The present invention relates generally to metallurgy, and, more particularly, to a method and apparatus for containing a metal melt while it is processed as a semi-solid thixotropic metallic slurry and for ejecting the thixotropic metallic slurry once it is processed.
The present invention relates in general to an apparatus which is constructed and arranged for producing an “on-demand” semi-solid material for use in a casting process. Included as part of the overall apparatus are various stations which have the requisite components and structural arrangements which are to be used as part of the process. The method of producing the on-demand semi-solid material, using the disclosed apparatus, is included as part of the present invention.
More specifically, the present invention incorporates a high temperature and corrosion resistant container to hold the semi-solid material during processing and an electromagnetic ejection system to facilitate the transference of the semi-solid material from the container after processing. Also included are structural arrangements and techniques to discharge the semi-solid material directly into a casting machine shot sleeve. As used herein, the concept of “on-demand” means that the semi-solid material goes directly to the casting step from the vessel where the material is produced. The semi-solid material is typically referred to as a “slurry” and the slug which is produced as a “single shot” is also referred to as a billet.
It is well known that semi-solid metal slurry can be used to produce products with high strength, leak tight and near net shape. However, the viscosity of semi-solid metal is very sensitive to the slurry's temperature or the corresponding solid fraction. In order to obtain good fluidity at high solid fraction, the primary solid phase of the semi-solid metal should be nearly spherical.
In general, semi-solid processing can be divided into two categories; thixocasting and rheocasting. In thixocasting, the microstructure of the solidifying alloy is modified from dendritic to discrete degenerated dendrite before the alloy is cast into solid feedstock, which will then be re-melted to a semi-solid state and cast into a mold to make the desired part. In rheocasting, liquid metal is cooled to a semi-solid state while its microstructure is modified. The slurry is then formed or cast into a mold to produce the desired part or parts.
The major barrier in rheocasting is the difficulty to generate sufficient slurry within preferred temperature range in a short cycle time. Although the cost of thixocasting is higher due to the additional casting and remelting steps, the implementation of thixocasting in industrial production has far exceeded rheocasting because semi-solid feedstock can be cast in large quantities in separate operations which can be remote in time and space from the reheating and forming steps.
In a semi-solid casting process, generally, a slurry is formed during solidification consisting of dendritic solid particles whose form is preserved. Initially, dendritic particles nucleate and grow as equiaxed dendrites within the molten alloy in the early stages of slurry or semi-solid formation. With the appropriate cooling rate and stirring, the dendritic particle branches grow larger and the dendrite arms have time to coarsen so that the primary and secondary dendrite arm spacing increases. During this growth stage in the presence of stirring, the dendrite arms come into contact and become fragmented to form degenerate dendritic particles. At the holding temperature, the particles continue to coarsen and become more rounded and approach an ideal spherical shape. The extent of rounding is controlled by the holding time selected for the process. With stirring, the point of “coherency” (the dendrites become a tangled structure) is not reached. The semi-solid material comprised of fragmented, degenerate dendrite particles continues to deform at low shear forces.
When the desired fraction solid and particle size and shape have been attained the semi-solid material is ready to be formed by injecting into a die-mold or some other forming process. Solid phase particle size is controlled in the process by limiting the slurry creation process to temperatures above the point at which the solid phase begins to form and particle coarsening begins.
It is known that the dendritic structure of the primary solid of a semi-solid alloy can be modified to become nearly spherical by introducing the following perturbation in the liquid alloy near liquidus temperature or semi-solid alloy:
While using high-speed mechanical stirring within an annular thin gap can generate high shear rate sufficient to break up the dendrites in a semi-solid metal mixture, the thin gap becomes a limit to the process's volumetric throughput. The combination of high temperature, high corrosion (e.g. of molten aluminum alloy) and high wearing of semi-solid slurry also makes it very difficult to design, to select the proper materials and to maintain the stirring mechanism.
Prior references disclose the process of forming a semi-solid slurry by reheating a solid billet, formed by thixocasting, or directly from the melt using mechanical or electromagnetic stirring. The known methods for producing semi-solid alloy slurries include mechanical stirring and inductive electromagnetic stirring. The processes for forming a slurry with the desired structure are controlled, in part, by the interactive influences of the shear and solidification rates.
In the early 1980's, an electromagnetic stirring process was developed to cast semi-solid feedstock with discrete degenerate dendrites. The feedstock is cut to proper size and then remelt to semi-solid state before being injected into mold cavity. Although this magneto hydrodynamic (MHD) casting process is capable of generating high volume of semi-solid feedstock with adequate discrete degenerate dendrites, the material handling cost to cast a billet and to remelt it back to a semi-solid composition reduces the competitiveness of this semi-solid process compared to other casting processes, e.g. gravity casting, low-pressure die-casting or high-pressure die-casting. Most of all, the complexity of billet heating equipment, the slow billet heating process and the difficulties in billet temperature control have been the major technical barriers in semi-solid forming of this type.
The billet reheating process provides a slurry or semi-solid material for the production of semi-solid formed (SSF) products. While this process has been used extensively, there is a limited range of castable alloys. Further, a high fraction of solids (0.7 to 0.8) is required to provide for the mechanical strength required in processing with this form of feedstock. Cost has been another major limitation of this approach due to the required processes of billet casting, handling, and reheating as compared to the direct application of a molten metal feedstock in the competitive die and squeeze casting processes.
In the mechanical stirring process to form a slurry or semi-solid material, the attack on the rotor by reactive metals results in corrosion products that contaminate the solidifying metal. Furthermore, the annulus formed between the outer edge of the rotor blades and the inner vessel wall within the mixing vessel results in a low shear zone while shear band formation may occur in the transition zone between the high and low shear rate zones. There have been a number of electromagnetic stirring methods described and used in preparing slurry for thixocasting billets for the SSF process, but little mention has been made of an application for rheocasting.
The rheocasting, i.e., the production by stirring of a liquid metal to form semi-solid slurry that would immediately be shaped, has not been industrialized so far. It is clear that rheocasting should overcome most of limitations of thixocasting. However, in order to become an industrial production technology, i.e., producing stable, deliverable semi-solid slurry on-line (i.e., on-demand) rheocasting must overcome the following practical challenges: cooling rate control, microstructure control, uniformity of temperature and microstructure, the large volume and size of slurry, short cycle time control and the handling of different types of alloys, as well as the means and method of transferring the slurry to a vessel and directly from the vessel to the casting shot sleeve.
One of the ways to overcome above challenges, according to the present invention, is to apply electromagnetic stirring of the liquid metal when it is solidified into semi-solid ranges. Such stirring enhances the heat transfer between the liquid metal and its container to control the metal temperature and cooling rate, and generates the high shear rate inside of the liquid metal to modify the microstructure with discrete degenerate dendrites. It increases the uniformity of metal temperature and microstructure by means of the molten metal mixture. With a careful design of the stirring mechanism and method, the stirring drives and controls a large volume and size of semi-solid slurry, depending on the application requirements. The stirring helps to shorten the cycle time by controlling the cooling rate, and this is applicable to all type of alloys, i.e., casting alloys, wrought alloys, MMC, etc.
while propeller type mechanical stirring has been used in the context of making a semi-solid slurry, there are certain problems and limitations. For example, the high temperature and the corrosive and high wearing characteristics of semi-solid slurry make it very difficult to design a reliable slurry apparatus with mechanical stirring. However, the most critical limitation of using mechanical stirring in rheocasting is that its small throughput cannot meet the requirements production capacity. It is also known that semi-solid metal with discrete degenerated dendrite can also be made by introducing low frequency mechanical vibration, high-frequency ultra-sonic waves, or electric-magnetic agitation with a solenoid coil. While these processes may work for smaller samples at slower cycle time, they are not effective in making larger billet because of the limitation in penetration depth. Another type of process is solenoidal induction agitation, because of its limited magnetic field penetration depth and unnecessary heat generation, it has many technological problems to implement for productivity. Vigorous electromagnetic stirring is the most widely used industrial process permits the production of a large volume of slurry. Importantly, this is applicable to any high-temperature alloys.
Two main variants of vigorous electromagnetic stirring exist, one is rotational stator stirring, and the other is linear stator stirring. With rotational stator stirring, the molten metal is moving in a quasi-isothermal plane, therefore, the degeneration of dendrites is achieved by dominant mechanical shear. U.S. Pat. No. 4,434,837, issued Mar. 6, 1984 to Winter, describes an electromagnetic stirring apparatus for the continuous making of thixotropic metal slurries in which a stator having a single two pole arrangement generates a non-zero rotating magnetic field which moves transversely of a longitudinal axis. The moving magnetic field provides a magnetic stirring force directed tangentially to the metal container, which produces a shear rate of at least 50 sec−1 to break down the dendrites. With linear stator stirring, the slurries within the mesh zone are re-circulated to the higher temperature zone and remelted, therefore, the thermal processes play a more important role in breaking down the dendrites. U.S. Pat. No. 5,219,018, issued Jun. 15, 1993 to Meyer, describes a method of producing thixotropic metallic products by continuous casting with polyphase current electromagnetic agitation. This method achieves the conversion of the dendrites into nodules by causing a refusion of the surface of these dendrites by a continuous transfer of the cold zone where they form towards a hotter zone.
A part formed according to this invention will typically have equivalent or superior mechanical properties, particularly elongation, as compared to castings formed by a fully liquid-to-solid transformation within the mold, the latter castings having a dendritic structure characteristic of other casting processes.
It is known in the art that in addition to being relatively dense and heavy and to holding a great deal of heat, some molten metals are also quite corrosive. Aluminum, for example, is extremely corrosive in its molten state. A crucible or vessel for containing such a molten metal must necessarily be strong as well as resistant to corrosion and thermal degradation. If the metal is to be magnetically stirred as part of a process for forming a thixotropic semi-solid metal slurry in the crucible, it is important that the crucible be as transparent as possible to lines of magnetic force so that they may pass through the crucible with minimal obstruction.
It is also important to be able to readily remove the thixotropic metal slurry once it has been processed in the crucible. Due to its thixotropic nature, the slurry is maintained at a temperature just above its solidus or coherency point. Therefore, mechanical manipulation is problematic, since a slight increase in temperature through mechanical contact could radically lower the viscosity of the slurry, and a slight decrease in temperature could provoke the formation of a solid skin around the slurry or even bulk crystallization of the slurry.
Another problem with ejection of the slurry from the crucible is that thixotropic semi-solid metal slurries tend to adhere to the inner surface of crucibles. Drag at the crucible inner surface reduces the shear on the thixotropic slurry, producing a region of higher viscosity slurry adjacent the crucible inner surface. Also, the slurry tends to interlock with any present crucible porosity, further contributing to adherence to the crucible.
Moreover, once the thixotropic semi-solid slurry is removed from the crucible, there is the problem of residual metallic deposits on the crucible walls. These can be a source of impurities, such as insoluble metallic oxides. Further, if the crucible must handle more than one metallic composition, any residual metal can of itself be an impurity.
There is therefore a need for a crucible system capable of containing a molten metal billet for thixotropic processing and also capable of readily and cleanly ejecting the processed thixotropic semi-solid slurry. The present invention addresses this need.
The present invention relates to a container system including a vessel for holding a thixotropic semi-solid metallic slurry during its formation and an ejection system for cleanly discharging the processed thixotropic semi-solid metallic slurry. One form of the present invention includes a crucible made of a chemically and thermally stable material (such as graphite or a ceramic) crucible defining a mixing volume and having a movable bottom portion mounted on a piston. A liquid metal precursor is transferred into the crucible and vigorously stirred and controlledly cooled to form a thixotropic semi-solid billet. Once the billet is formed, the piston is activated to push the bottom of the crucible through the mixing volume to discharge the billet. The billet is pushed from the crucible into a shot sleeve and immediately placed in a mold (such as by injection) and molded into a desired form.
Another form of the present invention includes a chemically and thermally stable crucible having an open top and defining a mixing volume. An electromagnetic coil is positioned proximate the crucible. A liquid metal precursor is transferred into the crucible, vigorously stirred and controlledly cooled to form a thixotropic semi-solid billet. The electromagnetic coil is actuated by a high frequency AC current, inducing eddy currents in the outer surface of the billet to produce a layer of liquid metal. The electromagnetic coil also induces a radially inwardly directed compressive electromotive force on the billet. The billet, thereby compressed and having a lubricating melted outer layer, may be easily removed from the crucible onto the shot sleeve by means such as pushing the billet out with a plunger or tilting the crucible.
Yet another form of the present invention includes a chemically and thermally stable crucible formed from two half crucibles. The crucible is split by a plane oriented in parallel with the crucible central axis. The crucible is held together by a clamp, bolted flanges, or the like. A liquid metal precursor is transferred into the crucible, vigorously stirred and controlledly cooled to form a thixotropic semi-solid billet. The billet is discharged from the crucible by separating the two halves.
One object of the present invention is to provide an improved system for producing thixotropic semi-solid metallic slurries. Related objects and advantages of the present invention will be apparent from the following description.
For the purposes of promoting an understanding of the principles of the invention, reference will now be made to the embodiment illustrated in the drawings and specific language will be used to describe the same. It will nevertheless be understood that no limitation of the scope of the invention is thereby intended, and alterations and modifications in the illustrated device, and further applications of the principles of the invention as illustrated therein are herein contemplated as would normally occur to one skilled in the art to which the invention relates.
FIGS. 1 and 2A–B illustrate a first embodiment of the present invention, a crucible assembly 10 for containing a quantity of molten metal, such as molten aluminum, for metallurgical processing. The crucible assembly 10 includes a refractory vessel or crucible 20. Crucible 20 is preferably cylindrical in shape, and is more preferably a right circular cylinder, although any convenient cross sectional shape (such as hexagonal or octagonal, for example) may be chosen. Additionally, the crucible 20 may include a draft angle of up to about 10°, with a draft angle of about 2° preferred. The inclusion of a draft angle aids in the emptying of the crucible 20, but likewise reduces the working volume of the crucible 20; therefore, a draft angle of less than about 10° is preferred. The crucible 20 preferably has a substantially flat circular bottom portion 22 and cylindrical sidewall 24 connected to the bottom portion 22 defining a right angle. The sidewall 24 has an outer surface 26 and an inner surface 28. A crucible inner volume 30 is defined by the bottom portion 22 and the inner surface 28 extending therefrom. The inner diameter of the crucible 20 is determined by the inner diameter of the receiving shot sleeve 63A (see
The crucible 20 is preferably formed from a material suitable for containing a corrosive liquid metal at temperatures substantially above its melting point (for example, liquid aluminum at 700–800° C.) The crucible 20 is more preferably formed from a material such as graphite, stainless steel, or a suitable ceramic or ceramic composite composition. Since the crucible 20 must contain corrosive molten metals at elevated temperatures, it must necessarily be resistant to corrosion and have high strength at elevated temperatures. During thixotropic processing, the molten metals will be magnetically stirred, so the crucible 20 must also offer low resistance to penetration by the electromagnetic stirring fields. It is also preferred that the crucible 20 be a good thermal conductor (at least radially) so the liquid metal can be quickly and controlledly cooled by removal of heat from the sidewall outer surface 26.
One preferred crucible 20 material is a non-magnetic stainless steel composition (i.e., austenitic stainless steel). Stainless steels have relatively high thermal conductivity and high strength at elevated temperatures. Stainless steels can be coated with a ceramic or alloy layer to become resistant to corrosion from molten aluminum. Stainless steel compositions can be chosen to be non-magnetic, a property preferred for the crucible 20 since it is preferred that the crucible 20 have low resistance to penetration by magnetic flux. The high strength and toughness of a stainless steel produce a durable crucible 20.
It is possible to increase the corrosion resistance and decrease the adhesion of metal to the crucible inner wall 28 of a crucible 20 by adding an interior layer of corrosion resistant ceramic material, such as glassy-phase free polycrystalline alumina, zirconia or boron nitride. Some alloys, such as nickel-aluminum compositions, have also proven useful as crucible 20 coatings. The coating is preferably about 0.1 to 2 mm. thick. Alternately, a molten-aluminum-resistant graphitic or ceramic insert or sleeve 25 may be used with a stainless steel crucible 20 to provide corrosion resistance see
Graphite is another preferred crucible 20 material since, although it is porous, it is not wet by molten aluminum. Preferred grades of graphite include SES G10 and SES G20, although other convenient grades of graphite may be used. It should be noted that in general the specific characteristics of a given alloy composition may mandate the use of a different grade of graphite (or any crucible material) as the crucible 20. In other words, the specific physical properties required of a crucible 20 are a function of, among other parameters, the alloy composition desired to be contained as a liquid phase therein. Other such factors influencing crucible design include, but are not limited to, the range of operating temperatures, the speed of heating and/or cooling, the pH of the material to be contained in the crucible, the reactivity of the material with the crucible material, and cost.
Graphite is resistant to corrosion and with strength that increases with increasing temperature. Graphite also has a relatively low thermal expansion coefficient, high thermal shock resistance (due to a combination of high thermal conductivity and low Young's modulus) and high dimensional stability, making it attractive as a material for forming pieces that will be repeatedly thermally cycled. Graphite is an anisotropic material, best modeled as stacked planes (basal planes) of carbon atoms, with the bonds within the planes being extremely strong (about 9×1012 dynes/cm2 or 130×106 p.s.i.), stronger than the covalent bonds in diamond and contributing to a high longitudinal strength. The bonds between the planes are not as strong, and contribute to lower transverse strength. As used herein, “longitudinal” indicates a direction substantially within or parallel to the basal graphite plane and “transverse” indicates a direction substantially perpendicular to the basal graphite plane. The anisotropic physical properties of graphite may be exploited through the choice of graphite forming techniques. For example, extrusion tends to aligh the anisotropic graphite crystallites along the axis of extrusion, resulting in a graphite piece with widely varying physical properties in the axial and transverse directions, while hot pressing from a powder precursor can yield a graphite piece with nearly isotropic physical properties. Careful attention to forming techniques allows fairly precise control of the degree of isotropy of the physical properties of the resulting graphite body.
Graphite also has the interesting physical property of actually increasing in strength with increasing temperature to about 2500° C. At about 800° C., a typical polycrystalline graphite member has a strength of 2800 dynes/cm2. in the longitudinal direction and of about 1850 dynes/cm2. in the transverse direction. The thermal conductivity of graphite is likewise anisotropic, with the thermal conductivity within the basal plane being about 1.3 cal/cm.sec. ° C. at 800° C. and across basal planes being about 0.01 cal/cm.sec. ° C. at 800° C. The thermal conductivity of polycrystalline graphite can therefore be tailored to be isotropic within a graphite body or highly anisotropic, as a function of the orientation of the constituent graphitic grains. The magnetoresistivity of graphite is isotropic and at elevated temperatures is negligible.
The primary drawback for using graphite as a crucible 20 material is that it is more brittle than steel and subject to cracking from impact or wear damage. This concern may be addressed by cladding or otherwise reinforcing the graphite crucible 20.
Another preferred material for forming the crucible is a ceramic composition resistant to attack by molten aluminum (such as polycrystalline Al2O3 formed without a glassy grain-boundary phase). Ceramic materials can be found that offer high strength at elevated temperatures, resistance to corrosion, and low magnetoresistivity. While many ceramic materials have low to moderate thermal conductivity, some can be found that have sufficiently high thermal conductivity to allow quick and controlled cooling of the molten metal. Nonporous ceramics or those with pores having very small diameters are preferred as crucibles 20, to decrease the adhesion of the cooling metal to the crucible inner wall 28. Like graphite, ceramic compositions tend to have the disadvantage of being brittle, although (like graphite) they may be reinforced, either through the addition of a reinforcing cladding or casing layer or as a ceramic composite material. Ceramic materials also have the disadvantage of having low thermal conductivities, making them (as a class) less attractive as crucibles 20, although certain ceramic materials and/or composites may be found with relatively high thermal conductivities.
The crucible 20 is preferably formed as a monolithic piece, but may also be formed from 2 or more pieces. For instance, FIGS. 3 and 13–15 show a crucible 20 formed from a pair of “clam-shell” crucible halves.
In operation, actuation of the solenoid 64B induces rapidly alternating eddy currents in the outer skin 68B of an electrically conductive slurry billet 60B contained in the crucible 20B. The eddy currents give rise to Joule heating sufficient to melt the outer skin 68B and to break its possible bonding with the crucible 20B. At the same time, the electromagnetic field also generates a squeezing force on the slurry-billet 60B to separate it from the crucible 20B. Once the outer skin 68B is melted, the crucible 20B is tilted to discharge the slurry billet 60B therefrom with the molten metal skin 68B providing lubrication for the slurry billet 60B discharge as well as substantially preventing adhesion of the slurry billet 60B to the inner crucible wall 28B (thereby minimizing distortion of the slurry billet 60 and build-up of metal residue within the crucible 20B.) Preferably, discharge of the slurry billet 60B is performed gravitationally; i.e. the crucible is tilted to allow the slurry billet 60B to slide out. This is illustrated in
In operation, a variation of the technique known as electromagnetic forming is used to eject a billet 60C from the crucible 20C. Electromagnetic forming is a well-known metallurgical technique in which a burst of electromagnetic energy created by a brief high frequency discharge of high voltage electric energy through an inductive coil is used to generate an electromotive force. It comprises two variants, known respectively under the name of “magnetoforming” and “electroforming”. In magnetoforming, an electromagnetic field propels a workpiece to be shaped (which must be at least partially electrically conducting metal) at high speed against another piece forming a die whose shape it assumes. In electroforming (also known as electro-hydraulic forming), an electric pulse is applied to an explosive wire placed in an insulating and incompressible medium. The explosion creates a shock wave that is transmitted through the incompressible medium to the piece to be shaped so as to cause expansion thereof.
In the magnetoforming process, an electromagnetic field is produced by passing a time varying electric current through a coil (the workcoil). The current in the workcoil can be provided by the discharge of a capacitor (or more typically by a bank of capacitors) resulting in a pulse output. The workpiece can be maintained at a temperature so that it is somewhat malleable to aid the forming process, although this is not necessary. Various methods and apparatus are known for forming conductive materials through the use of electromagnetic pulses. Conventionally, such apparatus establishes a magnetic field of sufficiently high intensity and duration to create a high amperage electrical current pulse which when passed through a conductor in the form of a coil creates a pulse magnetic field of high intensity in the proximity of one or more selectively positioned conductive workpieces. A current pulse is thereby induced in the workpieces that interacts with the magnetic field to produce a force acting on the work pieces. When high magnitudes of electrical current are passed through the solenoid or coil, very high pressures are applied to the electrically conductive workpiece, and the electrically conductive workpiece is reduced in transverse dimensions.
In the instant case, a high voltage pulse is passed through the solenoid 64C to induce a pulse of current flowing in the opposite direction within the electrically conductive slurry billet 60C. As described above, very high electromagnetic pressures are generated in the transverse (radially inward) direction on the slurry billet 60C. Since the solenoid 64C and the crucible 20C (and therefore the slurry billet 60C within the crucible 20C) are not oriented coaxially, the compressive forces acting on the slurry billet 60C will not be radially symmetrically balanced, and a resultant axial force will be generated, forcing the deformable billet 60C out of the crucible 20C. This is roughly analogous to squeezing a wet bar of soap until it squirts out of your hand. Alternately, the solenoid 64C may be positioned coaxially with the crucible 20C. Upon pulsed actuation of the solenoid, the slurry billet 60C will be subjected to substantially symmetrical radially compressive forces. Since the slurry billet 60C is thixotropic and therefore deformable, the radially compressive forces will squeeze the slurry billet 60C, resulting in a net axial force upon the slurry billet 60C. Since the crucible 20C has a bottom portion 22C but no top portion, the net effect is that the slurry billet 60C will be squeezed from the crucible 20C. The crucible 20C is also preferably tilted to direct the emerging slurry billet 60C onto a desired resting surface, such as a shot sleeve or into a die.
In operation, the solenoid 64D produces an electrical field pulse, inducing a pulse of current flowing in the opposite direction in the portion of the slurry billet 60D proximate the bottom portion 22D of the crucible 20D. The compressive forces so generated on the slurry billet 60D are therefore directed parallel to the crucible central axis of rotation 70D and away from the bottom portion 22D, and so urge the slurry billet 60D out of the crucible 20D.
In operation, the solenoid 64E of the present embodiment combines the effects of the solenoids 64C, 64D of the fourth and fifth embodiments. When actuated, the solenoid 64E produces a high voltage electrical field pulse, inducing a pulse of current flowing in the opposite direction in the slurry billet 60E. The compressive forces so generated on the slurry billet 60E are therefore directed inwardly on the side and bottom surfaces of the slurry billet 60E. The combination of forces acting on the thixotropic slurry billet 60E produce a net force vector directed in a substantially axial direction away from the bottom portion 22E to urge the slurry billet 60E out of the crucible 20E.
In operation, the cleaning brush 76F is rotated sufficiently rapidly to impart enough kinetic energy to any residual metal adhering to the crucible 20F to cause its removal. The crucible 20F is preferably opened at a fixed angle to better facilitate cleaning. Preferably, the crucible 20F is cleaned after each cycle.
While the invention has been illustrated and described in detail in the drawings and foregoing description, the same is to be considered as illustrative and not restrictive in character, it being understood that only the preferred embodiment has been shown and described and that all changes and modifications that come within the spirit of the invention are desired to be protected.
The present Application is a divisional of U.S. patent application Ser. No. 10/160,726, filed Jun. 3, 2002 now U.S. Pat. No. 6,932,938, which is a continuation of U.S. patent application Ser. No. 09/585,296, filed Jun. 1, 2000 now U.S. Pat. No. 6,399,017, the contents of each application hereby being incorporated by reference in their entirety.
Number | Name | Date | Kind |
---|---|---|---|
972429 | Baird | Oct 1910 | A |
1506281 | Baily | Aug 1924 | A |
1776355 | Eppensteiner | Sep 1930 | A |
2215887 | Seigle et al. | Sep 1940 | A |
2758831 | Winter, Jr. | Aug 1956 | A |
3472502 | Schott | Oct 1969 | A |
3523785 | Gero | Aug 1970 | A |
3730257 | Haussner | May 1973 | A |
3735010 | Turpin | May 1973 | A |
3791015 | Lucenti | Feb 1974 | A |
3840364 | Flemings et al. | Oct 1974 | A |
3842895 | Mehrabian et al. | Oct 1974 | A |
3882923 | Alberny et al. | May 1975 | A |
3902544 | Flemings et al. | Sep 1975 | A |
3948650 | Flemings et al. | Apr 1976 | A |
3951651 | Mehrabian et al. | Apr 1976 | A |
3981351 | Dompass | Sep 1976 | A |
3995678 | Zavaras et al. | Dec 1976 | A |
4088295 | Medovar et al. | May 1978 | A |
4089680 | Flemings et al. | May 1978 | A |
4106956 | Bercovici | Aug 1978 | A |
4108643 | Flemings et al. | Aug 1978 | A |
4125364 | Stephens | Nov 1978 | A |
4174214 | Bennett et al. | Nov 1979 | A |
4229210 | Winter et al. | Oct 1980 | A |
4281263 | Virolleau et al. | Jul 1981 | A |
4321958 | Delassus | Mar 1982 | A |
4345637 | Flemings et al. | Aug 1982 | A |
4354831 | Shinkawa et al. | Oct 1982 | A |
4415374 | Young et al. | Nov 1983 | A |
4433715 | Smith | Feb 1984 | A |
4434837 | Winter et al. | Mar 1984 | A |
4434839 | Vogel | Mar 1984 | A |
4450893 | Winter et al. | May 1984 | A |
4457354 | Dantzig et al. | Jul 1984 | A |
4457355 | Winter et al. | Jul 1984 | A |
4463795 | Chielens et al. | Aug 1984 | A |
4465118 | Dantzig et al. | Aug 1984 | A |
4482012 | Young et al. | Nov 1984 | A |
4494461 | Pryor et al. | Jan 1985 | A |
4510987 | Collot | Apr 1985 | A |
4523624 | Dantzig et al. | Jun 1985 | A |
4524820 | Gullotti et al. | Jun 1985 | A |
4530404 | Vives | Jul 1985 | A |
4534003 | Manzione | Aug 1985 | A |
4555272 | Ashok et al. | Nov 1985 | A |
4565241 | Young | Jan 1986 | A |
4569218 | Baker et al. | Feb 1986 | A |
4607682 | Dantzig et al. | Aug 1986 | A |
4614225 | Ernst et al. | Sep 1986 | A |
4621676 | Steward | Nov 1986 | A |
4669529 | Evertz et al. | Jun 1987 | A |
RE32529 | Vives | Oct 1987 | E |
4709746 | Young et al. | Dec 1987 | A |
4712413 | Koch | Dec 1987 | A |
4729422 | Ernst et al. | Mar 1988 | A |
4774992 | George | Oct 1988 | A |
4838988 | Lang et al. | Jun 1989 | A |
4877079 | Long et al. | Oct 1989 | A |
4972334 | Yamabe et al. | Nov 1990 | A |
4989166 | Akasaka et al. | Jan 1991 | A |
5010501 | Arakawa | Apr 1991 | A |
5031108 | Fujita et al. | Jul 1991 | A |
5031127 | Fujita et al. | Jul 1991 | A |
5050114 | Lee | Sep 1991 | A |
5098487 | Brauer et al. | Mar 1992 | A |
5129035 | Saji et al. | Jul 1992 | A |
5135564 | Fujikawa et al. | Aug 1992 | A |
5219018 | Meyer | Jun 1993 | A |
5247988 | Kurzinski | Sep 1993 | A |
5265040 | Saji et al. | Nov 1993 | A |
5315530 | Gerhardt et al. | May 1994 | A |
5332200 | Gorin et al. | Jul 1994 | A |
5377119 | Backer et al. | Dec 1994 | A |
5402366 | Kihara et al. | Mar 1995 | A |
5408638 | Sagawa et al. | Apr 1995 | A |
5411686 | Hata | May 1995 | A |
5416795 | Kaniuk et al. | May 1995 | A |
5425048 | Heine et al. | Jun 1995 | A |
5432718 | Molvig et al. | Jul 1995 | A |
5499198 | Gaidos et al. | Mar 1996 | A |
5501266 | Wang et al. | Mar 1996 | A |
5529391 | Kindman et al. | Jun 1996 | A |
5539183 | Beckley | Jul 1996 | A |
5549732 | Dube et al. | Aug 1996 | A |
5553206 | Meshkat | Sep 1996 | A |
5572434 | Wang et al. | Nov 1996 | A |
5585067 | Leroy et al. | Dec 1996 | A |
5625579 | Hinsberg et al. | Apr 1997 | A |
5630466 | Garat et al. | May 1997 | A |
5640331 | Dahm et al. | Jun 1997 | A |
5661670 | Bharathan et al. | Aug 1997 | A |
5677844 | Kubo | Oct 1997 | A |
5701942 | Adachi et al. | Dec 1997 | A |
5732192 | Malin et al. | Mar 1998 | A |
5756017 | Togawa et al. | May 1998 | A |
5781581 | Fishman et al. | Jul 1998 | A |
5800640 | Yamamoto et al. | Sep 1998 | A |
5801969 | Nagahama | Sep 1998 | A |
5803154 | Sugawara et al. | Sep 1998 | A |
5819073 | Nakamura | Oct 1998 | A |
5838587 | Maisotsenko et al. | Nov 1998 | A |
5887640 | Brown et al. | Mar 1999 | A |
5899567 | Morris, Jr. | May 1999 | A |
5900080 | Baldi et al. | May 1999 | A |
5912823 | Grant | Jun 1999 | A |
5925199 | Shiina et al. | Jul 1999 | A |
5940309 | White et al. | Aug 1999 | A |
5953239 | Teixeira et al. | Sep 1999 | A |
5979534 | Shibata et al. | Nov 1999 | A |
5988259 | Welker et al. | Nov 1999 | A |
6003585 | Williams et al. | Dec 1999 | A |
6003590 | Pavlicevic et al. | Dec 1999 | A |
6009741 | Wagner | Jan 2000 | A |
6019930 | Baresich | Feb 2000 | A |
6021842 | Bulhoff et al. | Feb 2000 | A |
6064810 | Raad et al. | May 2000 | A |
6065526 | Kono | May 2000 | A |
6165411 | Adachi et al. | Dec 2000 | A |
6443216 | Lombard et al. | Sep 2002 | B1 |
6845809 | Norville et al. | Jan 2005 | B1 |
6932938 | Norville et al. | Aug 2005 | B1 |
20050151308 | Norville et al. | Jul 2005 | A1 |
Number | Date | Country |
---|---|---|
2424532 | Dec 1975 | DE |
19738821 | Mar 1999 | DE |
0005676 | Nov 1979 | EP |
411329 | Feb 1991 | EP |
0 701 002 | Mar 1996 | EP |
0701002 | Mar 1996 | EP |
0 710 515 | May 1996 | EP |
0 745 694 | Dec 1996 | EP |
0 841 406 | May 1998 | EP |
0 903 193 | Mar 1999 | EP |
0931607 | Jul 1999 | EP |
947262 | Oct 1999 | EP |
2 042 386 | Sep 1980 | GB |
2238498 | Jun 1991 | GB |
61-67555 | Apr 1986 | JP |
1-192446 | Aug 1989 | JP |
6-28939 | Feb 1994 | JP |
WO 9519237 | Jul 1995 | WO |
WO 9721509 | Jun 1997 | WO |
WO 9823403 | Jun 1998 | WO |
WO 9830346 | Jul 1998 | WO |
WO 9912678 | Mar 1999 | WO |
WO 9950007 | Oct 1999 | WO |
WO 0005015 | Feb 2000 | WO |
Number | Date | Country | |
---|---|---|---|
20050087917 A1 | Apr 2005 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 10160726 | Jun 2002 | US |
Child | 10989137 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 09585296 | Jun 2000 | US |
Child | 10160726 | US |