View source for Helium

{{About|the chemical element}}
{{Redirect|2He|the isotope of helium with two nucleons ({{chem2|^{2}He}})|Helium-2}}
{{pp-semi-indef|small=yes}}
{{Infobox helium}}
'''Helium''' (from {{langx|grc|ἥλιος|[[helios]]|lit=sun}}) is a [[chemical element]]; it has [[chemical symbol|symbol]] '''He''' and [[atomic number]] 2. It is a colorless, odorless, non-toxic, [[inert gas|inert]], [[monatomic]] [[gas]] and the first in the [[noble gas]] group in the [[periodic table]].{{efn|A few authors dispute the placement of helium in the noble gas column, preferring to place it above [[beryllium]] with the [[alkaline earth metal]]s. They do so on the grounds of helium's 1s<sup>2</sup> electron configuration, which is analogous to the ns<sup>2</sup> valence configurations of the alkaline earth metals, and furthermore point to some specific trends that are more regular if helium is placed in group 2.<ref>{{cite journal |last1=Grochala |first1=Wojciech |date=1 November 2017 |title=On the position of helium and neon in the Periodic Table of Elements |journal=Foundations of Chemistry |volume=20 |pages=191–207 |issue=2018 |doi=10.1007/s10698-017-9302-7 |doi-access=free }}</ref><ref>{{cite journal |last1=Bent Weberg |first1=Libby |date=18 January 2019 |title="The" periodic table |url=https://cen.acs.org/articles/97/i3/Reactions.html |journal=Chemical & Engineering News |volume=97 |issue=3 |access-date=27 March 2020}}</ref><ref>{{cite journal |last1=Grandinetti |first1=Felice |date=23 April 2013 |title=Neon behind the signs |journal=Nature Chemistry |volume=5 |issue=2013 |pages=438 |doi=10.1038/nchem.1631 |pmid=23609097 |bibcode=2013NatCh...5..438G |doi-access=free }}</ref><ref>{{cite journal |last1=Kurushkin |first1=Mikhail |date=2020 |title=Helium's placement in the Periodic Table from a crystal structure viewpoint |url=https://www.researchgate.net/publication/342152661 |journal=IUCrJ |volume=7 |issue=4 |pages=577–578 |doi=10.1107/S2052252520007769 |pmid=32695406 |pmc=7340260 |access-date=19 June 2020|doi-access=free |bibcode=2020IUCrJ...7..577K }}</ref><ref>{{cite journal |last1=Labarca |first1=Martín |last2=Srivaths |first2=Akash |date=2016 |title=On the Placement of Hydrogen and Helium in the Periodic System: A New Approach |url=https://www.academia.edu/27974090 |journal=Bulgarian Journal of Science Education |volume=25 |issue=4 |pages=514–530 |access-date=19 June 2020 |archive-date=29 November 2021 |archive-url=https://web.archive.org/web/20211129140234/https://www.academia.edu/27974090 |url-status=dead }}</ref> These tend to relate to [[kainosymmetry]] and the first-row anomaly: the first orbital of any type is unusually small, since unlike its higher analogues, it does not experience interelectronic repulsion from a smaller orbital of the same type. Because of this trend in the sizes of orbitals, a large difference in atomic radii between the first and second members of each main group is seen in groups 1 and 13–17: it exists between neon and argon, and between helium and beryllium, but not between helium and neon. This similarly affects the noble gases' boiling points and solubilities in water, where helium is too close to neon, and the large difference characteristic between the first two elements of a group appears only between neon and argon. Moving helium to group 2 makes this trend consistent in groups 2 and 18 as well, by making helium the first group 2 element and neon the first group 18 element: both exhibit the characteristic properties of a kainosymmetric first element of a group.<ref>{{cite book|title=Concise Chemistry of the Elements|year=2002|publisher=Horwood|isbn=978-1-898563-71-6|last1=Siekierski|first1=S.|last2=Burgess|first2 =J. |pages=23–26}}</ref> However, the classification of helium with the other noble gases remains near-universal, as its extraordinary inertness is extremely close to that of the other light noble gases neon and argon.<ref>{{Cite book|title = Modeling Marvels: Computational Anticipation of Novel Molecules|url = https://books.google.com/books?id=IoFzgBSSCwEC|publisher = Springer Science & Business Media|date = 5 December 2008|isbn = 978-1-4020-6973-4|first = Errol G.|last = Lewars|pages = 69–71|url-status=live|archive-url = https://web.archive.org/web/20160519021952/https://books.google.com/books?id=IoFzgBSSCwEC|archive-date = 19 May 2016|df = dmy-all}}</ref>}} Its [[boiling point]] is the lowest among all the [[Chemical element|elements]], and it does not have a [[melting point]] at standard pressures. It is the second-lightest and second-most [[Abundance of the chemical elements|abundant element]] in the observable [[universe]], after [[hydrogen]]. It is present at about 24% of the total elemental mass, which is more than 12 times the mass of all the heavier elements combined. Its abundance is similar to this in both the [[Sun]] and [[Jupiter]], because of the very high [[nuclear binding energy]] (per [[nucleon]]) of [[helium-4]] with respect to the next three elements after helium. This helium-4 binding energy also accounts for why it is a product of both [[nuclear fusion]] and [[radioactive decay]]. The most common isotope of helium in the universe is helium-4, the vast majority of which was formed during the [[Big Bang]]. Large amounts of new helium are created by nuclear fusion of hydrogen in [[stars]].

Helium was first detected as an unknown, yellow [[spectral line]] signature in sunlight during a [[Solar eclipse of August 18, 1868|solar eclipse in 1868]] by [[Georges Rayet]],<ref>Rayet, G. (1868) [https://web.archive.org/web/20180817142616/https://babel.hathitrust.org/cgi/pt?id=umn.31951d000083928;view=1up;seq=763 "Analyse spectral des protubérances observées, pendant l'éclipse totale de Soleil visible le 18 août 1868, à la presqu'île de Malacca"] (Spectral analysis of the protuberances observed during the total solar eclipse, seen on 18 August 1868, from the Malacca peninsula), ''Comptes rendus'' ... , '''67''' : 757–759. From p. 758: ''" ... je vis immédiatement une série de neuf lignes brillantes qui ... me semblent devoir être assimilées aux lignes principales du spectre solaire, B, D, E, b, une ligne inconnue, F, et deux lignes du groupe G."'' ( ... I saw immediately a series of nine bright lines that ... seemed to me should be classed as the principal lines of the solar spectrum, B, D, E, b, an unknown line, F, and two lines of the group G.)</ref> Captain C. T. Haig,<ref>Captain C. T. Haig (1868) [https://books.google.com/books?id=glFJAAAAcAAJ&pg=PA74 "Account of spectroscopic observations of the eclipse of the sun, August 18th, 1868"] ''Proceedings of the Royal Society of London'', '''17''' : 74–80. From p. 74: "I may state at once that I observed the spectra of two red flames close to each other, and in their spectra two broad bright bands quite sharply defined, one rose-madder and the other light golden."</ref> [[N. R. Pogson|Norman R. Pogson]],<ref>Pogson filed his observations of the 1868 eclipse with the local Indian government, but his report wasn't published. ([[Biman B. Nath]], ''The Story of Helium and the Birth of Astrophysics'' (New York, New York: Springer, 2013), [https://books.google.com/books?id=Zko_Na5IQL8C&pg=PA8 p. 8.]) Nevertheless, Lockyer quoted from his report. [https://babel.hathitrust.org/cgi/pt?id=mdp.39015038750884;view=1up;seq=360;size=150 From p. 320] {{Webarchive|url=https://web.archive.org/web/20180817113022/https://babel.hathitrust.org/cgi/pt?id=mdp.39015038750884;view=1up;seq=360;size=150|date=17 August 2018}} of Lockyer, J. Norman (1896) "The story of helium. Prologue," ''Nature'', '''53''' : 319–322 : "Pogson, in referring to the eclipse of 1868, said that the yellow line was "at D, or near D." "</ref> and Lieutenant John Herschel,<ref>Lieutenant John Herschel (1868) [https://books.google.com/books?id=glFJAAAAcAAJ&pg=PA104 "Account of the solar eclipse of 1868, as seen at Jamkandi in the Bombay Presidency,"] ''Proceedings of the Royal Society of London'', '''17''' : 104–120. From p. 113: As the moment of the total solar eclipse approached, " ... I recorded an increasing brilliancy in the spectrum in the neighborhood of D, so great in fact as to prevent any measurement of that line till an opportune cloud moderated the light. I am not prepared to offer any explanation of this." From p. 117: "I also consider that there can be no question that the ORANGE LINE was identical with D, so far as the capacity of the instrument to establish any such identity is concerned."</ref> and was subsequently confirmed by French astronomer [[Pierre Janssen|Jules Janssen]].<ref>In his initial report to the French Academy of Sciences about the 1868 eclipse, Janssen made no mention of a yellow line in the solar spectrum. See:
* Janssen (1868) [https://books.google.com/books?id=hpZDAQAAIAAJ&pg=PA838 "Indication de quelques-uns des résultats obtenus à Cocanada, pendant l'éclipse du mois d'août dernier, et à la suite de cette éclipse"] (Information on some of the results obtained at Cocanada, during the eclipse of the month of last August, and following that eclipse), ''Comptes rendus'' ... , '''67''' : 838–839.
* Wheeler M. Sears, ''Helium: The Disappearing Element'' (Heidelberg, Germany: Springer, 2015), [https://books.google.com/books?id=5SvABgAAQBAJ&pg=PA44 p. 44.]
* Françoise Launay with Storm Dunlop, trans., ''The Astronomer Jules Janssen: A Globetrotter of Celestial Physics'' (Heidelberg, Germany: Springer, 2012), [https://books.google.com/books?id=3YaAup49nqoC&pg=PA45 p. 45.]
However, subsequently, in an unpublished letter of 19 December 1868 to Charles Sainte-Claire Deville, Janssen asked Deville to inform the French Academy of Sciences that : "Several observers have claimed the bright D line as forming part of the spectrum of the prominences on 18 August. The bright yellow line did indeed lie very close to D, but the light was more refrangible [i.e., of shorter wavelength] than those of the D lines. My subsequent studies of the Sun have shown the accuracy of what I state here." (See: (Launay, 2012), p. 45.)</ref> Janssen is often jointly credited with detecting the element, along with [[Norman Lockyer]]. Janssen recorded the helium spectral line during the solar eclipse of 1868, while Lockyer observed it from Britain. However, only Lockyer proposed that the line was due to a new element, which he named after the Sun. The formal [[discovery of the chemical elements|discovery of the element]] was made in [[1895]] by chemists [[Sir William Ramsay]], [[Per Teodor Cleve]], and [[Nils Abraham Langlet]], who found helium emanating from the [[uranium]] ore [[cleveite]], which is now not regarded as a separate mineral species, but as a variety of [[uraninite]].<ref name="mindat cleveite">{{cite web |url=https://www.mindat.org/min-29957.html |title=Cleveite |website=Mindat.org |access-date=14 February 2020}}</ref><ref name="mindat uraninite">{{cite web |url=https://www.mindat.org/min-4102.html |title=Uraninite |website=Mindat.org |access-date=14 February 2020}}</ref> In 1903, large reserves of helium were found in [[natural gas field]]s in parts of the United States, by far the largest supplier of the gas today.

Liquid helium is used in [[Helium cryogenics|cryogenics]] (its largest single use, consuming about a quarter of production), and in the [[Cryocooler|cooling]] of [[superconducting magnet]]s, with its main commercial application in [[MRI]] scanners. Helium's other industrial uses—as a pressurizing and purge gas, as a protective atmosphere for [[arc welding]], and in processes such as growing [[crystal]]s to make [[silicon wafer]]s—account for half of the gas produced. A small but well-known use is as a [[lifting gas]] in [[balloon]]s and [[airship]]s.<ref>{{cite web |url=http://www.photonics.com/Article.aspx?AID=35225 |title=Helium: Up, Up and Away? |first=Melinda |last=Rose |website=Photonics Spectra |date=October 2008 |access-date=27 February 2010 |archive-url=https://web.archive.org/web/20100822172353/http://www.photonics.com/Article.aspx?AID=35225 |archive-date=22 August 2010 |url-status=live }} For a more authoritative but older 1996 pie chart showing U.S. helium use by sector, showing much the same result, see the chart reproduced in "Applications" section of this article.</ref> As with any gas whose density differs from that of air, inhaling a small volume of helium temporarily changes the timbre and quality of the [[human voice]]. In scientific research, the behavior of the two fluid phases of helium-4 (helium&nbsp;I and helium&nbsp;II) is important to researchers studying [[quantum mechanics]] (in particular the property of [[superfluidity]]) and to those looking at the phenomena, such as [[superconductivity]], produced in [[matter]] near [[absolute zero]].

On Earth, it is relatively rare—5.2 [[parts per million|ppm]] by volume in the [[atmosphere]]. Most terrestrial helium present today is created by the natural [[radioactive decay]] of heavy radioactive elements ([[thorium]] and uranium, although there are other examples), as the [[alpha particle]]s emitted by such decays consist of helium-4 [[atomic nucleus|nuclei]]. This [[radiogenic]] helium is trapped with [[natural gas]] in concentrations as great as 7% by volume, from which it is extracted commercially by a low-temperature separation process called [[fractional distillation]]. Terrestrial helium is a non-renewable resource because once released into the atmosphere, it promptly [[Atmospheric escape|escapes into space]]. Its supply is thought to be rapidly diminishing.<ref name="Connor">{{cite news |last=Connor |first=Steve |url=https://www.independent.co.uk/news/science/why-the-world-is-running-out-of-helium-2059357.html |title=Why the world is running out of helium |work=The Independent |date=23 August 2010 |access-date=16 September 2013 |location=London |archive-url=https://web.archive.org/web/20130927231657/http://www.independent.co.uk/news/science/why-the-world-is-running-out-of-helium-2059357.html |archive-date=27 September 2013 |url-status=live }}</ref><ref>{{cite web |author-link=Ethan Siegel |first=Ethan |last=Siegel |url=http://scienceblogs.com/startswithabang/2012/12/12/why-the-world-will-run-out-of-helium/ |title=Why the World Will Run Out of Helium |website=Starts with a Bang |publisher=Scienceblogs.com |date=12 December 2012 |access-date=16 September 2013 |archive-url=https://web.archive.org/web/20130914120934/http://scienceblogs.com/startswithabang/2012/12/12/why-the-world-will-run-out-of-helium/ |archive-date=14 September 2013 |url-status=live }}</ref> However, some studies suggest that helium produced deep in the Earth by radioactive decay can collect in natural gas reserves in larger-than-expected quantities,<ref>{{Cite web|url=http://www.gizmag.com/helium-source-natural-gas-fields/39038/|title=We may not be running out of helium after all|last=Szondy|first=David|website=www.gizmag.com|access-date=1 April 2016|archive-url=https://web.archive.org/web/20160325044958/http://www.gizmag.com/helium-source-natural-gas-fields/39038/|archive-date=25 March 2016|url-status=live|date=24 August 2015}}</ref> in some cases having been released by volcanic activity.<ref name="Sample">{{cite news|url=https://www.theguardian.com/science/2016/jun/28/huge-helium-gas-tanzania-east-africa-averts-medical-shortage|title=Huge helium gas find in east Africa averts medical shortage|work=The Guardian|first=Ian|last=Sample|date=28 June 2016|access-date=29 June 2016|archive-url=https://web.archive.org/web/20160629022834/https://www.theguardian.com/science/2016/jun/28/huge-helium-gas-tanzania-east-africa-averts-medical-shortage|archive-date=29 June 2016|url-status=live}}</ref>

==History==

===Scientific discoveries===
The first evidence of helium was observed on August 18, 1868, as a bright yellow line with a [[wavelength]] of 587.49 nanometers in the [[Emission spectrum|spectrum]] of the [[chromosphere]] of the [[Sun]]. The line was detected by French astronomer [[Pierre Janssen|Jules Janssen]] during [[Solar eclipse of August 18, 1868|a total solar eclipse]] in [[Guntur]], India.<ref name="frnch">{{Cite journal|title = French astronomers in India during the 17th&nbsp;– 19th centuries |journal = Journal of the British Astronomical Association|volume =101|issue = 2|pages = 95–100|bibcode = 1991JBAA..101...95K|author = Kochhar, R. K.|date=1991}}</ref><ref name="nbb" /> This line was initially assumed to be [[sodium]]. On October 20 of the same year, English astronomer [[Norman Lockyer]] observed a yellow line in the solar spectrum, which he named the D<sub>3</sub> because it was near the known D<sub>1</sub> and D<sub>2</sub> [[Fraunhofer line]]s of sodium.<ref name="Lockyer 1868">{{cite journal |last1=Lockyer |first1=J. N. |title=Notice of an observation of the spectrum of a solar prominence |journal= Proceedings of the Royal Society of London |volume=17 |date=October 1868 |pages=91–92 |url= https://babel.hathitrust.org/cgi/pt?id=hvd.32044106279359;view=1up;seq=109 |jstor=112357 |access-date=3 June 2018 |bibcode=1868RSPS...17...91L |doi=10.1098/rspl.1868.0011|s2cid=163097539 |url-access=subscription }}</ref><ref name="enc">{{Cite book|title= The Encyclopedia of the Chemical Elements |pages =256–268 |first = Clifford A. |last=Hampel |location=New York |isbn = 978-0-442-15598-8 |date = 1968 |publisher =Van Nostrand Reinhold}}</ref> He concluded that it was caused by an element in the Sun unknown on Earth. Lockyer named the element with the Greek word for the Sun, ἥλιος (''[[helios]]'').<ref>{{OEtymD|helium}}</ref><ref>{{Cite journal |last=Thomson |first=William |date=August 3, 1871 |volume=4 |pages=261–278 [268] |doi=10.1038/004261a0 |title=Inaugural Address of Sir William Thomson |journal=Nature |url=https://books.google.com/books?id=IogCAAAAIAAJ&pg=PA268 |quote=Frankland and Lockyer find the yellow prominences to give a very decided bright line not far from D, but hitherto not identified with any terrestrial flame. It seems to indicate a new substance, which they propose to call Helium |bibcode=1871Natur...4..261. |issue=92 |pmc=2070380 |access-date=February 22, 2016 |archive-url=https://web.archive.org/web/20161202011154/https://books.google.com/books?id=IogCAAAAIAAJ&pg=PA268 |archive-date=December 2, 2016 |url-status=live }}</ref> It is sometimes said that English chemist [[Edward Frankland]] was also involved in the naming, but this is unlikely as he doubted the existence of this new element. The ending "-ium" is unusual, as it normally applies only to metallic elements; probably Lockyer, being an astronomer, was unaware of the chemical conventions.<ref name=jensen>{{Cite journal |last=Jensen |first=William B. |date=2004 |volume=81 |issue=7 |page=944 |doi=10.1021/ed081p944 |title=Why Helium ends in "-ium" |journal=Journal of Chemical Education|bibcode=2004JChEd..81..944J }}</ref>
[[File:Helium spectrum.jpg|left|thumb|Spectral lines of helium|alt=Picture of visible spectrum with superimposed sharp yellow and blue and violet lines]]
In 1881, Italian physicist [[Luigi Palmieri]] detected helium on Earth for the first time through its D<sub>3</sub> spectral line, when he analyzed a material that had been [[Sublimation (phase transition)|sublimated]] during a recent eruption of [[Mount Vesuvius]].<ref name="Palmieri 1881">{{cite journal |last1=Palmieri |first1=Luigi |title=La riga dell'Helium apparsa in una recente sublimazione vesuviana |trans-title=The line of helium appeared in a recently sublimated material [from Mt.] Vesuvius. |journal=Rendiconto dell'Accademia delle Scienze Fisiche e Matematiche (Naples, Italy) |volume=20 |date=1881 |page=223 |url=https://babel.hathitrust.org/cgi/pt?id=hvd.hnl7mr;view=1up;seq=251 |access-date=1 May 2017 |quote= ''Raccolsi alcun tempo fa una sostanza amorfa di consistenza butirracea e di colore giallo sbiadato sublimata sull'orlo di una fumarola prossima alla bocca di eruzione. Saggiata questa sublimazione allo spettroscopio, ho ravvisato le righe del sodio e del potassio ed una lineare ben distinta che corrisponde esattamente alla D<sub>3</sub> che è quella dell'Helium. Do per ora il semplice annunzio del fatto, proponendomi di ritornare sopra questo argomento, dopo di aver sottoposta la sublimazione ad una analisi chimica.'' (I collected some time ago an amorphous substance having a buttery consistency and a faded yellow color which had sublimated on the rim of a fumarole near the mouth of the eruption. Having analyzed this sublimated substance with a spectroscope, I recognized the lines of sodium and potassium and a very distinct linear line which corresponds exactly to D<sub>3</sub>, which is that of helium. For the present, I'm making a mere announcement of the fact, proposing to return to this subject after having subjected the sublimate to a chemical analysis.) |archive-url= https://web.archive.org/web/20180901111504/https://babel.hathitrust.org/cgi/pt?id=hvd.hnl7mr;view=1up;seq=251 |archive-date=1 September 2018 |url-status=live }}</ref>

[[File:William Ramsay working.jpg|thumb|upright|Sir [[William Ramsay]], the discoverer of terrestrial helium]]
[[File:Clevite sample (35321726345).jpg|thumb|upright|The cleveite sample from which Ramsay first purified helium<ref name="Kirk">{{cite web| last1=Kirk|first1=Wendy L.| title= Cleveite [not Clevite] and helium| url=https://blogs.ucl.ac.uk/museums/2013/01/11/cleveite-and-helium-not-clevite/| website=Museums & Collections Blog| publisher=[[University College London]]| access-date=18 August 2017|archive-url= https://web.archive.org/web/20181018054313/http://blogs.ucl.ac.uk/museums/2013/01/11/cleveite-and-helium-not-clevite/| archive-date=18 October 2018|url-status= live}}</ref>]]
On March 26, 1895, Scottish chemist [[William Ramsay|Sir William Ramsay]] isolated helium on Earth by treating the mineral cleveite (a variety of uraninite with at least 10% [[rare-earth elements]]) with mineral [[acid]]s. Ramsay was looking for [[argon]] but, after separating [[nitrogen]] and [[oxygen]] from the gas, liberated by [[sulfuric acid]], he noticed a bright yellow line that matched the D<sub>3</sub> line observed in the spectrum of the Sun.<ref name="enc" /><ref>{{Cite journal|title = On a Gas Showing the Spectrum of Helium, the Reputed Cause of D<sub>3</sub>, One of the Lines in the Coronal Spectrum. Preliminary Note| last = Ramsay | first= William|author-link = William Ramsay| journal = Proceedings of the Royal Society of London|volume = 58|issue = 347–352|pages = 65–67| date = 1895|doi = 10.1098/rspl.1895.0006| bibcode = 1895RSPS...58...65R| s2cid = 129872109| url = https://zenodo.org/record/1432083|doi-access = free}}</ref><ref>{{Cite journal| title = Helium, a Gaseous Constituent of Certain Minerals. Part I|last = Ramsay | first= William|journal = Proceedings of the Royal Society of London|volume = 58| issue = 347–352|pages = 81–89|date = 1895 |doi = 10.1098/rspl.1895.0010| bibcode = 1895RSPS...58...80R|doi-access = free}}</ref><ref>{{Cite journal |title = Helium, a Gaseous Constituent of Certain Minerals. Part II – Density|last = Ramsay | first= William| journal = Proceedings of the Royal Society of London|volume = 59|issue = 1|pages = 325–330|date = 1895 |doi = 10.1098/rspl.1895.0097|bibcode = 1895RSPS...59..325R|s2cid = 96589261}}</ref> These samples were identified as helium by Lockyer and British physicist [[William Crookes]].<ref>{{Cite journal|title = On the new gas obtained from uraninite. Preliminary note, part II|author = Lockyer, J. Norman|author-link = Norman Lockyer| journal = Proceedings of the Royal Society of London|volume = 58|issue = 347–352| pages = 67–70|date = 1895|doi = 10.1098/rspl.1895.0008|doi-access = free}}</ref><ref>See:
* {{cite journal| last= Crookes| first= William | year= 1895 | url= https://books.google.com/books?id=YCLOAAAAMAAJ&pg=PA151 | title= The spectrum of the gas from clèveite | journal= The Chemical News and Journal of Physical Science| volume= 71 | number= 1844 | page= 151}}
*  {{cite journal| last= Crookes| first= William | year= 1895 | url= https://books.google.com/books?id=lSLOAAAAMAAJ&pg=PA87 | title= The spectrum of helium | journal= The Chemical News and Journal of Physical Science | volume= 72 | number= 1865 | pages=87–89}}</ref> It was independently isolated from cleveite in the same year by chemists [[Per Teodor Cleve]] and [[Abraham Langlet]] in [[Uppsala]], Sweden, who collected enough of the gas to accurately determine its [[atomic weight]].<ref>See:
*  {{cite journal |last1=Clève |first1=P.T. |title=Sur la présence de l'hélium dans le clévéite |journal=Comptes rendus hebdomadaires des séances de l'Académie des sciences |date=1895 |volume=120 |page=834 |url=https://babel.hathitrust.org/cgi/pt?id=mdp.39015035451122&view=1up&seq=844&skin=2021 |trans-title=On the presence of helium in cleveite |language=French}}
*  English translation:  {{cite journal |last1=Clève |first1=P.T. |title=On the presence of helium in clèveite |journal=The Chemical News and Journal of Physical Science |date=1895 |volume=71 |issue=1849 |page=212 |url=https://babel.hathitrust.org/cgi/pt?id=hvd.32044048675458&view=1up&seq=272&skin=2021}}
*  {{cite journal |last1=Thorpe |first1=T. E. |title=Terrestrial helium? |journal=Nature |date=1895 |volume=51 |issue=1329 |page=586 |url=https://babel.hathitrust.org/cgi/pt?id=uc1.31210011061270&view=1up&seq=632&skin=2021}}
*  {{cite journal |last1=Clève |title=Sur la densité de l'hélium |journal=Comptes rendus hebdomadaires des séances de l'Académie des sciences |date=1895 |volume=120 |page=1212 |url=https://babel.hathitrust.org/cgi/pt?id=mdp.39015035451122&view=1up&seq=1226&skin=2021 |trans-title=On the density of helium |language=French}}</ref><ref>{{Cite journal|title = Das Atomgewicht des Heliums|trans-title = The atomic weight of helium|author = Langlet, N. A.|journal = Zeitschrift für Anorganische Chemie|volume = 10|issue = 1| pages = 289–292|date = 1895|url=https://books.google.com/books?id=sHcWAAAAIAAJ&pg=PA289|doi =10.1002/zaac.18950100130|language= de}}</ref><ref name="nbb" /><ref>{{cite book |last1=Weaver |first1=E.R. |title=Circular of the Bureau of Standards No. 81: Bibliography of Scientific Literature Relating to Helium |date=1919 |page=6 |publisher=U.S. Government Printing Office |location=Washington, D.C., USA |url=https://nvlpubs.nist.gov/nistpubs/Legacy/circ/nbscircular81.pdf}}</ref> Helium was also isolated by American geochemist [[William Francis Hillebrand]] prior to Ramsay's discovery, when he noticed unusual spectral lines while testing a sample of the mineral uraninite. Hillebrand, however, attributed the lines to [[nitrogen]].<ref>Hillebrand (1890) [https://babel.hathitrust.org/cgi/pt?id=uc1.b2968310&view=1up&seq=511 "On the occurrence of nitrogen in uraninite and on the composition of uraninite in general,"] ''Bulletin of the U.S. Geological Survey'', no. 78, pp. 43–79.</ref> His letter of congratulations to Ramsay offers an interesting case of discovery, and near-discovery, in science.<ref>{{Cite book|last=Munday|first=Pat|author-link=Pat Munday|date=1999|title=Biographical entry for W.F. Hillebrand (1853–1925), geochemist and U.S. Bureau of Standards administrator in American National Biography|editor=John A. Garraty|editor2=Mark C. Carnes|volume=10–11|publisher=Oxford University Press|pages= 808–9; 227–8|title-link=American National Biography}}</ref>

In 1907, [[Ernest Rutherford]] and [[Thomas Royds]] demonstrated that [[alpha particle]]s are helium [[atomic nucleus|nuclei]] by allowing the particles to penetrate the thin glass wall of an [[evacuated tube]], then creating a discharge in the tube, to study the spectrum of the new gas inside.<ref>{{Cite journal| doi = 10.1080/14786440808636511| title = XXIV.Spectrum of the radium emanation| journal = Philosophical Magazine| series = series 6| volume = 16| issue = 92| pages = 313–317| year = 1908| last1 = Rutherford| first1 = E.| last2 = Royds| first2 = T.| url = https://babel.hathitrust.org/cgi/pt?id=umn.31951000614205r;view=1up;seq=349| url-access = subscription}}</ref> In 1908, helium was first liquefied by Dutch physicist [[Heike Kamerlingh Onnes]] by cooling the gas to less than {{convert|5|K|C F}}.<ref>Onnes, H. Kamerlingh (1908) [https://web.archive.org/web/20180809111624/https://babel.hathitrust.org/cgi/pt?id=uva.x002433831;view=1up;seq=309 "The liquefaction of helium,"] ''Communications from the Physical Laboratory at the University of Leiden'', '''9''' (108) : 1–23.</ref><ref>{{Cite journal|title = Little cup of Helium, big Science |author = van Delft, Dirk |journal = Physics Today |url = http://www-lorentz.leidenuniv.nl/history/cold/VanDelftHKO_PT.pdf |pages = 36–42 |date = 2008 |access-date = 2008-07-20|archive-url = https://web.archive.org/web/20080625064354/http://www-lorentz.leidenuniv.nl/history/cold/VanDelftHKO_PT.pdf |archive-date = June 25, 2008|url-status=dead|bibcode = 2008PhT....61c..36V|volume = 61|doi = 10.1063/1.2897948|issue = 3}}</ref> He tried to solidify it by further reducing the temperature but failed, because helium does not solidify at atmospheric pressure. Onnes' student [[Willem Hendrik Keesom]] was eventually able to solidify 1&nbsp;cm<sup>3</sup> of helium in 1926 by applying additional external pressure.<ref>See:
* Preliminary notice: Keesom, W. H. (17 July 1926) Letters to the Editor: "Solidification of helium," ''Nature'', '''118''' : 81.
* Preliminary notice: Keesom, W. H. (1926) [https://archive.org/stream/ComptesRendusAcademieDesSciences0183/ComptesRendusAcadmieDesSciences-Tome183-Juillet-dcembre1926#page/n25/mode/2up "L'hélium solidifié,"] {{Webarchive|url=https://web.archive.org/web/20161022075647/https://archive.org/stream/ComptesRendusAcademieDesSciences0183/ComptesRendusAcadmieDesSciences-Tome183-Juillet-dcembre1926#page/n25/mode/2up |date=2016-10-22 }} ''Comptes rendus'' ... , '''183''' : 26.
* Keesom, W. H. (1926) "Solid Helium," ''Communications from the Physical Laboratory at the University of Leiden'', '''17''' (184) .</ref><ref>{{Cite news| title = Coldest Cold| publisher = Time Inc.| date = 1929-06-10| url = http://www.time.com/time/magazine/article/0,9171,751945,00.html| access-date = 2008-07-27| archive-url = https://web.archive.org/web/20081206015739/http://www.time.com/time/magazine/article/0,9171,751945,00.html| archive-date = 2008-12-06| url-status = dead}}</ref>

In 1913, [[Niels Bohr]] published his "trilogy"<ref name = Hoyer>{{cite book|first = Ulrich|last = Hoyer|chapter = Constitution of Atoms and Molecules|pages = 103–316 (esp. pp. 116–122)|title = Niels Bohr – Collected Works: Volume 2 – Work on Atomic Physics (1912–1917)|chapter-url = https://books.google.com/books?id=zGczmJjSO6kC&pg=PA117|editor-first = Ulrich|editor-last = Hoyer|publisher = [[North Holland Publishing Company]]|location = Amsterdam|year = 1981|isbn = 978-0720418002}}</ref><ref>{{cite book|last = Kennedy|first = P. J.|year = 1985|chapter = A Short Biography|editor1-last = French|editor1-first = A. P.|editor2-last = Kennedy|editor2-first = P. J.|title = Niels Bohr: A Centenary Volume|pages = 3–15|publisher = [[Harvard University Press]]|isbn = 978-0-674-62415-3|chapter-url-access = registration|chapter-url = https://archive.org/details/nielsbohrcentena00bohr}}</ref> on atomic structure that included a reconsideration of the [[Pickering–Fowler series]] as central evidence in support of his [[Bohr model|model of the atom]].<ref>{{cite journal|last = Bohr|first = N.|author-link = Niels Bohr|year = 1913|title = On the constitution of atoms and molecules, part I|journal = [[Philosophical Magazine]]|volume = 26|issue = 151|pages = 1–25|doi = 10.1080/14786441308634955|url = http://web.ihep.su/dbserv/compas/src/bohr13/eng.pdf|access-date = 2017-12-27|archive-url = https://web.archive.org/web/20190404184145/http://web.ihep.su/dbserv/compas/src/bohr13/eng.pdf|archive-date = 2019-04-04|url-status = live|bibcode = 1913PMag...26....1B}}<br />{{cite journal|last = Bohr|first = N.|author-link = Niels Bohr|year = 1913|title = On the constitution of atoms and molecules, part II: Systems Containing Only a Single Nucleus|journal = [[Philosophical Magazine]]|volume = 26|issue = 153|pages = 476–502|url = http://web.ihep.su/dbserv/compas/src/bohr13b/eng.pdf|doi = 10.1080/14786441308634993|access-date = 2017-12-27|archive-url = https://web.archive.org/web/20171215041355/http://web.ihep.su/dbserv/compas/src/bohr13b/eng.pdf|archive-date = 2017-12-15|url-status = live|bibcode = 1913PMag...26..476B}}<br />{{cite journal|last = Bohr|first = N.|author-link = Niels Bohr|year = 1913|title = On the constitution of atoms and molecules, part III: Systems containing several nuclei|journal = [[Philosophical Magazine]]|volume = 26|issue = 155|pages = 857–875|doi = 10.1080/14786441308635031|url = https://zenodo.org/record/1430922|bibcode = 1913PMag...26..857B}}</ref><ref name = Robotti>{{cite journal|title = The Spectrum of ζ Puppis and the Historical Evolution of Empirical Data|first = Nadia|last = Robotti|author-link=Nadia Robotti|journal = [[Historical Studies in the Physical Sciences]]|volume = 14|issue = 1|year = 1983|pages = 123–145|doi = 10.2307/27757527|jstor = 27757527}}</ref> This series is named for [[Edward Charles Pickering]], who in 1896 published observations of previously unknown lines in the spectrum of the star [[Zeta Puppis|ζ Puppis]]<ref>{{cite journal|last = Pickering|first = E. C.|author-link = Edward Charles Pickering|journal = [[Harvard College Observatory Circular]]|volume = 12|title = Stars having peculiar spectra. New variable stars in Crux and Cygnus|pages = 1–2|year = 1896|bibcode = 1896HarCi..12....1P}} Also published as: {{cite journal|title = Stars having peculiar spectra. New variable stars in Crux and Cygnus|last1 = Pickering|first1 = E. C.|author-link = Edward Charles Pickering|last2 = Fleming|first2 = W. P.|author-link2 = Williamina Fleming|journal = [[Astrophysical Journal]]|volume = 4|pages = 369–370|year = 1896|doi = 10.1086/140291|bibcode = 1896ApJ.....4..369P|doi-access = free}}</ref> (these are now known to occur with [[Wolf-Rayet star|Wolf–Rayet]] and other hot stars).<ref>{{cite journal|title = The relation between the Wolf–Rayet stars and the planetary nebulae|first = W. H.|last = Wright|journal = [[Astrophysical Journal]]|volume = 40|pages = 466–472|year = 1914|doi = 10.1086/142138|bibcode = 1914ApJ....40..466W|doi-access = free}}</ref> Pickering attributed the observation (lines at 4551, 5411, and 10123&nbsp;[[Ångström|Å]]) to a new form of hydrogen with half-integer transition levels.<ref>{{cite journal|title = Stars having peculiar spectra. New variable Stars in Crux and Cygnus|first = E. C.|last = Pickering|author-link = Edward Charles Pickering|year = 1897|journal = [[Astronomische Nachrichten]]|volume = 142|issue = 6|pages = 87–90|doi = 10.1002/asna.18971420605|bibcode = 1896AN....142...87P|url = https://zenodo.org/record/1424755|access-date = 2019-08-24|archive-url = https://web.archive.org/web/20190824143848/https://zenodo.org/record/1424755/files/article.pdf|archive-date = 2019-08-24|url-status = live}}</ref><ref>{{cite journal|title = The spectrum of zeta Puppis|last = Pickering|first = E. C.|author-link = Edward Charles Pickering|year = 1897|journal = [[Astrophysical Journal]]|volume = 5|pages = 92–94|doi = 10.1086/140312|bibcode = 1897ApJ.....5...92P|doi-access = free}}</ref> In 1912, [[Alfred Fowler]]<ref>{{cite book|title = The Methodology of Scientific Research Programmes|first = Imre|last = Lakatos|author-link = Imre Lakatos|publisher = [[Cambridge University Press]]|year = 1980|isbn = 9780521280310|editor1-first = John|editor1-last = Worrall|editor2-first = Gregory|editor2-last = Currie|chapter-url = https://books.google.com/books?id=RRniFBI8Gi4C&pg=PA62|chapter = Bohr: A Research Programme Progressing on Inconsistent Foundations|pages = 55–68}}</ref> managed to produce similar lines from a hydrogen-helium mixture, and supported Pickering's conclusion as to their origin.<ref>{{cite journal|title = Observations of the Principal and other Series of Lines in the Spectrum of Hydrogen|first = A.|last = Fowler|author-link = Alfred Fowler|journal = [[Monthly Notices of the Royal Astronomical Society]]|volume = 73|issue = 2|year = 1912|pages = 62–63|doi = 10.1093/mnras/73.2.62|bibcode = 1912MNRAS..73...62F|doi-access = free}}</ref> Bohr's model does not allow for half-integer transitions (nor does quantum mechanics) and Bohr concluded that Pickering and Fowler were wrong, and instead assigned these spectral lines to ionised helium, He<sup>+</sup>.<ref>{{cite journal|title = The Spectra of Helium and Hydrogen|first = N.|last = Bohr|author-link = Niels Bohr|journal = [[Nature (journal)|Nature]]|volume = 92|issue = 2295|year = 1913|pages = 231–232|doi = 10.1038/092231d0|bibcode = 1913Natur..92..231B|s2cid = 11988018|url = https://zenodo.org/record/1429570}}</ref> Fowler was initially skeptical<ref>{{cite journal|title = The Spectra of Helium and Hydrogen|first = A.|last = Fowler|author-link = Alfred Fowler|journal = [[Nature (journal)|Nature]]|volume = 92|issue = 2291|year = 1913|pages = 95–96|doi = 10.1038/092095b0|bibcode = 1913Natur..92...95F|s2cid = 3972599|url = https://zenodo.org/record/1429568}}</ref> but was ultimately convinced<ref>{{cite journal|title = Reply to: The Spectra of Helium and Hydrogen|first = A.|last = Fowler|author-link = Alfred Fowler|journal = [[Nature (journal)|Nature]]|volume = 92|issue = 2295|year = 1913|pages = 232–233|doi=10.1038/092232a0|bibcode = 1913Natur..92..232F|s2cid = 3981817|url = https://zenodo.org/record/1429568}}</ref> that Bohr was correct,<ref name = Hoyer /> and by 1915 "spectroscopists had transferred [the Pickering–Fowler series] definitively [from hydrogen] to helium."<ref name = Robotti /><ref>{{cite journal|title = The Spectra of Hydrogen and Helium|first = N.|last = Bohr|author-link = Niels Bohr|journal = [[Nature (journal)|Nature]]|volume = 95|issue = 6–7|pages = 6–7|year = 1915|doi = 10.1038/095006a0|bibcode = 1915Natur..95....6B|s2cid = 3947572|url = https://zenodo.org/record/1429597}}</ref> Bohr's theoretical work on the Pickering series had demonstrated the need for "a re-examination of problems that seemed already to have been solved within classical theories" and provided important confirmation for his atomic theory.<ref name = Robotti />

In 1938, Russian physicist [[Pyotr Leonidovich Kapitsa]] discovered that [[helium-4]] has almost no [[viscosity]] at temperatures near [[absolute zero]], a phenomenon now called [[superfluidity]].<ref>{{Cite journal|title = Viscosity of Liquid Helium below the λ-Point |author = Kapitza, P. |author-link = Pyotr Leonidovich Kapitsa |journal =Nature|volume = 141|issue = 3558 |page = 74 |doi = 10.1038/141074a0 |date = 1938|bibcode = 1938Natur.141...74K |s2cid = 3997900 |doi-access = free }}</ref> This phenomenon is related to [[Bose–Einstein condensation]]. In 1972, the same phenomenon was observed in [[helium-3]], but at temperatures much closer to absolute zero, by American physicists [[Douglas D. Osheroff]], [[David M. Lee]], and [[Robert Coleman Richardson|Robert C. Richardson]]. The phenomenon in helium-3 is thought to be related to pairing of helium-3 [[fermion]]s to make [[boson]]s, in analogy to [[Cooper pairs]] of electrons producing [[superconductivity]].<ref>{{Cite journal|title = Evidence for a New Phase of Solid He<sup>3</sup> |author = Osheroff, D. D. |author2 = Richardson, R. C. |author3 = Lee, D. M. |journal = Phys. Rev. Lett. |volume = 28 |issue = 14 |pages = 885–888 |doi = 10.1103/PhysRevLett.28.885 |date = 1972 |bibcode=1972PhRvL..28..885O|s2cid = 89609083 |doi-access = free }}</ref>

In 1961, Vignos and Fairbank reported the existence of a different phase of solid helium-4, designated the gamma-phase. It exists for a narrow range of pressure between 1.45 and 1.78 K.<ref>{{Cite journal |last1=Vignos |first1=James H. |last2=Fairbank |first2=Henry A. |date=1961-03-15 |title=<nowiki>New Solid Phase in ${\mathrm{He}}^{4}$</nowiki> |url=https://link.aps.org/doi/10.1103/PhysRevLett.6.265 |journal=Physical Review Letters |volume=6 |issue=6 |pages=265–267 |doi=10.1103/PhysRevLett.6.265|url-access=subscription }}</ref>

===Extraction and use===
{{Globalize|section|date=February 2022|discuss=Talk:Helium#Other history}}
[[File:Kansas Helium Marker.jpg|thumb|Historical marker, denoting a massive helium find near [[Dexter, Kansas]]]]
After an oil drilling operation in 1903 in [[Dexter, Kansas]] produced a gas geyser that would not burn, Kansas state geologist [[Erasmus Haworth]] collected samples of the escaping gas and took them back to the [[University of Kansas]] at Lawrence where, with the help of chemists [[Hamilton Cady]] and David McFarland, he discovered that the gas consisted of, by volume, 72% nitrogen, 15% [[methane]] (a [[combustible]] percentage only with sufficient oxygen), 1% hydrogen, and 12% an unidentifiable gas.<ref name="nbb" /><ref>{{Cite journal|author = McFarland, D. F. |title = Composition of Gas from a Well at Dexter, Kan |volume = 19|pages = 60–62 |date = 1903 |journal = Transactions of the Kansas Academy of Science |doi = 10.2307/3624173|jstor = 3624173}}</ref> With further analysis, Cady and McFarland discovered that 1.84% of the gas sample was helium.<ref>{{cite web | title = Discovery of Helium in Natural Gas at the University of Kansas | website = National Historic Chemical Landmarks | publisher = American Chemical Society | url = http://www.acs.org/content/acs/en/education/whatischemistry/landmarks/heliumnaturalgas.html | access-date = 2014-02-21 | archive-url = https://web.archive.org/web/20140226053732/http://www.acs.org/content/acs/en/education/whatischemistry/landmarks/heliumnaturalgas.html | archive-date = 2014-02-26 | url-status = live }}</ref><ref>{{Cite journal|author = Cady, H. P. |last2=McFarland|first2=D. F.|title = Helium in Natural Gas |journal = Science |volume = 24 |issue = 611|page = 344 |doi = 10.1126/science.24.611.344 |date = 1906 |pmid = 17772798|bibcode = 1906Sci....24..344D |s2cid=27441003 |url=https://zenodo.org/record/1447970}}</ref> This showed that despite its overall rarity on Earth, helium was concentrated in large quantities under the [[American Great Plains]], available for extraction as a byproduct of [[natural gas]].<ref>{{Cite journal|author = Cady, H. P.|author2 = McFarland, D. F.|title = Helium in Kansas Natural Gas |journal = Transactions of the Kansas Academy of Science |volume = 20 |pages = 80–81 |date = 1906|doi = 10.2307/3624645|jstor = 3624645}}</ref>

Following a suggestion by Sir [[Richard Threlfall]], the [[United States Navy]] sponsored three small experimental helium plants during World War I. The goal was to supply [[barrage balloon]]s with the non-flammable, lighter-than-air gas. A total of {{convert|5700|m3|ft3|abbr=on}} of 92% helium was produced in the program even though less than a cubic meter of the gas had previously been obtained.<ref name="enc" /> Some of this gas was used in the world's first helium-filled airship, the U.S. Navy's [[C-class blimp]] C-7, which flew its maiden voyage from [[Hampton Roads, Virginia]], to [[Bolling Field]] in Washington, D.C., on December 1, 1921,<ref>{{Cite book |editor=Emme, Eugene M. comp. |editor-link=Eugene M. Emme |title=Aeronautics and Astronautics: An American Chronology of Science and Technology in the Exploration of Space, 1915–1960 |date=1961 |pages=11–19 |chapter=Aeronautics and Astronautics Chronology, 1920–1924 |chapter-url=http://www.hq.nasa.gov/office/pao/History/Timeline/1920-24.html |publisher=[[NASA]] |location=Washington, D.C. |access-date=2006-10-27 |archive-date=2019-07-14 |archive-url=https://web.archive.org/web/20190714112810/https://www.hq.nasa.gov/office/pao/History/Timeline/1920-24.html |url-status=dead }}</ref> nearly two years before the Navy's first ''rigid'' helium-filled airship, the [[Naval Aircraft Factory]]-built [[USS Shenandoah (ZR-1)|USS ''Shenandoah'']], flew in September 1923.

Although the extraction process using low-temperature [[gas liquefaction]] was not developed in time to be significant during World War I, production continued. Helium was primarily used as a [[lifting gas]] in lighter-than-air craft. During World War II, the demand increased for helium for lifting gas and for shielded arc [[welding]]. The [[helium mass spectrometer]] was also vital in the atomic bomb [[Manhattan Project]].<ref>{{Cite book|chapter=Leak Detection|last=Hilleret|first=N.|publisher=[[CERN]]|title=CERN Accelerator School, vacuum technology: proceedings: Scanticon Conference Centre, Snekersten, Denmark, 28 May&nbsp;– 3 June 1999 |editor=S. Turner |location=Geneva, Switzerland|chapter-url=http://cdsweb.cern.ch/record/455564 |chapter-format=PDF| date=1999 |pages=203–212 |doi=10.5170/CERN-1999-005.203 |quote=At the origin of the helium leak detection method was the Manhattan Project and the unprecedented leak-tightness requirements needed by the uranium enrichment plants. The required sensitivity needed for the leak checking led to the choice of a mass spectrometer designed by Dr. A.O.C. Nier tuned on the helium mass.}}</ref>

The [[government of the United States]] set up the [[National Helium Reserve]] in 1925 at [[Amarillo, Texas]], with the goal of supplying military [[airship]]s in time of war and commercial airships in peacetime.<ref name="enc" /> Because of the [[Helium Act of 1925]], which banned the export of scarce helium on which the US then had a production monopoly, together with the prohibitive cost of the gas, German [[Zeppelin]]s were forced to use hydrogen as lifting gas, which would gain infamy in the [[Hindenburg disaster]]. The helium market after World War II was depressed but the reserve was expanded in the 1950s to ensure a supply of [[liquid helium]] as a coolant to create oxygen/hydrogen [[rocket fuel]] (among other uses) during the [[Space Race]] and [[Cold War]]. Helium use in the United States in 1965 was more than eight times the peak wartime consumption.<ref>{{Cite journal| doi = 10.2307/3627447| author = Williamson, John G.| title = Energy for Kansas| journal = Transactions of the Kansas Academy of Science| volume = 71| issue = 4| pages = 432–438|date =1968| jstor = 3627447}}</ref>

After the Helium Acts Amendments of 1960 (Public Law 86–777), the [[United States Bureau of Mines|U.S. Bureau of Mines]] arranged for five private plants to recover helium from natural gas. For this helium conservation program, the Bureau built a {{convert|425|mi|km|adj=on}} pipeline from [[Bushton, Kansas]], to connect those plants with the government's partially depleted Cliffside gas field near Amarillo, Texas. This helium-nitrogen mixture was injected and stored in the Cliffside gas field until needed, at which time it was further purified.<ref>{{Cite journal|journal = Federal Register|date = 2005-10-06|volume = 70|issue = 193|page = 58464|url = http://edocket.access.gpo.gov/2005/pdf/05-20084.pdf|title = Conservation Helium Sale|access-date = 2008-07-20|archive-url = https://web.archive.org/web/20081031082452/http://edocket.access.gpo.gov/2005/pdf/05-20084.pdf|archive-date = 2008-10-31|url-status = live}}</ref>

By 1995, a billion cubic meters of the gas had been collected and the reserve was US$1.4&nbsp;billion in debt, prompting the [[Congress of the United States]] in 1996 to discontinue the reserve.<ref name="nbb" /><ref name="stwertka">Stwertka, Albert (1998). ''Guide to the Elements: Revised Edition''. New York; Oxford University Press, p. 24. {{ISBN|0-19-512708-0}}</ref> The resulting [[Helium Privatization Act of 1996]]<ref>{{USPL|104|273|Helium Privatization Act of 1996}}</ref> (Public Law 104–273) directed the [[United States Department of the Interior]] to empty the reserve, with sales starting by 2005.<ref>{{Cite book |url = http://www.nap.edu/openbook.php?isbn=0309070384 |title = Executive Summary |publisher = nap.edu |access-date = 2008-07-20 |archive-url = https://web.archive.org/web/20080327004306/http://www.nap.edu/openbook.php?isbn=0309070384 |archive-date = 2008-03-27 |url-status = live |doi = 10.17226/9860 |year = 2000 |isbn = 978-0-309-07038-6 }}</ref>

Helium produced between 1930 and 1945 was about 98.3% pure (2% nitrogen), which was adequate for airships. In 1945, a small amount of 99.9% helium was produced for welding use. By 1949, commercial quantities of Grade A 99.95% helium were available.<ref>{{Cite book|publisher=Bureau of Mines / Minerals yearbook 1949|date=1951|last1=Mullins|first1=P. V.|last2=Goodling|first2=R. M.|title=Helium|pages=599–602|url=http://digicoll.library.wisc.edu/cgi-bin/EcoNatRes/EcoNatRes-idx?type=div&did=ECONATRES.MINYB1949.PVMULLINS&isize=text|access-date=2008-07-20|archive-url=https://web.archive.org/web/20081206011210/http://digicoll.library.wisc.edu/cgi-bin/EcoNatRes/EcoNatRes-idx?type=div&did=ECONATRES.MINYB1949.PVMULLINS&isize=text|archive-date=2008-12-06|url-status=live}}</ref>

For many years, the United States produced more than 90% of commercially usable helium in the world, while extraction plants in Canada, Poland, Russia, and other nations produced the remainder. In the mid-1990s, a new plant in [[Arzew]], Algeria, producing {{convert|17|e6m3|e6ft3|abbr=off}} began operation, with enough production to cover all of Europe's demand. Meanwhile, by 2000, the consumption of helium within the U.S. had risen to more than 15 million kg per year.<ref>{{cite web|url=https://minerals.usgs.gov/ds/2005/140/helium-use.pdf|title=Helium End User Statistic|access-date=2008-07-20|publisher=U.S. Geological Survey|archive-url=https://web.archive.org/web/20080921114913/http://minerals.usgs.gov/ds/2005/140/helium-use.pdf|archive-date=2008-09-21|url-status=live}}</ref> In 2004–2006, additional plants in [[Ras Laffan Industrial City|Ras Laffan]], [[Qatar]], and [[Skikda]], Algeria were built. Algeria quickly became the second leading producer of helium.<ref name="wwsupply">{{Cite journal
 |title=Challenges to the Worldwide Supply of Helium in the Next Decade |last1=Smith|first1=E. M. |last2=Goodwin|first2=T. W. |last3=Schillinger|first3=J. |journal=Advances in Cryogenic Engineering |volume=A |issue=710 |pages=119–138
 |series=49
 |date=2003 |doi=10.1063/1.1774674 |bibcode=2004AIPC..710..119S|s2cid=109060534}}</ref> Through this time, both helium consumption and the costs of producing helium increased.<ref name="Kaplan2007">{{cite journal
 |last=Kaplan |first=Karen H. |date = June 2007|title=Helium shortage hampers research and industry
 |periodical=[[Physics Today]] |publisher=[[American Institute of Physics]]
 |volume=60 |issue=6 |pages=31–32
 |doi=10.1063/1.2754594
|bibcode = 2007PhT....60f..31K }}</ref> From 2002 to 2007 helium prices doubled.<ref name="Basu2007">{{Cite news |last=Basu |first=Sourish |editor-last=Yam |editor-first=Philip |date=October 2007 |title=Updates: Into Thin Air |access-date=2008-08-04 |periodical=Scientific American |publisher=Scientific American, Inc. |volume=297 |issue=4 |page=18 |url=http://www.sciamdigital.com/index.cfm?fa=Products.ViewIssuePreview&ARTICLEID_CHAR=E0D18FB2-3048-8A5E-104115527CB01ADB |archive-url=https://web.archive.org/web/20081206032004/http://www.sciamdigital.com/index.cfm?fa=Products.ViewIssuePreview&ARTICLEID_CHAR=E0D18FB2-3048-8A5E-104115527CB01ADB |archive-date=2008-12-06 |url-status=dead }}</ref>

{{as of|2012}}, the [[National Helium Reserve|United States National Helium Reserve]] accounted for 30 percent of the world's helium.<ref name="Newcomb">{{cite magazine|first=Tim|last=Newcomb|url=https://newsfeed.time.com/2012/08/23/theres-a-helium-shortage-on-and-its-affecting-more-than-just-balloons/|title=There's a Helium Shortage On—and It's Affecting More than Just Balloons|magazine=[[Time (magazine)|Time]]|date=21 August 2012|access-date=2013-09-16|archive-url=https://web.archive.org/web/20131229061210/http://newsfeed.time.com/2012/08/23/theres-a-helium-shortage-on-and-its-affecting-more-than-just-balloons/|archive-date=29 December 2013|url-status=live}}</ref> The reserve was expected to run out of helium in 2018.<ref name="Newcomb" /> Despite that, a proposed bill in the [[United States Senate]] would allow the reserve to continue to sell the gas. Other large reserves were in the [[Hugoton Natural Gas Area|Hugoton]] in [[Kansas]], United States, and nearby gas fields of Kansas and the [[panhandles]] of [[Texas]] and [[Oklahoma]]. New helium plants were scheduled to open in 2012 in [[Qatar]], Russia, and the US state of [[Wyoming]], but they were not expected to ease the shortage.<ref name="Newcomb" />

In 2013, Qatar started up the world's largest helium unit,<ref>{{cite web |url=http://www.airliquide.com/en/qatar-start-up-of-worlds-largest-helium-unit.html |title=Air Liquide {{pipe}} the world leader in gases, technologies and services for Industry and Health |access-date=2015-05-25 |url-status=dead |archive-url=https://web.archive.org/web/20140914141342/http://www.airliquide.com/en/qatar-start-up-of-worlds-largest-helium-unit.html |archive-date=2014-09-14 |date=19 February 2015 }} Air Liquide Press Release.</ref> although the [[2017 Qatar diplomatic crisis]] severely affected helium production there.<ref>{{Cite news|url=https://www.washingtonpost.com/news/wonk/wp/2017/06/26/middle-east-turmoil-is-disrupting-a-vital-resource-for-nuclear-energy-space-flight-and-birthday-balloons|title=Middle East turmoil is disrupting a vital resource for nuclear energy, space flight and birthday balloons|date=26 June 2017|work=washingtonpost.com|access-date=26 June 2017|archive-url=https://web.archive.org/web/20170626211653/https://www.washingtonpost.com/news/wonk/wp/2017/06/26/middle-east-turmoil-is-disrupting-a-vital-resource-for-nuclear-energy-space-flight-and-birthday-balloons/|archive-date=26 June 2017|url-status=live}}</ref> 2014 was widely acknowledged to be a year of over-supply in the helium business, following years of renowned shortages.<ref>{{cite web |url=http://www.gasworld.com/2015-what-lies-ahead-part-1/2004706.article |url-status=live |archive-url=https://web.archive.org/web/20150117012529/http://www.gasworld.com/2015-what-lies-ahead-part-1/2004706.article |archive-date=2015-01-17 |work=Gasworld |date=25 December 2014 |title=2015 – What lies ahead? Part 1 |last=Cockerill |first=Rob |access-date=15 September 2021}}</ref> Nasdaq reported (2015) that for [[Air Products]], an international corporation that sells gases for industrial use, helium volumes remain under economic pressure due to feedstock supply constraints.<ref>{{Cite web|url=https://www.nasdaq.com/article/will-air-products-apd-earnings-surprise-estimates-in-q2-analyst-blog-cm470472|title=Will Air Products' (APD) Earnings Surprise Estimates in Q2? - Analyst Blog|date=April 28, 2015|website=NASDAQ.com|access-date=August 4, 2019|archive-url=https://web.archive.org/web/20190715085145/https://www.nasdaq.com/article/will-air-products-apd-earnings-surprise-estimates-in-q2-analyst-blog-cm470472|archive-date=July 15, 2019|url-status=live}}</ref>

==Characteristics==

===Atom===
{{Main|Helium atom}}
[[File:Helium atom QM.svg|thumb|right|alt=Picture of a diffuse gray sphere with grayscale density decreasing from the center. Length scale about 1 Angstrom. An inset outlines the structure of the core, with two red and two blue atoms at the length scale of 1 femtometer.|'''The helium atom.''' Depicted are the [[atomic nucleus|nucleus]] (pink) and the [[electron cloud]] distribution (black). The nucleus (upper right) in helium-4 is in reality spherically symmetric and closely resembles the electron cloud, although for more complicated nuclei this is not always the case.]]

====In quantum mechanics====
In the perspective of [[quantum mechanics]], helium is the second simplest [[atom]] to model, following the [[hydrogen atom]]. Helium is composed of two electrons in [[atomic orbital]]s surrounding a nucleus containing two protons and (usually) two neutrons. As in Newtonian mechanics, no system that consists of more than two particles can be solved with an exact analytical mathematical approach (see [[3-body problem]]) and helium is no exception. Thus, numerical mathematical methods are required, even to solve the system of one nucleus and two electrons. Such [[computational chemistry]] methods have been used to create a quantum mechanical picture of helium electron binding which is accurate to within < 2% of the correct value, in a few computational steps.<ref>{{Cite news|url=http://www.sjsu.edu/faculty/watkins/helium.htm|last=Watkins|first=Thayer|publisher=San Jose State University|title=The Old Quantum Physics of Niels Bohr and the Spectrum of Helium: A Modified Version of the Bohr Model|access-date=2009-06-24|archive-url=https://web.archive.org/web/20090526074018/http://www.sjsu.edu/faculty/watkins/helium.htm|archive-date=2009-05-26|url-status=live}}</ref> Such models show that each electron in helium partly screens the nucleus from the other, so that the [[effective nuclear charge]] ''Z''<sub>eff</sub> which each electron sees is about 1.69 units, not the 2 charges of a classic "bare" helium nucleus.

====Related stability of the helium-4 nucleus and electron shell====
The nucleus of the helium-4 atom is identical with an [[alpha particle]]. High-energy electron-scattering experiments show its charge to decrease exponentially from a maximum at a central point, exactly as does the charge density of helium's own [[electron cloud]]. This symmetry reflects similar underlying physics: the pair of neutrons and the pair of protons in helium's nucleus obey the same quantum mechanical rules as do helium's pair of electrons (although the nuclear particles are subject to a different nuclear binding potential), so that all these [[fermion]]s fully occupy 1s orbitals in pairs, none of them possessing orbital angular momentum, and each cancelling the other's intrinsic spin. This arrangement is thus energetically extremely stable for all these particles and has [[nuclear astrophysics|astrophysical]] implications.<ref name=Parker2022>{{cite journal |first1=M. C. |last1=Parker |first2=C. |last2=Jeynes |first3=W. N. |last3=Catford |title=Halo Properties in Helium Nuclei from the Perspective of Geometrical Thermodynamics |journal=Annalen der Physik |date=2022 |volume=534 |number=2100278 |article-number=2100278 |doi=10.1002/andp.202100278 |doi-access=free|bibcode=2022AnP...53400278P }}</ref> Namely, adding another particle – proton, neutron, or alpha particle – would consume rather than release energy; all systems with [[mass number]] 5, as well as [[beryllium-8]] (comprising two alpha particles), are unbound.<ref name=8gap>{{cite journal |last1=Coc |first1=A. |last2=Vangioni |first2=E. |title=The triple-alpha reaction and the ''A''&nbsp;=&nbsp;8 gap in BBN and Population III stars |journal=Memorie della Società Astronomica Italiana |volume=85 |pages=124–129 |date=2014 |bibcode=2014MmSAI..85..124C |url=http://inspirehep.net/record/1338211/files/2014MmSAI..85..124C.pdf?version=1}}</ref>

For example, the stability and low energy of the electron cloud state in helium accounts for the element's chemical inertness, and also the lack of interaction of helium atoms with each other, producing the lowest melting and boiling points of all the elements. In a similar way, the particular energetic stability of the helium-4 nucleus, produced by similar effects, accounts for the ease of helium-4 production in atomic reactions that involve either heavy-particle emission or fusion. Some stable helium-3 (two protons and one neutron) is produced in fusion reactions from hydrogen, though its estimated abundance in the universe is about {{val|e=-5}} relative to helium-4.<ref name=Pitrou18/>

[[File:Binding energy curve - common isotopes.svg|thumb|right|Binding energy per nucleon of common isotopes. The binding energy per particle of helium-4 is significantly larger than all nearby nuclides.]]
The unusual stability of the helium-4 nucleus is also important [[Cosmology|cosmologically]]: it explains the fact that in the first few minutes after the [[Big Bang]], as the "soup" of free protons and neutrons which had initially been created in about 6:1 ratio cooled to the point that nuclear binding was possible, almost all first compound atomic nuclei to form were helium-4 nuclei. Owing to the relatively tight binding of helium-4 nuclei, its production consumed nearly all of the free neutrons in a few minutes, before they could beta-decay, and thus few neutrons were available to form heavier atoms such as lithium, beryllium, or boron. Helium-4 nuclear binding per nucleon is stronger than in any of these elements (see [[nucleogenesis]] and [[binding energy]]) and thus, once helium had been formed, no energetic drive was available to make elements 3, 4 and 5.<ref name=bbn99>{{cite journal |title=Cosmic lithium-beryllium-boron story |date=1999 |first1=E. |last1=Vangioni-Flam |first2=M. |last2=Cassé |doi=10.1023/A:1002197712862 |journal=Astrophysics and Space Science |volume=265 |issue=1–4 |pages=77–86 |arxiv=astro-ph/9902073|bibcode=1999Ap&SS.265...77V |s2cid=10627727 }}</ref> It is barely energetically favorable for helium to fuse into the next element with a lower energy per [[nucleon]], carbon. However, due to the short lifetime of the intermediate beryllium-8, this process requires three helium nuclei striking each other nearly simultaneously (see [[triple-alpha process]]).<ref name=8gap/> There was thus no time for significant carbon to be formed in the few minutes after the Big Bang, before the early expanding universe cooled to the temperature and pressure point where helium fusion to carbon was no longer possible. This left the early universe with a very similar ratio of hydrogen/helium as is observed today (3 parts hydrogen to 1 part helium-4 by mass), with nearly all the neutrons in the universe trapped in helium-4.

All heavier elements (including those necessary for rocky planets like the Earth, and for carbon-based or other life) have thus been created since the Big Bang in stars which were hot enough to fuse helium itself. All elements other than hydrogen and helium today account for only 2% of the mass of atomic matter in the universe. Helium-4, by contrast, comprises about 24% of the mass of the universe's ordinary matter—nearly all the ordinary matter that is not hydrogen.<ref name=Pitrou18>{{cite journal |title=Precision big bang nucleosynthesis with improved Helium-4 predictions |journal=Physics Reports |volume=754 |date=2018 |pages=1–66 |first1=C. |last1=Pitrou |first2=A. |last2=Coc |first3=J.-P. |last3=Uzan |first4=E. |last4=Vangioni |doi=10.1016/j.physrep.2018.04.005 |doi-access=free|arxiv=1801.08023 |bibcode=2018PhR...754....1P }}</ref><ref name=Hsyu20>{{cite journal |title=The PHLEK Survey: A New Determination of the Primordial Helium Abundance |first1=T. |last1=Hsyu |first2=R. J. |last2=Cooke |first3=J. X. |last3=Prochaska |first4=M. |last4=Bolte |date=2020 |journal=The Astrophysical Journal |volume=896 |number=77 |page=77 |doi=10.3847/1538-4357/ab91af |doi-access=free|arxiv=2005.12290 |bibcode=2020ApJ...896...77H }}</ref>

===Gas and plasma phases===
[[File:HeTube.jpg|thumb|left|upright|Helium discharge tube shaped into 'He', the element's symbol.|alt=Illuminated light red gas discharge tubes shaped as letters H and e]]
Helium is the second least reactive noble gas after [[neon]], and thus the second least reactive of all elements.<ref>{{Cite book
|url=https://books.google.com/books?id=IoFzgBSSCwEC&pg=PA70|title=Modelling Marvels|last=Lewars|first=Errol G. |publisher=Springer|date=2008|isbn=978-1-4020-6972-7|pages=70–71|bibcode=2008moma.book.....L}}</ref> It is [[chemically inert]] and monatomic in all standard conditions. Because of helium's relatively low molar (atomic) mass, its [[thermal conductivity]], [[specific heat]], and [[Speed of sound|sound speed]] in the gas phase are all greater than any other gas except [[hydrogen]]. For these reasons and the small size of helium monatomic molecules, helium [[diffusion|diffuses]] through solids at a rate three times that of air and around 65% that of hydrogen.<ref name="enc" />

Helium is the least water-[[solubility|soluble]] monatomic gas,<ref>{{Cite journal|title = Solubility of helium and neon in water and seawater|last = Weiss|first=Ray F.| date = 1971| journal = J. Chem. Eng. Data|volume = 16|issue = 2|pages = 235–241 |doi = 10.1021/je60049a019}}</ref> and one of the least water-soluble of any gas ([[Tetrafluoromethane|CF<sub>4</sub>]], [[Sulfur hexafluoride|SF<sub>6</sub>]], and [[Octafluorocyclobutane|C<sub>4</sub>F<sub>8</sub>]] have lower mole fraction solubilities: 0.3802, 0.4394, and 0.2372 x<sub>2</sub>/10<sup>−5</sup>, respectively, versus helium's 0.70797 x<sub>2</sub>/10<sup>−5</sup>),<ref>{{Cite journal|title = Solubility of gases in water: Correlation between solubility and the number of water molecules in the first solvation shell |last1 = Scharlin|first1=P. |last2 = Battino|first2=R.|last3=Silla|first3=E. |last4 = Tuñón|first4=I. |last5 = Pascual-Ahuir|first5=J. L.| date = 1998| journal = Pure and Applied Chemistry |volume = 70|issue = 10|pages = 1895–1904 |doi= 10.1351/pac199870101895 |s2cid = 96604119|doi-access = free}}</ref> and helium's [[index of refraction]] is closer to unity than that of any other gas.<ref>{{Cite journal|title = Using helium as a standard of refractive index: correcting errors in a gas refractometer |last1 = Stone|first1=Jack A. |last2 = Stejskal|first2=Alois|date = 2004| journal = Metrologia|volume = 41|issue = 3|pages = 189–197 |doi =10.1088/0026-1394/41/3/012|bibcode = 2004Metro..41..189S | s2cid=250809634 |url=https://www.researchgate.net/publication/231064946}}</ref> Helium has a negative [[Joule–Thomson coefficient]] at normal ambient temperatures, meaning it heats up when allowed to freely expand. Only below its [[Joule–Thomson inversion temperature]] (of about 32 to 50&nbsp;K at 1 atmosphere) does it cool upon free expansion.<ref name="enc" /> Once precooled below this temperature, helium can be liquefied through expansion cooling.

Most extraterrestrial helium is [[plasma (physics)|plasma]] in stars, with properties quite different from those of atomic helium. In a plasma, helium's electrons are not bound to its nucleus, resulting in very high electrical conductivity, even when the gas is only partially ionized. The charged particles are highly influenced by magnetic and electric fields. For example, in the [[solar wind]] together with ionized hydrogen, the particles interact with the Earth's [[magnetosphere]], giving rise to [[Birkeland current]]s and the [[aurora]].<ref>{{Cite journal|title = Helium isotopes in an aurora|last1 = Buhler|first1=F.|last2 = Axford|first2=W. I.|last3 = Chivers|first3=H. J. A.|last4 = Martin|first4=K.| date = 1976|journal = J. Geophys. Res.|volume = 81|issue = 1|pages = 111–115|doi = 10.1029/JA081i001p00111|bibcode=1976JGR....81..111B}}</ref>

===Liquid phase===
{{Main|Liquid helium}}
[[File:Phase diagram of Helium-4-en.svg|thumb|upright=1.25|Phase diagram of helium-4. (Atmospheric pressure is about 0.1 MPa)]]
[[File:2 Helium.png|thumb|Liquefied helium. This helium is not only liquid, but has been cooled to the point of [[superfluid]]ity. The drop of liquid at the bottom of the glass represents helium spontaneously escaping from the container over the side, to empty out of the container. The energy to drive this process is supplied by the potential energy of the falling helium.]]

Helium liquifies when cooled below 4.2&nbsp;K at atmospheric pressure. Unlike any other element, however, helium remains liquid down to a temperature of [[absolute zero]]. This is a direct effect of quantum mechanics: specifically, the [[zero point energy]] of the system is too high to allow freezing. Pressures above about 25 atmospheres are required to freeze it. There are two liquid phases: Helium I is a conventional liquid, and Helium II, which occurs at a lower temperature, is a [[superfluid]].

====Helium I====
Below its [[boiling point]] of {{convert|4.22|K|C F}} and above the [[lambda point]] of {{convert|2.1768|K|C F}}, the [[isotope]] helium-4 exists in a normal colorless liquid state, called ''helium&nbsp;I''.<ref name="enc" /> Like other [[cryogenic]] liquids, helium&nbsp;I boils when it is heated and contracts when its temperature is lowered. Below the lambda point, however, helium does not boil, and it expands as the temperature is lowered further. <!-- clarifyme / The rate of expansion decreases below the lambda point until about 1&nbsp;K is reached; at which point expansion completely stops and helium&nbsp;I starts to contract again. / if it is below the lambda point, should not it be helium II?-->

Helium&nbsp;I has a gas-like [[index of refraction]] of 1.026 which makes its surface so hard to see that floats of [[Expanded polystyrene|Styrofoam]] are often used to show where the surface is.<ref name="enc" /> This colorless liquid has a very low [[viscosity]] and a density of 0.145–0.125 g/mL (between about 0 and 4 K),<ref name="crc6120">{{RubberBible86th|page=6–120}}</ref> which is only one-fourth the value expected from [[classical physics]].<ref name="enc" /> [[Quantum mechanics]] is needed to explain this property and thus both states of liquid helium (helium I and helium II) are called ''quantum fluids'', meaning they display atomic properties on a macroscopic scale. This may be an effect of its boiling point being so close to absolute zero, preventing random molecular motion ([[thermal energy]]) from masking the atomic properties.<ref name="enc" />

====Helium II====
{{main|Superfluid helium-4}}
Liquid helium below its lambda point (called ''helium&nbsp;II'') exhibits very unusual characteristics. Due to its high [[thermal conductivity]], when it boils, it does not bubble but rather evaporates directly from its surface. [[Helium-3]] also has a [[superfluid]] phase, but only at much lower temperatures; as a result, less is known about the properties of the isotope.<ref name="enc" />
[[File:helium-II-creep.svg|thumb|upright|Unlike ordinary liquids, helium&nbsp;II will creep along surfaces in order to reach an equal level; after a short while, the levels in the two containers will equalize. The [[Rollin film]] also covers the interior of the larger container; if it were not sealed, the helium&nbsp;II would creep out and escape.<ref name="enc" />|alt=A cross-sectional drawing showing one vessel inside another. There is a liquid in the outer vessel, and it tends to flow into the inner vessel over its walls.]]

Helium&nbsp;II is a superfluid, a [[Macroscopic quantum phenomena|quantum mechanical state]] of matter with strange properties. For example, when it flows through capillaries as thin as 10 to 100 [[Nanometre|nm]] it has no measurable [[viscosity]].<ref name="nbb" /> However, when measurements were done between two moving discs, a viscosity comparable to that of gaseous helium was observed. Existing theory explains this using the ''two-fluid model'' for helium II. In this model, liquid helium below the lambda point is viewed as containing a proportion of helium atoms in a [[ground state]], which are superfluid and flow with exactly zero viscosity, and a proportion of helium atoms in an excited state, which behave more like an ordinary fluid.<ref>{{Cite journal|doi = 10.1006/aphy.2000.6019 |title = Microscopic Theory of Superfluid Helium |journal = Annals of Physics |volume = 281 |issue = 1–2 |date = 2000|pages = 636–705 12091211 |author = Hohenberg, P. C. |author2 = Martin, P. C.|bibcode = 2000AnPhy.281..636H }}</ref>

In the ''fountain effect'', a chamber is constructed which is connected to a reservoir of helium&nbsp;II by a [[sintering|sintered]] disc through which superfluid helium leaks easily but through which non-superfluid helium cannot pass. If the interior of the container is heated, the superfluid helium changes to non-superfluid helium. In order to maintain the equilibrium fraction of superfluid helium, superfluid helium leaks through and increases the pressure, causing liquid to fountain out of the container.<ref>{{cite web|last=Warner|first=Brent|url=http://cryowwwebber.gsfc.nasa.gov/introduction/liquid_helium.html |title=Introduction to Liquid Helium |publisher=NASA|access-date=2007-01-05 |url-status=dead|archive-url=https://web.archive.org/web/20050901062951/http://cryowwwebber.gsfc.nasa.gov/introduction/liquid_helium.html |archive-date=2005-09-01}}</ref>

The thermal conductivity of helium&nbsp;II is greater than that of any other known substance, a million times that of helium&nbsp;I and several hundred times that of [[copper]].<ref name="enc" /> This is because heat conduction occurs by an exceptional quantum mechanism. Most materials that conduct heat well have a [[valence band]] of free electrons which serve to transfer the heat. Helium&nbsp;II has no such valence band but nevertheless conducts heat well. The [[heat transfer|flow of heat]] is governed by equations that are similar to the [[wave equation]] used to characterize sound propagation in air. When heat is introduced, it moves at 20 meters per second at 1.8&nbsp;K through helium&nbsp;II as waves in a phenomenon known as ''[[second sound]]''.<ref name="enc" />

Helium&nbsp;II also exhibits a creeping effect. When a surface extends past the level of helium&nbsp;II, the helium&nbsp;II moves along the surface, against the force of [[gravity]]. Helium&nbsp;II will escape from a vessel that is not sealed by creeping along the sides until it reaches a warmer region where it evaporates. It moves in a 30&nbsp;nm-thick film regardless of surface material. This film is called a [[Rollin film]] and is named after the man who first characterized this trait, [[Bernard V. Rollin]].<ref name="enc" /><ref>{{Cite journal|doi = 10.1103/PhysRev.76.1209 |title = Rollin Film Rates in Liquid Helium |journal = Physical Review |volume = 76 |issue = 8 |pages = 1209–1211|date = 1949 |author = Fairbank, H. A. |author2 = Lane, C. T. |bibcode=1949PhRv...76.1209F}}</ref><ref>{{Cite journal|doi = 10.1016/S0031-8914(39)80013-1 |title = On the 'film' phenomenon of liquid helium II |journal = Physica |volume = 6 |issue = 2 |date = 1939 |pages = 219–230 |author = Rollin, B. V. |author2 = Simon, F. |bibcode=1939Phy.....6..219R}}</ref> As a result of this creeping behavior and helium&nbsp;II's ability to leak rapidly through tiny openings, it is very difficult to confine. Unless the container is carefully constructed, the helium&nbsp;II will creep along the surfaces and through valves until it reaches somewhere warmer, where it will evaporate. Waves propagating across a Rollin film are governed by the same equation as [[gravity wave]]s in shallow water, but rather than gravity, the restoring force is the [[van der Waals force]].<ref>{{cite web |author = Ellis, Fred M. |url = http://fellis.web.wesleyan.edu/research/thrdsnd.html |title = Third sound |publisher = Wesleyan Quantum Fluids Laboratory |date = 2005 |access-date = 2008-07-23 |archive-url = https://web.archive.org/web/20070621202145/http://fellis.web.wesleyan.edu/research/thrdsnd.html |archive-date = 2007-06-21 |url-status = live }}</ref> These waves are known as ''[[third sound]]''.<ref>{{Cite journal|doi = 10.1103/PhysRev.188.370 |title = Hydrodynamics and Third Sound in Thin He II Films |journal = Physical Review |volume = 188 |issue = 1|date = 1949 |pages = 370–384|author = Bergman, D.|bibcode = 1969PhRv..188..370B }}</ref><!-- "van", see cite itself and [[Talk:Van der Waals#Van should be capitalized unless preceded by first name]] rebuttal -->

===Solid phases===
Helium remains liquid down to [[absolute zero]] at atmospheric pressure, but it freezes at high pressure. Solid helium requires a temperature of 1–1.5&nbsp;K (about −272&nbsp;°C or −457&nbsp;°F) at about 25 bar (2.5&nbsp;MPa) of pressure.<ref>{{cite web|date = 2005-10-05 |url = http://www.phys.ualberta.ca/~therman/lowtemp/projects1.htm |title = Solid Helium |publisher = Department of Physics [[University of Alberta]]|access-date=2008-07-20| archive-url = https://web.archive.org/web/20080531145546/http://www.phys.ualberta.ca/~therman/lowtemp/projects1.htm| archive-date = May 31, 2008}}</ref> It is often hard to distinguish solid from liquid helium since the [[refractive index]] of the two phases are nearly the same. The solid has a sharp [[melting point]] and has a [[crystal]]line structure, but it is highly [[Compressibility|compressible]]; applying pressure in a laboratory can decrease its volume by more than 30%.<ref name="LANL.gov">{{RubberBible86th}}</ref> With a [[bulk modulus]] of about 27 [[megapascal|MPa]]<ref>{{Cite journal|author = Grilly, E. R.|title = Pressure-volume-temperature relations in liquid and solid 4He |journal = Journal of Low Temperature Physics|volume = 11 |issue = 1–2 |pages = 33–52 |doi = 10.1007/BF00655035|date = 1973|bibcode = 1973JLTP...11...33G|s2cid = 189850188 }}</ref> it is ~100 times more compressible than water. Solid helium has a density of {{val|0.214|0.006|u=g/cm<sup>3</sup>}} at 1.15&nbsp;K and 66&nbsp;atm; the projected density at 0&nbsp;K and 25 bar (2.5 MPa) is {{val|0.187|0.009|u=g/cm<sup>3</sup>}}.<ref>{{Cite journal|author = Henshaw, D. B. |title = Structure of Solid Helium by Neutron Diffraction |journal = Physical Review Letters |volume = 109 |issue = 2 |pages = 328–330 |doi = 10.1103/PhysRev.109.328 |date = 1958|bibcode = 1958PhRv..109..328H }}</ref> At higher temperatures, helium will solidify with sufficient pressure. At room temperature, this requires about 114,000 atm.<ref name="Pinceaux1979">{{cite journal |last1=Pinceaux |first1=J.-P. |last2=Maury |first2=J.-P. |last3=Besson |first3=J.-M. |title=Solidification of helium, at room temperature under high pressure |journal=Journal de Physique Lettres |date=1979 |volume=40 |issue=13 |pages=307–308 |doi=10.1051/jphyslet:019790040013030700|s2cid=40164915 |url=https://hal.archives-ouvertes.fr/jpa-00231630/file/ajp-jphyslet_1979_40_13_307_0.pdf }}</ref>

Helium-4 and helium-3 both form several crystalline solid phases, all requiring at least 25&nbsp;bar. They both form an α phase, which has a [[Hexagonal crystal family#Hexagonal close packed|hexagonal close-packed]] (hcp) crystal structure, a β phase, which is [[Cubic crystal system|face-centered cubic]] (fcc), and a γ phase, which is [[Cubic crystal system|body-centered cubic]] (bcc).<ref name="Keller 1969">{{cite book | last=Keller | first=William E. | chapter=Compressed He3 and He4 | title=Helium-3 and Helium-4 | publisher=Springer US | publication-place=Boston, MA | year=1969 | isbn=978-1-4899-6232-4 | doi=10.1007/978-1-4899-6485-4_9 | pages=347–404}}</ref>

===Isotopes===
{{Main|Isotopes of helium}}
There are nine known [[isotope]]s of helium of which two, [[helium-3]] and [[helium-4]], are [[stable isotope|stable]]. In the Earth's atmosphere, one atom is {{chem|3|He}} for every million that are {{chem|4|He}}.<ref name="nbb">{{Cite book| author = Emsley, John| title = Nature's Building Blocks| publisher = Oxford University Press| date = 2001| location = Oxford| pages = 175–179| isbn = 978-0-19-850341-5}}</ref> Unlike most elements, helium's isotopic abundance varies greatly by origin, due to the different formation processes. The most common isotope, helium-4, is produced on Earth by [[alpha decay]] of heavier radioactive elements; the alpha particles that emerge are fully ionized helium-4 nuclei. Helium-4 is an unusually stable nucleus because its [[nucleon]]s are arranged into [[Nuclear shell model|complete shells]]. It was also formed in enormous quantities during [[Big Bang nucleosynthesis]].<ref name="bigbang" />

Helium-3 is present on Earth only in trace amounts. Most of it has been present since Earth's formation, though some falls to Earth trapped in [[cosmic dust]].<ref name="heliumfundamentals">{{cite web |url = http://www.mantleplumes.org/HeliumFundamentals.html |title = Helium Fundamentals |author = Anderson, Don L. |author2 = Foulger, G. R. |author3 = Meibom, A. |date = 2006-09-02 |access-date = 2008-07-20 |publisher = MantlePlumes.org |archive-url = https://web.archive.org/web/20070208194933/http://www.mantleplumes.org/HeliumFundamentals.html |archive-date = 2007-02-08 |url-status = live }}</ref> Trace amounts are also produced by the [[beta decay]] of [[tritium]].<ref>{{Cite journal|title= Half-Life of Tritium| journal=Physical Review|volume= 72|issue= 10|date= 1947| pages= 972|last= Novick|first=Aaron| doi=10.1103/PhysRev.72.972.2|bibcode = 1947PhRv...72..972N }}</ref> Rocks from the Earth's crust have isotope ratios varying by as much as a factor of ten, and these ratios can be used to investigate the origin of rocks and the composition of the Earth's [[Mantle (geology)|mantle]].<ref name="heliumfundamentals" /> {{chem|3|He}} is much more abundant in stars as a product of nuclear fusion. Thus in the [[interstellar medium]], the proportion of {{chem|3|He}} to {{chem|4|He}} is about 100 times higher than on Earth.<ref>{{Cite journal|title=Isotopic Composition and Abundance of Interstellar Neutral Helium Based on Direct Measurements| journal=Astrophysics| volume=45| issue=2|date=2002| pages=131–142| last1=Zastenker | first1=G. N. | doi=10.1023/A:1016057812964|bibcode = 2002Ap.....45..131Z|last2=Salerno | first2=E. | last3=Buehler |first3=F.|last4=Bochsler | first4=P.|last5=Bassi | first5=M. |last6=Agafonov | first6=Yu. N. |last7=Eisomont| first7=N. A. |last8=Khrapchenkov | first8=V. V. | last9=Busemann | first9=H.| s2cid=116957905| display-authors = 8 }}</ref> Extraplanetary material, such as [[Moon|lunar]] and [[asteroid]] [[regolith]], have trace amounts of helium-3 from being bombarded by [[solar wind]]s. The [[Moon]]'s surface contains helium-3 at concentrations on the order of 10 [[Parts per billion|ppb]], much higher than the approximately 5 [[Parts per trillion|ppt]] found in the Earth's atmosphere.<ref>{{cite web|url = http://fti.neep.wisc.edu/research/he3|title = Lunar Mining of Helium-3|date = 2007-10-19|access-date = 2008-07-09|publisher = Fusion Technology Institute of the University of Wisconsin-Madison|archive-url = https://web.archive.org/web/20100609234057/http://fti.neep.wisc.edu/research/he3|archive-date = 2010-06-09|url-status = live}}</ref><ref>{{cite journal|url= http://www.lpi.usra.edu/meetings/lpsc2007/pdf/2175.pdf|title= The estimation of helium-3 probable reserves in lunar regolith|author= Slyuta, E. N.|author2= Abdrakhimov, A. M.|author3= Galimov, E. M.|journal= Lunar and Planetary Science Conference|issue= 1338|pages= 2175|date= 2007|access-date= 2008-07-20|bibcode= 2007LPI....38.2175S|archive-url= https://web.archive.org/web/20080705122316/http://www.lpi.usra.edu/meetings/lpsc2007/pdf/2175.pdf|archive-date= 2008-07-05|url-status= live}}</ref> A number of people, starting with Gerald Kulcinski in 1986,<ref>{{Cite news|url = http://www.thespacereview.com/article/536/1|title = A fascinating hour with Gerald Kulcinski|author = Hedman, Eric R.|date = 2006-01-16|work = The Space Review|access-date = 2008-07-20|archive-url = https://web.archive.org/web/20110109082500/http://thespacereview.com/article/536/1|archive-date = 2011-01-09|url-status = dead}}</ref> have proposed to explore the Moon, mine lunar regolith, and use the helium-3 for [[Nuclear fusion|fusion]].

Liquid helium-4 can be cooled to about {{convert|1|K|C F}} using [[evaporative cooling]] in a [[1-K pot]]. Similar cooling of helium-3, which has a lower boiling point, can achieve about {{val|0.2|u=kelvin}} in a [[Helium-3#Cryogenics|helium-3 refrigerator]]. Equal mixtures of liquid {{chem|3|He}} and {{chem|4|He}} below {{val|0.8|u=K}} separate into two immiscible phases due to their dissimilarity (they follow different [[quantum statistics]]: helium-4 atoms are [[boson]]s while helium-3 atoms are [[fermion]]s).<ref name = enc/> [[Dilution refrigerator]]s use this immiscibility to achieve temperatures of a few millikelvins.<ref>{{Cite journal | doi = 10.1016/j.cryogenics.2021.103390|issn=0011-2275| title = Development of Dilution refrigerators – A review | journal = Cryogenics| volume = 121| year = 2022| last1 = Zu | first1 = H.| last2 = Dai | first2 = W.| last3 = de Waele | first3 = A.T.A.M.|s2cid=244005391}}</ref>

It is possible to produce [[exotic helium isotopes]], which rapidly decay into other substances. The shortest-lived heavy helium isotope is the [[nuclear drip line|unbound]] helium-10 with a [[half-life]] of {{val|2.6|(4)|e=-22|u=s}}.{{NUBASE2020|ref}} Helium-6 decays by emitting a [[beta particle]] and has a half-life of 0.8 second. Helium-7 and helium-8 are created in certain [[nuclear reaction]]s.<ref name="enc" /> Helium-6 and helium-8 are known to exhibit a [[nuclear halo]].<ref name = enc/>

=== Properties ===
Table of thermal and physical properties of helium gas at atmospheric pressure:<ref>{{Cite book |last=Holman |first=Jack P. |title=Heat Transfer |publisher=McGraw-Hill Companies, Inc. |year=2002 |isbn=9780072406559 |edition=9th |location=New York, NY |pages=600–606 |language=English}}</ref><ref>{{Cite book |last1=Incropera |last2=Dewitt |last3=Bergman |last4=Lavigne |first1=Frank P. |first2=David P. |first3=Theodore L. |first4=Adrienne S. |title=Fundamentals of Heat and Mass Transfer |publisher=John Wiley and Sons, Inc. |year=2007 |isbn=9780471457282 |edition=6th |location=Hoboken, NJ |pages=941–950 |language=English }}</ref>
{|class="wikitable mw-collapsible mw-collapsed"
|[[Temperature]] (K)
|[[Density]] (kg/m^3)
|[[Specific heat]] (kJ/kg °C)
|[[Dynamic viscosity]] (kg/m s)
|[[Kinematic viscosity]] (m^2/s)
|[[Thermal conductivity]] (W/m °C)
|[[Thermal diffusivity]] (m^2/s)
|[[Prandtl number]]
|-
|100
| 
|5.193
|9.63E-06
|1.98E-05
|0.073
|2.89E-05
|0.686
|-
|120
|0.406
|5.193
|1.07E-05
|2.64E-05
|0.0819
|3.88E-05
|0.679
|-
|144
|0.3379
|5.193
|1.26E-05
|3.71E-05
|0.0928
|5.28E-05
|0.7
|-
|200
|0.2435
|5.193
|1.57E-05
|6.44E-05
|0.1177
|9.29E-05
|0.69
|-
|255
|0.1906
|5.193
|1.82E-05
|9.55E-05
|0.1357
|1.37E-04
|0.7
|-
|366
|0.1328
|5.193
|2.31E-05
|1.74E-04
|0.1691
|2.45E-04
|0.71
|-
|477
|0.10204
|5.193
|2.75E-05
|2.69E-04
|0.197
|3.72E-04
|0.72
|-
|589
|0.08282
|5.193
|3.11E-05
|3.76E-04
|0.225
|5.22E-04
|0.72
|-
|700
|0.07032
|5.193
|3.48E-05
|4.94E-04
|0.251
|6.66E-04
|0.72
|-
|800
|0.06023
|5.193
|3.82E-05
|6.34E-04
|0.275
|8.77E-04
|0.72
|-
|900
|0.05451
|5.193
|4.14E-05
|7.59E-04
|0.33
|1.14E-03
|0.687
|-
|1000
| 
|5.193
|4.46E-05
|9.14E-04
|0.354
|1.40E-03
|0.654
|}

==Compounds==
{{main|Helium compounds}}
[[File:Helium-hydride-cation-3D-SF.png|thumb|Structure of the [[helium hydride ion]],<ref>{{Cite journal |last=Evett |first=Arthur A. |date=January 1, 1956 |title=Ground State of the Helium-Hydride Ion |url=https://doi.org/10.1063/1.1700818 |journal=The Journal of Chemical Physics |volume=24 |issue=1 |pages=150–152 |doi=10.1063/1.1700818 |bibcode=1956JChPh..24..150E |issn=0021-9606|url-access=subscription }}</ref> HeH<sup>+</sup>]]
[[File:Fluoroheliate-ion-3D-vdW.png|thumb|Structure of the suspected fluoroheliate anion, OHeF<sup>−</sup>]]
Helium has a [[Valence (chemistry)|valence]] of zero and is chemically unreactive under all normal conditions.<ref name="LANL.gov" /> It is an electrical insulator unless [[ion]]ized. As with the other noble gases, helium has metastable [[energy level]]s that allow it to remain ionized in an electrical discharge with a [[voltage]] below its [[ionization potential]].<ref name="enc" /> Helium can form unstable [[compound (chemistry)|compounds]], known as [[excimer]]s, with tungsten, iodine, fluorine, sulfur, and phosphorus when it is subjected to a [[glow discharge]], to electron bombardment, or reduced to [[Plasma physics|plasma]] by other means. The molecular compounds HeNe, HgHe<sub>10</sub>, and WHe<sub>2</sub>, and the molecular ions {{chem|He|2|+}}, {{chem|He|2|2+}}, {{chem|link=Helium hydride ion|HeH|+}}, and {{chem|HeD|+}} have been created this way.<ref>{{Cite journal|title = Massenspektrographische Untersuchungen an Wasserstoff- und Heliumkanalstrahlen ({{chem|H|3|+}}, {{chem|H|2|-}}, {{chem|HeH|+}}, {{chem|HeD|+}}, {{chem|He|-}}) |author = Hiby, Julius W. |journal = [[Annalen der Physik]] |volume = 426 |issue = 5 |pages = 473–487 |date = 1939 |doi = 10.1002/andp.19394260506 |bibcode = 1939AnP...426..473H }}</ref> HeH<sup>+</sup> is also stable in its ground state but is extremely reactive—it is the strongest [[Brønsted–Lowry acid–base theory|Brønsted acid]] known, and therefore can exist only in isolation, as it will protonate any molecule or counteranion it contacts. This technique has also produced the neutral molecule He<sub>2</sub>, which has a large number of [[spectral band|band systems]], and HgHe, which is apparently held together only by polarization forces.<ref name="enc" />

[[Van der Waals compound]]s of helium can also be formed with cryogenic helium gas and atoms of some other substance, such as [[LiHe]] and [[dihelium|He<sub>2</sub>]].<ref name="fr13">{{cite magazine|last1=Friedrich|first1=Bretislav|title=A Fragile Union Between Li and He Atoms|magazine=Physics|date=8 April 2013|volume=6|article-number=42|doi=10.1103/Physics.6.42|bibcode=2013PhyOJ...6...42F|url=https://physics.aps.org/featured-article-pdf/10.1103/PhysRevLett.110.153201|access-date=24 August 2019|archive-url=https://web.archive.org/web/20170829154727/https://physics.aps.org/featured-article-pdf/10.1103/PhysRevLett.110.153201|archive-date=29 August 2017|url-status=live|hdl=11858/00-001M-0000-000E-F3CF-5|hdl-access=free}}</ref>

Theoretically, other true compounds may be possible, such as helium fluorohydride (HHeF), which would be analogous to [[Argon fluorohydride|HArF]], discovered in 2000.<ref>{{Cite journal|title = Prediction of a Metastable Helium Compound: HHeF |author = Wong, Ming Wah|journal = [[Journal of the American Chemical Society]] |volume = 122 |issue = 26 |pages = 6289–6290 |date = 2000 |doi = 10.1021/ja9938175| bibcode=2000JAChS.122.6289W | url=http://scholarbank.nus.edu.sg/handle/10635/77551 }}</ref> Calculations show that two new compounds containing a helium-oxygen bond could be stable.<ref>{{Cite journal|title = On Chemical Bonding Between Helium and Oxygen|first = W.|last = Grochala|journal = Polish Journal of Chemistry|volume = 83|pages = 87–122|date =2009}}</ref> Two new molecular species, predicted using theory, CsFHeO and N(CH<sub>3</sub>)<sub>4</sub>FHeO, are derivatives of a metastable FHeO<sup>−</sup> anion first theorized in 2005 by a group from Taiwan.<ref>{{cite web|url = http://www.uw.edu.pl/en/strony/news/chemist.pdf|archive-url = https://web.archive.org/web/20090319180147/http://www.uw.edu.pl/en/strony/news/chemist.pdf|archive-date = 2009-03-19|title = Collapse of helium's chemical nobility predicted by Polish chemist|access-date = 2009-05-15}}</ref>

Helium atoms have been inserted into the hollow carbon cage molecules (the [[fullerene]]s) by heating under high pressure. The [[endohedral fullerene|endohedral fullerene molecules]] formed are stable at high temperatures. When chemical derivatives of these fullerenes are formed, the helium stays inside.<ref>{{Cite journal|title = Stable Compounds of Helium and Neon: He@C<sub>60</sub> and Ne@C<sub>60</sub> |author = Saunders, Martin |author2 = Jiménez-Vázquez, Hugo A. |author3 = Cross, R. James |author4 = Poreda, Robert J. |journal = Science |volume = 259 |issue = 5100 |pages = 1428–1430 |date = 1993 |doi = 10.1126/science.259.5100.1428 |pmid = 17801275|bibcode = 1993Sci...259.1428S |s2cid = 41794612 }}</ref> If [[helium-3]] is used, it can be readily observed by helium [[nuclear magnetic resonance spectroscopy]].<ref>{{Cite journal|title = Probing the interior of fullerenes by <sup>3</sup>He NMR spectroscopy of endohedral <sup>3</sup>He@C<sub>60</sub> and <sup>3</sup>He@C<sub>70</sub> |last1=Saunders|first1=Martin|journal = Nature |volume = 367|issue = 6460|pages = 256–258 |date = 1994 |doi = 10.1038/367256a0|bibcode = 1994Natur.367..256S|first2 = Hugo A.|last2=Jiménez-Vázquez|first3 = R. James|last3=Cross|first4 = Stanley|last4=Mroczkowski|first5 = Darón I.|last5=Freedberg|first6 = Frank A. L.|last6=Anet|s2cid=4273677}}</ref> Many fullerenes containing helium-3 have been reported. Although the helium atoms are not attached by covalent or ionic bonds, these substances have distinct properties and a definite composition, like all stoichiometric chemical compounds.

Under high pressures helium can form compounds with various other elements. Helium-nitrogen [[clathrate]] (He(N<sub>2</sub>)<sub>11</sub>) crystals have been grown at room temperature at pressures ca. 10 GPa in a [[diamond anvil cell]].<ref>{{cite journal|doi=10.1038/358046a0|title=A high-pressure van der Waals compound in solid nitrogen-helium mixtures|journal=Nature|volume=358|issue=6381|pages=46–48|year=1992|last1=Vos|first1=W. L.|last2=Finger|first2=L. W.|last3=Hemley|first3=R. J.|last4=Hu|first4=J. Z.|last5=Mao|first5=H. K.|last6=Schouten|first6=J. A.|bibcode=1992Natur.358...46V|s2cid=4313676}}</ref> The [[Insulator (electricity)|insulating]] [[electride]] [[Disodium helide|Na<sub>2</sub>He]] has been shown to be thermodynamically stable at pressures above 113 GPa. It has a [[fluorite]] structure.<ref name="DongOganov2017">{{cite journal |last1=Dong|first1=Xiao |last2=Oganov|first2=Artem R. |last3=Goncharov|first3=Alexander F. |last4=Stavrou|first4=Elissaios |last5=Lobanov|first5=Sergey |last6=Saleh|first6=Gabriele |last7=Qian|first7=Guang-Rui |last8=Zhu|first8=Qiang |last9=Gatti|first9=Carlo |last10=Deringer|first10=Volker L. |last11=Dronskowski|first11=Richard |last12=Zhou|first12=Xiang-Feng |last13=Prakapenka|first13=Vitali B. |last14=Konôpková|first14=Zuzana |last15=Popov|first15=Ivan A. |last16=Boldyrev|first16=Alexander I. |last17=Wang|first17=Hui-Tian |title=A stable compound of helium and sodium at high pressure |journal=Nature Chemistry |volume=9 |issue=5 |pages=440–445 |year=2017 |issn=1755-4330 |doi=10.1038/nchem.2716 |pmid=28430195 |bibcode=2017NatCh...9..440D|arxiv=1309.3827 |s2cid=20459726 }}</ref>

==Occurrence and production==

===Natural abundance===
Although it is rare on Earth, helium is the second most abundant element in the known Universe, constituting 23% of its [[baryon]]ic mass. Only hydrogen is more abundant.<ref name="nbb" /> The vast majority of helium was formed by [[Big Bang nucleosynthesis]] one to three minutes after the Big Bang. As such, measurements of its abundance contribute to cosmological models. The first [[molecular bond]]s when formed when primordial helium atoms combined with protons to form helium hydride ions,<ref>{{Cite journal |last1=Güsten |first1=Rolf |last2=Wiesemeyer |first2=Helmut |last3=Neufeld |first3=David |last4=Menten |first4=Karl M. |last5=Graf |first5=Urs U. |last6=Jacobs |first6=Karl |last7=Klein |first7=Bernd |last8=Ricken |first8=Oliver |last9=Risacher |first9=Christophe |last10=Stutzki |first10=Jürgen |date=April 2019 |title=Astrophysical detection of the helium hydride ion HeH+ |url=https://www.nature.com/articles/s41586-019-1090-x |journal=Nature |language=en |volume=568 |issue=7752 |pages=357–359 |doi=10.1038/s41586-019-1090-x |pmid=30996316 |issn=0028-0836|arxiv=1904.09581 }}</ref> HeH<sup>+</sup>.  In [[star]]s, helium is formed by the [[nuclear fusion]] of hydrogen in [[proton–proton chain|proton–proton chain reaction]]s and the [[CNO cycle]], part of [[stellar nucleosynthesis]].<ref name="bigbang">{{cite web|author=Weiss, Achim|title=Elements of the past: Big Bang Nucleosynthesis and observation|url=http://www.einstein-online.info/spotlights/BBN_obs/?set_language=en|publisher=[[Max Planck Institute for Gravitational Physics]]|access-date=2008-06-23|archive-url=https://web.archive.org/web/20100729042805/http://www.einstein-online.info/spotlights/BBN_obs/?set_language=en|archive-date=2010-07-29|url-status=dead}}; {{Cite journal|last1=Coc | first1=Alain | last2=Vangioni-Flam |first2=Elisabeth| last3=Descouvemont |first3=Pierre|last4=Adahchour | first4=Abderrahim|last5= Angulo | first5=Carmen |title=Updated Big Bang Nucleosynthesis confronted to WMAP observations and to the Abundance of Light Elements|journal=[[Astrophysical Journal]]| volume=600 |year=2004|issue=2| pages=544–552 |doi=10.1086/380121|bibcode=2004ApJ...600..544C|arxiv = astro-ph/0309480| s2cid=16276658 }}</ref>

In the [[Earth's atmosphere]], the concentration of helium by volume is only 5.2 parts per million.<ref>{{Cite journal|author=Oliver, B. M.|author2=Bradley, James G.|date=1984 |title= Helium concentration in the Earth's lower atmosphere |journal=Geochimica et Cosmochimica Acta |volume=48 |issue=9 |pages=1759–1767 |doi=10.1016/0016-7037(84)90030-9|bibcode = 1984GeCoA..48.1759O }}</ref><ref>{{cite web|url=http://www.srh.weather.gov/jetstream/atmos/atmos_intro.htm |title=The Atmosphere: Introduction |website=JetStream&nbsp;– Online School for Weather |publisher=[[National Weather Service]] |date = 2007-08-29 |access-date = 2008-07-12|archive-url = https://web.archive.org/web/20080113234621/http://www.srh.weather.gov/jetstream/atmos/atmos_intro.htm |archive-date = January 13, 2008|url-status=dead}}</ref> The concentration is low and fairly constant despite the continuous production of new helium because most helium in the Earth's atmosphere [[atmospheric escape|escapes into space]] by several processes.<ref>{{Cite journal|author=Lie-Svendsen, Ø.|author2=Rees, M. H.|date=1996 |title=Helium escape from the terrestrial atmosphere: The ion outflow mechanism |journal=Journal of Geophysical Research |volume=101 |issue=A2 |pages=2435–2444 |doi=10.1029/95JA02208|bibcode=1996JGR...101.2435L}}</ref><ref>{{cite web|url=http://www.astronomynotes.com/solarsys/s3.htm|title=Atmospheres|website=Nick Strobel's Astronomy Notes|date=2007|access-date=2007-09-25|author=Strobel, Nick|archive-url=https://web.archive.org/web/20100919031142/http://astronomynotes.com//solarsys/s3.htm|archive-date=2010-09-19|url-status=dead}}</ref><ref name="TalkOriginsCreationism">{{cite web|author=G. Brent Dalrymple|title=How Good Are Those Young-Earth Arguments?|url=http://www.talkorigins.org/faqs/dalrymple/creationist_age_earth.html|access-date=2011-02-13|archive-url=https://web.archive.org/web/20110607162749/http://www.talkorigins.org/faqs/dalrymple/creationist_age_earth.html|archive-date=2011-06-07|url-status=live}}</ref> In the Earth's [[heterosphere]], a part of the upper atmosphere, helium and hydrogen are the most abundant elements.

Most helium on Earth is a result of [[radioactive decay]]. Helium is found in large amounts in minerals of [[uranium]] and [[thorium]], such as [[uraninite]] and its varieties [[cleveite]] and pitchblende,<ref name="mindat cleveite"/><ref name="mindat pitchblende">{{cite web |url=https://www.mindat.org/min-3222.html |title=Pitchblende |website=Mindat.org |access-date=14 February 2020}}</ref> as well as [[carnotite]] and [[monazite]] (a group name; "monazite" usually refers to [[monazite-(Ce)]]),<ref name="mindat monazite">{{cite web |url=https://www.mindat.org/min-2750.html |title=Monazite |website=Mindat.org |access-date=14 February 2020}}</ref><ref name="mindat monaziteCe">{{cite web |url=https://www.mindat.org/min-2751.html |title=Monazite-(Ce) |website=Mindat.org |access-date=14 February 2020}}</ref> because they emit alpha particles (helium nuclei, He<sup>2+</sup>) to which electrons immediately combine as soon as the particle is stopped by the rock. In this way an estimated 3000 metric tons of helium are generated per year throughout the [[lithosphere]].<ref name="cook">{{Cite journal|author=Cook, Melvine A. |date=1957 |title=Where is the Earth's Radiogenic Helium? |journal= Nature |volume=179|issue=4552 |page=213 |doi=10.1038/179213a0|bibcode = 1957Natur.179..213C |s2cid=4297697 |doi-access=free }}</ref><ref>{{Cite journal|author= Aldrich, L. T.|author2= Nier, Alfred O.|date=1948 |title=The Occurrence of He<sup>3</sup> in Natural Sources of Helium |journal = Phys. Rev. |volume=74|issue= 11 |pages= 1590–1594 |doi=10.1103/PhysRev.74.1590|bibcode = 1948PhRv...74.1590A }}</ref><ref>{{Cite journal|author=Morrison, P.|author2=Pine, J.|date=1955 |title= Radiogenic Origin of the Helium Isotopes in Rock |journal = Annals of the New York Academy of Sciences |volume=62 |issue=3 |pages=71–92 |doi=10.1111/j.1749-6632.1955.tb35366.x|bibcode = 1955NYASA..62...71M |s2cid=85015694}}</ref> In the Earth's crust, the concentration of helium is 8 parts per billion. In seawater, the concentration is only 4 parts per trillion. There are also small amounts in mineral [[spring (hydrosphere)|springs]], volcanic gas, and [[meteoric iron]]. Because helium is trapped in the subsurface under conditions that also trap natural gas, the greatest natural concentrations of helium on the planet are found in natural gas, from which most commercial helium is extracted. The concentration varies in a broad range from a few ppm to more than 7% in a small gas field in [[San Juan County, New Mexico]].<ref>{{Cite journal |author=Zartman, R. E. |date=1961 |title=Helium Argon and Carbon in Natural Gases |journal=Journal of Geophysical Research |volume=66 |issue=1 |pages=277–306 |doi=10.1029/JZ066i001p00277 |last2=Wasserburg |first2=G. J. |last3=Reynolds |first3=J. H. |bibcode=1961JGR....66..277Z |url=https://authors.library.caltech.edu/51508/1/jgr2272.pdf |access-date=2019-01-29 |archive-url=https://web.archive.org/web/20170809221530/http://authors.library.caltech.edu/51508/1/jgr2272.pdf |archive-date=2017-08-09 |url-status=live }}</ref><ref>{{Cite journal|last=Broadhead|first=Ronald F. |date=2005 |title= Helium in New Mexico—geology distribution resource demand and exploration possibilities |journal = New Mexico Geology |volume=27 |issue=4 |pages=93–101 |article-number=119744 |doi=10.58799/NMG-v27n4.93 |doi-broken-date=9 September 2025 |s2cid=29360086 |url=http://geoinfo.nmt.edu/publications/periodicals/nmg/downloads/27/n4/nmg_v27_n4_p93.pdf |url-status=dead|archive-url=https://web.archive.org/web/20120330094105/http://geoinfo.nmt.edu/publications/periodicals/nmg/downloads/27/n4/nmg_v27_n4_p93.pdf|archive-date=2012-03-30|access-date=2008-07-21}}</ref>

{{as of|2021}}, the world's helium reserves were estimated at 31 billion cubic meters, with a third of that being in [[Qatar]].<ref>{{cite web|url=https://pubs.usgs.gov/periodicals/mcs2021/mcs2021-helium.pdf|title=Helium|work=Mineral Commodity Summaries|publisher=U.S. geological survey|date=January 2021|access-date=12 February 2022}}</ref> In 2015 and 2016 additional probable reserves were announced to be under the Rocky Mountains in North America<ref>{{cite web|title=Press release: The unbearable lightness of helium...|url=http://www.eag.eu.com/about/media/lightness-of-helium/|website=European Association of Geochemistry|access-date=5 March 2017|archive-url=https://web.archive.org/web/20150906100157/http://www.eag.eu.com/about/media/lightness-of-helium/|archive-date=2015-09-06|url-status=dead}}</ref> and in the [[East African Rift]].<ref name="Sample" />

The [[Bureau of Land Management]] (BLM) has proposed an October 2024 plan for managing natural resources in western Colorado. The plan involves closing 543,000 acres to oil and gas leasing while keeping 692,300 acres open. Among the open areas, 165,700 acres have been identified as suitable for helium recovery. The United States possesses an estimated 306 billion cubic feet of recoverable helium, sufficient to meet current consumption rates of 2.15 billion cubic feet per year for approximately 150 years.<ref>{{cite web | last=Rom | first=Zoë | title=How a dwindling helium supply is impacting public land management | website=High Country News | date=2024-11-18 | url=https://www.hcn.org/articles/how-a-dwindling-helium-supply-is-impacting-public-land-management/ | access-date=2024-11-24}}</ref>

===Modern extraction and distribution===
{{see also|Helium production in the United States}}
Extracting helium from air is not economical.<ref>{{Cite book |url=http://www.nap.edu/openbook.php?record_id=9860&page=40 |title=The Impact of Selling the Federal Helium Reserve |date=2000-05-18 |publisher=National Academies Press |isbn=978-0-309-07038-6 |location=Washington, D.C. |doi=10.17226/9860 |bibcode=2000nap..book.9860N |access-date=2025-08-09 |archive-url=https://web.archive.org/web/20140529150642/http://www.nap.edu/openbook.php?record_id=9860&page=40  |archive-date=2014-05-29}}</ref> 
For large-scale use, helium is extracted by [[fractional distillation]] from natural gas, which can contain as much as 7% helium.<ref>{{cite web| author = Winter, Mark| title = Helium: the essentials| publisher = University of Sheffield| date = 2008| url = http://www.webelements.com/helium/| access-date = 2008-07-14| archive-url = https://web.archive.org/web/20080714102813/http://www.webelements.com/helium/| archive-date = 2008-07-14| url-status = live}}</ref> Since helium has a lower [[boiling point]] than any other element, low temperatures and high pressure are used to liquefy nearly all the other gases (mostly [[nitrogen]] and [[methane]]). The resulting crude helium gas is purified by successive exposures to lowering temperatures, in which almost all of the remaining nitrogen and other gases are precipitated out of the gaseous mixture. [[Activated charcoal]] is used as a final purification step, usually resulting in 99.995% pure Grade-A helium.<ref name="enc" /> The principal impurity in Grade-A helium is [[neon]]. In a final production step, most of the helium that is produced is liquefied via a [[cryogenic]] process. This is necessary for applications requiring liquid helium and also allows helium suppliers to reduce the cost of long-distance transportation, as the largest liquid helium containers have more than five times the capacity of the largest gaseous helium tube trailers.<ref name="wwsupply" /><ref>{{cite conference| author = Cai, Z. | display-authors = etal|title = Modelling Helium Markets| publisher = University of Cambridge| date = 2007| url = http://www.jbs.cam.ac.uk/programmes/phd/downloads/conference_spring2007/papers/cai.pdf| access-date = 2008-07-14|archive-url=https://web.archive.org/web/20090326072513/http://www.jbs.cam.ac.uk/programmes/phd/downloads/conference_spring2007/papers/cai.pdf|archive-date=2009-03-26}}</ref>

In 2008, approximately 169 million [[standard cubic meter]]s (SCM) of helium were extracted from natural gas or withdrawn from helium reserves, with approximately 78% from the United States, 10% from Algeria, and most of the remainder from Russia, Poland, and Qatar.<ref>{{cite conference| title = Helium| work = Mineral Commodity Summaries| pages = 74–75| publisher = U.S. Geological Survey| date = 2009| url = https://minerals.usgs.gov/minerals/pubs/commodity/helium/mcs-2009-heliu.pdf| access-date = 2009-12-19| archive-url = https://web.archive.org/web/20090814020157/http://minerals.usgs.gov/minerals/pubs/commodity/helium/mcs-2009-heliu.pdf| archive-date = 2009-08-14| url-status = live}}</ref> By 2013, increases in helium production in Qatar (under the company [[Qatargas]] managed by [[Air Liquide]]) had increased Qatar's fraction of world helium production to 25%, making it the second largest exporter after the United States.<ref name="bloomberg.com">{{Cite web|title=Air Liquide and Linde in Helium Hunt as Texas Reserves Dry Up|publisher=Bloomberg|year=2014|url=https://www.bloomberg.com/news/articles/2014-07-10/air-liquide-and-linde-in-helium-hunt-as-texas-reserves-dry-up|access-date=2017-03-07|archive-url=https://web.archive.org/web/20170310193243/https://www.bloomberg.com/news/articles/2014-07-10/air-liquide-and-linde-in-helium-hunt-as-texas-reserves-dry-up|archive-date=2017-03-10|url-status=live}}</ref> In 2024, the United States surpassed Qatar as the world's largest producer of the gas, having extracted 68&nbsp;million SCM of helium that year compared to Qatar's 64&nbsp;million SCM.<ref name=":0">{{Cite web |last=United States Geological Survey |date=March 2025 |title=Helium |url=https://pubs.usgs.gov/periodicals/mcs2025/mcs2025.pdf#page=92 |access-date=1 November 2025 |series=Mineral Commodities Summaries}}</ref>
An estimated {{convert|54|e9ft3}} deposit of helium was found in Tanzania in 2016,<ref>{{Cite news|url=https://www.bbc.com/news/science-environment-36651048|work=BBC News|title=Helium discovery a 'game-changer'|first=Helen|last=Briggs|date=28 June 2016|access-date=2016-06-28|archive-url=https://web.archive.org/web/20160628131948/http://www.bbc.com/news/science-environment-36651048|archive-date=28 June 2016|url-status=live}}</ref> and a large-scale helium plant was opened in [[Ningxia]], [[China]] in 2020.<ref>{{Cite news|title=China opens first large-scale helium plant as it tries to reduce reliance on US imports|url=https://www.scmp.com/news/china/science/article/3094905/china-opens-first-large-scale-helium-plant-it-tries-reduce|last=Chen|first=Stephen|date=28 Jul 2020|access-date=28 Jul 2020|work=South China Morning Post|location=Beijing, China|language=en}}</ref>

In the United States, most helium is extracted from the natural gas of the [[Hugoton Natural Gas Area|Hugoton]] and nearby gas fields in Kansas, Oklahoma, and the Panhandle Field in Texas.<ref name="wwsupply" /><ref>Pierce, A. P., Gott, G. B., and Mytton, J. W. (1964). "Uranium and Helium in the Panhandle Gas Field Texas, and Adjacent Areas", Geological Survey Professional Paper 454-G, Washington:US Government Printing Office</ref> Much of this gas was once sent by pipeline to the [[National Helium Reserve]], but since 2005, this reserve has been depleted and sold off, and it was expected to be largely depleted by 2021<ref name="bloomberg.com" /> under the October 2013 ''Responsible Helium Administration and Stewardship Act'' (H.R. 527).<ref>{{cite web|title=Responsible Helium Administration and Stewardship Act (H.R. 527)|url=http://naturalresources.house.gov/newsroom/documentsingle.aspx?DocumentID=320460|website=House Committee on Natural Resources|publisher=Committee on Natural Resources United States House of Representatives|access-date=5 March 2017|archive-url=https://web.archive.org/web/20170306033258/http://naturalresources.house.gov/newsroom/documentsingle.aspx?DocumentID=320460|archive-date=2017-03-06|url-status=dead}}</ref> Despite efforts to sell the remaining reserve in 2021, the remnants of the National Helium Reserve were auctioned off by the [[Bureau of Land Management]] over the course of 3 years.<ref name="NBC 2023-02-07">{{cite news |last=Pflum |first=Mary |date=February 7, 2023 |title=The fate of America's largest supply of helium is up in the air |url=https://www.nbcnews.com/science/science-news/fate-americas-largest-supply-helium-air-rcna69309 |publisher=NBC News}}</ref><ref name="GSA sale page">{{cite web |date=September 19, 2023 |title=Federal Helium System at Cliffside |url=https://www.gsa.gov/real-estate/real-estate-services/real-property-disposition/property-sales/federal-helium-system-at-cliffside |url-status=dead |archive-url=https://web.archive.org/web/20230815223135/https://www.gsa.gov/real-estate/real-estate-services/real-property-disposition/property-sales/federal-helium-system-at-cliffside |archive-date=August 15, 2023 |access-date=September 30, 2023 |publisher=U.S. General Services Administration}}</ref><ref>{{cite magazine |date=January 24, 2024 |title=In Amarillo, the Nation's Helium Stockpile Goes on Sale |url=https://www.texasmonthly.com/news-politics/amarillo-federal-helium-reserve-auction/ |access-date=January 25, 2024 |magazine=Texas Monthly}}</ref> It was finally sold to Messer Group<ref>{{cite news |date=January 25, 2024 |title=The U.S. just sold its helium stockpile. |url=https://www.nbcnews.com/health/health-news/us-just-sold-helium-stockpile-s-medical-world-worried-rcna134785 |access-date=January 25, 2024 |publisher=NBC News}}</ref> on June 27, 2024.<ref name=":0" /> The helium fields of the western United States are emerging as an alternate source of helium supply, particularly those of the "[[Four Corners]]" region (the states of Arizona, Colorado, New Mexico and Utah).<ref>{{Cite web|title = When a Rush Begins: A Field Guide to the Helium Hopefuls of the United States|url = https://www.goldandrevolution.com/when-a-rush-begins-a-field-guide-to-the-helium-hopefuls-of-the-usa/|website = Gold and Revolution|access-date = 2023-07-30|date = 2023-07-23|last = Fresne|first = Patrick}}</ref> 

Diffusion of crude natural gas through special [[semipermeable membrane]]s and other barriers is another method to recover and purify helium.<ref>{{Cite journal|title = Membrane technology—A new trend in industrial gas separation |last1 = Belyakov|first1=V. P. |last2 = Durgar'yan|first2=S. G. |last3 = Mirzoyan|first3=B. A.|journal = Chemical and Petroleum Engineering |volume = 17 |issue = 1 |pages = 19–21 |date = 1981 |doi = 10.1007/BF01245721| bibcode=1981CPE....17...19B |s2cid = 109199653}}</ref> In 1996, the U.S. had ''proven'' helium reserves in such gas well complexes of about 147 billion [[standard cubic feet]] (4.2 billion SCM).<ref>Committee on the Impact of Selling, [http://www.nap.edu/openbook.php?record_id=9860&page=44 Table 4.2] {{Webarchive|url=https://web.archive.org/web/20140910195702/http://www.nap.edu/openbook.php?record_id=9860&page=44 |date=2014-09-10 }}</ref> At rates of use at that time (72 million SCM per year in the U.S.; see pie chart below) this would have been enough helium for about 58 years of U.S. use, and less than this (perhaps 80% of the time) at world use rates, although factors in saving and processing impact effective reserve numbers.

Helium is commercially available in either liquid or gaseous form. As a liquid, it can be supplied in small insulated containers called [[Dewar flask|dewars]] which hold as much as 1,000 liters of helium, or in large ISO containers, which have nominal capacities as large as 42&nbsp;m<sup>3</sup> (around 11,000 U.S. [[gallon]]s). In gaseous form, small quantities of helium are supplied in high-pressure cylinders holding as much as 8&nbsp;m<sup>3</sup> (approximately . 282 standard cubic feet), while large quantities of high-pressure gas are supplied in tube trailers, which have capacities of as much as 4,860&nbsp;m<sup>3</sup> (approx. 172,000 standard cubic feet).

===Conservation advocates===
{{Main|Helium storage and conservation}}

According to helium conservationists like Nobel laureate physicist [[Robert Coleman Richardson]], writing in 2010, the free market price of helium has contributed to "wasteful" usage (e.g. for [[Tethered helium balloon|helium balloons]]). Prices in the 2000s had been lowered by the decision of the U.S. Congress to sell off the country's large helium stockpile by 2015.<ref name="Connor" /> Richardson posited that the price of helium needed to be multiplied by 20 to eliminate excessive wasting of the gas. In a 2012 paper by Nuttall and colleagues titled "Stop squandering helium", they proposed to create an International Helium Agency that would build a sustainable helium market.<ref>{{cite journal |last1=Nuttall |first1=William J. |last2=Clarke |first2=Richard H. |last3=Glowacki |first3=Bartek A. |date=2012 |title=Resources: Stop squandering helium |journal=Nature |volume=485 |issue=7400 |pages=573–575 |bibcode=2012Natur.485..573N |doi=10.1038/485573a |pmid=22660302 |s2cid=10351068|doi-access=free }}</ref>

==Applications==
[[File:Modern 3T MRI.JPG|thumb|The largest single use of liquid helium is to cool the superconducting magnets in modern [[MRI Scanner|MRI scanners]].|alt=A large solid cylinder with a hole in its center and a rail attached to its side.]]

{{Pie chart
 | caption=Estimated 2014 U.S. fractional helium use by category. Total use is 34 million cubic meters.<ref name="usgs-helium">{{cite book |author= U.S. Department of the Interior, U.S. Geological Survey |date= 2015 |title= Mineral Commodity Summaries 2014 |chapter= Helium |pages= 72–73 |doi= 10.3133/70194932 |chapter-url= https://minerals.usgs.gov/minerals/pubs/commodity/helium/mcs-2015-heliu.pdf |url= https://minerals.usgs.gov/minerals/pubs/mcs/index.html |access-date= 2014-05-31 |archive-url= https://web.archive.org/web/20140404122859/http://minerals.usgs.gov/minerals/pubs/mcs/index.html |archive-date= 2014-04-04 |url-status= live }}</ref>
 | other = yes
 | label1 = Cryogenics
 | value1 = 32
 | label2 = Pressurizing and purging
 | value2 = 18
 | label4 = Controlled atmospheres
 | value4 = 18
 | label3 = Welding
 | value3 = 13
 | label5 = Leak detection
 | value5 = 4
 | label6 = Breathing mixtures
 | value6 = 2
}}

While balloons are perhaps the best-known use of helium, they are a minor part of all helium use.<ref name="stwertka" /> Helium is used for many purposes that require some of its unique properties, such as its low [[boiling point]], low [[density]], low [[solubility]], high [[thermal conductivity]], or [[Chemically inert|inertness]]. Of the 2014 world helium total production of about 32 million kg (180 million standard cubic meters) helium per year, the largest use (about 32% of the total in 2014) is in cryogenic applications, most of which involves cooling the superconducting magnets in medical [[MRI]] scanners and [[NMR]] spectrometers.<ref>[http://physicsworld.com/cws/article/news/2010/jan/27/helium-sell-off-risks-future-supply Helium sell-off risks future supply] {{Webarchive|url=https://web.archive.org/web/20120610175902/http://physicsworld.com/cws/article/news/2010/jan/27/helium-sell-off-risks-future-supply |date=2012-06-10 }}, Michael Banks, ''Physics World'', 27 January 2010. accessed February 27, 2010.</ref> Other major uses were pressurizing and purging systems, welding, maintenance of controlled atmospheres, and leak detection. Other uses by category were relatively minor fractions.<ref name="usgs-helium" />

=== Controlled atmospheres ===
Helium is used as a protective gas in growing [[silicon]] and [[germanium]] crystals, in [[titanium]] and [[zirconium]] production, and in [[gas chromatography]],<ref name="LANL.gov" /> because it is inert. Because of its inertness, [[ideal gas|thermally and calorically perfect]] nature, high [[speed of sound]], and high value of the [[heat capacity ratio]], it is also useful in [[supersonic wind tunnel]]s<ref>{{Cite journal|last1 = Beckwith|first1=I. E.|last2 = Miller|first2=C. G.|title = Aerothermodynamics and Transition in High-Speed Wind Tunnels at Nasa Langley |journal = Annual Review of Fluid Mechanics |volume = 22|issue = 1 |pages = 419–439 |date= 1990 |doi = 10.1146/annurev.fl.22.010190.002223|bibcode = 1990AnRFM..22..419B }}</ref> and [[impulse facility|impulse facilities]].<ref>{{Cite book|author = Morris, C.I. |title = Shock Induced Combustion in High Speed Wedge Flows |date= 2001 |series = Stanford University Thesis |url = http://thermosciences.stanford.edu/pdf/TSD-143.pdf|archive-url = https://web.archive.org/web/20090304210445/http://thermosciences.stanford.edu/pdf/TSD-143.pdf|archive-date = 2009-03-04}}</ref>

=== Gas tungsten arc welding ===
{{main|Gas tungsten arc welding}}

Helium is used as a [[shielding gas]] in [[arc welding]] processes on materials that are contaminated and weakened by air or nitrogen at welding temperatures.<ref name="nbb" /> A number of inert shielding gases are used in gas tungsten arc welding, but helium is used instead of cheaper [[argon]] especially for welding materials that have higher [[heat conductivity]], like [[aluminium]] or [[copper]].

=== Minor uses ===

==== Industrial leak detection ====
[[File:Ac-system 2.jpg|thumb|left|A dual chamber helium leak detection machine|alt=Photo of a large, metal-framed device (about 3×1×1.5 m) standing in a room.]]

One industrial application for helium is [[leak detection]]. Because helium [[diffusion|diffuses]] through solids three times faster than air, it is used as a tracer gas to detect [[leak]]s in high-vacuum equipment (such as cryogenic tanks) and high-pressure containers.<ref name="nostrand">{{cite encyclopedia| title = Helium|editor = Considine, Glenn D.| encyclopedia = Van Nostrand's Encyclopedia of Chemistry| pages = 764–765|publisher = Wiley-Interscience|date = 2005|isbn = 978-0-471-61525-5}}</ref> The tested object is placed in a chamber, which is then evacuated and filled with helium. The helium that escapes through the leaks is detected by a sensitive device ([[helium mass spectrometer]]), even at the leak rates as small as 10<sup>−9</sup> mbar·L/s (10<sup>−10</sup> Pa·m<sup>3</sup>/s). The measurement procedure is normally automatic and is called helium integral test. A simpler procedure is to fill the tested object with helium and to manually search for leaks with a hand-held device.<ref>{{Cite book|url=https://books.google.com/books?id=5L8uIAFm4SoC&pg=PA493|page=493|title=High-vacuum technology: a practical guide|author=Hablanian, M. H.|publisher=CRC Press|date=1997|isbn=978-0-8247-9834-5}}</ref>

Helium leaks through cracks should not be confused with gas permeation through a bulk material. While helium has documented permeation constants (thus a calculable permeation rate) through glasses, ceramics, and synthetic materials, inert gases such as helium will not permeate most bulk metals.<ref>{{Cite book|author=Ekin, Jack W.|title=Experimental Techniques for Low-Temperature measurements|url=https://archive.org/details/experimentaltech0000ekin|url-access=registration|publisher=Oxford University Press|date=2006|isbn=978-0-19-857054-7}}</ref>

==== Flight ====
[[File:Goodyear-blimp.jpg|thumb|left|Because of its low density and incombustibility, helium is the gas of choice to fill airships such as the [[Goodyear blimp]].|alt=The Good Year Blimp]]
Because it is [[lighter than air]], [[airship]]s and balloons are inflated with helium for [[Lifting gas|lift]]. While hydrogen gas is more buoyant and escapes permeating through a membrane at a lower rate, helium has the advantage of being non-flammable, and indeed [[fire-retardant]]. Another minor use is in [[rocket]]ry, where helium is used as an [[ullage]] medium to backfill rocket propellant tanks in flight and to condense hydrogen and oxygen to make [[rocket fuel]]. It is also used to purge fuel and oxidizer from ground support equipment prior to launch and to pre-cool liquid hydrogen in [[space vehicle]]s. For example, the [[Saturn V]] rocket used in the [[Apollo program]] needed about {{convert|370,000|m3|e6ft3|abbr=off}} of helium to launch.<ref name="LANL.gov" />

==== Minor commercial and recreational uses ====
Helium as a breathing gas has no [[Nitrogen narcosis|narcotic properties]], so helium mixtures such as [[Trimix (breathing gas)|trimix]], [[heliox]] and [[Trimix (breathing gas)#Heliair|heliair]] are used for [[deep diving]] to reduce the effects of narcosis, which worsen with increasing depth.<ref>{{Cite journal |last1=Fowler |first1=B. |last2=Ackles |first2=K. N. |first3=Porlier |last3=G |date=1985 |title=Effects of inert gas narcosis on behavior—a critical review |journal=Undersea Biomedical Research |pmid=4082343 |url=http://archive.rubicon-foundation.org/3019 |access-date=2008-06-27 |volume=12 |issue=4 |pages=369–402 |archive-url=https://web.archive.org/web/20101225052236/http://archive.rubicon-foundation.org/3019 |archive-date=2010-12-25 |url-status=usurped }}</ref><ref name="thomas">{{Cite journal |author=Thomas, J. R. |date=1976 |title=Reversal of nitrogen narcosis in rats by helium pressure |journal=Undersea Biomed. Res. |volume=3 |issue=3 |pages=249–59 |pmid=969027 |url=http://archive.rubicon-foundation.org/2771 |access-date=2008-08-06 |archive-url=https://web.archive.org/web/20081206035952/http://archive.rubicon-foundation.org/2771 |archive-date=2008-12-06 |url-status=usurped }}</ref> As pressure increases with depth, the density of the breathing gas also increases, and the low molecular weight of helium is found to considerably reduce the effort of breathing by lowering the density of the mixture. This reduces the [[Reynolds number]] of flow, leading to a reduction of [[turbulent flow]] and an increase in [[laminar flow]], which requires less breathing.<ref>{{Cite journal| author = Butcher, Scott J.| author2 = Jones, Richard L.| author3 = Mayne, Jonathan R.| author4 = Hartley, Timothy C.| author5 = Petersen, Stewart R.| title = Impaired exercise ventilatory mechanics with the self-contained breathing apparatus are improved with heliox| journal = European Journal of Applied Physiology| volume = 101| issue = 6|date = 2007| doi = 10.1007/s00421-007-0541-5| pmid = 17701048| pages = 659–69| s2cid = 7311649}}</ref><ref name="BOCheox21">{{cite web |url=http://www.bochealthcare.co.uk/en/products/heliox/index.shtml |title=Heliox21 |publisher=Linde Gas Therapeutics |date=27 January 2009 |access-date=13 April 2011 |archive-url=https://web.archive.org/web/20110910232729/http://www.bochealthcare.co.uk/en/products/heliox/index.shtml |archive-date=10 September 2011 |url-status=live }}</ref> At depths below {{convert|150|m|ft}} divers breathing helium-oxygen mixtures begin to experience tremors and a decrease in psychomotor function, symptoms of [[high-pressure nervous syndrome]].<ref name="HungerBennett">{{cite journal |last1=Hunger | first1=W. L. Jr. |first2=P. B. |last2=Bennett |title=The causes, mechanisms and prevention of the high pressure nervous syndrome |journal=Undersea Biomed. Res. |volume=1 |issue=1 |pages=1–28 |date=1974 |issn=0093-5387 |oclc=2068005 |pmid=4619860 |url=http://archive.rubicon-foundation.org/2661 |access-date=2008-04-07 |archive-url=https://web.archive.org/web/20101225053451/http://archive.rubicon-foundation.org/2661 |archive-date=2010-12-25 |url-status=usurped }}</ref> This effect may be countered to some extent by adding an amount of narcotic gas such as hydrogen or nitrogen to a helium–oxygen mixture.<ref>{{Cite journal |author=Rostain, J. C. |author2=Gardette-Chauffour, M. C. |author3=Lemaire, C. |author4=Naquet, R. |title=Effects of a H<sub>2</sub>-He-O<sub>2</sub> mixture on the HPNS up to 450 msw |journal=Undersea Biomed. Res. |volume=15 |issue=4 |pages=257–70 |date=1988 |oclc=2068005 |pmid=3212843 |url=http://archive.rubicon-foundation.org/2487 |access-date=2008-06-24 |archive-url=https://web.archive.org/web/20081206035912/http://archive.rubicon-foundation.org/2487 |archive-date=2008-12-06 |url-status=usurped }}</ref>

[[Helium–neon laser]]s, a type of low-powered gas laser producing a red beam, had various practical applications which included [[barcode reader]]s and [[laser pointer]]s, before they were almost universally replaced by cheaper [[diode laser]]s.<ref name="nbb" />

For its inertness and high [[thermal conductivity]], neutron transparency, and because it does not form radioactive isotopes under reactor conditions, helium is used as a heat-transfer medium in some [[gas-cooled reactor|gas-cooled nuclear reactor]]s.<ref name="nostrand" />

Helium, mixed with a heavier gas such as xenon, is useful for [[thermoacoustic refrigeration]] due to the resulting high [[heat capacity ratio]] and low [[Prandtl number]].<ref>{{Cite journal|title=Working gases in thermoacoustic engines |journal=The Journal of the Acoustical Society of America |date=1999 |volume=105 |issue=5 |pages=2677–2684 |doi=10.1121/1.426884|author1 = Belcher, James R.|pmid=10335618|bibcode = 1999ASAJ..105.2677B|author2=Slaton, William V.|author3=Raspet, Richard|author4=Bass, Henry E.|author5=Lightfoot, Jay|doi-access=free}}</ref> The inertness of helium has environmental advantages over conventional refrigeration systems which contribute to ozone depletion or global warming.<ref>{{Cite book|title=Mending the Ozone Hole: Science, Technology, and Policy |author=Makhijani, Arjun |author2=Gurney, Kevin |publisher=MIT Press |date=1995 |isbn=978-0-262-13308-1}}</ref>

Helium is also used in some [[hard disk drive]]s.<ref>{{Cite web|url=https://arstechnica.com/information-technology/2013/11/hgst-balloons-disk-capacity-with-helium-filled-6tb-drive/|title=HGST balloons disk capacity with helium-filled 6TB drive|first=Sean|last=Gallagher|date=November 4, 2013|website=Ars Technica|access-date=June 14, 2017|archive-url=https://web.archive.org/web/20170707231259/https://arstechnica.com/information-technology/2013/11/hgst-balloons-disk-capacity-with-helium-filled-6tb-drive/|archive-date=July 7, 2017|url-status=live}}</ref>

==== Scientific uses ====
The use of helium reduces the distorting effects of temperature variations in the space between [[lens (optics)|lenses]] in some [[telescope]]s due to its extremely low [[index of refraction]].<ref name="enc" /> This method is especially used in solar telescopes where a vacuum tight telescope tube would be too heavy.<ref>{{Cite journal|author = Jakobsson, H. |title = Simulations of the dynamics of the Large Earth-based Solar Telescope |journal = Astronomical & Astrophysical Transactions |volume = 13 |issue = 1 |pages = 35–46 |date= 1997 |doi = 10.1080/10556799708208113|bibcode = 1997A&AT...13...35J }}</ref><ref>{{Cite journal|bibcode = 1983ApOpt..22...10E|title = Tests of vacuum VS. helium in a solar telescope|author = Engvold, O.|author2 = Dunn, R.B.|author3 = Smartt, R. N.|author4 = Livingston, W. C.| journal = Applied Optics|date = 1983|pages = 10–12|issue = 1|volume = 22|pmid = 20401118|doi = 10.1364/AO.22.000010}}</ref>

Helium is a commonly used carrier gas for [[gas chromatography]].

The age of rocks and minerals that contain uranium and thorium can be estimated by measuring the level of helium with a process known as [[helium dating]].<ref name="nbb" /><ref name="enc" />

Helium at low temperatures is used in [[cryogenics]] and in certain cryogenic applications. As examples of applications, liquid helium is used to cool certain metals to the extremely low temperatures required for [[superconductivity]], such as in [[superconducting magnet]]s for [[magnetic resonance imaging]]. The [[Large Hadron Collider]] at [[CERN]] uses 96 [[metric ton]]s of liquid helium to maintain the temperature at {{convert|1.9|K|C F}}.<ref name="CERN-LHC">{{cite web|url=http://visits.web.cern.ch/visits/guides/tools/presentation/LHC_booklet-2.pdf |archive-url=https://web.archive.org/web/20110706223231/http://visits.web.cern.ch/visits/guides/tools/presentation/LHC_booklet-2.pdf |archive-date=2011-07-06 |title=LHC: Facts and Figures|publisher=[[CERN]]|access-date=2008-04-30}}</ref>

==== Medical uses ====
Helium was approved for medical use in the United States in April 2020 for humans and animals.<ref>{{cite web | title=Helium, USP: FDA-Approved Drugs | website=U.S. Food and Drug Administration | url=https://www.accessdata.fda.gov/scripts/cder/daf/index.cfm?event=overview.process&ApplNo=213990 | archive-url=https://web.archive.org/web/20200626003406/https://www.accessdata.fda.gov/scripts/cder/daf/index.cfm?event=overview.process&ApplNo=213990 | url-status=dead | archive-date=June 26, 2020 | access-date=30 April 2020}}</ref><ref>{{cite web | url=https://www.accessdata.fda.gov/drugsatfda_docs/appletter/2020/213990orig1s000MGltr.pdf | title=FDA approval letter | date=14 April 2020 | access-date=30 April 2020}}</ref>

==As a contaminant==
While chemically inert, helium contamination impairs the operation of [[microelectromechanical systems]] (MEMS) such that iPhones may fail.<ref>{{cite news |last1=Oberhaus |first1=Daniel |title=Why a Helium Leak Disabled Every iPhone in a Medical Facility |url=https://www.vice.com/en/article/why-a-helium-leak-disabled-every-iphone-in-a-medical-facility/ |access-date=31 October 2018 |work=Motherboard |publisher=[[Vice Media]] |date=30 October 2018 |archive-url=https://web.archive.org/web/20181101015429/https://motherboard.vice.com/en_us/article/gye4aw/why-a-helium-leak-disabled-every-iphone-in-a-medical-facility |archive-date=1 November 2018 |url-status=live }}</ref>

==Inhalation and safety==

===Effects===
Neutral helium at standard conditions is non-toxic, plays no biological role and is found in trace amounts in human blood.

{{Listen|right|filename=Helium article read with helium.ogg|title=Effect of helium on a human voice|description=The effect of helium on a human voice|format=[[Ogg]]}}
The [[speed of sound]] in helium is nearly three times the speed of sound in air. Because the [[fundamental frequency|natural resonance frequency]] of a gas-filled cavity is proportional to the speed of sound in the gas, when helium is inhaled, a corresponding increase occurs in the [[resonant frequency|resonant frequencies]] of the [[vocal tract]], which is the amplifier of vocal sound.<ref name="nbb" /><ref>{{Cite journal |last1=Ackerman |first1=M. J. |last2=Maitland |first2=G. |title=Calculation of the relative speed of sound in a gas mixture |journal=Undersea Biomed Res |volume=2 |issue=4 |pages=305–10 |date=1975 |pmid=1226588 |url=http://archive.rubicon-foundation.org/2738 |access-date=2008-08-09 |archive-url=https://web.archive.org/web/20110127113335/http://archive.rubicon-foundation.org/2738 |archive-date=2011-01-27 |url-status=usurped }}</ref> This increase in the resonant frequency of the amplifier (the vocal tract) gives increased amplification to the high-frequency components of the sound wave produced by the direct vibration of the vocal folds, compared to the case when the voice box is filled with air. When a person speaks after inhaling helium gas, the muscles that control the voice box still move in the same way as when the voice box is filled with air; therefore the [[fundamental frequency]] (sometimes called [[Pitch (music)|pitch]]) produced by direct vibration of the vocal folds does not change.<ref>{{cite web|date=14 July 2000|title=Why does helium make your voice squeaky?|url=http://www.straightdope.com/columns/read/1803/why-does-helium-make-your-voice-squeaky|url-status=live|archive-url=https://web.archive.org/web/20130324072558/http://www.straightdope.com/columns/read/1803/why-does-helium-make-your-voice-squeaky|archive-date=24 March 2013|access-date=2013-06-08}}</ref> However, the high-frequency-preferred amplification causes a change in [[timbre]] of the amplified sound, resulting in a reedy, duck-like vocal quality. The opposite effect, lowering resonant frequencies, can be obtained by inhaling a dense gas such as [[sulfur hexafluoride]] or [[xenon]].

===Hazards===
{{Chembox

| Name = Helium
| container_only = yes
|Section7={{Chembox Hazards
| ExternalSDS =
| GHSPictograms = {{GHS04}}
| GHSSignalWord = Warning
| HPhrases = {{H-phrases|280}}
| PPhrases = {{P-phrases|410+403}}<ref name=airgas1>{{Cite web|url=https://www.airgas.com/msds/001025.pdf|title=Helium|website=[[Airgas]]|date=March 28, 2025 |access-date=November 1, 2025}}</ref>
| NFPA-H = 1
| NFPA-F = 0
| NFPA-R = 0
| NFPA-S = 
| NFPA_ref = <ref name=airgas1 />
 }}
}}
Inhaling helium can be dangerous if done to excess, since helium is a simple [[asphyxiant gas|asphyxiant]] and so displaces oxygen needed for normal respiration.<ref name="nbb" /><ref name="Grass">{{Cite journal|title = Suicidal asphyxiation with helium: Report of three cases Suizid mit Helium Gas: Bericht über drei Fälle|journal = Wiener Klinische Wochenschrift| volume = 119|issue =9–10|date = 2007|doi = 10.1007/s00508-007-0785-4|author = Grassberger, Martin|author2 = Krauskopf, Astrid |pages = 323–325 |language=de, en|pmid = 17571238|s2cid = 22894287}}</ref> Fatalities have been recorded, including a youth who suffocated in Vancouver in 2003 and two adults who suffocated in South Florida in 2006.<ref name="sptimes.com">{{cite news | title = 2 found dead under deflated balloon | url = http://www.sptimes.com/2006/06/03/Tampabay/2_found_dead_under_de.shtml | author = Montgomery B. | author2 = Hayes S. | date = 2006-06-03 | newspaper = Tampa Bay Times | access-date = 2013-12-29 | archive-url = https://web.archive.org/web/20131230235619/http://www.sptimes.com/2006/06/03/Tampabay/2_found_dead_under_de.shtml | archive-date = 2013-12-30 | url-status = live }}</ref><ref name="cbc.ca">{{cite news| url = http://www.cbc.ca/news/world/two-students-die-after-breathing-helium-1.623684| title = Two students die after breathing helium| publisher = CBC| date = 4 June 2006| access-date = 30 December 2013| archive-url = https://web.archive.org/web/20131231000044/http://www.cbc.ca/news/world/two-students-die-after-breathing-helium-1.623684| archive-date = 31 December 2013| url-status = live}}</ref> In 1998, an Australian girl from Victoria fell unconscious and temporarily [[cyanosis|turned blue]] after inhaling the entire contents of a party balloon.<ref name="balloonartists.com.au">{{cite web | url = http://balloonartists.com.au/helium-dangers.html | title = Helium inhalation – it's no laughing matter – Article courtesy of BOC Gases | publisher = Balloon Artists & Suppliers Association of Australasia Ltd | access-date = 2014-01-03 | archive-url = https://web.archive.org/web/20140114214605/http://www.balloonartists.com.au/helium-dangers.html | archive-date = 2014-01-14 | url-status = live }}</ref><ref name="lousballoons.com.au">{{cite web | url = http://www.lousballoons.com.au/dangers-of-helium.html | title = Dangers of Helium Inhalation | publisher = Lou's Balloons | url-status=dead | archive-url = https://web.archive.org/web/20140104032013/http://www.lousballoons.com.au/dangers-of-helium.html | archive-date = 2014-01-04 }}</ref><ref name="bouncetime.co.uk">{{cite web | url = http://www.bouncetime.co.uk/others_files/helium-gas-safety.htm | title = Helium Gas Safety & Data Sheet | publisher = bouncetime | access-date = 2014-01-03 | archive-url = https://web.archive.org/web/20150422003602/http://www.bouncetime.co.uk/others_files/helium-gas-safety.htm | archive-date = 2015-04-22 | url-status = live }}</ref>
Inhaling helium directly from pressurized cylinders or even balloon filling valves is extremely dangerous, as high flow rate and pressure can result in [[barotrauma]], fatally rupturing lung tissue.<ref name="Grass" /><ref name="slate">{{Cite news| author = Engber, Daniel| title = Stay Out of That Balloon!| publisher = Slate.com| date = 2006-06-13| url = http://www.slate.com/articles/news_and_politics/explainer/2006/06/stay_out_of_that_balloon.html| access-date = 2008-07-14| archive-url = https://web.archive.org/web/20111020154111/http://www.slate.com/articles/news_and_politics/explainer/2006/06/stay_out_of_that_balloon.html| archive-date = 2011-10-20| url-status = live}}</ref>

Death caused by helium is rare. The first media-recorded case was that of a 15-year-old girl from Texas who died in 1998 from helium inhalation at a friend's party; the exact type of helium death is unidentified.<ref name="balloonartists.com.au" /><ref name="lousballoons.com.au" /><ref name="bouncetime.co.uk" />

In the United States, only two fatalities were reported between 2000 and 2004, including a man who died in North Carolina of barotrauma in 2002.<ref name="sptimes.com" /><ref name="slate" /> A youth asphyxiated in Vancouver during 2003, and a 27-year-old man in Australia had an embolism after breathing from a cylinder in 2000.<ref name="sptimes.com" /> Since then, two adults asphyxiated in South Florida in 2006,<ref name="sptimes.com" /><ref name="cbc.ca" /><ref>{{cite journal | pmc = 1117755 | date = 2000 | last1 = Josefson | first1 = D. | title = Imitating Mickey Mouse can be dangerous | volume = 320 | issue = 7237 | pages = 732 | journal = BMJ: British Medical Journal | pmid=10720344}}</ref> and there were cases in 2009 and 2010, one of whom was a Californian youth who was found with a bag over his head, attached to a helium tank,<ref>{{cite news|url=http://www.ktla.com/news/landing/ktla-riverside-teen-helium,0,6589649.story |archive-url=https://web.archive.org/web/20120109032345/http://www.ktla.com/news/landing/ktla-riverside-teen-helium%2C0%2C6589649.story |archive-date=January 9, 2012 |title=Teen Dies After Inhaling Helium |date=January 6, 2010 |work=KTLA News |publisher=ktla.com |access-date=2010-11-19 |location=RIVERSIDE |url-status=dead }}</ref> and another teenager in Northern Ireland died of asphyxiation.<ref>{{cite news |url=https://www.bbc.co.uk/news/uk-northern-ireland-11795984 |title=Tributes to 'helium death' teenager from Newtownabbey |date=19 November 2010 |work=[[BBC Online]] |access-date=2010-11-19 |archive-url=https://web.archive.org/web/20101120085647/http://www.bbc.co.uk/news/uk-northern-ireland-11795984 |archive-date=20 November 2010 |url-status=live }}</ref> At [[Eagle Point, Oregon]] a teenage girl died in 2012 from barotrauma at a party.<ref>{{cite news|author=Mather, Kate|title=Parents of Eagle Point girl who died from inhaling helium hope to save others from same fate|url=http://www.oregonlive.com/pacific-northwest-news/index.ssf/2012/02/parents_of_eagle_point_girl_wh.html|work=The Oregonian|date=24 February 2012|access-date=2013-06-08|archive-url=https://web.archive.org/web/20131206170024/http://www.oregonlive.com/pacific-northwest-news/index.ssf/2012/02/parents_of_eagle_point_girl_wh.html|archive-date=6 December 2013|url-status=live}}</ref><ref name="huffingtonpost.com">{{cite news |last=Barnard |first=Jeff |title=Ashley Long, Oregon Teenager, Dies After Inhaling Helium at Wild Party (VIDEO) |url=http://www.huffingtonpost.com/2012/02/22/oregon-teenager-ashley-long_n_1294989.html |work=Huffington Post |date=22 February 2012 |access-date=30 December 2013 |archive-url=https://web.archive.org/web/20131231000509/http://www.huffingtonpost.com/2012/02/22/oregon-teenager-ashley-long_n_1294989.html |archive-date=31 December 2013 |url-status=live }}</ref><ref name="today.com">{{cite web |url=http://www.today.com/id/46487997 |title=Teen girl dies after inhaling helium at party |first=Jeff |last=Barnard |date=23 February 2012 |agency=AP |website=Today |access-date=2013-12-30 |url-status=dead |archive-url=https://web.archive.org/web/20131230233944/http://www.today.com/id/46487997 |archive-date=2013-12-30 }}</ref> A girl from Michigan died from hypoxia later in the year.<ref>''The Oxford Leader Newspaper'', Sherman Publications, Inc., December 3, 2012.</ref>

On February 4, 2015, it was revealed that, during the recording of their main TV show on January 28, a 12-year-old member (name withheld) of Japanese all-girl singing group [[3B Junior]] suffered from [[air embolism]], losing consciousness and falling into a [[coma]] as a result of air bubbles blocking the flow of blood to the brain after inhaling huge quantities of helium as part of a game. The incident was not made public until a week later.<ref>{{cite news|url=http://www.j-cast.com/2015/02/05227178.html|title=テレ朝事故で分かったヘリウム変声缶の危険性 意識を失うケースの大半が子ども|date=5 February 2015|access-date=2015-02-05|language=ja|archive-url=https://web.archive.org/web/20150205172253/http://www.j-cast.com/2015/02/05227178.html|archive-date=5 February 2015|url-status=live}}</ref><ref>{{cite magazine|url=https://time.com/3697523/jpop-3b-junior-helium-stunt/|title=J-Pop Teen Star Left in Coma After Inhaling Helium for TV Stunt|magazine=[[Time (magazine)|Time]]|date=5 February 2015|access-date=2015-02-06|first=Noah|last=Rayman|archive-url=https://web.archive.org/web/20150205195944/http://time.com/3697523/jpop-3b-junior-helium-stunt/|archive-date=5 February 2015|url-status=live}}</ref> The staff of [[TV Asahi]] held an emergency press conference to communicate that the member had been taken to the hospital and is showing signs of rehabilitation such as moving eyes and limbs, but her consciousness has not yet been sufficiently recovered. Police have launched an investigation due to a neglect of safety measures.<ref>{{cite news|url=http://www.sponichi.co.jp/entertainment/news/2015/02/04/kiji/K20150204009750570.html|title=アイドルが収録中に倒れ病院搬送 テレ朝、ヘリウムガス吸引|date=4 April 2015|access-date=2015-02-04|language=ja|archive-url=https://web.archive.org/web/20150204230036/http://www.sponichi.co.jp/entertainment/news/2015/02/04/kiji/K20150204009750570.html|archive-date=4 February 2015|url-status=live}}<br />{{cite news|url=http://www.sankei.com/affairs/news/150204/afr1502040032-n1.html|title=テレビ番組収録中、12歳アイドルが意識失い救急搬送 ヘリウムガスが原因か|date=4 February 2015|access-date=2015-02-04|language=ja|archive-url=https://web.archive.org/web/20150204230008/http://www.sankei.com/affairs/news/150204/afr1502040032-n1.html|archive-date=4 February 2015|url-status=live}}<br />{{cite news|url=http://www.hochi.co.jp/entertainment/20150204-OHT1T50098.html|title=テレ朝謝罪、12歳アイドルがヘリウム吸い救急搬送|date=4 February 2015|access-date=2015-02-04|language=ja|url-status=dead|archive-url=https://web.archive.org/web/20150204090914/http://www.hochi.co.jp/entertainment/20150204-OHT1T50098.html|archive-date=2015-02-04}}<br />{{cite news|url=http://www.tokyoreporter.com/2015/02/04/3b-junior-idol-in-coma-after-inhaling-helium-on-tv-asahi-program/|title=3b Junior idol in coma after inhaling helium on TV Asahi program|date=4 February 2015|access-date=2015-02-04|archive-url=https://web.archive.org/web/20150204230158/http://www.tokyoreporter.com/2015/02/04/3b-junior-idol-in-coma-after-inhaling-helium-on-tv-asahi-program/|archive-date=4 February 2015|url-status=live}}<br />{{cite news|url=http://www.tokyo-sports.co.jp/entame/entertainment/363851/|title=アイドル救急搬送騒動で制作会社が実績削除の不可解|date=4 February 2015|access-date=2015-02-04|language=ja|archive-url=https://web.archive.org/web/20150204124022/http://www.tokyo-sports.co.jp/entame/entertainment/363851/|archive-date=4 February 2015|url-status=live}}</ref><ref>{{cite news|url=https://www.bbc.com/news/entertainment-arts-31147038|title=Japanese child star in coma after helium stunt goes wrong|publisher=[[BBC]]|date=5 February 2015|access-date=2015-02-06|archive-url=https://web.archive.org/web/20150205195830/http://www.bbc.com/news/entertainment-arts-31147038|archive-date=5 February 2015|url-status=live}}</ref>

The safety issues for cryogenic helium are similar to those of [[liquid nitrogen]]; its extremely low temperatures can result in [[frostbite|cold burns]], and the liquid-to-gas expansion ratio can cause explosions if no pressure-relief devices are installed. Containers of helium gas at 5 to 10 K should be handled as if they contain liquid helium due to the rapid and significant [[thermal expansion]] that occurs when helium gas at less than 10 K is warmed to [[room temperature]].<ref name="LANL.gov" />

At high pressures (more than about 20&nbsp;atm or two&nbsp;[[MPa]]), a mixture of helium and oxygen ([[heliox]]) can lead to [[high-pressure nervous syndrome]], a sort of reverse-anesthetic effect; adding a small amount of nitrogen to the mixture can alleviate the problem.<!--<ref>{{cite web| last = Campbell| first = Ernest S.| title = High Pressure Nervous Syndrome| work = Physics and Problems With Gases|date = 2008-05-13| url = http://www.scuba-doc.com/HPNS.html| access-date = 2008-07-16}}</ref>--><ref>{{Cite journal|author=Rostain J.C.|author2=Lemaire C.|author3=Gardette-Chauffour M.C.|author4=Doucet J.|author5=Naquet R.|title=Estimation of human susceptibility to the high-pressure nervous syndrome |journal=J Appl Physiol |volume=54 |issue=4 |pages=1063–70 |date=1983|pmid=6853282|doi=10.1152/jappl.1983.54.4.1063}}</ref><ref name="HungerBennett" />

==See also==
{{Colbegin|colwidth=20em}}
* [[Abiogenic petroleum origin]]
* [[Helium-3 propulsion]]
* [[Leidenfrost effect]]
* [[Superfluid]]
* [[Tracer-gas leak testing method]]
* [[Hamilton Cady]]
{{colend}}

== Notes ==
{{notelist}}

==References==
{{Reflist|30em}}

==Bibliography==
<!-- Commented out the already noted references-->
{{refbegin}}
* {{Cite book |author=Bureau of Mines |title=Minerals yearbook mineral fuels Year 1965 |volume=II |publisher=U. S. Government Printing Office |date=1967}}<!--Can't find this in worldcat -->
* {{Cite book |title=The Impact of Selling the Federal Helium Reserve |author1=Committee on the Impact of Selling the Federal Helium Reserve |author2=((Commission on Physical Sciences, Mathematics, and Applications)) |author3=Commission on Engineering and Technical Systems |author4=National Research Council |publisher=The National Academies Press |date=2000 |isbn=978-0-309-07038-6 |url=http://www.nap.edu/openbook.php?record_id=9860&page=27 |access-date=2010-04-02}}
* {{Cite book |author=Emsley, John |title=The Elements |edition=3rd |location=New York |publisher=Oxford University Press |date=1998 |isbn=978-0-19-855818-7}}
* {{cite web |url=http://www.oma.be/BIRA-IASB/Public/Research/Thermo/Thermotxt.en.html |title=The thermosphere: a part of the heterosphere |author=Vercheval, J. |date=2003 |access-date=2008-07-12 |publisher=Belgian Institute for Space Aeronomy |archive-url=https://web.archive.org/web/20050101090349/http://www.oma.be/BIRA-IASB/Public/Research/Thermo/Thermotxt.en.html |archive-date=2005-01-01 |url-status=dead}}
{{refend}}

==External links==
{{Spoken Wikipedia|Helium.ogg|date=2009-07-15}}
* [https://minerals.usgs.gov/minerals/pubs/commodity/helium/ U.S. Geological Survey publications on helium] {{Webarchive|url=https://web.archive.org/web/20080916115230/http://minerals.usgs.gov/minerals/pubs/commodity/helium/ |date=2008-09-16 }} beginning 1996: [https://minerals.usgs.gov/minerals/pubs/commodity/helium/mcs-2012-heliu.pdf Helium] {{Webarchive|url=https://web.archive.org/web/20190111143447/https://minerals.usgs.gov/minerals/pubs/commodity/helium/mcs-2012-heliu.pdf |date=2019-01-11 }}

* [http://www.periodicvideos.com/videos/002.htm Helium] at ''[[The Periodic Table of Videos]]'' (University of Nottingham)
* [http://boojum.hut.fi/research/theory/helium.html Helium] {{Webarchive|url=https://web.archive.org/web/20050412070034/http://boojum.hut.fi/research/theory/helium.html |date=2005-04-12 }} at the [[Helsinki University of Technology]]; includes pressure-temperature phase diagrams for helium-3 and helium-4
* [http://www.physics.lancs.ac.uk/research/condmatt/ult/index.htm Lancaster University, Ultra Low Temperature Physics]&nbsp;– includes a summary of some low temperature techniques
*[http://www.alfredleitner.com/p/liquid-helium.html Demonstration of superfluid helium] (Alfred Leitner, 1963, 38 min.)

{{Periodic table (navbox)}}{{Subject bar
|book1=Helium
|book2=Period 1 elements
|book3=Noble gases
|book4=Chemical elements (sorted&nbsp;alphabetically)
|book5=Chemical elements (sorted by number)
|portal=Chemistry
|commons=y
|wikt=y
|v=y
|v-search=Helium atom
|b=y
|b-search=Wikijunior:The Elements/Helium
}}{{Authority control}}

[[Category:Helium| ]]
[[Category:Chemical elements]]
[[Category:Noble gases]]
[[Category:Quantum phases]]
[[Category:Airship technology]]
[[Category:Coolants]]
[[Category:Nuclear reactor coolants]]
[[Category:Underwater diving equipment]]
[[Category:E-number additives]]
[[Category:Helios]]