WO2006003849A1 - リチウム二次電池用負極材料及びその製造方法、並びにそれを用いたリチウム二次電池用負極及びリチウム二次電池 - Google Patents
リチウム二次電池用負極材料及びその製造方法、並びにそれを用いたリチウム二次電池用負極及びリチウム二次電池 Download PDFInfo
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- WO2006003849A1 WO2006003849A1 PCT/JP2005/011641 JP2005011641W WO2006003849A1 WO 2006003849 A1 WO2006003849 A1 WO 2006003849A1 JP 2005011641 W JP2005011641 W JP 2005011641W WO 2006003849 A1 WO2006003849 A1 WO 2006003849A1
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01M—PROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
- H01M4/00—Electrodes
- H01M4/02—Electrodes composed of, or comprising, active material
- H01M4/36—Selection of substances as active materials, active masses, active liquids
- H01M4/58—Selection of substances as active materials, active masses, active liquids of inorganic compounds other than oxides or hydroxides, e.g. sulfides, selenides, tellurides, halogenides or LiCoFy; of polyanionic structures, e.g. phosphates, silicates or borates
- H01M4/583—Carbonaceous material, e.g. graphite-intercalation compounds or CFx
- H01M4/587—Carbonaceous material, e.g. graphite-intercalation compounds or CFx for inserting or intercalating light metals
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01M—PROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
- H01M10/00—Secondary cells; Manufacture thereof
- H01M10/05—Accumulators with non-aqueous electrolyte
- H01M10/052—Li-accumulators
- H01M10/0525—Rocking-chair batteries, i.e. batteries with lithium insertion or intercalation in both electrodes; Lithium-ion batteries
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- C—CHEMISTRY; METALLURGY
- C01—INORGANIC CHEMISTRY
- C01B—NON-METALLIC ELEMENTS; COMPOUNDS THEREOF; METALLOIDS OR COMPOUNDS THEREOF NOT COVERED BY SUBCLASS C01C
- C01B32/00—Carbon; Compounds thereof
- C01B32/20—Graphite
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- C—CHEMISTRY; METALLURGY
- C01—INORGANIC CHEMISTRY
- C01B—NON-METALLIC ELEMENTS; COMPOUNDS THEREOF; METALLOIDS OR COMPOUNDS THEREOF NOT COVERED BY SUBCLASS C01C
- C01B32/00—Carbon; Compounds thereof
- C01B32/20—Graphite
- C01B32/21—After-treatment
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01M—PROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
- H01M4/00—Electrodes
- H01M4/02—Electrodes composed of, or comprising, active material
- H01M4/04—Processes of manufacture in general
- H01M4/0402—Methods of deposition of the material
- H01M4/0404—Methods of deposition of the material by coating on electrode collectors
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01M—PROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
- H01M4/00—Electrodes
- H01M4/02—Electrodes composed of, or comprising, active material
- H01M4/04—Processes of manufacture in general
- H01M4/043—Processes of manufacture in general involving compressing or compaction
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01M—PROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
- H01M4/00—Electrodes
- H01M4/02—Electrodes composed of, or comprising, active material
- H01M4/36—Selection of substances as active materials, active masses, active liquids
- H01M4/362—Composites
- H01M4/364—Composites as mixtures
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01M—PROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
- H01M4/00—Electrodes
- H01M4/02—Electrodes composed of, or comprising, active material
- H01M2004/021—Physical characteristics, e.g. porosity, surface area
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E60/00—Enabling technologies; Technologies with a potential or indirect contribution to GHG emissions mitigation
- Y02E60/10—Energy storage using batteries
Definitions
- Negative electrode material for lithium secondary battery method for producing the same, and negative electrode for lithium secondary battery using the same and lithium secondary battery
- the present invention relates to a negative electrode material for a lithium secondary battery, a method for producing the same, and a negative electrode for a lithium secondary battery and a lithium secondary battery using the same.
- a lithium secondary battery negative electrode material comprising graphite powder, characterized in that the battery performance is excellent in a well-balanced manner even when used at high electrode density.
- the present invention relates to a negative electrode material and a method for producing the same, and a negative electrode for a lithium secondary battery using the same and a lithium secondary battery.
- Amorphous carbon, artificial graphite, natural graphite and the like have been studied as a negative electrode material for lithium secondary batteries.
- natural graphite unlike the above-mentioned artificial graphite, has a high discharge capacity close to the theoretical capacity due to the developed graphite crystal, and the press load at the time of electrode formation is small and wide in that it is inexpensive. It has been used.
- Patent Document 1 discloses cycle characteristics and preservation by subjecting highly crystalline natural graphite to a purification treatment at a temperature of 2400 ° C. or higher in a nitrogen gas or argon gas atmosphere. It is described to obtain a natural graphite negative electrode material having excellent properties.
- Patent Document 2 the packing property is high by forming highly crushed natural graphite or artificial graphite into relatively isotropic rounded particles by mechanical energy treatment. It is described that an electrode having high capacity and excellent load characteristics and cycle characteristics can be obtained. It is also described that after mechanical energy treatment, if the true density is less than 2.25 gZ cm 3 and the crystallinity is not very high, the heat treatment to further enhance the crystallinity is performed at 2000 ° C. or higher.
- Patent Document 3 discloses that a natural graphite or the like having an average particle diameter in a specific range is re-heat treated at a temperature of 2000 ° C. or higher, and is required in Raman spectrum analysis using argon ion laser light. It is described that a negative electrode material excellent in load characteristics can be obtained by setting the Raman R value and the peak half width within a specific range.
- Patent Document 1 Patent No. 3188032
- Patent Document 2 Japanese Patent Application Laid-Open No. 2000-223120
- Patent Document 3 Japanese Patent Application Laid-Open No. 11-25979
- the graphite negative electrode particles are easily oriented parallel to the current collector, the electrode expansion due to the formation of the graphite interlayer compound with lithium increases, and the amount of the active material that can be packed per unit volume of the electrode active material Decrease, resulting in a decrease in battery capacity.
- Patent Document 1 When a natural graphite such as scaly, etc. is used in high pressure and electrode density in Patent Document 1 while the force is applied, the pores in the electrode are reduced and the crystals are reduced. Patent Document 1 does not mention the improvement at all, which has the problem that load characteristics are degraded because it is easy to align in the same direction.
- Patent Document 2 also describes that when the true density is less than 2.25 g Z cm 3 and the crystallinity is low, the heat treatment to further enhance the crystallinity is performed at 2000 ° C. or more.
- the true density is high at 2.25 gZ cm 3 or more after the chemical treatment, the need for heat treatment is not touched at all, and the surface functional group content of the graphite material is not touched at all.
- Patent Document 3 the use of highly crystalline scaly natural graphite or the like is insufficient in terms of suppressing expansion during battery charging in which the orientation ratio of the electrode active material is low. That is, even if the active material has high crystal and high capacity, the conventional graphite negative electrode material reduces pores in the electrode when the electrode density becomes higher (for example, 1.6 gZ cm 3 or more), and the crystals are identical. Since it is easy to align in the direction, it is difficult to simultaneously achieve high charge / discharge efficiency, high load characteristics, expansion suppression during battery charging, and suppression of gas generation amount.
- the present invention has been made in view of the above problems. That is, the present invention is a negative electrode material which also has a graphite powder power, and even when used at a high electrode density, it has excellent load characteristics in which the charge / discharge efficiency is high and the discharge capacity is high. , Anode materials capable of obtaining a lithium secondary battery excellent in balance with various battery performances, such as expansion suppressed at the time of battery charge and having a small amount of gas generation, and such anode materials efficiently and inexpensively It is an object of the present invention to provide a method for producing a negative electrode material for a lithium secondary battery that can be manufactured as well as a negative electrode for a lithium secondary battery and a lithium secondary battery using the same. Means to solve the problem
- the inventors of the present invention conducted intensive studies on a negative electrode material having a graphite powder power, and as a result, used a negative electrode material having a tap density, a Raman R value, and a BET specific surface area within a predetermined range.
- a negative electrode material having a tap density, a Raman R value, and a BET specific surface area within a predetermined range Even when used at a high electrode density, the press load force at the time of electrode formation, the charge and discharge efficiency at high discharge capacity are excellent, and the load characteristics are high, battery expansion is suppressed, and the gas generation amount is increased.
- the inventors have found that the above-described negative electrode material can be stably, efficiently and inexpensively manufactured, and
- the gist of the present invention is a negative electrode material for a lithium secondary battery which also has a graphite powder (A), and the tap density of the graphite powder (A) is 0.8 g / cm 3 or more, 1. 35 g. / cm 3 or less, surface functional group weight OZC value is 0 or more, 0.10 or less, BET specific surface area is 2.5 mg or more, 7.0 m 2 Zg or less, Raman R value is 0.0 2
- the present invention relates to a negative electrode material for a lithium secondary battery, characterized in that the above is not more than 0.05.
- the surface functional group amount OZC value and Raman R value are measured by the following method.
- Another aspect of the present invention is a method of producing a negative electrode material for a lithium secondary battery, which has a tap density of 0.8 g Z cm 3 or more and 1. 35 g Z cm 3 or less, and a BET specific surface area of 3 Natural graphite having a true density of 2.25 g Zcm 3 or more, which is 5 m 2 Zg or more and 11.0 m 2 Zg or less Is heat treated at 1600 ° C. or more and 3200 ° C. or less to obtain a graphite powder (C) having a surface functional group amount OZC value of 0.10 or less, a negative electrode material for a lithium secondary battery It belongs to the manufacturing method.
- Another aspect of the present invention is to provide a current collector and an active material layer formed on the current collector, and the active material layer is the negative electrode for lithium secondary battery described above.
- a negative electrode for a lithium secondary battery comprising the material or the negative electrode material for a lithium secondary battery obtained by the above-mentioned production method.
- another aspect of the present invention is characterized in that a positive electrode and a negative electrode capable of absorbing and desorbing lithium ions, and an electrolyte are provided, and the negative electrode is the above-described negative electrode for lithium secondary battery. Yes, they reside in lithium secondary batteries.
- the negative electrode material for a lithium secondary battery of the present invention even when used at a high electrode density, it is possible to realize a lithium secondary battery excellent in various types of battery performance in a well-balanced manner.
- the method for producing a negative electrode material for a lithium secondary battery according to the present invention heat-treats natural graphite as a raw material, the number of steps can be reduced, and the above-mentioned negative electrode material for lithium secondary battery can be efficiently obtained in a high yield. And it can be manufactured inexpensively, and is very useful industrially.
- the negative electrode material for a lithium secondary battery of the present invention (hereinafter appropriately referred to as “the negative electrode material of the present invention”) is characterized by comprising a graphite powder (A) satisfying the following characteristics. Although this graphite powder (A) may be used alone, it may be mixed with other carbon material (B) as needed as described later.
- the graphite powder (A) (hereinafter referred to as “graphite material of the present invention” as appropriate) used as the negative electrode material of the present invention has a tap density of 0.8 g Z cm 3 or more and 1. 35 g Z cm 3 or less.
- Amount OZC value is 0 or more, 0.10 or less
- BET specific surface area is 2.5 m 2 Zg or more
- Raman R value is 0.02 or more, 0. 05 or less It is characterized by
- the shape of the graphite material of the present invention is not particularly limited, and examples thereof include spheres and ovals.
- the degree of circularity of the graphite material of the present invention is not particularly limited, but is usually in the range of 0.90 or more, preferably 0.92 or more, and usually 0.96 or less, preferably 0.95 or less. If the degree of circularity falls below this range, the gaps between the particles become smaller, which may lower the load characteristics. On the other hand, in order to make the degree of circularity a value exceeding this range, it is necessary to perform spheric treatment strongly or for a long time, which is not preferable because the production cost becomes high.
- the diameter of a circle having a projected area of Z particles can be measured using a flow type particle image analyzer (for example, FPIA manufactured by SYSMETAS INDUSTRIAL CORPORATION).
- FPIA flow type particle image analyzer
- 0.2 g of a graphite material was mixed with a 0.2 volume% aqueous solution (about 50 ml) of polyoxyethylene (20) sonorebitan monoacrylate as a surfactant, and 28 kHz ultrasound was irradiated for 1 minute at an output of 60 W.
- the detection range is specified to 0.6 to 40 ⁇ m, and it is possible to use the value measured for particles in the range of 10 to 40 ⁇ m.
- the tap density of the graphite material of the present invention is usually 0. 8gZcm 3 or more, preferably 0. 9 g / cm 3 or more, more preferably 0. 95gZcm 3 or more, and usually 1. 35gZcm 3 or less, preferably 1. 2GZcm
- the range is 3 or less. If the tap density is less than this range, it is difficult to obtain a high capacity battery in which the packing density is increased and difficult when used as a negative electrode material. On the other hand, when this range is exceeded, the gaps between particles in the electrode become too small, it becomes difficult to secure the conductivity between the particles, and it is difficult to obtain desirable battery characteristics.
- a tap density using a sieve with an opening of 300 ⁇ m, drop the measurement target (here, a graphite material) in a 20 cm 3 tapping cell to fully fill the cell, and then use a powder density measuring device A tapping length of 10 mm may be tapped 1000 times using (for example, a tap denser manufactured by Seishin Enterprise Co., Ltd.), and a value obtained by measuring the tapping density at that time can be used.
- a tap denser manufactured by Seishin Enterprise Co., Ltd. for example, a tap denser manufactured by Seishin Enterprise Co., Ltd.
- the surface functional group weight O ZC value of the graphite material of the present invention measured using X-ray photoelectron spectroscopy (XPS) is usually in the range of 0 or more, and usually 0.10 or less, preferably 0.004 or less .
- XPS X-ray photoelectron spectroscopy
- the OZC value represents the ratio of oxygen atom concentration to carbon atom concentration on the surface of a graphite material or the like, and functional groups such as carboxyl group, phenolic hydroxyl group and carbonyl group are present on the surface. It is an index that represents quantity.
- a carbon material having a large surface functional group ozc value indicates that a surface oxygen-containing functional group is bonded to an end face or the like of a crystal face of particle surface carbon.
- the surface functional group content OZC value of the graphite material in X-ray photoelectron spectroscopy analysis, the peak area of the Cls and Ols spectrum is determined, and based on this, the atomic concentration ratio of C and O is determined. Calculate oZc (o atom concentration Zc atom concentration) and use this value.
- the specific measurement procedure is not particularly limited, and an example is as follows.
- the object to be measured (here, a graphite material) is placed on a sample table so that the surface is flat.
- the spectra of Cls (280 to 300 eV) and Ols (525 to 545 eV) are measured by multiplex measurement with ⁇ alpha rays as the X-ray source.
- the peak top of the obtained Cls is corrected to 284.3 eV, the peak areas of the Cls and Ols spectra are determined, and the device sensitivity coefficients are multiplied to calculate the surface atomic concentrations of C and O respectively.
- the atomic concentration ratio OZC (O atomic concentration ZC atomic concentration) of the obtained O and C is calculated, and this is defined as the surface functional group weight OZC value of the graphite material.
- the specific surface area of the graphite material of the present invention measured using the BET method is usually 2.5 m 2 Zg or more, preferably 3.0 m 2 Zg or more, and usually 7.0 m 2 Zg or less, preferably 5 .5m g or less.
- the specific surface area falls below this range, lithium readily deteriorates in lithium acceptability at the time of charging when used as a negative electrode material, which is not preferable from the viewpoint of safety, because lithium is easily deposited on the electrode surface.
- when exceeding this range it was used as a negative electrode material
- the reactivity with the electrolyte increases, and it is difficult to obtain a preferable battery which easily generates a large amount of gas.
- the BET specific surface area using a surface area meter (for example, a fully automatic surface area measuring device manufactured by Okura Riken), preliminary drying is carried out at 350 ° C. for 15 minutes under a stream of nitrogen against the object to be measured (here, a graphite material). After carrying out, use the value measured by the nitrogen adsorption by the gas flow method using the BET one-point method using a nitrogen-helium mixed gas that has been precisely adjusted so that the value of the relative pressure of nitrogen to the atmospheric pressure is 0.3. it can.
- a surface area meter for example, a fully automatic surface area measuring device manufactured by Okura Riken
- the Raman R value of the graphite material of the present invention measured using the Raman method is usually in the range of not less than 0.02, preferably not less than 0.03, and usually not more than 0.05, preferably not more than 0.04. is there.
- Raman R-value force S Below this range, the crystallinity of the particle surface becomes too high, and in the case of high density, the crystal tends to be oriented parallel to the electrode plate, which may cause a decrease in load characteristics. There is. On the other hand, if this range is exceeded, crystals on the particle surface may be disturbed, the reactivity with the electrolytic solution may be increased, and the efficiency may be decreased or gas generation may be increased.
- the Raman half width of the graphite material of the present invention is not particularly limited, it is usually in the range of usually 18.0 or more, preferably 19.0 or more, and usually 22.5 or less, preferably 21.5 or less. is there. If the Raman half width is less than this range, the crystallinity of the particle surface becomes too high, and in the case of high density, crystals tend to be oriented parallel to the electrode plate, which may cause deterioration in load characteristics. Ru. On the other hand, if this range is exceeded, crystals on the particle surface may be disturbed, the reactivity with the electrolytic solution may be increased, and the efficiency may be reduced or gas generation may be increased.
- a sample is charged by naturally dropping a measurement target (here, a graphite material) into a measurement cell using a Raman spectrometer (for example, Raman spectrometer manufactured by Nippon Bunko Co., Ltd.).
- the cell surface is rotated in a plane perpendicular to the laser beam while irradiating the sample surface with argon ion laser beam.
- the Raman measurement conditions here are, for example, as follows.
- the volume-based average particle size of the graphite material of the present invention is not particularly limited, but is usually in the range of preferably 14 ⁇ m or more, and usually 50 ⁇ m or less, preferably 40 ⁇ m or less. Below this range, when mixed with a binder which easily aggregates when used as a negative electrode material, it may become lumpy and the coated electrode may become nonuniform. On the other hand, if this range is exceeded, coating unevenness is likely to occur when the electrode is manufactured by coating as a negative electrode material.
- volume-based average particle diameter, 2 volumes 0/0 aqueous solution of polyoxyethylene (20) sorbitan monolaurate as a surfactant (about lml) were mixed to graphite powders, a dispersing medium of ion-exchanged water
- a value obtained by measuring the volume-based average particle diameter (median diameter) with a laser diffraction particle size distribution analyzer (for example, LA-700 manufactured by Horiba, Ltd.) can be used as As the ratio of 90% particle diameter to 10% particle diameter (d / ⁇ ), similarly measure 90% particle diameter and 10% particle diameter based on volume,
- the ratio of (d / ⁇ ) can be used.
- the spacing d of the (002) plane of the graphite material of the present invention measured by X-ray diffraction is particularly limited although not preferred, it is usually in the range of 0.3356 nm or less, preferably 0.3355 nm or less. If this range is exceeded, that is, if the crystallinity is poor, the discharge capacity per unit weight of the active material may decrease when the electrode is manufactured. On the other hand, the lower limit of the surface separation d
- 002 is usually 0.33 nm or more as a theoretical limit.
- 00 is not particularly limited, it is usually in the range of 90 nm or more, preferably 100 nm or more.
- the graphite material of the present invention as an active material, the electrode density 1. 63 ⁇ 0. 05g / cm 3, i.e., 1. 58GZcm 3 or 1. active material orientation ratio of the formed electrode to be within the scope of 68GZcm 3 Is usually 0.02 or more, preferably 0.30 or more, more preferably 0.004 or more, and usually 0.09 or less, preferably 0.80 or less. Below this range, the electrode expansion during battery charging when the battery is manufactured becomes large, and there is a possibility that the battery capacity per unit volume of the electrode can not be increased. On the other hand, if it exceeds this range, the crystallinity of the active material is lowered, and the press load at the time of electrode formation tends to be large, and it is difficult to increase the packing density of the electrode after pressing.
- the active material orientation ratio of the electrode is an index indicating the degree of orientation of the graphite crystal hexagonal network in the thickness direction of the electrode. As the orientation ratio is larger, the direction of the graphite crystal hexagonal mesh plane of the particles is more uniform, which represents the state.
- the specific procedure for measuring the active material orientation ratio of the electrode is as follows.
- Graphite material CMC (carboxymethylcellulose) aqueous solution as a thickener, SBR (styrene 'butadiene rubber) aqueous solution as a binder resin, with respect to the total weight of the mixture of graphite material, CMC and SBR after drying, Mix and agitate so that CMC and SBR become 1% by weight, respectively, to make a slurry. Then, using a doctor blade, 18 m thick copper foil Apply slurry on top. Coating thickness, after drying the electrode weight (exclusive of the copper foil) to select the gap so that lOmgZc m 2. After drying this electrode at 80 ° C, press the electrode density (excluding copper foil) to a force S1. 63 ⁇ 0. 05 g / cm 3 .
- the active material orientation ratio of the electrode For the electrode after pressing, measure the active material orientation ratio of the electrode by X-ray diffraction.
- the specific method is not particularly limited, as a standard method, the charts of the (110) plane and the (004) plane of the graphite material are measured by X-ray diffraction, and the asymmetric pieson is used as a profile function for the measured chart. Peak separation is performed by fitting using VII, and integrated intensities of the (110) plane and (004) plane peaks are calculated. From the obtained integrated intensity, a ratio represented by (110) area intensity intensity Z (004) area intensity is calculated and defined as an active material orientation ratio of the electrode.
- the X-ray diffraction measurement conditions here are as follows.
- 2 ⁇ indicates the diffraction angle.
- the active material orientation ratio by X-ray diffraction can be determined for an electrode formed to have an electrode density of 1.63 ⁇ 0.5 g / cm 3 .
- the discharge capacity of the lithium secondary battery is, for example, 355 mAh or more. Furthermore, it will be in the range of 360 mAh Zg or more. If the discharge capacity falls below this range, it becomes difficult to improve the battery capacity. Also, the higher the discharge capacity, the higher the better! /, But the upper limit is usually about 370 mAh Zg. There are no particular limitations on the specific method of measuring the discharge capacity, but a standard measurement method is as follows.
- an electrode using a graphite material is produced.
- the electrode is manufactured by using a copper foil as a current collector and forming an active material layer on the current collector.
- a mixture of a graphite material and styrene butadiene rubber (SBR) as binder resin is used for the active material layer.
- SBR styrene butadiene rubber
- the amount of noinda resin is 1% by weight with respect to the weight of the electrode.
- the electrode density is in the range of 1.45 g Z cm 3 or more and 1. 95 g Z cm 3 or less.
- the evaluation of the discharge capacity is carried out by preparing a two-electrode coin cell using metal lithium as a counter electrode on the manufactured electrode and performing a charge-discharge test.
- the electrolyte of the two-pole coin cell is an optional force.
- the separator used in the bipolar coin cell may be any force, for example, a polyethylene sheet having a thickness of 15 ⁇ m to 35 ⁇ m.
- a charge / discharge test is performed using the two-pole coin cell manufactured in this manner to determine the discharge capacity. Specifically, charge to 5mV with respect to the lithium counter electrode at a current density of 0.2mAZcm 2 and charge to a current value of 0.20mA at a constant voltage of 5mV, and dope lithium into the negative electrode. After that, repeat the charge and discharge cycle of discharging the lithium counter electrode to 1.5 V at a current density of 0.4 mAZcm 2 for 3 cycles, and let the discharge value for the third cycle be the discharge capacity.
- the method for producing the above-mentioned graphite powder (A) (the graphite material of the present invention) is not particularly limited, but preferred examples include the following methods.
- the method for producing a negative electrode material for a lithium secondary battery of the present invention (hereinafter appropriately referred to as “the production method of the present invention”) has a tap density of 0.8 g Z cm 3 or more and 1. 35 g Z cm 3 or less in and, BET specific surface area of 3. 5 m 2 Zg above, 11. and a 0 m 2 Zg hereinafter, true density of 2. 25 g / c
- the surface functional group amount OZC value of black bell powder after heat treatment is set to 0.10 or less.
- natural graphite as a raw material is preferably a spheroidized graphite powder.
- natural graphite is used as a starting material.
- natural graphite is classified into flake-like graphite (Flake Graphite), flake-like graphite (Crystalline (Vein) Graphite), and soil graphite (Amorphous Graphite) according to its properties (" Industrial Technology Center Co., Ltd., See Graphite issued in 1959, and “HAND BOOK OF CARBON, GRAPHITE, DIAMOND AND FULLERENES”, published by Noy es Publications).
- the degree of graphitization is as high as 100% for scaly graphite followed by 99.9% for scaly graphite and as low as 28% for soil graphite.
- the quality of natural graphite is mainly determined by the production site and veins.
- Flaky graphite is produced in Madagascar, China, Brazil, Ukraine, China and other countries, and flaky graphite is produced mainly in Sri Lanka. Soil graphite is mainly produced on the Korean peninsula, China, Mexico and other countries.
- scale-like graphite and scale-like graphite are preferable as the raw material of the present invention because they have advantages such as a small amount of impurities having a high graphite density.
- the above-mentioned natural graphite is subjected to an acid treatment such as hydrochloric acid or hydrofluoric acid and a purification treatment to remove ash by heat treatment at Z or 2000.degree.
- an acid treatment such as hydrochloric acid or hydrofluoric acid
- a purification treatment to remove ash by heat treatment at Z or 2000.degree.
- the ash content of natural graphite subjected to the above-mentioned ash removal is not particularly limited, but is usually not less than 0.00% by weight, and usually not more than 0.20% by weight, preferably not more than 0.15% by weight. It is a range. Ash force S If this range is exceeded, there is a risk that the storage characteristics may deteriorate due to self-discharge.
- the method defined in JIS M 8812 can be used.
- the true density of natural graphite before heat treatment is usually in the range of 2.25 g Z cm 3 or more.
- the true density hardly changes due to the heat treatment described later. Below this range, the heat treatment The crystallinity is not improved, and the discharge capacity per unit weight of the active material may be reduced when the electrode is manufactured, which is not preferable.
- the upper limit of the true density is usually 2.27 gZ cm 3 or less as a theoretical limit.
- the tap density of the natural graphite before the heat treatment is usually 0. 8gZcm 3 or more, preferably 0. 9 g / cm 3 or more, more preferably 0. 95gZcm 3 or more, and usually 1. 35gZcm 3 or less, preferably 1. 2GZcm
- the range is 3 or less.
- the tap density may change due to heat treatment to be described later, but using natural graphite having a tap density in this range, the tap density of natural black lead after heat treatment may be within the range defined above. It is possible. If the tap density of natural black lead before heat treatment falls below this range, it is difficult to obtain a high capacity battery in which the packing density is increased and difficult when the heat treated graphite material is used as the active material. On the other hand, when this range is exceeded, the number of voids between particles in the electrode when the heat-treated graphite material is used as the active material is too large, the conductivity between particles is difficult to be secured, and favorable battery characteristics are difficult to obtain. .
- the method for measuring the tap density is as described above.
- the BET specific surface area of natural graphite before heat treatment is usually 3.5 m 2 Zg or more, preferably 4.5 m 2 Zg or more, and usually 1.10 m 2 Zg or less, preferably 9.0 m 2 Zg or less, more preferably 7 0 m 2 Zg or less Since the BET specific surface area is reduced by heat treatment described later, by using natural graphite having a BET specific surface area within this range, the BET specific surface area of the natural graphite after heat treatment should be within the range defined above. Is possible.
- the measurement method of the BET specific surface area is as described above.
- the Raman R value of natural graphite before heat treatment is not particularly limited, but is usually 0.10 or more, preferably Or 0.20 or more, and usually 0.35 or less, preferably 0.30 or less.
- the R value is below this range, the crystallinity of the particle surface of the graphite material becomes too high after heat treatment, and when the density is increased, the crystals tend to be oriented parallel to the electrode plate, and the load characteristics are degraded. There is a risk of On the other hand, if this range is exceeded, the crystal restoration of the particle surface of the graphite material after heat treatment is insufficient, the reactivity with the electrolytic solution is increased, and the efficiency may be decreased and the gas generation may be increased.
- the Raman half value width of natural graphite before heat treatment is not particularly limited, but is usually in the range of 21.0 or more, preferably 21.5 or more, and usually 26.0 or less, preferably 24.0 or less. It is. If the half width is less than this range, the crystallinity of the particle surface becomes too high, and when the density is increased, the crystals may be easily oriented in the parallel direction to the electrode plate, which may lead to a decrease in load characteristics. On the other hand, if this range is exceeded, the crystal surface of the particle is not sufficiently repaired in the subsequent heat treatment step, and the as-disturbed crystal remains, increasing the reactivity with the electrolytic solution, reducing the efficiency and generating gas. May cause an increase in
- the spacing d of the (002) plane measured by X-ray diffraction of natural graphite before heat treatment is particularly limited.
- the range is usually 0.33 nm or less, preferably 0.33 nm or less. If this range is exceeded, that is, if the crystallinity is poor, the crystal repair of the particles is not sufficiently performed in the subsequent heat treatment step, and the discharge capacity per unit weight of the active material is small when the electrode is manufactured. There is a risk of On the other hand, the lower limit of the above-mentioned face separation d is a theoretical limit.
- the discharge capacity per weight of the active material may be reduced when the electrode is manufactured.
- the measuring method of surface spacing is based on the said description.
- the degree of circularity of natural graphite before heat treatment is not particularly limited, but is usually 0.90 or more, preferably Is in the range of 0.92 or more and usually 0.96 or less, preferably 0.95 or less. If the degree of circularity is less than this range, when the heat-treated graphite material is used as the negative electrode material, the gaps between the particles become small, and the load characteristics may be deteriorated. On the other hand, in order to exceed this range, it is necessary to perform processing such as spheroidizing treatment strongly or for a long time, and it is necessary to remove a large amount of fine powder by-produced at the time of spheroid treatment. Not desirable.
- the measuring method of circularity is based on the said description.
- the method for obtaining natural graphite before heat treatment having a tap density in the above range is not particularly limited, but natural graphite spheroidized by spheroidizing treatment is preferable.
- a device that repeatedly applies mechanical action such as compression, friction, shear force, etc., including particle interaction mainly based on impact force.
- it has a rotor with a large number of blades installed inside the casing, and when the rotor rotates at high speed, mechanical such as impact compression, friction, and shear force are applied to the carbon material introduced inside.
- An apparatus that exerts action and performs surface treatment is preferred.
- a hybridisation system manufactured by Nara Machinery Co., Ltd. can be mentioned.
- Heat treatment is performed on natural graphite having a tap density in the above range under the following conditions.
- the crystals on the surface of the natural graphite particles may be disordered, and the disorder is particularly pronounced when the above-mentioned spheroidizing treatment is carried out, but the heat treatment produces a disordered graphite particle surface.
- the crystals can be repaired to reduce the Raman R value and BET specific surface area.
- the temperature conditions at the time of heat treatment are not particularly limited, but are usually 1600 ° C. or more, preferably 2000 ° C. or more, more preferably 2500 ° C. or more, and usually 3200 ° C. or less, preferably 3100 ° C. or less It is a range. If the temperature condition is below this range, the crystal restoration on the surface of the graphite particle disturbed by the spheroidizing treatment is insufficient, and the Raman R value and the BET specific surface area force S are not small, which is not preferable. On the other hand, if the above range is exceeded, the amount of sublimation of graphite tends to be large, which is also not preferable.
- the holding time to keep the temperature condition in the above range is not particularly limited. However, it is usually longer than 10 seconds and less than 72 hours.
- the heat treatment is performed in an inert gas atmosphere such as nitrogen gas, or in a non-acidic atmosphere with a gas generated from the raw material graphite.
- the apparatus used for the heat treatment is not particularly limited.
- a shuttle furnace, a tunnel furnace, an electric furnace, a lead hammer furnace, a rotary kiln, a direct current conduction furnace, an atchison furnace, a resistance heating furnace, an induction heating furnace, etc. can be used. .
- the surface functional group content of the graphite can be controlled, for example, by controlling the atmosphere oxygen concentration at the time of heat treatment.
- the surface functional group weight OZC value is not more than 0.01 by controlling the atmospheric oxygen concentration, the treatment temperature and the treatment time.
- the surface functional group content of natural graphite before heat treatment is not particularly limited, but is usually in the range of 0.70 or less, preferably 0.04 or less.
- Surface Functional Group Amount When the OZC value exceeds this range, the surface functional group amount after heat treatment, the OZC value does not easily fall within the previously defined range.
- the amount of surface functional groups OZC of the graphite powder after the heat treatment is not particularly limited, but is usually in the range of 0.10 or less, preferably 0.004 or less.
- Surface Functional Group Amount When the OZC value exceeds this range, the functional group amount on the particle surface increases, the reactivity with the electrolytic solution increases, and there is a possibility that the gas generation amount may be increased.
- the classification process is for removing coarse and fine powders which make the particle size after graphitization process the target particle size.
- the apparatus used for classification treatment is not particularly limited.
- the apparatus used for classification treatment is not particularly limited.
- dry sieving in the case of dry sieving
- inertia type classifier inertia type classifier, centrifugal type classifier (classifier, cyclone etc.) etc.
- wet sieving mechanical wet classifier, hydraulic classifier, sedimentation classifier, centrifugal wet classification A machine etc. can be used, respectively.
- the classification process can be performed before the heat treatment, or may be performed at other timings, for example, after the heat treatment. Furthermore, it is possible to omit the classification process itself. However, graphite From the viewpoint of the productivity of the powder negative electrode material, it is preferable to carry out classification treatment immediately after the spheronization treatment and before heat treatment.
- the above-mentioned graphite powder (A) (or the heat-treated graphite powder obtained by the above-mentioned production method of the present invention.
- This is referred to as graphite powder (C)
- graphite powder (C) can be used as it is as a negative electrode material.
- two or more kinds of graphite powder (A) (or graphite powder (C)) which are good even when any one kind of graphite powder (A) (or graphite powder (C)) is used alone, and any combination and It may be used in combination.
- the negative electrode material that is, one or more of graphite powder (A) (or graphite powder (C)) is mixed with other one or more carbon materials (B), and this is used as a negative electrode material. You may use it as,.
- the total amount of (A) and (B) (or (C) and (B) is usually 5% by weight or more, preferably 20% or more, and usually 95% by weight or less, preferably 80% by weight or less.
- the mixing ratio of the carbon material (B) falls below the above range, the effect of the addition of (B) hardly occurs, which is not preferable.
- the properties of the graphite powder (A) (or the graphite powder (C)) are impaired, which is also preferable.
- the carbon material (B) a material selected from natural graphite, artificial graphite, amorphous-coated graphite, resin-coated graphite and amorphous carbon is used. These materials may be used alone or in any combination of two or more in any combination and composition.
- natural graphite for example, highly purified scaly graphite or spherical graphite can be used.
- the volume-based average particle size of natural graphite is usually 8 m or more, preferably 12 m or more, and usually 60 ⁇ m or less, preferably 40 ⁇ m or less.
- the BET specific surface area of natural graphite is usually in the range of 4 m 2 Zg or more, preferably 4.5 m 2 Zg or more, usually 7 m 2 Zg or less, preferably 5.5 m 2 Zg or less.
- artificial graphite for example, particles obtained by compounding Cotus powder or natural graphite with a binder, particles obtained by firing single black ship precursor particles in powder state, or the like can be used.
- amorphous coated graphite for example, particles obtained by coating natural graphite or artificial graphite with an amorphous precursor and firing the particles, or particles obtained by coating natural graphite or an artificial graphite with amorphous by CVD are used. It is possible to
- the resin-coated graphite for example, particles obtained by coating natural graphite or artificial graphite with a polymer material and drying it can be used.
- amorphous carbon for example, particles obtained by firing a noble mesophase or particles obtained by subjecting a carbon precursor to infusiblization treatment and firing can be used.
- carbon materials (b) and ⁇ ⁇ ) selected from the group consisting of
- binder constituting the carbon material (b) petroleum-based and coal-based condensed polycyclic aromatic compounds having a soft pitch power up to a hard pitch are preferable, as long as they are carbonaceous materials capable of graphitizing. There is no particular limitation.
- natural graphite particles constituting the carbon material (b) for example, highly purified scaly black lead or spherical graphite can be used.
- the volume-based average particle size of natural graphite is usually 10 ⁇ m or more, preferably 12 ⁇ m or more, and usually 50 ⁇ m or less, preferably 30 ⁇ m or less.
- the BET specific surface area of natural graphite is usually 4 m 2 Zg or more, preferably 4.5 m 2 / g or more, and usually 10 m 2 / g or less, preferably 6 m 2 / g or less.
- the ratio of the carbon material (b) to the total amount of the graphite powder (A) (or graphite powder (C)) and the carbon material (b) is The content is usually 10% by weight or more, preferably 30% by weight or more, more preferably 50% by weight or more, most preferably 60% by weight or more, and usually 90% by weight or less, more preferably 80% by weight or less.
- the total of them should be within the above range.
- carbon material (B) When mixing carbon material (B) with graphite powder (A) (or graphite powder (C)), carbon material
- (B) There is no particular limitation on the selection of (B), but, for example, by mixing, it is possible to improve cycle characteristics and charge acceptance by improving conductivity, to reduce irreversible capacity, and to improve pressability. It is possible to select a carbon material (B) that can be improved depending on the case.
- An apparatus used for mixing the graphite powder (A) (or the graphite powder (C)) and the carbon material (B) is not particularly limited, but in the case of, for example, a rotary mixer: a cylindrical mixer, In the case of twin cylindrical mixer, double cone mixer, regular cubic mixer, vertical mixer, fixed mixer: spiral mixer, ribbon mixer, Muller mixer, HelicalFlight type A mixer, a Pug mill mixer, a fluidizing mixer, etc. can be used.
- the above-described negative electrode material of the present invention (graphite powder (A) or graphite powder (C), or a mixture of these graphite powder and carbon material (B)) is a positive electrode capable of absorbing and releasing lithium ions. And a negative electrode, and a lithium secondary battery provided with an electrolytic solution, preferably used as a material of the negative electrode.
- the negative electrode material of the present invention even when used at a high electrode density, the load capacity at the time of forming the electrode is small, the discharge capacity is high, and the charge / discharge efficiency is high. Thus, it is possible to obtain a lithium secondary battery excellent in balance with various battery performances, such as a small amount of gas generation.
- heat treatment is performed using natural graphite having physical properties in a predetermined range as a raw material, so the number of steps can be reduced. It can be manufactured and is very useful industrially.
- selection of the necessary members There is no particular limitation on the selection of the necessary members.
- the details of the negative electrode for a lithium secondary battery and the lithium secondary battery using the negative electrode material of the present invention will be exemplified below, but materials that can be used, methods of manufacturing, etc. are limited to the following specific examples. .
- a negative electrode for lithium secondary battery By forming a layer (negative electrode layer) containing the negative electrode material of the present invention as an active material on a current collector, a negative electrode for lithium secondary battery can be produced.
- the negative electrode may be produced according to a conventional method. For example, a binder, a thickener, a conductive material, a solvent, and the like are added to a negative electrode active material (the negative electrode material of the present invention) to form a slurry, which is coated on a current collector, dried and pressed to obtain high density. Ways to As the negative electrode active material, the present invention These negative electrode materials may be used alone, or may be used together with other active materials.
- the density of [0099] active material layer is usually 1. 40gZcm 3 or more, preferably 1. 50gZcm 3 or more, more favorable Mashiku is When 1. 60gZcm 3 or more ranges, preferred because the capacity of the battery increases.
- the active material layer is a layer formed of an active material, a binder, a conductive agent and the like on the current collector, and the density thereof is the density at the time of assembly into a battery.
- any material can be used as long as it is a material stable to the solvent and the electrolyte used in electrode production.
- poly (vinyl fluoride), polytetrafluoroethylene, polyethylene, polypropylene, styrene 'butadiene rubber (SBR), isopropyl rubber, butadiene rubber, ethylene acrylic acid copolymer, ethylene methacrylic acid copolymer and the like can be mentioned. These may be used alone or in combination of two or more in any combination and ratio.
- any known one may be optionally selected and used.
- CMC carboxinolemethinoresenoresulose
- methinoresenorelos methinoresenorelos
- hydroxymethinoresenorelos ethylcellulose
- Polybutyl alcohol oxidized starch
- phosphorylated starch phosphorylated starch and casein etc.
- the conductive material may, for example, be a metal material such as copper or nickel; or a carbon material such as graphite or carbon black. These may be used alone or in combination of two or more in any combination and ratio.
- the material of the current collector for the negative electrode may, for example, be copper, nickel or stainless steel.
- copper foil is preferred in view of easy processing into a thin film and cost. These may be used alone or in combination of two or more in any combination and ratio.
- a lithium secondary battery can be formed by combining the above-described negative electrode for a lithium secondary battery with a positive electrode capable of absorbing and desorbing lithium, and an electrolyte.
- the method for producing the positive electrode is not particularly limited, and the method for producing the positive electrode is the same as the method for producing the negative electrode described above. It can manufacture by forming the layer (positive electrode layer) containing a positive electrode active material on a collector.
- Examples of the material of the positive electrode active material include lithium transition metal complex oxide materials such as lithium complex oxide, lithium nickel oxide, lithium manganese oxide and the like; diacid manganese Materials capable of absorbing and desorbing lithium such as transition metal oxide materials such as carbonaceous materials such as fluorinated graphite can be used.
- lithium transition metal complex oxide materials such as lithium complex oxide, lithium nickel oxide, lithium manganese oxide and the like
- diacid manganese Materials capable of absorbing and desorbing lithium such as transition metal oxide materials such as carbonaceous materials such as fluorinated graphite can be used.
- MnO and non-stoichiometric compounds thereof MnO, TiS, FeS, Nb S, Mo S, CoS,
- V 2 O, P 2 O, CrO, V 2 O, TeO, GeO or the like can be used.
- valve metals metals belonging to IIIb, IVa, Va group (3B, 4A, 5A) and their alloys can be exemplified.
- Al, Ti, Zr, Hf, Nb, Ta and alloys containing these metals can be exemplified, and Al, Ti, Ta and alloys containing these metals can be preferably used.
- A1 and its alloys are lightweight and high in energy density and desirable.
- any electrolyte such as an electrolytic solution or a solid electrolyte can be used.
- electrolyte refers to all of the ion conductors, and the electrolyte, the electrolyte and the solid electrolyte are both included in the electrolyte.
- the electrolytic solution for example, one in which a solute is dissolved in a non-aqueous solvent can be used.
- alkali metal salts As the solute, alkali metal salts, quaternary ammonium salts and the like can be used. Specifically, LiCIO, LiPF, LiBF, LiCFSO, LiN (CF3SO4), LiN (CF2CF2SO4)
- non-aqueous solvent for example, cyclic carbonates such as ethylene carbonate, propylene carbonate, butylene carbonate and vinyl carbonate, cyclic ester compounds such as y-butyrolactone, etc .; Chain ethers; cyclic ethers such as crown ether, 2-methyltetrahydrofuran, 1,2 dimethyltetrahydrofuran, 1,3 dioxsolane, tetrahydrofuran, etc .; linear carbonates such as jetyl carbonate, ethyl methyl carbonate, dimethyl carbonate, etc. it can.
- the solute and the solvent may be used alone or in combination of two or more.
- non-aqueous solvents containing cyclic carbonate and linear carbonate are preferable.
- the non-aqueous electrolytic solution may contain an organic polymer compound in the electrolytic solution to form a gel-like or rubber-like or solid sheet-like solid electrolyte.
- organic polymer compound include polyether polymers such as polyethylene oxide and polypropylene oxide; cross-linked polymers of polyether polymers; and polymers such as polyvinyl alcohol and polyvinyl butyral.
- Alcohol-based polymer compounds Insolubilized products of bule alcohol-based polymer compounds; polyepichlorohydrin; polyphosphazene; polysiloxanes; polybole-based polymer compounds such as polypyrrole pyrrolidone, polybi-idene carbonate, polyacrylonitrile and the like; Polymer copolymers such as poly ( ⁇ -methoxyorganoethylene methacrylate), poly ( ⁇ -methoxy oligoethylene methacrylate) methyl methacrylate, and the like can be mentioned.
- an outer can, a separator, a gasket, a sealing plate, a cell case, and the like can be used as the lithium secondary battery, as necessary.
- the material and shape of the separator are not particularly limited.
- the separator separates the positive electrode and the negative electrode so that they do not physically contact each other, and preferably has high ion permeability and low electrical resistance.
- the separator is preferably selected from materials which are stable to the electrolyte and have excellent liquid retention.
- the above-mentioned electrolytic solution can be impregnated using a porous sheet or non-woven fabric made of polyolefin such as polyethylene and polypropylene as a raw material.
- the negative electrode is placed on the outer can, the electrolytic solution and the separator are provided on the outer can, and the positive electrode is placed to face the negative electrode.
- the battery can be made tight together with the mouth plate.
- the shape of the battery is not particularly limited.
- a cylinder type having a spiral sheet electrode and separator a cylinder type having an inside-out structure combining a pellet electrode and a separator, a coin type having a pellet electrode and a separator laminated, etc. It is possible to Example
- Spheronization treatment at 6500 rpm for 5 minutes, and then 45% by weight of fine powder is removed using a pneumatic classifier (OMC-100 made by Seishin Co., Ltd.), volume-based average particle size ( median diameter) 17 ⁇ m, tap density Spheroidized graphite powder with a specific surface area of 7.5 g / cm 3 and a BET specific surface area of 7.5 m 2 / g was obtained.
- the classified spheroidized graphite powder is packed in a graphite crucible, and graphitized at 3000 ° C. for 5 hours in an inert atmosphere using a direct current furnace to obtain graphite powder (negative electrode material of Example 1) Got)
- the physical properties of the negative electrode material of Example 1 obtained were measured, and the median diameter was 17 m, d / ⁇ .
- an electrode having an electrode density of 1. 63 ⁇ 0. 05 gZcm 3 was produced according to the following method, and the active material orientation ratio of the electrode was determined. Met.
- the press load at the time of electrode formation was 60 kg.
- a lithium secondary battery was produced according to the following method, and the discharge capacity, charge / discharge efficiency, and load characteristics were measured. Similarly, a lithium secondary battery is fabricated, disassembled in the charged state, and the thickness of the electrode is measured to obtain the charge expansion coefficient. The measurements were taken.
- Weight of negative electrode active material (weight of electrode) (weight of copper foil) (weight of binder)
- press load line pressure
- the press load load per 1 cm width of electrode at the time of electrode formation was determined.
- EC ethylene carbonate
- DEC Z jetyl carbonate
- a coin battery (lithium secondary battery) was produced using a polyethylene separator as a capacitor and a lithium metal counter electrode as a counter electrode.
- the charge termination condition of the 4th cycle was carried out with a constant capacity charge of 300 mAh Zg.
- the charged coin battery was disassembled so as not to short-circuit in an argon glove box, the electrode was taken out, and the thickness of the electrode (excluding copper foil) at the time of charging was measured. Based on the thickness (excluding copper foil) of the press electrode before battery preparation, the charge expansion coefficient was determined based on the following equation.
- Example 1 a lithium secondary battery was produced according to the following method, and the amount of gas generation was measured.
- This slurry was applied onto a copper foil using a doctor blade in the same manner as in the above-described electrode production method.
- the coating thickness was selected so that the electrode basis weight (excluding copper foil) after drying was 15 mg / cm 2 .
- Weight of negative electrode active material (weight of electrode) (weight of copper foil) (weight of binder) ⁇ Method of Producing Lithium Secondary Battery for Measurement of Gas Generation>
- a lithium secondary battery was manufactured according to the same procedure as that of the above-described lithium secondary battery, except that an assembled cell having a constant cell volume with a valve was used instead of the coin battery.
- OMC-100 manufactured by Seishin Enterprise Co., Ltd.
- the classified spheroidized graphite powder was heat treated in the same manner as in Example 1, and the physical properties of the negative electrode material of Example 2 obtained were measured.
- the active material orientation ratio of the electrode was determined. Met.
- the press load at the time of electrode formation was 40 kg.
- a lithium secondary battery is manufactured in the same manner as in Example 1 using the negative electrode material of Example 2, and measurement of discharge capacity, charge / discharge efficiency, load characteristics, charge expansion coefficient, and gas generation amount is performed.
- a classifier OMC-100, manufactured by Seishin Enterprise Co., Ltd.
- 20% by weight fine powder was removed to obtain a spheroidized graphite powder having a median diameter of 22 m, a tap density of 0.9 g Z cm 3 , and a BET specific surface area of 5.8 m 2 Z g .
- the values of median diameter, tap density, and BET specific surface area were measured using the method described above.
- Example 3 The classified spheroidized graphite powder was heat-treated in the same manner as in Example 1, and the physical properties of the negative electrode material of Example 3 obtained were measured.
- a median diameter of 22 / zmd / ⁇ 2. 7, a tap density 0
- the active material orientation ratio of the electrode was determined using the negative electrode material of Example 3, and found to be 0.03.
- the press load at the time of electrode formation was 36 kg.
- a lithium secondary battery is manufactured in the same manner as in Example 1 using the negative electrode material of Example 3, and measurement of discharge capacity, charge and discharge efficiency, load characteristics, charge expansion coefficient, and gas generation amount is performed.
- Example 4 The same treatment as in Example 1 is performed except that the heat treatment temperature of the spheroidized graphite powder is set to 2000 ° C. It was The physical properties of the negative electrode material of Example 4 obtained were measured, and the median diameter was 17 m, d
- the active material orientation ratio of the electrode was calculated to be 0.5.
- the press load at the time of electrode formation was 62 kg.
- Example 4 Furthermore, a lithium secondary battery was produced in the same manner as in Example 1 using the negative electrode material of Example 4, and the discharge capacity, charge and discharge efficiency, load characteristics, charge expansion coefficient, and gas generation amount were measured. The evaluation results of the physical properties of the negative electrode material of Example 4 are shown in Table 1.
- the physical properties of the negative electrode material of Example 5 obtained by mixing were measured.
- the median diameter 19 m, d / ⁇ 2.5, tap density 1.0 g Z cm 3 , surface functional group weight OZC value 0. 015 , BET
- Example 5 when the negative electrode material of Example 5 was used to determine the active material orientation ratio of the electrode, it was 0.004.
- the press load at the time of electrode formation was 48 kg.
- Example 5 Furthermore, a lithium secondary battery was produced in the same manner as in Example 1 using the negative electrode material of Example 5, and the discharge capacity, charge and discharge efficiency, load characteristics, charge expansion coefficient, and gas generation amount were measured. The evaluation results of the physical properties of the negative electrode material of Example 5 are shown in Table 1.
- Example 6 Heat treatment and anode material 40 weight 0/0 of Example 2, the median diameter 13 m, tap density 1. Og / cm 3, spheroidized natural graphite powder as the BE T specific surface area 7. 5 m 2 Zg is a petroleum soft pitch
- a negative electrode material of Example 6 was obtained by mixing 60% by weight of a carbon material (b) obtained by coating the whole or a part of the carbon material.
- the physical properties of the negative electrode material of Example 6 obtained were measured, and the median diameter was 18 m, d / ⁇ .
- the product was 2.6 m 2 Zg, Raman R value 0.09, and Raman half width was 21.5 cm_1 .
- the median diameter, tap density, BET specific surface area, surface functional group amount OZC value, Raman R value, Raman half value width, and circularity were values measured by the method described above.
- the active material orientation ratio of the electrode was determined using the negative electrode material of Example 6, and found to be 0.5.
- the press load at the time of electrode formation was 70 kg.
- Example 6 Furthermore, using the negative electrode material of Example 6, a lithium secondary battery was produced in the same manner as in Example 1.
- the electrode preparation was performed using the negative electrode material of Comparative Example 1, it becomes an uneven film at the time of coating, and peeling from a copper foil after pressing makes it impossible to obtain battery characteristics. To the end of the day.
- Natural graphite (ash content: 0.5% by weight) having a median diameter of 20 m, a tap density of 0.75 g Z cm 3 , and a BET specific surface area of 3 m 2 Z g which had been highly purified and treated as in Example 1 without being spheroidized. Heat-treated.
- the active material orientation ratio of the electrode was determined using the negative electrode material of Comparative Example 2, it was 0.2.
- the press load at the time of electrode formation was 30 kg.
- a lithium secondary battery is produced using the negative electrode material of Comparative Example 2 in the same procedure as in Example 1, and measurement of discharge capacity, charge / discharge efficiency, load characteristics, charge expansion coefficient, and gas generation amount is performed. became.
- Example 2 The same treatment as in Example 1 was carried out except that the heat treatment temperature of the spheroidized graphite powder was changed to 1200.degree.
- the physical properties of the negative electrode material of Comparative Example 3 obtained were measured, and the median diameter was 17 m, d
- the active material orientation ratio of the electrode was determined using the negative electrode material of Comparative Example 3 to be 0.5.
- the press load at the time of electrode formation was 58 kg.
- a lithium secondary battery is manufactured using the negative electrode material of Comparative Example 3 in the same procedure as in Example 1, and measurement of discharge capacity, charge / discharge efficiency, load characteristics, charge expansion coefficient, and gas generation amount is performed.
- Example 2 The same process as in Example 1 was performed except that the heat treatment of the spheroidized graphite powder was not performed.
- the physical properties of the negative electrode material of Comparative Example 4 obtained were measured, and the median diameter was 17 m, d / ⁇ .
- the active material orientation ratio of the electrode was determined using the negative electrode material of Comparative Example 4 to be 0.5.
- the press load at the time of electrode formation was 56 kg.
- Spherical artificial graphite (mesocarbon single microbeads) was heat treated in the same manner as in Example 1 instead of graphite powder obtained by spheroidizing scaly natural graphite.
- the active material orientation ratio of the electrode was determined using the negative electrode material of Comparative Example 5 to be 0.12.
- the press load at the time of electrode formation was 400 kg.
- Example 1 a lithium secondary battery was produced in the same manner as in Example 1 using the negative electrode material of Comparative Example 5, and the discharge capacity, charge / discharge efficiency, load characteristics, charge expansion coefficient, and gas generation amount were measured.
- the evaluation results of the physical properties of the negative electrode material of Comparative Example 5 are shown in Table 1.
- the heat-treated spheroidized graphite powder obtained in Example 1 was subjected to oxidation treatment with ozone gas to obtain a negative electrode material of Comparative Example 6.
- the physical properties of the negative electrode material of Comparative Example 6 obtained were measured.
- the median diameter, tap density, BET specific surface area, surface functional group amount OZC value, Raman R value, Raman half value width, and circularity were measured using the method described above.
- the surface functional group amount OZC value, BET specific surface area, and Raman R value are included in the defined range of the present invention, but the tap density is lower than the defined range of the present invention, As a result, the charge expansion rate at which the load characteristics are low is also large.
- the tap density, the surface functional group amount OZC value, and the BET specific surface area are included in the specified range of the present invention, and the Raman R value is within the specified range of the present invention because the heat treatment temperature is low. As a result, the amount of gas generation is large.
- the surface functional group amount OZC value, BET specific surface area, and Raman R value of the present invention were obtained because the tap density was not subjected to the force heat treatment contained in the specified range of the present invention. It exceeds the specified range, and as a result, the amount of gas generation to lower the charge and discharge efficiency is large, and the load characteristics are also low.
- the tap density, the BET specific surface area, and the Raman R value are included in the specified range of the present invention, but the surface functional group weight OZC value exceeds the specified range of the present invention, As a result, the amount of gas generation is large.
- the negative electrode materials of Examples 1 to 4 all of the tap density, Raman R value, surface functional group weight OZC value, and BET specific surface area satisfy the specified range of the present invention.
- the press load at the time of electrode formation decreases, and the produced battery exhibits high discharge capacity, and the charge expansion coefficient and gas generation amount of the electrode also have high charge / discharge efficiency and load characteristics. It is kept low.
- the press load at the time of electrode formation is small.
- the manufactured battery exhibits a high discharge capacity, and the charge expansion coefficient of the electrode and the amount of gas generation, which also increase the charge and discharge efficiency and the load characteristics, are suppressed to a low level.
- the negative electrode material for a lithium secondary battery of the present invention even when used at a high electrode density, a load characteristic in which the press load at the time of electrode formation decreases and the discharge capacity increases and the charge and discharge efficiency increases. It is possible to realize a lithium secondary battery that is excellent in various battery performances with a good balance, such as low expansion of the battery at the time of battery charging, and a small amount of gas generation. And so on.
- the above-described negative electrode material for a lithium secondary battery can be stably and efficiently produced at low cost. In the industrial production field, its value is great.
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Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US11/630,470 US8637187B2 (en) | 2004-06-30 | 2005-06-24 | Negative electrode material for lithium secondary battery, method for producing same, negative electrode for lithium secondary battery using same and lithium secondary battery |
EP05765121.8A EP1775785B1 (en) | 2004-06-30 | 2005-06-24 | Negative electrode material for lithium secondary battery, method for producing same, negative electrode for lithium secondary battery using same and lithium secondary battery |
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US (1) | US8637187B2 (ja) |
EP (1) | EP1775785B1 (ja) |
JP (2) | JP5082207B2 (ja) |
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CN111732096A (zh) * | 2019-03-25 | 2020-10-02 | 中信国安盟固利动力科技有限公司 | 一种高功率锂离子电池的负极材料及其制备方法 |
CN114572978A (zh) * | 2022-03-16 | 2022-06-03 | 江西紫宸科技有限公司 | 一种高倍率石墨负极材料的制备方法、负极材料和锂电池 |
CN114572978B (zh) * | 2022-03-16 | 2024-01-26 | 江西紫宸科技有限公司 | 一种高倍率石墨负极材料的制备方法、负极材料和锂电池 |
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Publication number | Publication date |
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JP5082207B2 (ja) | 2012-11-28 |
EP1775785A4 (en) | 2011-11-09 |
US20080274406A1 (en) | 2008-11-06 |
KR100826890B1 (ko) | 2008-05-06 |
EP1775785A1 (en) | 2007-04-18 |
CN1981393A (zh) | 2007-06-13 |
US8637187B2 (en) | 2014-01-28 |
EP1775785B1 (en) | 2013-08-21 |
JP5561232B2 (ja) | 2014-07-30 |
CN100464446C (zh) | 2009-02-25 |
JP2006049288A (ja) | 2006-02-16 |
KR20070026786A (ko) | 2007-03-08 |
JP2011181505A (ja) | 2011-09-15 |
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