ELECTRODE MATERIALS FROM HYDROUS METAL AND/OR HYDROUS MIXED METAL OXIDES AND METHOD OF PREPARING THE SAME

Abstract: An electrode material comprised of hydrous metal oxide, such as ruthenium oxide, is annealed up to temperature just below the temperature at which the hydrous metal oxide would crystallize. Therefore, the hydrous metal oxide remains amorphous or non-crystalline. A hydrous metal oxide material treated in this manner provides a charge storage capacity and energy density greater than 747 F/g and 92 joules/gram, respectively, over 1 V range in a sulfuric acid electrolyte. This invention also provides a method of material preparation, wherein a sol-gel process is used to fabricate the hydrous metal oxides and wherein commercially available hydrous ruthenium oxide powders are treated and annealed.

Description: Title ELECTRODE MATERIALS FROM HYDROUS METAL AND/OR HYDROUS MIXED METAL OXIDES AND METHOD OF PREPARING THE SAME Attorney Docket No CECOM-5275 GOVERNMENT INTEREST The invention described herein may be made, used, sold or licensed, by or on behalf of the Government of the United States of Ameπca, without the payment to us of any royalties thereon BACKGROUND OF THE INVENTION 1 Technical Field This invention relates to electrochemical capacitor electrodes compπsed of materials from hydrous ruthenium oxide, other hydrous metal oxides, or hydrous mixed metal oxides More particularly, the invention relates to such electrodes comprised of hydrous ruthenium oxide, or other hydrous metal oxides, or hydrous mixed metal oxides and to electrochemical capacitors or electrochemical power sources comprising such electrodes This invention also relates to a method for the preparation of fine powders or thick films of such materials at low temperatures 2 Background Art Electrochemical capacitors (EC's) are devices which store electrical energy at the interface between an ionically-conducting electrolyte phase and an electronically-conducting electrode material EC's were first descπbed in a 1957 patent by Becker The first practical devices were pioneered by SOHIO as described in U S Pat No 3,536,963 based on the double-layer capacitance developed at the interface between high-area carbon electrodes and sulfuric acid electrolyte solution A complementary system, but originating from a different electrochemical phenomenon, that is development of pseudocapacitance associated with a surface reaction, was developed by Conway in 1975, in collaboration with Continental Group, Inc See Can Pat by Craig which is listed infra The materials possessing pseudocapacitance discovered in Conway et al 's work are metal oxides which include ruthenium oxide (RuO 2 ), iridium oxide (IrO 2 ), cobalt oxide (CoO 2 ), molybdenum oxide (MoO 2 ), and tungsten oxide (WO 3 ) The most effective material discovered was RuO 2 which gives a reversibly accessible pseudocapacitance of many Farads per gram over a 1 4 V range Heretofore, RuO 2 , has been fabricated by the thermal decomposition of ruthenium chloride or hydrous ruthenium chloride RuO 2 , like other dioxides of the platinum group, e g RhO 2 , OsO 2 , and IrO 2 , exhibits metallic conductivity and possesses the rutile structure The pseudocapacitance, which arises at the RuO and the electrolyte interface, is due to the facile ionic species absoφtion on the surface of the RuO 2 electrode material In order to maximize the charge or energy storage per unit weight of oxides in this type of system, it is desirable to maximize the surface area of the electrode material Such a maximum BET surface area of 130 m 2 /gram was achieved by Raistrick for optimized processing The observed capacitance per unit mass (F/g) and the observed capacitance per unit area (F/cm 2 ), which are determined from the measured electrochemical capacitance, the measured surface area, and the known amount of RuO 2 present in the electrode, are 380 F/g and 200-300 μF/cm 2 , respectively, in a 1 V range in sulfuric acid electrolyte Based on the assumption that one H may be adsorbed on each exposed O atom, a charge density of 200 μC/cm is estimated by Raistrick This suggests that the observed capacitance 380 F/g is the maximum value that can be achieved for RuO, These and other references, which are relevant to the present invention, include Can Pat No 1,196,683 issued in 1985 to Craig, U S Pat 2,800,616 issued in 1957 to Becker, and U S Pat 3,536,963 issued in 1970 to Boos, Conway, Journal of the Electrochemical Society, vol 138, pp 1539- 15, 1991 , Raistrick, Proceedings of First Conference on Capacitors and Similar Energy Storage Devices, Deerfield Beach, FL, Dec 9-11, 1991, Ansum Enterprises Inc , Boca Raton, FL, and U.S Patent No 5,003,428, issued to Shepherd on March 26, 1991 DISCLOSURE OF INVENTION Accordingly, one object of the present invention is to provide materials that have higher capacitance or higher energy density than that of ruthenium oxide (RuO 2 ), the highest energy density material available today, for use as an improved electrode material in electrochemical capacitors Possible applications of such a hydrous ruthenium oxide include the following electrode material for electrochemical capacitors, oxygen or chlorine evolution anodes, thin film resistors in very large scale integrated circuits, or diffusion buffer layers in silicon contact metallization According to the present invention, a new electrode material is formed which has an energy density which is more than two times greater than the state-of-the-art material, RuO 2 Therefore, the size of the capacitors and similar applications made of the material of this invention will be about half of the present devices Further, this invention provides advantages over prior art, such as (1) Ease of material process, and (2) Smaller capacitor size as a result of higher charge storage capability These objectives and advantages are provided by forming an electrode material comprised of hydrous ruthenium oxide which remains amoφhous in structure This material provides a charge storage capacity and energy density greater than 747 F/g and 92 joules/gram, respectively, over 1 V range in a sulfuric acid electrolyte This invention also provides a method of material preparation, wherein a sol-gel process is used to fabricate the hydrous metal oxides and wherein commercially available hydrous ruthenium oxide powders are treated and annealed Furthermore, the invention also provides a capacitor incoφorating the electrode material of this invention, which capacitor includes (1) an anode (a negative electrode) comprising hydrous ruthenium oxide, (2) an electrolyte comprising sulfuric acid of various concentration or other electrolytes, (3) a cathode (a positive electrode) comprising hydrous ruthenium oxide Such capacitors having electrodes comprised of hydrous ruthenium oxide (RuO 2 xH 2 O) exhibit an enhanced, linear voltage-charge relationship, excellent reversibility, and long cycle life The energy storage mechanism for capacitors made with RuO 2 xH O electrodes are mainly fast faradaic reactions occurring between the bulk of the RuO 2 xH 2 O electrode and the electrolyte It is different with that of double layer capacitors The energy storage of double layer capacitors is due to the separation of charges at the interface between a solid electrode and an electrolyte The faradaic reaction mechanism between the amoφhous RuO 2 xH 2 O electrode and the electrolyte is the hydrogenation of the ruthenium oxide, which is similar to that between a crystalline Ru 2 O electrode and the electrolyte The hydorgenation reaction can be expressed as follows δH" + RuO 2 (or RuO 2 xH 2 O) + δe " => H δ RuO 2 (or HsRuO 2 xH 2 O), where 0<δ<2 Eq 1 However, for crystalline anhydrous Ru 2 O electrodes, the faradaic reaction can only occur at the surface of the electrode The energy storage density is dependent on the specific surface area of the electrode material For amoφhous RuO 2 xH 2 O electrodes made in accordance with the present invention, however, the faradaic reaction will occur in the whole bulk of the electrode Therefore, the energy density of the amoφhous RuO 2 xH 2 O electrode will be much higher than that of any anhydrous crystalline ruthenium oxide electrode The H 2 O content, x, in the oxide affects the charge storage capacity The x value varies between zero and two The x value decreases as the annealing temperature increases As shown in Figs 3 and 4, the charge storage capacity increases as the annealing temperature increases However, the maintenance of the amoφhous phase is critical When the temperature is high enough, the amorphous phase of the material will convert to crystalline phase The charge storage capacity decreases dramatically as soon as the material becomes crystalline The capacitance density of RuO 2 xH 2 O provided by the sol-gel method and properly treated according to the present invention acheived a value greater than 747 farad/gram A single cell capacitor was fabricated and tested with this new electrode material The energy storage density of the capacitor was greater than 92 joule/gram These results show clearly that RuO 2 xH 2 O treated in accordance to the methods of the present invention is an excellent electrode material for electrochemical capacitors This material may also be used as electrode material for batteries and catalyst for fuel cells This invention provides methods for preparing the materials with high charge storage capacity and high energy density More importantly, this invention provides materials with specific qualities irrespective fo the preparation methods It is the specific qualities of the materials that result in the high charge storage capacity and therefore, high energy density The most critical quality of these materials is the amoφhous state of the materials BRIEF DESCRIPTION OF THE DRAWINGS These and other objects of the present invention will be better understood in light of the Detailed Description Of The Preferred Embodiments and the associated drawings wherein Fig. 1 is a plot of X-ray diffraction patterns for RuO 2 .xH 2 O prepared by a sol-gel process and annealed at different temperatures. Fig. 2 is a plot of X-ray diffraction patterns for RuO 2 xH 2 O made from commercial powders and annealed at different temperatures. Fig. 3 is a graph of the specific capacitance of RuO 2 xH 2 O electrodes as a function of the annealing temperature. The RuO 2 .xH 2 O electrodes were prepared by a sol-gel process and were annealed at different temperatures The specific capacitance was calculated based on the cyclic voltammetric measurement The electrolyte was 0 5 molar solution of H 2 SO 4 Fig 4 is a graph of the specific capacitance of RuO 2 xH 2 O electrodes as a function of the annealing temperature. The RuO 2 xH 2 O electrodes were made from commercial powders and were annealed at different temperatures Fig 5 is a graph of the weight loss as function of the annealing temperatures The solid line was measured by a thermogravimetric analyzer at a temperature scan rate of 10°C/min The starting material at 25° C was Ru(OH) 4 at a quantity of 12 93 mg The dotted line is the derivative weight loss. BEST MODES FOR CARRYING OUT THE INVENTION The electrochemical capacitor of this invention includes electrodes comprising hydrous ruthenium oxide, RuO 2 .xH 2 O or ruthenium oxide in the hydrous form The hydrous ruthenium oxide for use in the electrodes of the electrochemical capacitor of this invention has properties which are different from those heretofore described in the prior art as for example in Conway In accordance with one method of the present invention, this material, which has a different composition from that of anhydrous ruthenium oxide, is attained by a novel process. In prior art methods, ruthenium oxide, RuO 2 , was prepared by decomposing the aqueous ruthenium chloride, RuCl 3 , solution at approximately temperatures of 300°-400°C In contrast, the process used in this invention involves hydrolyzing ruthenium chloride in an aqueous solution, the hydrolysis being promoted by the addition of the hydroxide of sodium, lithium, or ammonia, which controls and stabilizes the pH of the solution Therefore, the gel formed can be precipitated by then adjusting the pH to higher values The above process is also called the sol-gel process The surface area of hydrous ruthenium oxides thus formed by the present invention has of a value as 45 m 2 /gram or higher This sol-gel process also allows the formation of films or buffers at low temperatures The hydrous ruthenium oxide can be further heated and formed with ruthenium oxide at temperatures above 270°C to have a surface area of 26 m 2 /gram The hydrous ruthenium oxide exhibits electronic properties similar to those of ruthenium oxide as well as enhanced ionic properties which allows additional charge storage for protons in both the surface and the bulk of the oxides Further, the preparation of hydrous ruthenium oxide has been reported However, the use of hydrous ruthenium oxide for electrochemical capacitors has not been reported before Similarly, the use of other hydrous metal oxides has not been reported Of course, as those skilled in the art will recognize, the preparation of other mixed metal oxides is also known, and therefore, the present invention will also extend to other hydrous metal oxides and hydrous mixed metal oxides For example, this invention would apply to hydrous metal oxides wherein the metal may be ruthenium, rhodium, rhenium, osmium or iridium Moreover, an example of a hydrous mixed metal oxide would be Ru x Ti y xH 2 O wherein x + y = l and the precipitate would be a solid solution Of course, those skilled in art will readily recognize from this disclosure that other mixed metals/metals would include cobalt, tungsten, manganese, tantalum, molybdenum, etc Therefore, it is expected that the hydrous mixed metal oxides will maintain electronic properties similar to those of mixed metal oxides as well as provide additional charge storage In one preferred method of fabricating the new electrode material, RuO 2 xH 2 O is produced from a starting material, RuCl 3 nH 2 O (42% Ru), by a sol-gel process which is described in detail below Briefly though, the Ru(OH) powder is formed by mixing solutions of RuCl 3 nH 2 O and NaOH to form precipitating powders of Ru(OH) 4 The weight of this precipitate should measure to be approximately 76% of the weight of the starting material of RuCl 3 nH 2 O From this weight measurement, it may be inferred that the precipitated powder may be Ru(OH) However, for puφoses of the present invention, it is not important what kind ruthenium compound is used at this stage, because this is only an intermediate product Accordingly, and as those skilled in the art will readily appreciate, the Ru(OH) can be made with different starting materials and reduction agents For example, the starting materials can be ruthenium chloride, ruthenium bromide, ruthenium nitrosyl chloride, ruthenium nitrosylnitrate and ruthenium 2,4-pentanedιonate Moreover, the reduction agents can be various alkalies or salts such as NaOH, NaCO 3 , NaHCO ., NaNO 3 , KOH, K 2 CO 3 , KNO 3 , and NH-.OH, etc After the Ru(OH) 4 is produced, then RuO 2 xH 2 O and RuO 2 are formed by heating the Ru(OH) 4 to temperatures of 100°C and 300°C respectively It is critical, however, that the treated powders according to the present invention not be subjected to temperatures above 300°C The annealing temperature of the present invention is a very important factor in determining the specific capacitance of the electrode At lower temperatures, i e below 200°C, RuO 2 xH 2 O remains in an amoφhous state When the annealing temperature is increased, both the amount of the powders in the crystalline phase and the crystallite size increases At temperatures above 300° C, the cyrstalline phase of anhydrous RuO 2 is formed Figs 1 and 2 show from X-ray diffraction analysis that depending the source of the RuO 2 xH 2 O, the crystalline phase of RuO 2 xH 2 O can be between 200° C and 300° C Fig 1 is a plot of X-ray diffraction patterns for RuO 2 xH 2 O prepared by a sol-gel process and annealed at different temperatures As shown the crystalline peaks begin to form around 175° C and are well defined at 200° C for RuO 2 xH O formed by the sol-gel process of the present invention However, Fig 2 shows that for RuO 2 xH 2 O made from commercial powders and annealed at different temperatures the crystalline peaks do not form until 300° C Therefore, depending upon the process used to form the RuO 2 xH 2 O, it is critical to the present invention that the RuO 2 xH 2 O remain in an amoφhous state and the annealing temperature used must not rise above the crystalline formation temperature Therefore, the maximum specific capacitance can be obtained from an electrode, which is prepared in accordance with the present invention either from the RuO 2 xH 2 O formed by the sol- gel process described in detail below or from commercially available RuO 2 xH 2 O powders, by annealing either powder at a temperature just below the critical temperature to form the crystalline phase of the hydrous metal oxide Figs 3 and 4 show graphs of the specific capacitance as a function of annealing temperature for electrodes made from the sol-gel process (Fig 3) and commercially available RuO 2 xH 2 O (Fig 4) The water content of these materials exhibits the maximum capacitance value where x is between 0 to 0 5 By comparing the results between the specific capacitance and the crystalline phase, it is found that for the electrode with the amoφhous phase, the specific capacitance is high and increases with the annealing temperature However, when the crystalline structure is formed, the specific capacitance of the electrode drops rapidly Therefore, the maximum value of the specific capacitance can be obtained at the temperature which is just below the critical temperature at which the crystalline phase of RuO 2 .xH 2 O starts to be formed As shown a maximum specific capacitance as high as 768 F/g is obtained from an electrode prepared at this optimal annealing temperature One specific example of the method of forming RuO 2 xH 2 O according to present invention is set forth below Example of Forming RuO 2 xH 2 O The Ru(OH) 4 powder is prepared as follows the required amount of RuCl 3 nH 2 O (42% wt Ru) is dissolved in distilled water to give a concentration of 0 1 mol At the same time, the NaOH is dissolved in distilled water to a concentration of 0 3 mol Then, the NaOH solution is added slowly into the RuCl 3 nH 2 O solution In this process, the NaOH is employed primarily for the puφose of adjusting and stabilizing the pH at a value of approximately 7, the point at which a controlled precipitation occurs During mixing, the RuC nH 2 O solution is stirred After stopping the stirring and waiting for a while, it can be seen that Ru(OH) 4 fine powders will precipitate in the NaCl solution Thus, the process used in this invention involves hydrolyzing ruthenium chloride in an aqueous solution, the hydrolysis being promoted by the addition of the hydroxide of sodium, lithium, or ammonia, which controls and stabilizes the pH of the solution Therefore, the gel formed can be precipitated by then simply adjusting the pH to higher values without the need of decomposing the aqueous ruthenium chloride, RuCl 3 , solution at approximately temperatures of 300°-400°C, as was previously done in the prior art Ru(OH) 4 fine powders are, then, separated from the NaCl solution by a filter with 8 μ pore size The hydrolysis product is washed five times in distilled water by the following procedures' An amount of distilled water is added into a beaker containing Ru(OH) 4 powders to give a concentration of 0.2 mol and is stirred with a magnetic stirrer for about 30 min Then, the solution is filtered The dry Ru(OH) 4 powders can be obtained by drying the precipitate in a vacuum At this stage, the final fine powders should be Ru(OH) 4 based on the weight change from the starting material However, the final fine powder may be Ru(OH) 3 xH 2 O or RuO 2 .2H 2 O since the molecular weights of Ru(OH) 4 , Ru(OH) 3 xH 2 O and RuO 2 2H 2 O are so close The RuO 2 .xH 2 O and RuO 2 are formed by heating Ru(OH) 4 to 100°C and 300°C in air for about 16 hours, respectively The weight loss should be approximately 12 5% and 21 5%, respectively It should be noted, however, that the process of using vacuum to dry Ru(OH) 4 , is an unnecessary step for formations of RuO 2 xH 2 O and RuO 2 because they can be formed by directly heating the wet Ru(OH) 4 to higher temperatures After forming the RuO 2 xH 2 O, the inventors herein studied various quality aspect of this material for use in capacitors From the following, those skilled in the art will readily recognize the advantages of this material for use in capacitors. A thermogravimetric analyzer (TGA) was used to study the weight change during the thermal processes as shown in Fig 5. It was found that the weight decreased continually with increasing the temperature up to 300°C At temperatures above 300°C, the rate of the weight loss was much lower with increasing the temperature Two peaks were obtained from a derivation of the TGA curve and appeared at 100°C and 300°C The first peak at 100°C is believed to be due to the formation of RuO 2 xH 2 O The weight change between the first and the second peak is due to dehydration process to form RuO 2 The precision weight losses were measured for powders after annealing at 100°C and 300°C and were 12 5% and 21 5%, respectively These results confirmed the inference that RuO 2 xH 2 O and RuO 2 were formed at temperatures of 100°C and 300°C, respectively This inference was also confirmed by crystalline structure measurements shown in Fig 1. The crystalline structure of powders was characterized by an X-ray diffractometer No shaφ peaks were obtained from the powder annealed at 100°C, which indicates that the RuO 2 xH 2 O is amoφhous From those powders annealed at 300°C, three strong x-ray difiractive peaks were obtained at 28°, 35° and 54° which correspond to (1 10), (101) and (21 1) lattice planes of the RuO 2 crystal See Fig 1 From the TGA and the x-ray diffractometer studies, it was found that the temperature for formation of RuO 2 xH 2 O or RuO 2 are critical The RuO 2 xH 2 O may only be formed in the temperature range from 50°C to 200°C, and the crystalline RuO 2 is formed at temperatures higher than 200°C. Usually the longer time was needed for the lower temperature to completely form above chemical compounds Combining the results from the TGA -ray diffraction, and specific capacitance measurements, it was also found that the water content, x, was in the range of 0.2 to 2 0 preferably from 0.5 to 1 8 and the RuO xH 2 O material was of an amoφhous phase The specific surface areas of RuO 2 xH 2 O and RuO 2 powders were determined by the nitrogen absoφtion measurement and were 44 7 and 26.2 m2/gram, respectively These values are much less than those of carbon based electrode materials which were widely used for double layer capacitors. It was found that the higher specific surface area of RuO 2 .xH 2 O or RuO 2 can be achieved with the lower concentration of the RuCl 3 .nH 2 O and NaOH solutions. It was found that in general the specific surface area reduces when the annealing temperature is increased. It was also found that the specific surface area is dependent on the other sample preparation conditions, such as the concentration of the RuCl 3 .xH 2 O and NaOH solutions, as well as greatly depending on the pH value at which two solutions were mixed. It has been shown that the specific surface area of the RuO 2 powder is less than that of the RuO 2 xH 2 O powder This is because the small particles tend to nucleate and to form larger crystalline particles at high temperatures However, it was also found that that the specific capacitance is insensitive to the specific surface area for the RuO 2 xH 2 O electrodes made at the optimal temperature But for other powders having exhibiting some crystalline phase, the specific capacitance is strongly dependent on the value of the specific surface area It is difficult to obtain the resistivity from powder materials However, pellets of RuO 2 .xH 2 O and RuO 2 were made by pressing powders under a pressure of 800 Pa The resistivity of these pellets was measured to be 4 5xl0 "3 Ω-cm and 6 0x10 "3 Ω-cm, respectively These values are at least two orders of magnitude higher than those of bulk materials. Nevertheless, the resistivity of the RuO 2 .xH 2 O pellet is lower than that of the RuO 2 pellet The high resistivity is mainly contributed from the contacting resistance between particles The real resistivity of RuO 2 .xH 2 O itself should be much lower than this value It was demonstrated that highly conductive RuO 2 electrodes could be made by coating the RuCl 3 solution on the metallic substrate, which is then thermally decomposed The highly conductive RuO 2 .xH 2 O thin film electrode, therefore, can also be achieved. Further, the resistivity of RuO 2 .xH 2 O pellets was also calculated based on the value of the sheet resistance measured by a standard four probe technique These pellets were made by pressing RuO 2 .xH 2 O powders at a pressure of 8,000 lb/cm 2 It was found that for RuO 2 xH 2 O powders made at lower temperatures, the resistivity of the RuO 2 xH 2 O pellet was higher (>10 "3 Ω- cm). But for RuO 2 .xH 2 O powders made at temperatures higher than 100° C, the resistivity of the RuO 2 .xH 2 O pellet is insensitive to the annealing temperature and was on the order of 10 "3 Ω-cm The resistivity of the RuO 2 .xH 2 O pellet made at the optimal temperature was about 2-3x10 "3 Ω- cm. This value is believed to be dominated by the contact resistance of the powders. The bulk resistivity of RuO 2 .xH 2 O may be much lower than this value. However, overall the resistivity of the RuO 2 xH 2 O pellets was sufficiently low for use in electrochemical capacitors The capacitance densities of RuO xH 2 O, RuO 2 and carbon black were measured by the cyclic voltammetric measurement in the electrolyte of 0.5 mol H 2 SO 4 The details of this measurement are described below. From Table 1, it can be seen that the capacitance density of RuO 2 .xH 2 O is the highest one The most remarkable feature is that the specific capacitance of Ru 2 xH 2 O is higher than that of RuO 2 As indicated, the higher capacitance density achieved in this new material is not only due to the higher surface area but also the intrinsic nature of the material. From the cyclic voltammetric curve, two peaks were obtained at potentials of about 0.4 volt and 0 9 volt verse the saturated calomel electrode Therefore, the capacitance developed between this material and the electrolyte is believed to be predominantly pseudocapacitive Capacitance Density The capacitance densities of carbon black pearls-2000, RuO 2 and RuO 2 .xH 2 O powders were measured by the cyclic voltammetry The carbon black pearls-2000 is commercially available and has the specific surface area of 1470 m 2 /gram Firstly, the carbon black, RuO 2 or RuO 2 .xH 2 O powders soaked in 0.5 mol H 2 SO at the boiling temperature During the measurement, the working electrode was made with the electrode material pasted on the platinum gauze The counter electrode was a platinum gauze, 80 times as large as the working electrode The reference electrode was a saturated calomel electrode (SCE) The electrolyte, 0 5 mol H 2 SO solution, was bubbled with nitrogen gas to avoid the influence of dissolved oxygen The voltammetric curves at 0.5 mV/sec were recorded in the potential range from 0 to 1 0 volt (vs SCE) Capacitance densities of different electrode materials were average values within the potential range from 0 to 1 0 volt (vs SCE) and are summarized in Table 1, which includes surface area, capacitance density and specific capacitances of carbon black pearls-2000, RuO 2 and RuO 2 xH 2 O fine particles. The specific surface area was measured by a nitrogen absoφtion method The capacitance density was measured by a cyclic voltammetry. Table 1 Electrode Material Specific Surface Area Capacitance Density Specific Capacitance (m /gram) (farad/gram) (μfarad/cm 2 ) Carbon Black 1475 250 17 RuO 2 262 200 756 RuO 2 x H 2 O 44 7 747 1671 RuOzx H 2 O(95%) — 630 — Teflon(5%) In application, RuO 2 .χH O is introduced in a capacitor For puφoses of this application single cell capacitors will be described However, as those skilled in the art will readily recognize other capacitor applications will also benefit from the present invention, such as those mentioned in the Summary of the Invention For comparison, single cell capacitors were built with two different types of electrodes The detailed configuration of these capacitors is descπbed below The energy densities of the two capacitors were measured to be 92 J/gram (184 J/cm 2 ) and 68 J/gram (121 J/cm 3 ) for a capacitor using a powder RuO 2 .χH 2 O electrode and a capacitor using a film electrode, respectively The film electrode contained RuO 2 .χH 2 O powder mixed with 5% teflon As shown in Table 2, the energy density of RuO 2 .χH 2 O corresponds to capacitance densities of 738 farad/gram for a single electrode and agrees with the measurement of the cyclic voltammetry The most important feature to be noted is that the energy density of this new material is the highest one available today and is at least two times higher than that reported for RuO 2 Capacitor formation Three types of capacitors were fabricated and tested The first type was made using the powder form of RuO .xH 2 O directly as electrodes The RuO .χH 2 O powder was impregnated with acid solution of 38% weight H 2 SO 4 at the boiling temperature Then, the excess acid solution was filtered The size of each electrode had a diameter of 0 5 inch and a thickness of 23 mil The gravimetric density of the electrode was about 2 gram/cm 3 for the RuO 2 .xH 2 O electrode only A 2 mil thick tantalum foil was used as the current collector and a 5 mil thick glass fiber paper, which was soaked with the acid solution, was used as the separator The capacitor was finally sealed by a Teflon™ container The second type was made using a 5% Teflon™ bonded RuO 2 .χH 2 O electrode of a thickness about 12 mil. The basic configuration of the capacitor is the same as the first one. The electrolyte includes a sulfuric acid of a concentration which varies from 0.5 to 4 moles. Other electrolytes including KOH of various concentrations, solid polymeric electrolytes (such as Nafion™), and organic electrolyte may also be employed in this invention. Capacitances of these two capacitors were measured by a dc charge and discharge method at a constant current for the voltage range from 0 to 1 volt between two electrodes. The capacitance was calculated by the current multiplied by the time of the discharge process which is summarized in Table 2 for the various electrode materials. The energy densities were calculated based on these capacitance values and the operating voltage of 1 volt The capacitance densities and the energy densities, measured with dc charge and discharge method are shown in Table 2. Table 2 ectrode Material Capacitance Capacitance Energy Energy Densitv Densitv Densitv Densitv (F/g) (F/cm 3 ) (J/g) (J/cm 3 ) Carbon Black 82 60 10 7.5 RuO 2 198 542 24.8 68 RuO 2 x H 2 O 738 1475 92.3 184 RuO 2 x H 2 O 540 970 68 121 Teflon It must be pointed out that the capacitance or the energy densities described in this embodiment are not the maximum values for this new material. For every ruthenium oxide, two hydrogen could be inserted into the new material as shown in Eq 1 This suggests that the capacitance of a value of 1,000 F/g could be achieved with materials according to the present invention. A lower value of 760 F/g for this new material achieved in this invention may be due to slight impurities present during preparation. Therefore, the higher capacitance and energy densities can be expected for the RuO 2 .χH 2 O electrode material. A third capacitor was built with the RuO 2 .xH 2 O powder electrodes which were made at the optimal annealing temperature. The electrode material was pre-wetted by back filling the electrolyte in a vacuum. 39 weight % of sulfuric acid solution was used as the electrolyte. Two identical electrodes separated by a porous membrane with a thickness about 50μm. The porous membrane was impregnated with the electrolyte. The maximum voltage which could be applied on a single cell was found to be over one volt. The energy density was calculated from the dc discharge process of the capacitor and was about 96 J/g (or 26.7 Whr/kg) based on the weight of the hydrous ruthenium oxide powders only. This value is consistent with that calculated from the value of the specific surface area which is measured by the cyclic voltammogram. The energy deliverable efficiency was estimated from the capacity ratio between the discharge and charge processes and was over 95%. This third capacitors performance was also studied at different temperatures. It was found that within the temperature range from -52°C to 73°C, the variation of the capacitance was less than 20%. The cycle life test was also performed for this capacitor and it was cycled for about 60,000 cycles. The stability of this new material was also studied by the inventors. To accomplish this, a capacitor was built with the powder electrode and was tested under the dc charge and discharge Until now, this capacitor has been cycled over 4000 times It was found that the capacitance decayed 5% during the first three cycles, since then the capacitance was much stable and only decayed another 5% until the 4000th cycle. From the dc charge and discharge measurement, the efficiency of the capacitor can be obtained and is higher than 90% Although the present invention has been described with regard to three specific embodiments as to how to manufacture the above identified material, those skilled in the art will readily recognize that other variations of manufacturing this material are available. Accordingly, the inventors do not wish to be limited by the present specification, but only by the appended claims.

Claims: WHAT IS CLAIMED IS: 1 A method of forming a hydrous metal oxide with a high energy density comprising the steps of providing the hydrous metal oxide, and annealing the hydrous metal oxide at a temperature just below a critical temperature at which the hydrous metal oxide would crystallize 2 A method of forming a hydrous metal oxide with a high energy density by a sol-gel process comprising the steps of hydrolyzing a metal halide in an aqueous solution and a reduction agent, controlling the pH of the solution so as to maintain a stable pH, and heating a resultant precipitate in the temperature range between 50° and 200° Celsius wherein the resultant precipitate is an amoφhous hydrous metal oxide and has a capacitance density greater than 380 farads per gram 3 The method of claim 2 wherein the metal halide comprises a metal selected from the group consisting of ruthenium, rhodium, rhenium, osmium, iridium and titanium, cobalt, tungsten, manganese, tantalum, molybdenum, and nickel 4 The method of claim 2 wherein the reduction agent is selected from the group consisting of hydroxide of sodium, lithium, ammonia, NaCO 3 , NaHCO 3 , NaNO , KOH K 2 CO 3 , and KNO 3 5 The method of claim 2 wherein the resultant precipitate is heated in the temperature range between 80° and 175° Celsius 6 A method of forming a hydrous ruthenium oxide with a high energy density by a sol-gel process comprising the steps of mixing a ruthenium compound dissolved in an aqueous solution and a reduction agent to form a precipitate, the ruthenium compound being selected from the group consisting of ruthenium chloride, ruthenium bromide, ruthenium nitrosyl chloride, ruthenium nitrosylnitrate and ruthenium 2,4-pentanedionate, controlling the pH of the solution by the addition of buffers so as to maintain a stable pH, and heating the precipitate in a temperature range between 50° and 200° Celsius to form the hydrous ruthenium oxide wherein the hydrous ruthenium oxide is amoφhous and has a capacitance density greater than 380 farads per gram. 7 The method of claim 6 wherein the reduction agent is selected from the group consisting of hydroxide of sodium, lithium, ammonia, NaCO 3 , NaHCO 3 , NaNO 3 , KOH, K 2 CO 3 , and KNO 3 8 The method of claim 7 wherein the precipitate is selected from the group consisting of Ru(OH) 4 , Ru(OH) 3 .xH 2 O, and RuO 2 .2H 2 O 9 A capacitor comprising an anode comprised of an amoφhous hydrous metal oxide, an electrolyte, and a cathode comprised of an amoφhous hydrous metal oxide 10 The capacitor of claim 9 wherein the hydrous metal oxide is comprised of a metal selected from the group consisting of ruthenium, rhodium, rhenium, osmium and indium 11 An electrode formed from the method of claim 2 12 An electrode formed from the method of claim 6 13 A method of forming a hydrous mixed metal oxide with a high energy density by a sol-gel process comprising the steps of hydrolyzing a metal halide in an aqueous solution and a reduction agent, controlling the pH of the solution so as to maintain a stable pH, and heating a resultant precipitate up to a temperature of approximately 200° Celsius wherein the resultant precipitate is an amoφhous, hydrous mixed metal oxide and has a capacitance density greater than 380 farads per gram 14 The method of claim 13 wherein the mixed metal halide comprises a metal selected from the group consisting of ruthenium, rhodium, rhenium, osmium, iridium and titanium, cobalt, tungsten, manganese, tantalum, molybdenum, and nickel 15 The method of claim 13 wherein the reduction agent is selected from the group consisting of hydroxide of sodium, lithium, ammonia, NaCO 3 , NaHCO 3 , NaNO 3 , KOH K 2 CO 3 , and KNO 3 16 An electrode material for electrochemical devices comprising amoφhous, hydrous ruthenium oxide having the formula RuO 2 xH 2 O, where x is a water content value which is between 0 2 and 2 0 17 The electrode materal of claim 16 wherein x is between 0 5 and 1 8 18 An electrode material for electrochemical devices compnsing amoφhous, hydrous mixed metal oxide having the general formula M x N y O zH 2 O, where x + y=l , M is metal selected from the group consisting of ruthenium, rhodium, rhenium, osmium, and iridium, N is selected from the group consisting of titanium, cobalt, tungsten, manganese, tantalum, molybdenum, iron, and nickel, and, where z is a water content value which is between 0 2 and 2 0 19 The electrode materal of claim 18 wherein z is between 0 5 and 1 8 AMENDED CLAIMS [received by the International Bureau on 10 September 1997 (10.09.97); original claims 1-8 and 11-19 cancelled; original claims 9 and 10 amended; new claim 20 added; (3 pages)] 2 ,4-ρentancd ionate ; controlling the pH of the solution by the addition of buffers so as to maintain a stable pH; and heating the precipitate in a temperature range between 50" and 200" Celsius to form the hydrous ruthenium oxide wherein the hydrous ruthenium oxide is amorphous and has a capacitance density greater than 380 farads per gram. 7. The method of claim 6 wherein the reduction agent is selected from the group consisting of hydroxide of sodium, lithium, ammonia, NaCO,, NaHCO,, NaNO 3 , KOH, K 2 CO j , and KNO 8. The method of claim 7 wherein the precipitate is selected from the group consisting of Ru(OH) 4 , Ru(OH) 3 .xH-O, and RuO 2 .2H 2 O. 9. A capacitor comprising: an anode comprising a first thin film of an amoφhous mixed metal oxide on a first substrate, wherein the first thin film of amorphous mixed metal oxide is noncrystalline; an electrolyte; and a cathode comprising a second thin film of an amorphous metal oxide on a second substrate, wherein the second thin film of amoφhous mixed metal oxide is noncrystalline. 10. The capacitor of claim 9 wherein the amorphous mixed metal oxide is comprised of a metal selected from the group consisting of ruthenium, rhodium, rhenium, iridium and titanium, cobalt, tungsten, manganese, tantalum, molybcndum, lead, or nickel and the first and second substrates are metal. 11. An electrode formed from the method of claim 2. 12. An electrode formed from the method of claim 6. 13. A method of forming a hydrous mixed metal oxide with a high energy density by a sol- gel process comprising the steps of: hydrolyzing a metal halide in an aqueous solution and a reduction agent; controlling the pH of the solution so as to maintain a stable pH; and heating a resultant precipitate up to a temperature of approximately 200" Celsius wherein the resultant precipitate is an amoφhous, hydrous mixed metal oxide and has a capacitance density greater than 380 farads per gram. 14. The method of claim 13 wherein the mixed metal halide comprises a metal selected from the group consisting of ruthenium, rhodium, rhenium, osmium, iridium and titanium, cobalt, tungsten, manganese, tantalum, molybdenum, and nickel. 15. The method of claim 13 wherein the reduction agent is selected from the group consisting of hydroxide of sodium, lithium, ammonia, NaC0 3 , NaHCO-,, NaNO 3 , KOH, K j C0 3 , and KNO 3 . 16. An electrode material for electrochemical devices comprising amoφhous, hydrous ruthenium oxide having the formula RuO 2 .xHjO, where x is a water content value which is between 0.2 and 2.0. 1 . The electrode material of claim 16 wherein x is between 0.5 and 1.8. 18. An electrode material for electrochemical devices comprising amorphous, hydrous mixed metal oxide having the general formula M,N,O.zH 2 O, where x + y = 1, M is metal selected from the group consisting of ruthenium, rhodium, rhenium, osmium, and iridium, N is selected from the group consisting of titanium, cobalt, tungsten, manganese, tantalum, molybdenum, iron, and nickel, and, where z is a water content value which is between 0.2 and 2.0. 19. The electrode material of claim 18 wherein 2 is between 0.5 and 1.8. 20. The capacitor of claim 9 wherein the amoφhous mixed metal oxide is comprised of a metal selected from the group consisting of ruthenium, rhodium, rhenium, iridium and titanium, cobalt, tungsten, mangane e, tantalum, molybendum, lead, or nickel and the first and second substrates are a carbanaceous material.

Inventors: JOW T RICHARD, ZHENG JIAN-PING, JOW, T., RICHARD, ZHENG, JIAN-PING
Applicants: US ARMY, THE UNITED STATES OF AMERICA
Application year: 1996
Main classification: H01G9
IPC codes: C01B13, C01G55, H01G9, H01M4