Source: http://www.freshpatents.com/-dt20110106ptan20110003206.php
Timestamp: 2013-05-18 11:51:23
Document Index: 80879656

Matched Legal Cases: ['art, 3', 'arts 2', 'arts 50', 'art 50', 'arts 50', 'art 50', 'art 50', 'arts 50', 'arts 2', 'arts 50', 'art 50']

Positive Electrode Active Element And Lithium Secondary Battery 1 views for this patent on FreshPatents.comupdated 05/17/13
Patents sorted by company.	01/06/11 | Class 429 Monitor | RSS | Browse: Prev - Next Positive electrode active element and lithium secondary battery Abstract: A positive electrode active material having a specific surface area of 0.1 to 0.5 m2/g, which contains a large number of crystal grains containing primary particles of 5 to 20 μm in particle diameter, composed of lithium manganate of spinel structure containing lithium and manganese as the constituent elements, and a bismuth compound containing bismuth, wherein the proportion of the primary particles contained in the large number of crystal grains is 70 areal % or more and the proportion of the bismuth contained in the bismuth compound is 0.005 to 0.5 mol % relative to the manganese contained in the lithium manganate. ...
Agent: Burr & Brown - Syracuse, NY, USInventors: Yukinobu YURA, Nobuyuki KOBAYASHI, Tsutomu NANATAKI, Kazuyuki KAIGAWAUSPTO Applicaton #: #20110003206 - Class: 429224 (USPTO) - 01/06/11 - Class 429 Related Terms: Bismuth The Patent Description & Claims data below is from USPTO Patent Application 20110003206, Positive electrode active element and lithium secondary battery.
The present invention relates to a positive electrode active material and a lithium secondary battery. More particularly, the present invention relates to a positive electrode active material usable for production of a lithium secondary battery improved in cycle characteristics at high temperatures, and a lithium secondary battery improved in cycle characteristics at high temperatures.
As the positive electrode active material of lithium secondary battery, there are known lithium cobaltate of layered rock salt structure, lithium nickelate of layered rock salt structure, lithium manganate of spinel structure, etc. Lithium cobaltate of layered rock salt structure is unstable in supply because the reserve of cobalt is small and the cobalt-producing regions are unevenly distributed. Also, lithium nickelate of layered rock salt structure has a problem of unstable structure under charging condition.
Lithium manganate of spinel structure, as compared with lithium cobaltate of layered rock salt structure and lithium nickelate of layered rock salt structure, is known to be high in safety as well as rate characteristics and low in cost. The lithium manganate of spinel structure, however, generally has problems of deterioration in properties at high temperatures such as reduction in cycle characteristics at high temperatures, deterioration in storage property at high temperatures, and the like. In order to improve the cycle characteristics at high temperatures, there is disclosed a positive electrode active material for lithium secondary battery, characterized by being composed of a mixture of a chalcogen compound of at least one element selected from the element group consisting of Ge, Sn, Pb, In, Sb, Bi and Zn and a Li—Mn-based composite oxide (see, for example, JP-A-10-302767).
In order to achieve a superior filling property, a high initial capacity and a high capacity maintenance factor, is also disclosed a positive electrode active material for lithium ion secondary cells mainly containing an Li—Mn composite oxide particles having a spinel structure wherein the average of the porosity of the particles represented by a particular expression is 15% or less (see, for example, WO 2001/004975). In the WO 2001/004975, it is disclosed that, in the positive electrode active material for lithium ion secondary cells, the average particle diameter of primary particles is restricted preferably at 3 μm or less in order to maintain the average of the porosity of the particles at 15% or less.
In conventional positive electrode active materials for lithium secondary battery using lithium manganate, the cycle characteristics at high temperatures when used in lithium secondary battery is not sufficient and further improvement therefor is required.
The present invention has been made in view of the above-mentioned problem of the prior art. The present invention has an object of providing a positive electrode active material which is usable for production of a lithium secondary battery improved in cycle characteristics at high temperatures.
The present inventors made an extensive study in order to achieve the above object. As a result, it was found that the above object could be achieved by allowing a positive electrode active material to contain a large number of crystal grains which contain primary particles of particle diameters specified in a given numerical range and a bismuth compound, and further to have a specific surface area controlled in a particular numerical range. The finding has led to the completion of the present invention.
The present invention provides a positive electrode active material and a lithium secondary battery, both shown below.
[1] A positive electrode active material having a specific surface area of 0.1 to 0.5 m2/g, which contains a large number of crystal grains containing primary particles of 5 to 20 μm in particle diameter, composed of lithium manganate of spinel structure containing lithium and manganese as the constituent elements, and a bismuth compound containing bismuth, wherein the proportion of the primary particles contained in the large number of crystal grains is 70 areal % or more and the proportion of the bismuth contained in the bismuth compound is 0.005 to 0.5 mol % relative to the manganese contained in the lithium manganate.
[2] The positive electrode active material according to [1], wherein the value of a lattice strain (η) in powder X-ray diffraction pattern is 0.7×10−3 or less.
[3] The positive electrode active material according to [1], wherein the bismuth compound is a compound of bismuth and manganese.
[4] The positive electrode active material according to [2], wherein the bismuth compound is a compound of bismuth and manganese.
[5] The positive electrode active material according to [3], wherein the compound of bismuth and manganese is Bi2Mn4O10.
[6] The positive electrode active material according to [4], wherein the compound of bismuth and manganese is Bi2Mn4O10.
[7] The positive electrode active material according to [1], wherein the large number of crystal grains contain single particles by 40 areal % or more.
[8] The positive electrode active material according to [2], wherein the large number of crystal grains contain single particles by 40 areal % or more.
[9] The positive electrode active material according to [3], wherein the large number of crystal grains contain single particles by 40 areal % or more.
[10] The positive electrode active material according to [1], wherein the large number of crystal grains further contain secondary particles formed by mutual connection of a plurality of the primary particles.
[11] The positive electrode active material according to [2], wherein the large number of crystal grains further contain secondary particles formed by mutual connection of a plurality of the primary particles.
[12] The positive electrode active material according to [3], wherein the large number of crystal grains further contain secondary particles formed by mutual connection of a plurality of the primary particles.
[13] The positive electrode active material according to [1], wherein the bismuth compound is present on at least either of the surfaces of the primary particles or the particle boundary parts where a plurality of the primary particles are connected to each other.
[14] The positive electrode active material according to [2], wherein the bismuth compound is present on at least either of the surfaces of the primary particles or the particle boundary parts where a plurality of the primary particles are connected to each other.
[15] The positive electrode active material according to [3], wherein the bismuth compound is present on at least either of the surfaces of the primary particles or the particle boundary parts where a plurality of the primary particles are connected to each other.
[16] A lithium secondary battery which has an electrode body comprising a positive electrode containing a positive electrode active material according to [1] and a negative electrode containing a negative electrode active material.
[17] A lithium secondary battery which has an electrode body comprising a positive electrode containing a positive electrode active material according to [2] and a negative electrode containing a negative electrode active material.
[18] A lithium secondary battery which has an electrode body comprising a positive electrode containing a positive electrode active material according to [3] and a negative electrode containing a negative electrode active material.
The positive electrode active material of the present invention is usable for production of a lithium secondary battery improved in cycle characteristics at high temperatures.
The lithium secondary battery of the present invention is improved in cycle characteristics at high temperatures.
FIG. 1 is a perspective view showing an example of the state in which a plurality of primary particles are connected to each other.
FIG. 2 is a perspective view showing other example of the state in which a plurality of primary particles are connected to each other.
FIG. 3 is a sectional view showing an embodiment of the lithium secondary battery of the present invention.
FIG. 4 is a schematic view showing an example of the electrode body constituting other embodiment of the lithium secondary battery of the present invention.
FIG. 5A is an electron micrograph showing an embodiment of a large number of crystal grains according to the positive electrode active material of the present invention.
FIG. 5B is an electron micrograph showing other embodiment of a large number of crystal grains according to the positive electrode active material of the present invention.
FIG. 5C is an electron micrograph showing still other embodiment of a large number of crystal grains according to the positive electrode active material of the present invention.
FIG. 5D is an electron micrograph showing still other embodiment of a large number of crystal grains according to the positive electrode active material of the present invention.
FIG. 6A is a schematic view showing a state in which crystal grains adhere to each other in a cross-section of the positive electrode active material of the present invention.
FIG. 6B is a schematic view showing a state in which crystal grains adhere to each other in a cross-section of the positive electrode active material of the present invention.
FIG. 6C is a schematic view showing a state in which crystal grains adhere to each other in a cross-section of the positive electrode active material of the present invention.
FIG. 6D is a schematic view showing a state in which crystal grains adhere to each other in a section of the positive electrode active material of the present invention.
1: primary particle, 2: particle boundary part, 3: crystal face, 4: battery case, 5: insulation gasket, 6: separator, 7: core, 8: bismuth compound, 10, 20, 30: secondary particle, 11: lithium secondary battery, 12: positive electrode plate, 13: negative electrode plate, 14: positive electrode layer, 15: positive electrode collector, 16: negative electrode layer, 17: negative electrode collector, 18: positive electrode side container, 19: negative electrode side container, 21: electrode body, 22: tab for positive electrode, 23: a tab for negative electrode, 31 to 38: crystal grain, 40: single particle, 41 to 43: fine particle, 50a to 50 g: adhesion part (a particle boundary part).
The embodiment of the present invention is described below. However, the present invention is in no way restricted to the following embodiment. It should be construed that appropriate changes, improvements, etc. can be added to the following embodiment based on the ordinary knowledge possessed by those skilled in the art as long as there is no deviation from the gist of the present invention and that the resulting embodiments as well fall in the scope of the present invention.
I. Positive Electrode Active Material
The positive electrode active material of the present invention contains a large number of crystal grains which contain primary particles of 5 to 20 μm in particle diameter, composed of lithium manganate of spinel structure containing lithium and manganese as the constituent elements and a bismuth compound, and the specific surface area of the positive electrode active material is 0.1 to 0.5 m2/g.
1. Primary Particles
The primary particles are particles of 5 to 20 μm in particle diameter, composed of lithium manganate of spinel structure containing lithium and manganese as the constituent elements.
The chemical formula of lithium manganate is ordinarily represented by LiMn2O4. In the positive electrode active material of the present invention, however, there can be used, in addition to lithium manganate of the above chemical formula, lithium manganate represented by, for example, the following general formula (I), as long as it has a spinel structure.
LiMxMn2-xO4 (1)
In the general formula (1), M is at least one kind of element (substituting element) selected from the group consisting of Li, Fe, Ni, Mg, Zn, Al, Co, Cr, Si, Sn, P, V, Sb, Nb, Ta, Mo and W. The substituting element may further include Ti, Zr and Ce, in addition to the above-mentioned at least one kind of element. X is the substituting number of the substituting element M. Li becomes + mono-valent ion; Fe, Mn, Ni, Mg and Zn each become + bi-valent ion; B, Al, Co and Cr each become + tri-valent ion; Si, Ti, Sn, Zr and Ce each become + tetra-valent ion; P, V, Sb, Nb and Ta each become + penta-valent ion; Mo and W each become + hexa-valent ion; and all these elements are present theoretically in LiMn2O4 in the form of solid solution. Incidentally, Co and Sn may take + bi-valency; Fe, Sb and Ti may take + tri-valency; Mn may take + tri- and + tetra-valencies; and Cr may take + tetra- and + hexa-valencies. Therefore, the substituting element M may be present in a state of mixed valencies. The number of oxygen atoms need not be absolutely 4 and may be excessive or insufficient as long as the required crystal structure can be secured.
The crystal grains may be particles composed of lithium manganate (e.g. LiNi0.5Mn1.5O4) in which 25 to 55 mol % of the total Mn is substituted by Ni, Co, Fe, Cu, Cr or the like. The positive electrode active material obtained by using such a lithium manganate allows production of a lithium secondary battery which is superior in high-temperature cycle characteristics as well as in rate characteristics and which further has a high charge-discharge potential and a high energy density. Therefore, it allows production of a lithium secondary battery having an electromotive force of 5 V level.
The particle diameters of the primary particles are 5 to 20 μm, preferably 7 to 20 μm, more preferably 10 to 20 μm. When the particle diameters of the primary particles are not within this range, there may be a reduction in cycle characteristics. The reason therefor is uncertain but is considered to be as follows. That is, when the particle diameters are smaller than 5 μm, Mn ion dissolves into electrolytic solution easily; meanwhile, when the particle diameters are larger than 20 μm, cracks appear easily in the particles owing to the stress caused by the volume change of particles during charge-discharge, which incurs an increase in internal resistance.
Incidentally, the particle diameters are a value specified as follows. First, a positive electrode active material powder is placed on a carbon tape so that there is no piling of particles; Au is sputtered thereon in a thickness of about 10 nm using an ion sputtering apparatus (JFC-1500 (trade name), a product of JEOL Ltd.); then, a secondary electron image of particles is taken, using a scanning electron microscope (JSM-6390 (trade name), a product of JEOL Ltd.), by selecting such a display magnification that 20 to 50 primary particles each having the maximum diameter of 5 μm or larger are seen in the visual field. For each primary particle in the image obtained, there is calculated an average of the maximum diameter of the particle part not hidden by other particles and the largest diameter of the diameters at right angles to the above maximum diameter, and the average is taken as the particle diameter (μm) of the primary particle. In this way, particles diameters are measured for all primary particles excluding the particles which are hidden by other particles and are uncalculable.
The proportion of the primary particles of 5 to 20 μm in particle diameter is 70 areal % or more, preferably 80 areal % or more, more preferably 90 areal % or more, relative to the area (100 areal %) occupied by all the crystal grains whose particle diameters are measurable as mentioned above. Incidentally, the proportion of the primary particles of 5 to 20 μm in particle diameter can be calculated, for example, by measuring the area (A) occupied by all the crystal grains whose particle diameters are measurable and the area (a) occupied by the primary particles of 5 to 20 μm in particle diameter, using an image edit software (“Photoshop” (trade name), a product of Adobe Systems Incorporated) and substituting them into an expression (a/A)×100.
2. Bismuth Compound
The proportion of bismuth contained in the bismuth compound is 0.005 to 0.5 mol %, preferably 0.01 to 0.2 mol %, more preferably 0.01 to 0.1 mol %, relative to the manganese contained in the lithium manganate. When the proportion is smaller than 0.005 mol %, there may be a reduction in cycle characteristics at high temperatures. Meanwhile, when the proportion is larger than 0.5 mol %, there may be a reduction in initial capacity. Incidentally, the proportion of bismuth can be obtained by quantitatively determining lithium, manganese and bismuth using an ICP (inductively coupled plasma) optical emission spectrometer (“ULTIMA 2” (trade name), a product of HORIBA, Ltd.) and making calculation using the results of the determination.
The bismuth compound includes, for example, bismuth oxide and a compound of bismuth and manganese. The bismuth compound is preferably a compound of bismuth and manganese. As the compound of bismuth and manganese, there can be specifically mentioned compounds represented by chemical formulas of Bi2Mn4O10 and Bi12MnO20. Of these, a compound represented by a chemical formula of Bi2Mn4O10 is preferred particularly. Incidentally, the bismuth compound can be identified by X-ray diffraction measurement (hereinafter, this is referred to also as “XRD”) or by electron probe microanalysis (hereinafter, this is referred to also as “EPMA”).
FIG. 5A to FIG. 5D are each an electron micrograph showing an embodiment of a large number of crystal grains according to the positive electrode active material of the present invention. It is presumed that the bismuth compound, particularly the compound of bismuth and manganese suppresses the dissolution of Mn from the surface of each primary particle or from the particle boundary parts of a plurality of primary particles connected to each other to improve cycle characteristics effectively. Therefore, it is preferred that, as shown in FIG. 5A to FIG. 5D, the bismuth compound 8 is present either on the surface of each primary particle or on the particle boundary parts 2 of a plurality of primary particles 1 connected to each other. Incidentally, the presence of the bismuth compound can be confirmed, for example, by using an electron microscope (“JSM-6390” (trade name), a product of JEOL Ltd.).
3. Single Particles
The large number of crystal grains contained in the positive electrode active material of the present invention preferably contain single particles by 40 areal % or more. That is, the proportion of the single particles contained in the large number of crystal grains is preferably 40 areal % or more. When the proportion of the single crystals is less than 40 areal %, the amount of secondary particles such as polycrystal particles, agglomerated particles and the like is relatively large; thereby, the diffusion of Li ion is hindered at the particle boundary parts of secondary particles, which may cause a reduction in rate characteristics. Incidentally, in the present Specification, “single particle” refers to a crystal grain present independently, of the crystal grains contained in the large number of crystal grains; that is, a crystal grain not forming a polycrystalline particle or an agglomerated particle.
The proportion (areal %) of the single particles contained in the large number of crystal grains can be determined by the following method. A positive electrode active material is mixed with a conductive resin (“Technovit 5000” (trade name), a product of Heraeus Kulzer GmbH), followed by curing. Then, the cured material is subjected to mechanical grinding and then ion-polished using a cross section polisher (“SM-09010” (trade name), a product of JEOL Ltd.). The backscattered electron image of the ion-polished material is taken, using a scanning electron microscope (“ULTRA 55” (trade name), a product of Carl Zeiss, Inc.), and the cross section of the positive electrode active material is observed.
In the backscattered electron image, the contrast differs owing to channeling effect when the direction of crystal differs. Therefore, when a grain boundary part is present in the crystal grain being observed, the grain boundary part becomes clear or unclear by slightly changing the direction of observation of sample (the inclination of sample). Utilizing this phenomenon, the presence of grain boundary part can be confirmed; thereby, there can be identified whether or not a crystal grain is a single particle, or a polycrystal particle formed by connection of primary particles of different crystallographic directions or an agglomerated particle.
There is a case in which microparticles (crystal grains) significantly smaller in diameter (e.g. about 0.1 to 1 μm) than the particle diameter of single particle adhere onto the surface of a crystal grain (see FIG. 6A). Also, there is a case in which polycrystal particles or agglomerated particles adhere onto each other at a small part (see FIG. 6B). In such cases, the parts (adhesion parts 50a to 50c in FIG. 6A) at which microparticles 41 to 43 adhere onto the surface of a crystal grain 31, and the part (adhesion part 50d in FIG. 6B) at which crystal grains 32 and 33 are in contact with each other, are slight; therefore, there is no influence on rate characteristics and durability. Accordingly, such crystal grains can be regarded substantially as single particle. Specifically explaining, when the length of adhesion part (the total of all adhesion parts when there is a plurality of adhesion parts) of a crystal grain is ⅕ or smaller relative to the circumference of the crystal grain estimated from the backscattered electron image by using an image edit software (“Image-Pro” (trade name), a product of Media Cybernetics, Inc.), the crystal grain is regarded as single particle and is calculated.
FIG. 6A to FIG. 6D are each a schematic drawing showing a state in which crystal grains adhere to each other, in the section of the positive electrode active material of the present invention. For example, FIG. 6A is a case in which three microparticles 41 to 43 adhere onto the surface of a crystal grain 31 and the total of the lengths of adhesion parts 50a to 50c is ⅕ or smaller relative to the circumference of the crystal grain 31. In this case, the crystal grain 31 is regarded as single particle. Meanwhile, any of the microparticles 41 to 43 is not regarded as single particle because the length of each adhesion part is ⅕ or larger relative to the circumference of each fine particle. FIG. 6B is a case in which crystal grains 32 and 33 adhere to each other and the length of adhesion part 50d is ⅕ or smaller relative to the circumference of the crystal grain 32 or 33. In this case, the crystal grains 32 and 33 are each regarded as single particle. FIG. 6C is a case in which crystal grains 34 and 35 adhere to each other and the length of adhesion part 50e is ⅕ or larger relative to the circumference of the crystal grain 34 or 35. In this case, any of the crystal grains 34 and 35 is not regarded as single particle. FIG. 6D is a case in which two small crystal grains 37 and 38 (not microparticles) adhere onto the surface of a crystal grain 36 and the total of the lengths of adhesion parts 50f and 50g is ⅕ or smaller relative to the length of the circumference of the crystal grain 36. In this case, the crystal grain 36 is regarded as single particle. Meanwhile, any of the crystal grains 37 and 38 is not regarded as single particle because the length of each adhesion part is ⅕ or larger relative to the circumference of the crystal grain 37 or 38.
In this way, there is judged whether or not each crystal grain is a single particle. The proportion (areal %) of single particles can be calculated by measuring the area (B) occupied by all crystal grains whose areas can be measured from the backscattered electron image and the area (b) occupied by all single particles by using the above-mentioned image edit software and substituting them into an expression (b/B)×100.
4. Secondary Particles
Preferably, the large number of crystal grains contain secondary particles formed by mutual connection of a plurality of primary particles. Each secondary particle is formed by mutual connection of a plurality of primary particles. FIGS. 1 and 2 are each a perspective view showing an example of the state in which a plurality of primary particles are connected to each other. As shown in FIG. 1, in a secondary particle 10, a plurality of primary particles 1 are connected to each other at their boundary parts 2. In FIG. 1, a plurality of primary particles 1 are connected to each other so that one crystal face 3 of each primary particle is on one same plane. Incidentally, the secondary particles are not restricted to those formed by the above connection and may be, for example, those formed by such mutual connection that a plurality of primary particles 1 are piled up in such a manner that one crystal face 3 of each primary particle 1 is directed to one same direction, as shown in FIG. 2. Of these secondary particles, preferred are those formed by in-plane connection of a plurality of primary particles 1, such as shown in FIG. 1, because such connection provides the following advantages. That is, in the FIG. 1 connection, there is no particle boundary part (which inhibits the diffusion of Li) in the thickness direction of each primary particle 1; therefore, there can be maintained about the same charge-discharge property as when there is used a positive electrode active material containing a large number of single particles free from secondary particles; meanwhile, there is obtained a smaller specific surface area than in the large number of single particles free from secondary particles, resulting in the higher durability (higher cycle characteristics) of positive electrode active material.
When the secondary particles are formed by in-plane connection of primary particles, it is preferable that 2 to 20 primary particles of 5 to 20 μm in particle diameter are connected. When the number of connection of primary particles is larger than 20, the secondary particles has a flat shape of large aspect ratio; when filling is made so that the flat face is parallel to the surface of positive electrode plate, the diffusion path of Li ion into the thickness direction of positive electrode plate becomes long and a reduction in rate characteristics is incurred, which is not preferred.
As to the production method of the positive electrode active material of the present invention, there is no particular restriction, and there is the following method, for example. First, there is prepared a mixed powder containing a lithium compound, a manganese compound and a bismuth compound (e.g. bismuth oxide). Incidentally, as the manganese compound and the bismuth compound, there may be used a compound of manganese and bismuth (e.g. Bi2Mn4O10). Also, it is possible to add a bismuth compound to lithium manganate (e.g. LiMn2O4). The mixed powder may further contain, for promotion of grain growth, a seed crystal composed of lithium manganate of spinel structure as a nucleus of grain growth. Further, a seed crystal and a bismuth compound may be added. In this case, the bismuth compound may be added in a state that it is adhered to the seed crystal.
As the lithium compound, there can be mentioned, for example, Li2CO3, LiNO3, LiOH, Li2O2, Li2O and CH3COOLi. As the manganese compound, there can be mentioned, for example, MnO2, MnO, Mn2O3, Mn3O4, MnCO3 and MnOOH. When Mn is substituted by a substituting element other than Li, the mixed powder may contain an aluminum compound, a magnesium compound, a nickel compound, a cobalt compound, a titanium compound, a zirconium compound, a cerium compound, etc. As the aluminum compound, there can be mentioned, for example, α-Al2O3, γ-Al2O3, AlOOH and Al(OH)3. As the magnesium compound, there can be mentioned, for example, MgO, Mg(OH)2 and MgCO3. As the nickel compound, there can be mentioned, for example, NiO, Ni(OH)2, and NiNO3. As the cobalt compound, there can be mentioned, for example, CO3O4, CoO and Co(OH)3. As the titanium compound, there can be mentioned, for example, TiO, TiO2 and Ti2O3. As the zirconium compound, there can be mentioned, for example, ZrO2, Zr(OH)4 and ZrO(NO3)2. As the cerium compound, there can be mentioned, for example, CeO2, Ce(OH)4 and Ce(NO3)3.
The mixed powder may be ground as necessary. The particle diameter of the mixed powder is preferably 10 μm or smaller. When the particle diameter of the mixed powder is larger than 10 μm, the mixed powder may be subjected to dry or wet grinding to make the particle diameter 10 μm or smaller. There is no particular restriction as to the method for grinding, and the grinding can be conducted using, for example, a pot mill, a beads mill, a hammer mill or a jet mill.
Next, the mixed powder prepared is formed into a formed article. There is no particular restriction as to the shape of the formed article, and there can be mentioned, for example, a sheet shape, a granular shape, a hollow-granule shape, a flake shape, a honeycomb shape, a bar shape and a roll shape (a wound shape). In order to more effectively obtain primary particles of 5 to 20 μm in diameter, the formed article can be produced as, for example, a sheet-shaped formed article of 10 to 30 μm in thickness, a hollow-granular-shaped formed article having a shell thickness of 10 to 30 μm, a grain-shaped formed article of 10 to 30 μm in diameter, a flake-shaped formed article of 10 to 30 μm in thickness and 50 μm to 10 mm in size, a honeycomb-shaped formed article of 10 to 30 μm in partition wall thickness, a roll-shaped (wound) formed article of 10 to 30 μm in thickness, and a bar-shaped formed article of 10 to 30 μm in diameter. Of these, a sheet-shaped formed article of 10 to 30 μm in thickness is preferred.
The method for forming a sheet-shaped or flake-shaped formed article is not particularly restricted and the forming can be conducted, for example, by a doctor blade method, by a drum drier method in which a slurry of a mixed powder is coated on a hot drum and dried and then the dried material is scraped off using a scraper, by a disc drier method in which a slurry of a mixed powder is coated on a hot disc and dried and then the dried material is scraped off using a scraper, or by an extrusion method in which a clay containing a mixed powder is extruded through a die with slits. Of these forming methods, there is preferred a doctor blade method capable of forming a uniform sheet-shaped formed article. The density of the shaped formed article obtained by the above forming method may be increased by pressing using a roller or the like. A hollow-granular formed article can be produced by appropriately setting the conditions of spray dryer. As the method for producing a grain-shaped formed article (a bulk shaped formed article) of 10 to 30 μm in diameter, there can be mentioned, for example, a spray dry method, a method of pressing a mixed powder by a roller or the like, and a method of cutting an extrudate which is a bar-shaped or sheet-shaped formed article. As the method for producing a honeycomb-shaped or bar-shaped formed article, there can be mentioned, for example, an extrusion method. Also, as the method for producing a roll-shaped formed article, there can be mentioned, for example, a drum dryer method.
Then, the formed article obtained is fired to obtain a sintered article. There is no particular restriction as to the method for firing. The firing of the sheet-shaped formed article is preferably conducted by placing each sheet on a setter one by one so as to minimize the piling-up of sheets, or by placing crumpled sheets in a cover-opened sagger.
Incidentally, the mixed powder per se may be fired. In this case, in order to obtain good contact of the mixed powder with the atmosphere during firing, it is preferred that the mixed powder is fired, for example, by making the deposited height of the mixed powder in a crucible or a sagger to make large the contact area of the mixed powder with the atmosphere. It is also preferred that the mixed powder is fired while stirring using a rotary kiln or the like. Incidentally, a sintered article (whose shape is plate-like, spherical or the like) of a getter material (e.g. zirconia) capable of absorbing bismuth is placed in the mixed powder as necessary.
The firing is conducted preferably in a state that the vaporization of bismuth is promoted so that the proportion of bismuth contained in bismuth compound becomes 0.005 to 0.5 mol % relative to the manganese contained in lithium manganate. The firing temperature is preferably 830 to 1,050° C. When the firing temperature is lower than 830° C., the grain growth of primary particles may be insufficient. Meanwhile, when the firing temperature is higher than 1,050° C., there is a case that lithium manganate releases oxygen and is decomposed into lithium manganate of layered rock salt structure and manganese oxide. The atmosphere of the firing may be an atmosphere of high oxygen partial pressure. In this case, the oxygen partial pressure is preferably, for example, 50% or higher relative to the pressure of the firing atmosphere. Thereby, the release of oxygen from lithium manganate becomes difficult and the decomposition thereof becomes difficult.
It is presumed that the presence of bismuth compound and above-mentioned seed crystal in firing is effective for the promotion of grain growth of primary particles even at a relatively low temperature (about 900° C.), resulting in a small specific surface area and high crystallinity. By thus conducting the firing, there can be prepared a polycrystal composed of primary particles having relatively large particle diameters and high crystallinity. Incidentally, in firing a sheet-shaped formed article, by growing particles sufficiently until the particles become singleness in the thickness direction of sheet, the particle diameters are restricted at about the thickness of sheet and there can be prepared a sheet-shaped sintered article in which primary particles uniform in particle diameters are connected to each other in a plane.
By conducting the firing with a controlled temperature elevation rate, the particle diameter of primary particles after firing can be uniformized. In this case, the temperature elevation rate may be, for example, 50 to 500° C. per hour. Also, by keeping the atmospheric temperature in a low temperature range and then conducting the firing at the firing temperature, it is possible to grow primary particles uniformly. In this case, the low temperature range may be 400 to 800° C. when the formed article is fired, for example, at 900° C. The uniform growth of primary particles is also possible by forming crystal nuclei at a temperature higher than the firing temperature and then conducting the firing at a firing temperature. In this case, the temperature higher than the firing temperature may be 1,000° C., for example, when the firing temperature of the firing material is 900° C.
The firing can also be conducted in two stages. For example, a mixed powder of manganese oxide and alumina is formed into a sheet shape, the formed article is fired, a lithium compound is added thereto, and firing is conducted again, whereby lithium manganate can be produced. Also, lithium manganate crystal of high lithium content is produced, then manganese oxide or alumina is added, and firing is conducted again, whereby lithium manganate can be produced.
Then, the polycrystal or sintered article obtained is subjected to wet or dry grinding, to grind primary particles to such an extent that particles boundary parts break away with no breakage of primary particles, and/or is subjected to classification, whereby crystal grains having intended particle diameters and an intended proportion of single particles can be obtained. As the method for grinding, there is no particular restriction. There can be mentioned, for example, a method of disintegrating the sintered article by pressing it against a mesh or a screen of 10 to 100 μm in opening diameter, and a method of using a pot mill, a beads mill, a hammer mill, a jet mill the like. As to the method for classification, there is no particular restriction. There can be mentioned, for example, a method of conducting sieving using a mesh of 5 to 100 μm in opening diameter, a method by water elutriation, and a method of using an air classifier, a sieve classifier, an elbow jet classifier or the like.
By re-heating the obtained crystal grains having intended particle diameters and an intended proportion of single particles at a temperature lower than the above-mentioned firing temperature, oxygen defect is cured, the distortion of crystallinity taking place during the grinding is recovered, and there can be produced a positive electrode active material containing a large number of crystal grains containing secondary particles formed by mutual connection of a plurality of single particles or primary particles. The re-heating can be conducted also by maintaining at a given temperature for a given period of time, prior to the grinding, that is, during the temperature lowering of the first firing, and this re-heating as well is effective for the curing of oxygen defect. When the re-heating is conducted after the grinding (or after the classification), the powder after re-heating may be subjected again to grinding and classification. The grinding and the classification can be conducted by the above-mentioned methods, etc.
A positive electrode active material of the present invention can be produced by the above-mentioned production method.
According to the above-mentioned production method, there can be obtained a positive electrode active material having a specific surface area of 0.1 to 0.5 m2/g, which contains a large number of crystal grains containing
primary particles of 5 to 20 μm in particle diameter, composed of lithium manganate of spinel structure containing lithium and manganese as the constituent elements, and
a bismuth compound containing bismuth,
wherein the proportion of the primary particles contained in the large number of crystal grains is 70 areal % or more and the proportion of the bismuth contained in the bismuth compound is 0.005 to 0.5 mol % relative to the manganese contained in the lithium manganate.
The specific surface area of the positive electrode active material is 0.1 to 0.5 m2/g, preferably 0.15 to 0.4 m2/g, more preferably 0.2 to 0.35 m2/g. When the specific surface area of the positive electrode active material is not within this range, there may be a reduction in cycle characteristics. Incidentally, the specific surface area can be measured using “Flowsorb III 2305” (trade name) (a product of Shimadzu Corporation), by using nitrogen as an adsorption gas.
The value of a lattice strain (η) in powder X-ray diffraction pattern of the positive electrode active material is preferably 0.7×10−3 or less, more preferably 0.5×10−3 or less, particularly preferably 0.3×10−3 or less. When the value of the lattice strain (η) is not within this range, there may be a reduction in rate characteristics. Incidentally, the value of the lattice strain (η) can be calculated using the following numerical expression (2).
β cos θ=λ/D+2η sin θ (2)
(In the expression (2), β indicates an integrated full width at half maximum (rad); θ indicates a diffraction angle (°); λ indicates a wavelength ({acute over (Å)}) of X-ray; and D indicates a crystallite size ({acute over (Å)}).)
More specifically, the value of the lattice strain (η) can be calculated by analyzing the diffraction image of powder X-ray diffraction pattern using an analytical software “TOPAS”, according to the WPPD (Whole Powder Pattern Decomposition) method. Incidentally, the powder X-ray diffraction pattern can be measured using, for example, “D8 ADVANCE” (a product of Bruker AXS Ltd.).
II. Lithium Secondary Battery
The lithium secondary battery of the present invention has an electrode body which comprises a positive electrode containing the positive electrode active material described in “I. Positive electrode active material” and a negative electrode containing a negative electrode active material. The lithium secondary battery of the present invention is superior in cycle characteristics at high temperatures. Such a characteristics appears strikingly particularly in large-capacity secondary batteries produced using a large amount of an electrode active material. Therefore, the lithium secondary battery of the present invention can be used preferably, for example, as a motor driven electric source of electric vehicle or hybrid electric vehicle. However, the lithium secondary battery of the present invention can also be used preferably as a small-capacity cell (e.g. coin cell).
The positive electrode can be obtained, for example, by mixing a positive electrode active material with acetylene black (a conductive agent), polyvinylidene fluoride (PVDF) (a binder), polytetrafluoroethylene (PTFE), etc. at given proportions to prepare a positive electrode material and coating the positive electrode material on the surface of metal foil or the like. As the positive electrode active material, there may be used lithium manganate of spinel structure alone, or a mixture thereof with a different active material (e.g. lithium nickelate, lithium cobaltate, lithium cobalt-nickel-manganate (so-called ternary system), or lithium iron phosphate). Lithium nickelate consumes the hydrofluoric acid which generates in the electrolytic solution of battery and which causes the dissolution of manganese (the dissolution is the main cause of durability deterioration of lithium manganate), and suppresses the dissolution of manganese effectively.
As the materials (other than the positive electrode active material) required as the components of the lithium secondary battery of the present invention, there can be used various known materials. As the negative electrode active material, there can be used, for example, an amorphous carbonaceous material (e.g. soft carbon or hard carbon), highly graphitized carbon material (e.g. artificial graphite or natural graphite) and acetylene black. Of these, a highly graphitized carbon material (which is high in lithium capacity) is used preferably. Using such a negative electrode active material, a negative electrode material is prepared; the negative electrode material is coated on a metal foil or the like; thereby, a negative electrode is obtained.
As the organic solvent used in the non-aqueous electrolytic solution, there can be preferably used a carbonic acid ester type solvent (e.g. ethylene carbonate (EC), diethyl carbonate (DEC), dimethyl carbonate (DMC) or propylene carbonate (PC)), a single solvent (e.g. γ-butyrolactone, tetrahydrofuran, acetonitrile or the like), or a mixed solvent thereof.
As specific examples of the electrolyte, there can be mentioned a lithium complex fluoride compound (e.g. lithium phosphate hexafluoride (LiPF6) or lithium borofluoride (LiBF4)) and a lithium halide (e.g. lithium perchlorate (LiClO4)). Ordinarily, at least one kind of such electrolyte is used by being dissolved in the above-mentioned organic solvent. Of these electrolytes, LiPF6 is used preferably because it hardly causes oxidative decomposition and gives a high conductivity in non-aqueous electrolytic.
As specific examples of the battery structure, there can be mentioned a coin cell type lithium secondary battery (coin cell) 11 such as shown in FIG. 3, wherein an electrolytic solution is filled between a positive electrode plate 12 and a negative electrode plate 13 with a separator 6 provided between them; and a cylindrical lithium secondary battery such as shown in FIG. 4, using an electrode body 21 formed by winding or laminating, via a separator 6, a positive electrode plate 12 (prepared by coating a positive electrode active material on a metal foil) and a negative electrode 13 (prepared by coating a negative electrode active material on a metal foil).
The present invention is described specifically below by way of Examples. However, the present invention is in no way restricted to the following Examples. Incidentally, in the following Examples and Comparative Examples, “parts” are based on mass unless otherwise specified. The measurement methods of properties and the evaluation methods of properties are shown below.
[Proportion (Areal %) of Primary Particles of 5 to 20 μm in Particle Diameter]
The area (A) occupied by all the crystal grains whose particle diameters can be measured and the area (a) occupied by the primary particles of 5 to 20 μm in particle diameter were measured using an image edit software (“Photoshop” (trade name), a product of Adobe Systems Incorporated); they were substituted into an expression ((a/A)×100); thereby, the proportion of the primary particles of 5 to 20 μm in particle diameter was calculated.
[Particle Diameters (μm) of Primary Particles]
A positive electrode active material powder was placed on a carbon tape so that there was no piling of particles; Au was sputtered thereon in a thickness of about 10 nm using an ion sputtering apparatus (“JFC-1500” (trade name), a product of JEOL Ltd.); then, a secondary electron image of particles was taken, using a scanning electron microscope (“JSM-6390”(trade name), a product of JEOL Ltd.), by selecting such a display magnification that 20 to 50 primary particles each having the maximum diameter of 5 μm or larger were in the visual field (the photographing conditions were accelerating voltage of 15 kV and working distance of 10 mm). For each primary particle in the image obtained, there was calculated an average of the maximum diameter of the particle part not hidden by other particles and the largest diameter of the diameters at right angles to the above maximum diameter, and the average was taken as the particle diameter (μm) of the primary particle. In this way, particle diameters were measured for all primary particles excluding particles which are hidden by other particles and are uncalculable.
[Specific Surface Area (m2/g)]
Measured using “Flowsorb III 2305” (trade name) (a product of Shimadzu Corporation), by using nitrogen as an adsorption gas.
[Proportion (mol %) of Bismuth]
Measured using an ICP (inductively coupled plasma) optical emission spectrometer. Specifically explaining, a sample solution prepared by adding hydrochloric acid to crystal grains and decomposing the mixture under pressure was placed in an ICP optical emission spectrometer (“ULTIMA 2” (trade name), a product of HORIBA, Ltd.) to quantitatively determine Li, Mn and Bi, and the proportion of the bismuth contained in bismuth compound relative to the manganese contained in lithium manganate was calculated based on the determination results.
[Kind of Bi Compound]
Identified by X-ray diffraction measurement (“RAD-IB” (trade name), a product of Rigaku Corporation) (hereinafter, referred to as “XRD”). When the compound amount was so small as not to be identified by the X-ray diffraction measurement, there was used electron probe microanalysis (“JXA-8800” (trade name), a product of JEOL Ltd.) (hereinafter, referred to as “EPMA”); when other component was detected at a region where Bi was detected, it was interpreted that Bi was present as a compound with the other component.
[Proportion (areal %) of Single Particles]
A positive electrode active material was mixed with a conductive resin (“Technovit 5000” (trade name), a product of Heraeus Kulzer GmbH), followed by curing. Then, the cured material was subjected to mechanical grinding and then ion-polished using a cross section polisher (“SM-09010” (trade name), a product of JEOL Ltd.). The backscattered electron image of the ion-polished material was taken, using a scanning electron microscope (“ULTRA 55” (trade name), a product of Carl Zeiss, Inc.), and the cross section of the positive electrode active material was observed.
In the backscattered electron image, the contrast differs owing to channeling effect when the direction of crystal differs. Therefore, when a grain boundary part is present in the crystal grain being observed, the grain boundary part becomes clear or unclear by slightly changing the direction of observation of sample (the inclination of sample). Utilizing this phenomenon, the presence of grain boundary part can be confirmed; thereby, there can be identified whether or not a crystal grain is a single particle, or a polycrystal particle formed by connection of primary particles of different crystal directions or an agglomerated particle.
There is a case in which microparticles (crystal grains) significantly smaller in diameter (e.g. about 0.1 to 1 μm) than the particle diameter of single particle adhere onto the surface of a crystal grain (see FIG. 6A). Also, there is a case in which polycrystal particles or agglomerated particles adhere onto each other at a small part (see FIG. 6B). In such cases, the parts (adhesion parts 50a to 50c in FIG. 6A) at which microparticles 41 to 43 adhere onto the surface of a crystal grain 31, and the part (adhesion part 50d in FIG. 6B) at which crystal grains 32 and 33 are in contact with each other, are slight; therefore, there is no influence on rate characteristics and durability. Accordingly, such crystal grains can be regarded substantially as single particle. Specifically explaining, when the length of adhesion part (the total of all adhesion parts when there was a plurality of adhesion parts) of a crystal grain was ⅕ or smaller relative to the circumference of the crystal grain estimated from the backscattered electron image by using an image edit software (“Image-Pro” (trade name), a product of Media Cybernetics, Inc.), the crystal grain was regarded as single particle and was counted.
In this way, there was judged whether or not each crystal grain was a single particle. The proportion (areal %) of single particles was calculated by measuring the area (B) occupied by all crystal grains whose areas could be measured from the backscattered electron image and the area (b) occupied by all single particles by using the above-mentioned image edit software and substituting them into an expression (b/B)×100.
[Initial Capacity (mAh/g)]
At a test temperature of 20° C., constant-current charge was conducted at a current of 0.1 C rate until the battery voltage became 4.3 V. Constant-voltage charge was conducted at a current condition of keeping the battery voltage at 4.3 V until the current decreased to 1/20. Then, a halt of 10 minutes was conducted. Subsequently, constant-current discharge was conducted at a current of 10 rate until the battery voltage became 3.0 V. Then, a halt of 10 minutes was conducted. This charge-discharge operation was taken as 1 cycle. Total 3 cycles were repeated at 20° C. A discharge capacity at the 3rd cycle was measured and taken as initial capacity.
[Value of Lattice Strain (η)]
The powder X-ray diffraction pattern of a sample was obtained, using “D8 ADVANCE” (a product of Bruker AXS Ltd.) under the following conditions and analyzed according to the WPPD method to calculate the value of the lattice strain of the sample.
X-ray output: 40 kV×40 mA
Goniometer radius: 250 mm
Divergence slit: 0.6°
Scattering slit: 0.6°
Soller slit: 2.5° (incidence side, receiving side)
Measurement method: 2θ/θ method in a Focusing optical geometry of horizontally-placed sample type (2θ of 15 to 140° was measured, step width of 0.01°)
Scanning time: Set so that the intensity of main peak ((111) face) became about 10,000 counts.
The specific analytical procedure is described below. The value of the lattice strain (η) obtained by other analytical procedure may be different from the value of the lattice strain (η) obtained by the present analytical procedure; however, these are not excluded from the scope of the present invention. In the present invention, the evaluation of the value of the lattice strain should be made using the value of the lattice strain (η) obtained by the present analytical procedure.
1. Start of software (TOPAS) and load of measured data
2. Setting of emission profile (selection of Cu tube and Bragg-Brentano type focusing optical geometry)
3. Setting of background (the Legendre polynominal is used as profile function, and the number of terms is set at 8 to 20.)
4. Setting of instrument (fundamental parameter is used, and slit conditions, filament length and sample length are input.)
5. Setting of corrections (sample displacement is used; absorption is also used when the filling density of sample in sample holder is low; in this case, absorption is set at the linear absorption coefficient of sample.)
6. Setting of crystal structure (space group is set at F-d3m; lattice constant, crystallite size and lattice strain are used; and the spread of profile by crystallite size and lattice strain is set as Lorenz function.)
7. Calculation (background, sample displacement, diffraction intensity, lattice constant, crystallite size and lattice strain are made precise.)
8. Analysis is over when the standard deviation of crystallite size is 6% or smaller of the crystallite size which has been made precise. When the standard deviation is larger than 6%, moves to the following procedure.
9. The spread of profile by lattice strain is set as Gauss function (the setting of the crystallite size as Lorenz function is unchanged.)
10. Calculation (background, sample displacement, diffraction intensity, lattice constant, crystallite size and lattice strain are made precise.)
11. Analysis is over when the standard deviation of crystallite size is 6% or smaller of the crystallite size which has been made precise. When the standard deviation is larger than 6%, analysis is impossible.
12. The value of the lattice strain obtained is multiplied by π/180, and the value is taken as η.
[Cycle Characteristics (%)]
At a test temperature of 60° C., charge was conducted at a constant current and constant voltage of 1 C rate until the battery voltage became 4.3 V, and discharge was conducted at a constant current of 1 C rate until the battery voltage became 3.0 V. This was taken as 1 cycle. 100 cycles of charge-discharge were repeated. Thereafter, the discharge capacity of the battery was divided by the initial capacity and the quotient (expressed in %) was taken as cycle characteristics.
[Rate Characteristics (%)]
At a test temperature of 20° C., constant-current charge was conducted at a current of 0.1 C rate until the battery voltage became 4.3 V. Constant-voltage charge was conducted at a current condition of keeping the battery voltage at 4.3 V until the current decreased to 1/20. Then, a halt of 10 minutes was conducted. Subsequently, constant-current discharge was conducted at a current of 1 C rate until the battery voltage became 3.0 V. Then, a halt of 10 minutes was conducted. This charge-discharge operation was taken as 1 cycle. Total 3 cycles were repeated at 20° C. A discharge capacity at the 3rd cycle was measured and taken as discharge capacity C(1 C). Next, at a test temperature of 20° C., constant-current charge was conducted at a current of 0.1 C rate until the battery voltage became 4.3 V. Constant-voltage charge was conducted at a current condition of keeping the battery voltage at 4.3 V until the current decreased to 1/20. Then, a halt of 10 minutes was conducted. Subsequently, constant-current discharge was conducted at a current of 5 C rate until the battery voltage became 3.0 V. Then, a halt of 10 minutes was conducted. This charge-discharge operation was taken as 1 cycle. Total 3 cycles were repeated at 20° C. A discharge capacity at the 3rd cycle was measured and taken as discharge capacity C(5 C). The capacity maintenance rate (%) of the discharge capacity C(5 C) at 5 C rate to the discharge capacity C(1 C) at 1 C rate was calculated and taken as rate characteristics.
Production of Positive Electrode Active Materials
(1) Raw Material Preparation Step
There were weighed a Li2CO3 powder (a product of The Honjo Chemical Corporation, fine grade, average particle diameter: 3 μm) and a MnO2 powder (a product of Tosoh Corporation, electrolytic manganese dioxide, FM grade, average particle diameter: 5 μm, purity: 95%) so that the two powders gave a chemical formula of Li1.1Mn1.9O4. Further, a Bi2O3 powder (average particle diameter: 0.3 μm, a product of Taiyo Koko Co., Ltd.) was weighed so that the addition amount of Bi relative to the Mn contained in the MnO2 raw material became an amount shown in Table 1 or Table 2. Hundred parts of these powders and 100 parts of an organic solvent (as a dispersing medium) (a mixed solvent of equal volumes of toluene and isopropyl alcohol) were placed in a cylindrical, wide-mouthed bottle made of a synthetic resin and subjected to wet mixing and grinding for 16 hours with a ball mill containing zirconia balls of 5 mm in diameter, to obtain a mixed powder.
(2) Sheet Formation Step
Ten parts of a polyvinyl butyral (as a binder) (“S-LEC BM-2” (trade name), a product of Sekisui Chemical Co., Ltd.), 4 parts of a plasticizer ((“DOP” (trade name), a product of Kurogane Kasei Co., Ltd.) and 2 parts of a dispersing agent (“RHEODOL SP-O 30” (trade name), a product of Kao Corporation) were added to the mixed powder, followed by mixing, thereby a forming material of slurry state was obtained. The forming material of slurry state was degassed under vacuum with stirring, to adjust the slurry viscosity to 4,000 mPa·s. The viscosity-adjusted forming material of slurry state was spread on a PET film by doctor blade method, to obtain each sheet-shaped formed article. Incidentally, the thickness of each sheet-shaped formed article after drying is shown in Table 1 or Table 2.
The sheet-shaped formed article was peeled off from the PET film, cut into a 300 mm×300 mm size using a cutter, and placed in an alumina-made sagger (dimension: 90 mm×90 mm×60 mm (height)) in a crumpled state. Degreasing was conducted at 600° C. for 2 hours in a cover-opened state (that is, under the air), after that firing was conducted at a temperature shown in Table 1 or Table 2, for 12 hours.
The sheet-shaped formed article after firing was placed on a polyester-made mesh having an average opening diameter selected under the following conditions, and pressed against the mesh lightly using a spatula, for disintegration.
When the sheet-shaped formed article had a thickness of 10 μm or less: average opening diameter=10 μm
When the sheet-shaped formed article had a thickness of 11 to 20 μm: average opening diameter=20 μm
When the sheet-shaped formed article had a thickness of more than 20 μm: average opening diameter=40 μm
The powder obtained was dispersed in ethanol and subjected to an ultrasonic treatment (38 kHz, 5 minutes) using an ultrasonic cleaner. Then, the resulting material was passed through a polyester-made mesh having an average opening diameter of 5 μm in order to remove the fine powder of 5 μm or less in particle diameter generated during the firing or grinding, and then a powder remaining on the mesh was recovered.
(6) Re-Heating Step
The primary particles having an intended diameter, recovered via the grinding step and the classification step, were heat-treated under the air at 650° C. for 24 hours to produce a positive electrode active material.
In Table 1 and Table 2 are shown the addition amount of Bi in the raw material preparation step, the thickness of the sheet-shaped formed article after drying, the firing temperature in the firing step, the proportion of primary particles of 5 to 20 μm in particle diameter, the specific surface area of positive electrode active material, the proportion of Bi, and the kind of Bi compound, in each of Examples 1 to 12 and Comparative Examples 1 to 14.
Properties of positive electrode active material
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