- 🇬🇧 Tin
- 🇺🇦 Олово
- 🇨🇳 錫
- 🇳🇱 Tin
- 🇫🇷 étain
- 🇩🇪 Zinn
- 🇮🇱 בדיל
- 🇮🇹 Stagno
- 🇯🇵 スズ
- 🇵🇹 Estanho
- 🇪🇸 Estaño
- 🇸🇪 Tenn
- 🇷🇺 Олово
Tin atoms have 50 electrons and the shell structure is 2.8.18.18.4.
The ground state electron configuration of ground state gaseous neutral tin is [Kr].4d10.5s2.5p2 and the term symbol is 3P0.
Atomic spectrum
A representation of the atomic spectrum of tin.
Ionisation Energies and electron affinity
The electron affinity of tin is 107.3 kJ mol‑1. The ionisation energies of tin are given below.
| Ionisation energy number | Enthalpy / kJ mol‑1 |
|---|---|
| 1st | 708.58 |
| 2nd | 1411.88 |
| 3rd | 2943.4 |
| 4th | 3931 |
| 5th | 7432 |
| 6th | 9070 |
| 7th | 10890 |
| 8th | 13030 |
| 9th | 15050 |
| 10th | 17750 |
| 11th | 20070 |
| 12th | 22380 (calculated) |
| 13th | 24900 |
| 14th | 27200 |
| 15th | 36600 |
| 16th | 39300 |
| 17th | 42200 |
| 18th | 45000 |
| 19th | 48800 |
| 20th | 51800 |
| 21st | 58700 |
Effective Nuclear Charges
The following are "Clementi-Raimondi" effective nuclear charges, Zeff. Follow the hyperlinks for more details and for graphs in various formats.
| 1s | 48.99 | ||||||
|---|---|---|---|---|---|---|---|
| 2s | 36.86 | 2p | 45.89 | ||||
| 3s | 32.42 | 3p | 32.35 | 3d | 35.74 | ||
| 4s | 22.66 | 4p | 21.27 | 4d | 17.97 | 4f | (no data) |
| 5s | 10.63 | 5p | 9.10 | 5d | (no data) | ||
| 6s | (no data) | 6p | (no data) | ||||
| 7s |
References
These effective nuclear charges, Zeff, are adapted from the following references:
- E. Clementi and D.L.Raimondi, J. Chem. Phys. 1963, 38, 2686.
- E. Clementi, D.L.Raimondi, and W.P. Reinhardt, J. Chem. Phys. 1967, 47, 1300.
Electron binding energies
| Label | Orbital | eV [literature reference] |
|---|---|---|
| K | 1s | 29200 [1] |
| L I | 2s | 4465 [1] |
| L II | 2p1/2 | 4156 [1] |
| L III | 2p3/2 | 3929 [1] |
| M I | 3s | 884.7 [3] |
| M II | 3p1/2 | 756.5 [3] |
| M III | 3p3/2 | 714.6 [3] |
| M IV | 3d3/2 | 493.2 [3] |
| M V | 3d5/2 | 484.9 [3] |
| N I | 4s | 137.1 [3] |
| N II | 4p1/2 | 83.6 [3, one-particle approximation not valid owing to short core-hole lifetime] |
| N III | 4p3/2 | 83.6 [3, one-particle approximation not valid owing to short core-hole lifetime] |
| N IV | 4d3/2 | 24.9 [3] |
| N V | 4d5/2 | 23.9 [3] |
Notes
I am grateful to Gwyn Williams (Jefferson Laboratory, Virginia, USA) who provided the electron binding energy data. The data are adapted from references 1-3. They are tabulated elsewhere on the WWW (reference 4) and in paper form (reference 5).
References
- J. A. Bearden and A. F. Burr, "Reevaluation of X-Ray Atomic Energy Levels," Rev. Mod. Phys., 1967, 39, 125.
- M. Cardona and L. Ley, Eds., Photoemission in Solids I: General Principles (Springer-Verlag, Berlin) with additional corrections, 1978.
- Gwyn Williams WWW table of values
- D.R. Lide, (Ed.) in Chemical Rubber Company handbook of chemistry and physics , CRC Press, Boca Raton, Florida, USA, 81st edition, 2000.
- J. C. Fuggle and N. Mårtensson, "Core-Level Binding Energies in Metals," J. Electron Spectrosc. Relat. Phenom., 1980, 21, 275.