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JP6954214B2 - Filling member, battery assembly, and heat transfer control method - Google Patents

Filling member, battery assembly, and heat transfer control method Download PDF

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JP6954214B2
JP6954214B2 JP2018070431A JP2018070431A JP6954214B2 JP 6954214 B2 JP6954214 B2 JP 6954214B2 JP 2018070431 A JP2018070431 A JP 2018070431A JP 2018070431 A JP2018070431 A JP 2018070431A JP 6954214 B2 JP6954214 B2 JP 6954214B2
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heat transfer
filling member
partition member
heat
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陽子 渡邉
陽子 渡邉
川井 友博
友博 川井
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Mitsubishi Chemical Corp
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    • YGENERAL 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
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Description

本発明は、充填部材、組電池、及び熱伝達の制御方法に関する。 The present invention relates to a filling member, an assembled battery, and a method for controlling heat transfer.

近年、車両等の電源としての二次電池の使用が急増している。車両等の限られた空間に搭載する際の自由度を向上させること、一度の充電に対して走行可能な航続距離を伸ばすこと等を目的として、二次電池の高エネルギー密度化の検討が進められている。 In recent years, the use of secondary batteries as a power source for vehicles and the like has increased rapidly. For the purpose of improving the degree of freedom when mounting in a limited space such as a vehicle and extending the cruising range that can be traveled for one charge, studies on increasing the energy density of the secondary battery are underway. Has been done.

二次電池の安全性はエネルギー密度とは相反する傾向にあり、エネルギー密度が高くなるほど二次電池の安全性は低下する傾向にある。例えば、航続距離が数百kmに及ぶような電気自動車に搭載される二次電池では、過充電や内部短絡等により二次電池が損傷した場合の電池表面温度が数百℃を超え、1000℃近くに及ぶ場合もある。 The safety of the secondary battery tends to contradict the energy density, and the higher the energy density, the lower the safety of the secondary battery. For example, in a secondary battery mounted on an electric vehicle having a cruising range of several hundred km, the battery surface temperature exceeds several hundred ° C when the secondary battery is damaged due to overcharging or an internal short circuit, and the temperature exceeds 1000 ° C. It may reach nearby.

車両等の電源に使用される二次電池は、一般に複数の単電池(以下、「セル」ともいう)から成る組電池として用いられる。このため、組電池を構成する単電池の一つが損傷し上記のような温度域に到達した場合、その発熱により隣接する電池が損傷を受け、連鎖的に組電池全体に損傷が拡がるおそれがある。 A secondary battery used as a power source for a vehicle or the like is generally used as an assembled battery composed of a plurality of cell cells (hereinafter, also referred to as "cells"). Therefore, if one of the cells constituting the assembled battery is damaged and reaches the above temperature range, the adjacent battery may be damaged by the heat generation, and the damage may spread to the entire assembled battery in a chain reaction. ..

ところで、多数の単電池を連結して構成される組電池は、充放電する電流で発熱する。特に、車両用の電源装置として使用される組電池の発熱量は、充放電の電流が極めて大きいことから大きくなる。発熱による温度上昇は電池の電気特性を低下させる原因となる。また、多数の単電池を連結して出力電圧を高くしている車両用の組電池は、組電池を構成する個々の単電池間の温度差をできる限り小さくすることが極めて大切である。それは、単電池間の温度差が電池の電気特性のバランスを崩して残容量を不均一にし、特定の単電池の寿命を短くするからである。このため、通常、車両用の電源装置では、充放電時の温度上昇を少なくするために電池を冷却する装置を備えている。このような冷却装置について、連結された多数の単電池をできるだけ効率的に、かつ均等に冷却することが重要である。 By the way, an assembled battery formed by connecting a large number of cells generates heat by a current that charges and discharges. In particular, the amount of heat generated by the assembled battery used as a power supply device for a vehicle is large because the charging / discharging current is extremely large. The temperature rise due to heat generation causes the electrical characteristics of the battery to deteriorate. Further, in a vehicle assembly battery in which a large number of cells are connected to increase the output voltage, it is extremely important to minimize the temperature difference between the individual cells constituting the assembly battery. This is because the temperature difference between the cells upsets the balance of the electrical characteristics of the batteries, makes the remaining capacity non-uniform, and shortens the life of a specific cell. For this reason, a power supply device for a vehicle is usually provided with a device for cooling a battery in order to reduce a temperature rise during charging / discharging. For such a cooling device, it is important to cool a large number of connected cells as efficiently and evenly as possible.

例えば、特許文献1に記載されているように、通常、冷却装置は熱伝導率の良い金属等で構成される。しかし、電池と冷却装置とが直接に接触すると通電するおそれがあるため、電池と冷却装置の隙間には絶縁性を有する部材が設置される。また、電池と冷却装置の間に隙間ができ冷却効率が低下することを防ぐため、電池と冷却装置を密着させる目的においても充填材が設置される。 For example, as described in Patent Document 1, the cooling device is usually composed of a metal having good thermal conductivity or the like. However, if the battery and the cooling device come into direct contact with each other, there is a risk of energization. Therefore, an insulating member is installed in the gap between the battery and the cooling device. Further, in order to prevent a gap between the battery and the cooling device and a decrease in cooling efficiency, a filler is installed for the purpose of bringing the battery and the cooling device into close contact with each other.

また、特許文献2では、以下の手法が提案されている。複数の単電池を連結した車両用の電源装置は、各々の単電池の間にあって、単電池の表面に熱結合状態に接触してなるセパレータを備える。また、上記電源装置において、単電池の間に冷却隙間を設けてセパレータを介して積層するように固定し、この冷却隙間に冷却気体を強制送風する送風機構を備える。さらに、上記電源装置は、各々の単電池の外周面に熱結合してなる温度均等化プレートを備え、この温度均等化プレートの熱伝導率を単電池間に備えられたセパレータの熱伝導率よりも大きくする。 Further, Patent Document 2 proposes the following method. A power supply device for a vehicle in which a plurality of cells are connected is provided with a separator between the cells, which is in contact with the surface of the cells in a heat-bonded state. Further, the power supply device is provided with a blowing mechanism in which a cooling gap is provided between the cells and fixed so as to be stacked via a separator, and a cooling gas is forcibly blown into the cooling gap. Further, the power supply device includes a temperature equalizing plate formed by heat-bonding to the outer peripheral surface of each cell, and the thermal conductivity of the temperature equalizing plate is based on the thermal conductivity of the separator provided between the cells. Also increase.

特表2014−505333号公報Japanese Patent Application Laid-Open No. 2014-505333 特開2010−272430号公報Japanese Unexamined Patent Publication No. 2010-272430

しかしながら、特許文献1に記載されているような冷却装置は、組電池を構成する単電池のうちの一つが損傷し高温に達した場合にも、隣接する電池への熱の移動を促進してしまうおそれがある。つまり、冷却装置が他の単電池への熱伝導を促進する結果、他の単電池も損傷するおそれがあった。 However, a cooling device as described in Patent Document 1 promotes heat transfer to an adjacent battery even when one of the cells constituting the assembled battery is damaged and reaches a high temperature. There is a risk that it will end up. That is, as a result of the cooling device promoting heat conduction to the other cell, the other cell may also be damaged.

一方、特許文献2においては、組電池を構成する単電池の一つが損傷を受けた場合に冷却用部材を介して隣接する電池に伝わる熱量について、組電池を構成する単電池の発熱量や、組電池を構成する電池以外の部材による伝熱の影響を定量的に考慮した上での検討は十分になされていない。また、異常時に冷却装置の冷媒フローが止まった場合を想定した上での検討はなされていない。異常時に冷却装置の冷媒フローが止まった場合には、冷却装置による組電池外部への除熱効率が低下し、冷却装置を介した隣接セルへの伝熱への寄与が高まるため、より延焼のおそれがある。このため、冷却装置の冷媒フローが止まった状態をも想定して安全性への対策を構築しておくことが極めて重要である。 On the other hand, in Patent Document 2, when one of the cells constituting the assembled battery is damaged, the amount of heat transferred to the adjacent battery via the cooling member is determined by the amount of heat generated by the cells constituting the assembled battery. The study has not been sufficiently conducted after quantitatively considering the influence of heat transfer by members other than the batteries constituting the assembled battery. In addition, no studies have been made on the assumption that the refrigerant flow of the cooling device is stopped in the event of an abnormality. If the refrigerant flow of the cooling device is stopped in the event of an abnormality, the efficiency of heat removal to the outside of the assembled battery by the cooling device will decrease, and the contribution to heat transfer to the adjacent cells via the cooling device will increase, so there is a risk of further fire spread. There is. For this reason, it is extremely important to establish safety measures assuming a state in which the refrigerant flow of the cooling device is stopped.

本発明は、複数の単電池を含む組電池において、単電池間の熱移動を好適に制御する充填部材を提供することを目的とする。 An object of the present invention is to provide a filling member that suitably controls heat transfer between cells in an assembled battery including a plurality of cells.

本発明者は上述した従来技術において十分に検討されていなかった、冷却用部材を介して単電池間を伝達される熱量について着目し、その影響について詳細な検討を行った。その結果、組電池を構成する第1及び第2の単電池を仕切る仕切り部材、並びに組電池を構成する複数の単電池と冷却用部材との間に介装される充填部材について、仕切り部材及び充填部材の熱移動抵抗を適切な範囲内に抑えることで、異常が発生した第1の単電池から第2の単電池に伝わる熱移動量を適切に制御することが重要であることを見出し、本発明に至った。本発明は以下の通りである。 The present inventor paid attention to the amount of heat transferred between the cells via the cooling member, which had not been sufficiently studied in the above-mentioned prior art, and conducted a detailed study on its influence. As a result, the partition member and the partition member for partitioning the first and second cell cells constituting the assembled battery, and the filling member interposed between the plurality of cell cells constituting the assembled battery and the cooling member are provided. We found that it is important to appropriately control the amount of heat transfer from the first cell to the second cell in which an abnormality has occurred by suppressing the heat transfer resistance of the filling member within an appropriate range. The present invention has been reached. The present invention is as follows.

[1] 第1の単電池と、第2の単電池と、前記第1の単電池と前記第2の単電池との間を仕切る仕切り部材とともに組電池を構成する充填部材であって、
前記充填部材は、厚み方向と前記厚み方向に直交する面方向とを有し、前記面方向に沿った第1の面と第2の面とを有し、前記第1の単電池及び前記第2の単電池と前記第1の面において接触するとともに、前記第2の面において前記第1及び第2の単電池を冷却可能な冷却部材と接触し、
前記第1の単電池から発せられる熱が前記仕切り部材を介して前記第2の単電池へ移動する場合の前記仕切り部材の熱移動感度Sが以下の式1により定義され、
前記仕切り部材の熱移動感度S[W/K]=
前記仕切り部材の熱伝導率k[W/m・K]×前記仕切り部材と前記第1および第2の単電池との接触面積A[m]/前記仕切り部材の厚みd[m]・・・(式1)
前記第1の単電池から発せられる熱が前記充填部材及び前記冷却部材を介して前記第2の単電池へ移動する場合の前記充填部材の熱移動感度Sが以下の式2により定義され、
前記充填部材の熱移動感度S[W/K]=
前記充填部材の熱伝導率k[W/m・K]×前記充填部材と前記第1及び第2の単電池との接触面積A[m]/前記充填部材の厚みd[m]・・・(式2)
前記第1の単電池の温度が異常発熱状態の温度以上となった場合において、前記仕切り部材の熱移動感度Sが以下の式3を満たし、
0< S ≦ 2 ・・・(式3)
前記熱移動感度Sと前記充填部材の熱移動感度Sbとの関係が以下の式4を満たす
0.3 ≦(S/S)≦ 4.0 ・・・(式4)
ことを特徴とする充填部材。
[1] A filling member that constitutes an assembled battery together with a partition member that partitions the first cell, the second cell, and the first cell and the second cell.
The filling member has a thickness direction and a surface direction orthogonal to the thickness direction, has a first surface and a second surface along the surface direction, and has the first cell and the first unit. The second cell is in contact with the first surface, and the first and second cells are in contact with a cooling member capable of cooling the first and second cells on the second surface.
The heat transfer sensitivity S d of the partition member when the heat generated from the first cell is transferred to the second cell via the partition member is defined by the following equation 1.
Heat transfer sensitivity of the partition member S d [W / K] =
Thermal conductivity of the partition member k d [W / m · K] × Contact area between the partition member and the first and second cells Ad [m 2 ] / Thickness of the partition member d [m] ... (Equation 1)
The heat transfer sensitivity S b of the filling member when the heat generated from the first cell is transferred to the second cell via the filling member and the cooling member is defined by the following equation 2.
Heat transfer sensitivity of the filling member S b [W / K] =
Thermal conductivity of the filling member k b [W / m · K] × Contact area between the filling member and the first and second cells A b [m 2 ] / thickness of the filling member d [m] ... (Equation 2)
When the temperature of the first cell becomes equal to or higher than the temperature in the abnormal heat generation state, the heat transfer sensitivity S d of the partition member satisfies the following equation 3.
0 <S d ≤ 2 ... (Equation 3)
The relationship between the heat transfer sensitivity S d and the heat transfer sensitivity Sb of the filling member satisfies the following equation 4 0.3 ≤ (S d / S b ) ≤ 4.0 ... (Equation 4)
A filling member characterized by that.

[2] 前記充填部材の厚み方向の熱伝導率が2.0×10−2W/m・K以上10.0W/m・K以下である、[1]に記載の充填部材。 [2] the thickness direction of the thermal conductivity of the filling member is 2.0 × 10 -2 W / m · K or more 10.0 W / m · K or less, the filling member according to [1].

[3] 前記充填部材の厚みが5.0×10−5m以上5.0×10−3m以下である、[1]又は[2]に記載の充填部材。 [3] The filling member according to [1] or [2], wherein the thickness of the filling member is 5.0 × 10 -5 m or more and 5.0 × 10 -3 m or less.

[4] [1]に記載の仕切り部材であって、前記第1の単電池及び前記第2の単電池が異常発熱状態の温度に昇温していない場合において、前記熱移動感度Sの値が2より大きい、仕切り部材。 [4] In the partition member according to [1], when the first cell and the second cell have not been heated to a temperature in an abnormal heat generation state, the heat transfer sensitivity S d . A partition member with a value greater than 2.

[5] [1]に記載の仕切り部材であって、厚み方向と前記厚み方向に直交する面方向とを有し、前記仕切り部材の厚み方向の二面のうち一方の平均温度が180℃を超える場合において、前記厚み方向の熱伝導率が2.0×10−2W/m・K以上2.0W/m・K以下である、仕切り部材。 [5] The partition member according to [1], which has a thickness direction and a surface direction orthogonal to the thickness direction, and the average temperature of one of the two surfaces of the partition member in the thickness direction is 180 ° C. in the case where more than the thermal conductivity of the thickness direction is 2.0 × 10 -2 W / m · K or more 2.0 W / m · K or less, the partition member.

[6] 前記仕切り部材の厚み方向の二面のうち双方の平均温度が80℃を超えない場合において、前記厚み方向の熱伝導率が5.0×10−2W/m・K以上50W/m・K以下である、[4]又は[5]に記載の仕切り部材。 [6] When the average temperature of both of the two surfaces of the partition member in the thickness direction does not exceed 80 ° C., the thermal conductivity in the thickness direction is 5.0 × 10-2 W / m · K or more and 50 W / The partition member according to [4] or [5], which is m · K or less.

[7] 前記第1及び第2の単電池の厚みがLmmである場合に、厚みがL/50mm以上L/10mm以下である、[4]から[6]のいずれか1項に記載の仕切り部材。 [7] The partition according to any one of [4] to [6], wherein when the thickness of the first and second cells is L mm, the thickness is L / 50 mm or more and L / 10 mm or less. Element.

[8] [1]から[3]のいずれか1項に記載の充填部材を含む組電池。
[9] [4]から[7]のいずれか1項に記載の仕切り部材を含む組電池。
[8] An assembled battery including the filling member according to any one of [1] to [3].
[9] An assembled battery including the partition member according to any one of [4] to [7].

[10] 前記熱移動感度Sが式3を満たすとともに、前記熱移動感度Sと前記熱移動感度Sbとの関係が式4を満たす、[1]に記載の前記仕切り部材及び前記充填部材を用いて、前記第1の単電池から前記仕切り部材、前記充填部材及び前記冷却部材を介して前記第2の単電池に伝わる熱量を制御する、熱伝達の制御方法。 [10] The heat transfer sensitivity S d is fulfills Equation 3, the relationship between the heat transfer sensitivity Sb and the heat transfer sensitivity S d satisfies the equation 4, the partition member and the filling member according to [1] A method for controlling heat transfer, which controls the amount of heat transferred from the first cell cell to the second cell cell via the partition member, the filling member, and the cooling member.

本発明によれば、複数の単電池を含む組電池において、単電池間の熱移動を好適に制御することができる。 According to the present invention, in an assembled battery including a plurality of cells, heat transfer between the cells can be suitably controlled.

図1は、充填部材及び冷却部材の構成を説明するとともに、充填部材の熱移動感度を説明する図である。FIG. 1 is a diagram for explaining the configurations of the filling member and the cooling member and explaining the heat transfer sensitivity of the filling member. 図2は、実施形態に係る組電池の一例を示す上面図である。FIG. 2 is a top view showing an example of the assembled battery according to the embodiment. 図3は、図2に示した組電池の側面を、手前側の側板を外した状態で模式的に示す側面図である。FIG. 3 is a side view schematically showing the side surface of the assembled battery shown in FIG. 2 with the side plate on the front side removed. 図4は、単電池の一例を示す図である。FIG. 4 is a diagram showing an example of a cell. 図5は、図4に示した単電池の正面図である。FIG. 5 is a front view of the cell cell shown in FIG. 図6は、図4に示した単電池の側面図である。FIG. 6 is a side view of the cell cell shown in FIG. 図7は、仕切り部材の説明図である。FIG. 7 is an explanatory view of the partition member. 図8は、単電池内部で発した熱の伝達経路を模式的に示す図である。FIG. 8 is a diagram schematically showing a heat transfer path generated inside the cell.

以下、図面を参照して、本発明の実施の形態に係る充填部材、組電池、及び熱伝達の制
御方法を説明する。以下に記載する実施形態の説明は一例であり、本発明は実施形態で説明する構成に限定されない。
Hereinafter, the filling member, the assembled battery, and the heat transfer control method according to the embodiment of the present invention will be described with reference to the drawings. The description of the embodiments described below is an example, and the present invention is not limited to the configuration described in the embodiments.

本実施形態に係る充填部材は、第1の単電池と、第2の単電池と、第1の単電池と第2の単電池との間を仕切る仕切り部材とともに組電池を構成する。また、充填部材は、厚み方向と厚み方向に直交する面方向とを有し、面方向に沿った第1の面と第2の面とを有し、前記第1の単電池及び前記第2の単電池と前記第1の面において接触するとともに、前記第2の面において前記第1及び第2の単電池を冷却可能な冷却部材と接触する。また、充填部材に関して、第1の単電池から発せられる熱が充填部材及び冷却部材を介して第2の単電池へ移動する場合の充填部材の熱移動感度Sは、以下の式(1)により定義される。
熱移動感度S[W/K]=充填部材の熱伝導率k[W/m・K]×充填部材と第1及び第2の単電池との接触面積A[m]/充填部材の厚みd[m]・・・(1)
The filling member according to the present embodiment constitutes an assembled battery together with a partition member that partitions the first cell, the second cell, and the first cell and the second cell. Further, the filling member has a thickness direction and a plane direction orthogonal to the thickness direction, has a first plane and a second plane along the plane direction, and has the first cell and the second. The first and second cells are in contact with the cooling member capable of cooling the first and second cells on the first surface. Further, regarding the filling member, the heat transfer sensitivity S b of the filling member when the heat generated from the first cell is transferred to the second cell via the filling member and the cooling member is given by the following equation (1). Defined by.
Thermal transfer sensitivity S b [W / K] = Thermal conductivity of the filling member k b [W / m · K] × Contact area between the filling member and the first and second cells Ab [m 2 ] / filling the thickness of the member d b [m] ··· (1 )

ここで、本発明において、或る単電池を構成する電極や電解液等を構成する化学物質の一部ないし全てが、単電池の内部で発熱を伴いながら分解反応を起こすことにより、単電池の温度が上昇し、単電池の一部ないし全領域が200℃以上になった状態を「異常発熱状態」という。 Here, in the present invention, some or all of the chemical substances constituting the electrodes and the electrolytic solution constituting a certain cell cause a decomposition reaction inside the cell with heat generation, thereby causing the cell cell to undergo a decomposition reaction. A state in which the temperature rises and a part or the whole area of the cell becomes 200 ° C. or higher is called an "abnormal heat generation state".

[熱移動感度]
図1は、充填部材及び冷却部材の構成を説明するとともに、充填部材の熱移動感度を説明する図である。図1において、例えば、第1の単電池は、単電池200a(セル#1)であり、第2の単電池は単電池200b(セル#2)である。図1を用いて、充填部材10の熱移動感度Sを説明する。熱移動感度Sとは、充填部材10と組電池100を構成する第1の単電池(セル#1)と第1の単電池と異なる第2の単電池(セル#2)とが接触しており、第1の単電池から発せられた熱が第2の単電池に移動する際に、充填部材と第1及び第2の単電池との接触部分を経由して移動する熱量の程度を示す尺度である。
[Heat transfer sensitivity]
FIG. 1 is a diagram for explaining the configurations of the filling member and the cooling member and explaining the heat transfer sensitivity of the filling member. In FIG. 1, for example, the first cell is a cell 200a (cell # 1), and the second cell is a cell 200b (cell # 2). The heat transfer sensitivity S b of the filling member 10 will be described with reference to FIG. The heat transfer sensitivity S b means that the filling member 10 and the first cell (cell # 1) constituting the assembled battery 100 and the second cell (cell # 2) different from the first cell come into contact with each other. When the heat generated from the first cell is transferred to the second cell, the degree of heat transferred via the contact portion between the filling member and the first and second cells is determined. It is a scale to show.

熱移動感度Sは、充填部材10として使用される材料の厚み方向における熱伝導率(k[W/m・K])及び充填部材10とセル#1及びセル#2(第1及び第2の単電池)との接触部分の面積(A[m])と、充填部材10の厚み(d[m])を用いて表すことができる。 Heat transfer sensitivity S b is the thermal conductivity in the thickness direction of the material used as the filler member 10 (k b [W / m · K]) and the filling member 10 and the cell # 1 and cell # 2 (first and second area of the contact portion between the second cell) of the (a b [m 2]) , can be represented by the thickness of the filler member 10 (d b [m]) .

ここで、セル#1から充填部材10及び冷却部材400を介してセル#2に伝わる熱量を考える。充填部材10の厚み方向の2面(面方向に沿った2面)について、セル#1及びセル#2と接触する面を面10a、その裏面を面10bとする。図1において、充填部材10の厚み方向は図1紙面の高さ方向に伸びており、充填部材10の面方向は図1紙面の左右方向に伸びている。冷却部材400は、図1の例では、充填部材10の面10bと密着する平面を有する板状に形成されている。また、充填部材10の厚み方向の熱伝導率をk[W/m・K]と定義し、充填部材10の厚みをd[m]とする。 Here, consider the amount of heat transferred from the cell # 1 to the cell # 2 via the filling member 10 and the cooling member 400. Regarding the two surfaces of the filling member 10 in the thickness direction (two surfaces along the surface direction), the surface in contact with the cell # 1 and the cell # 2 is the surface 10a, and the back surface thereof is the surface 10b. In FIG. 1, the thickness direction of the filling member 10 extends in the height direction of the paper surface of FIG. 1, and the surface direction of the filling member 10 extends in the left-right direction of the paper surface of FIG. In the example of FIG. 1, the cooling member 400 is formed in a plate shape having a flat surface in close contact with the surface 10b of the filling member 10. Further, the thermal conductivity in the thickness direction of the filling member 10 is defined as kb [W / m · K], and the thickness of the filling member 10 is defined as db [m].

さらに、充填部材10の面10aとセル#1とが接触する領域(領域a1とする)の平均温度をT1[℃]、領域a1と面対称の関係となる面10b上の領域(領域b1とする)の平均温度をT2[℃]、充填部材10の面10aとセル#2とが接触する領域(領域a2とする)の平均温度をT4[℃]、領域a2と面対称の関係となる領域(領域b2)の平均温度をT3[℃]とする。 Further, the average temperature of the region where the surface 10a of the filling member 10 and the cell # 1 are in contact (referred to as the region a1) is T1 [° C.], and the region on the surface 10b having a plane-symmetrical relationship with the region a1 (region b1). The average temperature of T2 [° C.] is T2 [° C.], the average temperature of the region where the surface 10a of the filling member 10 and the cell # 2 are in contact (referred to as region a2) is T4 [° C.], and the relationship is plane-symmetrical with the region a2. Let the average temperature of the region (region b2) be T3 [° C.].

平均温度T2が平均温度T1より低い場合、充填部材10の領域a1と領域b1とで表面温度差(T1−T2)が生じている。この場合、充填部材10の領域a1の単位断面積当たりの熱流量(熱流束)q1は、以下の式(3)によって表すことができる。
q1 = k(T1−T2)/d [W/m] ・・・(3)
When the average temperature T2 is lower than the average temperature T1, a surface temperature difference (T1-T2) occurs between the region a1 and the region b1 of the filling member 10. In this case, the heat flow rate (heat flux) q1 per unit cross-sectional area of the region a1 of the filling member 10 can be expressed by the following equation (3).
q1 = k b (T1-T2 ) / d b [W / m 2] ··· (3)

また、平均温度T4が平均温度T3より低い場合、充填部材10の領域b2と領域a2とで表面温度差(T3−T4)が生じている。この場合、充填部材10の領域b2の単位断面積当たりの熱流量(熱流束)q2は、以下の式(4)によって表すことができる。
q2 = k(T3−T4)/d [W/m] ・・・(4)
Further, when the average temperature T4 is lower than the average temperature T3, a surface temperature difference (T3-T4) occurs between the region b2 and the region a2 of the filling member 10. In this case, the heat flow rate (heat flux) q2 per unit cross-sectional area of the region b2 of the filling member 10 can be expressed by the following equation (4).
q2 = k b (T3-T4 ) / d b [W / m 2] ··· (4)

ここで、冷却部材400は、例えば熱伝導性のよい金属等で構成することができる。このため、冷却部材400から外部環境への除熱効率が低く、冷却部材400の周囲が断熱された環境に近い状態となっている場合には、冷却部材400内部の温度はほぼ均一とみなすことができる。このような条件下では、平均温度T2と平均温度T3とがほぼ等しい(T2≒T3)と近似できる。この場合、充填部材10の領域b2の単位断面積当たりの熱流量(熱流束)q2は、以下の式(4−2)によって表すことができる。
q2 ≒ k(T2−T4)/d [W/m] ・・・(4−2)
Here, the cooling member 400 can be made of, for example, a metal having good thermal conductivity. Therefore, when the heat removal efficiency from the cooling member 400 to the external environment is low and the surroundings of the cooling member 400 are in a state close to an insulated environment, the temperature inside the cooling member 400 can be regarded as substantially uniform. can. Under such conditions, the average temperature T2 and the average temperature T3 can be approximated to be substantially equal (T2≈T3). In this case, the heat flow rate (heat flux) q2 per unit cross-sectional area of the region b2 of the filling member 10 can be expressed by the following equation (4-2).
q2 ≒ k b (T2-T4 ) / d b [W / m 2] ··· (4-2)

以上より、セル#1から冷却部材400へ充填部材10を経由して移動する接触面積A[m]当たりの熱量Q1、及び、冷却部材400からセル#2へ充填部材10を経由して移動する接触面積A[m]当たりの熱量Q2は、以下の式(5)および(6)によって表すことができる。
Q1 = A × q1 =A(T1−T2)/d [W] ・・・(5)
Q2 = A × q2 =A(T2−T4)/d [W] ・・・(6)
From the above, the amount of heat Q1 per contact area Ab [m 2 ] that moves from the cell # 1 to the cooling member 400 via the filling member 10, and the amount of heat Q1 from the cooling member 400 to the cell # 2 via the filling member 10 The amount of heat Q2 per moving contact area Ab [m 2 ] can be expressed by the following equations (5) and (6).
Q1 = A b × q1 = A b k b (T1-T2) / d b [W] ··· (5)
Q2 = A b × q2 = A b k b (T2-T4) / d b [W] ··· (6)

充填部材10の熱移動感度Sは、ある単電池から別の単電池に熱が移動する際、それらの単電池が充填部材10に接触している場合に、その充填部材10の接触部分を経由して移動する熱量の程度を示す尺度であるから、以下の式(7)および(8)で定義することができる。
Q1 = S × (T1−T2)[W] ・・・(7)
Q2 = S × (T2−T4)[W] ・・・(8)
Heat transfer sensitivity S b of the filling member 10, when the heat from one unit cell to another of the cells to move, if their unit cells is in contact with the filling member 10, the contact portion of the filling member 10 Since it is a scale indicating the degree of heat transferred via the device, it can be defined by the following equations (7) and (8).
Q1 = S b × (T1-T2) [W] ・ ・ ・ (7)
Q2 = S b × (T2-T4) [W] ・ ・ ・ (8)

熱移動感度Sは、式(5)、式(6)、式(7)、式(8)より、以下の式(9)で表すことができる。
= Q1/(T1−T2) = Q2/(T2−T4)
= A/d [W/K] ・・・(9)
The heat transfer sensitivity S b can be expressed by the following equation (9) from the equations (5), (6), (7), and (8).
S b = Q1 / (T1-T2) = Q2 / (T2-T4)
= A b k b / d b [W / K] ··· (9)

また、仕切り部材1の熱移動感度Sは、仕切り部材1と組電池100を構成する第1の単電池(例えばセル#1)と第1の単電池と異なる第2の単電池(例えばセル#2)とが接触しており、第1の単電池から発せられた熱が第2の単電池に移動する際に、仕切り部材1と第1及び第2の単電池との接触部分を経由して移動する熱量の程度を示す尺度である。 Further, the heat transfer sensitivity S d of the partition member 1 is different from the first cell cell (for example, cell # 1) constituting the partition member 1 and the assembled battery 100 and the second cell cell (for example, cell) different from the first cell cell. # 2) is in contact with each other, and when the heat generated from the first cell is transferred to the second cell, it passes through the contact portion between the partition member 1 and the first and second cells. It is a scale that indicates the degree of heat transfer.

熱移動感度Sは、仕切り部材1として使用される材料の厚み方向における熱伝導率(k[W/m・K])及び仕切り部材1とセル#1およびセル#2との接触部分の面積(A[m])と、仕切り部材1の厚み(d[m])を用いて表すことができる。 The thermal transfer sensitivity S d is the thermal conductivity (k d [W / m · K]) in the thickness direction of the material used as the partition member 1 and the contact portion between the partition member 1 and the cells # 1 and # 2. It can be expressed using the area ( Ad [m 2 ]) and the thickness of the partition member 1 ( dd [m]).

ここで、セル#1から仕切り部材1を介してセル#2に伝わる熱量を考える。仕切り部材1の厚み方向の2面(面1c及び面1d)について、セル#1と接触する面を面1c、その裏面を面1dとする。なお、面1dはセル#2と接触している(図2参照)。また、仕切り部材1の厚み方向の熱伝導率をk[W/m・K]と定義し、仕切り部材1の厚みをd[m]とする。 Here, consider the amount of heat transferred from the cell # 1 to the cell # 2 via the partition member 1. Regarding the two surfaces (surface 1c and surface 1d) in the thickness direction of the partition member 1, the surface in contact with the cell # 1 is defined as surface 1c, and the back surface thereof is defined as surface 1d. The surface 1d is in contact with the cell # 2 (see FIG. 2). Further, the thermal conductivity in the thickness direction of the partition member 1 is defined as k d [W / m · K], and the thickness of the partition member 1 is d d [m].

さらに、仕切り部材1の面1cとセル#1とが接触する領域(領域a3(図示せず)とする)の平均温度をT11[℃]、領域a2と面対称の関係となる面1d上の領域(領域b3(図示せず)とする)の平均温度をT12[℃]とする。 Further, the average temperature of the region where the surface 1c of the partition member 1 and the cell # 1 (referred to as the region a3 (not shown)) is T11 [° C.], and the surface 1d having a plane-symmetrical relationship with the region a2. The average temperature of the region (region b3 (not shown)) is T12 [° C.].

平均温度T12が平均温度T11より低い場合、仕切り部材1の領域a2と領域b2とで表面温度差(T11−T12)が生じている。この場合、仕切り部材1の領域a2の単位断面積当たりの熱流量(熱流束)q3は、上記した式(10)によって表すことができる。また、セル#1からセル#2へ仕切り部材1を経由して移動する接触面積A [m]当たりの熱量Q3は、上述した式(11)によって表すことができる。
q3 = k(T11−T12)/d [W/m] ・・・(10)
Q3 = A × q3 =A(T11−T12)/d [W] ・・・(11)
When the average temperature T12 is lower than the average temperature T11, a surface temperature difference (T11-T12) occurs between the region a2 and the region b2 of the partition member 1. In this case, the heat flow rate (heat flux) q3 per unit cross-sectional area of the region a2 of the partition member 1 can be expressed by the above equation (10). Further, the amount of heat Q3 per contact area Ad [m 2 ] moving from the cell # 1 to the cell # 2 via the partition member 1 can be expressed by the above equation (11).
q3 = k d (T11-T12) / d d [W / m 2 ] ・ ・ ・ (10)
Q3 = A d × q3 = A d k d (T11-T12) / d d [W] ··· (11)

熱移動感度Sは、式(10)及び式(11)より、以下の式(12)で表すことができる。
= Q3/(T11−T12) = A/d [W/K] ・・・(12)
The heat transfer sensitivity S d can be expressed by the following equation (12) from the equations (10) and (11).
S d = Q3 / (T11-T12) = A d k d / d d [W / K] ... (12)

本実施形態では、組電池100を構成する仕切り部材1及び充填部材10に関して、セル#1の温度が異常発熱状態の温度以上となった場合において、仕切り部材1の熱移動感度Sが0<S≦2の条件を満たし、この熱移動感度Sと充填部材10の熱移動感度Sとの関係が0.3≦(S/S)≦4.0との条件を満たすように構成される。このようにすれば、セル#1からの熱が充填部材10及び冷却部材400を介してセル#2に適切に伝達されるように制御できる。すなわち、好適な単電池間の熱移動を行うことができる。 In the present embodiment, with respect to the partition member 1 and the filling member 10 constituting the assembled battery 100, when the temperature of the cell # 1 becomes equal to or higher than the temperature in the abnormal heat generation state, the heat transfer sensitivity S d of the partition member 1 is 0 <. The condition of S d ≤ 2 is satisfied, and the relationship between the heat transfer sensitivity S d and the heat transfer sensitivity S b of the filling member 10 satisfies the condition of 0.3 ≤ (S d / S b ) ≤ 4.0. It is composed of. In this way, the heat from the cell # 1 can be controlled to be appropriately transferred to the cell # 2 via the filling member 10 and the cooling member 400. That is, heat transfer between suitable cells can be performed.

<組電池>
本発明の実施形態に係る組電池について説明する。組電池は、例えば、電気自動車(EV、Electric Vehicle)、ハイブリッド電気自動車(HEV、Hybrid Electric Vehicle)、プラグインハイブリッド電気自動車(PHEV、Plug−in Hybrid Electric Vehicle)、電動重機、電動バイク、電動アシスト自転車、船舶、航空機、電車、無停電電源装置(UPS、Uninterruptible Power Supply)、家庭用蓄電システム、風力/太陽光/潮力/地熱等の再生可能エネルギーを利用した電力系統安定化用蓄電池システム等に搭載される電池パックに適用される。但し、組電池100は、上述のEV等以外の機器に電力を供給する電力源としても使用し得る。
<Assembled battery>
The assembled battery according to the embodiment of the present invention will be described. The assembled battery includes, for example, an electric vehicle (EV, Electric Vehicle), a hybrid electric vehicle (HEV, Hybrid Electric Vehicle), a plug-in hybrid electric vehicle (PHEV, Plug-in Hybrid Electric Vehicle), an electric heavy machine, an electric motorcycle, and an electric assist. Bicycles, ships, aircraft, trains, power supply devices without power failure (UPS, Universal Power Supply), household power storage systems, storage battery systems for power system stabilization using renewable energy such as wind power / solar power / tidal power / geothermal power, etc. Applies to the battery pack installed in. However, the assembled battery 100 can also be used as a power source for supplying power to a device other than the above-mentioned EV or the like.

図2は、複数の単電池(「セル」ともいう)200を用いて形成された組電池100の一例の上面図を示し、図3は、図2に示した組電池100から側板300dを取り外した状態を模式的に示す側面図である。 FIG. 2 shows a top view of an example of an assembled battery 100 formed by using a plurality of cell batteries (also referred to as “cells”) 200, and FIG. 3 shows a side plate 300d removed from the assembled battery 100 shown in FIG. It is a side view which shows the state typically.

〔単電池〕
図4は組電池100を構成する単電池200の一例を示す図であり、図5は図4に示した単電池200の正面図であり、図6は、単電池の右側面図である。図4、図5及び図6に示す一例において、単電池200は、高さ方向(H)、幅方向(W)、厚み方向(D)を有する直方体状に形成されており、その上面に端子210、端子220が設けられている。単電池200は、例えば、リチウムイオンを吸蔵・放出可能な正極及び負極、並びに電解質を備えるリチウムイオン二次電池である。リチウムイオン二次電池以外に、リチウムイオン全固体電池、ニッケル水素電池、ニッケルカドミウム電池、鉛蓄電池等の二次電池を適用し得る。
[Batteries]
FIG. 4 is a diagram showing an example of the cell 200 constituting the assembled battery 100, FIG. 5 is a front view of the cell 200 shown in FIG. 4, and FIG. 6 is a right side view of the cell. In the example shown in FIGS. 4, 5 and 6, the cell 200 is formed in a rectangular parallelepiped shape having a height direction (H), a width direction (W), and a thickness direction (D), and terminals are formed on the upper surface thereof. 210 and terminal 220 are provided. The cell 200 is, for example, a lithium ion secondary battery including a positive electrode and a negative electrode capable of storing and releasing lithium ions, and an electrolyte. In addition to the lithium ion secondary battery, a secondary battery such as a lithium ion all-solid-state battery, a nickel hydrogen battery, a nickel cadmium battery, and a lead storage battery can be applied.

〔組電池〕
図2及び図3において、組電池100は、筐体300と筐体300内に収容された複数の単電池200とを含む。複数の単電池200は、その厚み方向“D”(図2の左右方向)に一列に並べて配置され、単電池200の間に仕切り部材1が介装されている。筐体300は、配列された複数の単電池200の側方を囲むように設けられた側板300a、300b、300c及び300dを有する。側板300a及び側板300bには、図示しない治具などを用いて両者間の距離が縮まるように圧力がかけられ、側板300a及び側板300bに挟まれた各単電池200はその厚み方向に圧力(拘束圧)がかけられた状態で保持される。なお、図2及び図3では、一例として5個の単電池200が例示されているが、単電池の数は適宜選択可能である。また、図2及び図3の例では、組電池100は端子210及び端子220が上方を向くように配置される例を示しているが、組電池100は端子210及び端子220が側方を向くように配置されてもよい。
[Battery set]
In FIGS. 2 and 3, the assembled battery 100 includes a housing 300 and a plurality of single batteries 200 housed in the housing 300. The plurality of cell cells 200 are arranged side by side in a row in the thickness direction "D" (left-right direction in FIG. 2), and a partition member 1 is interposed between the cell cells 200. The housing 300 has side plates 300a, 300b, 300c and 300d provided so as to surround the sides of the plurality of arranged cell batteries 200. Pressure is applied to the side plate 300a and the side plate 300b so as to shorten the distance between them by using a jig (not shown), and each cell 200 sandwiched between the side plate 300a and the side plate 300b is pressured (constrained) in the thickness direction thereof. It is held in a state where pressure) is applied. In addition, in FIG. 2 and FIG. 3, five cell batteries 200 are illustrated as an example, but the number of cell cells can be appropriately selected. Further, in the examples of FIGS. 2 and 3, the assembled battery 100 shows an example in which the terminals 210 and 220 are arranged so as to face upward, but the assembled battery 100 has the terminals 210 and 220 facing sideways. It may be arranged as follows.

上述したように、筐体300内において、複数の単電池200はその厚み方向に並べられ、単電池200間には、仕切り部材1が配置されている。仕切り部材1を介して隣り合う(対向する)単電池200の正極端子(例えば端子210)と負極端子(例えば端子220)とは、バスバー301によって電気的に直列に接続される。これによって、組電池100は、所定の電圧の電力を出力する。 As described above, in the housing 300, the plurality of cell cells 200 are arranged in the thickness direction thereof, and the partition member 1 is arranged between the cell cells 200. The positive electrode terminal (for example, terminal 210) and the negative electrode terminal (for example, terminal 220) of the adjacent (opposing) cell 200 via the partition member 1 are electrically connected in series by the bus bar 301. As a result, the assembled battery 100 outputs electric power having a predetermined voltage.

〔仕切り部材〕
仕切り部材1は、図7に示すように、高さ方向(H)、幅方向(W)及び厚み方向(D)を有する平行平板状、或いはシート状の全体形状を有する。
仕切り部材1は、その厚み方向(D)において、面1cと、この面1cと反対方向に向いた面1dとを有し、組電池100を構成する単電池200間を仕切るために使用される。仕切り部材1は、断熱材110等で構成することができる。また、仕切り部材1の厚みは、単電池200の厚みがL[mm]である場合に、通常、L/50mm以上L/10mm以下の範囲であり、好ましくは、L/30mm以上L/15mm以下の範囲である。
[Partition member]
As shown in FIG. 7, the partition member 1 has a parallel flat plate shape having a height direction (H), a width direction (W), and a thickness direction (D), or a sheet-like overall shape.
The partition member 1 has a surface 1c and a surface 1d facing in the direction opposite to the surface 1c in the thickness direction (D), and is used to partition the cell 200 constituting the assembled battery 100. .. The partition member 1 can be made of a heat insulating material 110 or the like. Further, the thickness of the partition member 1 is usually in the range of L / 50 mm or more and L / 10 mm or less, preferably L / 30 mm or more and L / 15 mm or less when the thickness of the cell 200 is L [mm]. Is the range of.

[断熱材]
断熱材110は、多孔質体材料等で形成される。多孔質体は、例えば、繊維質(繊維状無機物ともいう)や粒子(粉状無機物ともいう)から形成されているものを例示することができる。断熱材110は、例えば、繊維質や粒子を押し固める等の所定の成型技術を用いて形成することができる。
[Insulation]
The heat insulating material 110 is made of a porous material or the like. Examples of the porous body include those formed of fibrous materials (also referred to as fibrous inorganic substances) and particles (also referred to as powdery inorganic substances). The heat insulating material 110 can be formed by using a predetermined molding technique such as compacting fibers or particles.

繊維質(繊維状無機物)は、例えば、紙、コットンシート、ポリイミド繊維、アラミド繊維、ポリテトラフルオロエチレン(PTFE)繊維、ガラス繊維、ロックウール、セラミック繊維及び生体溶解性無機繊維からなる群から選ばれる少なくとも1つであることが好ましく、これらの中でもガラス繊維、ロックウール、セラミック繊維及び生体溶解性無機繊維から選ばれる少なくとも1つであることが特に好ましい。セラミック繊維は、主としてシリカとアルミナからなる繊維(シリカ:アルミナ=40:60〜0:100)であり、具体的には、シリカ・アルミナ繊維、ムライト繊維、アルミナ繊維を用いることができる。 The fiber (fibrous inorganic substance) is selected from the group consisting of, for example, paper, cotton sheet, polyimide fiber, aramid fiber, polytetrafluoroethylene (PTFE) fiber, glass fiber, rock wool, ceramic fiber and biosoluble inorganic fiber. Of these, at least one selected from glass fibers, rock wool, ceramic fibers and biosoluble inorganic fibers is particularly preferable. The ceramic fiber is a fiber mainly composed of silica and alumina (silica: alumina = 40: 60 to 0: 100), and specifically, silica-alumina fiber, mullite fiber, and alumina fiber can be used.

また、粒子(粉末状無機物)は、例えば、シリカ粒子、アルミナ粒子、ケイ酸カルシウム、粘土鉱物、バーミキュライト、マイカ、セメント、パーライト、フュームドシリカ及びエアロゲルからなる群から選ばれる少なくとも1つであることが好ましく、これらの中でもシリカ粒子、アルミナ粒子、粘土鉱物は主としてケイ酸マグネシウム(タルク、セピオライトを含む)、モンモリナイト、カオリナイトである。 Further, the particles (powdered inorganic substances) are at least one selected from the group consisting of, for example, silica particles, alumina particles, calcium silicate, clay minerals, vermiculite, mica, cement, pearlite, fumed silica and aerogel. Of these, silica particles, alumina particles, and clay minerals are mainly magnesium silicate (including talc and sepiolite), montmorillonite, and kaolinite.

[充填部材及び冷却部材]
図3に示すように、筐体300の底部には、冷却部材(冷却装置ともいう)400が配置されている。複数の単電池200の夫々の底面は、平行平板状の充填部材10の上面と接触し、充填部材10の下面の一部ないし全面は、冷却部材400と接している。各単電池200からの熱は、充填部材10を介して冷却部材400へ伝達可能となっている。
[Filling member and cooling member]
As shown in FIG. 3, a cooling member (also referred to as a cooling device) 400 is arranged at the bottom of the housing 300. The bottom surface of each of the plurality of cell cells 200 is in contact with the upper surface of the parallel flat plate-shaped filling member 10, and a part or the entire surface of the lower surface of the filling member 10 is in contact with the cooling member 400. The heat from each cell 200 can be transferred to the cooling member 400 via the filling member 10.

冷却部材400は、例えばヒートシンクなどである。冷却部材400は、その内部で流体(冷媒)を移動(循環等)させるものであってもなくてもよい。充填部材10は、例えば、一種類以上の材料、例えば一種類以上のプラスチック、プラスチックコンパウンド、プラスチック・金属複合材料などのうちの単独、又は適宜の組み合わせによって形成される。 The cooling member 400 is, for example, a heat sink or the like. The cooling member 400 may or may not move (circulate, etc.) a fluid (refrigerant) inside the cooling member 400. The filling member 10 is formed, for example, by one or more kinds of materials, for example, one or more kinds of plastics, plastic compounds, plastic / metal composite materials, etc., alone or in an appropriate combination.

図8は、単電池200内部で発した熱の伝達経路を模式的に示す。単電池200内部での発熱は、各種伝達経路を介して、他の単電池200に伝達される。図6の例では、複数の単電池200のうちの一つであるセル#1(CELL #1)からの熱の伝達経路が模式的に
示されている。例えば、単電池200(セル#1)内部での発熱は、仕切り部材1を介して、他の単電池200(セル#2(CELL #2))に伝達することができる。また、単電池
200からの熱は、バスバー301を介して外部に放熱される。また、単電池200からの熱は、充填部材10を介して冷却部材400に伝達され、冷却部材400から外部へ放熱することができる。
FIG. 8 schematically shows a heat transfer path generated inside the cell 200. The heat generated inside the cell 200 is transmitted to the other cell 200 via various transmission paths. In the example of FIG. 6, the heat transfer path from the cell # 1 (CELL # 1), which is one of the plurality of cell 200, is schematically shown. For example, the heat generated inside the cell 200 (cell # 1) can be transmitted to another cell 200 (cell # 2) via the partition member 1. Further, the heat from the cell 200 is dissipated to the outside via the bus bar 301. Further, the heat from the cell 200 is transferred to the cooling member 400 via the filling member 10, and can be dissipated from the cooling member 400 to the outside.

<組電池における発熱及び熱移動>
ここで、組電池100における発熱及び熱移動について説明する。単電池200を構成する電極や電解液等を構成する化学物質の一部ないし全てが、単電池200内部で発熱を伴いながら分解反応を起こすことにより、単電池200の温度が上昇し、単電池200の一部ないし全領域が200℃以上になる場合がある。即ち、単電池200が異常発熱状態となる場合がある。
<Heat generation and heat transfer in the assembled battery>
Here, heat generation and heat transfer in the assembled battery 100 will be described. Some or all of the chemical substances that make up the electrodes and electrolytes that make up the cellar 200 cause a decomposition reaction inside the cellar 200 with heat generation, which raises the temperature of the cellar 200 and causes the cellar battery 200 to rise in temperature. A part or all of 200 may reach 200 ° C. or higher. That is, the cell 200 may be in an abnormal heat generation state.

一般に、単電池200を構成する材料のうち正極材料の安全性について、充電による脱リチウム後の結晶構造の安定性が大きく影響していることが知られている。正極材料として一般に用いられるLiCoO、Li(Ni1/3Mn1/3Co1/3)O、Li(Ni0.8Co0.15Al0.05)O等の材料は、充電状態では高温下で、酸素放出を伴う結晶崩壊を起こす。正極から放出された酸素は電解液の酸化等を引き起こし、急激な発熱反応を伴う。放射光を用いた構造解析により、上記正極材料種では200℃付近で結晶の相転移が起こることが報告されている。このため、単電池200の一部ないし全領域が200℃以上になる場合、正極の結晶崩壊が進行している、つまり単電池200が熱暴走状態にあることを意味する(参考文献1:リチウムイオン電池の高安全技術と材料 シーエムシー出版、P.44/参考文献2:J.Dahn et al., Electrochemistry Communication, 9, 2534−2540 (2007)/参考文献3:小林弘典、「放射光を用いたリチウムイオン二次電池用正極材料の評価・解析技術」Spring−8利用推進協議会 ガラス・セラミックス研究会(第二回)(2011))。 In general, it is known that the stability of the crystal structure after delithiumization by charging has a great influence on the safety of the positive electrode material among the materials constituting the cell 200. Materials such as LiCoO 2 , Li (Ni 1/3 Mn 1/3 Co 1/3 ) O 2 , Li (Ni 0.8 Co 0.15 Al 0.05 ) O 2, which are generally used as positive electrode materials, can be charged. In the state, crystal collapse accompanied by oxygen release occurs at high temperature. Oxygen released from the positive electrode causes oxidation of the electrolytic solution and the like, accompanied by a rapid exothermic reaction. Structural analysis using synchrotron radiation has reported that the phase transition of crystals occurs at around 200 ° C. in the above positive electrode material species. Therefore, when a part or the whole region of the cell 200 is 200 ° C. or higher, it means that the crystal decay of the positive electrode is progressing, that is, the cell 200 is in a thermal runaway state (Reference 1: Lithium). High Safety Technology and Materials for Ion Batteries CMC Publishing, P.44 / Reference 2: J. Dahn et al., Electrochemical Communication, 9, 2534-2540 (2007) / Reference 3: Hironori Kobayashi, "Radiation Light Evaluation and analysis technology for positive electrode materials for lithium-ion secondary batteries used "Spring-8 Utilization Promotion Council Glass and Ceramics Study Group (2nd) (2011)).

また、単電池200を構成する材料のうち負極材料の安全性について、充電負極(リチウム挿入炭素負極)は基本的にリチウム金属と同様の強い還元性を示し、電解液との反応で負極表面上に被膜が形成され、それによってさらなる反応が抑制されていることが知られている。従って、その保護被膜の化学的組成や構造、熱安定性が温度上昇時の充電負極の熱安定性に多大な影響を与える。通常、充電負極と電解液との反応は、保護被膜の形成と、それに続く被膜破壊による爆発的な還元分解反応により説明される。一般に、負極上
での保護被膜形成反応は130℃付近から、引き続く被膜分解反応が200℃付近で進行し、最終的に爆発的還元分解反応に至ることが報告されている。このため、単電池200の一部ないし全領域が200℃以上になる場合、負極表面の被膜破壊が進行している、つまり単電池200が熱暴走状態にあることを意味する(参考文献4:電池ハンドブック第1版 オーム社、P.591/参考文献5:リチウムイオン電池の高安全技術・評価技術の最前線 シーエムシー出版、P.90)。
Regarding the safety of the negative electrode material among the materials constituting the cell 200, the charged negative electrode (lithium-inserted carbon negative electrode) basically exhibits the same strong reducing property as that of lithium metal, and reacts with the electrolytic solution on the negative electrode surface. It is known that a film is formed on the electrode, thereby suppressing further reactions. Therefore, the chemical composition, structure, and thermal stability of the protective coating have a great influence on the thermal stability of the charging negative electrode when the temperature rises. Usually, the reaction between the charged negative electrode and the electrolytic solution is explained by the formation of a protective film and the subsequent explosive reduction decomposition reaction due to film destruction. In general, it has been reported that the protective film forming reaction on the negative electrode proceeds from around 130 ° C., the subsequent film decomposition reaction proceeds at around 200 ° C., and finally reaches an explosive reduction decomposition reaction. Therefore, when a part or the entire region of the cell 200 is 200 ° C. or higher, it means that the coating on the negative electrode surface is being destroyed, that is, the cell 200 is in a thermal runaway state (Reference 4: Reference 4: Battery Handbook 1st Edition Ohm, P.591 / Reference 5: Forefront of high safety technology and evaluation technology for lithium-ion batteries CMC Publishing, p.90).

また、本発明において、単電池200を構成する電極や電解液等を構成する化学物質が、単電池200内部で一定以上の発熱速度を伴う分解反応を起こしていない状態を、「通常状態」という。ここで、反応性化学物質が断熱条件下で自己発熱分解する際の熱的挙動を定量的に測定する手段であるARC(Accelerating rate calorimetry)を用いて、単電池200の発熱状態を評価することができる。例えばDahnらは、ARCにおいて観測される発熱速度が0.04℃/minを上回る場合に、セル内部で自己発熱反応が進行しているものと定義しており、これに倣うことができる(参考文献6:J.Dahn et al., Electrochimica Acta, 49, 4599−4604 (2004))。 Further, in the present invention, a state in which the chemical substances constituting the electrodes and the electrolytic solution constituting the cell 200 do not undergo a decomposition reaction accompanied by a heat generation rate of a certain level or higher inside the cell 200 is referred to as a "normal state". .. Here, the heat generation state of the cell 200 is evaluated by using ARC (Accelerating rate assessment), which is a means for quantitatively measuring the thermal behavior when the reactive chemical substance self-heats and decomposes under adiabatic conditions. Can be done. For example, Dahn et al. Define that the self-exothermic reaction is proceeding inside the cell when the exothermic rate observed in ARC exceeds 0.04 ° C / min, which can be followed (reference). Reference 6: J. Dachn et al., Electrochimica Acta, 49, 4599-4604 (2004)).

また、本発明において、通常状態の単電池200を、「通常状態を保持している単電池」、通常状態を逸脱し異常発熱状態に至っていない単電池200を、「通常状態を逸脱した単電池」という。単電池200が通常状態を逸脱していない場合に想定される表面平均温度の上限値は通常80℃である。ここで、汎用電解液成分の沸点は、下記表1に示すように90℃以上である。汎用電解液成分は、例えば、エチレンカーボネート(EC)、ジエチルカーボネート、ジメチルカーボネート(DMC)、エチルメチルカーボネート(EMC)である。単電池200の表面平均温度が80℃より低い場合は、単電池200を構成する汎用電解液自体の沸騰には至らない。

Figure 0006954214
Further, in the present invention, the cell 200 in the normal state is referred to as a "cell that holds the normal state", and the cell 200 that deviates from the normal state and does not reach the abnormal heat generation state is referred to as a "cell that deviates from the normal state". ". The upper limit of the surface average temperature assumed when the cell 200 does not deviate from the normal state is usually 80 ° C. Here, the boiling point of the general-purpose electrolytic solution component is 90 ° C. or higher as shown in Table 1 below. General-purpose electrolyte components are, for example, ethylene carbonate (EC), diethyl carbonate, dimethyl carbonate (DMC), and ethyl methyl carbonate (EMC). When the surface average temperature of the cell 200 is lower than 80 ° C., the general-purpose electrolytic solution itself constituting the cell 200 does not boil.
Figure 0006954214

例えば、仕切り部材1に接触する単電池200が通常状態を逸脱し、異常発熱状態に至っていない場合に想定される表面平均温度の上限値が180℃とする。ここで、仕切り部材1の材料が、仮に、汎用セパレータ材であるポリエチレンやポリプロピレン製であると仮定する。この場合、そのメルトダウン温度は160〜200℃であることが知られている。このため、単電池200の表面平均温度が180℃を超える場合には、単電池200を構成する汎用セパレータ材の一部がメルトダウンし、異常発熱状態に至るおそれがある。 For example, the upper limit of the surface average temperature assumed when the cell 200 in contact with the partition member 1 deviates from the normal state and does not reach the abnormal heat generation state is 180 ° C. Here, it is assumed that the material of the partition member 1 is made of polyethylene or polypropylene, which is a general-purpose separator material. In this case, the meltdown temperature is known to be 160-200 ° C. Therefore, when the surface average temperature of the cell 200 exceeds 180 ° C., a part of the general-purpose separator material constituting the cell 200 may melt down, resulting in an abnormal heat generation state.

これに対し、仕切り部材1の、組電池100を構成する単電池200間を仕切る厚み方向の二面(厚み方向と直交する二面、すなわち面1c及び面1d)のうちの一方の平均温度が100℃を超えない範囲では、仕切り部材1は、組電池100中の単電池200(例えばセル#1)からの熱をその厚み方向に伝達し、セル#1に仕切り部材1を介して対向する他の単電池200(セル#2)や単電池200以外の部材(例えばバスバー301や冷却部材400)へ伝達することができる。これに対し、平均温度が100℃を超える場合には、熱により仕切り部材1が開口して内包された液体が気相状態又は液相状態で仕切り部材1の外部に流出する。この流出によって仕切り部材1内の断熱材110に空気(断熱作用を有する)が入り、厚み方向の断熱性(熱抵抗)を増加させる。これによって、セ
ル#1から仕切り部材1を介してセル#2へ伝達される熱量を減らすことができる。すなわち、或る単電池200が通常状態を逸脱した状態になることを契機に他の単電池200が通常状態を逸脱した状態となるのを回避することができる。
On the other hand, the average temperature of one of the two surfaces of the partition member 1 in the thickness direction (two surfaces orthogonal to the thickness direction, that is, the surfaces 1c and 1d) that partition the cell 200 constituting the assembled battery 100 is Within a range not exceeding 100 ° C., the partition member 1 transfers heat from the cell 200 (for example, cell # 1) in the assembled battery 100 in the thickness direction thereof, and faces the cell # 1 via the partition member 1. It can be transmitted to other members other than the cell 200 (cell # 2) and the cell 200 (for example, the bus bar 301 and the cooling member 400). On the other hand, when the average temperature exceeds 100 ° C., the partition member 1 is opened by heat and the contained liquid flows out of the partition member 1 in a vapor phase state or a liquid phase state. Due to this outflow, air (having a heat insulating action) enters the heat insulating material 110 in the partition member 1, and the heat insulating property (thermal resistance) in the thickness direction is increased. As a result, the amount of heat transferred from the cell # 1 to the cell # 2 via the partition member 1 can be reduced. That is, it is possible to prevent another cell 200 from deviating from the normal state when a certain cell 200 deviates from the normal state.

なお、仕切り部材1の、組電池を構成する単電池間を仕切る厚み方向の二面(面1c及び面1d)の双方の平均温度が80℃よりも低い場合は、内包された液体により厚み方向への熱移動が促進される。組電池100を構成する全ての単電池200が通常状態である場合、仕切り部材1の熱移動抵抗が従来品より低いため、組電池100内の単電池200間の均温化に奏功し、温度ムラによる単電池200の劣化を軽減する効果が期待できる。 If the average temperature of both the two surfaces (surfaces 1c and 1d) of the partition member 1 in the thickness direction that partition the cells constituting the assembled battery is lower than 80 ° C., the thickness direction is due to the contained liquid. Heat transfer to is promoted. When all the cells 200 constituting the assembled battery 100 are in the normal state, the heat transfer resistance of the partition member 1 is lower than that of the conventional product, so that the temperature can be leveled between the cells 200 in the assembled battery 100 and the temperature can be adjusted. The effect of reducing the deterioration of the cell 200 due to unevenness can be expected.

<異常発熱状態の単電池の冷却>
本実施形態に係る仕切り部材1は、材料や構造の選択によって、仕切り部材1の厚み方向の二面(面1c及び面1d)のうち一方の平均温度が180℃を超える場合において、厚み方向の熱伝導率が2.0×10−2W/m・K以上2.0W/m・K以下となるように構成される。また、仕切り部材1は、その厚み方向の二面(面1c及び面1d)のうち双方の平均温度が80℃を超えない場合において、厚み方向の熱伝導率が5.0×10−2W/m・K以上50W/m・K以下となるように構成される。
<Cooling of a single battery in an abnormal heat generation state>
The partition member 1 according to the present embodiment is in the thickness direction when the average temperature of one of the two surfaces (surface 1c and surface 1d) in the thickness direction of the partition member 1 exceeds 180 ° C. depending on the selection of the material and structure. The thermal conductivity is configured to be 2.0 × 10 -2 W / m · K or more and 2.0 W / m · K or less. Further, the partition member 1 has a thermal conductivity of 5.0 × 10-2 W in the thickness direction when the average temperature of both of the two surfaces (surface 1c and surface 1d) in the thickness direction does not exceed 80 ° C. It is configured to be at least / m · K and at least 50 W / m · K.

例えば、図3や図8に示すように、仕切り部材1によって仕切られる二つの単電池200(例えばセル#1とセル#2)があり、セル#1が面1cと接触し、セル#2が面1dと接触している状態において、面1c及び面1dの双方の平均温度が80℃以下の場合には、仕切り部材1を介しての熱移動が行われる。一方、セル#1及びセル#2の一方(例えばセル#1)の温度が昇温し、セル#1と接触する面1cの平均温度が180℃を超える場合には、仕切り部材1の熱伝導率が低下(断熱性が向上)し、熱がセル#2へ伝達されにくくなる。これにより、セル#2の損傷を回避する。 For example, as shown in FIGS. 3 and 8, there are two cell cells 200 (for example, cell # 1 and cell # 2) partitioned by the partition member 1, cell # 1 comes into contact with surface 1c, and cell # 2 becomes. When the average temperature of both the surface 1c and the surface 1d is 80 ° C. or lower in the state of being in contact with the surface 1d, heat transfer is performed through the partition member 1. On the other hand, when the temperature of one of cell # 1 and cell # 2 (for example, cell # 1) rises and the average temperature of the surface 1c in contact with cell # 1 exceeds 180 ° C., the heat conduction of the partition member 1 The rate is reduced (insulation is improved), and heat is less likely to be transferred to cell # 2. This avoids damage to cell # 2.

セル#1から発せられる熱の多くは、充填部材10を介して冷却部材400に伝達される。 Most of the heat generated from the cell # 1 is transferred to the cooling member 400 via the filling member 10.

また、充填部材10に移動した熱のうちの一部は、充填部材10や冷却部材400を介して、異常発熱状態になった単電池200以外の単電池200に伝達される。異常発熱状態になった単電池200以外の単電池200は、例えば、異常発熱状態になった単電池200と仕切り部材1を介して対向する(仕切り部材を挟んで隣接する)単電池200である。例えば、図8に示す例では、単電池200の一つであるセル#1が異常発熱状態となった場合に、そのセル#1からの熱の一部が充填部材10及び冷却部材400を介してセル#2に伝達される。 Further, a part of the heat transferred to the filling member 10 is transferred to the cell 200 other than the cell 200 which has become abnormally heat-generating through the filling member 10 and the cooling member 400. The cell 200 other than the cell 200 in the abnormal heat generation state is, for example, the cell 200 facing the cell battery 200 in the abnormal heat generation state via the partition member 1 (adjacent with the partition member interposed therebetween). .. For example, in the example shown in FIG. 8, when the cell # 1, which is one of the cell 200, is in an abnormal heat generation state, a part of the heat from the cell # 1 passes through the filling member 10 and the cooling member 400. Is transmitted to cell # 2.

充填部材の熱伝導率は、好ましくは2.0×10−2W/m・K以上50.0W/m・K以下である。また、充填部材の厚みは厚み5.0×10−5m以上5.0×10−2m以下であることが好ましい。 The thermal conductivity of the filling member is preferably 2.0 × 10 -2 W / m · K or more 50.0W / m · K or less. Further, the thickness of the filling member is preferably 5.0 × 10-5 m or more and 5.0 × 10 −2 m or less.

[充填部材]
このため、実施形態に係る充填部材10は、一例として、図1に示した構成を備える。本実施形態では、充填部材10は、平行平板状に形成され、その厚み方向は、仕切り部材1の高さ方向(H)に配置され、充填部材10の面方向は、仕切り部材1の厚み方向(D)に配置されている。また、充填部材10は、その面方向に沿った第1及び第2の面を有する。本実施形態では、充填部材10は、平行平板状に形成され、第1の面に相当する面
10a及び第2の面に相当する面10bを有する。面10aは上方を向き、面10bはその反対方向(下方)を向いている。充填部材10は、面10aにおいて、組電池100を構成する第1及び第2の単電池を含む複数の単電池と接触する。本実施形態では、セル#1が第1の単電池に相当し、セル#2が第2の単電池に相当する。また、充填部材10は、面10bにおいて、第1及び第2の単電池を含む複数の単電池を冷却可能な冷却部材400と接触する。
[Filling member]
Therefore, the filling member 10 according to the embodiment includes the configuration shown in FIG. 1 as an example. In the present embodiment, the filling member 10 is formed in a parallel flat plate shape, the thickness direction thereof is arranged in the height direction (H) of the partition member 1, and the surface direction of the filling member 10 is the thickness direction of the partition member 1. It is arranged in (D). Further, the filling member 10 has first and second surfaces along the surface direction thereof. In the present embodiment, the filling member 10 is formed in a parallel flat plate shape and has a surface 10a corresponding to the first surface and a surface 10b corresponding to the second surface. The surface 10a faces upward, and the surface 10b faces in the opposite direction (downward). The filling member 10 comes into contact with a plurality of batteries including the first and second batteries constituting the assembled battery 100 on the surface 10a. In this embodiment, cell # 1 corresponds to the first cell and cell # 2 corresponds to the second cell. Further, the filling member 10 comes into contact with the cooling member 400 capable of cooling a plurality of cells including the first and second cells on the surface 10b.

<実施例>
次に実施例により本発明の具体的態様を更に詳細に説明するが、本発明はこれらの例によって限定されるものではない。
<Example>
Next, specific embodiments of the present invention will be described in more detail with reference to Examples, but the present invention is not limited to these examples.

以下に説明する実施例及び比較例では、異常発熱状態となった単電池200から他の単電池200への伝熱経路のうち、単電池200間を仕切る仕切り部材1の熱移動量と、単電池200と冷却部材400との間に配置される充填部材10を介する熱移動量とに着目し、仕切り部材1及び充填部材10による単電池200間の伝熱量抑制の可能性を検討した。 In the examples and comparative examples described below, among the heat transfer paths from the cell 200 in the abnormally generated state to the other cell 200, the heat transfer amount of the partition member 1 partitioning between the cells 200 and the single unit. Focusing on the amount of heat transfer through the filling member 10 arranged between the battery 200 and the cooling member 400, the possibility of suppressing the amount of heat transfer between the cell 200 by the partition member 1 and the filling member 10 was examined.

評価対象の組電池100として、図8に示すような5つの単電池200が連結された組電池モデルを構築し、セル#1に異常発熱状態時相当の発熱量1.4×10[J/m](NMC系正極を用いたセル#2の熱量評価から推定される総発熱量)を与え、以下の実施例1〜5並びに比較例1及び2の条件において、熱伝導方程式を有限要素法により解くことにより、セル#1に隣接するセル#2の温度推移を推算し、充填部材10の熱移動感度の変化によるセル間の伝熱量抑制等の効果を評価した。ここで、解析にはCOMSOL AB社製の汎用物理シミュレーションソフトウエアであるCOMSOL Multiphysicsを用い、下記参考文献9、10を参照して解析した。なお、セル#1とセル#2との間の伝熱経路については、図8で説明した経路が想定される(参考文献9:特開2006−010648号公報、参考文献10:R.M.Spotnitz et al., J.Power Sources 163, 1080−1086,(2007))。 As the assembled battery 100 to be evaluated, a assembled battery model in which five cell batteries 200 as shown in FIG. 8 are connected is constructed, and the calorific value corresponding to the abnormal heat generation state is 1.4 × 10 9 [J]. / M 3 ] (total calorific value estimated from the calorific value evaluation of cell # 2 using the NMC-based positive electrode) was given, and the heat conduction equation was finite under the conditions of Examples 1 to 5 and Comparative Examples 1 and 2 below. By solving by the element method, the temperature transition of the cell # 2 adjacent to the cell # 1 was estimated, and the effect of suppressing the heat transfer amount between the cells due to the change in the heat transfer sensitivity of the filling member 10 was evaluated. Here, COMSOL Multiphysics, which is general-purpose physics simulation software manufactured by COMSOL AB, was used for the analysis, and the analysis was performed with reference to the following references 9 and 10. As the heat transfer path between cell # 1 and cell # 2, the path described in FIG. 8 is assumed (Reference 9: Japanese Patent Application Laid-Open No. 2006-010648, Reference 10: RM. Spotnitz et al., J. Power Sources 163, 1080-1086 (2007)).

実施例及び比較例において、セル#1〜#5の夫々のサイズは、ドイツ自動車工業会で規定されているPHEV2サイズ(縦91mm、幅148mm、厚み26.5mm)とした。また、簡単のため、冷却部材400はアルミニウムやアルミニウム合金等の金属で構成された厚み約4mmの板状材料であると想定し、熱伝導率は200W/m・Kとした。セル#1及び#2と冷却部材400との間に設置される充填部材10は、絶縁塗料等の塗膜またはプラスチックフィルムであると想定した。充填部材10に関しては、膜厚、フィラー(充填部材10内への詰め物)の種類や充填量、あるいは充填部材10の構造体をなすプラスチックの種類で熱移動抵抗を変更できる。また、セル#1とセル#2の間に設置される仕切り部材1は断熱性の材料であると想定した。バスバー301は、アルミニウム製であるものと想定し、熱伝導率は237W/m・Kとした。また、冷却部材400に関して、冷媒の流れ(フロー)が止まった状態を想定し、冷却部材400の周囲の環境には、自然対流相当の熱伝達係数を与えた。これらの条件下で、セル#1が異常発熱状態に至ってから300秒間のセル#2内の温度推移を推算した。 In Examples and Comparative Examples, the sizes of cells # 1 to # 5 were PHEV2 sizes (length 91 mm, width 148 mm, thickness 26.5 mm) specified by the German Association of the Automotive Industry. For simplicity, the cooling member 400 is assumed to be a plate-like material having a thickness of about 4 mm and made of a metal such as aluminum or an aluminum alloy, and has a thermal conductivity of 200 W / m · K. It is assumed that the filling member 10 installed between the cells # 1 and # 2 and the cooling member 400 is a coating film such as an insulating paint or a plastic film. Regarding the filling member 10, the heat transfer resistance can be changed by the film thickness, the type and filling amount of the filler (filling in the filling member 10), or the type of plastic forming the structure of the filling member 10. Further, it is assumed that the partition member 1 installed between the cells # 1 and the cell # 2 is a heat insulating material. The bus bar 301 was assumed to be made of aluminum and had a thermal conductivity of 237 W / m · K. Further, regarding the cooling member 400, assuming a state in which the flow of the refrigerant is stopped, a heat transfer coefficient equivalent to natural convection is given to the environment around the cooling member 400. Under these conditions, the temperature transition in the cell # 2 was estimated for 300 seconds after the cell # 1 reached the abnormal heat generation state.

なお、実施例1〜5並びに比較例1及び2においては、異常発熱状態の温度に達した単電池200から伝達された熱に起因する昇温の程度を明確にするため、セル#1以外のセル#2〜セル#5については、セルの自己発熱による昇温を考慮していない。 In Examples 1 to 5 and Comparative Examples 1 and 2, in order to clarify the degree of temperature rise due to the heat transferred from the cell 200 that has reached the temperature of the abnormal heat generation state, other than cell # 1. Regarding cells # 2 to cell # 5, the temperature rise due to the self-heating of the cells is not taken into consideration.

以下の表2に、実施例1−1〜1−5並びに比較例1−1及び1−2の結果を示す。

Figure 0006954214
Table 2 below shows the results of Examples 1-1 to 1-5 and Comparative Examples 1-1 and 1-2.
Figure 0006954214

実施例1−1〜1−5並びに比較例1−1及び1−2では、仕切り部材1の膜厚(厚み方向の寸法)は1mmで固定とした。また、仕切り部材1の熱伝導率kについては、面1cや面1dの平均温度の変化に拘わらず一定(0.1W/(m・K))とした。膜厚及び熱伝導率kが一定のため、熱移動感度Sも一定の値(1.35W/K)であった。この熱移動感度Sは、0<S≦2の範囲に収まる。一方、充填部材10に関しては、熱伝導率kを変化させて測定を行った。各熱伝導率kに対する熱移動感度Sと感度比(S/S)とを求めた。 In Examples 1-1 to 1-5 and Comparative Examples 1-1 and 1-2, the film thickness (dimension in the thickness direction) of the partition member 1 was fixed at 1 mm. Further, the thermal conductivity k d of the partition member 1 was set to be constant (0.1 W / (m · K)) regardless of the change in the average temperature of the surface 1c and the surface 1d. Since the film thickness and the thermal conductivity k d were constant, the heat transfer sensitivity S d was also a constant value (1.35 W / K). This heat transfer sensitivity S d falls within the range of 0 <S d ≦ 2. On the other hand, with respect to the filling member 10, the measurement was carried out by changing the thermal conductivity k b. The heat transfer sensitivity S b and the sensitivity ratio (S d / S b ) for each thermal conductivity k b were determined.

(比較例1−1)
充填部材10に熱伝導率kが2.0W/m・Kの材料を用い、膜厚は1mmとした。セル#1に異常が発生してから152秒後に、セル#2内部の最高温度が212.4℃に到達するものと推算された。この場合の充填部材10の熱移動感度Sは7.84W/Kであり、感度比S/Sは0.172であった。
(Comparative Example 1-1)
The thermal conductivity k b is a material of 2.0 W / m · K in the filling member 10, the film thickness was 1 mm. It was estimated that the maximum temperature inside cell # 2 would reach 212.4 ° C. 152 seconds after the abnormality occurred in cell # 1. In this case, the heat transfer sensitivity S b of the filling member 10 was 7.84 W / K, and the sensitivity ratio S d / S b was 0.172.

(実施例1−1)
充填部材10に熱伝導率kが1.0W/m・Kの材料を用い、膜厚は1mmとした。セル#1に異常が発生してから168秒後に、セル#2内部の最高温度が208.7℃に到達するものと推算された。この場合の充填部材10の熱移動感度Sは3.92W/Kであり、感度比S/Sは0.344であった。
(Example 1-1)
The thermal conductivity k b is a material of 1.0 W / m · K in the filling member 10, the film thickness was 1 mm. It was estimated that the maximum temperature inside cell # 2 reached 208.7 ° C. 168 seconds after the abnormality occurred in cell # 1. In this case, the heat transfer sensitivity S b of the filling member 10 was 3.92 W / K, and the sensitivity ratio S d / S b was 0.344.

(実施例1−2)
充填部材10に熱伝導率kが0.8W/m・Kの材料を用い、膜厚は1mmとした。セル#1に異常が発生してから168秒後に、セル#2内部の最高温度が207.9℃に到達するものと推算された。この場合の充填部材10の熱移動感度Sは3.13W/Kであり、感度比S/Sは0.431であった。
(Example 1-2)
The thermal conductivity k b is a material of 0.8 W / m · K in the filling member 10, the film thickness was 1 mm. It was estimated that the maximum temperature inside cell # 2 reached 207.9 ° C. 168 seconds after the abnormality occurred in cell # 1. In this case, the heat transfer sensitivity S b of the filling member 10 was 3.13 W / K, and the sensitivity ratio S d / S b was 0.431.

(実施例1−3)
充填部材10に熱伝導率kが0.6W/m・Kの材料を用い、膜厚は1mmとした。セル#1に異常が発生してから175秒後に、セル#2内部の最高温度が207.1℃に到達するものと推算された。この場合の充填部材10の熱移動感度Sは2.35W/K
であり、感度比S/Sは0.574であった。
(Example 1-3)
The thermal conductivity k b is a material of 0.6 W / m · K in the filling member 10, the film thickness was 1 mm. It was estimated that the maximum temperature inside cell # 2 would reach 207.1 ° C. 175 seconds after the abnormality occurred in cell # 1. In this case, the heat transfer sensitivity S b of the filling member 10 is 2.35 W / K.
The sensitivity ratio S d / S b was 0.574.

(実施例1−4)
充填部材10に熱伝導率kが0.4W/m・Kの材料を用い、膜厚は1mmとした。セル#1に異常が発生してから188秒後に、セル#2内部の最高温度が207.3℃に到達するものと推算された。この場合の充填部材10の熱移動感度Sは1.57W/Kであり、感度比S/Sは0.860であった。
(Example 1-4)
The thermal conductivity k b is a material of 0.4 W / m · K in the filling member 10, the film thickness was 1 mm. It was estimated that the maximum temperature inside cell # 2 reached 207.3 ° C. 188 seconds after the abnormality occurred in cell # 1. In this case, the heat transfer sensitivity S b of the filling member 10 was 1.57 W / K, and the sensitivity ratio S d / S b was 0.860.

(実施例1−5)
充填部材10に熱伝導率kが0.2W/m・Kの材料を用い、膜厚は1mmとした。セル#1に異常が発生してから179秒後に、セル#2内部の最高温度が208.1℃に到達するものと推算された。この場合の充填部材10の熱移動感度Sは0.784W/Kであり、感度比S/Sは1.72であった。
(Example 1-5)
The thermal conductivity k b is a material of 0.2 W / m · K in the filling member 10, the film thickness was 1 mm. It was estimated that the maximum temperature inside cell # 2 reached 208.1 ° C. 179 seconds after the abnormality occurred in cell # 1. In this case, the heat transfer sensitivity S b of the filling member 10 was 0.784 W / K, and the sensitivity ratio S d / S b was 1.72.

(比較例1−2)
充填部材10に熱伝導率kが0.1W/m・Kの材料を用い、膜厚は1mmとした。セル#1に異常が発生してから208秒後に、セル#2内部の最高温度が211.0℃に到達するものと推算された。この場合の充填部材10の熱移動感度Sは0.196W/Kであり、感度比S/Sは6.89であった。
(Comparative Example 1-2)
The thermal conductivity k b is a material of 0.1 W / m · K in the filling member 10, the film thickness was 1 mm. It was estimated that the maximum temperature inside cell # 2 would reach 211.0 ° C. 208 seconds after the abnormality occurred in cell # 1. In this case, the heat transfer sensitivity S b of the filling member 10 was 0.196 W / K, and the sensitivity ratio S d / S b was 6.89.

実施例1−1〜1−5並びに比較例1−1及び1−2の結果から、以下のことがわかる。組電池100を構成する単電池200と電池温度の冷却および均等化のために備えられた冷却部材400との間に設置される充填部材10について、仕切り部材1の熱移動感度Sが一定の場合、充填部材10の熱移動抵抗(熱伝導率k)を適切な範囲内に収めることで、異常が発生したセル#1(第1の単電池)から冷却部材400を介して伝わる熱量に起因するセル#2(第2の単電池)の昇温の程度を制御できる、すなわち、実施例1−1〜1−5並びに比較例1−1及び1−2によれば、冷却部材400を介した単電池200間の熱移動を好適に制御できる可能性があることが示された。 From the results of Examples 1-1 to 1-5 and Comparative Examples 1-1 and 1-2, the following can be seen. The heat transfer sensitivity S d of the partition member 1 is constant with respect to the filling member 10 installed between the cell 200 constituting the assembled battery 100 and the cooling member 400 provided for cooling and equalizing the battery temperature. when the heat transfer resistance of the filler member 10 (the thermal conductivity k b) by fall within an appropriate range, the amount of heat transferred through the cooling member 400 from the abnormality occurs cell # 1 (the first unit cell) The degree of temperature rise of cell # 2 (second cell) due to this can be controlled, that is, according to Examples 1-1 to 1-5 and Comparative Examples 1-1 and 1-2, the cooling member 400 is used. It was shown that there is a possibility that the heat transfer between the cells 200 via the cell 200 can be suitably controlled.

実施例1−1〜1−5では、セル#2の最高温度を210℃より低い値にすることができるのに対し、比較例1−1及び1−2では、210℃を超える最高温度となった。これらより、熱移動感度Sと熱移動感度Sとの関係が0.3≦(S/S)≦4.0を満たす範囲では、好適な熱伝達の制御がなされていることがわかった。 In Examples 1-1 to 1-5, the maximum temperature of cell # 2 can be set to a value lower than 210 ° C., whereas in Comparative Examples 1-1 and 1-2, the maximum temperature exceeds 210 ° C. became. From these, it can be seen that suitable heat transfer control is performed in the range where the relationship between the heat transfer sensitivity S d and the heat transfer sensitivity S b satisfies 0.3 ≦ (S d / S b) ≦ 4.0. all right.

表3は、実施例2−1〜2−6並びに比較例2−1及び2−2の結果を示す。

Figure 0006954214
Table 3 shows the results of Examples 2-1 to 2-6 and Comparative Examples 2-1 and 2-2.
Figure 0006954214

実施例2−1〜2−6並びに比較例2−1及び2−2では、仕切り部材1の膜厚(厚み方向の寸法)は1mmで固定とした。これに対し、面1cや面1dの平均温度の変化に応じて熱伝導率kが1.0W/(m・K)から0.1W/(m・K)へ低下する仕切り部材1を用いた。膜厚は一定であり、熱伝導率kが変化後の熱移動感度Sは一定の値(1.35W/K)であった。この熱移動感度Sは、0<S≦2の範囲に収まる。一方、充填部材10に関しては、熱伝導率kを変化させて測定を行った。各熱伝導率kに対する熱移動感度Sと感度比(S/S)とを求めた。 In Examples 2-1 to 2-6 and Comparative Examples 2-1 and 2-2, the film thickness (dimension in the thickness direction) of the partition member 1 was fixed at 1 mm. On the other hand, the partition member 1 whose thermal conductivity k d decreases from 1.0 W / (m · K) to 0.1 W / (m · K) according to the change in the average temperature of the surface 1c and the surface 1d is used. board. The film thickness was constant, and the heat transfer sensitivity S d after the change in thermal conductivity k d was a constant value (1.35 W / K). This heat transfer sensitivity S d falls within the range of 0 <S d ≦ 2. On the other hand, with respect to the filling member 10, the measurement was carried out by changing the thermal conductivity k b. The heat transfer sensitivity S b and the sensitivity ratio (S d / S b ) for each thermal conductivity k b were determined.

(比較例2−1)
充填部材10に熱伝導率kが2.0W/m・Kの材料を用い、膜厚は1mmとした。セル#1に異常が発生してから137秒後に、セル#2内部の最高温度が210.4℃に到達するものと推算された。この場合の充填部材10の熱移動感度Sは7.84W/Kであり、感度比S/Sは0.172であった。
(Comparative Example 2-1)
The thermal conductivity k b is a material of 2.0 W / m · K in the filling member 10, the film thickness was 1 mm. It was estimated that the maximum temperature inside cell # 2 reached 210.4 ° C. 137 seconds after the abnormality occurred in cell # 1. In this case, the heat transfer sensitivity S b of the filling member 10 was 7.84 W / K, and the sensitivity ratio S d / S b was 0.172.

(実施例2−1)
充填部材10に熱伝導率kが1.0W/m・Kの材料を用い、膜厚は1mmとした。セル#1に異常が発生してから160秒後に、セル#2内部の最高温度が204.1℃に到達するものと推算された。この場合の充填部材10の熱移動感度Sは3.92W/Kであり、感度比S/Sは0.344であった。
(Example 2-1)
The thermal conductivity k b is a material of 1.0 W / m · K in the filling member 10, the film thickness was 1 mm. It was estimated that the maximum temperature inside cell # 2 would reach 204.1 ° C. 160 seconds after the abnormality occurred in cell # 1. In this case, the heat transfer sensitivity S b of the filling member 10 was 3.92 W / K, and the sensitivity ratio S d / S b was 0.344.

(実施例2−2)
充填部材10に熱伝導率kが0.8W/m・Kの材料を用い、膜厚は1mmとした。セル#1に異常が発生してから168秒後に、セル#2内部の最高温度が202.5℃に到達するものと推算された。この場合の充填部材10の熱移動感度Sは3.13W/Kであり、感度比S/Sは0.431であった。
(Example 2-2)
The thermal conductivity k b is a material of 0.8 W / m · K in the filling member 10, the film thickness was 1 mm. It was estimated that the maximum temperature inside cell # 2 would reach 202.5 ° C. 168 seconds after the abnormality occurred in cell # 1. In this case, the heat transfer sensitivity S b of the filling member 10 was 3.13 W / K, and the sensitivity ratio S d / S b was 0.431.

(実施例2−3)
充填部材10に熱伝導率kが0.6W/m・Kの材料を用い、膜厚は1mmとした。
セル#1に異常が発生してから180秒後に、セル#2内部の最高温度が200.6℃に到達するものと推算された。この場合の充填部材10の熱移動感度Sは2.35W/Kであり、感度比S/Sは0.574であった。
(Example 2-3)
The thermal conductivity k b is a material of 0.6 W / m · K in the filling member 10, the film thickness was 1 mm.
It was estimated that the maximum temperature inside cell # 2 would reach 200.6 ° C. 180 seconds after the abnormality occurred in cell # 1. In this case, the heat transfer sensitivity S b of the filling member 10 was 2.35 W / K, and the sensitivity ratio S d / S b was 0.574.

(実施例2−4)
充填部材10に熱伝導率kが0.4W/m・Kの材料を用い、膜厚は1mmとした。セル#1に異常が発生してから162秒後に、セル#2内部の最高温度が199.6℃に到達するものと推算された。この場合の充填部材10の熱移動感度Sは1.57W/Kであり、感度比S/Sは0.860であった。
(Example 2-4)
The thermal conductivity k b is a material of 0.4 W / m · K in the filling member 10, the film thickness was 1 mm. It was estimated that the maximum temperature inside cell # 2 reached 199.6 ° C. 162 seconds after the abnormality occurred in cell # 1. In this case, the heat transfer sensitivity S b of the filling member 10 was 1.57 W / K, and the sensitivity ratio S d / S b was 0.860.

(実施例2−5)
充填部材10に熱伝導率kが0.2W/m・Kの材料を用い、膜厚は1mmとした。セル#1に異常が発生してから169秒後に、セル#2内部の最高温度が200.1℃に到達するものと推算された。この場合の充填部材10の熱移動感度Sは0.784W/Kであり、感度比S/Sは1.72であった。
(Example 2-5)
The thermal conductivity k b is a material of 0.2 W / m · K in the filling member 10, the film thickness was 1 mm. It was estimated that the maximum temperature inside cell # 2 reached 200.1 ° C. 169 seconds after the abnormality occurred in cell # 1. In this case, the heat transfer sensitivity S b of the filling member 10 was 0.784 W / K, and the sensitivity ratio S d / S b was 1.72.

(実施例2−6)
充填部材10に熱伝導率kが0.1W/m・Kの材料を用い、膜厚は1mmとした。セル#1に異常が発生してから172秒後に、セル#2内部の最高温度が202.1℃に到達するものと推算された。この場合の充填部材10の熱移動感度Sは0.392W/Kであり、感度比S/Sは3.44であった。
(Example 2-6)
The thermal conductivity k b is a material of 0.1 W / m · K in the filling member 10, the film thickness was 1 mm. It was estimated that the maximum temperature inside cell # 2 reached 202.1 ° C. 172 seconds after the abnormality occurred in cell # 1. In this case, the heat transfer sensitivity S b of the filling member 10 was 0.392 W / K, and the sensitivity ratio S d / S b was 3.44.

(比較例2−2)
充填部材10に熱伝導率kが0.02W/m・Kの材料を用い、膜厚は1mmとした。セル#1に異常が発生してから186秒後に、セル#2内部の最高温度が207.4℃に到達するものと推算された。この場合の充填部材10の熱移動感度Sは0.078W/Kであり、感度比S/Sは17.3であった。
(Comparative Example 2-2)
The thermal conductivity k b is a material of 0.02 W / m · K in the filling member 10, the film thickness was 1 mm. It was estimated that the maximum temperature inside cell # 2 reached 207.4 ° C. 186 seconds after the abnormality occurred in cell # 1. In this case, the heat transfer sensitivity S b of the filling member 10 was 0.078 W / K, and the sensitivity ratio S d / S b was 17.3.

実施例2−1〜2−6並びに比較例2−1及び2−2の結果から、以下のことがわかる。充填部材10について、仕切り部材1の熱伝導率k低下後の熱移動感度Sが一定の場合、充填部材10の熱移動抵抗(熱伝導率k)を適切な範囲内に収めることで、異常が発生したセル#1(第1の単電池)から冷却部材400を介して伝わる熱量に起因するセル#2(第2の単電池)の昇温の程度を制御できる、すなわち、実施例2−1〜2−6並びに比較例2−1及び2−2によれば、冷却部材400を介した単電池200間の熱移動を好適に制御できる可能性があることが示された。 From the results of Examples 2-1 to 2-6 and Comparative Examples 2-1 and 2-2, the following can be seen. With respect to the filling member 10, when the heat transfer sensitivity S d after the decrease in the heat conductivity k d of the partition member 1 is constant, the heat transfer resistance (heat conductivity k b ) of the filling member 10 is kept within an appropriate range. , The degree of temperature rise of cell # 2 (second cell) due to the amount of heat transferred from cell # 1 (first cell) in which the abnormality has occurred via the cooling member 400 can be controlled, that is, in the embodiment. According to 2-1 to 2-6 and Comparative Examples 2-1 and 2-2, it was shown that the heat transfer between the cell 200 via the cooling member 400 may be suitably controlled.

実施例2−1〜2−6では、セル#2の最高温度を204.1℃以下にすることができるのに対し、比較例2−1及び2−2では、207.4℃以上の最高温度となった。実施例2−1〜2−6の結果より、仕切り部材1が表面温度に応じて熱伝導率kを変化(低下)させる機構(スイッチング機能)を有している場合においても、熱移動感度Sと熱移動感度Sとの関係が0.3≦(S/S)≦4.0を満たす範囲では、好適な熱伝達の制御がなされていることがわかった。 In Examples 2-1 to 2-6, the maximum temperature of cell # 2 can be set to 204.1 ° C or lower , whereas in Comparative Examples 2-1 and 2-2, the maximum temperature is 207.4 ° C or higher. It became the temperature. From the results of Examples 2-1 to 2-6, even when the partition member 1 has a mechanism (switching function) for changing (decreasing) the thermal conductivity dd according to the surface temperature, the heat transfer sensitivity It was found that suitable heat transfer control was performed in the range where the relationship between S d and the heat transfer sensitivity S b satisfied 0.3 ≦ (S d / S b) ≦ 4.0.

ここで、実施例1〜5並びに比較例1及び2では、充填部材10の厚み(膜厚)を1mmに固定したが、充填部材10の厚みは、5.0×10−5m以上5.0×10−3m以下であってもよい。このため、実施例1〜5並びに比較例1及び2の結果から、充填部材10の厚み方向における熱伝導率kが2.0×10−2W/m・K以上10.0W/m・K以下であることが好ましいことがわかった。また、セル#1及びセル#2が異常発熱状態の温度に昇温していない場合における熱移動感度Sの値は2より大きいことが好ましい。 Here, in Examples 1 to 5 and Comparative Examples 1 and 2, the thickness (film thickness) of the filling member 10 was fixed to 1 mm, but the thickness of the filling member 10 was 5.0 × 10-5 m or more. It may be 0 × 10 -3 m or less. Therefore, from the results of Examples 1 to 5 and Comparative Examples 1 and 2, the thermal conductivity k b is 2.0 × 10 -2 W / m · K or more in the thickness direction of the filling member 10 10.0 W / m · It was found that it is preferably K or less. Further, it is preferable that the value of the heat transfer sensitivity S d is larger than 2 when the temperature of the cells # 1 and the cell # 2 is not raised to the temperature in the abnormal heat generation state.

1 仕切り部材
10 充填部材
10a、10b 面
100 組電池
110 内包体
120 外装体
200 単電池
300 筐体
400 冷却部材
1 Partition member 10 Filling member 10a, 10b Surface 100 Assembly battery 110 Inner body 120 Exterior body 200 Single battery 300 Housing 400 Cooling member

Claims (10)

第1の単電池と、第2の単電池と、前記第1の単電池と前記第2の単電池との間を仕切る仕切り部材とともに組電池を構成する充填部材であって、
前記充填部材は、厚み方向と前記厚み方向に直交する面方向とを有し、前記面方向に沿った第1の面と第2の面とを有し、前記第1の単電池及び前記第2の単電池と前記第1の面において接触するとともに、前記第2の面において前記第1及び第2の単電池を冷却可能な冷却部材と接触し、
前記第1の単電池から発せられる熱が前記仕切り部材を介して前記第2の単電池へ移動する場合の前記仕切り部材の熱移動感度Sが以下の式1により定義され、
前記仕切り部材の熱移動感度S[W/K]=
前記仕切り部材の熱伝導率k[W/m・K]×前記仕切り部材と前記第1の単電池との接触面積A[m]/前記仕切り部材の厚みd[m]・・・(式1)
前記第1の単電池から発せられる熱が前記充填部材及び前記冷却部材を介して前記第2の単電池へ移動する場合の前記充填部材の熱移動感度Sbが以下の式2により定義され、
前記充填部材の熱移動感度S[W/K]=
前記充填部材の熱伝導率k[W/m・K]×前記充填部材と前記第1及び第2の単電池との接触面積A[m]/前記充填部材の厚みd[m]・・・(式2)
前記第1の単電池の温度が異常発熱状態の温度以上となった場合において、前記仕切り部材の熱移動感度Sが以下の式3を満たし、
0< S ≦ 2 ・・・(式3)
前記熱移動感度Sと前記充填部材の熱移動感度Sbとの関係が以下の式4を満たす
0.3 ≦(S/S)≦ 4.0 ・・・(式4)
ことを特徴とする充填部材。
A filling member that constitutes an assembled battery together with a partition member that partitions the first cell, the second cell, the first cell, and the second cell.
The filling member has a thickness direction and a surface direction orthogonal to the thickness direction, has a first surface and a second surface along the surface direction, and has the first cell and the first unit. The second cell is in contact with the first surface, and the first and second cells are in contact with a cooling member capable of cooling the first and second cells on the second surface.
The heat transfer sensitivity S d of the partition member when the heat generated from the first cell is transferred to the second cell via the partition member is defined by the following equation 1.
Heat transfer sensitivity of the partition member S d [W / K] =
Thermal conductivity of the partition member k d [W / m · K] × Contact area between the partition member and the first cell cell Ad [m 2 ] / Thickness of the partition member d d [m] ...・ (Equation 1)
The heat transfer sensitivity Sb of the filling member when the heat generated from the first cell is transferred to the second cell via the filling member and the cooling member is defined by the following equation 2.
Heat transfer sensitivity of the filling member S b [W / K] =
Thermal conductivity of the filling member k b [W / m · K] × Contact area between the filling member and the first and second cells A b [m 2 ] / Thickness of the filling member d b [m ] ... (Equation 2)
When the temperature of the first cell becomes equal to or higher than the temperature in the abnormal heat generation state, the heat transfer sensitivity S d of the partition member satisfies the following equation 3.
0 <S d ≤ 2 ... (Equation 3)
The relationship between the heat transfer sensitivity S d and the heat transfer sensitivity Sb of the filling member satisfies the following equation 4 0.3 ≤ (S d / S b ) ≤ 4.0 ... (Equation 4)
A filling member characterized by that.
前記充填部材の厚み方向の熱伝導率が2.0×10−2W/m・K以上10.0W/m・K以下である、請求項1に記載の充填部材。 The thickness direction of the thermal conductivity of the filling member is 2.0 × 10 -2 W / m · K or more 10.0 W / m · K or less, the filling member of claim 1. 前記充填部材の厚みが5.0×10−5m以上5.0×10−3m以下である、
請求項1又は2に記載の充填部材。
The thickness of the filling member is 5.0 × 10 -5 m or more and 5.0 × 10 -3 m or less.
The filling member according to claim 1 or 2.
請求項1に記載の仕切り部材であって、前記第1の単電池及び前記第2の単電池が異常発熱状態の温度に昇温していない場合において、前記熱移動感度Sの値が2より大きい、仕切り部材。 In the partition member according to claim 1, when the first cell and the second cell have not been heated to a temperature in an abnormal heat generation state, the value of the heat transfer sensitivity S d is 2. Larger, divider. 請求項1に記載の仕切り部材であって、厚み方向と前記厚み方向に直交する面方向とを有し、前記仕切り部材の厚み方向の二面のうち一方の平均温度が180℃を超える場合において、前記厚み方向の熱伝導率が2.0×10−2W/m・K以上2.0W/m・K以下である、仕切り部材。 The partition member according to claim 1, which has a thickness direction and a surface direction orthogonal to the thickness direction, and the average temperature of one of the two surfaces of the partition member in the thickness direction exceeds 180 ° C. , The partition member having a thermal conductivity in the thickness direction of 2.0 × 10 -2 W / m · K or more and 2.0 W / m · K or less. 前記仕切り部材の厚み方向の二面のうち双方の平均温度が80℃を超えない場合において、前記厚み方向の熱伝導率が5.0×10−2W/m・K以上50W/m・K以下である、
請求項4又は5に記載の仕切り部材。
When the average temperature of both of the two surfaces of the partition member in the thickness direction does not exceed 80 ° C., the thermal conductivity in the thickness direction is 5.0 × 10-2 W / m · K or more and 50 W / m · K. Is below,
The partition member according to claim 4 or 5.
前記第1及び第2の単電池の厚みがLmmである場合に、厚みがL/50mm以上L/10mm以下である、請求項4から6のいずれか1項に記載の仕切り部材。 The partition member according to any one of claims 4 to 6, wherein when the thickness of the first and second cells is L mm, the thickness is L / 50 mm or more and L / 10 mm or less. 請求項1から3のいずれか1項に記載の充填部材を含む組電池。 An assembled battery including the filling member according to any one of claims 1 to 3. 請求項4から7のいずれか1項に記載の仕切り部材を含む組電池。 An assembled battery including the partition member according to any one of claims 4 to 7. 前記熱移動感度Sが式3を満たすとともに、前記熱移動感度Sと前記熱移動感度Sとの関係が式4を満たす、請求項1に記載の前記仕切り部材及び前記充填部材を用いて、前記第1の単電池から前記仕切り部材、前記充填部材及び前記冷却部材を介して前記第2の単電池に伝わる熱量を制御する、熱伝達の制御方法。 The heat transfer sensitivity S d is fulfills Equation 3, the relationship between the heat transfer sensitivity S b and the heat transfer sensitivity S d satisfies the equation 4, using the partition member and the filling member of claim 1 A method for controlling heat transfer, which controls the amount of heat transferred from the first cell cell to the second cell cell via the partition member, the filling member, and the cooling member.
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