Using a spectrometer to analyze the chromosphere of the sun during a solar eclipse in 1868, French astronomer Jules Janssen noticed an unusual yellow line in the spectrum that he suspected indicated the presence of a yet-undiscovered element. Several months thereafter, English chemists Joseph Norman Lockyer and Edward Franklin observed the same spectral line in sunlight and came to the same conclusion; the two proposed the name “Helium” for the element after Helios, the Greek god of the sun, appropriate for the first element to be discovered in space rather than on earth. Scottish chemist William Ramsay was the first to successfully isolate the element in 1895 by treating a sample of the uranium ore cleveite, thereby proving its existence on earth.
Limited to the scope of the planet, helium is a relatively scarce element, produced only in via the radioactive decay of elements such as uranium and thorium. It is the sixth most abundant gas in the atmosphere at 5.2ppm and one of the only elements light enough to possess escape velocity, rising and exiting the atmosphere at a rate roughly equal to its formation on earth. In space, however, helium is far more prevalent; it is the second most abundant element in the universe after hydrogen, making up 24% of its total observable mass, and is primarily produced in the cores of hydrogen-burning stars that fuse protons into helium nuclei to produce light and heat.
Helium remained unknown by scientists for so long due to its extreme chemical inertness, making it difficult to detect via conventional methods. This inertness is characteristic of the elements known as “noble gases” (Group 18 on the periodic table, which includes neon and argon), whose extreme stability and unwillingness to react with other elements is due to the completeness of their outer valence shells. Odorless, colorless, and nontoxic, helium is the lightest of the noble gases, and the second lightest of all elements in the universe after hydrogen. 99.999% of all helium atoms exists as stable isotope helium-4, composed of two protons, two neutrons, and two electrons in a single shell. This structure structure that yields the most stable and inert element on the periodic table, a monoatomic gas that always exists in pure elemental form in its natural state. Neon is the only element other than helium that has never been observed to bond with other elements in stable compounds; however, at temperatures close to absolute zero and under extreme pressure, helium can form unstable eximer molecules with elements like sodium, fluorine, and nitrogen. The helium-4 nucleus on its own is known as an alpha particle, the particle emitted in alpha-type radioactive decay. Approximate 0.0001% of natural helium is composed of its other stable isotope, helium-3, the nucleus of which has one neutron and is referred to as a helion. The existence of helium-3 was proven by Luis W. Alvarez and Robert Cornog at the Lawrence Berkeley National Laboratory in 1939. Seven other highly unstable isotopes are known; Helium-9, for example, has a half-life of 7 zeptoseconds, or seven sextillionths of a second.
Helium has the lowest solubility in water of any known gas and the lowest melting point of all elements on the periodic table; in fact, it is the only element that cannot be effectively solidified by merely lowering its temperature, as it remains liquid in form down to nearly absolute zero. Close to those temperatures, helium form a superfluid, a quantum state first discovered by Russian physicist Pyotr Kapitsa and John F. Allen in 1937: with almost zero viscosity or entropy, the fluid exhibits superconductivity and can flow up and over the walls of containers, defying the laws of gravity and surface tension, and can pass through nanoscale holes that would normally be impermeable to the gas. At 0.95K, helium can be transformed into a so-called supersolid or quantum solid by applying 25 atmospheres of pressure; to achieve the same result at room temperature requires 114,000 atmospheres of pressure, over 100 times greater than pressure experienced at the deepest point on the ocean floor. The unusual crystalline structure of solid helium exhibits an internal frictionless flow of atoms that impart properties like high compressibility and reversible plasticity.
Billions of cubic feet of helium are produced for commercial consumption each year, primarily from the natural gas wells between Amarillo, Texas and Hugoton, Kansas in the central United States. Helium comprises up to 7% of natural gas deposits and can be isolated from methane and other contaminants via the process of fractional distillation. Both liquid and gaseous helium play a role in the commercial sphere. Helium was first liquefied by Dutch physicist Heike Kamerlingh Onnes in 1913, earning him the Nobel Prize, and approximately 25% of helium’s current commercial use is in liquid form for cryogenic refrigeration. Because helium remains in liquid form even at extremely low temperatures, it is used to cool superconducting wires in high-powered magnets used in magnetic resonance imaging (MRI) and large particle accelerators such as the Large Hadron Collider at CERN; it also serves as a heat-transfer medium for gas-cooled nuclear reactors thanks to its transparency to neutrons and high thermal conductivity. Buoyant in air, helium gas has had well-known use in ballooning since the early 20th century, eventually replacing hydrogen due to the latter’s extreme flammability (as demonstrated by the infamous 1937 Hindenburg airship disaster). The first gas lasers employed a combination of helium and neon, and the air tanks of scuba divers substitute helium for nitrogen to prevent decompression sickness due to helium’s lower blood solubility. Helium has applications in gas chromatography, industrial gas leak detection using helium mass spectrometers, and geological dating of thorium and uranium-containing rocks.
By far the most prominent commercial use for helium gas is providing an inert atmosphere for arc welding and semiconductor component fabrication, particularly during growth of high purity silicon and germanium single crystals. Other emerging roles in advanced technology for helium include allowing further investigation into the properties of quantum superfluids and supersolids, serving as a plasma source in plasma transistors that can operate at temperatures higher than silicon-based transistors, rocket propulsion from the fusion of helium-3 with deuterium, and using spin-polarized helium-3 beams for medical imaging and materials analysis.
Helium is a Block S, Group 18, Period 1 element. The number of electrons in each of Helium's shells is 2 and its electronic configuration is 1s2. In its elemental form helium's CAS number is 7440-59-7. The helium atom has a covalent radius of 28.pm and it's Van der Waals radius is 140.pm. Commercial helium is extracted from natural gas. Helium was discovered by Pierre Janssen and Norman Lockyer in 1868. It was first isolated by William Ramsay, Per Teodor Cleve and Abraham Langlet in 1895.
Helium information, including technical data, properties, other useful facts are specified below. Scientific facts such as the atomic structure, ionization energy, abundance on Earth, conductivity, and thermal properties are included.
|Element Category:||noble gases|
|Group, Period, Block:||18, 1, s|
|Other Names:||Elio, Hélio|
|Melting Point:||-272.2°C, -457.96°F, 0.950 K|
|Boiling Point:||-268.93°C, -452.074°F, 4.220 K|
|Density:||120 (4.22 K) kg·m3|
|Liquid Density @ Melting Point:||0.145 g/cm3|
|Density @ 20°C:||0.0001787 g/cm3|
|Density of Solid:||214 kg·m3|
|Triple Point:||2.177 K, 5.043 kPa|
|Critical Point:||5.1953 K, 0.22746 MPa|
|Heat of Fusion (kJ·mol-1):||0.021|
|Heat of Vaporization (kJ·mol-1):||0.082|
|Heat of Atomization (kJ·mol-1):||0|
|Thermal Conductivity:||0.1513 W·m-1·K-1|
|Molar Heat Capacity:||5R/2 = 20.786 J·mol-1·K-1|
|Speed of Sound:||972 m·s-1|
|Allred Rochow Electronegativity:||5.5|
|Mulliken-Jaffe Electronegativity:||3.49 (s orbital)|
|Refractive Index:||1.000035 (gas; liquid 1.028)|
|Covalent Radius:||28 pm|
|Covalent Radius (Å):||0.37|
|Van der Waals Radius:||140 pm|
|Crystal Structure:||hexagonal close-packed|
|Electron Affinity (kJ·mol-1)||Not stable|
|1st Ionization Energy:||2372.3 kJ·mol-1|
|2nd Ionization Energy:||5250.5 kJ·mol-1|
|3rd Ionization Energy:||N/A|
|Earth - Total:||N/A|
|Mercury - Total:||N/A|
|Venus - Total:||N/A|
|Earth - Seawater (Oceans), ppb by weight:||0.0072|
|Earth - Seawater (Oceans), ppb by atoms:||0.011|
|Earth - Crust (Crustal Rocks), ppb by weight:||5.5|
|Earth - Crust (Crustal Rocks), ppb by atoms:||30|
|Sun - Total, ppb by weight:||2.3E+08|
|Sun - Total, ppb by atoms:||74000000|
|Stream, ppb by weight:||N/A|
|Stream, ppb by atoms:||N/A|
|Meterorite (Carbonaceous), ppb by weight:||N/A|
|Meterorite (Carbonaceous), ppb by atoms:||N/A|
|Typical Human Body, ppb by weight:||N/A|
|Typical Human Body, ppb by atom:||N/A|
|Universe, ppb by weight:||2.3E+08|
|Universe, ppb by atom:||72000000|
|Discovered By:||Pierre Janssen, Norman Lockyer|
|First Isolation:||William Ramsay, Per Teodor Cleve, Abraham Langlet (1895)|
Health, Safety & Transportation Information for Helium
Helium is not toxic and is chemically inert, and thus poses minimal environmental or health threats. At room temperature, helium is typically only harmful when its presence leads to displacement of oxygen in the air, creating potential for asphyxiation. Liquid helium is extremely cold; therefore skin contact with the liquid can cause frostbite, and should be avoided.
|Material Safety Data Sheet||MSDS|
|Transport Information||UN 1046 2.2|
|Globally Harmonized System of
Classification and Labelling (GHS)
Helium has two stable isotopes: 3He and 4He.
|Nuclide||Isotopic Mass||Half-Life||Mode of Decay||Nuclear Spin||Magnetic Moment||Binding Energy (MeV)||Natural Abundance
(% by atom)
|2He||2.015894(2)||N/A||p to 2H||0+(#)||N/A||N/A||-|
|5He||5.01222(5)||700(30)E−24 s||n to 4He||3/2-||N/A||27.405672||-|
|6He||6.0188891(8)||806.7(15) ms||β- to 6Li||0+||N/A||29.269108||-|
|7He||7.028021(18)||2.9(5)E−21 s [159(28) keV]||n to 6He||(3/2)-||N/A||28.824289||-|
|8He||8.033922(7)||119.0(15) ms||β- to 8Li; β- + n to 7Li||0+||N/A||31.407892||-|
|9He||9.04395(3)||7(4)E−21 s||n to 8He||1/2(-#)||N/A||30.258837||-|
|10He||10.05240(8)||2.7(18)E−21 s||2n to 8He||0+||N/A||30.338511||-|
Recent Research & Development for Helium
- Experimental Evidence of Chemical Components in the Bonding of Helium and Neon with Neutral Molecules. Cappelletti D, Bartocci A, Grandinetti F, Falcinelli S, Belpassi L, Tarantelli F, Pirani F. Chemistry. 2015 Mar 6.
- Altering blood flow does not reveal differences between nitrogen and helium kinetics in brain or in skeletal miracle in sheep. Doolette DJ, Upton RN, Grant C. J Appl Physiol (1985). 2015 Mar 1
- Note: Control of liquid helium supply to cryopanels of Kolkata superconducting cyclotron. Bhattacharyya TK, Pal G. Rev Sci Instrum. 2015 Feb
- Resonant two-photon ionization spectroscopy of Al atoms and dimers solvated in helium nanodroplets. Krasnokutski SA, Huisken F. J Chem Phys. 2015 Feb 28
- Fine structure and ionization energy of the 1s2s2p 4P state of the helium negative ion He-. Wang L, Li C, Yan ZC, Drake GW. Phys Rev Lett. 2014 Dec 31
- Complexation of allyl radicals and hydrochloric Acid in helium nanodroplets. Leicht D, Habig D, Schwaab G, Havenith M. J Phys Chem A. 2015 Feb 12
- Comparison of classical and quantal calculations of helium three-body recombination. Pérez-Ríos J, Ragole S, Wang J, Greene CH. J Chem Phys. 2014 Jan 28
- A highly contrasting scanning helium microscope. Fahy A, Barr M, Martens J, Dastoor PC. Rev Sci Instrum. 2015 Feb
- Spectral and dynamic characteristics of helium plasma emission and its effect on a laser-ablated target emission in a double-pulse laser-induced breakdown spectroscopy (LIBS) experiment. Jobiliong E, Suyanto H, Marpaung AM, Abdulmadjid SN, Idris N, Hedwig R, Ramli M, Pardede M, Suliyanti MM, Kagawa K, Fukumoto K, Tjia MO, Lie TJ, Lie ZS, Kurniawan KH. Appl Spectrosc. 2015 Jan
- Helium induced fine structure in the electronic spectra of anthracene derivatives doped into superfluid helium nanodroplets. Pentlehner D, Slenczka A. J Chem Phys. 2015 Jan 7
- Targets Involved in Cardioprotection by the Non-Anaesthetic Noble Gas Helium. Weber NC, Smit KF, Hollmann MW, Preckel B. Curr Drug Targets. 2015 Jan 19.
- Characterization of deuterium clusters mixed with helium gas for an application in beam-target-fusion experiments. Bang W, Quevedo HJ, Bernstein AC, Dyer G, Ihn YS, Cortez J, Aymond F, Gaul E, Donovan ME, Barbui M, Bonasera A, Natowitz JB, Albright BJ, Fernández JC, Ditmire T. Phys Rev E Stat Nonlin Soft Matter Phys. 2014 Dec
- Unusual behavior in magnesium-copper cluster matter produced by helium droplet mediated deposition. Emery SB, Xin Y, Ridge CJ, Buszek RJ, Boatz JA, Boyle JM, Little BK, Lindsay CM. J Chem Phys. 2015 Feb 28
- Excitation of Sodium Atoms Attached to Helium Nanodroplets: The 3p ← 3s Transition Revisited. Loginov E, Hernando A, Beswick JA, Halberstadt N, Drabbels M. J Phys Chem A. 2015 Jan 29.
- Confined helium on Lagrange meshes. Baye D, Dohet-Eraly J. Phys Chem Chem Phys. 2015 Mar 3.
- Para-hydrogen and helium cluster size distributions in free jet expansions based on Smoluchowski theory with kernel scaling. Kornilov O, Toennies JP. J Chem Phys. 2015 Feb 21
- Atomic masses of tritium and helium-3. Myers EG, Wagner A, Kracke H, Wesson BA. Phys Rev Lett. 2015 Jan 9
- Prolonged Helium Postconditioning Protocols during Early Reperfusion Do Not Induce Cardioprotection in the Rat Heart In Vivo: Role of Inflammatory Cytokines. Oei GT, Aslami H, Kerindongo RP, Steenstra RJ, Beurskens CJ, Tuip-de Boer AM, Juffermans NP, Hollmann MW, Preckel B, Weber NC. J Immunol Res. 2015
- Surface protein gradients generated in sealed microchannels using spatially varying helium microplasma. Wettstein P, Priest C, Al-Bataineh SA, Short RD, Bryant PM, Bradley JW, Low SP, Parkinson L, Szili EJ. Biomicrofluidics. 2015 Feb 20
- A configurational study of helium clusters doped with He(*-) and He2 (*.). Rodríguez-Cantano R, González-Lezana T, Villarreal P, Gianturco FA. J Chem Phys. 2015 Mar 14