Therefore, the intercept b 0 is adjusted by multiplying the value of each electrode condition change by a constant set for each change to convert it into intercept b 0. Then, the correction amount of intercept b 0 can be calculated by integrating the shift amount Δb [A] of these intercepts.
ここで電極対向部面積[cm2]の定数を「i」、負極密度[mg/cm3]の定数を「j」、正極目付[mg/cm2]の定数を「k」、負極目付[mg/cm2]の定数を「l」とすると、これらを積算した切片b0に対する下向きのシフト量Δb[A]は以下の式で導かれる。 Here, if the electrode opposing area [ cm2 ] is a constant "i", the negative electrode density [mg/ cm3 ] is a constant "j", the positive electrode basis weight [mg/ cm2 ] is a constant "k", and the negative electrode basis weight [mg/ cm2 ] is a constant "l", the downward shift Δb [ A ] relative to the intercept b0 obtained by integrating these is derived by the following formula.
「シフト量Δb[A]=i×電極対向部面積低下率[%]+j×負極密度[mg/cm3]+k×正極目付[mg/cm2]+l×負極目付[mg/cm2]」
なお、この場合、「定数l」については、逆向き(上向き)のシフトであるので、定数lはマイナスの数となる。
"Shift amount Δb [A] = i × electrode opposing area reduction rate [%] + j × negative electrode density [mg/cm 3 ] + k × positive electrode area weight [mg/cm 2 ] + l × negative electrode area weight [mg/cm 2 ]"
In this case, since the "constant l" is a shift in the opposite direction (upward), the constant l is a negative number.
上述のようにシフト量Δb[A]を求めたら、基準相関線L0の切片b0をシフト量Δbだけずらし、切片b2となるように下方に平行移動して、補正相関線L1のようにする。
<正常範囲の規定>
補正相関線L1を求めたら、図3に示すように、製造するリチウムイオン二次電池の公差として許容される範囲である公差範囲内の領域を「正常範囲SZ」として規定する。この正常範囲SZから外れた領域は「異常範囲FZ」と規定する。
After the shift amount Δb[A] is calculated as described above, the intercept b0 of the reference correlation line L0 is shifted by the shift amount Δb, and translated downward to become the intercept b2 , resulting in a corrected correlation line L1 .
<Definition of normal range>
After the corrected correlation line L1 is obtained, the region within the tolerance range, which is the range permitted as the tolerance of the lithium ion secondary battery to be manufactured, is defined as the "normal range SZ" as shown in Fig. 3. The region outside this normal range SZ is defined as the "abnormal range FZ".
<リチウムイオン二次電池製造のステップ(S3)>
次に、リチウムイオン二次電池製造のステップ(S3)を行う。ここでは、検査の対象となるリチウムイオン二次電池をロット単位で製造する。同じロットでは、リチウムイオン二次電池の電極条件、すなわち電極対向部面積[cm2]、負極密度[mg/cm3]、正極目付[mg/cm2]、負極目付[mg/cm2]は、許容された公差の範囲内で、均一である。なお、電極条件が公差から外れる場合は、そのロットのリチウムイオン二次電池は、不良品として処理される。
<Step of manufacturing lithium ion secondary battery (S3)>
Next, a step (S3) of manufacturing the lithium ion secondary battery is performed. Here, the lithium ion secondary battery to be inspected is manufactured in lots. In the same lot, the electrode conditions of the lithium ion secondary battery, i.e., the electrode facing area [cm 2 ], the negative electrode density [mg/cm 3 ], the positive electrode basis weight [mg/cm 2 ], and the negative electrode basis weight [mg/cm 2 ], are uniform within the range of the allowable tolerance. If the electrode conditions are out of the tolerance, the lithium ion secondary battery of that lot is treated as a defective product.
<良品抜き取りのステップ(S4)>
続いて、良品抜き取りのステップ(S4)で、同じ生産ロットのリチウムイオン二次電池から、判定対象となるリチウムイオン二次電池を抜き出す。同じ生産ロットのリチウムイオン二次電池は、すべて同一の電極条件の設計の公差範囲にある良品であるので、ランダムの抜き取り検査である。抜き取り検査は、複数のサンプルとする。金属リチウムが析出する析出電流値[A]を測定するためには、複数のサンプルの析出電流値[A]を低温サイクル試験による検査により測定して比較する必要があるからである。
<Step of removing non-defective products (S4)>
Next, in a step of sampling good products (S4), lithium ion secondary batteries to be judged are sampled from lithium ion secondary batteries of the same production lot. Since all lithium ion secondary batteries of the same production lot are good products within the tolerance range of the design of the same electrode conditions, this is a random sampling inspection. A plurality of samples are sampled for sampling inspection. This is because, in order to measure the deposition current value [A] at which metallic lithium is precipitated, it is necessary to measure and compare the deposition current values [A] of the plurality of samples by inspection using a low-temperature cycle test.
なお、抜き取り検査としたのは、低温サイクル試験による析出電流値取得のステップ(S6)を行った場合、そのリチウムイオン二次電池は劣化する上、金属リチウムの析出を確認するための破壊検査が必要なため、全数検査は行い得ないためである。 The reason why a random inspection was performed is that when the step (S6) of obtaining the deposition current value by the low-temperature cycle test is performed, the lithium-ion secondary battery deteriorates, and a destructive inspection is required to confirm the deposition of metallic lithium, so a full inspection cannot be performed.
<反応抵抗取得のステップ(S5)>
抜き取ったリチウムイオン二次電池は、反応抵抗取得のステップ(S5)において、反応抵抗[mΩ]が測定される。その測定方法は、基準相関関係取得のステップ(S1)における交流インピーダンス測定と同一の方法により測定する。
<Reaction resistance acquisition step (S5)>
The reaction resistance [mΩ] of the removed lithium ion secondary battery is measured in the reaction resistance acquisition step (S5) by the same method as the AC impedance measurement in the reference correlation acquisition step (S1).
<析出電流値取得のステップ(S6)>
反応抵抗取得のステップ(S5)において、反応抵抗[mΩ]が測定された判定対象は、析出電流値取得のステップ(S6)により、析出電流値[A]を取得する。析出電流値[A]の測定は、基準相関関係取得のステップ(S1)における低温サイクル試験と同一の方法で測定される。
<Step of acquiring deposition current value (S6)>
In the step of acquiring the reaction resistance (S5), the object to be evaluated whose reaction resistance [mΩ] has been measured undergoes the step of acquiring the deposition current value (S6) to acquire the deposition current value [A]. The deposition current value [A] is measured in the same manner as in the low-temperature cycle test in the step of acquiring the reference correlation (S1).
<異常判定のステップ(S7)>
異常判定のステップ(S7)では、反応抵抗取得のステップ(S5)で取得した反応抵抗[mΩ]と、析出電流値取得のステップ(S6)で取得した析出電流値[A]との関係が、正常範囲規定のステップ(S6)で規定した正常範囲SZ内か、正常範囲を外れる異常は範囲FZかを判断する。
<Abnormality determination step (S7)>
In the abnormality determination step (S7), it is determined whether the relationship between the reaction resistance [mΩ] obtained in the reaction resistance acquisition step (S5) and the deposition current value [A] obtained in the deposition current value acquisition step (S6) is within the normal range SZ specified in the normal range definition step (S6), or whether an abnormality outside the normal range is in the range FZ.
ステップS8では、反応抵抗取得のステップ(S5)で取得した反応抵抗[mΩ]と、析出電流値取得のステップ(S6)で取得した析出電流値[A]との関係が、正常範囲規定のステップ(S2)で規定した正常範囲SZ内と判断した場合は(S8:YES)、正常と判定し(S9)、そのロットのリチウムイオン二次電池が正常な良品と判断して、製品として出荷する。 In step S8, if it is determined that the relationship between the reaction resistance [mΩ] obtained in the reaction resistance acquisition step (S5) and the deposition current value [A] obtained in the deposition current value acquisition step (S6) is within the normal range SZ defined in the normal range definition step (S2) (S8: YES), it is determined to be normal (S9), and the lithium ion secondary batteries in that lot are determined to be normal, non-defective products, and are shipped as products.
一方、反応抵抗取得のステップ(S5)で取得した反応抵抗[mΩ]と、析出電流値取得のステップ(S6)で取得した析出電流値[A]との関係が、正常範囲規定のステップ(S2)で規定した異常範囲FZと判断した場合は(S8:NO)、異常と判定し(S10)、そのロットのリチウムイオン二次電池全体が異常な不良品と判断して、製品としての出荷を停止する。 On the other hand, if it is determined that the relationship between the reaction resistance [mΩ] obtained in the reaction resistance acquisition step (S5) and the deposition current value [A] obtained in the deposition current value acquisition step (S6) is within the abnormal range FZ defined in the normal range definition step (S2) (S8: NO), it is determined to be abnormal (S10), and the entire lot of lithium ion secondary batteries is determined to be defective and shipment of the product is suspended.
(本実施形態の作用)
本発明のリチウムイオン二次電池の異常判定方法は、リチウムイオン二次電池の製造にばらつきがあった場合でも、判断基準を電極条件に合ったものに補正する。そのため、電極条件を反映してリチウム析出耐性の異常を正確に判定する。
(Operation of this embodiment)
The method for determining an anomaly in a lithium ion secondary battery of the present invention corrects the determination criteria to match the electrode conditions even if there is variation in the manufacturing process of the lithium ion secondary battery, and therefore accurately determines an anomaly in lithium precipitation resistance by reflecting the electrode conditions.
(本実施形態の効果)
(1)本実施形態のリチウムイオン二次電池の異常判定方法は、リチウムイオン二次電池の電極条件の製造にばらつきがあった場合でも、電極条件を反映してリチウム析出耐性の異常を正確に判定することができる。
(Effects of this embodiment)
(1) The method for determining an abnormality in a lithium ion secondary battery according to the present embodiment can accurately determine an abnormality in lithium precipitation resistance by reflecting the electrode conditions, even if there is variation in the manufacturing conditions of the electrode of the lithium ion secondary battery.
(2)電極条件として、リチウム析出耐性に密接な電極対向部面積[cm2]、負極密度[mg/cm3]、正極目付[mg/cm2]、負極目付[mg/cm2]に分けている。そのため電極条件を詳細に反映しているので、リチウムイオン二次電池のリチウム析出耐性をより正確に判定することができる。 (2) The electrode conditions are divided into the electrode facing area [cm 2 ], negative electrode density [mg/cm 3 ], positive electrode basis weight [mg/cm 2 ], and negative electrode basis weight [mg/cm 2 ], which are closely related to lithium precipitation resistance. As a result, the electrode conditions are reflected in detail, and the lithium precipitation resistance of lithium ion secondary batteries can be determined more accurately.
(3)基準相関関係は、反応抵抗に対する析出電流値の一次関数として取得され、正常範囲規定のステップにおいて、判定対象の電極条件に基づいて一次関数の傾きをそのままに、切片を調整することで前記補正相関関係を取得するため、処理が単純化される。 (3) The reference correlation is obtained as a linear function of the deposition current value against the reaction resistance, and in the step of defining the normal range, the corrected correlation is obtained by adjusting the intercept while keeping the slope of the linear function unchanged based on the electrode conditions to be evaluated, thus simplifying the process.
(4)切片b0の調整は、各電極条件の値にそれぞれ設定した定数を乗じて積算することで切片の補正量を算出するため、多面的な影響を総合的に盛り込んで正確に判定することができる。 (4) The adjustment of the intercept b0 calculates the correction amount of the intercept by multiplying the value of each electrode condition by a constant that is set for each electrode condition and integrating the results, so that an accurate judgment can be made by comprehensively taking into account various influences.
(5)判定対象は、予め電極条件の設計の公差範囲外の製品を除去した後に、良品から選択されるため、無駄な判定をすることなく効率的に判定することができる。
(6)析出電流値[A]は、低温サイクル試験により取得するため、低温時のハイレートの充放電を再現し、正確にリチウム析出耐性の判定をすることができる。
(5) Products to be judged are selected from non-defective products after removing products that are outside the design tolerance range of the electrode conditions in advance, so that the judgment can be made efficiently without making unnecessary judgments.
(6) The deposition current value [A] is obtained by a low-temperature cycle test, which reproduces high-rate charge and discharge at low temperatures and allows accurate determination of lithium deposition resistance.
(7)反応抵抗[mΩ]は交流インピーダンス測定により取得するため、正確に極板間の反応抵抗[mΩ]の測定をすることができ、リチウム析出耐性の判定を正確にすることができる。 (7) The reaction resistance [mΩ] is obtained by AC impedance measurement, so the reaction resistance [mΩ] between the electrodes can be accurately measured, enabling accurate assessment of lithium precipitation resistance.
(別例)
○本実施形態における数値は、一例であり、これらの数値に限定されないことは、言うまでもない。
(Another example)
The numerical values in the present embodiment are merely examples, and the present invention is not limited to these numerical values.
○本実施形態において電極条件は、電極対向部面積[cm2]、負極密度[mg/cm3]、正極目付[mg/cm2]、負極目付[mg/cm2]の4つを例示したが、これらに限定されるものではない。例えば、これらのうちのいずれか1~3つにより判定してもよい。また、これら4つのパラメータに限定されず基準相関関係に変化をもたらす、種々のパラメータを参照し得る。 In this embodiment, the electrode conditions are exemplified by four items, namely, the electrode facing area [cm 2 ], the negative electrode density [mg/cm 3 ], the positive electrode basis weight [mg/cm 2 ], and the negative electrode basis weight [mg/cm 2 ], but are not limited to these. For example, the electrode conditions may be determined based on any one to three of these. In addition, various parameters that change the reference correlation may be referenced, without being limited to these four parameters.
○本実施形態では、析出電流値[A]は、「低温サイクル試験」により取得しているが、析出電流値[A]を取得できれば、その方法は限定されない。他の方法による実測値はもちろん、理論的な推定値であってもよい。 In this embodiment, the deposition current value [A] is obtained by a "low-temperature cycle test," but the method is not limited as long as the deposition current value [A] can be obtained. It may be a theoretically estimated value, as well as an actual measurement value obtained by another method.
○本実施形態では、反応抵抗値[mΩ]値は、「交流インピーダンス測定」により取得しているが、反応抵抗値[mΩ]値を取得できれば、その方法は限定されない。他の方法による実測値はもちろん、理論的な推定値であってもよい。 In this embodiment, the reaction resistance value [mΩ] is obtained by "AC impedance measurement", but the method is not limited as long as the reaction resistance value [mΩ] can be obtained. It may be a theoretically estimated value, or an actual measurement value obtained by another method.
○本実施形態では、基準相関関係を、反応抵抗に対する析出電流値の一次関数である基線準相関線L0として取得している。そして、説明の便宜のため、正常範囲規定のステップ(S6)において、判定対象の電極条件に基づいて基線準相関線L0の傾きをそのままに、切片b0を調整することで補正相関関係を取得しているが、この態様に限定されない。例えば、グラフに基づかず、実際に電極条件を変えた場合の実測値を個々に記録して補正相関関係を取得してもよい。 In this embodiment, the reference correlation is obtained as a baseline quasi-correlation line L0 , which is a linear function of the deposition current value against the reaction resistance. For convenience of explanation, in the step (S6) of defining the normal range, the intercept b0 is adjusted while keeping the slope of the baseline quasi-correlation line L0 unchanged based on the electrode conditions to be determined to obtain a corrected correlation, but this is not limited to this embodiment. For example, the corrected correlation may be obtained by recording the actual measured values when the electrode conditions are actually changed, without using a graph.
○本実施形態では、車載用の薄板状のリチウムイオン二次電池を例示したが、円柱形の電池などにも適用できる。また、車載用に限らず、船舶用、航空機用、さらに定置用の電池にも適用できる。 In this embodiment, a thin-plate lithium-ion secondary battery for vehicle use is shown as an example, but the battery can also be applied to cylindrical batteries. The battery can also be applied not only to vehicle use, but also to marine, aircraft, and stationary batteries.
○図4に示すフローチャートは、例示であり当業者においてその手順を付加し削除し変更し、順序を変えて実施することができる。
○例えば、リチウムイオン二次電池製造のステップ(S3)の後、異常判定のステップ(S7)までに正常範囲規定のステップ(S6)を行うようにしてもよい。
The flowchart shown in FIG. 4 is an example, and a person skilled in the art can add, delete, or modify the steps, or change the order of steps.
For example, after the step of manufacturing the lithium ion secondary battery (S3), the step of determining the normal range (S6) may be performed before the step of determining an abnormality (S7).
○本発明は、特許請求の範囲の記載を逸脱しない範囲で、当業者によりその構成を付加し削除し変更し、順序を変えて実施することができることは言うまでもない。 It goes without saying that those skilled in the art may add, delete, or modify the components of the present invention, or change the order of the components, without departing from the scope of the claims.
L0…基準相関線
L1、L2、L3…補正相関線
b0、b1、b2…切片
L 0 : Reference correlation line L 1 , L 2 , L 3 : Corrected correlation lines b 0 , b 1 , b 2 : Intercepts
Claims (3)
判定対象となる前記リチウムイオン二次電池の反応抵抗を交流インピーダンス測定により取得する反応抵抗取得のステップと、
前記判定対象となる前記リチウムイオン二次電池において低温サイクル試験により金属リチウムが析出する最小電流値である析出電流値を取得する析出電流値取得のステップと、
前記判定対象となる前記リチウムイオン二次電池の前記電極条件と、予め取得した前記基準相関関係の前記電極条件との差に基づいて、前記基準相関関係を補正し補正相関関係を取得するとともに、当該補正相関関係に基づいて許容される正常範囲を規定する正常範囲規定のステップと、
前記反応抵抗取得のステップで取得した反応抵抗と、前記析出電流値取得のステップで取得した析出電流値との関係が、前記正常範囲を外れた場合に、当該判定対象となるリチウムイオン二次電池が異常であると判定する異常判定のステップとを備えたことを特徴とするリチウムイオン二次電池の異常判定方法。 a step of acquiring a reference correlation which is a linear function obtained from the relationship between a change in reaction resistance, which is charge transfer resistance, and a corresponding deposition current value, which is a minimum current value at which metallic lithium is deposited, the change being obtained by measuring the AC impedance of a lithium ion secondary battery selected from non-defective products within a tolerance range of a design of electrode conditions including at least one of an electrode opposing portion area, a negative electrode density, a positive electrode basis weight, and a negative electrode basis weight;
A reaction resistance acquisition step of acquiring a reaction resistance of the lithium ion secondary battery to be determined by AC impedance measurement ;
A deposition current value acquisition step of acquiring a deposition current value which is a minimum current value at which metallic lithium is deposited in the lithium ion secondary battery to be determined by a low-temperature cycle test ;
a step of correcting the reference correlation to obtain a corrected correlation based on a difference between the electrode condition of the lithium ion secondary battery to be determined and the electrode condition of the reference correlation obtained in advance, and defining a normal range that is permissible based on the corrected correlation;
A method for determining an abnormality in a lithium ion secondary battery, comprising: an abnormality determination step of determining that the lithium ion secondary battery being determined to be abnormal if the relationship between the reaction resistance obtained in the reaction resistance acquisition step and the deposition current value obtained in the deposition current value acquisition step is outside the normal range.
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