Cusped-field thruster

0001The invention relates to a cusped-field thruster for a space system and to a method for generating a thrust on a space system.

PRIOR ART

0002Electric thrusters have been under development for several decades by various companies and universities, for example for use in a space system.

0003Plasma accelerator configurations are described, for example, in <patcit id="pcit0001" dnum="DE10130464A1"><text>DE 101 30 464A1</text></patcit> and in <patcit id="pcit0002" dnum="DE10300776B3"><text>DE 103 00 776 B3</text></patcit>.

0004Another plasma accelerator configuration is described, for example, in <patcit id="pcit0003" dnum="DE10153723A1"><text>DE 101 53 723 A1</text></patcit>, wherein for the plasma accelerator configuration a multistage construction is disclosed with at least one intermediate electrode between electrodes enclosing a plasma chamber between them. Due to this so-called "high efficiency multistage plasma thruster" (HEMPT), increased efficiency is achieved by an uneven potential distribution to the potential stages formed by the plurality of electrodes with a high potential difference of the last stage on exit of the plasma jet and by a special design of a magnetic field permeating the plasma chamber in this last stage.

0005In <patcit id="pcit0004" dnum="US6448721B2"><text>US 6,448,721 B2</text></patcit>, an arrangement and a method for a plasma thruster are described that utilise a so-called Hall thruster with a cylindrical geometry. It is portrayed that this arrangement is suitable for operation with low energy. Efficient operation is accomplished in this case by magnetic fields with a generally radial component.

0006Other prior art is found, for example, in <patcit id="pcit0005" dnum="CN105736272A"><text>CN 105736272 A</text></patcit>; in <nplcit id="ncit0001" npl-type="s"><text>Courtney et al., "Diverging Cusped-Field Hall Thruster (DCHT)", IEPC-2007-39</text></nplcit>; in<nplcit id="ncit0002" npl-type="s"><text> Matlock et al., "Controlling Plume Divergence in a Cusped-Field Thruster", IEPC-2011-178</text></nplcit>; and in <nplcit id="ncit0003" npl-type="s"><text>Matyash et al., "Comparison of SPT and HEMP thruster concepts from kinetic simulations", IEPC-2009-159</text></nplcit>.

0007<figref idref="f0001">Figure 1</figref> (from <nplcit id="ncit0004" npl-type="s"><text>Matyash et al., "Comparison of SPT and HEMP thruster concepts from kinetic simulations", IEPC-2009-159</text></nplcit>) shows schematically a system of a cusped-field thruster 100 according to the prior art.

0008The cusped-field thruster 100 consists in this case of a plurality of magnets, the magnetic south poles and magnetic north poles of which are arranged respectively in an antipolar manner. A cathode 102 emits electrons for the discharge ignition, wherein the electrons further neutralise the xenon ion beam.

0009Xenon gas is admitted to the discharge chamber of the cusped-field thruster 100. In this example, a voltage between 300 V and 2000 V is then applied between the cathode 102 and the anode 104.

0010The xenon particles are ionised and then accelerated through the electric field. After the passage through the neutraliser (cathode 102), which supplies electrons to the ion beam again and thus renders it electrically neutral again, the neutralised particles are ejected in the form of a beam (see right-hand part of <figref idref="f0001">figure 1</figref>).

0011The cathode 102 as neutraliser here prevents charged particles from moving back to the space system in an arc.

0012As is to be seen in <figref idref="f0001">figure 1</figref>, the ionised xenon gas is accelerated through the magnetic field, which forms so-called cusps in this case, along the symmetry axis of the thruster.

0013<figref idref="f0002">Figure 2</figref> shows schematically another system of a cusped-field thruster 200 according to the prior art.

0014As in the cusped-field thruster shown in <figref idref="f0001">figure 1</figref>, in the cusped-field thruster 200 ionised xenon particles are accelerated along the axis of symmetry through the electric field, which is formed between the cathode 202 and the anode 204.

0015In contrast to the cusped-field thruster in <figref idref="f0001">figure 1</figref>, the magnetic field lines that are generated by the magnets 206 run parallel to the symmetry axis of the thruster in the region in front of the anode 204.

INVENTION

0016In space research, simple microthrusters that operate in the micro-Newton range were developed for future research missions but also for small satellite constellations. The research and development carried out was based here in particular on the aforesaid HEMPT concept. However, it has turned out that a relatively small thruster based on the HEMPT concept cannot be operated very efficiently in comparison with a larger HEMPT thruster. In the case of geometrically relatively small thruster external dimensions of approx. 30 mm and smaller in particular, the efficiency of the thruster is sharply reduced, the discharge unstable and the thrust range very small.

0017The object of the invention is to provide a cusped-field thruster of the type named at the beginning that permits improved efficiency.

0018To this end the invention shows a cusped-field thruster for a space system, wherein the cusped-field thruster comprises: <ol id="ol0001" compact="compact"><li>a) at least two substantially annular permanent magnets arranged in an antipolar manner, wherein a magnetic pole piece is formed between the permanent magnets; and</li><li>b) an anode, which comprises a permanent-magnetic material;</li><li>c) wherein the cusped-field thruster is configured in such a way that a cusp is formed in a region adjacent to the anode of the cusped-field thruster.</li></ol>

0019The magnetic field is changed in this case in such a way that a further axial cusp is located directly on the thruster anode at the end of the thruster channel.

0020The anode can consist completely of a permanent-magnetic material. Alternatively to this, only a part of the anode can consist of a permanent-magnetic material. For example, according to some embodiments an inner core region of the anode can consist of a permanent-magnetic material and/or the surface or a surface region of the anode can be manufactured from a permanent-magnetic material.

0021The permanent-magnetic material can comprise a ferrimagnetic or ferromagnetic material here.

0022The substantially annular structure of the at least two permanent magnets arranged in an antipolar manner here comprises structures in which the permanent magnets are annular, or have at least partially edged or angular structures, which do not adversely affect the functioning of the permanent magnets with regard to the shape of the magnetic field, however. In particular, the substantially annular design of the at least two permanent magnets arranged in an antipolar manner comprises any structures in which the magnets permit an implementation of a particle beam.

0023A preferred embodiment of the inventive cusped-field thruster for a space system provides that a diameter of the anode decreases in the direction of the region adjacent to the anode in which the cusp is formed. The anode can taper in this case, and be formed in a cylindrical shape, for example.

0024Another preferred embodiment of the inventive cusped-field thruster for a space system provides that the anode is formed as a fuel inlet of the cusped-field thruster. The anode can thus be used according to some embodiments both as an anode and as a pole piece and/or gas inlet.

0025Another preferred embodiment of the inventive cusped-field thruster for a space system provides that the cusped-field thruster further comprises a discharge chamber wall, which is arranged on a surface of the at least two substantially annular permanent magnets arranged in an antipolar manner and on a surface of the magnetic pole piece, wherein the surfaces face a discharge chamber of the cusped-field thruster.

0026The invention also shows a method for generating a thrust on a space system, wherein the method comprises: <ol id="ol0002" compact="compact"><li>a) providing a cusped-field thruster according to an embodiment described herein;</li><li>b) admitting a fuel into a discharge chamber of the cusped-field thruster; and</li><li>c) applying an electric voltage between the anode and an electron source.</li></ol>

0027Electrons are accelerated into the discharge chamber by this. The electrons are confined in the discharge chamber by a magnetic field, which is generated by the at least two substantially annular permanent magnets arranged in an antipolar manner and the anode. The electrons ionise the fuel in the discharge chamber. The ionised fuel is then accelerated through an electric field so that the thrust on the space system is generated.

0028Let it be noted that steps b) and c) can also be executed in reverse order or simultaneously.

0029Xenon gas, for example, can be used as fuel.

0030A preferred embodiment of the method according to the invention for generating a thrust on a space system provides that the anode of the cusped-field thruster has a tapering profile, so that the magnetic field strength is focused at the anode.

DRAWINGS

0031Exemplary embodiments of the invention are described in greater detail below with reference to the drawings. <ul id="ul0001" list-style="none"><li><figref idref="f0001">Figure 1</figref> shows schematically a system of a cusped-field thruster according to the prior art;</li><li><figref idref="f0002">Figure 2</figref> shows schematically another system of a cusped-field thruster according to the prior art;</li><li><figref idref="f0003">Figure 3</figref> shows schematically a cusped-field thruster according to an embodiment of the invention described herein; and</li><li><figref idref="f0004">Figure 4</figref> shows a flow chart according to a method for generating a thrust on a space system, putting the cusped-field thruster described herein into operation.</li></ul>

DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS

0032According to the invention described herein, the magnetic field inside the cusped-field thruster is changed in such a way that a further axial cusp is located directly on the thruster anode at the end of the thruster channel. The impedance of the thruster is increased by this and the loss cone of the electrons located in the thruster diminished to such an extent that substantially fewer electrons are lost. The thruster can thus be operated efficiently even with relatively small dimensions of approx. 30 mm and smaller.

0033In particular, it is achieved due to the anode, which comprises a permanent-magnetic material, that the thruster is characterised in that it runs very stably over a very wide thrust range (µN to mN) and has a high efficiency especially in the mN range (as compared with the HEMPT configuration described above).

0034Furthermore, the thruster according to the embodiments of the present invention starts reliably even with low anode potentials and with low mass flows, without special start algorithms (pressure surge, increase in anode voltage, etc.) being necessary.

0035<figref idref="f0003">Figure 3</figref> shows schematically a cusped-field thruster 300 according to an embodiment of the thruster according to the invention.

0036The cusped-field thruster 300 comprises in this example two permanent magnets 302a and 302b, between which a pole piece 304 is arranged (in this example a magnetic south pole is formed between the two permanent magnets 302a and 302b).

0037In this example the anode 306 comprises a magnetic material, so that a further axial cusp is formed in a region in front of the anode 306.

0038The cusped-field thruster 300 further comprises a discharge chamber wall 308, which shields the magnets 302a, 302b and pole piece 304 from the discharge chamber 310.

0039In <figref idref="f0003">figure 3</figref> the thruster configuration described is shown with three cusps. However, this can consist of fewer or more cusps depending on the number of pole pieces and magnets selected. The first cusp, with a predominantly axial component, is located directly in front of the anode and there prevents energetic electrons from being lost at the anode. The electron confinement in the discharge chamber is considerably improved by this.

0040As shown in <figref idref="f0003">figure 3</figref>, the other two cusps are formed directly in front of the pole pieces 304.

0041According to some embodiments, the pole pieces are manufactured from a ferromagnetic material. The magnet assembly, which consists of the magnets and pole pieces, is insulated from the plasma and from the anode in some variants of the thruster by a ceramic discharge chamber.

0042The anode, which comprises a magnetic material, is produced partly or entirely from a ferromagnetic material. In this example the symmetry axis of the cylindrical anode coincides substantially with the symmetry axis of the thruster or of the permanent magnets 302a, 302b.

0043In comparison with an arrangement such as that shown in <figref idref="f0002">figure 2</figref>, for example, in which the anode does not comprise any permanent-magnetic material, the further axial cusp formed in a region in front of the anode leads in any inventive embodiments to the magnetic field strength being increased in the region in front of the anode. This in turn leads to better confinement of the electrons in front of the anode. This is accomplished in particular in that the anode itself is magnetic (or comprises a magnetic material). The inventive embodiments, in which the horizontal cusp is formed, differ herein from the HEMPT configuration, for example. The better confinement of the electrons accomplished by the inventive configurations in front of the anode by the field lines concentrated at the anode leads to an increased efficiency of the thruster, as fewer (or no) electrons are lost at the anode and these can then contribute to the ionisation of the fuel gas.

0044The design of a tapering (for example, cylindrical) anode is particularly advantageous in this case, as the magnetic field strength is focused or concentrated at the anode itself by this and thus the effectiveness of the cusp in front of the anode is increased enormously (due to a lower loss of electrons at the anode).

0045Due to the inventive embodiments of the cusped-field thruster, an efficient thruster can be provided that has improved properties compared with the thrusters according to the prior art, such as, for example, an operation of the thruster, which is now possible in the low mN range.

0046Furthermore, the configuration of the inventive embodiments of the cusped-field thruster leads to relatively high efficiency (compared with the HEMPT design, for example). The special anode form also leads to improved starting behaviour of the thruster.

0047The magnetic field created by the permanent magnets and pole pieces produces different cusps. In front of the anode and in front of the pole pieces the magnetic field has its maxima in the interior of the discharge chamber. The spacing of the magnetic field lines is therefore reduced there, which leads to a magnetic mirror and to electron confinement.

0048The integral function of the anode as anode, pole piece and gas inlet represents a preferred embodiment of the cusped-field thruster in this case, due to which a compact design of the thruster can be produced, for example.

0049<figref idref="f0004">Figure 4</figref> shows a flow chart according to a method for generating a thrust on a space system, putting the cusped-field thruster described herein into operation.

0050In step 402 a cusped-field thruster, such as described herein according to the different embodiments, is provided.

0051In step 404 a fuel is then admitted to a discharge chamber of the cusped-field thruster.

0052In step 406 an electric voltage is applied between the anode and an electron source. Electrons are accelerated into the discharge chamber by this, wherein the electrons are confined in the discharge chamber by a magnetic field, which is generated by the at least two permanent magnets arranged in an antipolar manner and the anode. The electrons here ionise the fuel in the discharge chamber. The ionised fuel is then accelerated through an electric field, so that the thrust is generated on the space system.

0053Steps 404 and 406 can also be executed in reverse order or simultaneously.

0054In some embodiments a high voltage (of 100 V to 6000 V, for example) can be applied between anode and the electron source, which can lie outside the thruster and is also termed cathode, to operate the thruster. The anode lying at the positive high voltage potential serves according to some embodiments also as a gas/fuel inlet into the discharge chamber.

0055The electrons absorb energy and migrate in the direction of the anode into the interior of the thruster, where they are confined by the magnetic field. The electrons can then ionise the fuel gas there. In some examples the ions are accelerated out of the thruster by the same electric field and generate thrust. Due to the high mass of the fuel ions, the magnetic confinement does not act (or only acts to an irrelevant, small extent) on the ions.

0056Finally, let it be pointed out in particular that the exemplary embodiments discussed above only serve to describe the instruction claimed, but do not limit this to the exemplary embodiments.