Element: Lawrencium
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 | Lawrencium |
|---|---|
| Chemical symbol | Lr |
| Atomic number Z | 103 |
| Year discovered | 1961 |
| Standard state (25°C) | Solid |
| Category | Actinide |
| Block | f |
| Atomic mass | [266] |
| CPK color | #C70066 |
Physical properties
| Melting point | 1900 K (1627 °C) |
|---|
Energy properties
none - only single atoms have been produced
Atomic structure
| Protons | 103 (Atomic number) |
|---|---|
| Neutrons (Lr-266, longest-lived isotope) | 163 |
| Electrons | 103 |
| Electron configuration | [Rn] 7s² 5f¹⁴ 7p¹ Lawrencium is an exception. The orbital filling rules would give [Rn]7s2 5f14 6d1 (as listed e.g. by PubChem). In such a heavy atom, however, electrons close to the nucleus move at speeds comparable to the speed of light - relativistic effects lower the energy of the 7p orbital below 6d. Relativistic quantum calculations point to [Rn]7s2 5f14 7p1, and the first ionization energy of lawrencium measured in 2015 (Sato et al., Nature 520, 209) agrees with it. |
| Oxidation states | +3 |
| Electronegativity (Pauling) | 1.3 |
Ionization energies - NIST ASD (103 states)
| State | Charge | Ioniz. energy (eV) | Type |
|---|---|---|---|
| Lr I | 0+ | 4.96 ± 0.05 | measured |
| Lr II | 1+ | 14.54 ± 0.04 | calculated |
| Lr III | 2+ | 21.8 ± 0.04 | calculated |
| Lr IV | 3+ | 43.6 ± 0.4 | semi-empirical |
| Lr V | 4+ | 56 ± 1.9 | calculated |
| Lr VI | 5+ | 80 ± 2 | calculated |
| Lr VII | 6+ | 96 ± 2 | calculated |
| Lr VIII | 7+ | 121 ± 2.1 | calculated |
| Lr IX | 8+ | 143 ± 2.2 | calculated |
| Lr X | 9+ | 165 ± 2.2 | calculated |
| Lr XI | 10+ | 197 ± 2.4 | calculated |
| Lr XII | 11+ | 216 ± 2.5 | calculated |
| Lr XIII | 12+ | 244 ± 3 | calculated |
| Lr XIV | 13+ | 269 ± 14 | calculated |
| Lr XV | 14+ | 290 ± 15 | calculated |
| Lr XVI | 15+ | 322 ± 12 | calculated |
| Lr XVII | 16+ | 344 ± 17 | calculated |
| Lr XVIII | 17+ | 374 ± 19 | calculated |
| Lr XIX | 18+ | 403 ± 20 | calculated |
| Lr XX | 19+ | 431 ± 21 | calculated |
| Lr XXI | 20+ | 459 ± 24 | calculated |
| Lr XXII | 21+ | 487 ± 25 | calculated |
| Lr XXIII | 22+ | 510 ± 30 | calculated |
| Lr XXIV | 23+ | 540 ± 30 | calculated |
| Lr XXV | 24+ | 560 ± 30 | calculated |
| Lr XXVI | 25+ | 745 ± 4 | calculated |
| Lr XXVII | 26+ | 779 ± 4 | calculated |
| Lr XXVIII | 27+ | 814 ± 4 | calculated |
| Lr XXIX | 28+ | 852 ± 4 | calculated |
| Lr XXX | 29+ | 888 ± 4 | calculated |
| Lr XXXI | 30+ | 922 ± 4 | calculated |
| Lr XXXII | 31+ | 985 ± 4 | calculated |
| Lr XXXIII | 32+ | 1020 ± 4 | calculated |
| Lr XXXIV | 33+ | 1061 ± 5 | calculated |
| Lr XXXV | 34+ | 1098 ± 5 | calculated |
| Lr XXXVI | 35+ | 1280 ± 60 | calculated |
| Lr XXXVII | 36+ | 1320 ± 70 | calculated |
| Lr XXXVIII | 37+ | 1360 ± 70 | calculated |
| Lr XXXIX | 38+ | 1410 ± 70 | calculated |
| Lr XL | 39+ | 1570 ± 80 | calculated |
| Lr XLI | 40+ | 1620 ± 80 | calculated |
| Lr XLII | 41+ | 1760 ± 90 | calculated |
| Lr XLIII | 42+ | 1810 ± 90 | calculated |
| Lr XLIV | 43+ | 2010 ± 100 | calculated |
| Lr XLV | 44+ | 2100 ± 110 | calculated |
| Lr XLVI | 45+ | 2190 ± 110 | calculated |
| Lr XLVII | 46+ | 2290 ± 110 | calculated |
| Lr XLVIII | 47+ | 2380 ± 120 | calculated |
| Lr XLIX | 48+ | 2470 ± 120 | calculated |
| Lr L | 49+ | 2570 ± 120 | calculated |
| Lr LI | 50+ | 2670 ± 140 | calculated |
| Lr LII | 51+ | 2780 ± 140 | calculated |
| Lr LIII | 52+ | 2860 ± 150 | calculated |
| Lr LIV | 53+ | 2960 ± 150 | calculated |
| Lr LV | 54+ | 3060 ± 150 | calculated |
| Lr LVI | 55+ | 3150 ± 160 | calculated |
| Lr LVII | 56+ | 3250 ± 160 | calculated |
| Lr LVIII | 57+ | 3741 ± 6 | calculated |
| Lr LIX | 58+ | 3821 ± 6 | calculated |
| Lr LX | 59+ | 3906 ± 7 | calculated |
| Lr LXI | 60+ | 3996 ± 10 | calculated |
| Lr LXII | 61+ | 4082 ± 12 | calculated |
| Lr LXIII | 62+ | 4165 ± 15 | calculated |
| Lr LXIV | 63+ | 4360 ± 19 | calculated |
| Lr LXV | 64+ | 4448 ± 24 | calculated |
| Lr LXVI | 65+ | 4540 ± 30 | calculated |
| Lr LXVII | 66+ | 4630 ± 40 | calculated |
| Lr LXVIII | 67+ | 4990 ± 40 | calculated |
| Lr LXIX | 68+ | 5070 ± 50 | calculated |
| Lr LXX | 69+ | 5160 ± 50 | calculated |
| Lr LXXI | 70+ | 5250 ± 60 | calculated |
| Lr LXXII | 71+ | 5920 ± 60 | calculated |
| Lr LXXIII | 72+ | 6030 ± 70 | calculated |
| Lr LXXIV | 73+ | 6290 ± 90 | calculated |
| Lr LXXV | 74+ | 6390 ± 90 | calculated |
| Lr LXXVI | 75+ | 9920 ± 100 | calculated |
| Lr LXXVII | 76+ | 10110 ± 110 | calculated |
| Lr LXXVIII | 77+ | 10310 ± 120 | calculated |
| Lr LXXIX | 78+ | 10520 ± 120 | calculated |
| Lr LXXX | 79+ | 10720 ± 140 | calculated |
| Lr LXXXI | 80+ | 10920 ± 150 | calculated |
| Lr LXXXII | 81+ | 11470 ± 160 | calculated |
| Lr LXXXIII | 82+ | 11680 ± 170 | calculated |
| Lr LXXXIV | 83+ | 11910 ± 190 | calculated |
| Lr LXXXV | 84+ | 12120 ± 200 | calculated |
| Lr LXXXVI | 85+ | 12710 ± 220 | calculated |
| Lr LXXXVII | 86+ | 12890 ± 240 | calculated |
| Lr LXXXVIII | 87+ | 13090 ± 250 | calculated |
| Lr LXXXIX | 88+ | 13300 ± 300 | calculated |
| Lr XC | 89+ | 15300 ± 300 | calculated |
| Lr XCI | 90+ | 15600 ± 300 | calculated |
| Lr XCII | 91+ | 16000 ± 300 | calculated |
| Lr XCIII | 92+ | 16200 ± 400 | calculated |
| Lr XCIV | 93+ | 32400 ± 400 | calculated |
| Lr XCV | 94+ | 32900 ± 400 | calculated |
| Lr XCVI | 95+ | 33400 ± 400 | calculated |
| Lr XCVII | 96+ | 33900 ± 400 | calculated |
| Lr XCVIII | 97+ | 41600 ± 400 | calculated |
| Lr XCIX | 98+ | 42300 ± 500 | calculated |
| Lr C | 99+ | 43200 ± 500 | calculated |
| Lr CI | 100+ | 43759 ± 6 | calculated |
| Lr CII | 101+ | 170116 ± 8 | calculated |
| Lr CIII | 102+ | 172928 ± 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.
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
