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Ion-propelled aircraft

From Wikipedia, the free encyclopedia
Electrohydrodynamic aircraft propulsion
This article is about ion propelled aircraft. For ion propelled spacecraft, seeIon thruster.

Anion-propelled aircraft orionocraft is anaircraft that useselectrohydrodynamics (EHD) to providelift orthrust in the air without requiringcombustion ormoving parts. Current designs do not produce sufficient thrust for crewed flight or useful loads.

History

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Origins

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The principle ofionic wind propulsion withcorona-generated charged particles was discovered soon after the discovery ofelectricity with references dating to 1709 in a book titledPhysico-Mechanical Experiments on Various Subjects byFrancis Hauksbee.

VTOL "lifter" experiments

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American experimenterThomas Townsend Brown spent much of his life working on the principle, under the mistaken impression that it was ananti-gravity effect, which he named theBiefeld–Brown effect. Since his devices produced thrust in the direction of the field gradient, regardless of the direction of gravity, and did not work in a vacuum, other workers realized that the effect was due to EHD.[1][2]

VTOL ion-propelled aircraft are sometimes called "lifters". Early examples were able to lift about a gram of weight perwatt,[3] This was insufficient to lift the heavy high-voltage power supply necessary, which remained on the ground and supplied the craft via long, thin and flexible wires.

The use of EHD propulsion for lift was studied by American aircraft designer MajorAlexander Prokofieff de Seversky in the 1950s and 1960s. He filed a patent for an "ionocraft" in 1959.[4] He built and flew a model VTOL ionocraft capable of sideways manoeuvring by varying the voltages applied in different areas, although the heavy power supply remained external.[5]

The 2008Wingless Electromagnetic Air Vehicle (WEAV), a saucer-shaped EHD lifter with electrodes embedded throughout its surface, was studied by a team of researchers led bySubrata Roy at theUniversity of Florida in the early part of the twenty-first century. The propulsion system employed many innovations, including the use ofmagnetic fields to enhance the ionisation efficiency. A model with an external supply achieved minimal lift-off and hover.[6][7]

Onboard power

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Twenty-first century power supplies are lighter and more efficient.[8][9] The first ion-propelled aircraft to take off and fly using its own onboard power supply was a VTOL craft developed by Ethan Krauss of Electron Air in 2006.[10] His first patent application was filed in 2014, and he was awarded amicrogrant to support his project byStardust Startups in 2017.[11] The company currently owns US patent 10119527B2 and 11161631B2 in relation to this field.[12] The craft developed enough thrust to rise rapidly or to fly horizontally for several minutes.[10][13]

In November 2018 the first self-contained ion-propelled fixed-wing airplane, theMIT EAD Airframe Version 2 flew 60 meters. It was developed by a team of students led by Steven Barrett from theMassachusetts Institute of Technology. It had a 5-meter wingspan and weighed 2.45 kg.[14] The craft was catapult-launched using an elastic band, with the EAD system sustaining the aircraft in flight at low level.

Principles of operation

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Ionicair propulsion is a technique for creating a flow of air throughelectrical energy, without any moving parts. Because of this it is sometimes described as a "solid-state" drive. It is based on the principle of electrohydrodynamics.

In its basic form, it consists of twoparallelconductiveelectrodes, a leading emitter wire and a downstream collector. When such an arrangement is powered by highvoltage (in the range of kilovolts per mm), the emitterionizes molecules in the air that accelerate backwards to the collector, producingthrust in reaction. Along the way, these ions collide with electrically neutral air molecules and accelerate them in turn.

The effect is not directly dependent on electrical polarity, as the ions may be positively or negatively charged. Reversing the polarity of the electrodes does not alter the direction of motion, as it also reverses the polarity of the ions carrying charge. Thrust is produced in the same direction, either way. For positive corona,nitrogen ions are created initially, while for negative polarity, oxygen ions are the major primary ions. Both these types of ion immediately attract a variety of air molecules to create molecular cluster-ions[15] of either sign, which act ascharge carriers.

Current EHD thrusters are far less efficient than conventional engines.[16] An MIT researcher noted that ion thrusters have the potential to be far more efficient than conventional jet engines.[17]

Unlike pureion thruster rockets, theelectrohydrodynamic principle does not apply in the vacuum of space.[18]

Electrohydrodynamics

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Main article:Electrohydrodynamics

The thrust generated by an EHD device is an example of theBiefeld–Brown effect and can be derived through a modified use of theChild–Langmuir equation.[19]A generalized one-dimensional treatment gives the equation:F=Idk{\displaystyle F={\frac {Id}{k}}}where

  • F is the resulting force.
  • I is the electric current.
  • d is the air gap.
  • k is the ion mobility of the working fluid,[20] expressed in A⋅s2⋅kg−1 in SI units, but more commonly expressed with the unit m2⋅V−1⋅s−1. A typical value for air at surface pressure and temperature is1.5×10−4 m2⋅V−1⋅s−1).[20]

As applied to a gas such as air, the principle is also referred to as electroaerodynamics (EAD).

When the ionocraft is turned on, the corona wire becomes charged withhigh voltage, usually between 20 and 50kV. When the corona wire reaches approximately 30 kV, it causes the air molecules nearby to becomeionised by stripping theirelectrons from them. As this happens, the ions are repelled from the anode and attracted towards the collector, causing the majority of the ions to accelerate toward the collector. These ions travel at a constant average velocity termed thedrift velocity. Such velocity depends on themean free path between collisions, the strength of the external electric field, and the mass of ions and neutral air molecules.

The fact that the current is carried by acorona discharge (and not a tightly confinedarc) means that the moving particles diffuse into an expanding ion cloud, and collide frequently with neutral air molecules. It is these collisions that impart momentum to the neutral air molecules, which, because they are neutral, do not migrate back to the second electrode. Instead they continue to travel in the same direction, creating a neutral wind. As these neutral molecules are ejected from the ionocraft, there are, in agreement withNewton's third law of motion, equal and opposite forces, so the ionocraft moves in the opposite direction with an equal force. The force exerted is comparable to a gentle breeze. The resulting thrust depends on other external factors including air pressure and temperature, gas composition, voltage, humidity, and air gap distance.

The air mass in the gap between theelectrodes is impacted repeatedly by excited particles moving at high drift velocity. This creates electrical resistance, which must be overcome. The result of the neutral air caught in the process is to effectively cause an exchange in momentum and thus generate thrust. The heavier and denser the air, the higher the resulting thrust.

Aircraft configuration

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As with conventional reaction thrust, EAD thrust may be directed either horizontally to power afixed-wingairplane or vertically to support apowered lift craft, sometimes referred to as a "lifter".

Design

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Typical ionocraft construction

The thrust generating components of an ion propulsion system consist of three parts; a corona or emitter wire, an air gap and a collector wire or strip downstream from the emitter. A lightweight insulating frame supports the arrangement. The emitter and collector should be as close to each other as possible, i.e. with a narrow air gap, to achieve a saturated corona current condition that produces maximum thrust. However, if the emitter is too close to the collector it tends toarc across the gap.[citation needed]

Ion propulsion systems require many safety precautions due to the required high voltage.

Emitter

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The emitter wire is typically connected to the positive terminal of the high voltage power supply. In general, it is made from a small gauge bareconductivewire. Whilecopper wire can be used, it does not work as well asstainless steel. Similarly, thinner wire such as 44 or 50gauge tends to outperform more common, larger sizes such as 30 gauge, as the stronger electric field around the smaller diameter wire results in lower ionisation onset voltage and a larger corona current as described byPeek's law.[21]

The emitter is sometimes referred to as the "corona wire" because of its tendency to emit a purplecorona discharge glow while in use.[citation needed] This is simply a side effect of ionization.

Air gap

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The air gap insulates the two electrodes and allows the ions generated at the emitter to accelerate and transfer momentum to neutral air molecules, before losing their charge at the collector. The width of the air gap is typically 1 mm / kV.[22]

Collector

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The collector is shaped to provide a smooth equipotential surface underneath the corona wire. Variations of this include a wire mesh, parallel conductive tubes, or a foil skirt with a smooth, round edge. Sharp edges on the skirt degrade performance, as it generates ions of opposite polarity to those within the thrust mechanism.[citation needed]

See also

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References

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  1. ^Thompson, Clive (August 2003)."The Antigravity Underground".Wired Magazine.
  2. ^Tajmar, M. (2004). "Biefeld–Brown Effect: Misinterpretation of Corona Wind Phenomena".AIAA Journal.42 (2):315–318.Bibcode:2004AIAAJ..42..315T.doi:10.2514/1.9095.
  3. ^Lifter efficiency relation to ion velocity "J L Naudin’s Lifter-3 pulsed HV 1.13g/Watt"Archived 2014-08-08 at theWayback Machine
  4. ^U.S. patent 3,130,945, Filed Aug 31 1959, Published April 28, 1954.
  5. ^Major de Seversky's Ion-Propelled Aircraft. Vol. 122. Popular mechanics. August 1964. pp. 58–61.
  6. ^Greenemeier, Larry (7 July 2008)."The World's First Flying Saucer: Made Right Here on Earth".Scientific American.
  7. ^Roy, Subrata; Arnold, David; Lin, Jenshan; Schmidt, Tony; Lind, Rick; et al. (2011). Air Force Office of Scientific Research; University of Florida (eds.).Demonstration of a Wingless Electromagnetic Air Vehicle(PDF) (Report). Defense Technical Information Center.ASIN B01IKW9SES. AFRL-OSR-VA-TR-2012-0922.Archived(PDF) from the original on 17 May 2013.
  8. ^Borg, Xavier;"Full analysis & design solutions for EHD Thrusters at saturated corona current conditions",The General Science Journal (non-peer-review), 2004, Updated 2006.
  9. ^Granados, Victor H.; Pinheiro, Mario J.; Sa, Paulo A. (July 2016). "Electrostatic propulsion device for aerodynamics applications".Physics of Plasmas.23 (7): 073514.Bibcode:2016PhPl...23g3514G.doi:10.1063/1.4958815.
  10. ^ab"Ion-Powered Aircraft Invention".The Stardust-Startup Factory. 27 February 2019. Retrieved15 August 2019.The flying device originally lifted its power supply directly off of the ground with no moving parts in 2006.
  11. ^us 10119527 
  12. ^LLC, Electron Air."Electron Air LLC".Electron Air LLC. Retrieved21 February 2025.
  13. ^Video onYouTube
  14. ^Hern, Alex (21 November 2018)."First ever plane with no moving parts takes flight".the Guardian. Retrieved25 November 2018.
  15. ^Harrison, R. G. (2003)."Ion-aerosol-cloud processes in the lower atmosphere".Reviews of Geophysics.41 (3): 1012.Bibcode:2003RvGeo..41.1012H.doi:10.1029/2002rg000114.ISSN 8755-1209.S2CID 123305218.
  16. ^Chen, Angus."Silent and Simple Ion Engine Powers a Plane with No Moving Parts".Scientific American. Retrieved15 August 2019.
  17. ^"Ionic thrusters generate efficient propulsion in air".ScienceDaily. 3 April 2013. Retrieved14 March 2023.... In their experiments, they found that ionic wind produces 110 newtons of thrust per kilowatt, compared with a jet engine's 2 newtons per kilowatt ...
  18. ^"Ion Propulsion"(PDF). Archived fromthe original(PDF) on 15 May 2010.
  19. ^"Electrokinetic devices in air"(PDF). Retrieved25 April 2013.
  20. ^abTammet, H. (1998). "Reduction of air ion mobility to standard conditions".Journal of Geophysical Research: Atmospheres.103 (D12):13933–13937.Bibcode:1998JGR...10313933T.doi:10.1029/97JD01429.hdl:10062/50224.
  21. ^Peek, F.W. (1929).Dielectric Phenomena in High Voltage Engineering. McGraw-Hill.LCCN 30000280.
  22. ^Meesters, Koos; Terpstra, Wessel (2 December 2019)."ion drives and sustainability"(PDF). Retrieved3 December 2019.

Further reading

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External links

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Wikimedia Commons has media related toIon driven air thrusters.
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