Atomnummer | 90 |
---|---|
Atommassa | 232.0377 |
masstal | 232 |
Grupp | |
---|---|
Period | 7 |
Block | f |
Protoner | 90 p+ |
---|---|
Neutroner | 142 n0 |
Electrons | 90 e- |
atomradie | 180 pm
|
---|---|
molvolym | 19,8 cm³/mol
|
kovalent radie | 175 pm
|
Metallic Radius | |
ionic radius | 94 pm
|
Crystal Radius | 108 pm
|
Van der Waalsradie | 245 pm
|
densitet | 11,7 g/cm³
|
energi | |
proton affinity | |
Elektronaffinitet | |
joniseringsenergi | 6,3067 eV/particle
|
ångbildningsvärme | 513,7 kJ/mol
|
smältvärme | 16,11 kJ/mol
|
Bildningsentalpi | 602 kJ/mol
|
Electrons | |
electron shell | 2, 8, 18, 32, 18, 10, 2 |
valenselektron | 2 |
elektronkonfiguration | [Rn] 6d2 7s2 |
oxidationstal | -1, 1, 2, 3, 4 |
elektronegativitet |
1.3
|
Electrophilicity | |
Phases | |
aggregationstillstånd | Fast |
Gas Phase | |
Kokpunkt | 5 058,15 K
|
Smältpunkt | 2 023,15 K
|
critical pressure | |
critical temperature | |
trippelpunkt | |
Visual | |
färg | Silver
|
appearance | silvery, often with black tarnish |
Brytningsindex | |
materialegenskap | |
Värmeledningsförmåga | |
termisk expansion | 0,000011 1/K
|
molar heat capacity | 27,32 J/(mol K)
|
Specifik värmekapacitet | 0,118 J/(g⋅K)
|
heat capacity ratio | |
electrical properties | |
type | Conductor |
elektrisk konduktivitet | 6,7 MS/m
|
resistivitet | 0,00000015 m Ω
|
supraledare | 1,38 K
|
magnetism | |
type | paramagnetic |
magnetisk susceptibilitet (Mass) | 0,0000000072 m³/Kg
|
magnetisk susceptibilitet (Molar) | 0,0000000017 m³/mol
|
magnetisk susceptibilitet (Volume) | 0,000084
|
magnetic ordering | |
Curiepunkten | |
Néel temperature | |
Structure | |
Kristallstruktur | Ytcentrerat kubiskt (FCC) |
Gitterkonstant | 5,08 Å
|
Lattice Angles | π/2, π/2, π/2 |
mekanisk materialegenskap | |
hårdhet | 3 MPa
|
Kompressibilitet | 54 GPa
|
skjuvmodul | 31 GPa
|
Young's modulus | 79 GPa
|
Poissons konstant | 0,27
|
ljudhastighet | 2 490 m/s
|
klassificering | |
Kategori | Aktinider, Actinides |
CAS Group | |
IUPAC Group | |
Glawe Number | 34 |
Mendeleev Number | 16 |
Pettifor Number | 47 |
Geochemical Class | rare earth & related |
Goldschmidt classification | litophile |
övrigt | |
Gas Basicity | |
Dipole Polarizability | |
C6 Dispersion Coefficient | |
Allotropes | |
Träffyta | 7,4
|
Neutron Mass Absorption | 0,001
|
kvanttal | 3F2 |
rymdgrupp | 225 (Fm_3m) |
Stabila isotoper | 2 |
---|---|
Instabila isotoper | 30 |
Radioactive Isotopes | 32 |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 208 |
g-factor | 0
|
Halveringstid | 2,4 ± 1,2 ms
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 2010 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 209 |
g-factor | |
Halveringstid | |
Spinn | 5/2 |
nuclear quadrupole moment | |
upptäcktsdatum | |
Paritet | - |
decay mode | Intensitet |
---|---|
α (α emission) | % |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 210 |
g-factor | 0
|
Halveringstid | 16 ± 3,6 ms
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1995 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 211 |
g-factor | |
Halveringstid | 48 ± 20 ms
|
Spinn | 5/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1995 |
Paritet | - |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 212 |
g-factor | 0
|
Halveringstid | 31,7 ± 1,3 ms
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1980 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 213 |
g-factor | |
Halveringstid | 144 ± 21 ms
|
Spinn | 5/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1968 |
Paritet | - |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 214 |
g-factor | 0
|
Halveringstid | 87 ± 10 ms
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1968 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 215 |
g-factor | |
Halveringstid | 1,35 ± 0,14 s
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1968 |
Paritet | - |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 216 |
g-factor | 0
|
Halveringstid | 26,28 ± 0,16 ms
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1968 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 217 |
g-factor | |
Halveringstid | 248 ± 4 us
|
Spinn | 9/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1968 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 218 |
g-factor | 0
|
Halveringstid | 122 ± 5 ns
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1973 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 219 |
g-factor | |
Halveringstid | 1,023 ± 0,018 us
|
Spinn | 9/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1973 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 220 |
g-factor | 0
|
Halveringstid | 10,2 ± 0,3 us
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1973 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
ϵ (electron capture) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 221 |
g-factor | |
Halveringstid | 1,75 ± 0,02 ms
|
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1970 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 222 |
g-factor | 0
|
Halveringstid | 2,24 ± 0,03 ms
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1970 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
ϵ (electron capture) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 223 |
g-factor | |
Halveringstid | 600 ± 20 ms
|
Spinn | 5/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1952 |
Paritet |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 224 |
g-factor | 0
|
Halveringstid | 1,04 ± 0,02 s
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1949 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
2β+ (double β+ decay) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 225 |
g-factor | |
Halveringstid | 8,75 ± 0,04 m
|
Spinn | 3/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1949 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 90% |
ϵ (electron capture) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 226 |
g-factor | 0
|
Halveringstid | 30,7 ± 0,03 m
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1948 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
18O | 3.2% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 227 |
g-factor | |
Halveringstid | 18,693 ± 0,004 d
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1906 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 228 |
g-factor | 0
|
Halveringstid | 1,9125 ± 0,0007 y
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1905 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
20O | 1.13% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 229 |
g-factor | 0,184 ± 0,016
|
Halveringstid | 7,916 ± 0,017 ky
|
Spinn | 5/2 |
nuclear quadrupole moment | 3,11 ± 0,06
|
upptäcktsdatum | 1947 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
natural abundance | Radioactive ☢️ 0,02 ± 0,02
|
---|---|
relative atomic mass | |
masstal | 230 |
g-factor | 0
|
Halveringstid | 75,4 ± 0,3 ky
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1907 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
SF (spontaneous fission) | 4% |
24Ne (heavy cluster emission) | 5.8% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 231 |
g-factor | |
Halveringstid | 25,52 ± 0,01 h
|
Spinn | 5/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1911 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ 99,98 ± 0,02
|
---|---|
relative atomic mass | |
masstal | 232 |
g-factor | 0
|
Halveringstid | 14 ± 0,1 Gy
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1898 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
SF (spontaneous fission) | 1.1% |
26Ne | 2.78% |
2β− (double β− decay) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 233 |
g-factor | |
Halveringstid | 21,83 ± 0,04 m
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1935 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 234 |
g-factor | 0
|
Halveringstid | 24,107 ± 0,024 d
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1900 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
α (α emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 235 |
g-factor | |
Halveringstid | 7,2 ± 0,1 m
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1969 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 236 |
g-factor | 0
|
Halveringstid | 37,3 ± 1,5 m
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1973 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 237 |
g-factor | |
Halveringstid | 4,8 ± 0,5 m
|
Spinn | 5/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1993 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 238 |
g-factor | 0
|
Halveringstid | 9,4 ± 2 m
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1999 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
upptäckare eller uppfinnare | Jöns Berzelius |
---|---|
fyndplats | Sweden |
upptäcktsdatum | 1828 |
etymologi | Named for Thor, Norse god of thunder. |
uttal | THOR-i-em (engelska) |