Jetting device

Abstract

A jetting device includes: a fluid chamber connected to a nozzle and containing an electrically conductive liquid to be jetted out through the nozzle; a magnetic field generator arranged to create a magnetic field in the fluid chamber; a pair of electrodes contacting the electrically conductive liquid in the fluid chamber; and a controller arranged to control a flow of an electric current through the electrodes and the electrically conductive liquid. The magnetic field generator is arranged to create a rotating magnetic field in the fluid chamber.

Claims

1. A method of removing gas bubbles from a fluid chamber of a jetting device, the device comprising: a fluid chamber connected to a nozzle and containing an electrically conductive liquid to be jetted-out through the nozzle; a magnetic field generator arranged to create a magnetic field in the fluid chamber; a pair of electrodes contacting the electrically conductive liquid in the fluid chamber; and a controller arranged to control a flow of an electric current through the electrodes and the electrically conductive liquid, wherein the magnetic field generator includes at least one electromagnet, and wherein the magnetic field generator comprises a first magnet assembly arranged to create a magnetic field in a first direction normal to an axis of the nozzle, and a second magnet assembly arranged to create a magnetic field in a second direction normal to the axis of the nozzle and normal to said first direction, and the controller is arranged to modulate the magnetic fields created by the first and second magnet assemblies, the method comprising the step of controlling the magnetic field generator to rotate the magnetic field in the fluid chamber.

2. The method according to claim 1, further comprising a step of varying an angular velocity with which the magnetic field is rotated.

3. A jetting device comprising: a fluid chamber connected to a nozzle and containing an electrically conductive liquid to be jetted-out through the nozzle; a magnetic field generator arranged to create a magnetic field in the fluid chamber; a pair of electrodes contacting the electrically conductive liquid in the fluid chamber; and a controller arranged to control a flow of an electric current through the electrodes and the electrically conductive liquid, wherein the magnetic field generator is arranged to create a rotating magnetic field in the fluid chamber, wherein the magnetic field generator includes at least one electromagnet, and wherein the magnetic field generator comprises a first magnet assembly arranged to create a magnetic field in a first direction normal to an axis of the nozzle, and a second magnet assembly arranged to create a magnetic field in a second direction normal to the axis of the nozzle and normal to said first direction, and the controller is arranged to modulate the magnetic fields created by the first and second magnet assemblies.

4. The jetting device according to claim 3, wherein the controller is arranged to energize at least one of the electromagnets for generating a stationary magnetic field in an operating mode of the device.

5. The jetting device according to claim 3, wherein the magnetic field generator includes at least one permanent magnet.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) Embodiment examples will now be described in conjunction with the drawings, wherein:

(2) FIG. 1 is a schematic perspective view of a jetting device according to an embodiment of the invention:

(3) FIG. 2 is a longitudinal section of the jetting device shown in FIG. 1; and

(4) FIGS. 3 and 4 are schematic top plan views of the jetting device, illustrating the creation of a rotating magnetic field.

DETAILED DESCRIPTION OF THE DRAWINGS

(5) The jetting device shown in FIG. 1 comprises a crucible 10 that has the shape of an inverted truncated cone and tapers towards a cylindrical fluid chamber 12 that opens out into a nozzle 14 at the bottom end.

(6) The crucible 10 contains an electrically conductive liquid to be jetted, e.g. a molten metal. The walls of the crucible may contain heating elements (not shown) for keeping the metal in the molten state.

(7) The entire device is preferably kept in an inert gas atmosphere, e.g. an argon atmosphere, in order to prevent the molten metal from being oxidized.

(8) A magnetic field generator 16 is disposed around the outer periphery of the fluid chamber 12 and comprises four pairs of magnetic field concentrators 18 arranged at angular intervals of 90 in a horizontal plane, i.e. a plane orthogonal to the common central axis of the fluid chamber 12 and the nozzle 14. The field concentrators 18 are formed of a magnetisable material. In the example shown, each field concentrator 18 is surrounded by a solenoid 20, so that the field concentrator 18 forms the core of an electromagnet designated as A, B, C, and D, respectively.

(9) The solenoids 20 of the diametrically opposite electromagnets A and C are electrically connected in series, and the solenoids 20 of the other pair of electromagnets B and D are also electrically connected in series. Each pair of electromagnets is connected between an output terminal 22 and 24, respectively, and a ground terminal 26 of a controller 28.

(10) The field concentrator 18 of the electromagnet A includes an electrode 30 that is electrically isolated from the field concentrator 18 and passes through the entire length of the field concentrator and through the wall of the fluid chamber 12 so as to be in electric contact with the molten metal in the fluid chamber. The electrode 30 is connected to an output terminal 32 of the controller 28. The field concentrator 18 of the opposing electromagnet C has also an electrode 34 (FIG. 2) which is electrically connected to the ground terminal 26.

(11) Thus, the controller 28 may energize the pairs of electromagnets A, C and B, D, respectively, and may also control an electric current flowing through the electrodes 30 and 34 and through the electrically conductive liquid in the fluid chamber 12.

(12) In FIG. 2, it can be seen how the electrodes 30, 34 contact the conductive liquid which is designated by the reference numeral 36. When the jetting device is operated for jetting out droplets of the liquid 36 through the nozzle 14, the electromagnets B and D, which are not visible in FIG. 2, create a magnetic field that passes through the fluid chamber 12 in the direction normal to the plane of the drawing in FIG. 2. When a current pulse is passed through the electrodes 30, 34, the liquid in the fluid chamber 12 is subject to a Lorentz force that is directed downwardly and thus causes a droplet of the liquid 36, i.e. of the molten metal, to be jetted out from the nozzle. The electromagnets A and C may be switched off in this mode of operation.

(13) FIG. 3 shows a schematic cross-section of the fluid chamber 12 and illustrates a situation where the liquid 36 in the fluid chamber contains a gas bubble 38 (a bubble of argon gas in this example) that adheres to the peripheral wall of the fluid chamber. In order to detach and remove the bubble 38, the controller 28 is switched into a maintenance mode in which the electromagnets A and C are energized with a sinusoidal current I.sub.AC, as has been shown diagrammatically in FIG. 3. The electromagnets B and D are energized with a sinusoidal current I.sub.BD which has a phase offset of 90 relative to the current I.sub.AC. At a certain time instant t.sub.0, the current I.sub.AC is zero, and the current I.sub.BD has its maximum value, resulting in a magnetic field H that is created only by the electromagnets B and D and is therefore parallel to the common axis of these electromagnets. However, due to the modulation of the currents I.sub.AC and I.sub.BD the field H will rotate clock-wise in FIG. 3.

(14) FIG. 4 illustrates the situation at a time t.sub.1 where the current I.sub.AC has its maximum and the current I.sub.BD is zero. Consequently, the magnetic field H has been rotated by an angle of 90. In the course of time, the magnetic field H will continue to rotate and will thereby induce eddy currents in the liquid 36. These eddy currents induce secondary magnetic fields in the liquid 36, and due to interaction between these magnetic fields and the rotating field H, the liquid 36 is caused to co-rotate with the magnetic field H.

(15) The liquid 36 rotating in vortex fashion in the fluid chamber 12 is subject to centrifugal forces, with the result that the gas bubble 38, the density of which is considerably smaller than that of the liquid, is urged radially inwardly towards the central axis of the fluid chamber 12 and is thereby detached from the peripheral wall of the fluid chamber. Then, gravitational forces will cause the bubble 38 to float upwards into the crucible 10 and eventually to the top surface of the liquid. In this way, any gas bubbles in the fluid chamber 12 can be removed efficiently.

(16) The angular velocity with which the magnetic field H rotates may easily be varied by appropriately controlling the frequencies of the currents I.sub.AC and I.sub.BD.

(17) In the example that has been described so far, the stationary magnetic field that produces the Lorentz force in the operating mode of the device is created by the electromagnets A and C. In a modified example, this stationary magnetic field may be created by means of permanent magnets which may be attached to the outer ends of the field concentrators 18 of these electromagnets A, C. In the maintenance mode, it is preferable to remove these permanent magnets because the stationary magnetic field would counteract the vortex flow of the liquid that is to be induced with the rotating magnetic field.

(18) In yet another embodiment the field concentrators 18 of the electromagnets A and C may themselves be permanent magnets which create the static magnetic field. Then, in the maintenance mode, the electromagnets A and C would be energized to create a magnetic field with a polarity opposite to that of the permanent magnets. Consequently, at times where the current I.sub.AC has its maximum, the magnetic field of the permanent magnets will be largely suppressed. The current curve for the current curve I.sub.AC may be offset such that the current oscillates between zero and the maximum value. The current I.sub.BD is caused to oscillate about zero with the same amplitude as the current I.sub.AC, so that the combined effect of the four electromagnets and the permanent magnets will create a rotating magnetic field just as in FIGS. 3 and 4. This embodiment has the advantage that no current has to flow through the electromagnets A and C in the operating mode.