Atomnummer | 21 |
---|---|
Atommassa | 44.955908 |
masstal | 45 |
Grupp | 3 |
---|---|
Period | 4 |
Block | d |
Protoner | 21 p+ |
---|---|
Neutroner | 24 n0 |
Electrons | 21 e- |
fysisk egenskap | |
---|---|
atomradie | 160 pm
|
molvolym | 15 cm³/mol
|
kovalent radie | 148 pm
|
Metallic Radius | 144 pm
|
ionic radius | 74,5 pm
|
Crystal Radius | 88,5 pm
|
Van der Waalsradie | 215 pm
|
densitet | 2,99 g/cm³
|
energi | |
proton affinity | 914 kJ/mol
|
Elektronaffinitet | 0,188 eV/particle
|
joniseringsenergi | 6,56149 eV/particle
|
ångbildningsvärme | 332,7 kJ/mol
|
smältvärme | 15,8 kJ/mol
|
Bildningsentalpi | 377,8 kJ/mol
|
Electrons | |
electron shell | 2, 8, 9, 2 |
valenselektron | 2 |
elektronkonfiguration | [Ar] 3d1 4s2 |
oxidationstal | 0, 1, 2, 3 |
elektronegativitet | 1.36
|
Electrophilicity | 0,8934589851890408 eV/particle
|
Phases | |
aggregationstillstånd | Fast |
Gas Phase | |
Kokpunkt | 3 109,15 K
|
Smältpunkt | 1 814,15 K
|
critical pressure | |
critical temperature | |
trippelpunkt | |
Visual | |
färg | Silver
|
appearance | silvery white |
Brytningsindex | |
materialegenskap | |
Värmeledningsförmåga | 15,8 W/(m K)
|
termisk expansion | 0,0000102 1/K
|
molar heat capacity | 25,52 J/(mol K)
|
Specifik värmekapacitet | 0,568 J/(g⋅K)
|
heat capacity ratio | |
electrical properties | |
type | Conductor |
elektrisk konduktivitet | 1,8 MS/m
|
resistivitet | 0,00000055 m Ω
|
supraledare | 0,05 K
|
magnetism | |
type | paramagnetic |
magnetisk susceptibilitet (Mass) | 0,000000088 m³/Kg
|
magnetisk susceptibilitet (Molar) | 0,000000003956 m³/mol
|
magnetisk susceptibilitet (Volume) | 0,0002627
|
magnetic ordering | |
Curiepunkten | |
Néel temperature | |
Structure | |
Kristallstruktur | Enkelt hexagonalt (HEX) |
Gitterkonstant | 3,31 Å
|
Lattice Angles | π/2, π/2, 2 π/3 |
mekanisk materialegenskap | |
hårdhet | |
Kompressibilitet | 57 GPa
|
skjuvmodul | 29 GPa
|
Young's modulus | 74 GPa
|
Poissons konstant | 0,28
|
ljudhastighet | |
klassificering | |
Kategori | Övergångsmetaller, Transition metals |
CAS Group | IIIA |
IUPAC Group | IIIB |
Glawe Number | 48 |
Mendeleev Number | 11 |
Pettifor Number | 20 |
Geochemical Class | first series transition metal |
Goldschmidt classification | litophile |
övrigt | |
Gas Basicity | 892 kJ/mol
|
Dipole Polarizability | |
C6 Dispersion Coefficient | 1 383 a₀
|
Allotropes | |
Träffyta | 27,2
|
Neutron Mass Absorption | 0,025
|
kvanttal | 2D3/2 |
rymdgrupp | 194 (P63/mmc) |
Stabila isotoper | 1 |
---|---|
Instabila isotoper | 28 |
Radioactive Isotopes | 23 |
natural abundance | |
---|---|
relative atomic mass | |
masstal | 35 |
g-factor | |
Halveringstid | |
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | |
Paritet | - |
decay mode | Intensitet |
---|---|
p (proton emission) | % |
natural abundance | |
---|---|
relative atomic mass | |
masstal | 36 |
g-factor | |
Halveringstid | |
Spinn | |
nuclear quadrupole moment | |
upptäcktsdatum | |
Paritet |
decay mode | Intensitet |
---|---|
p (proton emission) | % |
natural abundance | |
---|---|
relative atomic mass | |
masstal | 37 |
g-factor | |
Halveringstid | |
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | |
Paritet | - |
decay mode | Intensitet |
---|---|
p (proton emission) | % |
natural abundance | |
---|---|
relative atomic mass | |
masstal | 38 |
g-factor | |
Halveringstid | |
Spinn | 2 |
nuclear quadrupole moment | |
upptäcktsdatum | |
Paritet | - |
decay mode | Intensitet |
---|---|
p (proton emission) | % |
natural abundance | |
---|---|
relative atomic mass | |
masstal | 39 |
g-factor | |
Halveringstid | |
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1988 |
Paritet | - |
decay mode | Intensitet |
---|---|
p (proton emission) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 40 |
g-factor | |
Halveringstid | 182,3 ± 0,7 ms
|
Spinn | 4 |
nuclear quadrupole moment | |
upptäcktsdatum | 1955 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
β+ p (β+-delayed proton emission) | 0.44% |
β+α (β+-delayed α emission) | 0.017% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 41 |
g-factor | 1,5509428571429 ± 0,0004
|
Halveringstid | 596,3 ± 1,7 ms
|
Spinn | 7/2 |
nuclear quadrupole moment | −0,145 ± 0,003
|
upptäcktsdatum | 1941 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 42 |
g-factor | 0
|
Halveringstid | 680,72 ± 0,26 ms
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1955 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 43 |
g-factor | 1,2931428571429 ± 0,0028571428571429
|
Halveringstid | 3,891 ± 0,012 h
|
Spinn | 7/2 |
nuclear quadrupole moment | −0,27 ± 0,05
|
upptäcktsdatum | 1935 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 44 |
g-factor | 1,249 ± 0,0025
|
Halveringstid | 4,0421 ± 0,0025 h
|
Spinn | 2 |
nuclear quadrupole moment | 0,1 ± 0,05
|
upptäcktsdatum | 1937 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | 100
|
---|---|
relative atomic mass | |
masstal | 45 |
g-factor | 1,3582857142857 ± 0,000022857142857143
|
Halveringstid | |
Spinn | 7/2 |
nuclear quadrupole moment | −0,22 ± 0,002
|
upptäcktsdatum | 1923 |
Paritet | - |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 46 |
g-factor | 0,76 ± 0,002
|
Halveringstid | 83,757 ± 0,014 d
|
Spinn | 4 |
nuclear quadrupole moment | 0,119 ± 0,006
|
upptäcktsdatum | 1936 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 47 |
g-factor | 1,5257142857143 ± 0,0057142857142857
|
Halveringstid | 3,3492 ± 0,0006 d
|
Spinn | 7/2 |
nuclear quadrupole moment | −0,22 ± 0,03
|
upptäcktsdatum | 1945 |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 48 |
g-factor | 0,62283333333333 ± 0,002
|
Halveringstid | 43,67 ± 0,09 h
|
Spinn | 6 |
nuclear quadrupole moment | |
upptäcktsdatum | 1937 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 49 |
g-factor | 1,6028571428571 ± 0,0085714285714286
|
Halveringstid | 57,18 ± 0,13 m
|
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1940 |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 50 |
g-factor | |
Halveringstid | 102,5 ± 0,5 s
|
Spinn | 5 |
nuclear quadrupole moment | |
upptäcktsdatum | 1959 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 51 |
g-factor | |
Halveringstid | 12,4 ± 0,1 s
|
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1966 |
Paritet |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 52 |
g-factor | |
Halveringstid | 8,2 ± 0,2 s
|
Spinn | 3 |
nuclear quadrupole moment | |
upptäcktsdatum | 1980 |
Paritet |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 53 |
g-factor | |
Halveringstid | 2,4 ± 0,6 s
|
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1980 |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 54 |
g-factor | |
Halveringstid | 526 ± 15 ms
|
Spinn | 3 |
nuclear quadrupole moment | |
upptäcktsdatum | 1990 |
Paritet |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | 16% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 55 |
g-factor | |
Halveringstid | 96 ± 2 ms
|
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1990 |
Paritet |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | 17% |
2n (2-neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 56 |
g-factor | |
Halveringstid | 26 ± 6 ms
|
Spinn | 1 |
nuclear quadrupole moment | |
upptäcktsdatum | 1997 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | % |
2n (2-neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 57 |
g-factor | |
Halveringstid | 22 ± 2 ms
|
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1997 |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | % |
2n (2-neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 58 |
g-factor | |
Halveringstid | 12 ± 5 ms
|
Spinn | 3 |
nuclear quadrupole moment | |
upptäcktsdatum | 1997 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | % |
2n (2-neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 59 |
g-factor | |
Halveringstid | |
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 2009 |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | % |
β− n (β−-delayed neutron emission) | % |
2n (2-neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 60 |
g-factor | |
Halveringstid | |
Spinn | 3 |
nuclear quadrupole moment | |
upptäcktsdatum | 2009 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | % |
β− n (β−-delayed neutron emission) | % |
2n (2-neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 61 |
g-factor | |
Halveringstid | |
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 2009 |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | % |
β− n (β−-delayed neutron emission) | % |
2n (2-neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 62 |
g-factor | |
Halveringstid | |
Spinn | |
nuclear quadrupole moment | |
upptäcktsdatum | 2018 |
Paritet |
decay mode | Intensitet |
---|---|
β− (β− decay) | % |
β− n (β−-delayed neutron emission) | % |
2n (2-neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 63 |
g-factor | |
Halveringstid | |
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | % |
β− n (β−-delayed neutron emission) | % |
2n (2-neutron emission) | % |
upptäckare eller uppfinnare | Lars Nilson |
---|---|
fyndplats | Sweden |
upptäcktsdatum | 1879 |
etymologi | Latin: Scandia, Scandinavia. |
uttal | SKAN-di-em (engelska) |
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 |