This disclosure is related to spacecraft thrusters and, in particular, to Hall-effect thrusters that provide propulsion via ionization and acceleration of a propellant in a direction away from the spacecraft.
Electric space propulsion engines are a class of propulsion engines that generate thrust by forming and ejecting ions at high velocities. Ions are often created by removing electrons from an otherwise electrically neutral propellant. Hall effect thrusters are a class of electric space propulsion engines that use electron bombardment as the mechanism for propellant ionization. Hall thrusters inject propellant into an annular channel within which propellant ionization and ion acceleration occurs. This propellant is often injected with the aid of a diffuser that serves to spread the propellant throughout the channel. The trajectory of the propellant as it exits the diffuser is significant because it influences how long the propellant ultimately remains inside the channel; increasing propellant lingering time (longevity) inside the channel increases the probability of ionization, which in turn increases thruster efficiency. Axial emission, which is a common injection method used in contemporary Hall thrusters, results in shorter longevity inside the thruster channel and thereby a lower thruster efficiency. For this reason, developing Hall thruster propellant diffusers that reduce axial velocity is advantageous.
Embodiments of a Hall effect thruster system include a thruster body and a diffuser configured to eject ionizable propellant into an annular channel formed in the thruster body. A Hall current provided in the annular thruster channel induces a torque on the thruster body in a first rotational direction, and ejection of the propellant from the diffuser applies a counter-torque to the thruster body in a second rotational direction opposite the first rotational direction.
The thruster system may additionally include one or more of the following features in any technically feasible combination:
Embodiments of a Hall effect thruster system include a thruster body and a diffuser configured to eject ionizable propellant into an annular channel formed in the thruster body in a direction that applies a torque on the thruster body.
The thruster system may additionally include one or more of the following features in any technically feasible combination:
Embodiments of a spacecraft include a Hall effect thruster system with any technically feasible combination of features of the above-listed systems.
Embodiments of a method of operating a spacecraft having a Hall thruster system include ejecting an ionizable propellant into an annular thruster channel of the system in a direction that counteracts a torque induced on the thruster system by a Hall current provided in the annular channel.
The direction in the step of ejecting may be a tangential direction relative to the annular channel, and/or the step of ejecting may include ejecting the propellant from a helical channel of a diffuser of the thruster system.
Described below is a mechanical diffuser which accepts a number of incoming propellant streams, divides these streams among a plurality of flows, and directs these flows to have an azimuthal trajectory upon being ejected into the annular channel of a Hall effect thruster within which propellant ionization and ion acceleration occurs. The plurality of flows serves to dispense the propellant evenly throughout the Hall thruster channel, while the azimuthal trajectory increases propellant longevity in the thruster channel, increasing the probability of propellant ionization when compared to conventional axial emission from the diffuser. The azimuthal ejection trajectory also imparts a reactionary torque on the diffuser which can be used as a counter-torque to at least partially counteract a Hall current-induced swirl torque. The diffuser may be constructed as a single, unitary component manufactured additively and having no moving components, reducing the likelihood of suboptimal or failed operation.
An x-y-z coordinate system is included in
When used as part of a Hall thruster system which incorporates center-mounted hardware, such as a hollow cathode or central magnetic poles, it may be advantageous to make the size of the hole through the center of the annular diffuser as large as possible. In this case, the diameter d of the hole through the center of the diffuser could be about 50-95% of the outer diameter D of the diffuser, or about 70-95%, or about 85-95%. Conversely, when used as a temperature managing component within a Hall thruster system it may be advantageous to make the size of the hole through the center of the annular diffuser as small as possible or remove the central hole entirely and use a set of smaller holes to accommodate specific hardware, such as bolts or magnetic poles. In this case, the diameter d of the hole through the center of the diffuser could be 0 to about 50% of the outer diameter D of the diffuser, or about 3-25%, or about 5-10%.
The inlet openings 9 of the channels 8 are azimuthally spaced and have a shape driven by the intersection between the helical channels 8 and the toroidal plenum 6 to allow propellant to flow from the plenum 6 into the helical channels 8. The helical channels 8 coil away from the plenum 6 and toward the outlet end 7 of the diffuser body 10, maintaining constant internal radii and a constant radial distance from the central axis A of the diffuser 1 in the first embodiment. The helical channels 8 are visible in
The inner helical geometry may be optimized to maximize the azimuthal flow of the propellant and thereby increase longevity of the propellant inside the channel 16 of a Hall thruster when the diffuser 1 is incorporated into a larger Hall thruster system 12 (an example of which is depicted in detail in
The helical channels 8 and the toroidal plenum 6 are hollow cavities of the hollow internal flow geometry 15 fully defined within the bulk material of the diffuser body 10 and thus are very difficult to manufacture with traditional subtractive manufacturing techniques. Additive manufacturing, however, may be used to manufacture the diffuser 1 by building up the bulk material of the diffuser body 10 around the requisite hollow features, enabling the manufacture of geometries impossible by traditional subtractive manufacturing techniques. Images of two versions of the first embodiment—each produced via additive manufacturing—are depicted in
In various embodiments, the diffuser has 2 to 500, 2 to 250, or 4 to 125 openings where outlet ends 5, 105 of the channels open on a surface of the outlet end 7 of the diffuser body 10 to provide for more even distribution of propellant. The diffuser may have 1 to 10 or 1 to 4 inlet openings 2, 102.
The radial thickness 13 (
In various embodiments, the angle of elevation θ of the helical channels 8, 108 is in the range of about 2 to 60 degrees, about 5 to 30 degrees, or about 8 to 13 degrees. In some cases, the diameters of the helical channels range from about 0.1 mm to about 10 cm, or about 1 mm to about 1 cm. In embodiments, the cross-section of the helical channels is circular, oblong, elliptical, rectangular, or has another polygonal shape.
One method of making the diffuser is by additive manufacturing. The dimensions of the channels and openings in the diffuser are selected based on the properties of the materials and manufacturing process used. Minimum feature size and wall thickness are two driving parameters of diffuser feature dimensions. These parameters are reported by individual manufacturers for materials and manufacturing techniques they use. In the embodiment shown in
While the illustrated diffuser is a unitary component, i.e. it is manufactured as a single, one-piece component, the diffuser alternatively can be made by forming sub-components which are fused, fastened, clamped, or otherwise attached together.
Testing was performed at the MIT Space Propulsion Laboratory. During testing, the thruster system shown in
A diffuser similar to the diffuser in Example 1 is created in which notches or other cutouts are made along the outer or inner walls of the diffuser to allow for the routing of electrical cables. This is done to allow the routing of power connections to the thruster anode, central electromagnet, and/or hollow cathode. These notches or cutouts do not impact performance.
Diffusers similar to that of Example 1 are formed, but with an increased number of outlet holes. In one case, 50 outlet holes are used to increase even distribution of propellant. In the other case, 100 outlet holes are added to increase even distribution of propellant.
A diffuser similar to that of Example 1 is formed, but in which multiple stages of plenums stacked in the axial direction are included to control the pressure gradient within the diffuser. This is done to equalize pressures throughout the diffuser, further improving equal propellant distribution.
A diffuser similar to that of Example 1 is formed, but for which the radial thickness 13 of the diffuser is increased. This is done to increase surface contact between the diffuser and channel walls, increasing heat transport between the two surfaces and could be advantageous in conducting heat away from the diffuser.
A diffuser similar to that of Example 1 is formed, in which the radial thickness 13 of the diffuser is decreased. This is done to decrease surface contact between the diffuser and channel walls, reducing heat transport between the two surfaces. This can be advantageous in preventing excessive heat from conducting into the diffuser. This also can be done to enable the inclusion of additional components.
Diffusers similar to that of Example 2 are formed, but in which ribs are placed along the inner and/or outer walls of the diffuser. In one case, helical ribs are used. In another case, circumferential ribs are used. The ribs are included to reduce thermal conduction between the diffuser and the surrounding components. This also can be done to create cavities within which other components can be placed or to create geometries that allow for novel constraining features.
A diffuser similar to that of Example 2 is formed, but in which the radial width of the diffuser is reduced and the propellant outlet holes are distributed around the outer wall of the diffuser, rather than the top wall surface, so that propellant is distributed into the gap between the outer wall of the diffuser and the thruster channel wall. This is done to enable inclusion of a thruster anode that sits directly on the top surface of the diffuser and would cover outlet holes that might otherwise be placed on that surface.
A diffuser similar to that of Example 3 is formed in which the diffuser and thruster channel walls are manufactured as a single component, but the propellant outlet holes are distributed around the outer side wall of the thruster channel, as opposed to the bottom surface of the thruster channel, which corresponds to the top surface of the diffuser. This geometry is enabled by the diffuser and thruster channel walls being manufactured as a single component and is done to enable inclusion of an anode that sits directly on the top surface of the diffuser and would cover outlet holes that might otherwise be placed on that surface.
A diffuser similar to that of Example 1 is formed, but in which the top and/or bottom side walls of the diffuser are not flat plane surfaces. Convex or concave shapes may be used to accommodate anodes of greater surface area than a plane and to enable more complex propellant injection geometries.
A diffuser similar to that of Example 1 is formed in which the shape of the outer wall of the diffuser is not round or cylindrical. Diffusers using polyhedral or other closed shape geometries may be used in Hall thrusters of non-standard shapes, such as “racetrack” thrusters, or as a component within other electric propulsion systems besides Hall thrusters.
A diffuser similar to any of the aforementioned examples is formed, but in which the diffuser is manufactured out of more than one part and these parts are fused, fastened, clamped, or otherwise attached together to form a complete diffuser. This assembly process may be used in order to create diffusers with subtractive manufacturing techniques that would otherwise prevent a single-body diffuser from being manufactured.
A Hall effect thruster system 12 generally operates by ionizing a propellant provided in the thruster channel 16 and then accelerating the ionized propellant out of the channel, the reaction force of which provides thrust. Several interrelated features are involved in this process, including an electric field across the thruster channel 16 in a first direction, a magnetic field across the thruster channel in a different second direction, an ionizable propellant in the thruster channel, and a Hall current in the thruster channel. In the illustrated example, the electric field is an axial field generated between the cathode 66 and the ring-shaped anode 18 at the bottom of the channel 16. The magnetic field is a radial field generated between opposite poles of the central electromagnet 58 and the surrounding set of electromagnets 46, for which one plate of the magnetic shunt 48 acts at the pole surrounding the channel 16.
The axial electric field attracts electrons and repels ions, while the magnetic field draws particles into orbits around magnetic field lines. The combined effect of these fields on charged particles is referred to as the Lorentz force, which induces a net particle motion in a direction perpendicular to the crossed electric and magnetic fields—i.e., in the azimuthal direction of the thruster channel 16. This motion is known as E×B drift, where E is the electric field and B is the magnetic field, and a drift velocity is calculable from the cross product of the electric and magnetic field strengths.
For purposes of the thruster system 12, the magnetic field strength is tuned so that electrons are strongly confined within the field and, thereby, within the channel 16, while ions are permitted escape. This differentiation between particles is possible due to the cyclotron radius of the ions being orders of magnitude larger than the cyclotron radius of the electrons. The confined electrons form a swirling azimuthal current in the thruster channel, which is referred to as the Hall current. This electron “swirl” is in the E×B direction. For a Hall thruster with a radially inward pointing magnetic field, the Hall current is a clockwise swirl, as indicated by reference character e in
The introduction of an ionizable propellant (e.g., xenon) into the channel 16 in which the Hall current is flowing leads to ionization of the propellant—i.e., dissociation of neutral propellant particles into a propellant cations and free electrons. The ions are repelled out of and away from the channel 16 by the electric field in a direction having an axial component, with the reaction force providing axial thrust in the opposite direction.
Only the electrons contribute to the overall Hall current—i.e., the current of electric charges in the channel 16—because they remain trapped in the thruster while the ions are ejected. Nevertheless, illustrative xenon propellant ions are six orders of magnitude more massive than electrons, so the majority of the swirl torque τswirl is induced by ion movement within the plasma in the channel 16, even though the ions are in the channel 16 for only a short time. The ion trajectories are highly complex, so their impact on swirl torque is difficult to calculate exactly. Furthermore, the magnitude of swirl torque is so small that it has not been directly measured on Earth, though active research is underway building instruments sensitive enough to measure it. A measurement has been made for the PPS-1350 thruster on the SMART-1 mission (60 μN-m), and prior simulation of the SPT-100 and SPT-140 thrusters yielded 51 and 267 μN-m, respectively.
While swirl torque τswirl is an unavoidable phenomenon in Hall effect thrusters, its effect on Earth-orbit objects (e.g., satellites) has been relatively easy to mitigate. Momentum/reaction wheels can be employed to effectively “absorb” swirl torque as it is generated. Periodically, angular momentum may be offloaded from reaction wheels by firing thrusters or employing magnetorquers to push against Earth's magnetic field in a process known as desaturation. An alternate mitigation strategy involves locating a Hall effect thruster on an actuator so that its angle can be adjusted throughout an orbit. Because Earth orbits are closed, swirl torque can be counteracted by clever adjustments to the thruster and spacecraft attitude throughout an orbit in a process called “spiral thrusting.” In deep space applications, however, the lack of a closed orbits and planetary magnetic fields make it difficult to offload swirl torque without dramatic desaturation maneuvers or special thrusters designated for desaturation. The latter approach is typically avoided because of the increased cost and complexity of adding an additional propulsion system, and the former approach is not ideal because it requires expenditure of additional propellant and loss of forward thrusting time. In theory, the swirl torque can be counteracted by reversing the polarity of the electromagnets generating the magnetic field. In practice, however, this can lead to accelerated channel wall erosion thereby reducing thruster lifetime.
The above-described diffuser offers an alternative mitigation strategy, which is a configuration that, upon ejection of propellant into the thruster channel, applies a net torque to the thruster system 12 in a direction opposite the swirl torque induced by the Hall current. In other words, the thruster system 12 can be constructed such that the Hall effect-induced swirl torque τswirl is in a known first rotational direction—e.g., counterclockwise as in
Embodiments of the Hall effect thruster system 12 may thus include a thruster body 52 and a diffuser 1 configured to eject ionizable propellant into an annular channel 16 formed in the thruster body. A Hall current provided in the annular thruster channel 16 induces a torque τswirl on the thruster body 52 in a first rotational direction, and ejection of the propellant from the diffuser 1 applies a counter-torque τd to the thruster body in a second rotational direction opposite the first rotational direction. The diffuser 1 may be configured to eject the propellant into the annular channel 16 with a tangential velocity—e.g., a velocity tangent to one of the above-described helical diffuser channels 8. Notably, application of the counter-torque τd is not limited to ejection of the propellant from helical diffuser channels. Any diffuser channel shape that results in application of a net torque τd opposite in direction from the swirl torque τswirl may be employed. The diffuser channels 8 could all be simply inclined with respect to the central axis A, for example, and need not eject the propellant into the thruster channel 16 with tangential velocity—i.e., only a component of the ejection velocity need be tangential.
However, while it may be possible to impart a counter-torque on the thruster body 52 via inclined rectilinear (non-curved) diffuser channels 8, curvilinear channels such as the helical channels of the diffusers of
While the magnitude of the counter-torque τd that can be produced is difficult to predict or calculate accurately, the discussion below provides additional information on possible parameters and features of the diffuser and thruster system that can affect its magnitude, along with some rough estimates.
There are two key interactions that contribute to diffuser torque τd. The first interaction is the propellant being ejected from the openings at the outlet end of the diffuser. This directly imparts a torque τazi about the central axis A of the diffuser. The second interaction is the propellant colliding with walls of the channel before being ionized. This collision transfers some of the momentum back into the thruster body, effectively canceling out a portion of the torque ejection torque τazi.
The torque imparted by propellant ejection can be modeled by the equation
where ro is the radius from the propellant exit orifice of the diffuser to the central axis A of the thruster, {dot over (m)} is the propellant mass flow rate, kB is Boltzmann's constant, Ti is the incident temperature of the propellant in Kelvin, m is the mass of a propellant particle, θ is the angle of ejection with respect to a radial plane (see
From here, a rough order of magnitude estimate can be made. Reasonable estimates for the values in Eq. 1 for a xenon-propelled SPT-140 Hall thruster as used in the NASA Psyche mission yields τazi≈10 μNm, for a divergence efficiency of 50%. TABLE I lists order of magnitude estimated values for injection torque parameters.
Assuming rarefied propellant flow, the net torque on a channel wall by a propellant particle is given by
where rw is the radius from the wall to the central axis A, Aeff is the effective wall surface area over which the torque is acting, α is the diffuse accommodation coefficient, ϕi represents the momentum flux incident on the wall, ϕr,d represents the diffuse contribution of reflected momentum flux, and ϕr,s represents the specular contribution of reflected momentum flux. The momentum fluxes are given as
where ni is the incident number density of particles, Tw is the channel wall temperature, and the reduced velocity
where ūi is the average incident speed and β is the angle of incidence with the wall. The above equations are highly nonlinear. Nevertheless a rough order of magnitude estimate can be made.
For the values listed in TABLE II, ϕi and ϕr,d are on the order of 10−4, with ϕi>ϕr,d.
A very rough estimate for the wall torque τwall is therefore τwall≈10−2 μNm, which is two orders of magnitude smaller than the estimated ejection torque injection torque τazi. Assuming the propellant experiences only one wall collision before ionization, the net torque applied on the system by the ejection of propellant from the diffuser is
If subsequent wall collisions occur before ionization, additional τwall interactions would need to be subtracted in Eq. 6. However, it appears from the above estimates that τwall<<τazi, such that many wall collisions would be required to make a significant difference. After ionization occurs, the ions are accelerated quickly out of the thruster body, and wall interactions can likely be ignored.
Based on the above estimates, the counter-torque τd exerted by the propellant diffuser on the thruster body is on the order of 10 μNm. The NASA Psyche mission estimated its swirl torque τswirl to be 267 μNm, meaning a gas diffuser as configured above—i.e., where the ejection velocity V is tangential and the ejection angle approaches zero (e.g. θ<10°)—can offset approximately 3.7% of the Psyche swirl torque. If the diffuser parameters include an ejection angle θ=10° and a divergence efficiency ηd=90%, the amount of counter-torque τd can be increased to approximately 12% of swirl torque. If the propellant is further pre-heated to a temperature of 500 K prior to ejection, this can be raised to 15.6%. Based on these estimates, it is believed that a counter-torque τd in a range between 10% and 20% of a Hall current induced swirl torque τd can be achieved.
While it is not entirely known what factors most affect divergence efficiency, shrinking the size of the orifice propellant outlet orifices (e.g., smaller diameter propellant channels) and increasing the mass flow rate may force the propellant gas out of the rarefied regime into a translational or fluid regime that would reduce jet divergence and increase the efficiency parameter. However, the near-vacuum condition in the thruster channel makes it difficult to determine a true maximum achievable efficiency term.
Consistent with the above description, embodiments of a method of operating a spacecraft 60 including a Hall effect thruster system 12 include ejecting an ionizable propellant into an annular thruster channel 16 of the system in a direction that counteracts a torque induced on the thruster system by a Hall current provided in the annular channel. As noted above, the propellant can be ejected into the thruster channel 16 from a diffuser 1, and the diffuser may be configured so that the direction of propellant ejection has a tangential component or is a tangential direction. The direction of propellant ejection can be defined at least in part by the shape of the propellant channels 8 formed in the diffuser body 10, which is preferably helical or otherwise curvilinear.
It is to be understood that the foregoing description is of one or more preferred example embodiments of the invention. The invention is not limited to the particular embodiment(s) disclosed herein, but rather is defined solely by the claims below. Furthermore, the statements contained in the foregoing description relate to particular embodiments and are not to be construed as limitations on the scope of the invention or on the definition of terms used in the claims, except where a term or phrase is expressly defined above. Various other embodiments and various changes and modifications to the disclosed embodiment(s) will become apparent to those skilled in the art. All such other embodiments, changes, and modifications are intended to come within the scope of the appended claims.
As used in this specification and claims, the terms “for example,” “e.g.,” “for instance,” and “such as,” and the verbs “comprising,” “having,” “including,” and their other verb forms, when used in conjunction with a listing of one or more components or other items, are each to be construed as open-ended, meaning that the listing is not to be considered as excluding other, additional components or items. Other terms are to be construed using their broadest reasonable meaning unless they are used in a context that requires a different interpretation.
Number | Date | Country | |
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63340566 | May 2022 | US |
Number | Date | Country | |
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Parent | 18196017 | May 2023 | US |
Child | 18802838 | US |