Atomnummer | 50 |
---|---|
Atommassa | 118.71 |
masstal | 120 |
Grupp | 14 |
---|---|
Period | 5 |
Block | p |
Protoner | 50 p+ |
---|---|
Neutroner | 70 n0 |
Electrons | 50 e- |
fysisk egenskap | |
---|---|
atomradie | 145 pm
|
molvolym | 16,3 cm³/mol
|
kovalent radie | 140 pm
|
Metallic Radius | 142 pm
|
ionic radius | 55 pm
|
Crystal Radius | 69 pm
|
Van der Waalsradie | 217 pm
|
densitet | 7,287 g/cm³
|
energi | |
proton affinity | |
Elektronaffinitet | 1,112067 eV/particle
|
joniseringsenergi | 7,343917 eV/particle
|
ångbildningsvärme | 296 kJ/mol
|
smältvärme | 7,07 kJ/mol
|
Bildningsentalpi | 301,2 kJ/mol
|
Electrons | |
electron shell | 2, 8, 18, 18, 4 |
valenselektron | 4 |
elektronkonfiguration | [Kr] 4d10 5s2 5p2 |
oxidationstal | -4, -3, -2, -1, 0, 1, 2, 3, 4 |
elektronegativitet | 1.96
|
Electrophilicity | 1,434238336293717 eV/particle
|
Phases | |
aggregationstillstånd | Fast |
Gas Phase | |
Kokpunkt | 2 859,15 K
|
Smältpunkt | 286,35 K
|
critical pressure | |
critical temperature | |
trippelpunkt | |
Visual | |
färg | Silver
|
appearance | silvery-white (beta, β) or gray (alpha, α) |
Brytningsindex | |
materialegenskap | |
Värmeledningsförmåga | 66,8 W/(m K)
|
termisk expansion | 0,000022 1/K
|
molar heat capacity | 26,99 J/(mol K)
|
Specifik värmekapacitet | 0,227 J/(g⋅K)
|
heat capacity ratio | |
electrical properties | |
type | Conductor |
elektrisk konduktivitet | 9,1 MS/m
|
resistivitet | 0,00000011 m Ω
|
supraledare | 3,72 K
|
magnetism | |
type | diamagnetic |
magnetisk susceptibilitet (Mass) | −0,0000000031 m³/Kg
|
magnetisk susceptibilitet (Molar) | −0,000000000368 m³/mol
|
magnetisk susceptibilitet (Volume) | −0,0000227
|
magnetic ordering | |
Curiepunkten | |
Néel temperature | |
Structure | |
Kristallstruktur | Rymdcentrerat tetragonalt (TET) |
Gitterkonstant | 5,82 Å
|
Lattice Angles | π/2, π/2, π/2 |
mekanisk materialegenskap | |
hårdhet | 1,5 MPa
|
Kompressibilitet | 58 GPa
|
skjuvmodul | 18 GPa
|
Young's modulus | 50 GPa
|
Poissons konstant | 0,36
|
ljudhastighet | 2 500 m/s
|
klassificering | |
Kategori | Posttransitionsmetaller, Poor metals |
CAS Group | IVB |
IUPAC Group | IVA |
Glawe Number | 83 |
Mendeleev Number | 90 |
Pettifor Number | 83 |
Geochemical Class | |
Goldschmidt classification | chalcophile |
övrigt | |
Gas Basicity | |
Dipole Polarizability | |
C6 Dispersion Coefficient | 659 a₀
|
Allotropes | White Tin, Gray Tin |
Träffyta | 0,62
|
Neutron Mass Absorption | 0,0002
|
kvanttal | 3P0 |
rymdgrupp | 141 (I41/amd) |
Stabila isotoper | 10 |
---|---|
Instabila isotoper | 32 |
Radioactive Isotopes | 32 |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 99 |
g-factor | |
Halveringstid | 24 ± 4 ms
|
Spinn | 9/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 2011 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
β+ p (β+-delayed proton emission) | 5% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 100 |
g-factor | 0
|
Halveringstid | 1,18 ± 0,08 s
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1994 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
β+ p (β+-delayed proton emission) | 17% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 101 |
g-factor | |
Halveringstid | 2,22 ± 0,05 s
|
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1994 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
β+ p (β+-delayed proton emission) | 21% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 102 |
g-factor | 0
|
Halveringstid | 3,8 ± 0,2 s
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1994 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 103 |
g-factor | |
Halveringstid | 7 ± 0,2 s
|
Spinn | 5/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1981 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
β+ p (β+-delayed proton emission) | 1.2% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 104 |
g-factor | 0
|
Halveringstid | 20,8 ± 0,5 s
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1985 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 105 |
g-factor | |
Halveringstid | 32,7 ± 0,5 s
|
Spinn | 5/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1981 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
β+ p (β+-delayed proton emission) | 0.011% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 106 |
g-factor | 0
|
Halveringstid | 1,92 ± 0,08 m
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1975 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 107 |
g-factor | |
Halveringstid | 2,9 ± 0,05 m
|
Spinn | 5/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1976 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 108 |
g-factor | 0
|
Halveringstid | 10,3 ± 0,08 m
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1968 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 109 |
g-factor | −0,4312 ± 0,0024
|
Halveringstid | 18,1 ± 0,2 m
|
Spinn | 5/2 |
nuclear quadrupole moment | 0,33 ± 0,11
|
upptäcktsdatum | 1966 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 110 |
g-factor | 0
|
Halveringstid | 4,154 ± 0,004 h
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1965 |
Paritet | + |
decay mode | Intensitet |
---|---|
ϵ (electron capture) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 111 |
g-factor | 0,17342857142857 ± 0,0011428571428571
|
Halveringstid | 35,3 ± 0,6 m
|
Spinn | 7/2 |
nuclear quadrupole moment | 0,2 ± 0,1
|
upptäcktsdatum | 1949 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | 0,97 ± 0,01
|
---|---|
relative atomic mass | |
masstal | 112 |
g-factor | 0
|
Halveringstid | |
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1927 |
Paritet | + |
decay mode | Intensitet |
---|---|
2β+ (double β+ decay) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 113 |
g-factor | −1,7554 ± 0,0016
|
Halveringstid | 115,08 ± 0,04 d
|
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1939 |
Paritet | + |
decay mode | Intensitet |
---|---|
β+ (β+ decay; β+ = ϵ + e+) | 100% |
natural abundance | 0,66 ± 0,01
|
---|---|
relative atomic mass | |
masstal | 114 |
g-factor | 0
|
Halveringstid | |
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1927 |
Paritet | + |
natural abundance | 0,34 ± 0,01
|
---|---|
relative atomic mass | |
masstal | 115 |
g-factor | |
Halveringstid | |
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1927 |
Paritet | + |
natural abundance | 14,54 ± 0,09
|
---|---|
relative atomic mass | |
masstal | 116 |
g-factor | 0
|
Halveringstid | |
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1922 |
Paritet | + |
natural abundance | 7,68 ± 0,07
|
---|---|
relative atomic mass | |
masstal | 117 |
g-factor | |
Halveringstid | |
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1923 |
Paritet | + |
natural abundance | 24,22 ± 0,09
|
---|---|
relative atomic mass | |
masstal | 118 |
g-factor | 0
|
Halveringstid | |
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1924 |
Paritet | + |
natural abundance | 8,59 ± 0,04
|
---|---|
relative atomic mass | |
masstal | 119 |
g-factor | |
Halveringstid | |
Spinn | 1/2 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1925 |
Paritet | + |
natural abundance | 32,58 ± 0,09
|
---|---|
relative atomic mass | |
masstal | 120 |
g-factor | 0
|
Halveringstid | |
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1926 |
Paritet | + |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 121 |
g-factor | 0,4646 ± 0,00073333333333333
|
Halveringstid | 27,03 ± 0,04 h
|
Spinn | 3/2 |
nuclear quadrupole moment | −0,02 ± 0,02
|
upptäcktsdatum | 1948 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | 4,63 ± 0,03
|
---|---|
relative atomic mass | |
masstal | 122 |
g-factor | 0
|
Halveringstid | |
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1928 |
Paritet | + |
decay mode | Intensitet |
---|---|
2β− (double β− decay) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 123 |
g-factor | −0,24876363636364 ± 0,0002
|
Halveringstid | 129,2 ± 0,4 d
|
Spinn | 11/2 |
nuclear quadrupole moment | 0,03 ± 0,04
|
upptäcktsdatum | 1948 |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | 5,79 ± 0,05
|
---|---|
relative atomic mass | |
masstal | 124 |
g-factor | 0
|
Halveringstid | |
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1922 |
Paritet | + |
decay mode | Intensitet |
---|---|
2β− (double β− decay) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 125 |
g-factor | −0,24472727272727 ± 0,00036363636363636
|
Halveringstid | 9,634 ± 0,015 d
|
Spinn | 11/2 |
nuclear quadrupole moment | 0,2 ± 0,2
|
upptäcktsdatum | 1939 |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 126 |
g-factor | 0
|
Halveringstid | 230 ± 14 ky
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1962 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 127 |
g-factor | −0,24127272727273 ± 0,0012727272727273
|
Halveringstid | 2,1 ± 0,04 h
|
Spinn | 11/2 |
nuclear quadrupole moment | 0,32 ± 0,14
|
upptäcktsdatum | 1951 |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 128 |
g-factor | 0
|
Halveringstid | 59,07 ± 0,14 m
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1956 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 129 |
g-factor | 0,502 ± 0,002
|
Halveringstid | 2,23 ± 0,04 m
|
Spinn | 3/2 |
nuclear quadrupole moment | 0,05 ± 0,12
|
upptäcktsdatum | 1962 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 130 |
g-factor | 0
|
Halveringstid | 3,72 ± 0,07 m
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1972 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 131 |
g-factor | 0,49733333333333 ± 0,0026666666666667
|
Halveringstid | 56 ± 0,5 s
|
Spinn | 3/2 |
nuclear quadrupole moment | −0,04 ± 0,09
|
upptäcktsdatum | 1963 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 132 |
g-factor | 0
|
Halveringstid | 39,7 ± 0,8 s
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1963 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 133 |
g-factor | |
Halveringstid | 1,37 ± 0,07 s
|
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1973 |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | 0.0294% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 134 |
g-factor | 0
|
Halveringstid | 0,93 ± 0,08 s
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1974 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | 17% |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 135 |
g-factor | |
Halveringstid | 515 ± 5 ms
|
Spinn | 7/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1994 |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | 21% |
2n (2-neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 136 |
g-factor | 0
|
Halveringstid | 355 ± 18 ms
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 1994 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | 28% |
2n (2-neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 137 |
g-factor | |
Halveringstid | 249 ± 15 ms
|
Spinn | 5/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 1994 |
Paritet | - |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | 48% |
2n (2-neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 138 |
g-factor | 0
|
Halveringstid | 148 ± 9 ms
|
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 2010 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | 100% |
β− n (β−-delayed neutron emission) | 36% |
2n (2-neutron emission) | % |
natural abundance | Radioactive ☢️ |
---|---|
relative atomic mass | |
masstal | 139 |
g-factor | |
Halveringstid | 120 ± 38 ms
|
Spinn | 5/2 |
nuclear quadrupole moment | |
upptäcktsdatum | 2015 |
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 | 140 |
g-factor | 0
|
Halveringstid | |
Spinn | 0 |
nuclear quadrupole moment | 0
|
upptäcktsdatum | 2018 |
Paritet | + |
decay mode | Intensitet |
---|---|
β− (β− decay) | % |
β− n (β−-delayed neutron emission) | % |
2n (2-neutron emission) | % |
upptäckare eller uppfinnare | Known to the ancients. |
---|---|
fyndplats | |
upptäcktsdatum | |
etymologi | Named after Etruscan god, Tinia; symbol from Latin: stannum (tin). |
uttal | TIN (engelska) |
1 | s | 1.008 |
2 | p | 4.1146 |
2 | s | 13.1406 |
3 | d | 14.2583 |
3 | p | 17.6468 |
3 | s | 17.5802 |
4 | d | 32.03 |
4 | p | 28.7348 |
4 | s | 27.342 |
5 | p | 40.898 |
5 | s | 39.3715 |