Field propulsion

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Rendering of the deployment of a solar sail for the Advanced Composite Solar Sail System (ACS3), released by NASA in 2023. Advanced Composite Solar Sail System deployment.gif
Rendering of the deployment of a solar sail for the Advanced Composite Solar Sail System (ACS3), released by NASA in 2023.

Field propulsion comprises proposed and researched concepts and production technologies of terrestrial or spacecraft propulsion in which thrust is generated by coupling a vehicle to external fields or ambient media rather than by expelling onboard propellant. In this broad sense, field propulsion schemes are thermodynamically open systems that exchange momentum or energy with their surroundings, for example by coupling to photon streams, radiation, magnetized plasma, or planetary magnetospheres. By contrast, hypothetical reactionless drives are closed systems that would claim to produce net thrust without any external interaction, a category widely regarded as inconsistent with the law of conservation of momentum and with established physics including the Standard Model.

Contents

Within aerospace engineering research, the label spans both established and proposed approaches that "push off" external reservoirs. Environment-coupled examples include photonic pressure from sunlight (sails), charged particle streams such as the solar wind (magsails and related magnetic structures), and interactions with planetary magnetospheres and ionospheric environments (electrodynamic tethers). In narrower usage, the term also covers efforts to engineer field–matter coupling using electromagnetic propulsion (for example electrohydrodynamics and magnetohydrodynamics) as well as speculative mechanisms that draw on general relativity, quantum field theory, or zero-point energy ideas to alter effective inertia or to couple directly to non-particulate fields of space.

Several elements of field-coupled propulsion have been demonstrated in the laboratory, field tests, and in low Earth orbit, most notably sails and tethers. Many spacecraft propulsion devices that rely on strong electromagnetic fields still expel carried propellant, and therefore close momentum through exhaust rather than through environmental momentum exchange. Field propulsion concepts developed alongside conventional rocketry, appearing in early classifications of advanced propulsion and in later criteria-driven research programs. The topic has been treated in targeted programs such as NASA's former Breakthrough Propulsion Physics Program and in studies by national space agencies, academic research groups, and industry organizations investigating propellantless or externally powered alternatives to conventional rocket engines and electric propulsion systems.

Background

A familiar traditional rocket launch of SpaceX Falcon Heavy in 2018. Falcon Heavy Demo Mission (39337245145).jpg
A familiar traditional rocket launch of SpaceX Falcon Heavy in 2018.
A view of the end of the thruster unit from Yamato 1, built in 1991, and its magnetohydrodynamic drive system, at the Ship Science Museum in Tokyo. Magnetohydrodynamic drive.jpg
A view of the end of the thruster unit from Yamato 1, built in 1991, and its magnetohydrodynamic drive system, at the Ship Science Museum in Tokyo.

The term field propulsion generally refers to propulsion system concepts in which thrust arises from interactions with external fields or ambient media, rather than primarily from onboard chemical propellant. [1] Examples include solar sails, magnetic sails, and electrodynamic tethers, which couple with external photon, plasma, or magnetic fields instead of expelling onboard propellant. [2] :1–2 Field propulsion is not a single technology but a spectrum of approaches, ranging from mature concepts that have been tested in flight to highly speculative theoretical constructs. [3] :2

Various types of field propulsion concepts include mechanisms where motion results from environmental coupling rather than from carrying and ejecting propellant. [4] :215–216 By interacting with such external reservoirs, a spacecraft can "push off" the surrounding medium, converting environmental energy or momentum into acceleration. [4] :216–217 In contrast, conventional rockets achieve motion by expelling mass. [5] :5–6 Most commonly, this is the combustion output from chemical propellants to generate thrust via Newton's third law, which is the familiar rocket launch with explosive flame and smoke beneath it. [5] :5–6

History of research and programs

Medium close-up view, captured with a 70 mm camera, shows tethered satellite system deployment in 1996 during STS-75. STS-75 Tethered Satellite System deployment.jpg
Medium close-up view, captured with a 70 mm camera, shows tethered satellite system deployment in 1996 during STS-75.

Traditional rocketry has dominated aerospace propulsion in the 20th and early 21st centuries. [6] Field propulsion concepts evolved alongside rocketry. Early research focused on electrical and electrostatic concepts. [7] :8 Over time, research treated field propulsion concepts as long-range prospects rather than near-term systems, as the terminology of "field" propulsion evolved and was kept alive in successive planning and research cycles. [8] :25 Field propulsion developed as a parallel conceptual track alongside conventional rocketry, moving between speculative physics, engineering classification frameworks, and periodic experimental demonstrations. While many proposals remained theoretical, certain environment-coupled systems such as electrodynamic tethers and solar sails were eventually demonstrated in space. [9] [10]

Early 20th century to the 1960s

Konstantin Tsiolkovsky writing in 1911 included an early published statement of the basic electric-propulsion idea: using electricity to increase the velocity of ejected particles. Tsiolkovsky wrote: [7] :4

It is possible that in time we may use electricity to produce a large velocity for the particles ejected from a rocket device.

Edgar Choueiri, writing in Journal of Propulsion and Power , described a 1917 patent application by Robert H. Goddard, granted in 1920, as "the world’s first documented electrostatic ion accelerator intended for propulsion." [7] :8 In his 1918-1919 manuscript "To whomsoever will read in order to build", Yuri Kondratyuk discussed electric propulsion in the context of cathode rays and described thrust from electrically discharging and repelling material particles, alongside a schematic that Choueiri noted may be the "first conceptualization of a colloid thruster". [7] :10 In 1928, J. Navascués of León, Spain described a field coupled dynamo-electric machine concept "producing translatory motion of machine by current reaction with earth's field", in which "Propulsion is caused by cutting with a closed conducting turn the earth's magnetic flux". [11] :7231 Hermann Oberth's 1929 book Wege zur Raumschiffahrt was cited by Choueiri as having "defined, for the first time publicly and unambiguously", that related propulsion concepts were "a serious and worthy pursuit in astronautics". [7] :11

Valentin Glushko joined the Gas Dynamics Laboratory in Leningrad in 1929, and by 1933 with staff developed an early electric thruster prototype, an electrothermal approach intended for spacecraft propulsion. [7] :11 The device was likely the first electric thruster to ever be studied on a thruster stand, and was the first electrothermal thruster ever built. [7] :11–12 According to Choueiri, early thinking and experimentation in related propulsion research focused mainly on electrostatic concepts, but that the first laboratory electric thruster was electrothermal and the first electric thruster to fly in space was a mostly electromagnetic pulsed plasma device. [7] :8

After the 1930s, related field propulsion research concepts reached a lull in public published activity for over a decade through and after World War II, appearing mainly in science fiction rather than in sustained technical development. [7] :12 The first clear postwar reappearance of these propulsion concepts in open scientific literature was in December 1945, in the Journal of the American Rocket Society , where the term "ion rocket" was first coined by Herbert Radd. [7] :12 In 1947 at Fort Bliss, Wernher von Braun encouraged Ernst Stuhlinger to investigate his spacecraft propulsion ideas, telling Stuhlinger, "I wouldn't be a bit surprised if one day we flew to Mars electrically!" [7] :13 The Franklin Institute's astronautics lecture series in 1958 included a section explicitly titled 'Field Propulsion', describing propulsion 'by the use of fields' as a way to avoid an exhaust jet. [12] :46–47 U.S. Air Force general Donald L. Putt predicted that upcoming spacecraft would deploy "photo or ion field-type propulsion". [13] :6

1960s-1970s

During the 1960s through the 1970s, electric and electromagnetic propulsion matured experimentally, with some systems flying in limited operational roles even as they continued to rely on propellant despite their strong field components. [14] :1–2 [5] :10–11,623 As spaceflight programs expanded throughout the 1960s, contractor studies for the U.S. Air Force and NASA organized advanced and theorized advanced propulsion concepts under three main headings: Thermal, Field, and Photon, so that unconventional ideas for spaceflight could be compared within a common framework. [8] :26 United Press International reported that in 1964 there was a proposal from the Westinghouse Air Brake Company to link Youngstown, Ohio with Pittsburgh via a "super conductor magnetic field propulsion" transit system. [15] :9

On July 20, 1964, two electrostatic ion engines were tested in space in the Space Electric Rocket Test (SERT I), and the mercury electron-bombardment engine produced thrust in flight. [16] :13 A University of Colorado paper from the Ann and H.J. Smead Department of Aerospace Engineering Sciences described SERT I as "not only the first electric satellite it was also the first spacecraft to incorporate any kind of electric propulsion." [17] :1,4 It reported that the mission's mercury electron bombardment ion engine "ran for 31 minutes becoming the first electric engine ever to operate in space." [17] :4 The November 30, 1964 Zond 2 mission to Mars from the Soviet Union marked the first planetary use of electric propulsion, followed by successive U.S. deployments culminating in the Nova satellite series. [14] :1

The Chicago Tribune reported on early NASA advocacy of field propulsion, called then "field resonance propulsion", and noted some research of magnetohydrodynamics began in 1971, as an extension of training astronauts on solar physics. [18] :15 A 1972 report from the Air Force Rocket Propulsion Laboratory, followed by Jet Propulsion Laboratory studies in 1975 and 1982, formalized this division by publishing roadmaps that again divided advanced concepts into the same Thermal, Field, and Photon classes as prior 1960s research had. [8] :25–26 These reports emphasized "infinite specific impulse" systems would obtain energy or working fluid from the ambient environment and suggested new advances in lasers and superconductors could breathe new life into earlier discarded concepts such as laser propulsion or ramjets. [8] :25–26,406

1980s-1990s

In the 1980s, earlier classification frameworks began giving way to attempts to identify and organize specific physical coupling mechanisms capable of producing measurable thrust. In 1980, NASA scientist Al Holt noted that proposed models for field propulsion interactions in this era ranged from Albert Einstein's united field theory efforts to work by "serious 'amateurs'," reflecting how wide the speculative literature around such ideas had become by that period. [19] That year, Holt was quoted by the Chicago Tribune in his advocacy of field propulsion: "One of the most important things to me is to help break down the inhibiting mental attitude that space-time field interactions will remain in the realm of science fiction for hundreds of years." [18] :18 Holt argued that progress toward field-dependent propulsion would require a dedicated "field physics laboratory" to quantify relationships among gravitation, electromagnetism, and spacetime structure, framing the potential payoff as performance beyond then-leading aircraft and spacecraft such as the Space Shuttle, SR-71A, and F-16. [19]

The Huntsville Times reported on a program by TRW Inc.'s Defense and Space Systems Group researching magnetic field based field propulsion, called "force field propulsion", for vehicle launch applications. [20] :4 In 1980, the Chicago Tribune highlighted solar electric propulsion as a possible field propulsion option under research. [18] Robert L. Forward in 1984 extended beamed-sail studies to the interstellar scale, suggesting that phased solar-system lasers could impart sustained acceleration to ultralight sails across astronomical distances. [21] :187 He calculated that such a system might accelerate a probe to ~0.11 c and reach Alpha Centauri in about four decades, bringing the timescale of an interstellar flyby to within a human lifetime. [21] :187,193

In 1990, the Daily Telegraph reported on Japanese development work toward a magnetohydrodynamic propulsion ship, including plans to install the magnetic propulsion equipment and conduct at-sea testing. [22] :11 By 1991–1992, the Ship & Ocean Foundation's experimental ship Yamato 1 had been completed and successfully propelled by superconducting MHD thrusters during trials in Kobe Harbor. [23] :402 A harbor demonstration in 1992 of Yamato 1 was completed using a superconducting magnetic propulsion system. [24] In 1992, the New York Times described U.S. investment in maglev development, noting that maglev trains would be lifted on magnetic cushions and propelled along a guideway by alternating magnetic fields that create a "magnetic wave". [25] :9 The report said Congress had authorized a six-year, $700 million demonstration program and noted existing demonstration systems in Germany and Japan, including a reported speed record of 273 miles per hour on a test track. [25] :9

STS-75 in 1996 deployed and proved the functionality of the space tether field propulsion concept on the 19th mission of the Columbia NASA Space Shuttle orbiter. [26]

NASA's Breakthrough Propulsion Physics Project (BPP) in 1998 framed research around the goals of propulsion with no propellant mass, maximum physically possible transit speeds, breakthrough energy sources, and emphasized empirical testability. [3] :1,3–4 Marc Millis of BPP framed the related "space coupling propulsion" problem as requiring a tangible reaction-mass-like property of the vacuum and a controllable coupling mechanism that yields net external thrust. [27] :93,94–95,95 It raised the question of whether propellantless effects could exist without violating conservation of momentum and energy. [3] :6 The more speculative end of the spectrum, such as concepts that couple to the environment without carrying reaction mass, remained in the research phase. [3] :1–2 [4] :215–216 BPP reframed field propulsion from a catalog of ideas into a research program defined by falsifiable physical requirements. Programmatically, BPP marked a shift from earlier classification-based surveys toward criteria-driven evaluation, establishing conservation-law consistency, measurable coupling mechanisms, and experimental reproducibility as the central benchmarks for field propulsion research. [3] :1–2,6

21st century

The British National Space Centre and Society of British Aerospace Companies began organizing an annual field propulsion research conference in 2001, inaugurated in Brighton at the Institute of Development Studies, with initial delegates including Harry Kroto. [28] [29] :13 British Aerospace was confirmed in 2001 to have initiated a research program called "Project Greenglow" to research "the possibility of the control of gravitational fields." [30] [29] :13

Subsequent work largely extended this research, examining whether identifiable environmental interactions could meet the same conservation law and measurement criteria. Later NASA Institute for Advanced Concepts (NIAC) studies continued in the same mold, examining whether Alfvén wave coupling or other plasma interactions might provide quasi-propellantless thrust. [2] :1–2 Yoshinari Minami of the Advanced Space Propulsion Investigation Committee argued in 2003 that a potential propulsion "breakthrough" could rely on field propulsion, defined as employing "a physical means to asymmetrically interact with the space vacuum." [31] :350 In its 2009 interstellar-transport discussion, Future Spacecraft Propulsion Systems described a then emerging category of "breakthrough propulsion concepts," including warp drive, traversable wormholes, and vacuum-energy ideas, while also noting strong skepticism about claims that appeared to conflict with conventional demonstrated physics. [32] :450–451 Millis summarized the matter as: "For field propulsion, the fields themselves must act as the reaction mass." [27] :95

LightSail 1 and LightSail 2 flew between 2015 and 2019, with functional field propulsion systems active in outer space. [9] [10]

Definitions

"Field" refers broadly to approaches that might exchange momentum or energy with external reservoirs, such as plasmas, magnetic fields, or directed energy sources, and therefore contrasted with both conventional rockets and nuclear-thermal designs. [8] :26 Examples of field propulsion technologies include systems that attempt to draw on the photon field of sunlight, the charged particles of the solar wind, or the magnetic fields of planetary environments. [2] :1–2 Broad definitions often include solar sail systems. [33] [34] :3 Magnetic sail concepts proposed by Dana Andrews and Robert Zubrin envisioned the use of large magnetic fields to couple with the solar wind and thereby transfer momentum to the spacecraft. [2] :1–2 [35] :197

Narrower definitions, however, focus on experimental electromagnetic propulsion mechanisms, including electrohydrodynamics (EHD) [36] :2 and magnetohydrodynamics (MHD), as well as more speculative proposals that invoke general relativity, quantum field theory, or zero-point energy as possible pathways to modify inertia or couple directly to the structured quantum vacuum. [4] :215–216,219

Momentum conservation is the fundamental boundary on all propulsion concepts. [3] :2 Conservation of momentum is a fundamental requirement of propulsion systems because momentum is always conserved. This conservation law is implicit in the published work of Isaac Newton and Galileo Galilei, but arises on a fundamental level from the spatial translation symmetry of the laws of physics, as given by Noether's theorem. [37] Open systems comply with the conservation of momentum by transferring it to or from the surrounding environment. [4] :216–217 Conservation laws can be satisfied in field propulsion via interaction with "a mass, a massive body, electromagnetic radiation, and space as a vacuum," as Minami described, adding that the "most promising interpretation" is treating vacuum as "a kind of reaction mass." [31] :351

For instance, MHD drives accelerate conductive fluids using electromagnetic fields, resulting in thrust through the Lorentz force, with momentum conserved via interaction with external media, such as the interplanetary or interstellar media, or solar winds. [36] :2 Environment-coupled approaches such as sails, tethers, or plasma-wave coupling remain possible if the method of external coupling is strong enough. [2] :1–2,11–12 Across all of these efforts, technical and scientific reviews acknowledged the conceptual appeal of field propulsion but also stressed the unresolved consistency issues that arise when no clear external momentum channel can be identified. [3] :2

Any propulsion method that claims to generate net thrust in a closed system without external interaction challenges physical law and is considered untenable under the Standard Model of physics, [a] Millis notes that proposed "space drive" schemes where forces act only internally produce no net motion, and relates this "net external force requirement" to the conservation of momentum. [40] :2–3 Some field propulsion reviews note that open systems exchange momentum or energy with external media and that proposals of closed-system 'reactionless drive' propulsion are viewed with skepticism because they conflict with thermodynamic laws and established scientific principles. [3] :2 [4] :216–217 Some speculative field propulsion concepts may require extensions to established physical theories, including beyond the Standard Model of particle physics and cosmology. [41] :9

Scope and terminology

Published technical surveys and program documents use "field" or field-adjacent language in different ways. Contractor studies for NASA grouped "advanced" options under headings such as Thermal Propulsion, Field Propulsion, and Photon Propulsion, with "field" covering externally powered and field-interactive concepts beyond conventional rocketry. [8] :26 BPP's research goals at NASA explicitly included "propulsion that requires no propellant mass," maximum physically possible transit speeds, and breakthrough energy methods to power such devices, framing the field propulsion question in terms of fundamental physics limits and testable claims. [3] :1 Framed with an emphasis on empirical testability, the BPP stated three goals: propulsion that requires no propellant mass, transit at the maximum speeds physically possible, and energy sources to power such devices. [3] :1,3–4 Separately, NIAC funded studies on using ambient plasmas and magnetic fields (e.g., solar wind, magnetospheres) to generate thrust without expelling onboard propellant, including Alfvén-wave coupling concepts. [2] :1–2

In practice, the viability of any open field-coupled concept depends on coupling strength to the surrounding environment. For example, momentum exchange with the solar wind or a magnetosphere scales with local plasma density, magnetic-field magnitude, and wave/field interaction efficiency; in weak or highly variable environments, thrust and control authority are correspondingly limited. [2] :7–10 These constraints contrast with classical chemical and conventional electric rockets, whose performance is governed primarily by onboard propellant and its energy, reflecting fundamental engineering limits on achievable exhaust velocity and energy density. [5] :39–40 Electromagnetic propulsion reviews describe solid-propellant pulsed plasma, magnetoplasmadynamic systems, and pulsed inductive thrusters as electromagnetic spaceflight technologies. [14] :1 Later NIAC work examined momentum exchange with ambient plasmas and magnetic fields as propellantless or quasi-propellantless mechanisms. [2] :1–2 Hypothetical field propulsion systems, in contrast, are framed in the literature as propellantless but encounter dependence on external media and unresolved consistency with conservation laws. [3] :2 Practical interstellar exploration was framed as a combined problem of propulsion theory and navigation theory, rather than as a propulsion-only problem. [42] :1419,1420

Beamed-energy propulsion

LightSail-2 with deployed solar sail, July 23, 2019. LightSail 2 with deployed solar sail.png
LightSail-2 with deployed solar sail, July 23, 2019.

Beamed-energy propulsion sends power from a remote source directly to a spacecraft propulsion system, using directed-energy technologies such as lasers, microwaves, or relativistic charged-particle beams, so that the propulsion power source remains independent of the spacecraft. [8] :iii,II-1 A NASA contractor report, Advanced Beamed-Energy and Field Propulsion Concepts, surveyed beamed-energy and field propulsion concepts, seeking improvements beyond chemical rocket propulsion to achieve large gains in payload, range, and terminal velocity, and focused on systems where power is beamed to the vehicle by laser, microwave, or relativistic charged particle beams so that the power source remains independent of the spacecraft. [8] :I-2,II-1 The NASA report organized prospects into thermal, field, and photon classes and identified enabling technologies (e.g., higher-current superconductors, potential room-temperature superconductors, metallic hydrogen) as then-potential paths to field propulsion prospects. [8] :I-2 It also described large swings in advanced propulsion funding over the previous decades, and highlighted significant studies by AFRPL (1972) and JPL (1975, 1982) as part of that history. [8] :I-1 The study emphasized a return to the unrestricted creativity and "free-thinking" that characterized propulsion research in the late 1950s and early 1960s. [8] :I-2

The AFRPL study concluded that propulsion researchers should focus on "infinite specific impulse" (Isp) concepts that draw both working fluid and energy from the ambient environment, because of their implications for outstanding performance. [8] :I-2 Some approaches use atmospheric or environmental material as working fluid or interaction medium, drawing reaction mass or momentum exchange from the ambient environment rather than from onboard propellant. [8] :I-2,IX-14–IX-15 Proposals also include advanced electrostatic and MHD-based concepts that could leverage charged particle interactions with atmospheric fields or ionospheric plasmas and geomagnetic fields to produce directed motion. [8] :IX-14–15,IX-33,XIII-1–3 The study suggested improvements in technologies like high-power lasers or new energy transfer methods could revitalize previously discarded propulsion ideas, including laser propulsion and infinite-Isp ramjets. [8] :I-2

Ambient plasma-wave propulsion

A NIAC Phase I study evaluated "ambient plasma wave propulsion," focusing on wave-mediated interactions with existing space environments including solar wind and magnetospheres. [2] :1–2 The study highlighted the appeal of no onboard reaction mass requirements for the method, combined with limits such as technical immaturity and shortfall of such concepts for significant maneuvering capabilities. [2] :11–12

Theoretical proposals

Alcubierre metric, related to Alcubierre drives, by Harold G. White, NASA Johnson Space Center. It depicts a "warp bubble", of artificial expansion of spacetime behind and contraction in front of a theoretical spacecraft, to generate propulsion. Alcubierre Metric, Nasa, Sonny White 2011-09-02.png
Alcubierre metric, related to Alcubierre drives, by Harold G. White, NASA Johnson Space Center. It depicts a "warp bubble", of artificial expansion of spacetime behind and contraction in front of a theoretical spacecraft, to generate propulsion.

NASA's Breakthrough Propulsion Physics (BPP) memo framed research questions at the limits of physics—no-propellant propulsion, ultimate transit speeds, and breakthrough energy production—explicitly to sort physically testable ideas from non-viable claims. [3] :1 Field propulsion alone was described as insufficient for practical interstellar exploration because no propulsion theory currently exceeds the speed of light, requiring a navigation theory as a secondary solution alongside propulsion theory. [42] :1419 A 2009 propulsion survey framed one motivation for field propulsion research in operational terms, arguing that if field interactions could reduce effective gravitational and inertial resistance, rocket thrust and propellant requirements for Earth-to-orbit flight would be substantially reduced. [32] :439

Minami and Musha in their 2012 study reviewed proposals that treat space as having a substantial physical structure, described at macroscopic scales by general relativity and at microscopic scales by quantum field theory. [4] :215–216 They outlined mechanisms such as vacuum polarization, engineered spacetime curvature, and zero-point field interactions. [4] :219 Their study frames the topic for this branch of field propulsion as theoretical as of 2012, and point to engineering that would excite localized regions of space. [4] :220 This dual framework places field propulsion concepts at the intersection of general relativity, which treats spacetime as a dynamic geometry, and quantum field theory, where the vacuum hosts fluctuating fields and latent energy. [4] :218–219

Minami's navigation theory framing was situated within similar extra-dimensional theory discussions, including Kaluza-Klein theory, supergravity theory, superstring theory, M theory, and D-brane-related superstring theory, as part of the paper's conceptual background for interstellar navigation. [42] :1420 Several mechanisms have been theorized to achieve such coupling, including spacetime-curvature effects in general relativity and interactions with electromagnetic zero-point fields in quantum field theory. [4] :216,218–219

Vacuum-fluctuation phenomena such as the Casimir effect have been measured in many precision experiments and are reviewed extensively in the mainstream literature. [43] :1827,1829–1830 However, attempts to obtain net thrust or a gravity coupling from static electromagnetic configurations (often framed as "electrogravitic" effects) have not produced reproducible anomalous forces in controlled tests. [44] :2,15 [45] :315,318

Types

NEXIS xenon ion engine testing in 2005. NEXIS thruster working.jpg
NEXIS xenon ion engine testing in 2005.
Magnetic waves, called Alfven S-waves, flow from the base of black hole jets. PIA19822-MagneticBlackHoleWaves-AlfvenS-waves-20150709.jpg
Magnetic waves, called Alfvén S-waves, flow from the base of black hole jets.

A wide range of propulsion methods have been proposed or demonstrated that fit within broad definitions of field propulsion. This taxonomy reflects how late twentieth-century contractor reports and program reviews organized the subject, and how later surveys distinguish environment-coupled momentum exchange from electric-propulsion devices that expel carried propellant. [8] :26 [2] :1–2 [14] :1–2 One group comprises environment-coupled systems that utilize their surroundings to produce thrust, including solar sails, magnetic sails, and, with certain restrictions, electrodynamic tethers, which use the solar wind or ambient magnetic fields to generate thrust. In one example design, a magnetic sail uses a loop of superconducting cable to create a magnetic field that deflects solar wind plasma and imparts momentum to the attached spacecraft. [2] :1–2 [35] :197 Other concepts use strong electromagnetic fields to accelerate carried propellant plasma (electric and electromagnetic thrusters). [14] :1 A more speculative class invokes direct interactions with a structured vacuum or with spacetime geometry, proposing thrust without expelling mass, an idea discussed in general relativity and quantum field theory literature but not empirically validated. [4] :215,218–219 The sections below follow this usage, separating internally accelerated propellant systems from approaches that exchange momentum with external fields or media.

Demonstrated

This section covers approaches with experimental validation, flight heritage, or sustained engineering development, including both propellant-expelling thrusters and environment-coupled systems.

Electric and electromagnetic with carried propellant

Several devices central to electromagnetic propulsion rely on strong fields yet remain conventional in the momentum sense because they accelerate carried propellant. [5] :647–649 A NASA electromagnetic-propulsion review identified three main types of electromagnetic propulsion systems: pulsed plasma thrusters (PPTs), magnetoplasmadynamic thrusters (MPD), and pulsed inductive thrusters (PIT). [14] :1 Representative families include pulsed plasma thrusters (PPTs), magnetoplasmadynamic thrusters (MPD), and pulsed-inductive thrusters (PIT), each with distinct trade-offs in lifetime, efficiency, and power scaling; PPTs have flown for attitude and drag makeup, MPD has flight heritage in experimental regimes, and PIT remains ground-tested. [14] :1–2

The review noted benefits of using electromagnetic thrusters include their ability to provide precision for satellite positioning, high specific impulse, robustness, high power processing capability, and simplicity; pulsed thrusters also permit relatively simple system level scaling with available spacecraft power. [14] :1 Within the electric-propulsion family, these devices illustrate how strong fields can dominate the internal acceleration physics while momentum closure still proceeds through exhaust. [14] :5–8 In programmatic roadmaps, these technologies frequently serve as baselines for comparison with environment-coupled concepts, anchoring expectations for power-to-thrust ratios, lifetime, and system mass at mission-relevant scales. [5] :648–649 [14] :5–8

A 1966 NASA Lewis Research Center overview stated that electric-propulsion spacecraft then under study could not be expected to take off from Earth and therefore would need to be launched to Earth orbit by chemical rockets before beginning low-thrust operation. [16] :6

PPTs are the only electromagnetic thrusters used on operational satellites, though both PPT and MPD thrusters have been flown in space. [14] :1 These efforts culminated in first flights of solid propellant pulsed plasma thrusters in the Soviet Union in 1964 and in the United States in 1968. [14] :1 Developed in the late 1960s, these thrusters initiate an arc discharge across a solid fluorinated polymer bar, ablating a small amount of propellant and accelerating it by the Lorentz body force. [14] :2 Unlike later concepts relying on inductive or steady-state operation, PPTs utilize compact, low-power, pulsed configurations suitable for satellite positioning and drag compensation. [14] :1,4

MPDs are another major class of electromagnetic propulsion systems investigated for both quasi-steady and steady-state spaceflight applications. [14] :5 MPDs operate through the Lorentz force generated by the interaction of discharge currents with self-induced or externally applied magnetic fields. [14] :5 MPD devices had space heritage in experimental regimes. [14] :1,8

PITs are a form of electromagnetic propulsion developed to overcome the erosion and lifetime limitations of electrode-based systems. [14] :8 By inducing plasma currents through time-varying magnetic fields, PITs accelerate neutral propellants without requiring physical contact between conductors and plasma. [14] :8 PITs sought to reduce electrode-erosion limits by inductive coupling. [14] :1,8 The concept originated in the late 1960s and evolved through successive experimental designs focused on performance scaling, circuit optimization, and propellant compatibility. [14] :7 Although no PIT system has flown in space, the thruster class remains of interest due to its potential for high-efficiency, long-duration propulsion with minimal material degradation, particularly in missions requiring flexible propellant selection and reduced contamination risk. [14] :7

Electron cyclotron resonance thrusters (ECR) use electron cyclotron resonance to ionize and accelerate a gaseous propellant (commonly xenon), particularly in ionospheric or high-altitude environments. ECRs using electron cyclotron resonance with microwave discharge have flown in space, most notably as the μ10 ion engine system on JAXA's Hayabusa and Hayabusa2 asteroid missions. [46] :2 [47] :2

Environment-coupled momentum exchange

Artist rendering of an interstellar light sail space craft Light Sail Probe to Alpha Centauri (26338959171).jpg
Artist rendering of an interstellar light sail space craft
NASA Goddard Space Flight Center schematic of Earth's magnetosphere showing regions of naturally occurring plasma waves (including chorus, magnetosonic, ultra-low frequency waves, and plasmaspheric hiss). These ambient wave-particle interactions are the type of environments that plasma-wave spacecraft propulsion concepts propose to couple into. NASA magnetosphere plasma waves diagram.png
NASA Goddard Space Flight Center schematic of Earth's magnetosphere showing regions of naturally occurring plasma waves (including chorus, magnetosonic, ultra-low frequency waves, and plasmaspheric hiss). These ambient wave–particle interactions are the type of environments that plasma–wave spacecraft propulsion concepts propose to couple into.

These systems generate thrust by exchanging momentum with external fields (magnetic, plasma, or photon), without expelling onboard reaction mass. Solar sails are a propellant-less propulsion method that produces thrust from solar photon pressure (solar radiation pressure), rather than by expelling reaction mass. [1] [34] :4,5 As with other environment coupled concepts, sail performance depends on local solar photon pressure: the Interstellar Probe concept uses a very close solar flyby to take advantage of "increased solar flux" and the resultant "increased solar photon pressure", and scaling to a 160,000 m2 sail would require advances in sail materials, deployment, and attitude control systems. [34] :4 The Chicago Tribune in 1980 highlighted solar electric propulsion as a possible field propulsion option under research. [18]

Sailcraft engineering couples ultra-light structures to stringent pointing and thermal constraints. [48] :2990,2995 [21] :188 Square and heliogyro designs use thin film sails on deployable booms; reliable deployment of large, low-mass structures and thin films is a key challenge. [48] :2991,3004–3005 Typical sail films have reflective front coats and high-emissivity back coats; wrinkling and billowing reduce efficiency. [48] :2993–2995 Once deployed, thrust is almost normal to the sail, so small attitude changes steer the thrust vector. [48] :2990–2991 Performance evolves with materials science and control: lower areal density directly increases acceleration, [21] :188 and by canting the sail the small continuous thrust can be steered for precise trajectory shaping. [48] :2990 Forward ( Journal of Spacecraft and Rockets, 1984) outlined a proposed method of how solar-system-based laser systems and a ~1,000 km diameter Fresnel zone "para-lens" could propel thin-film sails to ~0.11 c, enabling an unmanned flyby of Alpha Centauri in approximately 40 years. [21] :187,193 In Forward's proposal, a two-stage sail system in which a massive ring sail reflects laser light back onto a detached payload sail, enabling the unmanned spacecraft to rendezvous and brake within the Alpha Centauri system. [21] :193–194

Magnetic sails couple a spacecraft-supported magnetic field to the solar wind, producing thrust through solar-wind deflection. [35] :197 Analyses of magnetic sail concepts indicate thrust arises from deflecting the solar wind around a spacecraft-supported magnetic field, with performance set by the stand-off distance at which solar-wind dynamic pressure balances the sail's magnetic pressure; larger effective magnetic cross-sections increase momentum transfer but require large-radius, high-current superconducting coils. [35] :197–199 Key engineering challenges include the mass and size of the superconducting loop and the constraints imposed by achievable superconducting currents and magnetic fields. [35] :197–199

Mission studies of magnetic sails show that they can perform heliocentric transfers between circular orbits by using the solar wind for outbound acceleration and inbound braking. [35] :197–199 Magsails have also been proposed for interstellar missions, where interaction with the interstellar medium provides propellantless terminal deceleration into a destination solar system. [35] :201–203 The design tradeoffs emphasize achieving a large effective magnetic cross-section for the superconducting loop while keeping its mass low. [35] :199 Magnetospheric plasma propulsion (M2P2) is a NIAC proposal by Robert Winglee, in which plasma injection inflates a magnetic bubble that couples with the solar wind. It is considered a variant of magnetic sails. [49] [50] NIAC studies proposed "ambient plasma wave propulsion" in which RF energy is coupled into ambient plasma using a spacecraft antenna, generating Alfvén waves that travel along ambient magnetic field lines; the report describes the wave as adding momentum to the antenna and spacecraft and thereby providing thrust as a "truly propellantless propulsion system". [2] :1–2 The 2011 Phase I assessment found the approach technically immature but potentially enabling if sensitivity and power challenges can be overcome. [2] :1,25–26

The most studied examples are electrodynamic tethers (EDT), which generate Lorentz-force-based drag or thrust by coupling a long current-carrying conductor to a planetary magnetic field, thereby exchanging momentum with a planetary magnetosphere or ionosphere to enable propellantless drag or thrust in suitable environments (e.g., low Earth orbit), fall under broad definitions of field propulsion due to their use of external fields for momentum exchange, and have been deployed in several space tether missions, including the TSS-1, TSS-1R, and Plasma Motor Generator (PMG) experiments. [2] :1 [51] :136–138 [52] :153–155,83–84 As open systems, they conserve momentum by reaction with the ambient plasma and magnetic field. [52] :188,153–155 In operation, a conductive tether moving through a planetary magnetic field experiences a motional electromotive force; closing the circuit through the ambient ionosphere allows current to flow, and the resulting Lorentz force can provide either drag (for deorbit) or, with external power injection, thrust along specific orbital geometries. [52] :137,146–147 Electrodynamic tethers can also generate electrical power at the expense of orbital energy. [52] :151

Development and testing

This section groups concepts under active engineering development or testing that adapt field-based acceleration or coupling principles for new operational regimes.

Beamed-energy and externally powered thrust

Microwave electrothermal thrusters use microwave energy, potentially externally supplied, to heat a fluid propellant. When powered externally, it falls under beamed-energy propulsion with mass acceleration via directed fields. Laser ablation propulsion uses pulsed laser energy to ablate onboard material into a plasma jet; although it expels mass, the energy source is external, placing it within beamed-energy propulsion approaches.

Czysz and Bruno described Leik Myrabo's beamed-energy Lightcraft work as a decades-long program and characterized the concept as a projected-power, combined-cycle MHD system that could reconfigure across multiple flight regimes. [32] :193 Research has been limited to laboratory testing and subscale atmospheric Lightcraft demonstrations, with orbital proposals remaining unflown. Photonic laser thrusters are a photon-pressure system that relies on externally beamed lasers instead of sunlight. They also highlighted the concept's very low onboard propellant requirement, writing that it had "the least onboard propellants of any system". [32] :193 Myrabo's architecture was described as scalable by siting the projector on Earth, in orbit, or on the Moon, explicitly noting propulsion implications for geosynchronous orbit, the Moon, and nearby planetary/moon systems. [32] :193

Environment-fed electric propulsion

Atmosphere-breathing electric propulsion is a concept where spacecraft collect ambient particles in low orbit, ionize them, and accelerate them using electromagnetic fields. It avoids onboard propellant but still involves mass acceleration. Ground prototypes have been tested (ESA Sitael, ABEP, JAXA), but not yet flown in space. Closest heritage are ion thrusters and Hall-effect thrusters, which have flown widely (Deep Space 1, Dawn, SMART-1, BepiColombo) and demonstrate the same field-acceleration principle with onboard propellant.

Field-interaction in atmosphere or dense media

Yamato-1 on display in Kobe, Japan. Yamato 1 Left Front View at Kobe Maritime Museum November 10, 2012 01.jpg
Yamato-1 on display in Kobe, Japan.

Although not presently in wide use for space, there exist proven terrestrial examples of field propulsion in which electromagnetic fields act upon a conducting medium such as seawater or plasma for propulsion, known collectively as magnetohydrodynamics (MHD). MHD is similar in operation to electric motors, however, rather than using moving parts or metal conductors, fluid or plasma conductors are employed. The EMS-1 and more recently the Yamato 1 [53] :562 are examples of such electromagnetic field-propulsion systems, first described in 1994. [54] Electrohydrodynamics (EHD) is another method where electrically charged fluids are accelerated for propulsion and flow control; laboratory and flight demonstrations include devices driven by corona discharge. [36] :2 [55] :532–535 Magnetohydrodynamic interaction concepts extending magnetohydrodynamics (MHD) to space plasma propose generating thrust by exchanging momentum with ambient charged particles via Lorentz-force coupling. If the interacting plasma is external (e.g., ionospheric or solar wind), the system qualifies as field propulsion. [32] :450–451 If the plasma is internally supplied and expelled, it instead falls under electromagnetic or electrothermal propulsion. [32] :450–451

Magnetic levitation (maglev) ground transport systems are another terrestrial example of propulsion via externally generated fields: maglev employs magnetic forces to lift, guide, and propel a vehicle over a guideway, with propulsion typically provided by a linear motor whose traveling magnetic field pulls or pushes the vehicle along the track. [56] [57] :2342

Proposed and theorized

These concepts are discussed in aerospace literature primarily as theoretical or exploratory frameworks rather than operational propulsion technologies.

Field propulsion based on physical structure of space

Representation of Earth curving surrounding spacetime in general relativity, illustrating how gravitational fields are treated as distortions of the underlying spacetime structure. Some proposed field propulsion concepts aim to couple with such structural changes. Spacetime lattice analogy.svg
Representation of Earth curving surrounding spacetime in general relativity, illustrating how gravitational fields are treated as distortions of the underlying spacetime structure. Some proposed field propulsion concepts aim to couple with such structural changes.

Minami and Musha frame field propulsion at the physics frontier as interaction with a "substantial physical structure" of space, drawing on general relativity at macroscopic scales and quantum field theory at microscopic scales. [4] :215–216 They conclude that future engineering technologies for space travel will most likely require some form of field propulsion to excite properties of localized regions in space. [4] :220 As one candidate concept, Minami treated space as "an elastic body like rubber" and argued that space curvature could create an "acceleration field," stating that "a space drive is produced in the region of curved space." [31] :352 A 1979 NASA technical memorandum outlined a speculative field resonance propulsion concept that hypothesized thrust from a resonance between coherent pulsed electromagnetic field waveforms and gravitational waveforms associated with spacetime metrics, framed as potentially enabling galactic travel without prohibitive travel times. [58] :ii

Potential concepts studied by NASA and other parties have included vacuum polarization, engineered spacetime curvature, and zero-point-field interactions; none have been experimentally validated, and all face unresolved consistency issues with momentum conservation. [3] :2 Minami and Musha distinguish between two field propulsion concepts: one framed in terms of general relativity and one in terms of quantum field theory. [4] :215–220 In the general relativistic field propulsion system, space-time is considered to be an elastic field similar to rubber, which means space itself can be treated as an infinite elastic body. [59] :20–21 In Minami and Musha's framing, propulsive force arises from interaction with a physical structure of space instead of from expelling reaction mass. [4] :216–217 According to quantum field theory and quantum electrodynamics, the quantum vacuum is modeled as a nonradiating electromagnetic background, existing in a zero-point state, the minimum energy allowed by the theory. [59] :24–25 It was proposed that using this on a dielectric material could, via the resulting Lorentz force on bound charges, affect the inertia of the mass and that way create an acceleration of the material without creating stress or strain inside the material. [4] :216–219

See also

Notes

  1. Here, "under the Standard Model" means within the Lorentz-invariant and translation-invariant relativistic quantum field theory framework used to formulate the Standard Model: spacetime symmetry under spatial translations implies conservation of linear momentum (Noether's theorem). [38] :8 [39] :17

References

PD-icon.svg This article incorporates public domain material from websites or documents of the United States government .

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