Atomnummer | 81 |
---|---|
Atommassa | 204.38 |
masstal | 205 |
Grupp | 13 |
---|---|
Period | 6 |
Block | p |
Protoner | 81 p+ |
---|---|
Neutroner | 124 n0 |
Electrons | 81 e- |
fysisk egenskap | |
---|---|
atomradie | 190 pm
|
molvolym | 17,2 cm³/mol
|
kovalent radie | 144 pm
|
Metallic Radius | 144 pm
|
ionic radius | 150 pm
|
Crystal Radius | 164 pm
|
Van der Waalsradie | 196 pm
|
densitet | 11,8 g/cm³
|
energi | |
proton affinity | |
Elektronaffinitet | 0,377 eV/particle
|
joniseringsenergi | 6,108287 eV/particle
|
ångbildningsvärme | 162,4 kJ/mol
|
smältvärme | 4,31 kJ/mol
|
Bildningsentalpi | 182,2 kJ/mol
|
Electrons | |
electron shell | 2, 8, 18, 32, 18, 3 |
valenselektron | 3 |
elektronkonfiguration | [Xe] 4f14 5d10 6s2 6p1 |
oxidationstal | -5, -2, -1, 1, 2, 3 |
elektronegativitet |
1.8
|
Electrophilicity | 0,9173102715055317 eV/particle
|
Phases | |
aggregationstillstånd | Fast |
Gas Phase | |
Kokpunkt | 1 746,15 K
|
Smältpunkt | 577,15 K
|
critical pressure | |
critical temperature | |
trippelpunkt | |
Visual | |
färg | Silver
|
appearance | silvery white |
Brytningsindex | |
materialegenskap | |
Värmeledningsförmåga | 46,1 W/(m K)
|
termisk expansion | 0,0000299 1/K
|
molar heat capacity | 26,32 J/(mol K)
|
Specifik värmekapacitet | 0,129 J/(g⋅K)
|
heat capacity ratio | |
electrical properties | |
type | Conductor |
elektrisk konduktivitet | 6,7 MS/m
|
resistivitet | 0,00000015 m Ω
|
supraledare | 2,38 K
|
magnetism | |
type | diamagnetic |
magnetisk susceptibilitet (Mass) | −0,000000003 m³/Kg
|
magnetisk susceptibilitet (Molar) | −0,000000000613 m³/mol
|
magnetisk susceptibilitet (Volume) | −0,0000356
|
magnetic ordering | |
Curiepunkten | |
Néel temperature | |
Structure | |
Kristallstruktur | Enkelt hexagonalt (HEX) |
Gitterkonstant | 3,46 Å
|
Lattice Angles | π/2, π/2, 2 π/3 |
mekanisk materialegenskap | |
hårdhet | 1,2 MPa
|
Kompressibilitet | 43 GPa
|
skjuvmodul | 2,8 GPa
|
Young's modulus | 8 GPa
|
Poissons konstant | 0,45
|
ljudhastighet | 818 m/s
|
klassificering | |
Kategori | Posttransitionsmetaller, Poor metals |
CAS Group | IIIB |
IUPAC Group | IIIA |
Glawe Number | 81 |
Mendeleev Number | 85 |
Pettifor Number | 78 |
Geochemical Class | |
Goldschmidt classification | chalcophile |
övrigt | |
Gas Basicity | |
Dipole Polarizability | |
C6 Dispersion Coefficient | |
Allotropes | |
Träffyta | 3,4
|
Neutron Mass Absorption | 0,00059
|
kvanttal | 2P1/2 |
rymdgrupp | 194 (P63/mmc) |
Stabila isotoper | 2 |
---|---|
Instabila isotoper | 41 |
Radioactive Isotopes | 41 |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 176 |
g-factor | |
Halveringstid | 6,2 ± 2,3 ms
|
Spinn | 3 |
nuclear quadrupole moment | |
upptäcktsdatum | 2004 |
Paritet | - |
decay mode | Intensitet |
---|---|
p (proton emission) | 100% |
α (α emission) | % |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 177 |
g-factor | |
Halveringstid | 18 ± 5 ms
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1999 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 73% |
p (proton emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 178 |
g-factor | |
Halveringstid | 255 ± 9 ms
|
Spinn | 4 |
nuclear quadrupole moment | |
upptäcktsdatum | 1997 |
Paritet | - |
decay mode | Intensitet |
---|---|
α (α emission) | 62% |
β+ (β+ decay; β+ = ϵ + e+) | 38% |
β+ SF (β+-delayed fission) | 0.15% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 179 |
g-factor | |
Halveringstid | 437 ± 9 ms
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1983 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 60% |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 180 |
g-factor | |
Halveringstid | 1,09 ± 0,01 s
|
Spinn | 4 |
nuclear quadrupole moment | |
upptäcktsdatum | 1987 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 93% |
α (α emission) | 7% |
β+ SF (β+-delayed fission) | 0.0032% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 181 |
g-factor | |
Halveringstid | 2,9 ± 0,1 s
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1996 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | % |
α (α emission) | 8.6% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 182 |
g-factor | |
Halveringstid | 1,9 ± 0,1 s
|
Spinn | 4 |
nuclear quadrupole moment | |
upptäcktsdatum | 1991 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
α (α emission) | 0.49% |
β+ SF (β+-delayed fission) | 3.4% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 183 |
g-factor | |
Halveringstid | 6,9 ± 0,7 s
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1980 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | % |
α (α emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 184 |
g-factor | |
Halveringstid | 9,5 ± 0,2 s
|
Spinn | 2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1976 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 98.78% |
α (α emission) | 1.22% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 185 |
g-factor | |
Halveringstid | 19,5 ± 0,5 s
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1976 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
α (α emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 186 |
g-factor | |
Halveringstid | 3,5 ± 0,5 s
|
Spinn | 2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1975 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | % |
α (α emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 187 |
g-factor | 3,08 ± 0,12
|
Halveringstid | |
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1976 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
α (α emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 188 |
g-factor | |
Halveringstid | 71 ± 2 s
|
Spinn | 2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1970 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 189 |
g-factor | |
Halveringstid | 2,3 ± 0,2 m
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1972 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 190 |
g-factor | |
Halveringstid | 2,6 ± 0,3 m
|
Spinn | 2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1970 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 191 |
g-factor | 3,164 ± 0,008
|
Halveringstid | |
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1974 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 192 |
g-factor | 0,0995 ± 0,0015
|
Halveringstid | 9,6 ± 0,4 m
|
Spinn | 2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1961 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 193 |
g-factor | 3,17 ± 0,006
|
Halveringstid | 21,6 ± 0,8 m
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1960 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 194 |
g-factor | 0,0695 ± 0,0015
|
Halveringstid | 33 ± 0,5 m
|
Spinn | 2 |
nuclear quadrupole moment | −0,282 ± 0,007
|
upptäcktsdatum | 1960 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
α (α emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 195 |
g-factor | 3,14 ± 0,08
|
Halveringstid | 1,16 ± 0,05 h
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1955 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 196 |
g-factor | 0,036 ± 0,0015
|
Halveringstid | 1,84 ± 0,03 h
|
Spinn | 2 |
nuclear quadrupole moment | −0,178 ± 0,014
|
upptäcktsdatum | 1955 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 197 |
g-factor | 3,14 ± 0,04
|
Halveringstid | 2,84 ± 0,04 h
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1955 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 198 |
g-factor | 0 ± 0,005
|
Halveringstid | 5,3 ± 0,5 h
|
Spinn | 2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1949 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 199 |
g-factor | 3,18 ± 0,04
|
Halveringstid | 7,42 ± 0,08 h
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1949 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 200 |
g-factor | 0,02 ± 0,005
|
Halveringstid | 26,1 ± 0,1 h
|
Spinn | 2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1949 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 201 |
g-factor | 3,198 ± 0,006
|
Halveringstid | 3,0421 ± 0,0008 d
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1950 |
Paritet | + |
decay mode | Intensitet |
---|---|
ϵ (electron capture) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 202 |
g-factor | 0,03 ± 0,005
|
Halveringstid | 12,31 ± 0,08 d
|
Spinn | 2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1940 |
Paritet | - |
decay mode | Intensitet |
---|---|
ϵ (electron capture) | 100% |
natural abundance | 29,515 ± 0,044
|
---|---|
relative atomic mass | |
masstal | 203 |
g-factor | |
Halveringstid | |
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1931 |
Paritet | + |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 204 |
g-factor | 0,045 ± 0,005
|
Halveringstid | 3,783 ± 0,012 y
|
Spinn | 2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1953 |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | 97.08% |
EC+B+ | 2.92% |
natural abundance | 70,485 ± 0,044
|
---|---|
relative atomic mass | |
masstal | 205 |
g-factor | |
Halveringstid | |
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1931 |
Paritet | + |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 206 |
g-factor | 0
|
Halveringstid | 4,202 ± 0,011 m
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1935 |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 207 |
g-factor | 3,738 ± 0,01
|
Halveringstid | 4,77 ± 0,02 m
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1908 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 208 |
g-factor | 0,0582 ± 0,0026
|
Halveringstid | 3,053 ± 0,004 m
|
Spinn | 5 |
nuclear quadrupole moment | |
upptäcktsdatum | 1909 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 209 |
g-factor | |
Halveringstid | 2,162 ± 0,007 m
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1950 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 210 |
g-factor | |
Halveringstid | 1,3 ± 0,03 m
|
Spinn | 5 |
nuclear quadrupole moment | |
upptäcktsdatum | 1909 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | 0.009% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 211 |
g-factor | |
Halveringstid | 81 ± 16 s
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1998 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | 2.2% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 212 |
g-factor | |
Halveringstid | 31 ± 8 s
|
Spinn | 5 |
nuclear quadrupole moment | |
upptäcktsdatum | 1998 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | 1.8% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 213 |
g-factor | |
Halveringstid | 23,8 ± 4,4 s
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 2010 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | 7.6% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 214 |
g-factor | |
Halveringstid | 11 ± 2,4 s
|
Spinn | 5 |
nuclear quadrupole moment | |
upptäcktsdatum | 2010 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | 34% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 215 |
g-factor | |
Halveringstid | 9,7 ± 3,8 s
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 2010 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | 4.6% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 216 |
g-factor | |
Halveringstid | 5,9 ± 3,3 s
|
Spinn | 5 |
nuclear quadrupole moment | |
upptäcktsdatum | 2010 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | 11.5% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 217 |
g-factor | |
Halveringstid | |
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 2010 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | % |
β− n (β−-delayed neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 218 |
g-factor | |
Halveringstid | |
Spinn | 6 |
nuclear quadrupole moment | |
upptäcktsdatum | |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | % |
β− n (β−-delayed neutron emission) | % |
upptäckare eller uppfinnare | Sir William Crookes |
---|---|
fyndplats | England |
upptäcktsdatum | 1861 |
etymologi | Greek: thallos (green twig), for a bright green line in its spectrum. |
uttal | THAL-i-em (engelska) |
1 | s | 1.5591 |
2 | p | 4.5138 |
2 | s | 21.3158 |
3 | d | 13.4658 |
3 | p | 22.6335 |
3 | s | 23.5809 |
4 | d | 37.6112 |
4 | f | 38.1324 |
4 | p | 35.7832 |
4 | s | 34.9212 |
5 | d | 58.975 |
5 | p | 53.9115 |
5 | s | 51.878 |
6 | p | 68.7462 |
6 | s | 68.1804 |