Method and apparatus for producing bulk quantities of...

Electric heating – Metal heating – By arc

Reexamination Certificate

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C219S121590, C219S121520, C219S121500, C427S255120, C427S255290, C423SDIG001

Reexamination Certificate

active

06580051

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention generally relates to a method and system for the production of submicron materials, and in particular to a method and system of synthesizing, in bulk quantities, nanosized powders, including nanocrystalline ceramics. Even more particularly, the present invention relates to a method and system for increasing the rate and thereby reducing the cost of the production of bulk quantities of nanosized powders by electrothermal gun synthesis.
2. Description of Related Art
Ceramic materials are used in a wide variety of applications, and generally have excellent heat resistance, corrosion resistance, and abrasion resistance, as well as unique electrical and optical properties. Ceramic material, as used herein, generally refers to an oxide, nitride, boride or carbide of a metal, or a mixture thereof. Very fine ceramic powders are used in a large number of industrial processes to introduce or modify material properties. These materials can pose difficulties in sintering but, when they are converted to ultrafine particles, particularly submicron crystalline particles, numerous traditional problems are avoided. Accordingly, several processes have been devised for fabricating ultrafine, or submicron, crystalline materials, such as those of 1-500 nanometer size, referred to herein as “nanosized,” “nanocrystalline,” “nanoparticles,” and the like.
Techniques for producing nanocrystalline materials generally fall into one of three categories, namely, mechanical processing, chemical processing, or physical (thermal) processing. In mechanical processes, fine powders are commonly made from large particles using crushing techniques such as a high-speed ball mill. There are several disadvantages with this approach. Sometimes metallic powders and highly reactive metals are combined with and subjected to such milling, which can pollute the material with a nanocrystalline alloy. Fragmented powders produced by mechanical processes can also result in particles of inconsistent shapes and sizes, and are often coarse and so not suited for high-performance applications.
With chemical processes, nanocrystalline materials are created from a reaction that precipitates particles of varying sizes and shapes, using a family of materials known as organometallics (substances containing combinations of carbon and metals bonded together). It is difficult, however, to produce ultrafine ceramics using organometallics without introducing excess carbon, or nitrogen (or both) into the final composition. Solution-gelation (sol-gel) ceramic production is similar to organometallic processes, but sol-gel materials may be either organic or inorganic. Both approaches involve a high cost of raw materials and capital equipment, limiting their commercial acceptance.
One of the earliest forms of physical, or thermal, processing, involves the formation and collection of nanoparticles through the rapid cooling of a supersaturated vapor (gas phase condensation). See, e.g., U.S. Pat. No. 5,128,081. In that example, a raw metallic material is evaporated into a chamber and raised to very high temperatures, and then oxygen is rapidly introduced. See also U.S. Pat. No. 5,851,507, in which a carrier medium is mixed with precursor material which is vaporized and subsequently rapidly quenched.
Thermal processes create the supersaturated vapor in a variety of ways, including laser ablation, plasma torch synthesis, combustion flame, exploding wires, spark erosion, electron beam evaporation, sputtering (ion collision). In laser ablation, a high-energy pulsed laser is focused on a target containing the material to be processed. The high temperature of the resulting plasma (greater than 10,000° K) vaporizes the material so quickly that the rest of the source (any carrier and quenching gases) can operate at room temperature. The process is capable of producing a variety of nanocrystalline ceramic powders on the laboratory scale, but it has the great disadvantage of being extremely expensive due to the inherent energy inefficiency of lasers, and so it not available on an industrial scale.
The use of combustion flame and plasma torch to synthesize ceramic powders has advanced more toward commercialization. In both processes, the precursor material can be a solid, liquid or gas prior to injection into the flame or torch, under ambient pressure conditions (the most common precursor state is a solid material). The primary difference between the two processes is that the combustion flame involves the use of an oxidizing or reducing atmosphere, while the plasma torch uses an inert gas atmosphere. Each of these processes requires relatively expensive precursor chemicals, such as TiCl
4
for the production of TiO
2
by the flame process, or TiC and TiB
2
by the plasma process. A feature of both methods is the highly agglomerated state of the as-synthesized nanocrystalline ceramic powders. While for many applications the agglomeration of the powders is of little significance, there are situations where it is a shortcoming. Loosely agglomerated nanoparticle powders are produced in the combustion flame method of U.S. Pat. No. 5,876,683.
In the plasma process, reactants or feed materials are delivered to a plasma jet produced by a plasma torch. See generally, U.S. Pat. Nos. 4,642,207 and 5,486,675. Alternatively, the feed material may be delivered to the plasma stream by arc vaporization of the anode. The anode is normally metallic but may be a metal-ceramic composite.
An improved plasma torch process is described in U.S. Pat. No. 5,514,349. That process can produce non-agglomerated ceramic nanocrystalline powders starting from metalorganic precursors, and uses rapid thermal decomposition of a precursor/carrier gas stream in a hot tubular reactor combined with rapid condensation of the product particle species on a cold substrate. Plasma torch processes, while gaining some limited commercial acceptance, are still energy inefficient and often involve materials which are extraneous to the products being produced. For example, in the '349 patent, a working gas must be heated by the plasma arc, which is wasted energy. Also, since the product particles are suspended in the hot process gas stream, it is necessary to quench not just the particles but the process stream as well. The multiple gases used (the reaction gas, quench gas, and passivating gas) are either wasted, or must be separated for reuse.
Another apparatus for producing nanosized particles is the exploding wire device. A conventional exploding wire device is illustrated in
FIG. 5. A
pulsed current discharge is driven through a small diameter wire that is typically on the order of 0.1 mm. The resulting joule heating of the wire vaporizes and ionizes the wire resulting in plasma which expands radially. The nearly cylindrical plasma contact surface which expands into the ambient gas, undergoes a reaction with the gas and subsequently cools. The mixing process relies on molecular diffusion and the cooling process is nearly isentropic. Production rates are typically only a few milligrams owning to the small diameter wire necessary for complete vaporization.
Another device that builds on the exploding wire method is a conventional capillary plasma device, shown in FIG.
6
. Conventional capillary plasma devices produce hydrocarbon-based plasmas that are used to ignite explosives because the plasma will not negatively react with the explosive. The capillary plasma device consists of two non-eroding electrodes positioned at the ends of a non-conducting bore with one open end. A fuse wire is connected between the electrodes. The process begins with an electrical discharge that explosively vaporizes and ionizes the fuse wire between the two electrodes. The discharge is maintained by the erosion and subsequent ionization of the liner to produce a dense plasma inside the bore which then exits from the open end of the device. The sealed end or breech of the gun must be capable of withstanding extremely high pressures in the order of 1

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