Scandium (Sc)
transition-metalSolid
標準原子量
44.955908 u電子配置
[Ar] 4s2 3d1融点
1540.85 °C沸点
2835.85 °C密度
2990 kg/m³酸化数
0, +1, +2, +3電気陰性度（Pauling）
1.36第1イオン化エネルギー
6.56149 eV発見年
1879原子半径
160 pm詳細
Scandium is a light transition metal with chemistry dominated by the +3 oxidation state. It is chemically similar to yttrium and the lanthanides, but its small ionic radius gives some distinct coordination behavior. The element is widely dispersed in minerals and rarely occurs in rich, easily worked ores. Its technological importance is concentrated in specialty aluminum alloys, high-intensity lighting, and research materials rather than large-volume metal use.
Scandium is a silver-white metal which develops a slightly yellowish or pinkish cast upon exposure to air. A relatively soft element, scandium resembles yttrium and the rare-earth metals more than it resembles aluminum or titanium.
It is a very light metal and has a much higher melting point than aluminum, making it of interest to designers of spacecraft. Scandium is not attacked by a 1:1 mixture of HNO3 and 48% HF.
Chemically it is one of the alkaline earth elements; it readily forms a white coating of nitride in air, reacts with water, burns with a yellow-red flame.
The name derives from the Latin scandia for Scandinavia, where the mineral was found. It was discovered by the Swedish chemist Lars-Fredrik Nilson in 1879 in an ytterbium sample. In the same year, the Swedish chemist Per Theodore Cleve proved that scandium was Mendeleev's predicted "eka-boron".
Scandium was discovered by Lars Fredrik Nilson, a Swedish chemist, in 1879 while attempting to produce a sample of pure ytterbia from 10 kilograms of the mineral euxenite ((Y, Ca, Er, La, Ce, U, Th)(Nb, Ta, Ti)2O6). Scandium can be obtained from the minerals thortveitite ((Sc, Y)2Si2O7), bazzite (Be3(Sc, Al)2Si6O18) and wiikite, but is usually obtained as a byproduct of refining uranium. Metallic scandium was first produced in 1937 and the first pound (0.45 kilograms) of pure scandium was produced in 1960. Scandium is a soft, light metal that might have applications in the aerospace industry. With a cost of $270 per gram ($122,500 per pound), scandium is too expensive for widespread use.
From the Latin word Scandia, Scandinavia. On the basis of the Periodic System, Mendeleev predicted the existence of ekaboron, which would have an atomic weight between 40 of calcium and 48 of titanium. The element was discovered by Nilson in 1878 in the minerals euxenite and gadolinite, which had not yet been found anywhere except in Scandinavia. By processing 10 kg of euxenite and other residues of rare-earth minerals, Nilson was able to prepare about 2g of highly pure scandium oxide. Later scientists pointed out that Nilson's scandium was identical with Mendeleev's ekaboron.
Pure scandium is a soft, silvery-white metal that tarnishes slowly in air, developing a yellowish or pinkish cast from surface oxidation. It is much less dense than most transition metals and can be cut or worked more readily than refractory metals.
Small additions of scandium strengthen aluminum alloys and improve weldability, especially in high-performance aerospace, sporting, and additive-manufactured components. Scandium iodide, ScI₃, has been used with sodium iodide, NaI, in metal-halide lamps to produce a bright, sunlight-like spectrum. Scandium compounds are also used in research on solid oxide fuel cells, ceramics, catalysts, and optical materials. The radioisotope ⁴⁴Sc is investigated for positron emission tomography, but such medical use depends on isotope production and radiochemical handling rather than bulk scandium metal.
Alloys of scandium and aluminum are used in some kinds of athletic equipment, such as aluminum baseball bats, bicycle frames and lacrosse sticks. It is expected that scandium-aluminum alloys will be important in the manufacture of fuel cells.
Scientists have only studied a few compounds of scandium. About 20 kilograms (44 pounds) of scandium oxide (Sc2O3), also known as scandia, are used each year in the United States in the production of high intensity lights. Scandium iodide (ScI3) is added to mercury vapor lamps so that they will emit light that closely resembles sunlight.
About 20 kg of scandium (as Sc2O3) are used yearly in the U.S. to produce high-intensity lights. The radioactive isotope 46Sc is used as a tracing agent in refinery crackers for crude oil, etc.
Scandium iodide added to mercury vapor lamps produces a highly efficient light source resembling sunlight, which is important for indoor or night-time color TV.
Isotopes in Biology
Radioactive 46Sc is used as a non-absorbed isotopic reference material for determining digestibility, absorption in the gut, and secretion sites for nutrients associated with feed residues in ruminating animals (animals that chew their food repeatedly for an extended period of time) [190] J. K. Miller, W. F. Byrne. J. Nutr.100, 1287 (1970)..
Isotopes in Earth/Planetary Science
The radioactive isotope 46Sc has been used for sediment labeling to determine the transportation of sediments by water flow in rivers, estuaries, harbors, and seas. The half-life of 46Sc is about 84 days and when released into an estuary with similar grain density and grain size, a gamma spectrometer (instrument for measuring the intensity of gamma radiation versus the energy of each photon) can be used to measure the intensities of 46Sc in the sediments and the movement of the sediments can be determined [191] A. Plata-Bedmar. Topical Reports, IAEA Bulletin (1988)., [192] K. Krishnamurthy, S. M. Rao. J. Hydrol.19, 189 (1973)., [193] I. Rehana, K. A. Shahid, S. Husain, D. Muhammad. Appl. Radiat. Isot.51, 115 (1999)..
Isotopes in Industry
46Sc is a beta emitter and has been used as a tracer in oil refinery crackers for crude oil (converting crude oil into gasoline and other lower-molecular weight hydrocarbon fractions). Its beta radiation enables the substance to be tracked as the oil travels [194] J. Guizerix, V. Markovic, P. Airey. Nuclear Techniques for Peaceful Development, IAEA Bulletin (1987).. Due to its easily traceable properties, coastal engineers use 46Sc to develop dredging strategies and to design navigation channels based on silt movement [192] K. Krishnamurthy, S. M. Rao. J. Hydrol.19, 189 (1973)..
Isotopes in Medicine
46Sc is used in isotope-carrying antibodies for bonding with tumor-associated cell surface antigens (substances that causes the production of an antibody when introduced into the body, e.g. toxins, bacteria, and viruses). 46Sc is added to DTPA-derivatized (process by which a compound is chemically changed, producing a new compound that has properties more amenable to a particular analytical method) monoclonal antibodies and has been shown to target tumor cells, specifically in vivo, where it accumulates to high levels in the tumor (Fig. IUPAC.21.1) [195] W. T. Anderson, M. Strand. Cancer Res.45, 2154 (1985)., [196] J. E. Eyles, I. D. Spiers, E. D. Williamson, H. O. Alpar, E. D. Williamson. J. Pharm. Pharmacol.53, 601 (2001)..
Scandium forms predominantly trivalent compounds containing Sc³⁺. Scandium oxide, Sc₂O₃, is a refractory white solid and an important intermediate for preparing other scandium materials. Scandium fluoride, ScF₃, and scandium chloride, ScCl₃, are common salts, with the anhydrous chloride used in some synthetic chemistry. Organoscandium and scandium triflate, Sc(OTf)₃, are useful Lewis acids in research-scale catalysis. Stable lower oxidation states are uncommon under ordinary conditions, although unusual low-valent scandium species can be stabilized in specialized molecular or solid-state environments.
See more information at the Scandium compound page.
Massive scandium metal has low acute toxicity data and is not known to be biologically essential. Finely divided metal dust can present fire or explosion hazards and may irritate the respiratory tract. Soluble scandium salts should be handled as toxicologically incompletely characterized metal compounds. Radioactive scandium isotopes present isotope-specific radiation hazards; ⁴⁶Sc, for example, is a gamma emitter used mainly as a tracer and calibration source.
Little is yet known about the toxicity of scandium; therefore it should be handled with care.
Scandium is a trace constituent of many crustal rocks, commonly substituting for magnesium, iron, aluminum, or rare-earth elements in minerals. It has no major independent biogeochemical cycle and is not a nutrient. Weathering can disperse scandium into soils and sediments, where it tends to remain in mineral phases or adsorb to oxides and clays. Environmental releases are usually associated with mining, ore processing, and industrial handling of scandium-bearing residues.
Scandium is not mined widely as a primary product. Commercial supply is usually recovered as a by-product from selected uranium, titanium, nickel, rare-earth, or bauxite-related processing streams, where scandium is present at low concentrations. The main barrier to wider alloy use is not intrinsic performance but dependable, low-cost supply and purification capacity. Recycling is limited because scandium is used in small amounts and often dispersed in aluminum alloy scrap. Substitution is possible in many applications, but few substitutes reproduce the same strengthening effect in aluminum at such low additions.
Scandium is apparently much more abundant (the 23rd most) in the sun and certain stars than on earth (the 50th most abundant). It is widely distributed on earth, occurring in very minute quantities in over 800 mineral species. The blue color of beryl (aquamarine variety) is said to be due to scandium. It occurs as a principal component in the rare mineral thortveitite, found in Scandinavia and Malagasy. It is also found in the residues remaining after the extraction of tungsten from Zinnwald wolframite, and in wiikite and bazzite.
Most scandium is presently being recovered from thortveitite or is extracted as a by-product from uranium mill tailings. Metallic scandium was first prepared in 1937 by Fischer, Brunger, and Grienelaus who electrolyzed a eutectic melt of potassium, lithium, and scandium chlorides at 700 to 800°C. Tungsten wire and a pool of molten zinc served as the electrodes in a graphite crucible. Pure scandium is now produced by reducing scandium fluoride with calcium metal.
The production of the first pound of 99% pure scandium metal was announced in 1960.
Scandium is a relatively rare odd-Z element in the cosmos. It is produced in stellar nucleosynthesis and supernova-related processes, but in lower abundance than neighboring even-Z elements such as calcium and titanium. In planetary materials it behaves lithophile, concentrating mainly in silicate minerals rather than metallic cores or volatile phases.
- Scandium was discovered after its existence was predicted from a gap below boron in early periodic tables.
- Its name comes from Scandinavia, where scandium-bearing minerals were first studied.
- Aluminum-scandium alloys can retain fine strengthening precipitates after welding better than many conventional aluminum
- Scandium is often grouped with rare-earth elements in processing, although it is not a lanthanide.
- Natural scandium consists almost entirely of the stable isotope ⁴⁵Sc.
- Scandium oxide has a high melting point and is used as a precursor for many scandium chemicals.
画像
性質
物理的性質
- 原子半径（経験値）
- 160 pm 全元素の原子半径（経験値）を比較 →
- 共有結合半径
- 170 pm 全元素の共有結合半径を比較 →
- ファンデルワールス半径
- 211 pm 全元素のファンデルワールス半径を比較 →
- 金属半径
- 144 pm 全元素の金属半径を比較 →
- 密度
- 2990 kg/m³ 全元素の密度を比較 →
- モル体積
- 0.015 L/mol
- 標準温度・圧力（STP）での相
- 固体 全元素の標準温度・圧力（STP）での相を比較 →
- 融点
- 1540.85 °C 全元素の融点を比較 →
- 沸点
- 2835.85 °C 全元素の沸点を比較 →
- 熱伝導率
- 15.8 W/(m·K) 全元素の熱伝導率を比較 →
- 比熱容量
- 0.568 J/(g·K) 全元素の比熱容量を比較 →
- モル熱容量
- 25.52 J/(mol·K) 全元素のモル熱容量を比較 →
- 結晶構造
- 六方最密充填構造 全元素の結晶構造を比較 →
化学的性質
- 電気陰性度（Pauling）
- 1.36 全元素の電気陰性度（Pauling）を比較 →
- 電気陰性度（Allen）
- 1.19
- 電子親和力
- 0.188 eV
- 第1イオン化エネルギー
- 6.56149 eV 全元素の第1イオン化エネルギーを比較 →
- 第2イオン化エネルギー
- 12.799814 eV 全元素の第2イオン化エネルギーを比較 →
- 第3イオン化エネルギー
- 24.756924 eV 全元素の第3イオン化エネルギーを比較 →
- 第4イオン化エネルギー
- 73.489653 eV 全元素の第4イオン化エネルギーを比較 →
- 第5イオン化エネルギー
- 91.950317 eV 全元素の第5イオン化エネルギーを比較 →
- 酸化数
- 0, +1, +2, +3 全元素の酸化数を比較 →
- 価電子
- 3 全元素の価電子を比較 →
- 電子配置
- [Ar] 4s2 3d1
熱力学的性質
- 融解熱
- 0.16582889 eV 全元素の融解熱を比較 →
- 蒸発熱
- 3.256465 eV 全元素の蒸発熱を比較 →
- 昇華熱
- 3.923926 eV
- 原子化熱
- 3.923926 eV
- 原子化エンタルピー
- 3.915635 eV
原子核
- 陽子数
- 21 全元素の陽子数を比較 →
- 中性子数
- 24 全元素の中性子数を比較 →
- 既知の同位体
- 29 全元素の既知の同位体を比較 →
- 安定同位体
- 1 全元素の安定同位体を比較 →
- 最も安定な同位体
- Sc-45
- 発見年
- 1879
存在度
- 存在度（地殻）
- 22 mg/kg 全元素の存在度（地殻）を比較 →
- 存在度（海洋）
- 6 × 10−7 mg/L 全元素の存在度（海洋）を比較 →
結晶構造
- 格子定数a
- 331 pm
電子構造
- 各電子殻の電子数
- 2, 8, 9, 2 全元素の各電子殻の電子数を比較 →
識別子
- CAS登録番号
- 7440-20-2 全元素のCAS登録番号を比較 →
- 項記号
- 2D3/2
- InChI
- InChI=1S/Sc
- InChI Key
- SIXSYDAISGFNSX-UHFFFAOYSA-N
電子配置 測定値
Sc: 3d¹ 4s²[Ar] 3d¹ 4s²1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹ 4s²原子モデル
同位体によって中性子数、質量、安定性は変わりますが、中性原子の電子配置は変わりません。
模式的な原子モデルです。実際の縮尺とは異なります。
原子の指紋
発光／吸収スペクトル
同位体分布
| 質量数 | 原子質量（u） | 天然存在比 | 半減期 |
|---|---|---|---|
| 45 安定 | 44.95590828 ± 0.00000077 | 100.0000% | 安定 |
相／状態
理由: 融点（1540.85 °C）より1515.8 °C低い
模式図、実際の縮尺とは異なります
相転移点
相転移エネルギー
融点で1 molを融解させるのに必要なエネルギー
沸点で1 molを蒸発させるのに必要なエネルギー
昇華点で1 molを昇華させるのに必要なエネルギー
密度
標準条件下
標準条件下
原子スペクトル
全21件中10件を表示しています。 イオンの電荷の昇順で並べています。
スペクトル線データの収録状況 ?
| イオン | 電荷 | スペクトル線の総数 | 遷移確率 | 準位の表記 |
|---|---|---|---|---|
| Sc I | 0 | 2198 | 260 | 1682 |
| Sc II | +1 | 829 | 139 | 829 |
| Sc III | +2 | 133 | 97 | 133 |
| Sc IV | +3 | 408 | 4 | 408 |
| Sc V | +4 | 456 | 16 | 456 |
| Sc VI | +5 | 79 | 12 | 75 |
| Sc VII | +6 | 70 | 37 | 70 |
| Sc VIII | +7 | 75 | 48 | 75 |
| Sc IX | +8 | 42 | 22 | 42 |
| Sc X | +9 | 99 | 29 | 99 |
準位データの収録状況 ?
| イオン | 電荷 | 準位 |
|---|---|---|
| Sc I | 0 | 478 |
| Sc II | +1 | 169 |
| Sc III | +2 | 44 |
| Sc IV | +3 | 129 |
| Sc V | +4 | 119 |
| Sc VI | +5 | 40 |
| Sc VII | +6 | 35 |
| Sc VIII | +7 | 27 |
| Sc IX | +8 | 27 |
| Sc X | +9 | 68 |
イオン半径
| 電荷 | 配位 | スピン | 半径 |
|---|---|---|---|
| +3 | 6 | データなし | 74.5 pm |
| +3 | 8 | データなし | 87 pm |
化合物
同位体 (1)
| 質量数 | 原子質量（u） | 天然存在比 | 半減期 | 崩壊形式 | |
|---|---|---|---|---|---|
| 45 安定 | 44.95590828 ± 0.00000077 | 100.0000% | 安定 | stable |
スペクトル線
全946件中50件を表示しています。 初期設定では、強度の測定値があるスペクトル線のみを表示します。
| 波長（nm） | 強度 | 電離段階 | 種類 | 遷移 | 精度 | 出典 | |
|---|---|---|---|---|---|---|---|
| 683.5026 nm | 640 | Sc I | emission | 3d2.(3P).4s 2P → 3d2.(3P).4p 2S* | 測定値 | NIST | |
| 681.9491 nm | 485 | Sc I | emission | 3d.4s.(1D).4p 2F* → 3d.4s.(3D).5s 2D | 測定値 | NIST | |
| 673.7872 nm | 465 | Sc I | emission | 3d.4s.(3D).4p 2F* → 3d.4s.(3D).4d 2G | 測定値 | NIST | |
| 673.945 nm | 360 | Sc I | emission | 3d.4s.(3D).4p 2F* → 3d.4s.(3D).4d 2G | 測定値 | NIST | |
| 681.7117 nm | 345 | Sc I | emission | 3d2.(3P).4s 2P → 3d2.(3P).4p 2S* | 測定値 | NIST | |
| 682.9509 nm | 335 | Sc I | emission | 3d.4s.(1D).4p 2F* → 3d.4s.(3D).5s 2D | 測定値 | NIST | |
| 406.8661 nm | 100 | Sc III | emission | 3p6.4d 2D → 3p6.4f 2F* | 測定値 | NIST | |
| 744.9141 nm | 90 | Sc III | emission | 3p6.5s 2S → 3p6.5p 2P* | 測定値 | NIST | |
| 406.121 nm | 80 | Sc III | emission | 3p6.4d 2D → 3p6.4f 2F* | 測定値 | NIST | |
| 625.6013 nm | 80 | Sc III | emission | 3p6.4d 2D → 3p6.5p 2P* | 測定値 | NIST | |
| 503.2072 nm | 60 | Sc III | emission | 3p6.5p 2P* → 3p6.5d 2D | 測定値 | NIST | |
| 630.7603 nm | 60 | Sc III | emission | 3p6.4d 2D → 3p6.5p 2P* | 測定値 | NIST | |
| 499.2886 nm | 50 | Sc III | emission | 3p6.5p 2P* → 3p6.5d 2D | 測定値 | NIST | |
| 652.5571 nm | 40 | Sc I | emission | 3d.4s.(3D).4p 2D* → 3d.4s.(3D).4d 2D | 測定値 | NIST | |
| 671.4599 nm | 40 | Sc I | emission | 3d.4s.(3D).4p 2D* → 3d.4s.(3D).4d 4D | 測定値 | NIST | |
| 655.7842 nm | 35 | Sc I | emission | 3d.4s.(1D).4p 2F* → 3d3 2D2 | 測定値 | NIST | |
| 688.5119 nm | 27 | Sc I | emission | 3d2.(3F).4p 4F* → 3d2.(3F).4d 4G | 測定値 | NIST | |
| 716.9083 nm | 27 | Sc I | emission | 3d.4s.(3D).4p 2D* → 3d.4s.(3D).4d 2F | 測定値 | NIST | |
| 688.1012 nm | 26 | Sc I | emission | 3d2.(3F).4p 4F* → 3d2.(3F).4d 4G | 測定値 | NIST | |
| 662.0207 nm | 21 | Sc I | emission | 3d.4s.(3D).4p 2F* → 3d3 2F | 測定値 | NIST | |
| 713.8107 nm | 19 | Sc I | emission | 3d.4s.(3D).4p 2D* → 3d.4s.(3D).4d 2F | 測定値 | NIST | |
| 467.0407 nm | 18 | Sc II | emission | 3p6.3d2 1D → 3p6.3d.4p 1F* | 測定値 | NIST | |
| 673.0754 nm | 18 | Sc I | emission | 3d2.(3F).4p 4D* → 4P | 測定値 | NIST | |
| 687.7343 nm | 18 | Sc I | emission | 3d2.(3F).4p 4F* → 3d2.(3F).4d 4G | 測定値 | NIST | |
| 431.4083 nm | 17 | Sc II | emission | 3p6.3d2 3F → 3p6.3d.4p 3D* | 測定値 | NIST | |
| 503.1021 nm | 17 | Sc II | emission | 3p6.3d2 1D → 3p6.3d.4p 1P* | 測定値 | NIST | |
| 680.4611 nm | 17 | Sc I | emission | 3d2.(3F).4p 4F* → 3d2.(3F).4d 4D | 測定値 | NIST | |
| 437.4457 nm | 16 | Sc II | emission | 3p6.3d2 3F → 3p6.3d.4p 3F* | 測定値 | NIST | |
| 523.9813 nm | 16 | Sc II | emission | 3p6.4s2 1S → 3p6.3d.4p 1P* | 測定値 | NIST | |
| 552.679 nm | 16 | Sc II | emission | 3p6.3d2 1G → 3p6.3d.4p 1F* | 測定値 | NIST | |
| 430.5714 nm | 15 | Sc II | emission | 3p6.3d2 3F → 3p6.3d.4p 3D* | 測定値 | NIST | |
| 432.0732 nm | 15 | Sc II | emission | 3p6.3d2 3F → 3p6.3d.4p 3D* | 測定値 | NIST | |
| 478.0863 nm | 15 | Sc III | emission | 3p6.5p 2P* → 3p6.6s 2S | 測定値 | NIST | |
| 565.7896 nm | 15 | Sc II | emission | 3p6.3d2 3P → 3p6.3d.4p 3P* | 測定値 | NIST | |
| 624.5637 nm | 15 | Sc II | emission | 3p6.3d2 3P → 3p6.3d.4p 3D* | 測定値 | NIST | |
| 577.1538 nm | 14 | Sc IV | emission | 3s2.3p5.(2P*<3/2>).5s 2[3/2]* → 3s2.3p5.(2P*<3/2>).5p 2[5/2] | 測定値 | NIST | |
| 637.0486 nm | 14 | Sc II | emission | 3p6.3d.4d 1F → 3p6.3d.4f 1G* | 測定値 | NIST | |
| 660.4601 nm | 14 | Sc II | emission | 3p6.3d2 1D → 3p6.3d.4p 1D* | 測定値 | NIST | |
| 680.3677 nm | 14 | Sc I | emission | 3d.4s.(3D).4p 2F* → 3d.4s.(3D).4d 2G | 測定値 | NIST | |
| 725.7589 nm | 14 | Sc I | emission | 3d2.(3F).4p 4F* → 3d.(2D).4p2.(3P) 4F | 測定値 | NIST | |
| 401.4484 nm | 13 | Sc II | emission | 3p6.3d.4s 1D → 3p6.3d.4p 3F* | 測定値 | NIST | |
| 429.4767 nm | 13 | Sc II | emission | 3p6.3d2 3F → 3p6.3d.4p 3D* | 測定値 | NIST | |
| 432.4996 nm | 13 | Sc II | emission | 3p6.3d2 3F → 3p6.3d.4p 3D* | 測定値 | NIST | |
| 564.1001 nm | 13 | Sc II | emission | 3p6.3d2 3P → 3p6.3d.4p 3P* | 測定値 | NIST | |
| 565.8361 nm | 13 | Sc II | emission | 3p6.3d2 3P → 3p6.3d.4p 3P* | 測定値 | NIST | |
| 566.9042 nm | 13 | Sc II | emission | 3p6.3d2 3P → 3p6.3d.4p 3P* | 測定値 | NIST | |
| 687.4193 nm | 13 | Sc I | emission | 3d2.(3F).4p 4F* → 3d2.(3F).4d 4G | 測定値 | NIST | |
| 385.9595 nm | 12 | Sc II | emission | 3p6.3d.4p 1F* → 3p6.3d.5s 1D | 測定値 | NIST | |
| 424.6822 nm | 12 | Sc II | emission | 3p6.3d.4s 1D → 3p6.3d.4p 1D* | 測定値 | NIST | |
| 435.4598 nm | 12 | Sc II | emission | 3p6.3d2 3F → 3p6.3d.4p 3F* | 測定値 | NIST |
詳細な性質
共有結合半径（詳細）
- 共有結合半径（Pyykkö）
- 148 pm
- 共有結合半径（Pyykkö、二重結合）
- 116 pm
- 共有結合半径（Pyykkö、三重結合）
- 114 pm
ファンデルワールス半径
- Batsanov
- 230 pm
- Alvarez
- 258 pm
- UFF
- 329.5 pm
- MM3
- 261 pm
原子半径と金属半径
- 原子半径（Rahm）
- 263 pm
- 金属半径（C12）
- 162 pm
番号付けの尺度
- Mendeleev
- 11
- Pettifor
- 20
- Glawe
- 48
電気陰性度の尺度
- Ghosh
- 0
- Miedema
- 3
- Gunnarsson–Lundqvist
- 4
- Robles–Bartolotti
- 3
分極率と分散
- 双極子分極率
- 97 a.u.
- 双極子分極率（不確かさ）
- 10 a.u.
- C₆
- 1383 Ha·Bohr6
- C₆ (Gould–Bučko)
- 1570 Ha·Bohr6
化学親和力
- プロトン親和力
- 914 kJ/mol
- 気相塩基性
- 892 kJ/mol
ミーデマパラメータ
- ミーデマモル体積
- 15.03 cm3/mol
- ミーデマ電子密度
- 2
供給リスクと経済性
- 生産集中度
- 97
- 相対供給リスク
- 10
- 埋蔵量の分布
- 50
- 政治的安定性（最大生産国）
- 24
- 政治的安定性（最大埋蔵国）
- 24
相転移と同素体
| 融点 | 1814.15 K |
| 沸点 | 3109.15 K |
酸化数の分類
専門参考データ
遮蔽定数 (7)
| n | 軌道 | σ |
|---|---|---|
| 1 | s | 0.5434 |
| 2 | p | 3.9454 |
| 2 | s | 6.4264 |
| 3 | d | 13.8801 |
| 3 | p | 11.5938 |
| 3 | s | 10.6602 |
| 4 | s | 16.3676 |
結晶半径の詳細 (2)
| 電荷 | CN | スピン | rcrystal (pm) | 由来 |
|---|---|---|---|---|
| 3 | VI | 88.5 | from r^3 vs V plots, | |
| 3 | VIII | 101 | from r^3 vs V plots, |
同位体の崩壊形式 (52)
| 同位体 | モード | 強度 |
|---|---|---|
| 35 | p | — |
| 36 | p | — |
| 37 | p | — |
| 38 | p | — |
| 39 | p | 100% |
| 40 | B+ | 100% |
| 40 | B+p | 0.4% |
| 40 | B+A | 0% |
| 41 | B+ | 100% |
| 42 | B+ | 100% |
X線散乱因子 (598)
| エネルギー (eV) | f₁ | f₂ |
|---|---|---|
| 10 | — | 1.06978 |
| 10.1617 | — | 1.07987 |
| 10.3261 | — | 1.09005 |
| 10.4931 | — | 1.10033 |
| 10.6628 | — | 1.11071 |
| 10.8353 | — | 1.12118 |
| 11.0105 | — | 1.13176 |
| 11.1886 | — | 1.14243 |
| 11.3696 | — | 1.15321 |
| 11.5535 | — | 1.16408 |
追加データ
Estimated Crustal Abundance
The estimated element abundance in the earth's crust.
2.2×101 milligrams per kilogram
参考文献 (1)
- [5] Scandium https://education.jlab.org/itselemental/ele021.html
Estimated Oceanic Abundance
The estimated element abundance in the earth's oceans.
6×10-7 milligrams per liter
参考文献 (1)
- [5] Scandium https://education.jlab.org/itselemental/ele021.html
Sources
Sources of this element.
Scandium is apparently much more abundant (the 23rd most) in the sun and certain stars than on earth (the 50th most abundant). It is widely distributed on earth, occurring in very minute quantities in over 800 mineral species. The blue color of beryl (aquamarine variety) is said to be due to scandium. It occurs as a principal component in the rare mineral thortveitite, found in Scandinavia and Malagasy. It is also found in the residues remaining after the extraction of tungsten from Zinnwald wolframite, and in wiikite and bazzite.
Most scandium is presently being recovered from thortveitite or is extracted as a by-product from uranium mill tailings. Metallic scandium was first prepared in 1937 by Fischer, Brunger, and Grienelaus who electrolyzed a eutectic melt of potassium, lithium, and scandium chlorides at 700 to 800°C. Tungsten wire and a pool of molten zinc served as the electrodes in a graphite crucible. Pure scandium is now produced by reducing scandium fluoride with calcium metal.
The production of the first pound of 99% pure scandium metal was announced in 1960.
参考文献 (1)
- [6] Scandium https://periodic.lanl.gov/21.shtml
参考文献
(9)
Data deposited in or computed by PubChem
The half-life and atomic mass data was provided by the Atomic Mass Data Center at the International Atomic Energy Agency.
Element data are cited from the Atomic weights of the elements (an IUPAC Technical Report). The IUPAC periodic table of elements can be found at https://iupac.org/what-we-do/periodic-table-of-elements/. Additional information can be found within IUPAC publication doi:10.1515/pac-2015-0703 Copyright © 2020 International Union of Pure and Applied Chemistry.
The information are cited from Pure Appl. Chem. 2018; 90(12): 1833-2092, https://doi.org/10.1515/pac-2015-0703.
Thomas Jefferson National Accelerator Facility (Jefferson Lab) is one of 17 national laboratories funded by the U.S. Department of Energy. The lab's primary mission is to conduct basic research of the atom's nucleus using the lab's unique particle accelerator, known as the Continuous Electron Beam Accelerator Facility (CEBAF). For more information visit https://www.jlab.org/
The periodic table at the LANL (Los Alamos National Laboratory) contains basic element information together with the history, source, properties, use, handling and more. The provenance data may be found from the link under the source name.
The periodic table contains NIST's critically-evaluated data on atomic properties of the elements. The provenance data that include data for atomic spectroscopy, X-ray and gamma ray, radiation dosimetry, nuclear physics, and condensed matter physics may be found from the link under the source name. Ref: https://www.nist.gov/pml/atomic-spectra-database
This section provides all form of data related to element Scandium.
The element property data was retrieved from publications.