Element: Rutherfordium
This element has only been produced a few atoms at a time, so most of its properties have never been measured - missing values are omitted.
General data
| Element name | Rutherfordium |
|---|---|
| Chemical symbol | Rf |
| Atomic number Z | 104 |
| Year discovered | 1964 |
| Standard state (25°C) | Solid |
| Category | Transition metal |
| Block | d |
| Atomic mass | [267] |
| CPK color | #CC0059 |
Physical properties
none - only single atoms have been produced
Energy properties
none - only single atoms have been produced
Atomic structure
| Protons | 104 (Atomic number) |
|---|---|
| Neutrons (Rf-267, longest-lived isotope) | 163 |
| Electrons | 104 |
| Electron configuration | [Rn] 7s² 5f¹⁴ 6d² |
| Oxidation states | +4 |
Ionization energies - NIST ASD (69 states)
| State | Charge | Ioniz. energy (eV) | Type |
|---|---|---|---|
| Rf I | 0+ | 6.02 ± 0.04 | calculated |
| Rf II | 1+ | 14.35 ± 0.04 | calculated |
| Rf III | 2+ | 23.84 ± 0.04 | calculated |
| Rf IV | 3+ | 31.87 ± 0.04 | calculated |
| Rf V | 4+ | 64 ± 1.9 | calculated |
| Rf VI | 5+ | 77 ± 2 | calculated |
| Rf VII | 6+ | 102 ± 2 | calculated |
| Rf VIII | 7+ | 119 ± 2.1 | calculated |
| Rf IX | 8+ | 146.1 ± 2.2 | calculated |
| Rf X | 9+ | 169 ± 2.2 | calculated |
| Rf XI | 10+ | 193 ± 2.4 | calculated |
| Rf XII | 11+ | 225 ± 2.5 | calculated |
| Rf XIII | 12+ | 244 ± 3 | calculated |
| Rf XIV | 13+ | 275 ± 3 | calculated |
| Rf XXVII | 26+ | 791 ± 4 | calculated |
| Rf XXVIII | 27+ | 825 ± 4 | calculated |
| Rf XXIX | 28+ | 860 ± 4 | calculated |
| Rf XXX | 29+ | 899 ± 4 | calculated |
| Rf XXXI | 30+ | 936 ± 4 | calculated |
| Rf XXXII | 31+ | 972 ± 4 | calculated |
| Rf XXXIII | 32+ | 1036 ± 4 | calculated |
| Rf XXXIV | 33+ | 1073 ± 5 | calculated |
| Rf XXXV | 34+ | 1114 ± 5 | calculated |
| Rf XXXVI | 35+ | 1151 ± 5 | calculated |
| Rf LIX | 58+ | 3857 ± 6 | calculated |
| Rf LX | 59+ | 3938 ± 7 | calculated |
| Rf LXI | 60+ | 4025 ± 10 | calculated |
| Rf LXII | 61+ | 4116 ± 12 | calculated |
| Rf LXIII | 62+ | 4203 ± 15 | calculated |
| Rf LXIV | 63+ | 4287 ± 19 | calculated |
| Rf LXV | 64+ | 4489 ± 24 | calculated |
| Rf LXVI | 65+ | 4580 ± 30 | calculated |
| Rf LXVII | 66+ | 4670 ± 40 | calculated |
| Rf LXVIII | 67+ | 4760 ± 40 | calculated |
| Rf LXIX | 68+ | 5130 ± 50 | calculated |
| Rf LXX | 69+ | 5210 ± 50 | calculated |
| Rf LXXI | 70+ | 5300 ± 60 | calculated |
| Rf LXXII | 71+ | 5390 ± 60 | calculated |
| Rf LXXIII | 72+ | 6100 ± 70 | calculated |
| Rf LXXIV | 73+ | 6200 ± 90 | calculated |
| Rf LXXV | 74+ | 6470 ± 90 | calculated |
| Rf LXXVI | 75+ | 6570 ± 100 | calculated |
| Rf LXXVII | 76+ | 10170 ± 110 | calculated |
| Rf LXXVIII | 77+ | 10360 ± 120 | calculated |
| Rf LXXIX | 78+ | 10560 ± 120 | calculated |
| Rf LXXX | 79+ | 10780 ± 140 | calculated |
| Rf LXXXI | 80+ | 10980 ± 150 | calculated |
| Rf LXXXII | 81+ | 11180 ± 160 | calculated |
| Rf LXXXIII | 82+ | 11750 ± 170 | calculated |
| Rf LXXXIV | 83+ | 11960 ± 190 | calculated |
| Rf LXXXV | 84+ | 12200 ± 200 | calculated |
| Rf LXXXVI | 85+ | 12410 ± 220 | calculated |
| Rf LXXXVII | 86+ | 13010 ± 240 | calculated |
| Rf LXXXVIII | 87+ | 13190 ± 250 | calculated |
| Rf LXXXIX | 88+ | 13400 ± 300 | calculated |
| Rf XC | 89+ | 13600 ± 300 | calculated |
| Rf XCI | 90+ | 15800 ± 300 | calculated |
| Rf XCII | 91+ | 16000 ± 300 | calculated |
| Rf XCIII | 92+ | 16400 ± 400 | calculated |
| Rf XCIV | 93+ | 16700 ± 400 | calculated |
| Rf XCV | 94+ | 33100 ± 400 | calculated |
| Rf XCVI | 95+ | 33600 ± 400 | calculated |
| Rf XCVII | 96+ | 34100 ± 400 | calculated |
| Rf XCVIII | 97+ | 34600 ± 400 | calculated |
| Rf XCIX | 98+ | 42700 ± 500 | calculated |
| Rf C | 99+ | 43400 ± 500 | calculated |
| Rf CI | 100+ | 44300 ± 500 | calculated |
| Rf CIII | 102+ | 174265 ± 9 | calculated |
| Rf CIV | 103+ | 177142 ± 9 | calculated |
Value type as given by NIST ASD: measured - from evaluated experimental data; calculated - from ab initio calculations (mostly highly ionised atoms that have not been measured; for the simplest ones, e.g. H I, the calculation is more accurate than measurement); semi-empirical - from interpolation, extrapolation or another semi-empirical method.
NIST gives no energy for some ionization stages - hence the gaps in numbering.
Data sources
- PubChem Periodic Table API - Retrieved on 29 June 2026 - licence: CC0
- IUPAC CIAAW - Abridged Standard Atomic Weights 2024 - Table version: 2024 - licence: Public domain
- NNDC Wallet Cards 2023 - Data as of 15 October 2024 - licence: Public domain
- NIST Atomic Spectra Database (ASD) - Retrieved on 29 June 2026 - licence: © U.S. Secretary of Commerce
- Images of Elements - Retrieved on 29 June 2026 - licence: CC BY 3.0
