PLASMA APPARATUS FOR THE PRODUCTION OF HIGH QUALITY SPHERICAL POWDERS AT HIGH CAPACITY

Abstract

An apparatus and a process for the production at high capacity of high purity powders from a wire using a combination of plasma torches and induction heating are disclosed. The process has good productivity by providing a preheating system. A mechanism is included in the apparatus, which allows adjusting the position of the plasma torches and their angle of attack with respect to the wire, permitting to control the particle size distribution.

Claims

1. An apparatus to produce powder from a wire by plasma atomization, comprising: a device for preheating the wire; at least one plasma torch for heating the wire to atomization; and a chamber for cooling atomized particles to solid state.

2. The apparatus of claim 1, wherein the device for preheating the wire includes an induction coil.

3. The apparatus of claim 2, wherein there is provided a wire guide for coupling with induction to transfer heat to the wire, for instance mainly by conduction, radiation and convection.

4. The apparatus of claim 2, wherein there is provided a wire guide that is transparent to induction, whereby heat from the induction coil is transferred directly to the wire.

5. The apparatus of any one of claims 1 to 4, wherein there is provided a system for adjusting at least one of an angle and a distance of the torch with respect to the wire.

6. The apparatus of any one of claims 1 to 5, wherein there is provided a feeding device adapted to accommodate larger rods and wire diameters.

7. The apparatus of claim 6, wherein the feeding device is adapted to feed and straighten the larger rods and wire diameters.

8. The apparatus of any one of claims 1 to 7, wherein the wire diameters are between and 6 inclusively.

9. The apparatus of claim 3, wherein, if the wire is electrically conductive, the wire is also heated by direct coupling at the same time as it is heated by the wire guide

10. An apparatus to produce powder from a wire by plasma atomization, comprising: plasma torches for atomizing the wire, the plasma torches being adapted to swivel and rotate on a reactor; and a chamber for cooling atomized particles to solid state.

11. An apparatus to produce metallic powder from a wire by plasma atomization, comprising: plasma torches for atomizing the wire, the angle of the plasma torches with the wire being adapted to be adjusted for adjusting powder particle size distribution; and a chamber for cooling atomized particles to solid state.

12. A method to produce metallic powder from a wire by plasma atomization, comprising: feeding a wire or a rod; preheating the wire; heating the wire to atomization; and cooling atomized particles to solid state.

13. The method of claim 12, wherein the wire is preheated by induction heat, either directly or indirectly.

14. The method of claim 13, wherein there is provided a wire guide for reacting with induction to transfer heat to the wire, for instance mainly by radiation and convection.

15. The method of claim 13, wherein there is provided a wire guide that is transparent to induction, whereby heat from the inductions coil is transferred directly to the wire.

16. The method of any one of claims 12 to 15, wherein the rod has a diameter of or larger.

17. A method to produce metallic powder from a wire by plasma atomization, comprising: providing plasma torches, the plasma torches being adapted to swivel and rotate on a reactor; adjusting the position of the plasma torches on the reactor; using the plasma torches for atomizing the wire; and cooling atomized particles to solid state.

18. A method to produce metallic powder from a wire by plasma atomization, comprising: providing plasma torches for atomizing the wire, adjusting the angle of the plasma torches with respect to the wire for adjusting powder particle size distribution; using the plasma torches for atomizing the wire; and cooling atomized particles to solid state.

19. A powder produced by the method of any one of claims 12 to 18.

20. A powder produced by the apparatus of any one of claims 1 to 11.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0037] For a better understanding of the embodiments described herein and to show more clearly how they may be carried into effect, reference will now be made, by way of example only, to the accompanying drawings, which show at least one exemplary embodiment, and in which:

[0038] FIG. 1 is a general schematic representation of a plasma apparatus in accordance with an exemplary embodiment;

[0039] FIG. 2 is an enlarged detailed cross-sectional view of an induction coil and wire guide in accordance with an exemplary embodiment; and

[0040] FIG. 3 is an enlarged detailed cross-sectional view of a torch angle adjustment mechanism using ball flanges in accordance with an exemplary embodiment.

DESCRIPTIVE OF VARIOUS EMBODIMENTS

[0041] In order to produce high quality powders, controlling particle size and maximizing production rate in a plasma atomization reactor, an apparatus P and a method by which torch angle can be adjusted and wire preheated are hereby presented.

[0042] As illustrated in FIG. 1, a wire 2 provided on a metallic wire spool 1 is uncoiled therefrom and is then fed through a wire feeder and straightener 3. The straight wire 2 is fed through a pass-through flange 4. Then, the wire 2 enters into a wire guide 5 that is surrounded by an induction coil 6, prior to being atomized by three plasma torches 7 at the apex 8 thereof (the apex being the meeting point of the wire 2 and the three torches 7). The powder so produced passes through an aperture plate 9 and cools down as it falls down a reactor 10.

[0043] Once preheated, the wire 2 then reaches the apex 8, which is the zone where the wire 2 and the three plasma torches 7 meet for the atomization. The melting atomized particles freeze back to solid state as they fall down into a chamber of the reactor 10. The powder 11 is then pneumatically conveyed to a cyclone 12. The cyclone 12 separates the powder from its gas phase. The powder is collected at the bottom of a canister 14 while clean gas is then sent, via outlet 15, to a finer filtering system (not shown). The canister 14 can be isolated from the cyclone 12 by a gas-tight isolation valve 13.

[0044] Now turning our attention to the induction coil 6, the current apparatus P uses an induction coil to preheat the wire, which uses a single power supply and as the heat source does not encumber the apex zone. In this configuration, the wire preheating comes from a single uniform and compact source. Wire temperature can be controlled by adjusting induction power, which is a function of the current in the induction coil 6.

[0045] The induction preheating device is illustrated in FIG. 2. The pass-through flange 4 is made of a non electrically conductive material to ensure that the whole reactor is insulated from the coil. The pass-through flange 4 has two gas-tight holes equipped with compression fittings 21 used for passing the leads 22 of the induction coil 6 into the reactor 10.

[0046] The wire guide 5 can be designed to either react with or to be transparent to induction. For example, the wire guide 5 could be made of alumina, or silicon nitride, which are transparent to induction. It could also be made of silicon carbide or graphite, which react with induction. In the latter case, the hot wire guide, heated by induction, will radiate heat back into the wire 2.

[0047] For example, when the wire used was a 41 diameter Ti-6Al-4V Grade 23 ELI, the optimal induction frequency for this wire has been found to be between 270 and 290 kHz. The optimum frequency varies with the materials as well as the shape and dimension.

[0048] It is known that wire preheating can contribute to a capacity increase. However, the wire cannot be heated higher than its melting point in order to keep it under its solid state. Also, above a temperature of 1000 C., the alloy will convert from to phase, which will alter the rigidity of the wire. Depending on the configuration and the distance to be run by the wire, one might choose to maintain the mechanical properties of the wire of its a phase in order to keep the wire stiff and straight. For example, for a diameter Ti-6Al-4V Grade 23 ELI, since the wire shall not be brought higher than its melting point prior to atomization by plasma, the maximum capacity increase provided by wire preheating is 2 kg/h. This is equivalent to a capacity increase by a factor of three to four compared to a system without preheating.

[0049] FIG. 3 illustrates an adjustable torch angle mechanism, which includes swivelling ball flanges 30. The three plasma torches 7 are used to atomize the wire 2. These three torches 7 are herein attached to the body of the reactor head using swivelling bail flanges. The ball flanges 30 each include 2 flanges that fit into each other, namely a bottom flange 31 and an upper flange 32, which can swivel in accordance to each other. The bottom flange 31 that is connected to the reactor head is fixed, while the upper flange 32 can rotate up to an angle of 4 in every axis. Assuming the reactor head has been designed to have a nominal angle of 30, this means that the torches 7 could cover any angle between 26 and 34.

[0050] As varying the torch angle in relation to the wire 2 will also move the location of the apex 8 (the meeting point of the wire 2 and the three torches 7), this will have an effect on efficiency since the torches 7 have a constant length. In order to avoid such problem, longer torches coupled with spacers can be used. By having longer torches and multiple sizes of spacers, it is possible to attain any angle while keeping the location of the apex 8 at the same place.

[0051] Pivoting the torches 7 seems to have an important effect on the plasma atomization process. Prior systems stated that the optimal angle was to be fixed at 30. Although one could have been tempted to doubt this statement, being able to swivel the torches was not an obvious alternative. Therefore, going with a fixed angle was justified in the case of previous systems. The present arrangement suggests giving flexibility to the system by adding swiveling ball flanges 30 to the design.

[0052] Varying the angle of attack between the wire 2 and the plasma jets can affect the atomization in several ways. The major difference between plasma atomization in regards to traditional gas atomization is that heat is supplied by the jet. Therefore, there are two major considerations to take into account; namely heat transfer from the torch 7 to the wire 2, and the atomization by itself.

[0053] An important aspect for plasma atomization is the quality of heat transfer between the torches and the wire. Indeed, a proper alignment is required. The angle of attack also has an effect on the heat transfer, in two different ways; steeper (or smaller) the angle is, the surface area (A) that will exchange heat will increase. On the other hand, a shallower (higher) angle will promote a higher exchange coefficient (h).

Q=hAT [0054] where: Q is the heat transferred; [0055] h is the heat transfer coefficient; [0056] A is the surface area used for exchange; and [0057] T is the temperature difference between the wire and the torch.

[0058] The equation above is a classic heat transfer formula. The objective is to maximize the value of Q. The angle will have an effect on both the h and the A. From a heat transfer point of view, the optimal angle is the one that maximizes Q for a specific wire feed rate, size and material.

[0059] For atomization to occur, some micro droplets must form at the surface of the wire 2 (heating phase). Then a gas flow is used to detach that droplet from the wire 2 and carry it in suspension into the gas phase (atomization phase). It is known that high velocities are required to break the bond between the wire and the droplet. The following equation, taken from water atomization of aluminum literature [5], relates the mean particle size to angle between the melt stream and the argon jet:

D=C/V sin [0060] where: V is the plasma jet velocity; [0061] C is a global constant regrouping the different parameters and conditions; and [0062] is the angle between the melt stream and the plasma jet.

[0063] Although the application is slightly different, the concept is similar; the plasma jets herein replace the water jets and the jets are herein used for heating instead of cooling. Indeed, the formula shows that higher gas velocities are able to detach finer particles, which makes sense as it requires more force to detach a finer droplet from a melting wire. Interestingly, the angle seems to have a similar effect according to this formula.

[0064] It becomes clearer that in order to optimize the plasma atomization process, the angle has to be variable in order to adapt to different conditions. The two previous equations have shown how the parameters are intertwined, and that being able to vary the angles constitutes a significant feature of the present apparatus P.

[0065] The apparatus P thus includes inter alia (1) an inductive preheating of the wire to increase capacity; and (2) torches that are installed onto the reactor head, using swivelling ball flanges 30 which allow flexibility in regards to the angles that can be reached by the torch alignment, to allow for controlling particle size distribution (powder quality).

[0066] While the above description provides examples of the embodiments, it will be appreciated that some features and/or functions of the described embodiments are susceptible to modification without departing from the spirit and principles of operation of the described embodiments. Accordingly, what has been described above has been intended to be illustrative of the embodiments and non-limiting, and it will be understood by persons skilled in the art that other variants and modifications may be made without departing from the scope of the embodiments as defined in the claims appended hereto.

REFERENCES

[0067] [1] P. G. Tsantrizos, F. Allaire and M. Entezarian, Method of production of metal and ceramic powders by plasma atomization. U.S. Pat. No. 5,707,419 A, 13 Jan. 1998. [0068] [2] C. F. Yolton and J. H. Moll, Method for Atomizing Titanium. U.S. Pat. No. 4,544,404, 12 Mar. 1985. [0069] [3] M. Drouet, Methods and Apparatuses for Preparing Spheroidal Powders. Patent application WO2011054113, 12 Apr. 2011. [0070] [4] C. F. Yolton, Induction melting titanium in a vacuum or nonoxidzing atmosphere and treatment of an electric current. U.S. Pat. No. 5,084,091A, 28 Jan. 1992. [0071] [5] B. Verlinden and L. Froyen, Aluminium Powder Metallurgy, Training in Aluminium Application Technologies, vol. Advanced level 1, 1994.