EP4384707A1 - Power supply assembly for a plasma thruster of a spacecraft - Google Patents
Power supply assembly for a plasma thruster of a spacecraftInfo
- Publication number
- EP4384707A1 EP4384707A1 EP23738832.7A EP23738832A EP4384707A1 EP 4384707 A1 EP4384707 A1 EP 4384707A1 EP 23738832 A EP23738832 A EP 23738832A EP 4384707 A1 EP4384707 A1 EP 4384707A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- current
- power supply
- supply assembly
- plasma
- measuring
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 238000011156 evaluation Methods 0.000 claims description 39
- 238000005259 measurement Methods 0.000 claims description 23
- 230000005355 Hall effect Effects 0.000 claims description 12
- 238000010884 ion-beam technique Methods 0.000 claims description 12
- 238000000034 method Methods 0.000 claims description 10
- 239000004020 conductor Substances 0.000 claims description 6
- 239000003380 propellant Substances 0.000 claims description 5
- 230000003472 neutralizing effect Effects 0.000 claims description 4
- 238000012546 transfer Methods 0.000 claims description 4
- 206010063493 Premature ageing Diseases 0.000 abstract description 5
- 230000015556 catabolic process Effects 0.000 abstract description 5
- 238000006731 degradation reaction Methods 0.000 abstract description 5
- 150000002500 ions Chemical class 0.000 description 25
- 208000032038 Premature aging Diseases 0.000 description 4
- 238000006386 neutralization reaction Methods 0.000 description 3
- 238000011084 recovery Methods 0.000 description 3
- 239000000523 sample Substances 0.000 description 2
- 230000032683 aging Effects 0.000 description 1
- 238000013461 design Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 238000012423 maintenance Methods 0.000 description 1
- 238000011022 operating instruction Methods 0.000 description 1
- 230000002028 premature Effects 0.000 description 1
- 238000012545 processing Methods 0.000 description 1
- 238000004088 simulation Methods 0.000 description 1
- 230000002123 temporal effect Effects 0.000 description 1
- 238000012360 testing method Methods 0.000 description 1
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F03—MACHINES OR ENGINES FOR LIQUIDS; WIND, SPRING, OR WEIGHT MOTORS; PRODUCING MECHANICAL POWER OR A REACTIVE PROPULSIVE THRUST, NOT OTHERWISE PROVIDED FOR
- F03H—PRODUCING A REACTIVE PROPULSIVE THRUST, NOT OTHERWISE PROVIDED FOR
- F03H1/00—Using plasma to produce a reactive propulsive thrust
- F03H1/0006—Details applicable to different types of plasma thrusters
- F03H1/0018—Arrangements or adaptations of power supply systems
Definitions
- the present description relates to an electrical power supply assembly for a spacecraft plasma thruster. It also relates to a plasma propulsion system and a spacecraft which incorporate this electrical power assembly.
- Plasma thrusters produce the thrust force which constitutes the propulsion of the spacecraft by emitting ions with a high value of ionic kinetic energy. To do this, they incorporate an appropriate ion emission system, which generates an ion beam towards the outside of the spacecraft. But they also incorporate a device for electrical neutralization of this ion beam, in order to reduce an electrostatic charge which is carried by the spacecraft and which could degrade certain of its on-board devices if this electrostatic charge becomes too great in relation to the electrical potential of the surrounding space.
- An electron emitter which is used for this purpose of neutralizing the ion beam comprises a neutralizer when the plasma thruster is of a gated ion type, GIT or RIT, or comprises a hollow cathode of the plasma thruster when the latter is of the Hall effect type.
- each of these electrical neutralization devices comprises a maintaining electrode, or “keeper” in English, which is arranged at an outlet of the electron emitter.
- This maintaining electrode is powered with an electric current which is dedicated and controlled, called maintaining current and denoted keeper.
- This holding current then constitutes a contribution to a return current which flows from the electron emitter to a common return point, or CRP for "common reference potential” in English, also called NRP for “Neutralizer Return Potential” or “Cathode Return Potential” depending on the type of plasma thruster.
- This return current, denoted Ibody is the sum of several contributions.
- a first contribution is the thrust control current, which is delivered to the ion emission system and designated by beam for a gated ion thruster, GIT or RIT, or by Id for a Hall effect thruster.
- a second contribution is the keeper holding current which is delivered to the holding electrode of the electron emitter used to neutralize the ion beam.
- the two currents beam or b on the one hand, and keeper on the other hand, are parameters which determine the operating point of the plasma thruster. Their values are provided by the manufacturer of this plasma thruster. However, it may appear that additional adjustment of the operation of the plasma thruster is necessary, beyond the current values provided by its manufacturer, depending on the type of mission for which the plasma thruster is intended, according to simulations. or field tests of the spacecraft which is equipped with the plasma thruster.
- Certain plasma thrusters require that the holding current be generated for a short period of time when the plasma thruster is switched on, then be stopped.
- Other plasma thrusters require that the holding current be maintained for the duration of a propulsion phase, regardless of that duration.
- the distinction between these two requirements comes from the intensity of the thrust control current that flows through the neutralizer or hollow cathode, depending on the type of plasma thruster. The higher this intensity, the more likely the plasma thruster is to operate without holding current. Conversely, the lower the intensity of the thrust control current which circulates in the neutralizer or in the hollow cathode, the more the operation of the plasma thruster is likely to require a sufficient holding current.
- the manufacturer of plasma thruster provides a value to adopt for the keeper holding current which is different for each prescribed value of the thrust control current beam or Id.
- Typical numerical values are for example: between 2.2 A (ampere) and 3, 8 A for the thrust control current, and between 3.1 A and 4.6 A for the holding current.
- the operating instructions for a plasma thruster which are provided by its manufacturer to the manufacturer of the spacecraft in which this plasma thruster is used further include a set value for the body return current which returns from the thruster to plasma from the electron emitter, towards the common CRP return point of its power supply assembly.
- a value for this return current which would be greater than the manufacturer's corresponding setpoint is likely to cause premature aging or degradation of the plasma thruster, and in particular of its electrical neutralization device.
- An aim of the present invention is then to further improve the precision in controlling the plasma thruster.
- a general aim of the present invention is to preserve or maximize the lifespan of a plasma thruster which is used on board a spacecraft.
- the invention aims to prevent premature wear or degradation of the plasma thruster.
- a first aspect of the invention proposes a new electrical power supply assembly for a spacecraft plasma thruster, adapted to transform electrical power which is received from a power bus of the spacecraft, in electrical voltages and currents which are supplied by this electrical power supply assembly to the plasma thruster, so that the latter generates an ion beam during operation of the plasma thruster.
- the power supply assembly includes a common return point for collecting a current of feedback from the plasma thruster during operation.
- the plasma thruster includes an electron emitter which is for neutralizing the ion beam during operation, and a holding electrode which is provided at an output of electrons emitted from the electron emitter.
- the electrical currents supplied by the power supply assembly include at least one holding current which is supplied to the holding electrode and which constitutes a contribution to the return current.
- the electrical power supply assembly is adapted to receive or produce successive evaluations of the return current or of a leakage current which flows from the common return point towards an electrical ground of the spacecraft.
- Such evaluations of the return current or the leakage current are received by the power supply assembly when the means for obtaining these evaluations are external to the power supply assembly.
- the electrical power supply assembly is arranged to adjust in real time during operation, the holding current as a function of evaluations of the return current or the leakage current, in accordance with a current setpoint value.
- the current setpoint value which is used according to the invention to adjust the holding current in real time during operation can be relative to the return current or to a sum of the holding current and the leakage current.
- the current setpoint value which is used according to the invention can be prescribed by the manufacturer of the plasma thruster. It may vary in accordance with several operating points which are provided by this manufacturer for the plasma thruster. In different embodiments of the invention, this current setpoint can concern either the return current, or a partial return current which is constituted by the holding current and the leakage current. In the latter case, the instruction for the partial return current can be obtained by subtracting from a return current setpoint a thrust control current setpoint.
- the present invention makes it possible to prevent the return current, which flows from the electron emitter of the plasma thruster to the common return point of the electrical power supply assembly of the plasma thruster. , does not exceed the instructions prescribed by the manufacturer of this plasma thruster.
- the invention therefore proposes to replace the use of a holding current setpoint possibly provided by the manufacturer of the plasma thruster by an adjustment of the holding current in order to respect the return current setpoint or the return current setpoint. partial return current.
- the electrical mass of the spacecraft can be constituted by its chassis. Return current flows from the electron emitter to the return common point, and leakage current flows from this return common point to the spacecraft's electrical ground.
- the return current is a grouping of the thrust control current that is supplied to the ion emission system of the plasma thruster, the holding current, and the leakage current. .
- the leakage current results from variations in an electrical charge that the spacecraft picks up as a function of various parameters such as the surface of its solar panels, their orientation , the bus voltage of the solar panels, the ion flux which is emitted by the plasma thruster, the solar irradiance, the distance from the Sun, etc.
- This leakage current therefore constitutes a contribution to the return current which flows from the electron emitter towards the common return point, in addition to the contributions of the thrust control current and the holding current.
- the leakage current then flows through a dedicated discharge conductor system, from the common return point to the space vehicle's electrical ground. In essence, the leakage current is not controlled or predictable with sufficient precision. It can be positive or negative.
- the leakage current can be of the order of 0.08 A to 0.1 A.
- the leakage current can cause the total or partial return current to exceed or fall short of the setpoint which has been prescribed by the manufacturer of the plasma engine.
- the present invention therefore prevents such overshooting or undershooting from occurring, thus preventing premature aging of the plasma thruster from occurring and preserving its proper operation.
- the holding current can be reduced or increased by the power supply assembly, depending on the sign and/or variations of the leakage current.
- the power supply assembly can be arranged to adjust the holding current in real time during operation according to a feedback loop which comprises a subtractor, a first input of the subtractor being arranged to receive the value current setpoint, and a second input of the subtractor being arranged to receive the evaluations of the return current or to receive a sum of a measurement result of the holding current and the evaluation of the leakage current.
- the power supply assembly is then configured to adjust the holding current based on a difference result which is output by the subtractor.
- the electrical power supply assembly comprises a measuring system which is arranged to deliver successive results of measuring the leakage current.
- each leakage current measurement result constitutes an evaluation.
- the electrical power supply assembly can then further comprise a summer which is arranged to receive on two inputs of this summer, at each of a series of successive instants during the operation of the plasma thruster, the current measurement result leakage and the holding current measurement result for this instant. An output of the adder is then connected to the second input of the subtractor.
- the electrical power supply assembly further comprises the measuring system for delivering the successive results of measuring the leakage current.
- the electrical power supply assembly can then further comprise a summation which is arranged to receive on three inputs of this summator, at each of a series of successive instants during the operation of the plasma thruster, the result of measuring the leakage current and the result of measuring the holding current for the same instant, and also an evaluation of a current thrust control which is provided at this time by the electrical power assembly to the ion emission system of the plasma thruster.
- the output of the adder is again connected to the second input of the subtractor.
- the measuring system which is used to deliver the successive leakage current measurement results can be of a type adapted to carry out electric current measurements.
- the electrical power supply assembly may further comprise a discharge conductor system which is intended to electrically connect the common return point to the electrical ground of the spacecraft.
- the measuring system which is used to deliver the successive results of measuring the leakage current can be of a type adapted to carry out measurements of electrical voltage, and be arranged to measure an electrical voltage which exists between terminals of at least part of the discharge conductive system.
- the power supply assembly is then configured to provide each leakage current measurement result as a result of dividing the electrical voltage measured across the terminals of the discharge conductive portion of the system by a resistance value of that part of the discharge conductive system.
- the electrical power supply assembly can be autonomous to have the resistance value of the part of the discharge conductive system at the terminals of which the electrical voltage is measured.
- the electrical power supply assembly comprises a measuring system which is arranged to deliver successive results of measuring the return current, each result of measuring the return current constituting an evaluation of it.
- the electrical power supply assembly is then arranged to transmit these successive results of measuring the return current to the second input of the subtractor during operation of the plasma thruster.
- the power supply assembly can be configured to adjust the holding current as a function of the result of difference which is output by the subtractor in accordance with a proportional-integral transfer function which is applied to this difference result.
- a second aspect of the invention proposes a plasma propulsion system for a spacecraft, which comprises:
- this plasma thruster comprising an electron emitter and a holding electrode which is arranged at an output of the electrons emitted by the electron emitter;
- This plasma propulsion system is arranged so that the electrical power supply assembly supplies the maintaining electrode of the plasma propellant, during operation of the latter, with a maintaining current which is adjusted in real time based on evaluations of return current or leakage current, in accordance with the current setpoint.
- the holding current which is supplied by the power supply assembly to the holding electrode can be consistent with the difference result which is output by the subtractor .
- the plasma propellant can be of one of the following types:
- the electron emitter comprises an electron gun which is intended to neutralize the ion beam during operation of the plasma thruster, and the electrode of maintaining is arranged at an electron outlet of the electron gun;
- the electron emitter is a neutralizing hollow cathode of the Hall effect thruster, and the maintaining electrode is arranged at an output opening of the hollow cathode.
- a third aspect of the invention proposes a spacecraft which comprises a plasma propulsion system conforming to the second aspect of the invention.
- a fourth aspect of the invention proposes a method of powering a plasma thruster on board a spacecraft, this method comprising the following steps that are performed while the ship is moving in space:
- the holding current that is supplied to the holding electrode can be adjusted so that the return current, or a sum of a current measurement result maintenance and evaluation of the leakage current, corresponds to the current setpoint value.
- the maintaining current which is supplied to the maintaining electrode at a moment of operation of the plasma thruster is adjusted according to evaluations or measurements which have been collected for the maintaining current, and for the return current or leakage current.
- the current setpoint value can be prescribed by a manufacturer of the plasma thruster. It relates to the return current or the sum of the holding current and the leakage current, also called partial return current.
- Such a method can be implemented using a power supply assembly which conforms to the first aspect of the invention, including the improvements which have been cited.
- This electrical power assembly is on board the spacecraft and arranged to supply electrical voltages and currents to the plasma thruster, so that the latter generates an ion beam so as to apply a desired thrust force to the spacecraft.
- the method of the invention may include subtracting the evaluation of the return current, or the evaluation of the sum of the holding current and the leakage current, from the current setpoint, then using a result subtraction to adjust the holding current.
- each evaluation of the return current can be obtained by measuring this return current, or by calculating a sum of a measurement result of the holding current with a measurement result of the leakage current, and with an evaluation of a thrust control current which is supplied to the ion emission system of the plasma thruster;
- the evaluation of the thrust control current can be formed by a set value which is used for this thrust control current, in particular prescribed by the manufacturer of the plasma thruster, or can be obtained by measuring this current of thrust control;
- the holding current can be adjusted by applying a proportional-integral transfer function to the subtraction result.
- FIG. 1 shows, in a schematic and simplified manner, a spacecraft in which the present invention is used
- FIG. 2 is a diagram which illustrates a first possible embodiment of the invention
- FIG. 3 corresponds to [Fig. 2] for a second possible embodiment of the invention
- FIG. 4 corresponds to [Fig. 2] for a third possible embodiment of the invention.
- the reference 100 designates a spacecraft, whatever the type of this vessel, for example a satellite or a space probe.
- the references 101 and 102 respectively designate the electrical power bus and the electrical mass of the spacecraft 100.
- the electrical mass 102 is constituted by a chassis of the spacecraft 100 on which all the on-board components are fixed.
- the reference 10 designates a plasma propulsion system, commonly referred to by the acronym PPS for “Plasma Propulsion Subsystem” in English.
- This plasma propulsion system 10 which is sometimes referred to as a subsystem in relation to the spacecraft 100, itself comprises at least one electrical power supply assembly 1, commonly designated by the acronym PPU for “Power Processing Unit”. in English, and at least one plasma thruster 2.
- the power supply assembly 1 and the plasma thruster 2 which are shown in the figure are associated with each other so that the plasma thruster 2 is powered in electrical energy appropriately by the electrical power supply assembly 1, in order to produce the thrust force which is desired at each instant of operation of the plasma thruster.
- the electrical power supply assembly 1 is connected between the electrical power bus 101 and the electrical mass 102 of the spacecraft 100, while the various components of the plasma thruster 2 are supplied with electrical currents and voltages via the power supply assembly 1.
- the reference 21 designates its ion emission system, whatever the type of the plasma thruster 2 among an ion thruster with grid and continuous discharge designated by GIT for “Gridded Ion Thruster”, a ion thruster grid and radio frequency discharge designated by RIT for “Radiofrequency Ion Thruster”, and a Hall effect thruster designated by HET for “Hall Effect Thruster”.
- the reference 23 designates an electron emitter whose function is to neutralize the ions which are emitted by the system 21.
- the electron emitter 23 is a neutralizer which is separated from the ion emission system 21.
- the electron emitter 23 is constituted by a hollow cathode associated with the ion emission system 21.
- a maintaining electrode 22, or "keeper" in English is associated with the electron emitter 23.
- the design and shape of this maintaining electrode 22 depend on the type of plasma thruster 2, but its function and its use in the present invention are the same regardless of the type of plasma thruster.
- the maintaining electrode 22 has the particular function of ensuring operational availability of the electron emitter 23, by keeping the plasma sufficiently hot.
- the holding electrode 22 is arranged near the exit of the electrons which are generated by the emitter 23.
- the holding electrode 22 physically surrounds an outlet opening of the electrons which are emitted, so as to create a maintaining plasma at this location, both for a GIT or RIT propellant neutralizer and for a hollow HET propellant cathode.
- an interface 11 is dedicated to electrically powering the ion emission system 21, with a current which is commonly denoted beam when the plasma thruster 2 is of the ionic type with GIT or RIT gates, or denoted Id to designate a discharge current when the plasma thruster 2 is of the Hall effect type HET.
- this power supply current of the ion emission system 21 is generically called thrust control current, and denoted beam/ld or beam, Id-
- an interface 12 which is distinct from the interface 11, is dedicated to supplying the holding electrode 22 with another current, which is called current keeper and commonly noted keeper.
- a return current which is denoted body circulates from the electron emitter 23 to a common return point which is commonly designated by CRP, for “Common Return Point” in English.
- This common return point CRP is itself electrically connected to the electrical mass 102 of the spacecraft 100 by a discharge conductive system 103, sometimes called “bleed conducting system” or “bleed resistor” in English, heak then designates a current of leak which flows from the common return point CRP to the electrical ground 102, through the discharge conductive system 103.
- a measuring system 104 can be arranged at the discharge conductor system 103, to measure in real time leakage current heak.
- the measuring system 104 can be a voltmeter which is connected to the terminals of the discharge conductor system 103, and the instantaneous value of the leakage current eak can then be calculated by dividing by the known ohmic value of the discharge conductor system 103 a voltage measurement result which is delivered by the voltmeter.
- the systems 103 and 104 can be integrated into the power supply assembly 1 to allow operation of this power supply assembly which is autonomous for measuring the leakage current eak-
- the electrical supply interface 11 of the ion emission system 21 has a first output terminal 11a which is connected to the emission system 21 of ions, to deliver to the latter the beam/b thrust control current.
- Interface 11 also has a second output terminal 11 b which is connected to the common return point CRP to recover the current Ibeam/ld from this point.
- the interface 12 has a first output terminal 12a which is connected to the holding electrode 22 to deliver the keeper holding current to the latter. It also has a second output terminal 12b which is connected to the common return point CRP to recover the keeper current from this point.
- the body return current is the sum of the Ibeam/ld thrust control current, the keeper holding current and the heak leakage current.
- body beam + keeper + heak for a plasma thruster 2 of the GIT or RIT type
- body h + keeper + heak for a plasma thruster 2 of the HET type.
- the values of the two currents b eam/ld and Leeper to be adopted are generally prescribed by the manufacturer of the plasma thruster 2, for one or more operating points of the latter depending on the thrust force which is desired . Furthermore, the manufacturer also provides a current setpoint value boby_max_crit for the current of body return, or a current setpoint value l W arm_crit for the keeper + heak sum of the holding current and the leakage current. But these setpoint values are provided assuming in both cases that the heak leakage current is zero or negligible. However, the leakage current eak depends on numerous parameters external to the spacecraft 100, and/or the orientation and/or the position of this spacecraft in space, etc.
- the value of the heak leakage current is difficult to predict, being able to be positive or negative.
- the heak leakage current can then cause significant differences between the real value of the return current Ibody and the setpoint lboby_max_crit, or between the real value of the keeper + heak sum and the setpoint lwarm_crit. Such deviations are likely to cause premature aging or degradation of the plasma thruster 2.
- the invention which is the subject of the present description proposes to add a loop of servo-control of the electrical power supply assembly 1, to adapt in real time the value of the keeper holding current in order to ensure that at each moment of operation of the plasma thruster 2 in space, i.e.
- the instantaneous value of the return current Ibody remains substantially equal to the set value lboby_max_crit which is prescribed by the manufacturer, or else in order to ensure that the sum keeper + heak of the holding current and the leakage current remains substantially equal to the setpoint value l wa rm_crit which is prescribed alternatively by the manufacturer.
- a circuit which produces such a control can in particular be incorporated in the electrical supply interface 12 of the maintaining electrode 22.
- the sum keeper + heak of the maintaining current and the current of leakage was called partial return current.
- the setpoint value lbob y _ max_crit OR lwarm_crit can be supplied to a subtractor 120 which is used in the embodiments described below, by appropriate setpoint recovery means 111.
- These means setpoint recovery 111 can be means of reading and selecting setpoint values which were initially recorded on a medium (not shown) on board the spacecraft 100, before the latter is launched into space.
- this recording medium and the setpoint recovery means 111 can be integrated into the power supply assembly 1, and are activated by a computer. on board the spacecraft 100.
- This on-board computer is designated by the reference 110 in [Fig. 1] and commonly noted OBC for “On-Board Computer” in English.
- the set values can be recorded for several operating points of the plasma thruster 2.
- the reading and selection means transmit the set values which correspond to an operating point specified by an operator of the spacecraft 100, in order to produce the desired thrust force on this spacecraft 100.
- FIG. 2 The embodiment of the invention which is illustrated by [Fig. 2] corresponds to the case where the values prescribed by the manufacturer are the value of the thrust control current lbeam/ld and the current setpoint value l wa rm_cnt for the keeper + heak sum of the holding current and the leakage current. It is possible for the manufacturer to prescribe a setpoint value for the keeper holding current, but this is reinterpreted according to the invention as the setpoint value l wa rm_crit relating to the sum keeper + heak.
- the reference 12 also designates the power supply interface of the holding electrode 22 as known before the present invention and presented previously with reference to [Fig.
- the reference 120 designates a subtractor
- the reference 121 designates an adder
- the reference 122 designates a system for measuring the keeper holding current which is effectively delivered by the interface 12 to the holding electrode 22.
- the system of measurement 122 can be arranged on the connection which electrically connects the output of interface 12 to the holding electrode 22, but other arrangements are alternatively possible.
- the adder 121 receives on its two inputs on the one hand a result of measuring the heak leakage current which is delivered by the system 104 and denoted M(heak), and on the other hand a result of measuring the keeper holding current which is delivered by system 122 and denoted M(keeper).
- the adder 121 thus provides as an output an evaluation of the sum of the keeper holding current and the leakage current eak, denoted E(kee P er + heak) in [Fig. 2],
- the subtractor 120 receives the setpoint value l war m_crit on its positive input, and the summation result which is provided by the adder 121 on its negative input.
- the deviation A which is calculated by the subtractor 120 is transmitted to a control input of the interface 12, and is used by the latter as an increment for adjusting the keeper holding current to be delivered.
- the keeper holding current is adjusted in real time during the operation of the plasma thruster 2, so that at each of a series of instants during this operation, the sum of the instantaneous values of this keeper holding current and the heak leakage current remains substantially equal to the set value lwarm_crit-
- the current setpoint value which is provided by the manufacturer or considered to control the power supply interface 12 of the maintaining electrode 22 is lbody_max_crit which relates to the return current Ibody.
- the adder 121 with two inputs is replaced by an adder 121 'with three inputs which respectively receive the result M(heak) of the measurement of the leakage current eak which is delivered by the system 104, the result M(lkeeper) of the measurement of the keeper holding current which is delivered by the system 122, and an evaluation E(lbeam/ld) of the thrust control current beam/b, respectively.
- the evaluation E(lbeam/ld) of the thrust control current can directly be the set value which is prescribed by the manufacturer for this current in order to obtain the desired thrust force.
- the evaluation E(lbeam/ld) can be a result of a measurement of the thrust control current Ibeam/ld which is actually delivered by the interface 11 to the ion emission system 21.
- Such a measurement of the Ibeam/ld thrust control current can be carried out in real time in one of the ways available to those skilled in the art.
- the adder 121 'thus provides at output an evaluation of the body return current, denoted E(lbody), then the subtractor 120 calculates a difference A' which exists between the set value lbody_max_crit and this evaluation E(lbody).
- FIG. 4 The embodiment of the invention which is illustrated by [Fig. 4] is derived from that of [Fig. 3] by replacing the evaluation E(body) of the body return current which was provided by the adder 121 'by a measurement of this return current.
- a system 123 for measuring the body return current is arranged on the electrical connection which connects the electron emitter 23 to the common return point CRP.
- This system 123 which is used to measure the body return current can also be of a type known to those skilled in the art.
- THE adder 121 ' is deleted.
- the principle of operation of the control loop which is shown in [Fig. 4] is otherwise unchanged compared to that of [Fig.
- this beeper holding current can be determined by additionally applying a low-pass type transfer function, in particular of the proportional-integral type, to the deviations A, A' or A” which are transmitted at the output by the subtractor 120 at successive moments of operation of the plasma thruster 2, for each of the embodiments of [Fig. 2]-[Fig. 4], An optional low-pass filter 124 which is used for this purpose can then be inserted between the output of the subtractor 120 and the control input of the electrical supply interface 12 of the holding electrode 22.
- a low-pass type transfer function in particular of the proportional-integral type
- the invention can be reproduced by modifying secondary aspects of the embodiments which have been described in detail above, while retaining at least some of the advantages cited.
- some of the components used in these embodiments can be replaced by others with equivalent functions or which produce equivalent combinations of functions.
- part or all of the components used to adjust the holding current according to the invention can advantageously be incorporated into the power supply interface of the holding electrode, in order to obtain autonomous operation of this interface.
- the plasma propulsion system can incorporate any number of thrusters, with associated electrical power interfaces.
- plasma thrusters which are separated can share the same electrical power interface while using the invention for this interface and these thrusters.
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Abstract
Description
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Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
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FR2207618A FR3138169B1 (en) | 2022-07-25 | 2022-07-25 | POWER SUPPLY ASSEMBLY FOR SPACESHIP PLASMA THRUSTER |
PCT/FR2023/050895 WO2024023409A1 (en) | 2022-07-25 | 2023-06-19 | Power supply assembly for a plasma thruster of a spacecraft |
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EP4384707A1 true EP4384707A1 (en) | 2024-06-19 |
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Application Number | Title | Priority Date | Filing Date |
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EP23738832.7A Pending EP4384707A1 (en) | 2022-07-25 | 2023-06-19 | Power supply assembly for a plasma thruster of a spacecraft |
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EP (1) | EP4384707A1 (en) |
FR (1) | FR3138169B1 (en) |
WO (1) | WO2024023409A1 (en) |
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US6518693B1 (en) * | 1998-11-13 | 2003-02-11 | Aerojet-General Corporation | Method and apparatus for magnetic voltage isolation |
FR2788084B1 (en) * | 1998-12-30 | 2001-04-06 | Snecma | PLASMA PROPELLER WITH CLOSED ELECTRON DRIFT WITH ORIENTABLE PUSH VECTOR |
FR3094046B1 (en) * | 2019-03-18 | 2021-04-23 | Centre Nat Rech Scient | Ion thruster control method, and ion propulsion system |
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2022
- 2022-07-25 FR FR2207618A patent/FR3138169B1/en active Active
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2023
- 2023-06-19 WO PCT/FR2023/050895 patent/WO2024023409A1/en unknown
- 2023-06-19 EP EP23738832.7A patent/EP4384707A1/en active Pending
Non-Patent Citations (1)
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GHISLANZONI LUCA ET AL: "Hall Effect Thruster Direct Drive PPUs, Experimental Investigation of the Cathode Potential Grounding Problem", E3S WEB OF CONFERENCES, vol. 16, 1 January 2017 (2017-01-01), pages 15002, XP093089519, Retrieved from the Internet <URL:https://www.e3s-conferences.org/articles/e3sconf/pdf/2017/04/e3sconf_espc2017_15002.pdf> DOI: 10.1051/e3sconf/20171615002 * |
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WO2024023409A1 (en) | 2024-02-01 |
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