JP2012230916A - Method for manufacturing collector - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide a method for manufacturing a collector capable of simplifying the manufacturing process and structure of a battery and reducing the weight by eliminating the need for an insulating member.SOLUTION: The method for manufacturing a collector comprises the steps of: preparing a collector composed of a high polymer material containing conductive particles randomly, and compressing the collector in the thickness direction by hot pressing.

Description

  The present invention relates to a method for manufacturing a current collector.

  In recent years, bipolar batteries having a small size and high energy density are known as power sources for vehicles and the like. The bipolar battery is formed by alternately laminating a bipolar electrode in which a positive electrode active material layer is formed on one surface of a current collector and a negative electrode active material layer on the opposite surface, and an electrolyte layer. In such a bipolar battery, if the current collectors are electrically connected to each other, they are short-circuited, and therefore an insulating member is inserted between the current collectors (see, for example, Patent Document 1).

JP-A-2005-310402

  However, in the bipolar battery as described above, the man-hour is increased by the amount necessary to insert the insulating member, and the structure of the battery becomes complicated. Furthermore, the weight is increased by the amount of insertion of the insulating member.

  The present invention has been made in view of the above circumstances, and it is an object of the present invention to provide a method for manufacturing a current collector that omits an insulating member, can simplify the battery manufacturing process and structure, and can further reduce the weight. To do.

  The method for producing a current collector includes a step of preparing a current collector in which conductive particles are randomly included in a polymer material, and a step of heat-pressing the current collector and compressing the current collector in the thickness direction.

  According to the current collector of the present invention, when applied to a bipolar battery, the conductivity in the thickness direction is higher than the conductivity in the plane direction, and a current flows only in the substantially thickness direction. That is, current does not flow or hardly flows in the surface direction. Therefore, even if the current collectors are in contact with each other at the end portion that is not in contact with the single battery layer composed of the positive electrode active material layer, the electrolyte layer, and the negative electrode active material layer, no current flows through the end portion, and thus a short circuit occurs. Does not occur. Therefore, it is not necessary to arrange an insulating member to prevent contact between the ends of the current collector. As a result, the assembly process of the bipolar battery can be simplified, and the finished structure can be simplified. The weight of the bipolar battery can be reduced by the amount of the insulating member.

It is a perspective view of a bipolar battery. FIG. 2 is a cross-sectional view taken along line 2-2 in FIG. It is a figure which shows the flow of the electric current in a collector. It is a line graph which shows the relationship between the addition amount of electroconductive particle, and the resistance value of the surface direction or thickness direction of a collector. It is a figure which shows the relationship between the addition amount of electroconductive particle, and the resistance value of the surface direction or thickness direction of a collector. It is a figure which shows the modification of a bipolar battery. It is a three-plane figure which shows an assembled battery. It is the schematic of the motor vehicle carrying an assembled battery. It is a figure which shows the voltage of 1 month after charging each bipolar battery. It is a figure which shows the ratio of the internal resistance of each other bipolar battery by making the internal resistance of the bipolar battery of Example 1 into 100%.

  Hereinafter, embodiments of the present invention will be described with reference to the accompanying drawings. In the description of the drawings, the same elements are denoted by the same reference numerals, and redundant description is omitted. In addition, the dimensional ratios in the drawings are exaggerated for convenience of explanation, and may be different from the actual ratios.

  Embodiments of the present invention will be described below with reference to the drawings.

(First embodiment)
FIG. 1 is a perspective view of a bipolar battery, and FIG. 2 is a cross-sectional view taken along line 2-2 of FIG.

  As shown in FIGS. 1 and 2, the bipolar battery 10 has a positive electrode tab 30a and a negative electrode tab 30b drawn out from a flat main body.

  As shown in FIG. 2, the bipolar battery 10 has a positive electrode active material layer 12 and a negative electrode active material layer 13 formed at the center of both surfaces of a current collector 11 other than both ends. A single battery layer 15 is formed by sandwiching an electrolyte layer 14 between the layer 12 and the negative electrode active material layer 13, and a plurality of single battery layers 15 are stacked in the same order. A material in which the positive electrode active material layer 12 is formed on one surface of the current collector 11 and the negative electrode active material layer 13 is formed on the other surface is referred to as a bipolar electrode 16. A current collector (referred to as an end current collector 17) at both ends is connected to the electrode 30a or the electrode 30b of the entire bipolar battery 10.

  A structure in which the positive electrode active material layer 12 and the negative electrode active material layer 13 are provided with the current collector 11 interposed therebetween is called a bipolar electrode.

The electrolyte layer 14 is not particularly limited as long as it is a polymer having ion conductivity. In the present embodiment, an all solid electrolyte is used for the electrolyte layer 14. The electrolyte layer 14 has a resistance value of 1 × 10 in a thickness direction and a plane direction in a non-contact range (see a range A indicated by a double arrow in FIG. 2) that is not in contact with the positive electrode active material layer 12 or the negative electrode active material layer 13. ⁷ Ω or more. With such a resistance value, insulation is ensured as the structure of the end portion of the bipolar battery. In the range A, a member different from the all solid electrolyte may be disposed.

  The electrolyte layers 14 and the bipolar electrodes 16 are alternately stacked to form the battery element 20.

  The battery element 20 is connected to electrode tabs 30a and 30b for drawing current. The electrode tab 30a is connected to the positive electrode side of the battery element 20, and the electrode tab 30b is connected to the negative electrode side. The electrode tabs 30a and 30b are pulled out from the exterior 40 as shown in FIG. The electrode tabs 30a and 30b are respectively connected to the end current collector 17 so as to cover the entire projection surface of the positive electrode active material layer 12 or the negative electrode active material layer 13 via the end current collector 17 of the battery element 20. Is attached.

  The exterior 40 is formed by two laminate sheets 41. The laminate sheet 41 has a three-layer structure in which both surfaces of an aluminum layer are covered with a resin layer. At least one of the laminate sheets 41 is processed into a medium-high shape in order to provide a space that encloses the battery element 20. The edge of the laminate sheet 41 is bonded by heat fusion or the like. Thereby, the battery element 20 is sealed inside the exterior 40.

  The configuration of the bipolar battery of the present invention is not particularly limited as long as a known material used for a general lithium ion secondary battery is used, except for those specifically described.

  The bipolar battery 10 of the present embodiment is particularly characterized by the current collector 11 in the above configuration. The current collector 11 will be described in detail.

(Current collector)
(Material of current collector)
In the present embodiment, an anisotropic conductive material is used for the current collector 11. The current collector 11 is formed such that the electrical conductivity in the thickness direction is higher than the electrical conductivity in the plane direction so that current flows only in the substantially thickness direction. That is, the current collector 11 does not or hardly flows current in the surface direction. The material constituting the current collector 11 is as follows.

  The current collector 11 is composed of a non-conductive polymer material and conductive conductive particles (also referred to as a conductive filler).

  The polymeric material may be, for example, a polyolefin such as polypropylene or polyethylene, a polyester such as polyethylene terephthalate (PET) or polyethylene naphthalate (PEN), polyimide, polyamide, polyvinylidene fluoride (PVdF), an epoxy resin, and a synthetic rubber material, or That mixture.

  The conductive particles are selected from conductive materials. The conductive particles are selected from materials that can withstand the applied positive electrode potential and negative electrode potential. Specific examples include aluminum particles, SUS particles, carbon particles, silver particles, gold particles, copper particles, and titanium particles, but are not limited thereto. Alloy particles may be used. The conductive particles are not limited to the above-described form, and carbon nanotubes or the like can also be used, and those that are put into practical use as so-called filler-based conductive resin compositions can be used.

  The distribution of the conductive particles in the current collector may not be uniform, and the particle distribution may vary within the current collector. A plurality of conductive particles may be used, and the distribution of the conductive particles may be changed inside the current collector. For example, preferable conductive particles may be selectively used in a portion in contact with the positive electrode and a portion in contact with the negative electrode. As the conductive particles used on the positive electrode side, aluminum particles, SUS particles, and carbon particles are preferable, and carbon particles are particularly preferable. As the conductive particles used for the negative electrode, silver particles, gold particles, copper particles, titanium particles, SUS particles, and carbon particles are preferable, and carbon particles are particularly preferable. Carbon particles such as carbon black and graphite have a very wide potential window, are stable in a wide range with respect to both the positive electrode potential and the negative electrode potential, and are excellent in conductivity. Also, since the carbon particles are very light, the increase in mass is minimized. Furthermore, since carbon particles are often used as a conductive aid for electrodes, even if they come into contact with these conductive aids, the contact resistance is very low because of the same material.

(Creation procedure of current collector)
FIG. 3 is a diagram showing the flow of current in the current collector.

  The current collector 11 is formed through the following steps in order to realize anisotropy. The polymer material randomly mixed with conductive particles is compressed in the thickness direction by thermocompression processing. The distribution of the polymer material in the thickness direction becomes dense by the amount compressed in the thickness direction, while the distribution of the conductive particles in the plane direction does not change. Therefore, the conductive particles are connected in the thickness direction, but are not connected in the surface direction. As a result, as indicated by arrows in FIG. 3, the current collector 11 passes a current in the thickness direction and does not flow a current in the surface direction. For the current collector 11, an anisotropic conductive film (manufactured by Hitachi Chemical Co., Ltd.), an anisotropic conductive film (manufactured by Fujikura Co., Ltd.) or the like formed in advance by the above-described steps can be used.

  The current collector 11 is compressed in advance, and may be further pressurized together with the positive electrode active material layer 12 and the negative electrode active material layer 13 when the bipolar electrode 15 is formed. Alternatively, a pressure sensitive film that realizes anisotropy by pressurization may be used as the current collector 11. In this case, the current collector 11 is not pressurized until the bipolar electrode 15 is produced, and anisotropy is manifested only after that.

(Resistance value of current collector)
Next, the resistance value of the current collector 11 can be defined from various aspects.

  FIG. 4 is a polygonal diagram showing the relationship between the amount of conductive particles added and the resistance value in the surface direction or thickness direction of the current collector, and FIG. It is a figure which shows the relationship with resistance value.

(Definition 1)
Definition 1: The amount of conductive particles added is determined so that an anisotropy can be realized in the current collector 11 in which a current flows in the thickness direction and a current does not flow (almost does not flow) in the plane direction. It is preferable to add conductive particles so that the volume resistance value in the surface direction is 1000 times or more the volume resistance value in the thickness direction.

  The resistance value of the current collector 11 can be divided into a resistance value in the thickness direction and a resistance value in the surface direction. The resistance values in the thickness direction and the surface direction vary depending on the proportion of conductive particles mixed in the current collector 11.

  The amount of conductive particles that satisfy Definition 1 can be determined experimentally. While changing the volume% of the conductive particles mixed in the current collector 11, the resistance values in the surface direction and the thickness direction of the current collector 11 formed by pressing in the thickness direction are measured. Then, the results as shown in FIGS. 4 and 5 were obtained. In FIG. 4, the horizontal axis represents the amount of conductive particles added (volume%), and the vertical axis represents the volume resistance value (Ω · cm).

When the addition amount of the conductive particles was 1 to 5% by volume, the volume resistance values in the plane direction and the thickness direction were both about 1 × 10 ¹⁰ Ω · cm and very high. This is because the conductive particles in the thickness direction are not connected to each other and the insulation in the thickness direction is maintained even if the conductive particles in the thickness direction are compressed in the thickness direction even when the conductive particles are mixed in the thickness direction.

When the addition amount of the conductive particles was larger than 5% by volume, the resistance value in the thickness direction was 2.00 × 10 ⁻² Ω · cm when the amount was 6% by volume. On the other hand, when the addition amount of the conductive particles was 6% by volume, the resistance value in the plane direction was as extremely high as 1.00 × 10 ¹⁰ Ω · cm, which was 10 ¹² times or more higher than the resistance value in the thickness direction. The resistance in the thickness direction of the current collector 11 was very small and the resistance in the plane direction was very high until the amount of conductive particles added was about 10% by volume. That is, the current collector 11 has anisotropy that allows current to flow only in the thickness direction.

Furthermore, when the addition amount of the conductive particles was larger than 10% by volume, the resistance value in the plane direction was 1.00 × 10 ⁴ Ω · cm, and suddenly decreased at 11% by volume. Therefore, the current easily flows in the plane direction, and the anisotropy of the current collector 11 in which the current flows only in the thickness direction is weakened.

  Based on the above experimental results, in order to exhibit the anisotropy that the current flows through the current collector 11 only in the thickness direction, it is sufficient to add conductive particles in the range indicated by the double-headed arrow in FIG. However, it should be noted that the optimum addition amount of the conductive particles also changes depending on the compressibility in the thickness direction when the current collector 11 is formed.

(Definition 2)
Definition 2: The total resistance value in the thickness direction of all current collectors 11 is 1/100 or less of the total internal resistance of all single battery layers 15 in bipolar battery 10.

  The total of the resistance values in the thickness direction of all the current collectors 11 can be adjusted so that the definition 2 is satisfied by adjusting the inside of the polymer material constituting each current collector 11 and the absolute amount of the conductive particles. The resistance value of the bipolar battery can be measured when discharging. In this case, discharge is performed at about 1 C from a charge amount of about 50% of depth of discharge (DOD), and the resistance of the battery is obtained from the voltage drop after about 5 seconds.

(Definition 3)
Definition 3: The volume resistivity in the thickness direction of the current collector 11 is 10 ⁻⁴ Ω · cm to 10 ³ Ω · cm.

  If the volume resistivity is within the range of definition 3, it can be used as a current collector for a bipolar battery without any problem.

(effect)
The effect of the bipolar battery 10 of the present embodiment will be described.

  As described above, in the bipolar battery 10 of the present embodiment, the current collector 11 has anisotropy in which a current flows only in the thickness direction. In the bipolar battery, most of the current flows only in the thickness direction of the current collector 11. That is, current does not flow or hardly flows in the surface direction of the current collector 11. Therefore, even if the current collector 11 is in contact with another current collector 11 at an end where the current collector 11 is not in contact with the single battery layer 15, no current flows through the end and no short circuit occurs. Therefore, it is not necessary to arrange an insulating member that has been conventionally arranged in order to prevent contact between the ends of the current collector 11. As a result, the assembly process of the bipolar battery can be simplified, and the finished structure can be simplified. The weight of the bipolar battery can be reduced by the amount of the insulating member.

  Moreover, the addition amount of electroconductive particle is determined so that the volume resistance value of a surface direction may be 1000 times or more of the volume resistance value of a thickness direction. Therefore, it is possible to prevent a current from flowing to the end of the current collector 11 and to prevent self-discharge.

  The total resistance value in the thickness direction of all the current collectors 11 is 1/100 or less of the internal resistance of the bipolar battery 10. Therefore, the resistance in the thickness direction of the current collector 11 does not hinder the high output of the bipolar battery 10. The resistance value in the thickness direction of all current collectors 11 is preferably as low as possible. However, the total resistance value in the thickness direction of all current collectors 11 is determined from the physical properties of current collector 11 including an insulating polymer material. The limit is 1 / 100,000,000 for the internal resistance.

The volume resistivity in the thickness direction of the current collector 11 is 10 ⁻⁴ Ω · cm to 10 ³ Ω · cm. If it is this range, it can be used as a collector of the bipolar battery 10.

  The current collector 11 is formed by mixing a polymer material and conductive particles. Since the polymer material is more flexible than the metal foil, the degree of freedom in design is high, and the polymer material can be easily designed to withstand the positive and negative electrode potentials electrochemically, and the retention of the electrode can be improved.

  Examples of the polymer material constituting the current collector 11 include a polyolefin such as polypropylene or polyethylene, a polyester such as polyethylene terephthalate (PET) or polyethylene naphthalate (PEN), polyimide, polyamide, and polyvinylidene fluoride ( PVdF), epoxy resins, and synthetic rubber materials, or mixtures thereof. If these materials are used, the potential window is very wide, and both the positive electrode potential and the negative electrode potential are stable. Furthermore, since these materials are lightweight, the weight of the battery can be reduced.

  The current collector 11 that develops anisotropy by pressurization is heated and pressed together with the positive electrode active material layer 12 and the negative electrode active material layer 13 to be compressed in the thickness direction to constitute the bipolar electrode 16. Since the density in the thickness direction of the conductive particles is further increased by the compression, the current collector 11 can exhibit more anisotropy through which current flows only in the thickness direction. When the current collector 11 is pressed together with the positive electrode active material layer 12 and the negative electrode active material layer 13, the end portions of the current collector 11 that are not in contact with the positive electrode active material layer 12 and the negative electrode active material layer 13 are not compressed. . Therefore, the volume resistivity at the end of the current collector 11 can be made higher than the portion where the positive electrode active material layer 12 and the negative electrode active material layer 13 are applied. Since the resistance of the end portions of the current collector 11 is high, a short circuit due to contact between the end portions of the current collector 11 can be more reliably prevented.

  The electrode tabs 30a and 30b are respectively connected to the end current collector 17 so as to cover the entire projection surface of the positive electrode active material layer 12 or the negative electrode active material layer 13 via the end current collector 17 of the battery element 20. Is attached. Therefore, it is possible to reduce the resistance of the part that draws current from the battery element 20 to the electrode tabs 30a and 30b.

  The electrolyte layer 14 is formed of an all solid electrolyte. Therefore, since there is no fluidity of the electrolyte, there is no need for a seal structure for preventing the electrolyte from flowing out, and the configuration of the bipolar battery can be simplified.

(Modification)
Next, a modification of the above embodiment will be described.

  In the above embodiment, the electrolyte layer 14 is formed of an all solid electrolyte. However, the electrolyte layer 14 can also be formed by holding a gel electrolyte in a separator. Here, the separator is, for example, a polymer skeleton formed of a resin selected from the group consisting of a polyester resin, an aramid resin, and a polyolefin resin, either alone or in combination. In this case, since the gel electrolyte has some fluidity, it is necessary to change the configuration of the bipolar battery 10.

  FIG. 6 is a diagram showing a modification of the bipolar battery.

  In the modification shown in FIG. 6, the current collectors 11 and 17 are fused and integrated at the ends. By sealing the ends of the current collectors 11 and 17, the single battery layers 15 are sealed. Therefore, the gel electrolyte of the gel electrolyte layer 14 ′ is sealed and does not come into contact with the gel electrolytes of the other single battery layers 15. Thus, since each single battery layer 15 can be sealed, the gel electrolyte layer 14 ′ can also be applied to a bipolar battery.

  Further, since the current collector 11 does not have conductivity in the surface direction as described above, even if the current collectors 11 and 17 are connected to each other at the end portions, no current flows at the end portions. Since there is no short circuit, there is no need to provide an insulating member against the short circuit.

(Second Embodiment)
In the second embodiment, a plurality of bipolar batteries of the first embodiment are connected in parallel and / or in series to constitute an assembled battery.

  FIG. 7 is a three-side view showing the assembled battery.

  As shown in FIG. 7, the assembled battery 70 includes, for example, a positive terminal 72 and a negative terminal 73 of a plurality of battery modules 71 connected by bus bars 74. That is, the battery modules 71 are connected in parallel to each other.

  In the case of the battery module 71, although not shown, a plurality of the bipolar batteries 10 described above are accommodated in a stacked state and connected in series. As a method of connecting a plurality of bipolar batteries 70, ultrasonic welding, thermal welding, laser welding, rivets, caulking, electron beam, or the like can be used. By adopting such a connection method, it is possible to manufacture the assembled battery 70 having long-term reliability.

  According to the assembled battery 70, by using the bipolar battery 10 according to the first embodiment described above to form an assembled battery, high capacity and high output can be obtained, and the reliability of each battery is high. Long-term reliability as an assembled battery can be improved.

  In addition, the connection of the bipolar battery 10 as an assembled battery may be all connected in parallel, all the bipolar batteries 10 may be connected in series, and further, the series connection and the parallel connection May be combined.

(Third embodiment)
In the third embodiment, the bipolar battery 10 of the first embodiment or the assembled battery 70 of the second embodiment is mounted as a driving power source to constitute a vehicle. As a vehicle using the bipolar battery 10 or the assembled battery 70 as a motor power source, there is an automobile whose wheels are driven by a motor, such as an electric vehicle and a hybrid vehicle.

  For reference, FIG. 8 shows a schematic diagram of an automobile 80 on which the assembled battery 70 is mounted. The assembled battery 70 mounted on the automobile has the characteristics described above. For this reason, an automobile equipped with the assembled battery 70 has high durability and can provide sufficient output even after being used for a long period of time.

(Example)
The effects of the present invention will be described using the following examples and comparative examples. However, the technical scope of the present invention is not limited only to the following examples.

Example 1
1. Preparation of current collector 20 μm in thickness including carbon fine particles (average particle size 0.8 μm; estimated for 70% by volume ready-made) and polypropylene (30% by volume estimated for ready-made) as polymer material A current collector was prepared. The volume resistivity in the thickness direction was 1 × 10 ⁻² Ω · cm, and the volume resistivity in the plane direction was 1 × 10 ⁸ Ω · cm.

2. Preparation of positive electrode active material layer LiMn ₂ O ₄ (85 wt%) as a positive electrode active material, acetylene black (5 wt%) as a conductive additive, polyvinylidene fluoride (PVDF; 10 wt%) as a binder, N-methyl as a slurry viscosity adjusting solvent Pyrrolidone (NMP; trace amount) was mixed to prepare a positive electrode slurry.

  A positive electrode slurry was applied to one side of the current collector, heated at 100 ° C. and dried to obtain a positive electrode.

3. Preparation of negative electrode active material layer Li ₄ Ti ₅ O ₁₂ (85 wt%) as a negative electrode active material, acetylene black (5 wt%) as a conductive auxiliary agent, PEO (10 wt%) as an ion conductive polymer, NMP as a slurry viscosity adjusting solvent (A trace amount) was mixed to prepare a negative electrode slurry.

  A negative electrode slurry was applied to the opposite surface of the current collector on which the positive electrode was formed on one side, heated at 100 ° C. and dried to obtain a negative electrode.

Then, 1M LiPF ₆ as a lithium salt was dissolved in a solvent of propylene carbonate (PC): ethylene carbonate (EC) = 1: 1 (mass ratio) as an electrolytic solution (90 wt%), and 10 HFP copolymers were used as a postpolymer. % Of PVdF-HFP (10 wt%) and dimethyl carbonate (DMC) as a viscosity adjusting solvent are mixed to prepare a gel electrolyte. The gel electrolyte is soaked by coating on the positive and negative electrode surfaces and further drying the DMC. Let

  According to procedures 2 and 3, a positive electrode active material layer and a negative electrode active material layer were formed on both sides of the current collector to complete a bipolar electrode. The resulting bipolar electrode was cut into 140 × 90 mm, and a positive electrode active material layer and a negative electrode active material layer were not applied to 10 mm around the electrode. As a result, the positive electrode active material layer and the negative electrode active material layer were applied in a central range of 120 × 70 mm, and an uncoated portion was formed in a range of 10 mm from the outer periphery to the inner side to produce a bipolar electrode.

4). Preparation of Gel Electrolyte Layer 1M LiPF ₆ as a lithium salt dissolved in a solvent of propylene carbonate (PC): ethylene carbonate (EC) = 1: 1 (mass ratio) as an electrolytic solution (90 wt%), HFP as a postpolymer A gel electrolyte was prepared by mixing PVdF-HFP (10 wt%) containing 10% of copolymer and dimethyl carbonate (DMC) as a viscosity adjusting solvent.

  The gel electrolyte material was applied on both sides of a polypropylene porous film separator 20 μm, and the DMC was dried to obtain a gel electrolyte layer. This gel electrolyte layer was cut into 130 × 80 mm to complete the gel electrolyte layer.

5. Production of Bipolar Battery Bipolar electrodes were laminated for five layers with the gel electrolyte layer sandwiched so that the positive electrode active material layer and the negative electrode active material layer faced to form a battery element. Overlay the area of 5mm from the outer periphery of the uncoated part formed around the bipolar electrode, heat press for 5 seconds under the conditions of pressure 0.2MPa and 200 ° C from the top and bottom, weld the periphery and seal each layer (See FIG. 6).

  Two high voltage terminals made of an aluminum plate having a size of 130 mm × 80 mm and a thickness of 100 μm were sandwiched so as to cover the entire projection surface of the positive electrode active material layer and the negative electrode active material layer of the outermost layer of the battery element. The battery element was vacuum sealed with aluminum laminate, and a part of the high voltage terminal was pulled out. The battery element was pressurized by atmospheric pressure to complete a bipolar battery with enhanced contact between the high voltage terminal and the battery element.

(Example 2)
A bipolar battery of Example 2 was fabricated in substantially the same manner as in Example 1 above. However, in Example 2, a current collector having anisotropy different from that in Procedure 1 of Example 1 was used.

In Example 2, the prepared current collector had a volume resistivity in the thickness direction of 1 × 10 ⁻² Ω · cm and a volume resistivity in the plane direction of 1 × 10 ⁶ Ω · cm.

(Example 3)
A bipolar battery of Example 3 was fabricated in substantially the same manner as in Example 1 above. However, in Example 3, a current collector having anisotropy different from the procedure 1 of Example 1 was used.

In Example 3, the prepared current collector had a volume resistivity of 1 × 10 ⁻² Ω · cm in the thickness direction and a volume resistivity of 1 × 10 ⁴ Ω · cm in the plane direction.

Example 4
A bipolar battery of Example 4 was fabricated in substantially the same manner as in Example 1 above. However, in Example 4, a current collector having anisotropy different from that in Procedure 1 of Example 1 was used.

In Example 4, the current collector was prepared, the thickness direction of the volume resistivity 1 × 10 ^-2 Ω · cm, the surface direction of the volume resistivity was 1 × 10 ² Ω · cm.

(Example 5)
A bipolar battery of Example 5 was fabricated in substantially the same manner as in Example 1 above. However, in Example 5, a current collector having anisotropy different from the procedure 1 of Example 1 was used.

In Example 5, the prepared current collector had a volume resistivity in the thickness direction of 1 × 10 ⁻² Ω · cm and a volume resistivity in the plane direction of 1 × 10 Ω · cm.

(Example 6)
A bipolar battery of Example 6 was fabricated in substantially the same manner as in Example 1 above. However, in Example 6, a current collector having anisotropy different from that in Procedure 1 of Example 1 was used.

In Example 6, the prepared current collector had a volume resistivity of 1 × 10 ⁻² Ω · cm in the thickness direction and a volume resistivity of 1 Ω · cm in the plane direction.

(Example 7)
A bipolar battery of Example 7 was fabricated in substantially the same manner as in Example 1 above. However, in Example 7, unlike the procedure 1 of Example 1, a current collector having a thickness of 20 μm containing a rubber material as a polymer material was prepared. Furthermore, in addition to the procedure 3 of Example 1, the formed bipolar electrode was press-rolled in the thickness direction at 170 ° C. to such an extent that the electrode active material layer did not break through the current collector. As a result, the current collector has anisotropy having conductivity only in the thickness direction.

(Example 8)
1. Preparation of current collector 20 μm in thickness including carbon fine particles (average particle size 0.8 μm; estimated for 70% by volume ready-made) and polypropylene (30% by volume estimated for ready-made) as polymer material A current collector was prepared. The volume resistivity in the thickness direction was 1 × 10 ⁻² Ω · cm, and the volume resistivity in the plane direction was 1 × 10 ⁸ Ω · cm.

2. Production of Positive Electrode Active Material Layer LiMn ₂ O ₄ (22 wt%) as a positive electrode active material, acetylene black (6 wt%) as a conductive additive, polyethylene oxide (PEO; 18 wt%) as an ion conductive polymer, and Li (as a supporting salt) C ₂ F ₅ SO ₂ ) ₂ N (9 wt%), N-methylpyrrolidone (NMP; 45 wt%) as a slurry viscosity adjusting solvent, azobisisobutyronitrile (AIBN; trace amount) as a polymerization initiator, A positive electrode slurry was prepared.

  A positive electrode slurry was applied to one side of the current collector, heated at 110 ° C. for 4 hours to proceed with thermal polymerization, and cured to obtain a positive electrode.

3. Preparation of negative electrode active material layer Li ₄ Ti ₅ O ₁₂ (14 wt%) as a negative electrode active material, acetylene black (4 wt%) as a conductive auxiliary agent, PEO (20 wt%) as an ion conductive polymer, Li (C as a supporting salt) ₂ F ₅ SO ₂ ) ₂ N (11 wt%), NMP (51 wt%) as a slurry viscosity adjusting solvent, and AIBN (trace amount) as a polymerization initiator were mixed to prepare a negative electrode slurry.

  A negative electrode slurry was applied to the opposite surface of the current collector on which the positive electrode was formed on one side, heated at 110 ° C. for 4 hours to proceed with thermal polymerization, and cured to obtain a negative electrode.

  According to procedures 2 and 3, a positive electrode active material layer and a negative electrode active material layer were formed on both sides of the current collector to complete a bipolar electrode. The resulting bipolar electrode was cut into 140 × 90 mm, and a positive electrode active material layer and a negative electrode active material layer were not applied to 10 mm around the electrode. As a result, the positive electrode active material layer and the negative electrode active material layer were applied in a central range of 120 × 70 mm, and an uncoated portion was formed in a range of 10 mm from the outer periphery to the inner side to produce a bipolar electrode.

4). Total solids PEO (64.5wt%) as prepared ion-conductive polymer electrolyte layer, _Li a _{(C 2 F 5 SO 2)} 2 N (35.5wt%) was prepared as a supporting salt, acetonitrile as viscosity preparing solvent Used to prepare an electrolyte slurry.

  An electrolyte slurry was poured between glass plates sandwiching a 50 μm gap and dried to prepare a 40 μm electrolyte layer. This solid electrolyte was cut into 130 × 80 mm to produce a solid electrolyte layer.

5. Production of Bipolar Battery Bipolar electrodes were laminated for five layers with the whole solid electrolyte layer sandwiched so that the positive electrode active material layer and the negative electrode active material layer faced to form a battery element.

  Two high voltage terminals made of an aluminum plate having a size of 130 mm × 80 mm and a thickness of 100 μm were sandwiched so as to cover the entire projection surface of the positive electrode active material layer and the negative electrode active material layer of the outermost layer of the battery element. The battery element was vacuum sealed with aluminum laminate, and a part of the high voltage terminal was pulled out. The battery element was pressurized by atmospheric pressure to complete a bipolar battery with enhanced contact between the high voltage terminal and the battery element.

(Comparative Example 1)
A bipolar battery of Comparative Example 1 was fabricated in substantially the same manner as in Example 1 above. However, in the comparative example 1, the collector different from the procedure 1 of Example 1 was used.

  In Comparative Example 1, a SUS foil having a thickness of 20 μm having no anisotropy was used as a current collector.

(Comparative Example 2)
A bipolar battery of Comparative Example 2 was fabricated in substantially the same manner as in Example 8 above. However, in Comparative Example 2, a current collector different from that in Procedure 1 of Example 8 was used.

  In Comparative Example 2, a SUS foil having a thickness of 20 μm and having no anisotropy was used as the current collector.

(Evaluation of bipolar battery using gel electrolyte)
A charge / discharge test was performed on the batteries of Examples 1 to 7 and Comparative Example 1. In the experiment, constant current charging (CC) was performed at a current of 0.5 mA up to 12.5 V, charging (CV) was then performed at a constant voltage, and charging was performed for 10 hours.

(Evaluation result 1)
The bipolar battery of Comparative Example 1 was not charged, and the voltage did not increase even when a current was passed. On the other hand, about Examples 1-7, charge was completed. From these results, in Examples 1 to 7, although the current collectors are in contact with each other at the end portions, the current collectors have anisotropy. You can see that the battery has been charged. Therefore, it has been found that there is no need to dispose an insulating member between the current collectors.

(Evaluation result 2)
Next, the fully charged battery was left for one month, and the subsequent voltage was measured. The measurement results are as shown in FIG. FIG. 9 is a diagram illustrating a voltage after one month has elapsed after charging each bipolar battery.

  As shown in FIG. 9, the volume resistivity in the thickness direction in the surface direction of the current collector is 1000 times or less compared to Examples 1 to 5 and 7 in which the volume resistivity in the thickness direction is 1000 times or more The voltage of Example 6 was greatly reduced. Therefore, it is understood that the anisotropy of the current collector used for the bipolar battery is better if the volume resistivity in the plane direction is 1000 times or more the volume resistivity in the thickness direction.

(Evaluation result 3)
Thereafter, discharging was performed at about 1 mA for 5 seconds, the internal resistance of the battery was measured from the voltage at that time, and the resistance values of Examples 3 to 7 when Example 1 was taken as 100% were measured. The measurement results are as shown in FIG. FIG. 10 is a graph showing the ratio of the internal resistance of each of the other bipolar batteries, where the internal resistance of the bipolar battery of Example 1 is 100%.

  As shown in FIG. 10, the internal resistance of the bipolar batteries of Examples 1 to 6 was around 100%, whereas the internal resistance of the bipolar battery of Example 7 was as low as 82%, which was found to be suitable. Therefore, as in Example 7, using a film that develops anisotropy in response to pressure as a current collector of a bipolar battery, the active material layer is heated and pressed together with the current collector to form a bipolar electrode. It turned out to be preferable.

(Evaluation of bipolar battery using solid electrolyte)
A charge / discharge test was performed on the batteries of Example 8 and Comparative Example 2. In the experiment, constant current charging (CC) was performed at a current of 0.1 mA up to 12.5 V, charging (CV) was then performed at a constant voltage, and charging was performed for 10 hours.

  The bipolar battery of Comparative Example 2 was not charged, and the voltage did not increase even when a current was passed. On the other hand, charging was completed in the bipolar battery of Example 8.

  From this result, as shown in FIG. 2, even in the case of a bipolar battery in which the ends of the current collector are free and the current collectors can be in contact with each other at the ends, the anisotropy of the current collector It was found that no short circuit occurred. That is, it was found that an insulating material is not necessary.

  Further, it was found that by using an all solid electrolyte, a seal structure as shown in FIG. 6 is unnecessary, and the structure can be further simplified.

10 Bipolar battery,
11 Current collector,
12 positive electrode active material layer,
13 negative electrode active material layer,
14 electrolyte layer,
14 'gel electrolyte layer,
15 cell layer,
16 bipolar electrodes,
17 End current collector,
20 battery elements,
30a, 30b electrodes,
40 exterior,
41 Laminate sheet,
70 battery packs,
80 cars.

Claims (4)

Preparing a current collector containing conductive particles at random in a polymer material;
Heating and pressing the current collector and compressing in the thickness direction;
The manufacturing method of the electrical power collector containing this.   The current collector has the positive electrode active material layer disposed on one surface and the negative electrode active material layer disposed on the other surface together with the positive electrode active material layer and the negative electrode active material layer. The method for producing a current collector according to claim 1.   The method for producing a current collector according to claim 1 or 2, wherein the current collector is obtained by randomly blending 6 to 10% by volume of conductive particles inside a polymer material.   The current collector has a positive electrode active material layer disposed on one surface, a negative electrode active material layer disposed on the other surface, and is laminated together with an electrolyte layer, thereby forming a bipolar battery. The manufacturing method of the electrical power collector as described in any one of Claims.

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