Atomnummer | 80 |
---|---|
Atommassa | 200.592 |
masstal | 202 |
Grupp | 12 |
---|---|
Period | 6 |
Block | d |
Protoner | 80 p+ |
---|---|
Neutroner | 122 n0 |
Electrons | 80 e- |
fysisk egenskap | |
---|---|
atomradie | 150 pm
|
molvolym | 14,8 cm³/mol
|
kovalent radie | 133 pm
|
Metallic Radius | 139 pm
|
ionic radius | 97 pm
|
Crystal Radius | 111 pm
|
Van der Waalsradie | 223 pm
|
densitet | 13,5336 g/cm³
|
energi | |
proton affinity | |
Elektronaffinitet | |
joniseringsenergi | 10,437504 eV/particle
|
ångbildningsvärme | 58,5 kJ/mol
|
smältvärme | 2,295 kJ/mol
|
Bildningsentalpi | 61,38 kJ/mol
|
Electrons | |
electron shell | 2, 8, 18, 32, 18, 2 |
valenselektron | 2 |
elektronkonfiguration | [Xe] 4f14 5d10 6s2 |
oxidationstal | -2, 1, 2 |
elektronegativitet | 1.9
|
Electrophilicity | |
Phases | |
aggregationstillstånd | Flytande |
Gas Phase | |
Kokpunkt | 629,769 K
|
Smältpunkt | 234,321 K
|
critical pressure | 167 MPa
|
critical temperature | 1 764,15 K
|
trippelpunkt | 234,3156 K
|
Visual | |
färg | Silver
|
appearance | silvery |
Brytningsindex | 1,000933
|
materialegenskap | |
Värmeledningsförmåga | 8,3 W/(m K)
|
termisk expansion | 0,000181 1/K
|
molar heat capacity | 27,983 J/(mol K)
|
Specifik värmekapacitet | 0,14 J/(g⋅K)
|
heat capacity ratio | |
electrical properties | |
type | Conductor |
elektrisk konduktivitet | 1 MS/m
|
resistivitet | 0,00000096 m Ω
|
supraledare | 4,154 K
|
magnetism | |
type | diamagnetic |
magnetisk susceptibilitet (Mass) | −0,0000000021 m³/Kg
|
magnetisk susceptibilitet (Molar) | −0,000000000421 m³/mol
|
magnetisk susceptibilitet (Volume) | −0,0000284
|
magnetic ordering | |
Curiepunkten | |
Néel temperature | |
Structure | |
Kristallstruktur | Enkelt trigonal (RHL) |
Gitterkonstant | 2,99 Å
|
Lattice Angles | 1.23081, 1.23081, 1.23081 |
mekanisk materialegenskap | |
hårdhet | |
Kompressibilitet | 25 GPa
|
skjuvmodul | |
Young's modulus | |
Poissons konstant | |
ljudhastighet | 1 407 m/s
|
klassificering | |
Kategori | Övergångsmetaller, Transition metals |
CAS Group | IIB |
IUPAC Group | IIB |
Glawe Number | 76 |
Mendeleev Number | 79 |
Pettifor Number | 74 |
Geochemical Class | |
Goldschmidt classification | chalcophile |
övrigt | |
Gas Basicity | |
Dipole Polarizability | |
C6 Dispersion Coefficient | |
Allotropes | |
Träffyta | 374
|
Neutron Mass Absorption | 0,063
|
kvanttal | 1S0 |
rymdgrupp | 166 (R_3m) |
Stabila isotoper | 7 |
---|---|
Instabila isotoper | 40 |
Radioactive Isotopes | 40 |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 170 |
g-factor | 0
|
Halveringstid | 310 ± 250 us
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 2019 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 171 |
g-factor | |
Halveringstid | 70 ± 30 us
|
Spinn | 3/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 2004 |
Paritet | - |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 172 |
g-factor | 0
|
Halveringstid | 231 ± 9 us
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1999 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 173 |
g-factor | |
Halveringstid | 800 ± 80 us
|
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1999 |
Paritet | - |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 174 |
g-factor | 0
|
Halveringstid | 2 ± 0,4 ms
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1997 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 175 |
g-factor | |
Halveringstid | 10,2 ± 0,3 ms
|
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1983 |
Paritet | - |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 176 |
g-factor | 0
|
Halveringstid | 20,3 ± 1,4 ms
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1983 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 90% |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 177 |
g-factor | −0,29142857142857 ± 0,014285714285714
|
Halveringstid | 117 ± 7 ms
|
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1975 |
Paritet | - |
decay mode | Intensitet |
---|---|
α (α emission) | 100% |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 178 |
g-factor | 0
|
Halveringstid | 266,5 ± 2,4 ms
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1971 |
Paritet | + |
decay mode | Intensitet |
---|---|
α (α emission) | 89% |
β+ (β+ decay; β+ = ϵ + e+) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 179 |
g-factor | −0,26857142857143 ± 0,0057142857142857
|
Halveringstid | 1,05 ± 0,03 s
|
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1970 |
Paritet | - |
decay mode | Intensitet |
---|---|
α (α emission) | 75% |
β+ (β+ decay; β+ = ϵ + e+) | 25% |
β+ p (β+-delayed proton emission) | 0.15% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 180 |
g-factor | 0
|
Halveringstid | 2,59 ± 0,01 s
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1970 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 52% |
α (α emission) | 48% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 181 |
g-factor | |
Halveringstid | 3,6 ± 0,1 s
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1969 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 73% |
α (α emission) | 27% |
β+ p (β+-delayed proton emission) | 0.014% |
β+α (β+-delayed α emission) | 9% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 182 |
g-factor | 0
|
Halveringstid | 10,83 ± 0,06 s
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1968 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 86.2% |
α (α emission) | 13.8% |
β+ p (β+-delayed proton emission) | 1% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 183 |
g-factor | |
Halveringstid | 9,4 ± 0,7 s
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1969 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 88.3% |
α (α emission) | 11.7% |
β+ p (β+-delayed proton emission) | 2.6% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 184 |
g-factor | 0
|
Halveringstid | 30,87 ± 0,26 s
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1969 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 98.89% |
α (α emission) | 1.11% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 185 |
g-factor | |
Halveringstid | 49,1 ± 1 s
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1960 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 94% |
α (α emission) | 6% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 186 |
g-factor | 0
|
Halveringstid | 1,38 ± 0,06 m
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1960 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
α (α emission) | 0.016% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 187 |
g-factor | |
Halveringstid | 1,9 ± 0,3 m
|
Spinn | 3/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1960 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
α (α emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 188 |
g-factor | 0
|
Halveringstid | 3,25 ± 0,15 m
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1960 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
α (α emission) | 3.7% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 189 |
g-factor | |
Halveringstid | 7,6 ± 0,2 m
|
Spinn | 3/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1955 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
α (α emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 190 |
g-factor | 0
|
Halveringstid | 20 ± 0,5 m
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1959 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
α (α emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 191 |
g-factor | |
Halveringstid | 49 ± 10 m
|
Spinn | 3/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1954 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
α (α emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 192 |
g-factor | 0
|
Halveringstid | 4,85 ± 0,2 h
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1952 |
Paritet | + |
decay mode | Intensitet |
---|---|
ϵ (electron capture) | 100% |
α (α emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 193 |
g-factor | −0,41673333333333 ± 0,00053333333333333
|
Halveringstid | 3,8 ± 0,15 h
|
Spinn | 3/2 |
nuclear quadrupole moment | −0,7 ± 0,3
|
upptäcktsdatum | 1952 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 194 |
g-factor | 0
|
Halveringstid | 447 ± 28 y
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1962 |
Paritet | + |
decay mode | Intensitet |
---|---|
ϵ (electron capture) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 195 |
g-factor | 1,0786 ± 0,0012
|
Halveringstid | 10,69 ± 0,16 h
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1952 |
Paritet | - |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | 0,15 ± 0,01
|
---|---|
relative atomic mass | |
masstal | 196 |
g-factor | 0
|
Halveringstid | |
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1930 |
Paritet | + |
decay mode | Intensitet |
---|---|
2β+ (double β+ decay) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 197 |
g-factor | 1,0506 ± 0,0012
|
Halveringstid | 64,93 ± 0,07 h
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1941 |
Paritet | - |
decay mode | Intensitet |
---|---|
ϵ (electron capture) | 100% |
natural abundance | 10,04 ± 0,03
|
---|---|
relative atomic mass | |
masstal | 198 |
g-factor | 0
|
Halveringstid | |
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1925 |
Paritet | + |
natural abundance | 16,94 ± 0,12
|
---|---|
relative atomic mass | |
masstal | 199 |
g-factor | 1,0078 ± 0,0012
|
Halveringstid | |
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1925 |
Paritet | - |
natural abundance | 23,14 ± 0,09
|
---|---|
relative atomic mass | |
masstal | 200 |
g-factor | 0
|
Halveringstid | |
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1925 |
Paritet | + |
natural abundance | 13,17 ± 0,09
|
---|---|
relative atomic mass | |
masstal | 201 |
g-factor | −0,372 ± 0,00046666666666667
|
Halveringstid | |
Spinn | 3/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1925 |
Paritet | - |
natural abundance | 29,74 ± 0,13
|
---|---|
relative atomic mass | |
masstal | 202 |
g-factor | 0
|
Halveringstid | |
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1920 |
Paritet | + |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 203 |
g-factor | |
Halveringstid | 46,61 ± 0,01 d
|
Spinn | 5/2 |
nuclear quadrupole moment | 0,344 ± 0,007
|
upptäcktsdatum | 1943 |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | 6,82 ± 0,04
|
---|---|
relative atomic mass | |
masstal | 204 |
g-factor | 0
|
Halveringstid | |
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1920 |
Paritet | + |
decay mode | Intensitet |
---|---|
2β− (double β− decay) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 205 |
g-factor | |
Halveringstid | 5,14 ± 0,09 m
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1940 |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 206 |
g-factor | 0
|
Halveringstid | 8,32 ± 0,07 m
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1961 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 207 |
g-factor | |
Halveringstid | 2,9 ± 0,2 m
|
Spinn | 9/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1982 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 208 |
g-factor | 0
|
Halveringstid | 135 ± 10 s
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1994 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 209 |
g-factor | |
Halveringstid | 6,3 ± 1,1 s
|
Spinn | 9/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1998 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 210 |
g-factor | 0
|
Halveringstid | 64 ± 12 s
|
Spinn | 0 |
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 | 211 |
g-factor | |
Halveringstid | 26,4 ± 8,1 s
|
Spinn | 9/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 2010 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | 6.3% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 212 |
g-factor | 0
|
Halveringstid | |
Spinn | 0 |
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 | 213 |
g-factor | |
Halveringstid | |
Spinn | 9/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 2010 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | % |
β− n (β−-delayed neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 214 |
g-factor | 0
|
Halveringstid | |
Spinn | 0 |
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 | 215 |
g-factor | |
Halveringstid | |
Spinn | 9/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 2010 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | % |
β− n (β−-delayed neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 216 |
g-factor | 0
|
Halveringstid | |
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 2010 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | % |
β− n (β−-delayed neutron emission) | % |
upptäckare eller uppfinnare | Known to the ancients. |
---|---|
fyndplats | |
upptäcktsdatum | |
etymologi | From the Roman god Mercury; symbol from Latin: hydrargyrus (liquid silver). |
uttal | MER-kyoo-ri (engelska) |
1 | s | 1.5419 |
2 | p | 4.499 |
2 | s | 20.8906 |
3 | d | 13.4804 |
3 | p | 22.4798 |
3 | s | 23.4587 |
4 | d | 37.532 |
4 | f | 38.2392 |
4 | p | 35.594 |
4 | s | 34.7552 |
5 | d | 59.144 |
5 | p | 54.033 |
5 | s | 51.889 |
6 | s | 68.8466 |