| Atomnummer | 110 |
|---|---|
| Atommassa | 281 |
| masstal | 267 |
| Grupp | 10 |
|---|---|
| Period | 7 |
| Block | d |
| proton | 110 p+ |
|---|---|
| neutron | 157 n0 |
| elektron | 110 e- |
| Atomradie | |
|---|---|
| molvolym | |
| Kovalent Radie | |
| Metallic Radius | |
| ionic radius | |
| Crystal Radius | |
| Van der Waalsradie | |
| densitet |
| energi | |
|---|---|
| proton affinity | |
| Elektronaffinitet | |
| joniseringsenergi | |
| ångbildningsvärme | |
| smältvärme | |
| Bildningsentalpi | |
| elektron | |
| electron shell | 2, 8, 18, 32, 32, 16, 2 |
| valenselektron | 1 ⓘ |
| elektronkonfiguration | [Rn] 5f14 6d9 7s1ⓘ 1s2 2s2 2p6 3s2 3p6 4s2 3d10 4p6 5s2 4d10 5p6 6s2 4f14 5d10 6p6 5f14 6d9 7s1 |
| oxidationstal | |
| elektronegativitet | |
| Electrophilicity Index | |
| fundamental state of matter | |
| aggregationstillstånd | {ERROR}|
| gaseous state of matter | |
| Kokpunkt | |
| Smältpunkt | |
| critical pressure | |
| critical temperature | |
| trippelpunkt | |
| appearance | |
| färg | Svart
|
| appearance | |
| Brytningsindex | |
| materialegenskap | |
| Värmeledningsförmåga | |
| termisk expansion | |
| molar heat capacity | |
| Specifik värmekapacitet | |
| heat capacity ratio | |
| electrical properties | |
| type | |
| elektrisk konduktivitet | |
| resistivitet | |
| supraledare | |
| magnetism | |
| type | |
| magnetisk susceptibilitet (Mass) | |
| magnetisk susceptibilitet (Molar) | |
| magnetisk susceptibilitet (Volume) | |
| magnetic ordering | |
| Curiepunkten | |
| Néel temperature | |
| struktur | |
| Kristallstruktur | {ERROR} |
| Gitterkonstant | |
| Lattice Angles | |
| mekanisk materialegenskap | |
| hårdhet | |
| Kompressibilitet | |
| skjuvmodul | |
| Young's modulus | |
| Poissons konstant | |
| ljudhastighet | |
| klassificering | |
| Kategori | Aktinider, Transition metals |
| CAS Group | VIIIA |
| IUPAC Group | VIII |
| Glawe Number | |
| Mendeleev Number | 70 |
| Pettifor Number | |
| Geochemical Class | |
| Goldschmidt classification | synthetic |
| Gas Basicity | |
|---|---|
| Polariserbarhet | |
| C6 Dispersion Coefficient | |
| allotrope | |
| Träffyta | |
| Neutron Mass Absorption | |
| kvanttal | 3D3 |
| rymdgrupp | () |
| Stabila isotoper | 0 |
|---|---|
| Instabila isotoper | 18 |
| Natural Isotopes | 0 |
| masstal | 267 |
|---|---|
| neutrontal | 157 |
| Relative Atomic Mass | |
| g-factor | |
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | 10 ± 8 us
|
| Spinn | 3/2 |
| nuclear quadrupole moment | |
| upptäcktsdatum | 1995 |
| Paritet | + |
| decay mode | Intensitet |
|---|---|
| α (α emission) | 100% |
| masstal | 268 |
|---|---|
| neutrontal | 158 |
| Relative Atomic Mass | |
| g-factor | 0
|
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | |
| Spinn | 0 |
| nuclear quadrupole moment | 0
|
| upptäcktsdatum | |
| Paritet | + |
| decay mode | Intensitet |
|---|---|
| α (α emission) |
| masstal | 269 |
|---|---|
| neutrontal | 159 |
| Relative Atomic Mass | |
| g-factor | |
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | 230 ± 110 us
|
| Spinn | |
| nuclear quadrupole moment | |
| upptäcktsdatum | 1995 |
| Paritet |
| decay mode | Intensitet |
|---|---|
| α (α emission) | 100% |
| masstal | 270 |
|---|---|
| neutrontal | 160 |
| Relative Atomic Mass | |
| g-factor | 0
|
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | 205 ± 48 us
|
| Spinn | 0 |
| nuclear quadrupole moment | 0
|
| upptäcktsdatum | 2001 |
| Paritet | + |
| decay mode | Intensitet |
|---|---|
| α (α emission) | 100% |
| SF (spontaneous fission) |
| masstal | 271 |
|---|---|
| neutrontal | 161 |
| Relative Atomic Mass | |
| g-factor | |
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | 144 ± 53 ms
|
| Spinn | |
| nuclear quadrupole moment | |
| upptäcktsdatum | 1998 |
| Paritet |
| decay mode | Intensitet |
|---|---|
| SF (spontaneous fission) | 75% |
| α (α emission) | 25% |
| masstal | 272 |
|---|---|
| neutrontal | 162 |
| Relative Atomic Mass | |
| g-factor | 0
|
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | |
| Spinn | 0 |
| nuclear quadrupole moment | 0
|
| upptäcktsdatum | |
| Paritet | + |
| decay mode | Intensitet |
|---|---|
| SF (spontaneous fission) |
| masstal | 273 |
|---|---|
| neutrontal | 163 |
| Relative Atomic Mass | |
| g-factor | |
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | 240 ± 100 us
|
| Spinn | |
| nuclear quadrupole moment | |
| upptäcktsdatum | 1996 |
| Paritet |
| decay mode | Intensitet |
|---|---|
| α (α emission) | 100% |
| masstal | 274 |
|---|---|
| neutrontal | 164 |
| Relative Atomic Mass | |
| g-factor | 0
|
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | |
| Spinn | 0 |
| nuclear quadrupole moment | 0
|
| upptäcktsdatum | |
| Paritet | + |
| decay mode | Intensitet |
|---|---|
| α (α emission) | |
| SF (spontaneous fission) |
| masstal | 275 |
|---|---|
| neutrontal | 165 |
| Relative Atomic Mass | |
| g-factor | |
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | |
| Spinn | |
| nuclear quadrupole moment | |
| upptäcktsdatum | |
| Paritet |
| decay mode | Intensitet |
|---|---|
| α (α emission) | |
| SF (spontaneous fission) |
| masstal | 276 |
|---|---|
| neutrontal | 166 |
| Relative Atomic Mass | |
| g-factor | 0
|
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | |
| Spinn | 0 |
| nuclear quadrupole moment | 0
|
| upptäcktsdatum | |
| Paritet | + |
| decay mode | Intensitet |
|---|---|
| α (α emission) | |
| SF (spontaneous fission) |
| masstal | 277 |
|---|---|
| neutrontal | 167 |
| Relative Atomic Mass | |
| g-factor | |
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | 6 ± 3 ms
|
| Spinn | |
| nuclear quadrupole moment | |
| upptäcktsdatum | 2010 |
| Paritet |
| decay mode | Intensitet |
|---|---|
| α (α emission) | 100% |
| SF (spontaneous fission) |
| masstal | 278 |
|---|---|
| neutrontal | 168 |
| Relative Atomic Mass | |
| g-factor | 0
|
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | |
| Spinn | 0 |
| nuclear quadrupole moment | 0
|
| upptäcktsdatum | |
| Paritet | + |
| decay mode | Intensitet |
|---|---|
| α (α emission) | |
| SF (spontaneous fission) |
| masstal | 279 |
|---|---|
| neutrontal | 169 |
| Relative Atomic Mass | |
| g-factor | |
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | 210 ± 40 ms
|
| Spinn | |
| nuclear quadrupole moment | |
| upptäcktsdatum | 2004 |
| Paritet |
| decay mode | Intensitet |
|---|---|
| SF (spontaneous fission) | 88% |
| α (α emission) | 12% |
| masstal | 280 |
|---|---|
| neutrontal | 170 |
| Relative Atomic Mass | |
| g-factor | 0
|
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | 25 ± 20 ms
|
| Spinn | 0 |
| nuclear quadrupole moment | 0
|
| upptäcktsdatum | 1999 |
| Paritet | + |
| decay mode | Intensitet |
|---|---|
| SF (spontaneous fission) | 100% |
| masstal | 281 |
|---|---|
| neutrontal | 171 |
| Relative Atomic Mass | |
| g-factor | |
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | 14 ± 3 s
|
| Spinn | |
| nuclear quadrupole moment | |
| upptäcktsdatum | 2004 |
| Paritet |
| decay mode | Intensitet |
|---|---|
| SF (spontaneous fission) | 90% |
| α (α emission) | 10% |
| masstal | 282 |
|---|---|
| neutrontal | 172 |
| Relative Atomic Mass | |
| g-factor | 0
|
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | 4,2 ± 3,3 m
|
| Spinn | 0 |
| nuclear quadrupole moment | 0
|
| upptäcktsdatum | 2016 |
| Paritet | + |
| decay mode | Intensitet |
|---|---|
| α (α emission) | 100% |
| SF (spontaneous fission) |
| masstal | 283 |
|---|---|
| neutrontal | 173 |
| Relative Atomic Mass | |
| g-factor | |
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | |
| Spinn | |
| nuclear quadrupole moment | |
| upptäcktsdatum | |
| Paritet |
| decay mode | Intensitet |
|---|---|
| α (α emission) | |
| SF (spontaneous fission) |
| masstal | 284 |
|---|---|
| neutrontal | 174 |
| Relative Atomic Mass | |
| g-factor | 0
|
| natural abundance | |
| radioaktivitet | ☢️ Radioaktivt grundämne |
| Halveringstid | |
| Spinn | 0 |
| nuclear quadrupole moment | 0
|
| upptäcktsdatum | |
| Paritet | + |
| decay mode | Intensitet |
|---|---|
| α (α emission) | |
| SF (spontaneous fission) |
| upptäckare eller uppfinnare | Heavy Ion Research Laboratory (HIRL) |
|---|---|
| fyndplats | Germany |
| upptäcktsdatum | 1994 |
| etymologi | Named after the city of Darmstadt, Germany where GSI Helmholtz Centre for Heavy Ion Research is located. |
| uttal | oon-nun-NIL-i-em (engelska) |
| Förekomst | |
|---|---|
| Abundance in Earth's crust | |
| natural abundance (världshav) | |
| natural abundance (människokropp) | 0 %
|
| natural abundance (meteoroid) | 0 %
|
| natural abundance (Solen) | 0 %
|
| Abundance in Universe | 0 %
|