Helium - 3 - wikipedia Helium - 3 This article is about the elemental isotope. For the record label, see Helium 3 ( record label ). Helium - 3 Helium - 3 Complete table of nuclides General Name, symbol Helium - 3, He - 3, He Neutrons Protons Nuclide data Natural abundance 0.000137 % ( % He on Earth ) Half - life stable Parent isotopes H ( beta decay of tritium ) Isotope mass 3.0160293 u Spin ​ ⁄ Helium - 3 ( He - 3, also written as He, see also helion ) is a light, non-radioactive isotope of helium with two protons and one neutron ( common helium having two protons and two neutrons ). Its hypothetical existence was first proposed in 1934 by the Australian nuclear physicist Mark Oliphant while he was working at the University of Cambridge Cavendish Laboratory. Oliphant had performed experiments in which fast deuterons collided with deuteron targets ( incidentally, the first demonstration of nuclear fusion ). Helium - 3 was thought to be a radioactive isotope until it was also found in samples of natural helium, which is mostly helium - 4, taken both from the terrestrial atmosphere and from natural gas wells. Other than protium, helium - 3 is the only stable isotope of any element with more protons than neutrons. Helium - 3 occurs as a primordial nuclide, escaping from the Earth 's crust into the atmosphere and into outer space over millions of years. Helium - 3 is also thought to be a natural nucleogenic and cosmogenic nuclide, one produced when lithium is bombarded by natural neutrons, which can be released by spontaneous fission and by nuclear reactions with cosmic rays. Some of the helium - 3 found in the terrestrial atmosphere is also a relic of atmospheric and underwater nuclear weapons testing. Much speculation has been made over the possibility of helium - 3 as a future energy source. Unlike most other nuclear fusion reactions, the fusion of helium - 3 atoms releases large amounts of energy without causing the surrounding material to become radioactive. However, the temperatures required to achieve helium - 3 fusion reactions are much higher than in traditional fusion reactions. The abundance of helium - 3 is thought to be greater on the Moon than on Earth, having been embedded in the upper layer of regolith by the solar wind over billions of years, though still lower in abundance than in the solar system 's gas giants. Contents 1 Physical properties 2 Fusion reactions 3 Neutron detection 4 Cryogenics 5 Medical lung imaging 6 Industrial production 7 Natural abundance 7.1 Solar nebula ( primordial ) abundance 7.2 Terrestrial abundance 8 Extraction from extraterrestrial sources 9 Power generation 10 Notes and references 10.1 Bibliography 11 External links Physical properties Because of its low atomic mass of 3.02 atomic mass units, helium - 3 has some physical properties different from those of helium - 4, with a mass of 4.00 atomic mass units. Because of the weak, induced dipole -- dipole interaction between the helium atoms, their microscopic physical properties are mainly determined by their zero - point energy. Also, the microscopic properties of helium - 3 cause it to have a higher zero - point energy than helium - 4. This implies that helium - 3 can overcome dipole -- dipole interactions with less thermal energy than helium - 4 can. The quantum mechanical effects on helium - 3 and helium - 4 are significantly different because with two protons, two neutrons, and two electrons, helium - 4 has an overall spin of zero, making it a boson, but with one fewer neutron, helium - 3 has an overall spin of one half, making it a fermion. Helium - 3 boils at 3.19 K compared with helium - 4 at 4.23 K, and its critical point is also lower at 3.35 K, compared with helium - 4 at 5.2 K. Helium - 3 has less than half the density of Helium - 4 when it is at its boiling point : 59 gram per liter compared to the 125 gram per liter of helium - 4 -- at a pressure of one atmosphere. Its latent heat of vaporization is also considerably lower at 0.026 kilojoules per mole compared with the 0.0829 kilojoules per mole of helium - 4. Fusion reactions Comparison of neutronicity of reactions Reactants Products Q n / MeV First - generation fusion fuels H + H ( D-D ) → He + n 3.268 MeV 0.306 H + H ( D-D ) → H + p 4.032 MeV 0 H + H ( D-T ) → He + n 17.571 MeV 0.057 Second - generation fusion fuel H + He ( D - He ) → He + p 18.354 MeV 0 Third - generation fusion fuels He + He → He + 2 p 12.86 MeV 0 B + p → 3 He 8.68 MeV 0 Net result of D burning ( sum of first 4 rows ) 6D → 2 ( He + n + p ) 43.225 MeV 0.046 Current nuclear fuel U + n → 2 FP + 2.5 n ~ 200 MeV 0.001 He can be produced by the low temperature fusion of H + p ( D-p ) → He + γ + 4.98 MeV. If the fusion temperature is below that for the helium nuclei to fuse, the reaction produces a high energy alpha particle which quickly acquires an electron producing a stable light helium ion which can be utilized directly as a source of electricity without producing dangerous neutrons. The fusion reaction rate increases rapidly with temperature until it maximizes and then gradually drops off. The DT rate peaks at a lower temperature ( about 70 keV, or 800 million kelvins ) and at a higher value than other reactions commonly considered for fusion energy. He can be used in fusion reactions by either of the reactions H + He → He + p + 18.3 MeV, or He + He → He + 2 p+ 12.86 MeV. The conventional deuterium + tritium ( `` D-T '' ) fusion process produces energetic neutrons which render reactor components radioactive with activation products. The appeal of helium - 3 fusion stems from the aneutronic nature of its reaction products. Helium - 3 itself is non-radioactive. The lone high - energy by - product, the proton, can be contained using electric and magnetic fields. The momentum energy of this proton ( created in the fusion process ) will interact with the containing electromagnetic field, resulting in direct net electricity generation. Because of the higher Coulomb barrier, the temperatures required for H + He fusion are much higher than those of conventional D-T fusion. Moreover, since both reactants need to be mixed together to fuse, reactions between nuclei of the same reactant will occur, and the D-D reaction ( H + H ) does produce a neutron. Reaction rates vary with temperature, but the D - He reaction rate is never greater than 3.56 times the D-D reaction rate ( see graph ). Therefore, fusion using D - 3He fuel at the right temperature and a D - lean fuel mixture, can produce a much lower neutron flux than D-T fusion, but is not clean, negating some of its main attraction. The second possibility, fusing He with itself ( He + He ), requires even higher temperatures ( since now both reactants have a + 2 charge ), and thus is even more difficult than the D - He reaction. However, it does offer a possible reaction that produces no neutrons ; the charged protons produced can be contained using electric and magnetic fields, which in turn results in direct electricity generation. He + He fusion is feasible as demonstrated in the laboratory and has immense advantages, but commercial viability is many years in the future. The amounts of helium - 3 needed as a replacement for conventional fuels are substantial by comparison to amounts currently available. The total amount of energy produced in the H + He reaction is 18.4 M eV, which corresponds to some 493 megawatt - hours ( 4.93 × 10 W h ) per three grams ( one mole ) of 3He. If the total amount of energy could be converted to electrical power with 100 % efficiency ( a physical impossibility ), it would correspond to about 30 minutes of output of a gigawatt electrical plant per mole of He. Thus, a year 's production ( at 6 grams for each operation hour ) would require 52.5 kilograms of helium - 3. The amount of fuel needed for large - scale applications can also be put in terms of total consumption : electricity consumption by 107 million U.S. households in 2001 totaled 1,140 billion kW h ( 1.14 × 10 W h ). Again assuming 100 % conversion efficiency, 6.7 tonnes per year of helium - 3 would be required for that segment of the energy demand of the United States, 15 to 20 tonnes per year given a more realistic end - to - end conversion efficiency. Neutron detection Helium - 3 is a most important isotope in instrumentation for neutron detection. It has a high absorption cross section for thermal neutron beams and is used as a converter gas in neutron detectors. The neutron is converted through the nuclear reaction n + He → H + H + 0.764 MeV into charged particles tritium ( T, H ) and protium ( p, H ) which then are detected by creating a charge cloud in the stopping gas of a proportional counter or a Geiger - Müller tube. Furthermore, the absorption process is strongly spin - dependent, which allows a spin - polarized helium - 3 volume to transmit neutrons with one spin component while absorbing the other. This effect is employed in neutron polarization analysis, a technique which probes for magnetic properties of matter. The United States Department of Homeland Security had hoped to deploy detectors to spot smuggled plutonium in shipping containers by their neutron emissions, but the worldwide shortage of helium - 3 following the drawdown in nuclear weapons production since the Cold War has to some extent prevented this. As of 2012, DHS determined the commercial supply of boron - 10 would support converting its neutron detection infrastructure to that technology. Cryogenics A helium - 3 refrigerator uses helium - 3 to achieve temperatures of 0.2 to 0.3 kelvin. A dilution refrigerator uses a mixture of helium - 3 and helium - 4 to reach cryogenic temperatures as low as a few thousandths of a kelvin. An important property of helium - 3, which distinguishes it from the more common helium - 4, is that its nucleus is a fermion since it contains an odd number of spin ​ ⁄ particles. Helium - 4 nuclei are bosons, containing an even number of spin ​ ⁄ particles. This is a direct result of the addition rules for quantized angular momentum. At low temperatures ( about 2.17 K ), helium - 4 undergoes a phase transition : A fraction of it enters a superfluid phase that can be roughly understood as a type of Bose -- Einstein condensate. Such a mechanism is not available for helium - 3 atoms, which are fermions. However, it was widely speculated that helium - 3 could also become a superfluid at much lower temperatures, if the atoms formed into pairs analogous to Cooper pairs in the BCS theory of superconductivity. Each Cooper pair, having integer spin, can be thought of as a boson. During the 1970s, David Lee, Douglas Osheroff and Robert Coleman Richardson discovered two phase transitions along the melting curve, which were soon realized to be the two superfluid phases of helium - 3. The transition to a superfluid occurs at 2.491 millikelvins on the melting curve. They were awarded the 1996 Nobel Prize in Physics for their discovery. Tony Leggett won the 2003 Nobel Prize in Physics for his work on refining understanding of the superfluid phase of helium - 3. In a zero magnetic field, there are two distinct superfluid phases of He, the A-phase and the B - phase. The B - phase is the low - temperature, low - pressure phase which has an isotropic energy gap. The A-phase is the higher temperature, higher pressure phase that is further stabilized by a magnetic field and has two point nodes in its gap. The presence of two phases is a clear indication that He is an unconventional superfluid ( superconductor ), since the presence of two phases requires an additional symmetry, other than gauge symmetry, to be broken. In fact, it is a p - wave superfluid, with spin one, S = 1, and angular momentum one, L = 1. The ground state corresponds to total angular momentum zero, J = S+L = 0 ( vector addition ). Excited states are possible with non-zero total angular momentum, J > 0, which are excited pair collective modes. Because of the extreme purity of superfluid He ( since all materials except He have solidified and sunk to the bottom of the liquid He and any He has phase separated entirely, this is the most pure condensed matter state ), these collective modes have been studied with much greater precision than in any other unconventional pairing system. Medical Lung Imaging Helium - 3 nuclei have an intrinsic nuclear spin of ​ ⁄, and a relatively high magnetogyric ratio. Helium - 3 can be hyperpolarized using non-equilibrium means such as spin - exchange optical pumping. During this process, circularly polarized infrared laser light, tuned to the appropriate wavelength, is used to excite electrons in an alkali metal, such as caesium or rubidium inside a sealed glass vessel. The angular momentum is transferred from the alkali metal electrons to the noble gas nuclei through collisions. In essence, this process effectively aligns the nuclear spins with the magnetic field in order to enhance the NMR signal. The hyperpolarized gas may then be stored at pressures of 10 atm, for up to 100 hours. Following inhalation, gas mixtures containing the hyperpolarized helium - 3 gas can be imaged with an MRI scanner to produce anatomical and functional images of lung ventilation. This technique is also able to produce images of the airway tree, locate unventilated defects, measure the alveolar oxygen partial pressure, and measure the ventilation / perfusion ratio. This technique may be critical for the diagnosis and treatment management of chronic respiratory diseases such as chronic obstructive pulmonary disease ( COPD ), emphysema, cystic fibrosis, and asthma. Industrial production Production, sales and distribution of helium - 3 in the United States are managed by the US Department of Energy ( DOE ) Isotope Program. Virtually all helium - 3 used in industry today is produced from the radioactive decay of tritium. Tritium is a radioactive isotope of hydrogen and is typically produced by bombarding lithium - 6 with neutrons in a nuclear reactor. The lithium nucleus absorbs a neutron and splits into helium - 4 and tritium. Tritium decays into helium - 3 with a half - life of 12.3 years, so helium - 3 can be produced by simply storing the tritium until it undergoes radioactive decay. Tritium is a critical component of nuclear weapons and historically it was produced and stockpiled primarily for this application. The decay of tritium into helium - 3 reduces the explosive power of the fusion warhead, so periodically the accumulated helium - 3 must be removed from warhead reservoirs and tritium in storage. Helium - 3 removed during this process is marketed for other applications. For decades this has been, and remains, the principal source of the world 's helium - 3. However, since the signing of the START I Treaty in 1991 the number of nuclear warheads that are kept ready for use has decreased This has reduced the quantity of helium - 3 available from this source. Helium - 3 stockpiles have been further diminished by increased demand, primarily for use in neutron radiation detectors and medical diagnostic procedures. US industrial demand for helium - 3 reached a peak of 70,000 liters ( approximately 8 kg ) per year in 2008. Price at auction, historically about $100 / liter, reached as high as $2000 / liter Since then, demand for helium - 3 has declined to about 6000 liters per year due to the high cost and efforts by the DOE to recycle it and find substitutes. The DOE recognized the developing shortage of both tritium and helium - 3. and began producing tritium by lithium irradiation at the Tennessee Valley Authority 's Watts Bar Nuclear Generating Station in 2010. In this process tritium - producing burnable absorber rods ( TPBARs ) containing lithium in a ceramic form are inserted into the reactor in place of the normal boron control rods Periodically the TPBARs are replaced and the tritium extracted. Currently only one reactor is used for tritium production but the process could, if necessary, be vastly scaled up to meet any conceivable demand simply by utilizing more of the nation 's power reactors. Substantial quantities of tritium and helium - 3 could also be extracted from the heavy water moderator in CANDU nuclear reactors. Natural abundance Solar nebula ( primordial ) abundance One early estimate of the primordial ratio of He to He in the solar nebula has been the measurement of their ratio in the atmosphere of Jupiter, measured by the mass spectrometer of the Galileo atmospheric entry probe. This ratio is about 1 : 10,000, or 100 parts of He per million parts of He. This is roughly the same ratio of the isotopes in lunar regolith, when it contains 28 ppm helium - 4 and 2.8 ppb helium - 3 ( which is at the lower end of actual sample measurements, which vary from about 1.4 to 15 ppb ). However, terrestrial ratios of the isotopes are lower by a factor of 100, mainly due to enrichment of helium - 4 stocks in the mantle by billions of years of alpha decay from uranium and thorium. Terrestrial abundance Main article : isotope geochemistry He is a primordial substance in the Earth 's mantle, considered to have become entrapped within the Earth during planetary formation. The ratio of He to He within the Earth 's crust and mantle is less than that for assumptions of solar disk composition as obtained from meteorite and lunar samples, with terrestrial materials generally containing lower He / He ratios due to ingrowth of He from radioactive decay. He has a cosmological ratio of 300 atoms per million atoms of He ( at. ppm ), leading to the assumption that the original ratio of these primordial gases in the mantle was around 200 - 300 ppm when Earth was formed. A lot of He was generated by alpha - particle decay of uranium and thorium, and now the mantle has only around 7 % primordial helium, lowering the total He / He ratio to around 20 ppm. Ratios of He / He in excess of atmospheric are indicative of a contribution of He from the mantle. Crustal sources are dominated by the He which is produced by the decay of radioactive elements in the crust and mantle. The ratio of helium - 3 to helium - 4 in natural Earth - bound sources varies greatly. Samples of the lithium ore spodumene from Edison Mine, South Dakota were found to contain 12 parts of helium - 3 to a million parts of helium - 4. Samples from other mines showed 2 parts per million. Helium is also present as up to 7 % of some natural gas sources, and large sources have over 0.5 % ( above 0.2 % makes it viable to extract ). The fraction of He in helium separated from natural gas in the U.S. was found to range from 70 to 242 parts per billion. Hence the US 2002 stockpile of 1 billion normal m would have contained about 12 to 43 kilograms of helium - 3. According to one expert, about 26 m or almost 5 kg of He is available annually for separation from the US natural gas stream. If the process of separating out the He could employ as feedstock the liquefied helium typically used to transport and store bulk quantities, estimates for the incremental energy cost range from US $34 to $300 per liter NTP, excluding the cost of infrastructure and equipment. Algeria 's annual gas production is assumed to contain 100 million normal cubic metres and this would contain between 7 and 24 m of helium - 3 ( about 1 to 4 kilograms ) assuming a similar He fraction. He is also present in the Earth 's atmosphere. The natural abundance of He in naturally occurring helium gas is 1.38 × 10 ( 1.38 parts per million ). The partial pressure of helium in the Earth 's atmosphere is about 0.52 Pa, and thus helium accounts for 5.2 parts per million of the total pressure ( 101325 Pa ) in the Earth 's atmosphere, and He thus accounts for 7.2 parts per trillion of the atmosphere. Since the atmosphere of the Earth has a mass of about 5.14 × 10 tonnes, the mass of He in the Earth 's atmosphere is the product of these numbers, or about 37,000 tonnes of He. He is produced on Earth from three sources : lithium spallation, cosmic rays, and beta decay of tritium ( H ). The contribution from cosmic rays is negligible within all except the oldest regolith materials, and lithium spallation reactions are a lesser contributor than the production of He by alpha particle emissions. The total amount of helium - 3 in the mantle may be in the range of 0.1 -- 1 million tonnes. However, most of the mantle is not directly accessible. Some helium - 3 leaks up through deep - sourced hotspot volcanoes such as those of the Hawaiian Islands, but only 300 grams per year is emitted to the atmosphere. Mid-ocean ridges emit another 3 kilogram per year. Around subduction zones, various sources produce helium - 3 in natural gas deposits which possibly contain a thousand tonnes of helium - 3 ( although there may be 25 thousand tonnes if all ancient subduction zones have such deposits ). Wittenberg estimated that United States crustal natural gas sources may have only half a tonne total. Wittenberg cited Anderson 's estimate of another 1200 metric tonnes in interplanetary dust particles on the ocean floors. In the 1994 study, extracting helium - 3 from these sources consumes more energy than fusion would release. Extraction from extraterrestrial sources Materials on the Moon 's surface contain helium - 3 at concentrations between 1.4 and 15 ppb in sunlit areas, and may contain concentrations as much as 50 ppb in permanently shadowed regions. A number of people, starting with Gerald Kulcinski in 1986, have proposed to explore the moon, mine lunar regolith and use the helium - 3 for fusion. Because of the low concentrations of helium - 3, any mining equipment would need to process extremely large amounts of regolith ( over 150 million tonnes of regolith to obtain one ton of helium 3 ), and some proposals have suggested that helium - 3 extraction be piggybacked onto a larger mining and development operation. The primary objective of Indian Space Research Organisation 's first lunar probe called Chandrayaan - I, launched on October 22, 2008, was reported in some sources to be mapping the Moon 's surface for helium - 3 - containing minerals. However, no such objective is mentioned in the project 's official list of goals, although many of its scientific payloads have noted helium - 3 - related applications. Cosmochemist and geochemist Ouyang Ziyuan from the Chinese Academy of Sciences who is now in charge of the Chinese Lunar Exploration Program has already stated on many occasions that one of the main goals of the program would be the mining of helium - 3, from which operation `` each year, three space shuttle missions could bring enough fuel for all human beings across the world. '' To `` bring enough fuel for all human beings across the world '', more than one Space Shuttle load ( and the processing of 4 million tonnes of regolith ) per week, at least 52 per year, would be necessary. In January 2006, the Russian space company RKK Energiya announced that it considers lunar helium - 3 a potential economic resource to be mined by 2020, if funding can be found. Mining gas giants for helium - 3 has also been proposed. The British Interplanetary Society 's hypothetical Project Daedalus interstellar probe design was fueled by helium - 3 mines in the atmosphere of Jupiter, for example. Jupiter 's high gravity makes this a less energetically favorable operation than extracting helium - 3 from the other gas giants of the solar system, however. Not all authors feel the extraterrestrial extraction of helium - 3 is feasible. Dwayne Day, writing in The Space Review, identifies some major obstacles to helium - 3 extraction from extraterrestrial sources for use in fusion, and questions the feasibility of extraterrestrial extraction when compared to production on Earth. Several science fiction works have featured helium - 3 extraction on the moon, including the films Moon ( 2009 ) and Iron Sky ( 2012 ), the manga and corresponding anime Planetes, the video game Anno 2205 ( 2015 ) and the novel Luna : New Moon ( 2015 ). The novel Morning Star ( Pierce Brown, 2016 ) features helium - 3 mining on Phobos ( a moon of Mars ), while his novel Red Rising ( 2014 ) features helium - 3 extraction from Mars itself. Power generation This section contains weasel words : vague phrasing that often accompanies biased or unverifiable information. Such statements should be clarified or removed. ( March 2013 ) A second - generation approach to controlled fusion power involves combining helium - 3 ( He ) and deuterium ( H ). This reaction produces a helium - 4 ion ( He ) ( like an alpha particle, but of different origin ) and a high - energy proton ( positively charged hydrogen ion ) ( p ). The most important potential advantage of this fusion reaction for power production as well as other applications lies in its compatibility with the use of electrostatic fields to control fuel ions and the fusion protons. High speed protons, as positively charged particles, can have their kinetic energy converted directly into electricity, through use of solid - state conversion materials as well as other techniques. Potential conversion efficiencies of 70 % may be possible, as there is no need to convert proton energy to heat in order to drive a turbine - powered electrical generator. There have been many claims about the capabilities of helium - 3 power plants. According to proponents, fusion power plants operating on deuterium and helium - 3 would offer lower capital and operating costs than their competitors due to less technical complexity, higher conversion efficiency, smaller size, the absence of radioactive fuel, no air or water pollution, and only low - level radioactive waste disposal requirements. Recent estimates suggest that about $6 billion in investment capital will be required to develop and construct the first helium - 3 fusion power plant. Financial breakeven at today 's wholesale electricity prices ( 5 US cents per kilowatt - hour ) would occur after five 1 - gigawatt plants were on line, replacing old conventional plants or meeting new demand. The reality is not so clear - cut. The most advanced fusion programs in the world are inertial confinement fusion ( such as National Ignition Facility ) and magnetic confinement fusion ( such as ITER and Wendelstein 7 - X ). In the case of the former, there is no solid roadmap to power generation. In the case of the latter, commercial power generation is not expected until around 2050. In both cases, the type of fusion discussed is the simplest : D-T fusion. The reason for this is the very low Coulomb barrier for this reaction ; for D+ He, the barrier is much higher, and it is even higher for He -- He. The immense cost of reactors like ITER and National Ignition Facility are largely due to their immense size, yet to scale up to higher plasma temperatures would require reactors far larger still. The 14.7 MeV proton and 3.6 MeV alpha particle from D -- He fusion, plus the higher conversion efficiency, means that more electricity is obtained per kilogram than with D-T fusion ( 17.6 MeV ), but not that much more. As a further downside, the rates of reaction for helium - 3 fusion reactions are not particularly high, requiring a reactor that is larger still or more reactors to produce the same amount of electricity. To attempt to work around this problem of massively large power plants that may not even be economical with D-T fusion, let alone the far more challenging D -- He fusion, a number of other reactors have been proposed -- the Fusor, Polywell, Focus fusion, and many more, though many of these concepts have fundamental problems with achieving a net energy gain, and generally attempt to achieve fusion in thermal disequilibrium, something that could potentially prove impossible, and consequently, these long - shot programs tend to have trouble garnering funding despite their low budgets. 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Helium Isotopic Abundance Variation in Nature. copy of paper BNL - 49331 `` Table II. 3He Abundance of Natural Gas... 3He in ppm... Aldrich 0.05 -- 0.5... Sano 0.46 -- 22.7 '', `` Table V... of Water... 3He in ppm... 1.6 -- 1.8 East Pacific... 0.006 -- 1.5 Manitoba Chalk River... 164 Japan Sea '' ( Aldrich measured Helium from US wells, Sano that of Taiwan gas ( 1 ) ) Jump up ^ WebElements Periodic Table : Professional Edition : Helium : key information. Webelements.com. Retrieved on 2011 - 11 - 08. ^ Jump up to : Smith, D.M. `` any concentration of helium above approximately 0.2 percent is considered worthwhile examining ''... `` U.S. government still owns approximately 1 billion nm of helium inventory '', `` Middle East and North Africa... many very large, helium - rich ( up to 0.5 percent ) natural gas fields '' ( Smith uses nm to mean `` normal cubic metre '', elsewhere called `` cubic metre at NTP ) Jump up ^ Davidson, Thomas A. ; Emerson, David E. ( 1990 ). Method and Apparatus for Direct Determination of Helium - 3 in Natural Gas and Helium ( Report ). Bureau of Mines, US Department of the Interior. Report of Investigations 9302. Jump up ^ The Mass of the Atmosphere : A Constraint on Global Analyses. Ams.allenpress.com ( 1970 - 01 - 01 ). Retrieved on 2011 - 11 - 08. Jump up ^ Wittenberg 1994 p. 3, Table 1 ; p. 9. Jump up ^ Wittenberg 1994 Page A-1 citing Anderson 1993, `` 1200 metric tone '' Jump up ^ Wittenberg 1994 Page A-4 `` 1 kg ( 3He ), pumping power would be 1.13 × 10 MYyr... fusion power derived... 19 MWyr '' Jump up ^ FTI Research Projects : : 3He Lunar Mining. Fti.neep.wisc.edu. Retrieved on 2011 - 11 - 08. Jump up ^ E.N. Slyuta ; A.M. Abdrakhimov ; E.M. Galimov ( 2007 ). `` The estimation of helium - 3 probable reserves in lunar regolith '' ( PDF ). Lunar and Planetary Science XXXVIII. Jump up ^ Eric R. Hedman ( January 16, 2006 ). `` A fascinating hour with Gerald Kulcinski ''. The Space Review. Jump up ^ I.N. Sviatoslavsky ( November 1993 ). `` The challenge of mining He - 3 on the lunar surface : how all the parts fit together '' ( PDF ). Wisconsin Center for Space Automation and Robotics Technical Report WCSAR - TR - AR3 - 9311 - 2. Jump up ^ `` With He - 3 on mind, India gets ready for lunar mission ''. The Times Of India. 2008 - 09 - 19. Jump up ^ Scientific Archived 2009 - 10 - 12 at the Wayback Machine... Isro.org ( 2008 - 11 - 11 ). Retrieved on 2011 - 11 - 08. Jump up ^ Luna C / I : : Chandrayaan - 1 Payload Feature # 2 : Sub KeV Atom Reflecting Analyser ( SARA ). Luna-ci.blogspot.com ( 2008 - 11 - 12 ). Retrieved on 2011 - 11 - 08. Jump up ^ He asked for the moon - and got it. Chinadaily.com.cn ( 2006 - 07 - 26 ). Retrieved on 2011 - 11 - 08. Jump up ^ Wittenberg 1994 Jump up ^ Russian Rocket Builder Aims for Moon Base by 2015, Reports Say. Associated Press ( via space.com ). 26 January 2006 Jump up ^ James Oberg ( February 6, 2006 ). `` Moonscam : Russians try to sell the Moon for foreign cash ''. Jump up ^ Dwayne A. Day ( March 5, 2007 ). `` Death throes and grand delusions ''. The Space Review. Jump up ^ Bryan Palaszewski. `` Atmospheric Mining in the Outer Solar System '' ( PDF ). Archived from the original ( PDF ) on 2009 - 03 - 27. NASA Technical Memorandum 2006 - 214122. AIAA -- 2005 -- 4319. Prepared for the 41st Joint Propulsion Conference and Exhibit cosponsored by AIAA, ASME, SAE, and ASEE, Tucson, Arizona, July 10 -- 13, 2005. Jump up ^ ( 2 ) The Helium - 3 Incantation Jump up ^ Paul DiMare ( October 2004 ). `` Mining The Moon ''. Retrieved 2007 - 05 - 06. Jump up ^ `` ITER & Beyond ''. Archived from the original on 2009 - 05 - 20. Retrieved 2009 - 08 - 04. Jump up ^ Todd Rider. `` A general critique of inertial - electrostatic confinement fusion systems ''. Retrieved 2007 - 05 - 07. Bibliography D.M. Smith, T.W. Goodwin, J.A. Schiller ( 26 September 2003 ). `` Challenges to the worldwide supply of helium in the next decade '' ( PDF ). Anchorage, Alaska : Air Products and Chemicals. Bibcode : 2004AIPC... 710... 119S. doi : 10.1063 / 1.1774674. Retrieved 2015 - 03 - 08. CS1 maint : Multiple names : authors list ( link ) L.J. Wittenberg ( July 1994 ). `` Non-Lunar He Resources '' ( PDF ). Retrieved 2008 - 07 - 01. H.H. Schmitt ( 2005 ). Return to the Moon : Exploration, Enterprise, and Energy in the Human Settlement of Space. Springer. ISBN 0 - 387 - 24285 - 6. J. Wilks ( 1967 ). The properties of liquid and solid helium. Oxford University Press. External links The Nobel Prize in Physics 2003, presentation speech Moon for Sale : A BBC Horizon documentary on the possibility of lunar mining of Helium - 3 Lighter : diproton Helium - 3 is an isotope of helium Heavier : helium - 4 Decay product of : lithium - 4 ( p ) hydrogen - 3 ( β − ) Decay chain of helium - 3 Decays to : Stable GND : 4159517 - 8 Retrieved from `` https://en.wikipedia.org/w/index.php?title=Helium-3&oldid=840022983 '' Categories : Isotopes of helium Nuclear fusion fuels Hidden categories : CS1 maint : Uses authors parameter Webarchive template wayback links All articles with unsourced statements Articles with unsourced statements from January 2011 Articles with unsourced statements from August 2007 All accuracy disputes Articles with disputed statements from July 2014 Articles with weasel words from March 2013 Articles with unsourced statements from April 2012 CS1 maint : Multiple names : authors list Wikipedia articles with GND identifiers Talk Contents About Wikipedia Български Català Čeština Deutsch Eesti Español فارسی Français 한국어 हिन्दी Bahasa Indonesia Interlingua Italiano עברית Latviešu Bahasa Melayu Nederlands 日本 語 Norsk Português Русский Suomi Svenska Türkçe Українська 中文 18 more Edit links This page was last edited on 7 May 2018, at 06 : 56. 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Question: where is helium 3 found on the moon
Answer: embedded in the upper layer of regolith