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Beryllium, 4Be
A dark, crystalline piece of rock standing on a piece of graph paper
Beryllium
Pronunciation/bəˈrɪliəm/ (bə-RIL-ee-əm)
Appearancewhite-gray metallic
Standard atomic weight Ar°(Be)
Beryllium in the periodic table
Hydrogen Helium
Lithium Beryllium Boron Carbon Nitrogen Oxygen Fluorine Neon
Sodium Magnesium Aluminium Silicon Phosphorus Sulfur Chlorine Argon
Potassium Calcium Scandium Titanium Vanadium Chromium Manganese Iron Cobalt Nickel Copper Zinc Gallium Germanium Arsenic Selenium Bromine Krypton
Rubidium Strontium Yttrium Zirconium Niobium Molybdenum Technetium Ruthenium Rhodium Palladium Silver Cadmium Indium Tin Antimony Tellurium Iodine Xenon
Caesium Barium Lanthanum Cerium Praseodymium Neodymium Promethium Samarium Europium Gadolinium Terbium Dysprosium Holmium Erbium Thulium Ytterbium Lutetium Hafnium Tantalum Tungsten Rhenium Osmium Iridium Platinum Gold Mercury (element) Thallium Lead Bismuth Polonium Astatine Radon
Francium Radium Actinium Thorium Protactinium Uranium Neptunium Plutonium Americium Curium Berkelium Californium Einsteinium Fermium Mendelevium Nobelium Lawrencium Rutherfordium Dubnium Seaborgium Bohrium Hassium Meitnerium Darmstadtium Roentgenium Copernicium Nihonium Flerovium Moscovium Livermorium Tennessine Oganesson


Be

Mg
lithiumberylliumboron
Atomic number (Z)4
Groupgroup 2 (alkaline earth metals)
Periodperiod 2
Block  s-block
Electron configuration[He] 2s2
Electrons per shell2, 2
Physical properties
Phase at STPsolid
Melting point1560 K ​(1287 °C, ​2349 °F)
Boiling point2742 K ​(2469 °C, ​4476 °F)
Density (at 20 °C)1.845 g/cm3[3]
when liquid (at m.p.)1.690 g/cm3
Critical point5400 K, 46 MPa (estimated)[4]
Heat of fusion12.2 kJ/mol
Heat of vaporization292 kJ/mol
Molar heat capacity16.443 J/(mol·K)
Vapor pressure
P (Pa) 1 10 100 1 k 10 k 100 k
at T (K) 1462 1608 1791 2023 2327 2742
Atomic properties
Oxidation statescommon: +2
0,[6] +1[8]
ElectronegativityPauling scale: 1.57
Ionization energies
  • 1st: 899.5 kJ/mol
  • 2nd: 1757.1 kJ/mol
  • 3rd: 14,848.7 kJ/mol
  • (more)
Atomic radiusempirical: 112 pm
Covalent radius96±3 pm
Van der Waals radius153 pm
Color lines in a spectral range
Spectral lines of beryllium
Other properties
Natural occurrenceprimordial
Crystal structurehexagonal close-packed (hcp) (hP2)
Lattice constants
Hexagonal close packed crystal structure for beryllium
a = 228.60 pm
c = 358.42 pm (at 20 °C)[3]
Thermal expansion10.98×10−6/K (at 20 °C)[3][a]
Thermal conductivity200 W/(m⋅K)
Electrical resistivity36 nΩ⋅m (at 20 °C)
Magnetic orderingdiamagnetic
Molar magnetic susceptibility−9.0×10−6 cm3/mol[10]
Young's modulus287 GPa
Shear modulus132 GPa
Bulk modulus130 GPa
Speed of sound thin rod12,890 m/s (at r.t.)[11]
Poisson ratio0.032
Mohs hardness6.0
Vickers hardness1670 MPa
Brinell hardness590–1320 MPa
CAS Number7440-41-7
History
Namingafter mineral Beryl, from Greek βήρυλλος, which referred to various blue-green stones
DiscoveryLouis Nicolas Vauquelin (1798)
First isolationFriedrich Wöhler & Antoine Bussy (1828)
Isotopes of beryllium
Main isotopes[12] Decay
Isotope abun­dance half-life (t1/2) mode pro­duct
7Be trace 53.22 d ε 7Li
8Be synth 8.2×10−17 s[n 1] α 4He
9Be 100% stable
10Be trace 1.387×106 y β 10B
 Category: Beryllium
| references

Beryllium is a chemical element; it has symbol Be and atomic number 4. It is a steel-gray, hard, strong, lightweight and brittle alkaline earth metal. It is a divalent element that occurs naturally only in combination with other elements to form minerals. Gemstones high in beryllium include beryl (aquamarine, emerald, red beryl) and chrysoberyl. It is a relatively rare element in the universe, usually occurring as a product of the spallation of larger atomic nuclei that have collided with cosmic rays. Within the cores of stars, beryllium is depleted as it is fused into heavier elements. Beryllium constitutes about 0.0004 percent by mass of Earth's crust. The world's annual beryllium production of 220 tons is usually manufactured by extraction from the mineral beryl, a difficult process because beryllium bonds strongly to oxygen.

In structural applications, the combination of high flexural rigidity, thermal stability, thermal conductivity and low density (1.85 times that of water) make beryllium a desirable aerospace material for aircraft components, missiles, spacecraft, and satellites.[13] Because of its low density and atomic mass, beryllium is relatively transparent to X-rays and other forms of ionizing radiation; therefore, it is the most common window material for X-ray equipment and components of particle detectors.[13] When added as an alloying element to aluminium, copper (notably the alloy beryllium copper), iron, or nickel, beryllium improves many physical properties.[13] For example, tools and components made of beryllium copper alloys are strong and hard and do not create sparks when they strike a steel surface. In air, the surface of beryllium oxidizes readily at room temperature to form a passivation layer 1–10 nm thick that protects it from further oxidation and corrosion.[14] The metal oxidizes in bulk (beyond the passivation layer) when heated above 500 °C (932 °F),[15] and burns brilliantly when heated to about 2,500 °C (4,530 °F).[16]

The commercial use of beryllium requires the use of appropriate dust control equipment and industrial controls at all times because of the toxicity of inhaled beryllium-containing dusts that can cause a chronic life-threatening allergic disease, berylliosis, in some people.[17] Berylliosis is typically manifested by chronic pulmonary fibrosis and, in severe cases, right sided heart failure and death.[18]

Characteristics

[edit]

Physical properties

[edit]

Beryllium is a steel gray and hard metal that is brittle at room temperature and has a close-packed hexagonal crystal structure.[13] It has exceptional stiffness (Young's modulus 287 GPa) and a melting point of 1287 °C. The modulus of elasticity of beryllium is approximately 35% greater than that of steel. The combination of this modulus and a relatively low density results in an unusually fast sound conduction speed in beryllium – about 12.9 km/s at ambient conditions. Among all metals, beryllium dissipates the most heat per unit weight, with both high specific heat (1925 J·kg−1·K−1) and thermal conductivity (216 W·m−1·K−1). Beryllium's conductivity and relatively low coefficient of linear thermal expansion (11.4×10−6 K−1), make it uniquely stable under extreme temperature differences.[19]: 11.1 

Nuclear properties

[edit]

Naturally occurring beryllium, save for slight contamination by the radioisotopes created by cosmic rays, is isotopically pure beryllium-9,[1] which has a nuclear spin of 3/2.[12] The inelastic scattering cross section of beryllium increases with relation to neutron energy,[20] allowing for significant slowing of higher-energy neutrons.[21] Therefore, it works as a neutron reflector and neutron moderator; the exact strength of neutron slowing depends on the purity and size of the crystallites in the material.[22]

The isotope 9Be can undergo a (n, 2n) neutron reaction with fast neutrons, to produce 8Be, which almost immediately breaks into two alpha particles. Thus, for high-energy neutrons, beryllium is a neutron multiplier, releasing more neutrons than it absorbs. This nuclear reaction is:[23]

9
4
Be
+ n → 2 4
2
He
+ 2 n

The isotope can liberate the neutron when struck by an alpha particle.[19] The nuclear reaction

9
4
Be
+ 4
2
He
12
6
C
+ n

is strongly exothermic, liberating a fast neutron.[23]

The isotope can also release the neutron when absorbing a gamma ray of sufficient energy (photodisintegration)[24] at a useful cross-section:

9
4
Be
+ gamma → 2 4
2
He
+ n

Thus, natural beryllium bombarded by alpha or gamma radiation from a suitable radioisotope is the most common radioisotope-powered neutron source for laboratory use.[25][26]

Finally, small amounts of tritium are also liberated by the high-energy neutrons in the three-step nuclear reaction

9
4
Be
+ n → 4
2
He
+ 6
2
He
,    6
2
He
6
3
Li
+ β,    6
3
Li
+ n → 4
2
He
+ 3
1
H

6
2
He
has a half-life of only 0.8 seconds, β is an electron, and 6
3
Li
has a high neutron absorption cross section. This is equivalent to the neutron-multiplication reaction with three output neutrons replaced by a triton, and a beta decay allowing that conversion. Tritium is a radioisotope of concern in nuclear reactor waste streams.[27]

Optical properties

[edit]

As a metal, beryllium is transparent or translucent to most wavelengths of X-rays and gamma rays, making it useful for the output windows of X-ray tubes and other such apparatus.[28]

Isotopes and nucleosynthesis

[edit]

Natural beryllium is made up of solely the stable isotope beryllium-9. Beryllium is the only monoisotopic element with an even atomic number.[1]

Beryllium-7 and beryllium-8 are key intermediates in stellar nucleosynthesis, but do not last long. It is believed that the beryllium in the universe was created in the interstellar medium when cosmic rays induced fission in heavier elements found in interstellar gas and dust, a process called cosmic ray spallation.[29][30]

About one billionth (10−9) of the primordial atoms created in the Big Bang nucleosynthesis were 7Be. This is a consequence of the low density of matter when the temperature of the universe cooled enough for small nuclei to be stable. Creating such nuclei requires nuclear collisions that are rare at low density.[31]: 297  Although 7Be is unstable and decays by electron capture into 7Li, with a half-life of 53.22 days under standard conditions, in the early universe the atoms were fully ionized and electron capture not significant. The conversion of 7Be to Li was only complete near the time of recombination.[32]

The isotope 7Be is also a cosmogenic nuclide and shows an atmospheric abundance inversely proportional to solar activity.[33] It decays exclusively by electron capture, and the 2s electrons of beryllium are the valence electrons responsible for chemical bonding. Therefore, when 7Be decays by L-electron capture, it does so by taking electrons from its atomic orbitals that may be participating in bonding. This makes its decay rate dependent to a measurable degree upon its chemical surroundings  – a rare occurrence in nuclear decay.[34]

Be-7 is also produced in cooling water of high-energy accelerators; it can be extracted from the water at high purity and sold for scientific experiments.[35]

Plot showing variations in solar activity, including variation in sunspot number (red) and 10Be concentration (blue). Note that the beryllium scale is inverted, so increases on this scale indicate lower 10Be levels

The isotope 10Be is similarly cosmogenic, and is produced in the same way - by cosmic ray spallation of nitrogen and oxygen.[36] Its behavior differ only because of its much longer half-life of 1.387 million years. It entirely accumulates at the soil surface and has a long residence time before decaying to boron-10. Thus, 10Be and its daughter product are used to examine natural soil erosion, soil formation and the development of lateritic soils, and as a proxy for measurement of the variations in solar activity and the age of ice cores.[37] As with 7Be, production of 10Be is inversely related to solar activity, because increased solar wind during periods of high solar activity decreases the flux of galactic cosmic rays that reach the Earth.[38] Nuclear explosions also form 10Be by the reaction of fast neutrons with 13C in the carbon dioxide in air. This is one of the indicators of past activity at nuclear weapon test sites.[39]

8Be is unstable but has a ground state resonance with an important role in the triple-alpha process in stellar helium burning. As first proposed by British astronomer Sir Fred Hoyle based solely on astrophysical analysis, the energy levels of 8Be and 12C allow carbon nucleosynthesis by increasing the effective cross-section between the three alpha particles in the carbon production process. The main carbon-producing reaction in the universe is where 4He is an alpha particle.[40]

The exotic isotopes 11Be and 14Be are known to exhibit a nuclear halo. That is, their nuclei have, respectively, 1 and 4 neutrons orbiting substantially outside the expected nuclear radius[41] and in each case the core the neutrons float around is one of 10Be.

Occurrence

[edit]
Beryllium ore with a U.S. penny for scale
Emerald is a naturally occurring compound of beryllium.

Beryllium is found in over 100 minerals,[42] but most are uncommon to rare. The more common beryllium-containing minerals include: bertrandite (Be4Si2O7(OH)2), beryl (Al2Be3Si6O18), chrysoberyl (Al2BeO4) and phenakite (Be2SiO4). Precious forms of beryl are aquamarine, red beryl and emerald.[19][43][44] The green color in gem-quality forms of beryl comes from varying amounts of chromium (about 2% for emerald).[45]

The two main ores of beryllium, beryl and bertrandite, are found in Argentina, Brazil, India, Madagascar, Russia and the United States.[45] Total world reserves of beryllium ore are greater than 400,000 tonnes.[45]

The Sun has a concentration of 0.1 parts per billion (ppb) of beryllium.[46] Beryllium has a concentration of 2 to 6 parts per million (ppm) in the Earth's crust and is the 47th-most abundant element.[47][48] It is most concentrated (6 ppm) in the soils.[48] Trace amounts of 9Be are found in the Earth's atmosphere.[48] The concentration of beryllium in sea water is 0.2–0.6 parts per trillion.[48][49] In stream water, however, beryllium is more abundant, with a concentration of 0.1 ppb.[50]

Extraction

[edit]

The extraction of beryllium from its compounds is a difficult process due to its high affinity for oxygen at elevated temperatures, and its ability to reduce water when its oxide film is removed. Currently the United States, China and Kazakhstan are the only three countries involved in the industrial-scale extraction of beryllium.[51] Kazakhstan produces beryllium from a concentrate stockpiled before the breakup of the Soviet Union around 1991. This resource had become nearly depleted by mid-2010s.[52]

Production of beryllium in Russia was halted in 1997, and is planned to be resumed in the 2020s.[53][54]

A bead of beryllium from a melt

Beryllium is most commonly extracted from the mineral beryl, which is either sintered using an extraction agent or melted into a soluble mixture. The sintering process involves mixing beryl with sodium fluorosilicate and soda at 770 °C (1,420 °F) to form sodium fluoroberyllate, aluminium oxide and silicon dioxide.[13] Beryllium hydroxide is precipitated from a solution of sodium fluoroberyllate and sodium hydroxide in water. The extraction of beryllium using the melt method involves grinding beryl into a powder and heating it to 1,650 °C (3,000 °F). The melt is quickly cooled with water and then reheated 250 to 300 °C (482 to 572 °F) in concentrated sulfuric acid, mostly yielding beryllium sulfate and aluminium sulfate. Aqueous ammonia is then used to remove the aluminium and sulfur, leaving beryllium hydroxide.[13]

Beryllium hydroxide created using either the sinter or melt method is then converted into beryllium fluoride or beryllium chloride. To form the fluoride, aqueous ammonium hydrogen fluoride is added to beryllium hydroxide to yield a precipitate of ammonium tetrafluoroberyllate, which is heated to 1,000 °C (1,830 °F) to form beryllium fluoride.[13] Heating the fluoride to 900 °C (1,650 °F) with magnesium forms finely divided beryllium, and additional heating to 1,300 °C (2,370 °F) creates the compact metal.[13] Heating beryllium hydroxide forms beryllium oxide, which becomes beryllium chloride when combined with carbon and chlorine. Electrolysis of molten beryllium chloride is then used to obtain the metal.[13]

Chemical properties

[edit]

A beryllium atom has the electronic configuration [He] 2s2. The predominant oxidation state of beryllium is +2; the beryllium atom losing both of its valence electrons. Beryllium's chemical behavior is largely a result of its small atomic and ionic radii. It thus has very high ionization potentials and does not form divalent cations. Instead it forms two covalent bonds with a tendency to polymerize, as in solid BeCl2.[13]: 37  Its chemistry has similarities to that of aluminium, an example of a diagonal relationship.[55]: 107  In the other direction, beryllium is attracted to electron density, generating intermolecular forces similar to hydrogen bonding.[56]

At room temperature, the surface of beryllium forms a 1−10 nm-thick oxide passivation layer that prevents further reactions with air, except for gradual thickening of the oxide up to about 25 nm. When heated above about 500 °C, oxidation into the bulk metal progresses along grain boundaries.[15] Once the metal is ignited in air by heating above the oxide melting point around 2500 °C, beryllium burns brilliantly,[16] forming a mixture of beryllium oxide and beryllium nitride. Beryllium dissolves readily in non-oxidizing acids, such as HCl and diluted H2SO4, but not in nitric acid or water as this forms the oxide. This behavior is similar to that of aluminium. Beryllium also dissolves and reacts with alkali solutions.[13][55]: 112 

Binary compounds of beryllium(II) are polymeric in the solid state. BeF2 has a silica-like structure with corner-shared BeF4 tetrahedra. BeCl2 and BeBr2 have chain structures with edge-shared tetrahedra. Beryllium oxide, BeO, is a white refractory solid which has a wurtzite crystal structure and a thermal conductivity as high as some metals. BeO is amphoteric. Beryllium sulfide, selenide and telluride are known, all having the zincblende structure.[57] Beryllium nitride, Be3N2, is a high-melting-point compound which is readily hydrolyzed. Beryllium azide, BeN6 is known and beryllium phosphide, Be3P2 has a similar structure to Be3N2. A number of beryllium borides are known, such as Be5B, Be4B, Be2B, BeB2, BeB6 and BeB12. Beryllium carbide, Be2C, is a refractory brick-red compound that reacts with water to give methane.[57] Beryllium silicides have been identified in the form of variously sized nanoclusters,[58] formed through a spontaneous reaction between pure beryllium and silicon.[59] The halides BeX2 (X = F, Cl, Br, and I) have a linear monomeric molecular structure in the gas phase.[55]: 117 

Lower oxidation states complexes of beryllium are exceedingly rare. For example, a stable complex with a Be-Be bond, which formally features beryllium in the +1 oxidation state, has been described.[7] Beryllium in the 0 oxidation state is also known in a complex with a Mg-Be bond.[5]

Aqueous solutions

[edit]
Schematic structure of basic beryllium acetate
Beryllium hydrolysis. Water molecules attached to Be are omitted in this diagram
Structure of the trimeric hydrolysis product of beryllium(II)

Solutions of beryllium salts, such as beryllium sulfate and beryllium nitrate, are acidic because of hydrolysis of the [Be(H2O)4]2+ ion. The concentration of the first hydrolysis product, [Be(H2O)3(OH)]+, is less than 1% of the beryllium concentration. The most stable hydrolysis product is the trimeric ion [Be3(OH)3(H2O)6]3+. Beryllium hydroxide, Be(OH)2, is insoluble in water at pH 5 or more. Consequently, beryllium compounds are generally insoluble at biological pH. Because of this, inhalation of beryllium metal dust leads to the development of the fatal condition of berylliosis. Be(OH)2 dissolves in strongly alkaline solutions.[60]

Beryllium(II) forms few complexes with monodentate ligands because the water molecules in the aquo-ion, [Be(H2O)4]2+ are bound very strongly to the beryllium ion. Notable exceptions are the series of water-soluble complexes with the fluoride ion:[61]

[Be(H2O)4]2+ + n F ⇌ Be[(H2O)2−nFn]2− + n H2O

Beryllium(II) forms many complexes with bidentate ligands containing oxygen-donor atoms.[60] The species [Be3O(H2PO4)6]2− is notable for having a 3-coordinate oxide ion at its center. Basic beryllium acetate, Be4O(OAc)6, has an oxide ion surrounded by a tetrahedron of beryllium atoms.[62]

With organic ligands, such as the malonate ion, the acid deprotonates when forming the complex. The donor atoms are two oxygens.

H2A + [Be(H2O)4]2+ ⇌ [BeA(H2O)2] + 2 H+ + 2 H2O
H2A + [BeA(H2O)2] ⇌ [BeA2]2− + 2 H+ + 2 H2O

The formation of a complex is in competition with the metal ion-hydrolysis reaction and mixed complexes with both the anion and the hydroxide ion are also formed. For example, derivatives of the cyclic trimer are known, with a bidentate ligand replacing one or more pairs of water molecules.[63]

Aliphatic hydroxycarboxylic acids such as glycolic acid form rather weak monodentate complexes in solution, in which the hydroxyl group remains intact. In the solid state, the hydroxyl group may deprotonate: a hexamer, Na4[Be6(OCH2(O)O)6], was isolated long ago.[63][64] Aromatic hydroxy ligands (i.e. phenols) form relatively strong complexes. For example, log K1 and log K2 values of 12.2 and 9.3 have been reported for complexes with tiron.[63][65]

Beryllium has generally a rather poor affinity for ammine ligands.[63][66] There are many early reports of complexes with amino acids, but unfortunately they are not reliable as the concomitant hydrolysis reactions were not understood at the time of publication. Values for log β of ca. 6 to 7 have been reported. The degree of formation is small because of competition with hydrolysis reactions.[63][66]

Organic chemistry

[edit]

Organometallic beryllium compounds are known to be highly reactive.[67] Examples of known organoberyllium compounds are dineopentylberyllium,[68] beryllocene (Cp2Be),[69][70][71][72] diallylberyllium (by exchange reaction of diethyl beryllium with triallyl boron),[73] bis(1,3-trimethylsilylallyl)beryllium,[74] Be(mes)2,[67] and (beryllium(I) complex) diberyllocene.[7] Ligands can also be aryls[75] and alkynyls.[76]

History

[edit]

The mineral beryl, which contains beryllium, has been used at least since the Ptolemaic dynasty of Egypt.[77] The Papyrus Graecus Holmiensis, written in the third or fourth century CE, contains notes on how to prepare artificial emerald and beryl.[78]

Louis-Nicolas Vauquelin discovered beryllium

Early analyses of emeralds and beryls by Martin Heinrich Klaproth, Torbern Olof Bergman, Franz Karl Achard, and Johann Jakob Bindheim [de] always yielded similar elements, leading to the mistaken conclusion that both substances are aluminium silicates.[79] Mineralogist René Just Haüy discovered that both crystals are geometrically identical, and he asked chemist Louis-Nicolas Vauquelin for a chemical analysis.[77]

In a 1798 paper read before the Institut de France, Vauquelin reported that he found a new "earth" by dissolving aluminium hydroxide from emerald and beryl in an additional alkali.[80] The editors of the journal Annales de chimie et de physique named the new earth "glucine" for the sweet taste of some of its compounds.[81][82] The name beryllium was first used by Friedrich Wöhler in 1828.[83][84] Both beryllium and glucinum were used concurrently until 1949, when the IUPAC adopted beryllium as the standard name of the element.[85][86]

Friedrich Wöhler was one of the men who independently isolated beryllium

Friedrich Wöhler[84] and Antoine Bussy[87] independently isolated beryllium in 1828 by the chemical reaction of metallic potassium with beryllium chloride, as follows:

BeCl2 + 2 K → 2 KCl + Be

Using an alcohol lamp, Wöhler heated alternating layers of beryllium chloride and potassium in a wired-shut platinum crucible. The above reaction immediately took place and caused the crucible to become white hot. Upon cooling and washing the resulting gray-black powder, he saw that it was made of fine particles with a dark metallic luster.[88] The highly reactive potassium had been produced by the electrolysis of its compounds.[89] He did not succeed to melt the beryllium particles.[88]

The direct electrolysis of a molten mixture of beryllium fluoride and sodium fluoride by Paul Lebeau in 1898 resulted in the first pure (99.5 to 99.8%) samples of beryllium.[88] However, industrial production started only after the First World War. The original industrial involvement included subsidiaries and scientists related to the Union Carbide and Carbon Corporation in Cleveland, Ohio, and Siemens & Halske AG in Berlin. In the US, the process was ruled by Hugh S. Cooper, director of The Kemet Laboratories Company. In Germany, the first commercially successful process for producing beryllium was developed in 1921 by Alfred Stock and Hans Goldschmidt.[90]

A sample of beryllium was bombarded with alpha rays from the decay of radium in a 1932 experiment by James Chadwick that uncovered the existence of the neutron.[45] This same method is used in one class of radioisotope-based laboratory neutron sources that produce 30 neutrons for every million α particles.[47]

Beryllium production saw a rapid increase during World War II due to the rising demand for hard beryllium-copper alloys and phosphors for fluorescent lights. Most early fluorescent lamps used zinc orthosilicate with varying content of beryllium to emit greenish light. Small additions of magnesium tungstate improved the blue part of the spectrum to yield an acceptable white light. Halophosphate-based phosphors replaced beryllium-based phosphors after beryllium was found to be toxic.[91]

Electrolysis of a mixture of beryllium fluoride and sodium fluoride was used to isolate beryllium during the 19th century. The metal's high melting point makes this process more energy-consuming than corresponding processes used for the alkali metals. Early in the 20th century, the production of beryllium by the thermal decomposition of beryllium iodide was investigated following the success of a similar process for the production of zirconium, but this process proved to be uneconomical for volume production.[92]

Pure beryllium metal did not become readily available until 1957, even though it had been used as an alloying metal to harden and toughen copper much earlier.[45] Beryllium could be produced by reducing beryllium compounds such as beryllium chloride with metallic potassium or sodium. Currently, most beryllium is produced by reducing beryllium fluoride with magnesium.[93] The price on the American market for vacuum-cast beryllium ingots was about $338 per pound ($745 per kilogram) in 2001.[94]

Between 1998 and 2008, the world's production of beryllium had decreased from 343 to about 200 tonnes. It then increased to 230 metric tons by 2018, of which 170 tonnes came from the United States.[95][96]

Etymology

[edit]

Beryllium was named for the semiprecious mineral beryl, from which it was first isolated.[97][98][99] Martin Klaproth, having independently determined that beryl and emerald share an element, preferred the name "beryllina" due to the fact that yttria also formed sweet salts.[100][83]

Although Humphry Davy failed to isolate it, he proposed the name glucium for the new metal, derived from the name glucina for the earth it was found in; altered forms of this name, glucinium or glucinum (symbol Gl) continued to be used into the 20th century.[101]

Applications

[edit]

Radiation windows

[edit]
Beryllium target which converts a proton beam into a neutron beam[102]
A square beryllium foil mounted in a steel case to be used as a window between a vacuum chamber and an X-ray microscope. Beryllium is highly transparent to X-rays owing to its low atomic number.

Because of its low atomic number and very low absorption for X-rays, the oldest and still one of the most important applications of beryllium is in radiation windows for X-ray tubes.[45] Extreme demands are placed on purity and cleanliness of beryllium to avoid artifacts in the X-ray images. Beryllium is used in X-ray windows because it is transparent to X-rays, allowing for clearer and more efficient imaging.[103] Thin beryllium foils are used as radiation windows for X-ray detectors, and their extremely low absorption minimizes the heating effects caused by high-intensity, low energy X-rays typical of synchrotron radiation. Vacuum-tight windows and beam-tubes for radiation experiments on synchrotrons are manufactured exclusively from beryllium. In scientific setups for various X-ray emission studies (e.g., energy-dispersive X-ray spectroscopy) the sample holder is usually made of beryllium because its emitted X-rays have much lower energies (≈100 eV) than X-rays from most studied materials.[19]

Low atomic number also makes beryllium relatively transparent to energetic particles. Therefore, it is used to build the beam pipe around the collision region in particle physics setups, such as all four main detector experiments at the Large Hadron Collider (ALICE, ATLAS, CMS, LHCb),[104] the Tevatron and at SLAC. The low density of beryllium allows collision products to reach the surrounding detectors without significant interaction, its stiffness allows a powerful vacuum to be produced within the pipe to minimize interaction with gases, its thermal stability allows it to function correctly at temperatures of only a few degrees above absolute zero, and its diamagnetic nature keeps it from interfering with the complex multipole magnet systems used to steer and focus the particle beams.[105]

Mechanical applications

[edit]

Because of its stiffness, light weight and dimensional stability over a wide temperature range, beryllium metal is used for lightweight structural components in the defense and aerospace industries in high-speed aircraft, guided missiles, spacecraft, and satellites, including the James Webb Space Telescope. Several liquid-fuel rockets have used rocket nozzles made of pure beryllium.[106][107] The high elastic stiffness of beryllium has led to its extensive use in precision instrumentation, e.g. in inertial guidance systems and in the support mechanisms for optical systems.[19] Beryllium powder was itself studied as a rocket fuel, but this use has never materialized.[45] A small number of extreme high-end bicycle frames have been built with beryllium.[108] From 1998 to 2000, the McLaren Formula One team used Mercedes-Benz engines with beryllium–aluminium alloy pistons.[109] The use of beryllium engine components was banned following a protest by Scuderia Ferrari.[110] An earlier major application of beryllium was in brakes for military airplanes because of its hardness, high melting point, and exceptional ability to dissipate heat. Environmental considerations have led to substitution by other materials.[19]

Alloys

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Mixing about 2.0% beryllium into copper forms an alloy called beryllium copper that is six times stronger than copper alone.[111] Beryllium alloys are used in many applications because of their combination of elasticity, high electrical conductivity and thermal conductivity, high strength and hardness, nonmagnetic properties, as well as good corrosion and fatigue resistance.[45][13] These applications include non-sparking tools that are used near flammable gases (beryllium nickel), springs, membranes (beryllium nickel and beryllium iron) used in surgical instruments, and high temperature devices.[45][13] As little as 50 parts per million of beryllium alloyed with liquid magnesium leads to a significant increase in oxidation resistance and decrease in flammability.[13]

Beryllium copper adjustable wrench

Beryllium-copper alloys were also applied as a hardening agent in "Jason pistols", which were used to strip the paint from the hulls of ships.[112]

Beryllium–copper alloys are also widely used in modern aerospace and defense applications, particularly in high-performance electrical connectors, battery safety fuses, and microswitches that require a balance of conductivity, corrosion resistance, and fatigue strength.[113]

A metal matrix composite material combining beryllium with aluminium developed under the trade name AlBeMet for the high performance aerospace industry has low weight but four times the stiffness of aluminum alone.[114]

Mirrors

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Large-area beryllium mirrors, frequently with a honeycomb support structure, are used, for example, in meteorological satellites where low weight and long-term dimensional stability are critical. Smaller beryllium mirrors are used in optical guidance systems and in fire-control systems, e.g. in the German-made Leopard 1 and Leopard 2 main battle tanks. In these systems, very rapid movement of the mirror is required, which again dictates low mass and high rigidity. Usually the beryllium mirror is coated with hard electroless nickel plating which can be more easily polished to a finer optical finish than beryllium. In some applications, the beryllium blank is polished without any coating. This is particularly applicable to cryogenic operation where thermal expansion mismatch can cause the coating to buckle.[19]

The James Webb Space Telescope has 18 hexagonal beryllium sections for its mirrors, each plated with a thin layer of gold.[115] Because JWST will face a temperature of 33 K, the mirror is made of gold-plated beryllium, which is capable of handling extreme cold better than glass. Beryllium contracts and deforms less than glass and remains more uniform in such temperatures.[116] For the same reason, the optics of the Spitzer Space Telescope are entirely built of beryllium metal.[117]

Magnetic applications

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A hollow beryllium sphere used in a gyrocompass of the Boeing B-52 Stratofortress aircraft[118]

Beryllium is non-magnetic. Therefore, tools fabricated out of beryllium-based materials are used by naval or military explosive ordnance disposal teams for work on or near naval mines, since these mines commonly have magnetic fuzes.[119] They are also found in maintenance and construction materials near magnetic resonance imaging (MRI) machines because of the high magnetic fields generated.[120]

Nuclear applications

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High purity beryllium can be used in nuclear reactors as a moderator,[121] reflector, or as cladding on fuel elements.[122][123] Thin plates or foils of beryllium are sometimes used in nuclear weapon designs as the very outer layer of the plutonium pits in the primary stages of thermonuclear bombs, placed to surround the fissile material. These layers of beryllium are good "pushers" for the implosion of the plutonium-239, and they are good neutron reflectors, just as in beryllium-moderated nuclear reactors.[124]

Beryllium is commonly used in some neutron sources in laboratory devices in which relatively few neutrons are needed (rather than having to use a nuclear reactor or a particle accelerator-powered neutron generator). For this purpose, beryllium-9 is mixed with a source of alpha particles such as polonium-210, radium-226, plutonium-238, or americium-241.[25] In the nuclear reaction that occurs, a beryllium nucleus is transmuted into carbon-12, and one free neutron is emitted, traveling in about the same direction as the alpha particle was heading. Such alpha decay-driven beryllium neutron sources, named "urchin" neutron initiators, were used in some early atomic bombs.[124] Neutron sources in which beryllium is bombarded with gamma rays from a gamma decay radioisotope are also used to produce laboratory neutrons.[24]

Two CANDU fuel bundles: Each about 50 cm in length and 10 cm in diameter. Notice the small appendages on the fuel clad surfaces

Beryllium is used in fuel fabrication for CANDU reactors. The fuel elements have small appendages that are resistance brazed to the fuel cladding using an induction brazing process with Be as the braze filler material. Bearing pads are brazed in place to prevent contact between the fuel bundle and the pressure tube containing it, and inter-element spacer pads are brazed on to prevent element to element contact.[125]

Beryllium is used at the Joint European Torus nuclear-fusion research laboratory, and it will be used in the more advanced ITER to condition the components which face the plasma.[126] Beryllium has been proposed as a cladding material for nuclear fuel rods, because of its good combination of mechanical, chemical, and nuclear properties.[19] Beryllium fluoride is one of the constituent salts of the eutectic salt mixture FLiBe, which is used as a solvent, moderator and coolant in many hypothetical molten salt reactor designs, including the liquid fluoride thorium reactor (LFTR).[127]

Acoustics

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The low weight and high rigidity of beryllium make it useful as a material for high-frequency speaker drivers. Because beryllium is expensive (many times more than titanium), hard to shape due to its brittleness, and toxic if mishandled, beryllium tweeters are limited to high-end home,[128][129][130] pro audio, and public address applications.[131][132] Some high-fidelity products have been fraudulently claimed to be made of the material.[133]

Some high-end phonograph cartridges used beryllium cantilevers to improve tracking by reducing mass.[134]

Beryllium was used for cantilevers in high-performance phonograph cartridge styli, where its extreme stiffness and low density allowed for tracking weights to be reduced to 1 gram while still tracking high frequency passages with minimal distortion.[135]

In sound amplification systems, the speed at which sound travels directly affects the resonant frequency of the amplifier, thereby influencing the range of audible high-frequency sounds. Beryllium stands out due to its exceptionally high speed of sound propagation compared to other metals.[136] This unique property allows beryllium to achieve higher resonant frequencies, making it an ideal material for use as a diaphragm in high-quality loudspeakers.[137]

Electronics

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Beryllium is a p-type dopant in III-V compound semiconductors. It is widely used in materials such as GaAs, AlGaAs, InGaAs and InAlAs grown by molecular-beam epitaxy (MBE).[138] Cross-rolled beryllium sheet is an excellent structural support for printed circuit boards in surface-mount technology. In critical electronic applications, beryllium is both a structural support and heat sink. The application also requires a coefficient of thermal expansion that is well matched to the alumina and polyimide-glass substrates. The beryllium-beryllium oxide composite "E-Materials" have been specially designed for these electronic applications and have the additional advantage that the thermal expansion coefficient can be tailored to match diverse substrate materials.[19]

Beryllium oxide is useful for many applications that require the combined properties of an electrical insulator and an excellent heat conductor, with high strength and hardness and a very high melting point. Beryllium oxide is frequently used as an insulator base plate in high-power transistors in radio frequency transmitters for telecommunications. Beryllium oxide is being studied for use in increasing the thermal conductivity of uranium dioxide nuclear fuel pellets.[139] Beryllium compounds were used in fluorescent lighting tubes, but this use was discontinued because of the disease berylliosis which developed in the workers who were making the tubes.[140]

Medical applications

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Beryllium is a component of several dental alloys.[141][142] In addition to standard X-ray equipment mentioned in Beryllium § Radiation windows, in medical imaging equipment, such as CT scanners and mammography machines, beryllium's strength and light weight enhance durability and performance.[143] Beryllium is used in analytical equipment for blood, HIV, and other diseases.[144] Beryllium alloys are used in surgical instruments, optical mirrors, and laser systems for medical treatments.[145][146]

Toxicity and safety

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Beryllium
Hazards
GHS labelling:[147]
GHS06: Toxic GHS08: Health hazardGHS09: Environmental hazard
Danger
H301, H315, H317, H319, H330, H335, H350i, H372
P201, P202, P280, P302, P304, P305+P351+P338, P310, P340, P352
NFPA 704 (fire diamond)
NFPA 704 four-colored diamondHealth 4: Very short exposure could cause death or major residual injury. E.g. VX gasFlammability 3: Liquids and solids that can be ignited under almost all ambient temperature conditions. Flash point between 23 and 38 °C (73 and 100 °F). E.g. gasolineInstability 3: Capable of detonation or explosive decomposition but requires a strong initiating source, must be heated under confinement before initiation, reacts explosively with water, or will detonate if severely shocked. E.g. hydrogen peroxideSpecial hazards (white): no code
4
3
3

Biological effects

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Approximately 35 micrograms of beryllium is found in the average human body, an amount not considered harmful.[148] Beryllium is chemically similar to magnesium and therefore can displace it from enzymes, which causes them to malfunction.[148] Because Be2+ is a highly charged and small ion, it can easily get into many tissues and cells, where it specifically targets cell nuclei, inhibiting many enzymes, including those used for synthesizing DNA. Its toxicity is exacerbated by the fact that the body has no means to control beryllium levels, and once inside the body, beryllium cannot be removed.[149]

Inhalation

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Chronic beryllium disease (CBD), or berylliosis, is a pulmonary and systemic granulomatous disease caused by inhalation of dust or fumes contaminated with beryllium; either large amounts over a short time or small amounts over a long time can lead to this ailment. Symptoms of the disease can take up to five years to develop; about a third of patients with it die and the survivors are left disabled.[148] The International Agency for Research on Cancer (IARC) lists beryllium and beryllium compounds as Category 1 carcinogens.[150]

Occupational exposure

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In the US, the Occupational Safety and Health Administration (OSHA) has designated a permissible exposure limit (PEL) for beryllium and beryllium compounds of 0.2 μg/m3 as an 8-hour time-weighted average (TWA) and 2.0 μg/m3 as a short-term exposure limit over a sampling period of 15 minutes. The National Institute for Occupational Safety and Health (NIOSH) has set a recommended exposure limit (REL) upper-bound threshold of 0.5 μg/m3. The IDLH (immediately dangerous to life and health) value is 4 mg/m3.[151] The toxicity of beryllium is on par with other toxic metalloids/metals, such as arsenic and mercury.[152][153]

Exposure to beryllium in the workplace can lead to a sensitized immune response, and over time development of berylliosis.[154] NIOSH in the United States researches these effects in collaboration with a major manufacturer of beryllium products. NIOSH also conducts genetic research on sensitization and CBD, independently of this collaboration.[154]

Acute beryllium disease in the form of chemical pneumonitis was first reported in Europe in 1933 and in the United States in 1943. A survey found that about 5% of workers in plants manufacturing fluorescent lamps in 1949 in the United States had beryllium-related lung diseases.[155] Chronic berylliosis resembles sarcoidosis in many respects, and the differential diagnosis is often difficult. It killed some early workers in nuclear weapons design, such as Herbert L. Anderson.[156]

Beryllium may be found in coal slag. When the slag is formulated into an abrasive agent for blasting paint and rust from hard surfaces, the beryllium can become airborne and become a source of exposure.[157]

Although the use of beryllium compounds in fluorescent lighting tubes was discontinued in 1949, potential for exposure to beryllium exists in the nuclear and aerospace industries, in the refining of beryllium metal and the melting of beryllium-containing alloys, in the manufacturing of electronic devices, and in the handling of other beryllium-containing material.[158]

Detection

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Early researchers undertook the highly hazardous practice of identifying beryllium and its various compounds from its sweet taste. A modern test for beryllium in air and on surfaces has been developed and published as an international voluntary consensus standard, ASTM D7202. The procedure uses dilute ammonium bifluoride for dissolution and fluorescence detection with beryllium bound to sulfonated hydroxybenzoquinoline, allowing up to 100 times more sensitive detection than the recommended limit for beryllium concentration in the workplace. Fluorescence increases with increasing beryllium concentration. The new procedure has been successfully tested on a variety of surfaces and is effective for the dissolution and detection of refractory beryllium oxide and siliceous beryllium in minute concentrations (ASTM D7458).[159][160] The NIOSH Manual of Analytical Methods contains methods for measuring occupational exposures to beryllium.[161]

Notes

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References

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Cited sources

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Further reading

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
Beryllium is a with the symbol Be and 4, classified as an in group 2 and period 2 of the periodic table. It appears as a steel-gray, lustrous, relatively soft solid at , with a low of 1.85 g/cm³, a high of 1287 °C, and a of 2469 °C. Beryllium is notable for its exceptional stiffness, high strength-to-weight ratio, and resistance to , making it brittle yet valuable in specialized applications despite its . The element was first identified in 1798 when French chemist Nicolas-Louis Vauquelin discovered its in the minerals beryl and emerald. The pure metal was independently isolated in 1828 by and Antoine Bussy through the reduction of with or magnesium. Beryllium occurs naturally at low concentrations in the , primarily in beryl (Be₃Al₂Si₆O₁₈) and bertrandite (Be₄Si₂O₇(OH)₂), with major deposits mined in the United States, , and . Chemically, it exhibits a +2 , forms a protective layer that prevents further oxidation, and reacts with acids but not with or alkalis under normal conditions. Beryllium's primary industrial uses stem from its alloys, particularly beryllium-copper, which provide high strength, electrical and conductivity, and non-sparking properties for tools, springs, and connectors in , defense, , and . Pure beryllium metal serves as a and reflector in nuclear reactors, in windows due to its low , and in structural components for satellites and brakes. Beryllium oxide ceramics are employed in high-performance , systems, , and management in cell phones and automotive parts. However, beryllium and its compounds are highly toxic, causing —a chronic —from of or fumes, necessitating stringent occupational standards. No known biological role exists for beryllium in living organisms, and it is not essential for life.

Characteristics

Physical properties

Beryllium is a with 4 and of 9.0121831(5) u. Its ground-state is [He] 2s². It has a calculated atomic radius of 112 pm. Elemental beryllium appears as a steel-gray, lustrous solid metal at . It has a low density of 1.85 g/cm³ at 20°C, making it the lightest rigid structural metal. Beryllium melts at 1560 K (1287°C, 2349°F) and boils at 2742 K (2469°C, 4476°F). Beryllium adopts a hexagonal close-packed (hcp) with lattice constants a = 0.2286 nm and c = 0.3584 nm at . The properties of beryllium include a of 1820 J/kg·K and a conductivity of 200 W/(m·K) at 25°C, the highest among non-carbon metals on a specific basis. Mechanically, beryllium exhibits a Young's modulus of 287 GPa, an ultimate tensile strength of 370 MPa for pure metal, and a Mohs hardness of 5.5. Its electrical resistivity is 30 × 10⁻⁹ Ω·m at 0°C. Beryllium is brittle at room temperature but becomes ductile above 1000°C, with a notably low Poisson's ratio of 0.032.

Chemical properties

Beryllium is highly electropositive, with a first of 899 kJ/mol, which facilitates the formation of the Be²⁺ cation in many compounds. However, due to its small (approximately 45 pm), high , and electronegativity of 1.57 on the Pauling scale, beryllium exhibits significant covalent character in its bonding, leading to polarized bonds rather than purely ionic interactions. This diagonal with aluminum further emphasizes its atypical behavior within Group 2. The oxide BeO is amphoteric, reacting with acids to form beryllium salts such as BeCl₂ and with bases to produce the tetrahydroxoberyllate ion, [Be(OH)₄]²⁻. For example: BeO+2H+Be2++H2O\text{BeO} + 2\text{H}^+ \rightarrow \text{Be}^{2+} + \text{H}_2\text{O} BeO+2OH+H2O[Be(OH)4]2\text{BeO} + 2\text{OH}^- + \text{H}_2\text{O} \rightarrow [\text{Be(OH)}_4]^{2-} Beryllium salts undergo slow hydrolysis in water, precipitating beryllium hydroxide, Be(OH)₂, due to the high charge density of Be²⁺ promoting acidic behavior in aqueous solutions. Beryllium halides display unique properties; BeCl₂ acts as a Lewis acid because of its electron-deficient nature, forming tetrahedral complexes such as [BeCl₄]²⁻ with chloride ions. In contrast, BeF₂ is highly soluble in water and adopts a polymeric, glass-like structure in the solid state with tetrahedral coordination around beryllium. Organoberyllium compounds, such as dimethylberyllium ((CH₃)₂Be), are pyrophoric and feature tetrahedral geometry around the beryllium atom in their dimeric or adduct forms. Beryllium passivates in air by forming a thin, adherent BeO layer, which provides corrosion resistance up to 600°C. However, in powder form, it ignites between 540 and 700°C, burning brilliantly to produce BeO. It reacts vigorously with non-oxidizing acids, as exemplified by: Be+2HClBeCl2+H2\text{Be} + 2\text{HCl} \rightarrow \text{BeCl}_2 + \text{H}_2

Nuclear properties

Beryllium has a single stable isotope, ^{9}Be, which constitutes 100% of naturally occurring beryllium and features a nuclear structure with 4 protons and 5 neutrons, exhibiting characteristics associated with a closed proton shell (Z=4) in the nuclear shell model. The nucleus of ^{9}Be interacts with s through reactions that highlight its utility in nuclear applications. Its thermal is low at 0.009 barns, enabling efficient with minimal capture. However, for incident s above approximately 1.8 MeV, ^{9}Be undergoes the (n, 2n) reaction, emitting a second and contributing to multiplication in designs. A prominent reaction is ^{9}Be(α, n)^{12}C, where alpha particles induce , forming the basis for compact sources used in research and ; this reaction has a well-characterized cross section peaking around several millibarns in the alpha range of 2–10 MeV. Beryllium's fission cross section remains low across energies due to its light mass and high fission barrier, exceeding 20 MeV, rendering it non-fissile under typical conditions. Unstable isotopes of beryllium decay via specific modes that influence their astrophysical and geochemical roles. For instance, ^{7}Be decays primarily by electron capture to ^{7}Li with a half-life of 53.22 days. Similarly, ^{10}Be undergoes beta decay to ^{10}B with a half-life of 1.387 × 10^{6} years. These nuclear properties position beryllium as an effective moderator in nuclear reactors, where its low absorption cross section allows neutrons to thermalize with reduced loss, as demonstrated in reflector assemblies that enhance core efficiency. In fusion research, beryllium oxide is employed in gyrotron windows to transmit high-power millimeter waves for plasma heating, leveraging its low dielectric loss and thermal stability.

Optical properties

Beryllium metal is opaque to visible light due to its metallic nature and electronic structure, exhibiting approximately 50% reflectivity in the . In the region, bare beryllium surfaces demonstrate high reflectivity, reaching up to 98% at wavelengths around 10.6 μm and exceeding 99% beyond 15 μm, attributed to its free electron response. The complex of beryllium in the visible range, such as n ≈ 3.36 at 589 nm, reflects its strong absorption and reflection properties, with significant imaginary component k contributing to opacity. Beryllium's low (Z=4) and result in minimal absorption of X-rays, making it highly transparent to this compared to higher-Z materials, with transmission efficiencies approaching 100% for thin foils in the hard regime. This property enables its use in , where low absorption coefficients in the soft range (e.g., below 1 keV) allow for efficient beam transmission through beryllium windows or masks without significant attenuation. Beryllium oxide (BeO), a key compound, possesses a wide direct bandgap of 10.6 eV, corresponding to a UV at approximately 117 nm, which positions it as an excellent for applications due to its transparency above this threshold. The of BeO is around 1.72 in the visible to near-IR range, supporting its role in optical coatings. In beryl minerals (Be₃Al₂Si₆O₁₈), the primary natural source of beryllium, the refractive indices are n_ω = 1.564–1.595 and n_ε = 1.568–1.602 at 589 nm, yielding an average value near 1.57 and uniaxial negative of δ = 0.004–0.009, which varies with alkali content in the crystal channels. Certain beryl varieties, such as those with trace impurities like or , exhibit under excitation, often appearing as orange-red or green emissions in shortwave UV due to activators within the lattice.

Isotopes

Beryllium has twelve known isotopes, with mass numbers ranging from ⁴Be to ¹⁵Be. Only ⁹Be is stable and occurs naturally, comprising 100% of terrestrial beryllium. This primordial isotope is effectively stable, with a theoretical half-life exceeding 10¹⁶ years, far longer than the age of the universe. Among the radioactive isotopes, ⁷Be is produced primarily through cosmic ray spallation of heavier nuclei in the atmosphere and decays via electron capture (EC) to ⁷Li, with a half-life of 53.22 days. Another notable long-lived isotope is ¹⁰Be, which undergoes β⁻ decay to ¹⁰B with a half-life of 1.387 × 10⁶ years and serves as a key tracer in geochronology. The ratio of ¹⁰Be to ⁹Be in environmental samples provides insights into paleoclimate variations, such as changes in solar activity and atmospheric circulation over glacial-interglacial cycles. In contrast, ⁸Be is highly unstable, existing as a short-lived resonance state that decays almost exclusively by α emission to two ⁴He nuclei, with a half-life of approximately 8 × 10⁻¹⁷ seconds; this property makes it central to the triple-alpha process in stellar nucleosynthesis. The are not formed through standard stellar fusion pathways due to the of ⁸Be and similar intermediates, which prevents efficient buildup beyond burning. Instead, they originate mainly from reactions, where high-energy cosmic rays fragment heavier elements like carbon, , and oxygen in the or Earth's atmosphere. This non-thermal production mechanism accounts for the low cosmic abundances of beryllium compared to lighter elements like and heavier ones like .

Occurrence and Production

Natural occurrence

Beryllium is a lithophile element that occurs naturally in the Earth's crust at an average concentration of approximately 2.7 parts per million (ppm), making it the 44th most abundant element overall. This level positions it as rarer than lithium (about 20 ppm) but comparable to other trace elements like scandium (around 22 ppm). Beryllium is primarily found in igneous rocks such as granites and pegmatites, where it substitutes for aluminum in silicate minerals due to their similar ionic radii. The principal beryllium-bearing minerals are beryl (Be₃Al₂Si₆O₁₈) and bertrandite (Be₄Si₂O₇(OH)₂). Beryl, a cyclosilicate, typically contains 2–4% beryllium (equivalent to 5–11% , ) in economic ores, though pure crystals can reach up to 11–12% . Bertrandite, a sorosilicate often formed as an alteration product of beryl in hydrothermal environments, has ores typically grading 0.5–0.8% at major deposits like Spor Mountain, Utah. Secondary minerals such as phenakite (Be₂SiO₄) and hambergite (Be₂BO₃OH) occur less commonly and are not major commercial sources. Significant deposits are located , particularly in Utah's Spor Mountain district, where bertrandite is mined from volcanic tuffs. Other key producers include , which relies on both domestic beryl and imports, and , a major supplier of beryllium concentrates. These locations account for the majority of global resources, estimated at over 100,000 metric tons of contained beryllium, with U.S. reserves at approximately 19,000 metric tons. In , beryllium concentrations are very low, averaging about 0.6 parts per trillion (ppt), or roughly 0.6 nanograms per liter, due to its strong adsorption onto particles and sediments. Beryllium exhibits no significant biological role and does not bioaccumulate in organisms or food chains to notable levels, limiting its environmental mobility in aquatic and terrestrial ecosystems. Beyond , beryllium occurs in trace amounts in meteorites, with concentrations ranging from 13 to 386 (ppb) in stony meteorites, reflecting incorporation during solar system formation. In the , it is primarily produced through , where high-energy protons fragment heavier nuclei like carbon, , and oxygen in the , contributing to its low overall galactic abundance.

Extraction and refining

Beryllium is primarily extracted from bertrandite ore, which is the dominant source for industrial production, particularly . The process begins with crushing and grinding the ore, followed by leaching with (H₂SO₄) to dissolve the beryllium as beryllium sulfate. The resulting solution undergoes solvent extraction using di(2-ethylhexyl)phosphoric acid in to separate beryllium from impurities such as iron and aluminum. The purified beryllium is then stripped with and precipitated as , Be(OH)₂, achieving approximately 87% recovery. The beryllium hydroxide is reacted with ammonium bifluoride (NH₄HF₂) to form ammonium tetrafluoroberyllate, (NH₄)₂BeF₄. This intermediate is thermally decomposed at around 1,000°C to yield , . The is subsequently reduced with magnesium metal at approximately 1,200°C in an inert atmosphere to produce metallic beryllium via the reaction:
\ceBeO+2Mg>Be+2MgO\ce{BeO + 2Mg -> Be + 2MgO}
This step yields beryllium in pebble form, which is then crushed and sized for further processing. The overall process is energy-intensive due to the high temperatures required, stemming from beryllium's melting point of 1,287°C.
For beryl ore, a more complex pretreatment is necessary owing to its refractory silicate structure. The ore is crushed, heated to its of about 1,650°C, and rapidly quenched in to form a friable . This material is reheated to 1,000°C, ground, and leached with , followed by solvent extraction and precipitation to yield , similar to the bertrandite process. An alternative method involves fusion with potassium tetrafluoroborate (KBF₄) to decompose the mineral, enabling subsequent leaching and recovery steps with approximately 90% overall yield. Beryl processing accounts for a smaller portion of global supply, primarily from imports in countries like and . Refining of crude beryllium metal to high purity (>99.9%) typically involves , where impurities with different vapor pressures are separated under reduced pressure, or of (BeCl₂) in a bath at 1,290–1,400°C to deposit pure metal flakes. These methods remove residual magnesium, fluorides, and other contaminants, producing material suitable for and nuclear applications. Global mine production of beryllium as of 2024 was estimated at 360 metric tons, with the leading at 180 tons, followed by (80 tons), (77 tons), and (24 tons); minor production occurred in , , and (1 ton each). This represents an increase from 320 tons in 2023, driven by higher output in . Major producers include Corporation in the , which operates the only domestic mine at Spor Mountain, , and facilities in such as the Ulba Metallurgical Plant, alongside Chinese operations like those of Shuikoushan.

History

Discovery and isolation

In 1798, French chemist identified (BeO), also known as beryllia, as a new earth while analyzing samples of beryl and emerald. He extracted the oxide from these minerals and recognized its distinct chemical properties, distinguishing it from similar earths like alumina. The metallic form of beryllium was first isolated in 1828 through independent experiments by German chemist and French chemist Antoine-Alexandre Brutus Bussy. Wöhler reduced (BeCl₂) with metal, while Bussy achieved the same result using molten , yielding small quantities of the metal (though impure). The first pure samples of beryllium metal were obtained in 1898 by French chemist Paul Lebeau through of a molten mixture of beryllium fluoride and . In the early , Swedish chemist confirmed beryllium as a distinct element and proposed the name "beryllium," contributing to early determinations of its atomic weight around 9. Initially, the element and its compounds were referred to as "glucina" or "glucinium," derived from word for , due to the sweet taste of some beryllium salts.

Etymology

The name beryllium is derived from the mineral beryl, from which the element was first isolated, with the term tracing back to Latin beryllus and Ancient Greek bēryllos, referring to a blue-green gemstone. This Greek word likely originates from Prakrit veruliya, denoting a pale green gem, ultimately from Sanskrit vaidūrya, possibly linked to the Dravidian name for the city of Velur (modern Belur) in southern India, a historical source of such stones. The mineral beryl has a long history of recognition in antiquity, with evidence of its use dating to , where deposits of emerald—a green variety of beryl—were mined in the Eastern Desert over 2,000 years ago, supplying gems to Mediterranean civilizations. The aquamarine variety, prized for its sea-blue hue, was also known in ancient Egyptian and Roman contexts as a talisman for sailors and healers. Around 300 BCE, the Greek philosopher , in his treatise On Stones, described emerald as a distinct green stone similar to beryl, marking an early attempt to classify these varieties based on color and properties. An alternative name for the element was glucinum (or glucinium), proposed due to the sweet taste of its soluble salts, from Greek glykys meaning "sweet"; this name was used alongside beryllium in early chemical literature. In , Swedish chemist adopted the symbol Be for beryllium (glucinum) in his systematic for elements, favoring it over alternatives like Gl for glucinum, which was ultimately rejected in favor of the beryl-derived name by the early .

Applications

Mechanical applications

Beryllium's exceptional stiffness-to-weight ratio makes it ideal for mechanical applications requiring lightweight structural integrity, particularly in environments with extreme temperatures and vibrations. On a weight-to-weight basis, beryllium is six times stiffer than steel while weighing approximately one-third as much, allowing for significant reductions in component mass without compromising rigidity. This property, combined with its ability to maintain shape across a wide temperature range, positions beryllium as a preferred material for load-bearing elements in high-performance systems. Emerging uses include beryllium alloys in additive manufacturing for lightweight, complex parts in aerospace and defense (as of 2024). In aerospace, beryllium is employed in structural components such as beams and trusses, where its high modulus enables precise load distribution and minimal deflection. For instance, it forms spars up to 13 feet long and box beams for structures, contributing to the lightweight design of missions like the Lunar Orbiter. In the , beryllium cross-rolled sheets were integrated into compression panels, truss beams, and shear beams, achieving weight savings of up to 23 kg per panel while withstanding loads at temperatures up to 316°C. These applications leverage beryllium's inherent vibration damping, which enhances dimensional stability in precision instruments and inertial guidance systems aboard and aircraft. For defense purposes, beryllium supports critical structural roles in and due to its low and high stiffness. It is used in nose cones for s such as the Maverick, , and Minuteman, where thermal and aerodynamic stresses demand materials that resist deformation. In like the F/A-18 and F-22, beryllium components contribute to braking systems, providing robust performance under high thermal loads and mechanical stress. Fabrication of beryllium for mechanical uses typically begins with ingots into structural shapes via processes like , , and hot-forming at around 1350°F to overcome its inherent , which stems from limited crystallographic slip systems. This makes the material during cutting, requiring specialized tools and controlled environments to prevent cracking, though it machines comparably to heat-treated cast aluminum. Post- heat treatments, such as annealing at 1500–1750°F, enhance and strength by reducing internal stresses and refining grain structure, enabling reliable assembly via fluxless or riveting for complex components.

Alloys

Beryllium alloys combine the element's and lightweight nature with the base metal's , enhancing overall mechanical performance in demanding environments. These alloys typically contain 0.5–3% beryllium by weight, which improves strength, resistance, and stability while maintaining good electrical and thermal conductivity. Production often involves or followed by to precipitate fine beryllium phases, avoiding cracking during processing. The most prominent beryllium alloy is (BeCu), particularly alloys like C17200 with 1.8–2.0% beryllium, which can be hardened to achieve tensile strengths exceeding 1200 MPa and yield strengths up to 1000 MPa. This hardening process involves solution treatment at around 800°C followed by aging at 300–320°C, resulting in a fine dispersion of beryllium- precipitates that provide exceptional strength without sacrificing much . BeCu exhibits an of approximately 130 GPa, making it ideal for applications requiring high resilience, such as springs, diaphragms, and precision instruments where repeated flexing is common. Its fatigue resistance allows endurance under cyclic loading up to 10^7 cycles at stresses around 400–500 MPa, outperforming many other alloys. BeCu also retains about 55% of the International Annealed Copper Standard (IACS) electrical conductivity in high-conductivity variants (e.g., Alloy 10 with 0.2–0.6% Be), balancing strength with efficient current carrying for connectors and relays. A key safety feature is its non-sparking behavior, achieved through low friction and controlled composition, which qualifies it for tools used in atmospheres like oil refineries or munitions handling. These properties stem from beryllium's role in refining the alloy's microstructure, enhancing resistance and tolerance in harsh conditions. Beryllium nickel alloys, containing around 2% beryllium, are valued for high-temperature applications due to their superior creep resistance and shape retention up to 500°C. These alloys, such as NiBeTi variants, offer ultra-high strength (over 1000 MPa) and elasticity, with excellent electrical conductivity similar to pure nickel but improved fatigue life for dynamic components. They are employed in turbine engine parts, springs, bellows, and valves where thermal stability and wear resistance are critical, often produced via powder metallurgy to ensure uniform dispersion and minimize defects. The addition of beryllium refines grain structure, boosting hardness and endurance under oxidative environments typical of aerospace and power generation systems.

Radiation and optical applications

Beryllium's low and high transparency to s make it ideal for applications requiring minimal beam attenuation, particularly in radiation-handling devices such as windows. These windows typically consist of thin beryllium foils with thicknesses ranging from 0.1 to 1 mm, which serve as vacuum seals and monochromators in analytical, , and industrial equipment. The material's mass absorption coefficient at 10 keV is approximately 0.15 cm²/g, enabling high transmission rates—often over 90% for soft s—while maintaining structural integrity under vacuum conditions. In synchrotron radiation facilities, beryllium windows are employed to isolate ultra-high vacuum beamlines from experimental areas without significantly degrading the X-ray beam quality. These 0.5 mm thick foils, for instance, are positioned after slits or monochromators to filter and transmit high-brilliance X-rays while sealing against atmospheric exposure. Their low absorption and resistance to thermal shock from intense beams ensure reliable performance in high-flux environments, as demonstrated in facilities like the European Synchrotron Radiation Facility. For optical applications, polished beryllium mirrors leverage the metal's stiffness, low density, and dimensional stability to achieve precise reflectivity in demanding environments. In space telescopes, such as the (JWST), the primary mirror comprises 18 hexagonal beryllium segments, each coated with a thin gold layer for enhanced performance. These mirrors exhibit approximately 98% reflectivity across the 0.6 to 30 μm wavelength range, enabling high-fidelity in the near- to mid- . Beryllium's exceptional cryogenic stability further supports its use in cooled optical systems, where it resists deformation down to 4 K without compromising figure accuracy. This property, arising from the material's low coefficient at low temperatures, allows mirrors to maintain sub-micrometer surface precision during thermal cycling, as verified in interferometric tests. Such stability is critical for applications like JWST, where mirrors operate near 40 K but benefit from beryllium's proven performance across broader cryogenic regimes.

Nuclear applications

Beryllium plays a critical role in due to its unique interaction properties, particularly its low absorption cross-section and ability to multiply s through the (n,2n) reaction. This reaction, represented as 9Be+n9Be+2n^9\mathrm{Be} + n \rightarrow ^9\mathrm{Be} + 2n, has a of 1.67 MeV and enables beryllium to act as both a moderator and reflector in nuclear reactors, enhancing economy by producing additional neutrons from fast incident particles. In research reactors such as the (HFIR) at , beryllium is employed as a reflector surrounding the core to redirect escaping neutrons back into the fission region, thereby increasing the overall and efficiency. The material's high cross-section for and fast neutrons, combined with minimal absorption, makes it superior to alternatives like in certain high-flux environments. (BeO) is also utilized in some designs as a moderator to slow down neutrons while maintaining structural integrity under irradiation. For neutron sources, beryllium is combined with alpha-emitting isotopes like polonium-210 or plutonium-239 to create compact, portable generators. In these devices, alpha particles from the radioactive decay interact with beryllium nuclei via the reaction 9Be+4He12C+n+5.7MeV^9\mathrm{Be} + ^4\mathrm{He} \rightarrow ^{12}\mathrm{C} + n + 5.7 \, \mathrm{MeV}, releasing neutrons with energies around 4-11 MeV suitable for calibration, activation analysis, and well-logging applications. These sources are valued for their simplicity and high neutron yield per unit volume compared to other isotopic options. In fusion reactors, beryllium serves as a neutron multiplier in the of the , where it captures high-energy neutrons from the deuterium- plasma and produces additional neutrons to breed fuel through (n,2n) and other reactions. This application leverages beryllium's ability to boost in the blanket region, improving tritium self-sufficiency. Additionally, beryllium windows are used in particle accelerators to separate regions while transmitting high-energy particle beams, owing to the material's low , high strength, and resistance to . These windows withstand intense proton or fluxes in facilities like those at and .

Electronic applications

Beryllium oxide (BeO) ceramics are widely utilized as substrates in electronic components due to their exceptional thermal management capabilities and electrical insulation properties. These ceramics serve as insulating bases for high-power transistors, where efficient heat dissipation is critical to prevent and maintain performance under high loads. With a thermal conductivity of approximately 250 W/m·K, BeO effectively conducts heat away from active elements, outperforming many alternative materials like alumina while remaining electrically insulating. Additionally, BeO's low dielectric constant of 6.7 enables minimal signal interference in high-frequency applications, making it ideal for substrates in RF power modules and amplifiers. In RF amplifiers, BeO substrates support the packaging of power transistors by providing stable thermal paths that allow devices to operate at elevated power densities without degradation. This is particularly valuable in and systems, where BeO's combination of high thermal conductivity and low ensures reliable signal amplification and longevity. For instance, in RF applications, BeO insulators facilitate the handling of large energy inputs with minimal losses, contributing to the efficiency of circuits. Beryllium copper (BeCu) alloys are employed in electronic connectors and springs for high-reliability applications, leveraging their superior mechanical strength, electrical conductivity, and fatigue resistance. These components, such as spring contacts in satellite electronics, maintain consistent electrical connections under extreme conditions including vibration, thermal cycling, and vacuum exposure. BeCu's ability to endure thousands of mating cycles without deformation makes it essential for interconnects in aerospace systems, where failure could compromise mission-critical operations. BeO ceramics also find use in , particularly in microwave devices, owing to their low rates and high thermal conductivity. In these applications, BeO serves as an insulator that minimizes gas release in high- environments, preserving tube integrity and performance over extended periods. This property, combined with , positions BeO as a preferred material for components in traveling wave and klystrons used in RF generation. Similarly, low-beryllium alloys exhibit extremely low , on the order of 10^{-14} Pa·m/s, enhancing their suitability for vacuum-sealed electronic assemblies.

Acoustic applications

Beryllium's exceptional rigidity and low properties make it ideal for acoustic applications, particularly in high-fidelity sound reproduction systems where minimal and rapid sound wave propagation are essential. In speaker , pure beryllium diaphragms are employed in tweeters to handle high-frequency signals with precision, as the material's high stiffness-to-weight ratio allows for thin, lightweight domes that resist deformation under . The in beryllium reaches approximately 12.9 km/s, significantly higher than in aluminum (around 6.4 km/s), enabling faster and extended frequency reproduction without breakup modes in the audible range. This property contributes to beryllium's low , where vibrational energy dissipates quickly, reducing and coloration in reproduced . Manufacturers such as Focal utilize 99% pure beryllium for their domes, highlighting its ability to scratch due to extreme rigidity while maintaining a low mass of about 0.07 grams for a 35 mm diaphragm. High-end tweeters from companies like Scan-Speak and TAD Laboratories incorporate beryllium domes to achieve responses extending beyond 40 kHz, surpassing hearing limits for superior imaging and detail in audio playback. For instance, Scan-Speak's Illuminator series features a 1-inch beryllium dome with a as low as 750 Hz and up to 90.9 dB, allowing crossover points as low as 3 kHz while maintaining flat response up to 26 kHz. TAD's TD-4001 uses a 100 mm beryllium diaphragm for , leveraging the material's high-speed sound conduction to minimize phase in large-scale systems. These applications underscore beryllium's role in enhancing clarity and dynamics, though its requires specialized handling during manufacturing.

Medical applications

Beryllium's medical applications are constrained by its , yet its low and high transparency to s enable specific diagnostic uses. Historically, beryllium windows were incorporated into early equipment to minimize absorption of soft s, allowing for higher-intensity beams in biophysical and during the mid-20th century. This property, stemming from beryllium's radiation transparency, persists in modern applications such as tubes for , where thin beryllium exit windows—typically around 127 microns thick—reduce beam hardening and filtration, improving image contrast for breast tissue detection while maintaining low patient skin doses, often below 2 rads per exposure. In surgical settings, beryllium-copper (BeCu) alloys are utilized for non-magnetic instruments, leveraging their strength, corrosion resistance, and lack of magnetic interference, which is critical in environments like MRI suites or precision procedures. Examples include dental tools such as needle holders and wire cutters, as well as components in monitoring devices that require reliable electrical conductivity without sparking risks. Beryllium's role in therapeutic applications remains investigational, particularly as a neutron source in boron neutron capture therapy (BNCT) for . In accelerator-based systems, protons striking thick beryllium targets generate epithermal neutrons, which, when combined with boron-10 compounds selectively accumulated in tumor cells, induce localized emission to destroy malignant tissue without widespread damage. Such setups, studied with proton energies of 3-4 MeV on beryllium, show promise for refractory cancers but are not yet clinically widespread. Due to its potential to induce granulomatous reactions upon implantation, beryllium sees no widespread use in bio-implants or prosthetics.

Health Effects and Safety

Biological effects

Beryllium has no known essential biological role in humans or other organisms, as it does not participate in any enzymatic or physiological processes. At the cellular level, beryllium exerts toxic effects primarily through its ability to act as a , binding to proteins and peptides to form neoantigens that are presented by () class II molecules on antigen-presenting cells. This interaction triggers a CD4+ T-cell mediated response, known as beryllium sensitization (BeS), where beryllium-specific T cells proliferate and release pro-inflammatory cytokines such as interferon-gamma, leading to immune dysregulation. In sensitized individuals, this mechanism underlies the development of chronic beryllium disease (CBD), also called , a systemic granulomatous disorder resembling . CBD manifests as a chronic condition characterized by the formation of non-caseating granulomas in the lungs and other tissues, resulting from persistent T-cell activation and recruitment. Among occupationally exposed workers, approximately 2–6% develop CBD following sensitization, with disease progression varying from asymptomatic granulomas to progressive , dyspnea, and cor pulmonale. The granulomatous in CBD contributes to beryllium's carcinogenicity; the International Agency for Research on Cancer (IARC) classifies beryllium and its compounds as carcinogens, based on sufficient evidence of risk in humans through chronic inflammatory processes that promote and DNA damage. Beryllium exhibits relatively low acute oral toxicity, with an LD50 >2000 mg/kg body weight in rats for elemental beryllium metal powder, though values vary significantly by compound (e.g., lower for soluble salts like beryllium at 120 mg Be/kg). Following absorption, beryllium distributes systemically and accumulates preferentially in , where it has a long of about 450 days, potentially contributing to skeletal over time.

Exposure routes

Beryllium exposure primarily occurs through , which is the most significant route for both occupational and environmental settings. Airborne beryllium particles, such as dust, fumes, or mists generated during , , or , can be inhaled into the . Particles smaller than 10 μm in aerodynamic diameter, particularly those under 5 μm, are capable of deep deposition, where soluble beryllium salts are absorbed rapidly into the bloodstream at rates around 20% of the lung burden, while insoluble forms like exhibit slower clearance with biological half-lives ranging from days to years. This route accounts for the majority of systemic uptake in exposed individuals. Dermal contact represents another key exposure pathway, though absorption through intact is generally low due to beryllium's binding to epidermal proteins and nucleic acids. However, skin injuries significantly enhance uptake: abrasions allow 7.8–11.4% absorption, cuts 18.3–22.9%, and penetrating wounds up to 34–38.8%. Fine particles under 1 μm can penetrate the barrier, leading to , while embedded particles from cuts may cause localized ulcers or granulomas. Systemic effects can arise from repeated dermal exposure, particularly in workers handling beryllium-containing materials. Dust from beryllium processes can also irritate the eyes, causing or other ocular discomfort. Ingestion is a less common and minor route of exposure, typically occurring incidentally through hand-to-mouth transfer of contaminated or via contaminated and . via this pathway is very low, with absorption rates under 1% in animal models, and most ingested beryllium is excreted in . Gastrointestinal may result from higher doses, but systemic absorption remains negligible compared to or dermal routes.

Occupational and environmental exposure

Occupational exposure to beryllium primarily occurs in industries involving the , grinding, and fabrication of beryllium metal and , as well as in processes like and . Approximately 62,000 workers are exposed to beryllium in workplaces such as these, with exposures generated during activities that produce airborne particulates. To protect workers, the (OSHA) established a (PEL) of 0.2 μg/m³ as an 8-hour time-weighted average (TWA) and a (STEL) of 2.0 μg/m³, updated in the 2017 standard to address risks at lower levels than the previous PEL of 2.0 μg/m³. Environmental exposure to beryllium is generally low for the general , with primary sources including runoff from operations and industrial discharges into bodies. Beryllium does not undergo significant long-range atmospheric due to its particulate nature and tendency to deposit locally, limiting widespread aerial dispersion. The U.S. Agency (EPA) regulates beryllium in under the National Primary Drinking Water Regulations, setting a maximum contaminant level (MCL) of 4 (ppb) for chronic exposure to prevent adverse health effects. Mitigation strategies in occupational settings emphasize such as local exhaust ventilation to capture airborne beryllium particles at the source, supplemented by (PPE) including NIOSH-approved respirators with high-efficiency particulate air () filters. Employers must also implement medical surveillance programs, including the beryllium lymphocyte proliferation test (BeLPT) to detect in blood samples from exposed workers. Additionally, of beryllium-containing materials in controlled facilities can reduce overall exposure by minimizing the need for primary and , which generate higher dust levels.

Detection and regulation

Detection of beryllium in environmental and occupational settings relies on sensitive analytical techniques to ensure compliance with safety thresholds. (AAS), particularly graphite furnace AAS, is widely used for quantifying beryllium in air and samples, achieving a limit of detection (LOD) of approximately 0.1 μg/m³ in air filters and swipe samples for surface contamination. This method involves sample digestion followed by aspiration into a or furnace, providing reliable measurements for monitoring where concentrations must remain below regulatory limits. For biological monitoring, the beryllium lymphocyte proliferation test (BeLPT) assesses by measuring the proliferative response of lymphocytes to beryllium salts , serving as an early indicator of immune reactivity in exposed individuals. Regulatory frameworks enforce strict controls on beryllium exposure due to its carcinogenic potential. The National Institute for Occupational Safety and Health (NIOSH) classifies beryllium as a potential occupational and recommends maintaining exposures to the lowest detectable level; a ceiling value not to exceed 0.5 μg/m³ has been referenced to prevent and disease. In the , under regulation, beryllium is subject to restrictions in Annex XVII, prohibiting certain uses and requiring risk management measures, while its classification as a Category 1B under the mandates hazard labeling on products containing it above specified thresholds. Products and materials contaminated with beryllium must be labeled with warnings indicating its carcinogenic and respiratory hazards, as required by occupational safety standards like OSHA's Hazard Communication Standard. For surface contamination assessment, portable (XRF) spectrometry offers rapid, non-destructive screening, though its effectiveness for beryllium is limited by the element's low , often requiring complementary wipe sampling and laboratory confirmation. Genetic screening for the HLA-DPB1 , particularly variants carrying at position 69 (E69), identifies workers at elevated risk for beryllium sensitization and chronic beryllium disease, enabling targeted medical surveillance in high-exposure industries. Internationally, the provides a health-based value of 12 μg/L for beryllium in , derived from a tolerable daily intake allocation, though no formal guideline value is set due to limited occurrence in water supplies.

References

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