โ–ธโ–ธ
  • ๐Ÿ‡ฌ๐Ÿ‡ง Tin
  • ๐Ÿ‡บ๐Ÿ‡ฆ ะžะปะพะฒะพ
  • ๐Ÿ‡จ๐Ÿ‡ณ ้Œซ
  • ๐Ÿ‡ณ๐Ÿ‡ฑ Tin
  • ๐Ÿ‡ซ๐Ÿ‡ท étain
  • ๐Ÿ‡ฉ๐Ÿ‡ช Zinn
  • ๐Ÿ‡ฎ๐Ÿ‡ฑ ื‘ื“ื™ืœ
  • ๐Ÿ‡ฎ๐Ÿ‡น Stagno
  • ๐Ÿ‡ฏ๐Ÿ‡ต ใ‚นใ‚บ
  • ๐Ÿ‡ต๐Ÿ‡น Estanho
  • ๐Ÿ‡ช๐Ÿ‡ธ Estaño
  • ๐Ÿ‡ธ๐Ÿ‡ช Tenn
  • ๐Ÿ‡ท๐Ÿ‡บ ะžะปะพะฒะพ

Tin - 50Sn: isotope data

Tin has the most stable isotopes (10) of all elements. Tin isotopes are used in a variety of applications. Sn-112 is used as precursor in the production of the radioisotope Sn-113 while Sn124 is used for producing Sb-124. Sn-116 and Sn-117 can both be used for the production of the medical radioisotope Sn-117m which is used in treating bone cancer. Both Sn-118 and Sn-119 have been evaluated for the production of Sn-119m.

Naturally occurring isotopes

This table shows information about naturally occuring isotopes, their atomic masses, their natural abundances, their nuclear spins, and their magnetic moments. Further data for radioisotopes (radioactive isotopes) of tin are listed (including any which occur naturally) below.
Isotope Mass / Da Natural abundance (atom %) Nuclear spin (I) Magnetic moment (μ/μN)
112Sn 111.904826 (5) 0.97 (1) 0
114Sn 113.902784 (4) 0.66 (1) 0
115Sn 114.903348 (3) 0.34 (1) 1/2 -0.91884
116Sn 115.901747 (3) 14.54 (9) 0
117Sn 116.902956 (3) 7.68 (7) 1/2 -1.00105
118Sn 117.901609 (3) 24.22 (9) 0
119Sn 118.903311 (3) 8.59 (4) 1/2 -1.04729
120Sn 119.9021991 (29) 32.58 (9) 0
122Sn 121.9034404 (30) 4.63 (3) 0
124Sn 123.9052743 (17) 5.79 (5) 0
Isotope abundances of tin
Isotope abundances of tin. In the above, the most intense ion is set to 100% since this corresponds best to the output from a mass spectrometer. This is not to be confused with the relative percentage isotope abundances which totals 100% for all the naturally occurring isotopes.

Radiosotope data

Further data for naturally occuring isotopes of tin are listed above. This table gives information about some radiosotopes of tin, their masses, their half-lives, their modes of decay, their nuclear spins, and their nuclear magnetic moments.
Isotope Mass / Da Half-life Mode of decay Nuclear spin Nuclear magnetic moment
110Sn 109.90785 4.1 h EC to 110In 0
111Sn 110.90774 35 m EC to 111In 7/2 0.61
113Sn 112.905174 115.1 d EC to 113In 1/2 -0.879
121Sn 120.904239 1.128 d β- to 121Sb 3/2 0.698
123Sn 122.905723 129.2 d β- to 123Sb 11/2 -1.370
125Sn 124.907785 9.63 d β- to 125Sb 11/2 -1.35
126Sn 125.90765 100000 y β- to 126Sb 0
127Sn 126.91035 2.12 h β- to 127Sb 11/2

References

  1. Naturally occurring isotope abundances: Commission on Atomic Weights and Isotopic Abundances report for the International Union of Pure and Applied Chemistry in Isotopic Compositions of the Elements 1989, Pure and Applied Chemistry, 1998, 70, 217. [Copyright 1998 IUPAC]
  2. For further information about radioisotopes see Jonghwa Chang's (Korea Atomic Energy Research Institute) Table of the Nuclides
  3. Masses, nuclear spins, and magnetic moments: I. Mills, T. Cvitas, K. Homann, N. Kallay, and K. Kuchitsu in Quantities, Units and Symbols in Physical Chemistry, Blackwell Scientific Publications, Oxford, UK, 1988. [Copyright 1988 IUPAC]

NMR Properties of tin

Common reference compound: Sn(CH3)4.

Table of NMR-active nucleus propeties of tin
  Isotope 1 Isotope 2 Isotope 3
Isotope 115Sn 117Sn 119Sn
Natural abundance /% 0.34 7.68 8.59
Spin (I) 1/2 1/2 1/2
Frequency relative to 1H = 100 (MHz) 32.718746 35.632256 37.290629
Receptivity, DP, relative to 1H = 1.00 0.000121 0.00354 0.00453
Receptivity, DC, relative to 13C = 1.00 0.694 20.2 25.9
Magnetogyric ratio, γ (107 rad T‑1 s-1) -8.8013 -9.58879 -10.0317
Magnetic moment, μ (μN) -1.5915 -1.73385 -1.81394
Nuclear quadrupole moment, Q/millibarn - - -132(1) [Mössbauer state]
Line width factor, 1056 l (m4) - - -

References

  1. R.K. Harris in Encyclopedia of Nuclear Magnetic Resonance, D.M. Granty and R.K. Harris, (eds.), vol. 5, John Wiley & Sons, Chichester, UK, 1996. I am grateful to Professor Robin Harris (University of Durham, UK) who provided much of the NMR data, which are copyright 1996 IUPAC, adapted from his contribution contained within this reference.
  2. J. Mason in Multinuclear NMR, Plenum Press, New York, USA, 1987. Where given, data for certain radioactive nuclei are from this reference.
  3. P. Pyykkö, Mol. Phys., 2008, 106, 1965-1974.
  4. P. Pyykkö, Mol. Phys., 2001, 99, 1617-1629.
  5. P. Pyykkö, Z. Naturforsch., 1992, 47a, 189. I am grateful to Professor Pekka Pyykkö (University of Helsinki, Finland) who provided the nuclear quadrupole moment data in this and the following two references.
  6. D.R. Lide, (ed.), CRC Handbook of Chemistry and Physics 1999-2000 : A Ready-Reference Book of Chemical and Physical Data (CRC Handbook of Chemistry and Physics, CRC Press, Boca Raton, Florida, USA, 79th edition, 1998.
  7. P. Pyykkö, personal communication, 1998, 204, 2008, 2010.