Scandium (Sc)
transition-metalSolid
标准原子量
44.955908 u电子排布
[Ar] 4s2 3d1熔点
1540.85 °C沸点
2835.85 °C密度
2990 kg/m³氧化态
0, +1, +2, +3电负性（鲍林）
1.36第一电离能
6.56149 eV发现年份
1879原子半径
160 pm详细信息
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.
图片
性质
物理性质
- 原子半径（经验值）
- 160 pm 比较所有元素的原子半径（经验值） →
- 共价半径
- 170 pm 比较所有元素的共价半径 →
- 范德华半径
- 211 pm 比较所有元素的范德华半径 →
- 金属半径
- 144 pm 比较所有元素的金属半径 →
- 密度
- 2990 kg/m³ 比较所有元素的密度 →
- 摩尔体积
- 0.015 L/mol
- 标准温度和压力下的物相
- 固态 比较所有元素的标准温度和压力下的物相 →
- 熔点
- 1540.85 °C 比较所有元素的熔点 →
- 沸点
- 2835.85 °C 比较所有元素的沸点 →
- 热导率
- 15.8 W/(m·K) 比较所有元素的热导率 →
- 比热容
- 0.568 J/(g·K) 比较所有元素的比热容 →
- 摩尔热容
- 25.52 J/(mol·K) 比较所有元素的摩尔热容 →
- 晶体结构
- 六方密堆积 比较所有元素的晶体结构 →
化学性质
- 电负性（鲍林）
- 1.36 比较所有元素的电负性（鲍林） →
- 电负性（Allen）
- 1.19
- 电子亲和能
- 0.188 eV
- 第一电离能
- 6.56149 eV 比较所有元素的第一电离能 →
- 第二电离能
- 12.799814 eV 比较所有元素的第二电离能 →
- 第三电离能
- 24.756924 eV 比较所有元素的第三电离能 →
- 第四电离能
- 73.489653 eV 比较所有元素的第四电离能 →
- 第五电离能
- 91.950317 eV 比较所有元素的第五电离能 →
- 氧化态
- 0, +1, +2, +3 比较所有元素的氧化态 →
- 价电子
- 3 比较所有元素的价电子 →
- 电子排布
- [Ar] 4s2 3d1
热力学性质
- 熔化热
- 0.16582889 eV 比较所有元素的熔化热 →
- 汽化热
- 3.256465 eV 比较所有元素的汽化热 →
- 升华热
- 3.923926 eV
- 原子化热
- 3.923926 eV
- 原子化焓
- 3.915635 eV
核性质
- 质子
- 21 比较所有元素的质子 →
- 中子
- 24 比较所有元素的中子 →
- 已知同位素
- 29 比较所有元素的已知同位素 →
- 稳定同位素
- 1 比较所有元素的稳定同位素 →
- 最稳定同位素
- Sc-45
- 发现年份
- 1879
丰度
- 丰度（地壳）
- 22 mg/kg 比较所有元素的丰度（地壳） →
- 丰度（海洋）
- 6 × 10−7 mg/L 比较所有元素的丰度（海洋） →
晶体结构
- 晶格常数a
- 331 pm
电子结构
- 各电子层电子数
- 2, 8, 9, 2 比较所有元素的各电子层电子数 →
标识符
- CAS登记号
- 7440-20-2 比较所有元素的CAS登记号 →
- 谱项符号
- 2D3/2
- InChI
- InChI=1S/Sc
- InChI Key
- SIXSYDAISGFNSX-UHFFFAOYSA-N
电子排布 实测值
Sc: 3d¹ 4s²[Ar] 3d¹ 4s²1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹ 4s²原子模型
不同同位素的中子数、质量和稳定性不同，但中性原子的电子排布不变。
原子模型示意图，未按比例绘制。
原子指纹
发射 / 吸收光谱
同位素分布
| 质量数 | 原子质量（u） | 天然丰度 | 半衰期 |
|---|---|---|---|
| 45 稳定 | 44.95590828 ± 0.00000077 | 100.0000% | 稳定 |
物相 / 状态
原因: 低于熔点（1540.85 °C）1515.8 °C
示意图，未按比例绘制
相变点
相变能
在熔点熔化1 mol物质所需的能量
在沸点汽化1 mol物质所需的能量
在升华点升华1 mol物质所需的能量
密度
标准条件下
标准条件下
原子光谱
已显示10项，共21项。 按离子电荷升序排列。
收录谱线 ?
| 离子 | 电荷 | 谱线总数 | 跃迁概率 | 能级标记 |
|---|---|---|---|---|
| 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 |
收录能级 ?
| 离子 | 电荷 | 能级 |
|---|---|---|
| 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 |
离子半径
| 电荷 | 配位 | 自旋 | 半径 |
|---|---|---|---|
| +3 | 6 | 暂无 | 74.5 pm |
| +3 | 8 | 暂无 | 87 pm |
化合物
同位素 (1)
| 质量数 | 原子质量（u） | 天然丰度 | 半衰期 | 衰变方式 | |
|---|---|---|---|---|---|
| 45 稳定 | 44.95590828 ± 0.00000077 | 100.0000% | 稳定 | stable |
谱线
已显示50项，共946项。 默认仅显示具有实测强度的谱线。
| 波长（nm） | 强度 | 电离级 | 类型 | 跃迁 | 准确度 | 来源 | |
|---|---|---|---|---|---|---|---|
| 683.5026 nm | 640 | Sc I | emission | 3d2.(3P).4s 2P → 3d2.(3P).4p 2S* | 实测值 | NIST | |
| 681.9491 nm | 485 | Sc I | emission | 3d.4s.(1D).4p 2F* → 3d.4s.(3D).5s 2D | 实测值 | NIST | |
| 673.7872 nm | 465 | Sc I | emission | 3d.4s.(3D).4p 2F* → 3d.4s.(3D).4d 2G | 实测值 | NIST | |
| 673.945 nm | 360 | Sc I | emission | 3d.4s.(3D).4p 2F* → 3d.4s.(3D).4d 2G | 实测值 | NIST | |
| 681.7117 nm | 345 | Sc I | emission | 3d2.(3P).4s 2P → 3d2.(3P).4p 2S* | 实测值 | NIST | |
| 682.9509 nm | 335 | Sc I | emission | 3d.4s.(1D).4p 2F* → 3d.4s.(3D).5s 2D | 实测值 | NIST | |
| 406.8661 nm | 100 | Sc III | emission | 3p6.4d 2D → 3p6.4f 2F* | 实测值 | NIST | |
| 744.9141 nm | 90 | Sc III | emission | 3p6.5s 2S → 3p6.5p 2P* | 实测值 | NIST | |
| 406.121 nm | 80 | Sc III | emission | 3p6.4d 2D → 3p6.4f 2F* | 实测值 | NIST | |
| 625.6013 nm | 80 | Sc III | emission | 3p6.4d 2D → 3p6.5p 2P* | 实测值 | NIST | |
| 503.2072 nm | 60 | Sc III | emission | 3p6.5p 2P* → 3p6.5d 2D | 实测值 | NIST | |
| 630.7603 nm | 60 | Sc III | emission | 3p6.4d 2D → 3p6.5p 2P* | 实测值 | NIST | |
| 499.2886 nm | 50 | Sc III | emission | 3p6.5p 2P* → 3p6.5d 2D | 实测值 | NIST | |
| 652.5571 nm | 40 | Sc I | emission | 3d.4s.(3D).4p 2D* → 3d.4s.(3D).4d 2D | 实测值 | NIST | |
| 671.4599 nm | 40 | Sc I | emission | 3d.4s.(3D).4p 2D* → 3d.4s.(3D).4d 4D | 实测值 | NIST | |
| 655.7842 nm | 35 | Sc I | emission | 3d.4s.(1D).4p 2F* → 3d3 2D2 | 实测值 | NIST | |
| 688.5119 nm | 27 | Sc I | emission | 3d2.(3F).4p 4F* → 3d2.(3F).4d 4G | 实测值 | NIST | |
| 716.9083 nm | 27 | Sc I | emission | 3d.4s.(3D).4p 2D* → 3d.4s.(3D).4d 2F | 实测值 | NIST | |
| 688.1012 nm | 26 | Sc I | emission | 3d2.(3F).4p 4F* → 3d2.(3F).4d 4G | 实测值 | NIST | |
| 662.0207 nm | 21 | Sc I | emission | 3d.4s.(3D).4p 2F* → 3d3 2F | 实测值 | NIST | |
| 713.8107 nm | 19 | Sc I | emission | 3d.4s.(3D).4p 2D* → 3d.4s.(3D).4d 2F | 实测值 | NIST | |
| 467.0407 nm | 18 | Sc II | emission | 3p6.3d2 1D → 3p6.3d.4p 1F* | 实测值 | NIST | |
| 673.0754 nm | 18 | Sc I | emission | 3d2.(3F).4p 4D* → 4P | 实测值 | NIST | |
| 687.7343 nm | 18 | Sc I | emission | 3d2.(3F).4p 4F* → 3d2.(3F).4d 4G | 实测值 | NIST | |
| 431.4083 nm | 17 | Sc II | emission | 3p6.3d2 3F → 3p6.3d.4p 3D* | 实测值 | NIST | |
| 503.1021 nm | 17 | Sc II | emission | 3p6.3d2 1D → 3p6.3d.4p 1P* | 实测值 | NIST | |
| 680.4611 nm | 17 | Sc I | emission | 3d2.(3F).4p 4F* → 3d2.(3F).4d 4D | 实测值 | NIST | |
| 437.4457 nm | 16 | Sc II | emission | 3p6.3d2 3F → 3p6.3d.4p 3F* | 实测值 | NIST | |
| 523.9813 nm | 16 | Sc II | emission | 3p6.4s2 1S → 3p6.3d.4p 1P* | 实测值 | NIST | |
| 552.679 nm | 16 | Sc II | emission | 3p6.3d2 1G → 3p6.3d.4p 1F* | 实测值 | NIST | |
| 430.5714 nm | 15 | Sc II | emission | 3p6.3d2 3F → 3p6.3d.4p 3D* | 实测值 | NIST | |
| 432.0732 nm | 15 | Sc II | emission | 3p6.3d2 3F → 3p6.3d.4p 3D* | 实测值 | NIST | |
| 478.0863 nm | 15 | Sc III | emission | 3p6.5p 2P* → 3p6.6s 2S | 实测值 | NIST | |
| 565.7896 nm | 15 | Sc II | emission | 3p6.3d2 3P → 3p6.3d.4p 3P* | 实测值 | NIST | |
| 624.5637 nm | 15 | Sc II | emission | 3p6.3d2 3P → 3p6.3d.4p 3D* | 实测值 | 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] | 实测值 | NIST | |
| 637.0486 nm | 14 | Sc II | emission | 3p6.3d.4d 1F → 3p6.3d.4f 1G* | 实测值 | NIST | |
| 660.4601 nm | 14 | Sc II | emission | 3p6.3d2 1D → 3p6.3d.4p 1D* | 实测值 | NIST | |
| 680.3677 nm | 14 | Sc I | emission | 3d.4s.(3D).4p 2F* → 3d.4s.(3D).4d 2G | 实测值 | NIST | |
| 725.7589 nm | 14 | Sc I | emission | 3d2.(3F).4p 4F* → 3d.(2D).4p2.(3P) 4F | 实测值 | NIST | |
| 401.4484 nm | 13 | Sc II | emission | 3p6.3d.4s 1D → 3p6.3d.4p 3F* | 实测值 | NIST | |
| 429.4767 nm | 13 | Sc II | emission | 3p6.3d2 3F → 3p6.3d.4p 3D* | 实测值 | NIST | |
| 432.4996 nm | 13 | Sc II | emission | 3p6.3d2 3F → 3p6.3d.4p 3D* | 实测值 | NIST | |
| 564.1001 nm | 13 | Sc II | emission | 3p6.3d2 3P → 3p6.3d.4p 3P* | 实测值 | NIST | |
| 565.8361 nm | 13 | Sc II | emission | 3p6.3d2 3P → 3p6.3d.4p 3P* | 实测值 | NIST | |
| 566.9042 nm | 13 | Sc II | emission | 3p6.3d2 3P → 3p6.3d.4p 3P* | 实测值 | NIST | |
| 687.4193 nm | 13 | Sc I | emission | 3d2.(3F).4p 4F* → 3d2.(3F).4d 4G | 实测值 | NIST | |
| 385.9595 nm | 12 | Sc II | emission | 3p6.3d.4p 1F* → 3p6.3d.5s 1D | 实测值 | NIST | |
| 424.6822 nm | 12 | Sc II | emission | 3p6.3d.4s 1D → 3p6.3d.4p 1D* | 实测值 | NIST | |
| 435.4598 nm | 12 | Sc II | emission | 3p6.3d2 3F → 3p6.3d.4p 3F* | 实测值 | NIST |
扩展性质
共价半径（扩展）
- 共价半径（Pyykkö）
- 148 pm
- 共价半径（Pyykkö，双键）
- 116 pm
- 共价半径（Pyykkö，三键）
- 114 pm
范德华半径
- Batsanov
- 230 pm
- Alvarez
- 258 pm
- UFF
- 329.5 pm
- MM3
- 261 pm
原子半径与金属半径
- 原子半径（Rahm）
- 263 pm
- 金属半径（C12）
- 162 pm
编号标度
- Mendeleev
- 11
- Pettifor
- 20
- Glawe
- 48
电负性标度
- Ghosh
- 0
- Miedema
- 3
- Gunnarsson–Lundqvist
- 4
- Robles–Bartolotti
- 3
极化率与色散
- 偶极极化率
- 97 a.u.
- 偶极极化率（不确定度）
- 10 a.u.
- C₆
- 1383 Ha·Bohr6
- C₆ (Gould–Bučko)
- 1570 Ha·Bohr6
化学亲和力
- 质子亲和能
- 914 kJ/mol
- 气相碱性
- 892 kJ/mol
Miedema参数
- Miedema摩尔体积
- 15.03 cm3/mol
- Miedema电子密度
- 2
供应风险与经济性
- 生产集中度
- 97
- 相对供应风险
- 10
- 储量分布
- 50
- 政治稳定性（最大生产国）
- 24
- 政治稳定性（最大储量国）
- 24
相变与同素异形体
| 熔点 | 1814.15 K |
| 沸点 | 3109.15 K |
氧化态分类
高级参考数据
屏蔽常数 (7)
| n | 轨道 | 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 |
晶体半径详情 (2)
| 电荷 | CN | 自旋 | rcrystal (pm) | 来源 |
|---|---|---|---|---|
| 3 | VI | 88.5 | from r^3 vs V plots, | |
| 3 | VIII | 101 | from r^3 vs V plots, |
同位素衰变方式 (52)
| 同位素 | 模式 | 强度 |
|---|---|---|
| 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射线散射因子 (598)
| 能量 (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 |
补充数据
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.