|
|
| General |
| Name, symbol,
number |
helium, He, 2 |
| Chemical series |
noble gases |
| Group, period,
block |
18, 1, s |
| Appearance |
colorless
 |
| Standard atomic weight |
4.002602(2) g·mol−1 |
| Electron configuration |
1s2 |
| Electrons per shell |
2 |
| Physical properties |
| Phase |
gas |
| Density |
(0 °C, 101.325 kPa)
0.1786 g/L |
| Melting point |
(at 2.5 MPa) 0.95 K
(−272.2 °C, −458.0 °F) |
| Boiling point |
4.22 K
(−268.93 °C, −452.07 °F) |
| Critical point |
5.19 K, 0.227 MPa |
| Heat of fusion |
0.0138 kJ·mol−1 |
| Heat of vaporization |
0.0829 kJ·mol−1 |
| Heat capacity |
(25 °C) 20.786 J·mol−1·K−1 |
|
|
| Atomic properties |
| Crystal structure |
hexagonal close-packed |
| Electronegativity |
no data (Pauling scale) |
| Ionization energies |
1st: 2372.3 kJ/mol |
| 2nd: 5250.5 kJ/mol |
| Atomic radius (calc.) |
31 pm |
| Covalent radius |
32 pm |
| Van der Waals radius |
140 pm |
| Miscellaneous |
| Thermal conductivity |
(300 K) 151.3 m W·m−1·K−1 |
| CAS registry number |
7440-59-7 |
| Selected isotopes |
|
|
| References |
|
Helium (He) is a colorless, odorless, tasteless, non-toxic, inert monatomic chemical element that heads the noble gas series in the periodic table and whose atomic number is 2. Its boiling and melting points are the lowest among the elements and it exists only as a gas
except in extreme conditions. Extreme conditions are also needed to create the small handful of helium compounds, that are all unstable at standard temperature and pressure. It has a second, rare,
stable isotope which is called helium-3. The behavior
of liquid helium-4's two fluid phases, helium I and helium II, is important to researchers
studying quantum mechanics (in particular the phenomenon of superfluidity) and to those looking at the effects that temperatures near absolute zero have on matter (such as superconductivity).
Helium is the second most abundant and second lightest element in the
universe and was one of the elements created in the Big Bang.
In the modern universe almost all new helium is created as a result of the nuclear fusion
of hydrogen in stars. On Earth it is created by the
radioactive decay of much heavier elements (alpha
particles are helium nuclei). After its creation, part of it is trapped with natural
gas in concentrations up to 7% by volume. It is extracted from the natural gas by a low temperature separation process called fractional
distillation.
In 1868 the French astronomer Pierre Janssen first detected helium as an unknown yellow spectral
line signature in light from a solar eclipse. Since then large reserves of helium
have been found in the natural gas fields of the United States, which is by far the largest supplier of the gas. It is used in cryogenics, in deep-sea breathing systems, to cool superconducting
magnets, in helium dating, for inflating balloons,
for providing lift in airships and as a protective gas for many industrial uses (such as
arc welding and growing silicon wafers). A much less
serious use is to temporarily change the timbre and quality of one's voice by inhaling a small volume of the gas (see precautions section below).
Notable characteristics
Gas and plasma phases
Helium is the least reactive member of the noble gas elements, and thus also the least
reactive of all elements; it is inert and monatomic in
virtually all conditions. Due to helium's relatively low molar (molecular) mass, in the gas phase it has a thermal conductivity, specific heat, and
sound conduction velocity that are all greater than any gas, except hydrogen. For similar reasons, and also due to the small size of its molecules, helium's diffusion rate through solids is three times that of air and around 65% that of
hydrogen.[1]
Helium is less water soluble than any other gas known, and helium's index of refraction is closer to unity than that of any other gas. 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 40 K at 1 atmosphere) does it cool upon free expansion. Once precooled below this
temperature, helium can be liquefied through expansion cooling.
Helium discharge tube shaped like the element's atomic symbol
Helium is chemically unreactive under all normal conditions due to its valence of
zero. It is an electrical insulator unless ionized. As with the other noble gases, helium has
metastable energy levels that allow it to remain ionized in an electrical discharge with a voltage below its ionization potential. Helium can form unstable compounds
with tungsten, iodine, fluorine, sulfur and phosphorus when it is
subjected to an electric glow discharge, through electron bombardment or is
otherwise a plasma. HeNe, HgHe10, WHe2 and the molecular ions
He2+, He2++, [[Hydrohelium(1+) ion|HeH+]], and HeD+ have been
created this way. This technique has also allowed the production of the neutral molecule He2, which has a large number
of band systems, and HgHe, which is apparently only held together by polarization
forces.[1] Theoretically, other
compounds, like helium fluorohydride (HHeF), may also be possible.
Helium has been put inside the hollow carbon cage molecules (the fullerenes) by heating under high pressure of the gas. The
neutral molecules formed are stable up to high temperatures. When chemical derivatives of these fullerenes are formed, the helium
stays inside. If helium-3 is used, it can be readily observed by helium NMR spectroscopy. Many
fullerenes containing helium-3 have been reported. These substances fit the definition of compounds in the Handbook of Chemistry
and Physics. They are the first stable neutral helium compounds to be formed.
Throughout the universe, helium is found mostly in a plasma state whose properties
are quite different from atomic helium. In a plasma, helium's electrons and protons are not bound together, 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,
they interact with the Earth's magnetosphere giving rise to Birkeland currents and the aurora.
Solid and liquid phases
-
Helium solidifies only under great pressure. The resulting colorless, almost invisible solid is
highly compressible; applying pressure in the laboratory can decrease its volume by more
than 30%.[2] With a bulk modulus on the order of 5×107 Pa[3] it is 50 times more compressible than water. Unlike any other element,
helium will fail to solidify and remain a liquid down to absolute zero at normal
pressures. This is a direct effect of quantum mechanics: specifically, the zero point
energy of the system is too high to allow freezing. Solid helium requires a temperature of 1–1.5 K (about
−272 °C or −457 °F) and about 25 bar (2.5 MPa) of pressure.[4] 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 crystalline structure.
Solid helium has a density of 0.214 ±0.006 g/ml (1.15 K, 66 atm) with a mean isothermal compressibility of
the solid at 1.15 K between the solidus and 66 atm of 0.0031 ±0.0008/atm. Also, no difference in density was noted
between 1.8 K and 1.5 K. This data projects that T=0 solid helium under 25 bar of pressure (the minimum
required to freeze helium) has a density of 0.187 ±0.009 g/ml.[5]
Helium I state
The boiling point of helium is 4.22 kelvin (-269
oC). The first scientist to obtain liquid helium was the Dutchman Heike
Kamerlingh Onnes. This achievement made the discovery of superconductivity
possible. Above the lambda point of 2.1768 kelvin, the isotope helium-4 exists in a normal colorless liquid state, called
helium I. Like other cryogenic liquids, helium I boils when it is heated. It also
contracts when its temperature is lowered until it reaches the lambda point, when it stops
boiling and suddenly expands. The rate of expansion decreases below the lambda point until about 1 K is reached; at which point
expansion completely stops and helium I starts to contract again.
Helium I has a gas-like index of refraction of 1.026 which makes its surface so hard
to see that floats of Styrofoam are often used to show where the surface is.[6] This colorless liquid has a very
low viscosity and a density 1/8th that of water, which is only 1/4th the value expected from classical physics.[6] Quantum mechanics is needed to explain this
property and thus both types of liquid helium are called quantum fluids, meaning they display atomic properties on a
macroscopic scale. This is probably due to its boiling point being so close to absolute zero, which prevents random molecular
motion (heat) from masking the atomic properties.[6]
Helium II state
Liquid helium below its lambda point begins to exhibit very unusual characteristics, in a state called helium II.
Boiling of helium II is not possible due to its high thermal conductivity; heat
input instead causes evaporation of the liquid directly to gas. The isotope helium-3 also
has a superfluid phase, but only at much lower temperatures; as a result, less is known about such properties in the isotope
helium-3.
Helium II will "creep" along surfaces in order to find its own 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 II would creep out and escape
Helium II is a superfluid, a quantum-mechanical state of matter with strange properties.
For example, when it flows through even capillaries of 10−7 to 10−8 m width it has no measurable
viscosity. However, when measurements were done between two moving discs, a viscosity
comparable to that of gaseous helium was observed. Current 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.[7]
Helium II also exhibits a "creeping" effect. When a surface extends past the level of helium II, the helium II moves along the
surface, seemingly against the force of gravity. Helium 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
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.[8][9] As a result of this creeping behavior and helium II's ability to leak rapidly through tiny openings,
it is very difficult to confine liquid helium. Unless the container is carefully constructed, the helium 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 waves in shallow water, but rather than
gravity, the restoring force is the Van der Waals force.[10] These waves are known as third sound.
In the fountain effect, a chamber is constructed which is connected to a reservoir of helium II by a 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.[11]
The thermal conductivity of helium II is greater than that of any other known substance, a million times that of helium I and
several hundred times that of copper. This is because heat conduction occurs by an exceptional
quantum-mechanical mechanism. Most materials that conduct heat well have a valence band of
free electrons which serve to transfer the heat. Helium II has no such valence band but nevertheless conducts heat well. The
flow of heat is governed by equations that are similar
to the wave equation used to characterize sound propagation
in air. So when heat is introduced, it will move at 20 meters per second at 1.8 K through helium II as waves in a phenomenon
called second sound.[8]
Applications
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 inertness. Helium is commercially available in either liquid or gaseous form. As a liquid, it can be supplied in
small containers called dewars which hold up to 1,000 liters of helium, or in large ISO containers which have nominal capacities
as large as 11,000 gallons (41,637 liters). In gaseous form, small quantities of helium are supplied in high pressure cylinders
holding up to 300 standard cubic feet, while large quantities of high pressure gas are supplied in tube trailers which have
capacities of up to 180,000 standard cubic feet.
As a lighter than air gas, airships and
balloons are inflated with helium for lift. In airships, helium is preferred over hydrogen
because it is not flammable and has 92.64% of the buoyancy (or lifting power) of the
alternative hydrogen (see calculation.)
Due to its low solubility in water, the major part of human blood, air mixtures of helium with
oxygen and nitrogen (Trimix), with oxygen only (Heliox), with common air
(heliair), and with hydrogen and oxygen
(hydreliox), are used in deep-sea breathing systems to reduce the high-pressure risk of
nitrogen narcosis, decompression
sickness, and oxygen toxicity.
Liquid helium can be used as a cryogenic material, and is used to cool certain metals to produce superconductivity, such as in superconducting magnets
use in magnetic resonance imaging and NMR
spectroscopy.
Due to its inertness, helium is used as a shielding gas in arc welding processes on materials that are contaminated easily by air. It is especially useful in overhead
welding, because it is lighter than air and thus floats, whereas other shielding gases sink. It is also used as a protective gas
in growing silicon and germanium crystals, in
titanium and zirconium production, in gas chromatography, and as an atmosphere for protecting historical documents. This property
also makes it useful in supersonic wind tunnels. In rocketry, helium is used as an ullage medium to displace fuel and
oxidizers in storage tanks 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 vehicles. For example, the
Saturn V booster used in the Apollo program needed
about 13 million cubic feet (370,000 m³) of helium to launch.[2]
Apart from its inertness, helium has high thermal conductivity, neutron transparency, and does not form radioactive isotopes under reactor conditions, so it is used
as a coolant in some nuclear reactors, such as pebble-bed reactors. The high thermal conductivity and sound velocity of helium is also desirable in
thermoacoustic refrigeration. The inertness of helium adds to the
environmental advantage of this technology over conventional refrigeration systems which may contribute to ozone depleting and
global warming effects.
Other applications include:
- The gain medium of the helium-neon
laser is a mixture of helium and neon.
- Because it diffuses through solids at a rate three times that of air, helium is used to
detect leaks in high-vacuum equipment and high-pressure containers.
- Because of its extremely low index of refraction, the use of helium reduces the
distorting effects of temperature variations in the space between lenses in some
telescopes.
- The age of rocks and minerals that contain
uranium and thorium, radioactive elements that emit helium nuclei called alpha particles,
can be discovered by measuring the level of helium with a process known as helium
dating.
- Because helium alone is less dense than atmospheric air, it will change the timbre (not
pitch[12])
of a person's voice when inhaled. However, inhaling it from a typical commercial source, such as that used to fill balloons, can
be dangerous due to the risk of asphyxiation from lack of oxygen, and the number of
contaminants that may be present. These could include trace amounts of other gases, in addition to aerosolized lubricating
oil.
History
Scientific discoveries
Evidence of helium was first detected on August 18, 1868 as a
bright yellow line with a wavelength of 587.49 nanometres in the spectrum of the chromosphere of the Sun, by French astronomer Pierre Janssen during a total solar eclipse in Guntur, India. 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
D3 line, for it was near the known D1 and D2 lines of
sodium,[13] and concluded that it was caused by an element
in the Sun unknown on Earth. He and English chemist Edward Frankland named the element
with the Greek word for the Sun, ἥλιος (helios)[14]
On 26 March 1895 British chemist William Ramsay isolated helium on Earth by treating the mineral cleveite with mineral acids.
Ramsay was looking for argon but, after separating nitrogen and
oxygen from the gas liberated by sulfuric acid, noticed a
bright-yellow line that matched the D3 line observed in the spectrum of the Sun.[15][16][17][18] [15] These samples were identified as helium by Lockyer and British physicist William Crookes. It was independently isolated from cleveite 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.[19] Helium was also isolated by the 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. His letter of congratulations to Ramsay offers an interesting case of discovery and
near-discovery in science.[20]
In 1907, Ernest Rutherford and Thomas Royds demonstrated that an alpha particle is a helium nucleus. In 1908, helium was first
liquefied by Dutch physicist Heike Kamerlingh Onnes by cooling the gas to less
than one kelvin. He tried to solidify it by further reducing the temperature but failed
because helium does not have a triple point temperature where the solid, liquid, and gas
phases are at equilibrium. It was first solidified in 1926 by his student Willem Hendrik
Keesom by subjecting helium to 25 atmospheres of pressure.
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. In 1972, the
same phenomenon was observed in helium-3 by American physicists Douglas D. Osheroff,
David M. Lee, and Robert C.
Richardson.
History of extraction and use
After an oil drilling operation in 1903 in Dexter, Kansas, USA 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 contained, by volume, 72% nitrogen, 15% methane—insufficient to make the gas combustible, 1% hydrogen, and 12% of an
unidentifiable gas.[21] With further
analysis, Cady and McFarland discovered that 1.84% of the gas sample was helium.[22] Far from being a rare element, helium was present in vast quantities under the American Great
Plains, available for extraction from natural gas.
This put the United States in an excellent position to become the world's leading
supplier of helium. Following a suggestion by Sir