Lawrencium (Lr)
actinideSolid
Standard Atomic Weight
[262]Electron configuration
[Rn] 7s2 5f14 6d1Melting point
1626.85 °C (1900 K)Boiling point
N/ADensity
1.560000e+4 kg/m³Oxidation states
+3Electronegativity (Pauling)
N/AIonization energy (1st)
Discovery year
1961Atomic radius
N/ADetails
Lawrencium is a synthetic, highly radioactive actinide and the last element of the actinide series. It has been made only in minute numbers of atoms in nuclear reactions, so its chemistry is known from rapid, atom-at-a-time experiments and theoretical calculations. Its most stable known isotopes are short-lived on ordinary laboratory timescales. In solution it behaves chiefly as a trivalent metal, Lr³⁺, broadly resembling late actinides and some trivalent lanthanides.
Lawrencium does not occur naturally in the Earth’s crust. Credit for the first synthesis of this element in 1971 is given jointly to Albert Ghiorso and his team at the University of California in Berkeley and Georgi Flerov and his team at the Joint Institute for Nuclear Research (JINR) in Dubna, Russia (Fig. IUPAC.103.1). The element is named for Ernest O. Lawrence (Fig. IUPAC.103.2), who developed the cyclotron. The chemical symbol for lawrencium was originally proposed as Lw. At the IUPAC General Assembly in 1963, lawrencium was officially accepted by IUPAC, but the symbol was changed to Lr because the Commission on Inorganic Nomenclature determined that the letter ‘w’ presented a problem in languages other than English [636], [640], [641], [642]. There are no known isotopic applications for lawrencium outside of scientific research.
Lawrencium behaves differently from dipositive nobelium and more like the tripositive elements earlier in the actinide series.
Lawrencium was created by four American scientists, Albert Ghiorso, Torbjørn Sikkeland, Almon E. Larsh and Robert M. Latimer, in March, 1961. Working at the Lawrence Radiation Laboratory in Berkeley, California, the scientists placed three micrograms (0.000003 grams) of californium in the target chamber of a device called a linear accelerator. The scientists used the accelerator to bombard the californium with boron ions. Several different isotopes of lawrencium were created and there is some confusion as to which isotope the group actually detected. Today, the Lawrence Radiation Laboratory is known as the Lawrence Berkeley Laboratory. Lawrencium's most stable isotope, lawrencium-262, has a half-life of about 4 hours. It decays into nobelium-262 through electron capture, mendelevium-258 through alpha decay or through spontaneous fission.
Named after Lawrence, inventor of the cyclotron. This member of the 5f transition elements (actinide series) was discovered in March 1961 by A. Ghiorso, T. Sikkeland, A.E. Larsh, and R.M. Latimer. A 3-Mg californium target, consisting of a mixture of isotopes of mass number 249, 250, 251, and 252, was bombarded with either 10B or 11B. The electrically charged transmutation nuclei recoiled with an atmosphere of helium and were collected on a thin copper conveyor tape which was then moved to place collected atoms in front of a series of solid-state detectors. The isotope of element 103 produced in this way decayed by emitting an 8.6 MeV alpha particle with a half-life of 8 s.
In 1967, Flerov and associates at the Dubna Laboratory reported their inability to detect an alpha emitter with a half-life of 8 s which was assigned by the Berkeley group to 257103. This assignment has been changed to 258Lr or 259Lr.
In 1965, the Dubna workers found a longer-lived lawrencium isotope, 256Lr, with a half-life of 35 s. In 1968, Thiorso and associates at Berkeley used a few atoms of this isotope to study the oxidation behavior of lawrencium. Using solvent extraction techniques and working very rapidly, they extracted lawrencium ions from a buffered aqueous solution into an organic solvent completing each extraction in about 30 s.
Images
Properties
Physical
Chemical
Thermodynamic
Nuclear
Abundance
N/A
Reactivity
N/A
Crystal Structure
N/A
Electronic Structure
Identifiers
Electron Configuration Measured
Lr: 5f¹⁴ 7s² 7p¹[Rn] 5f¹⁴ 7s² 7p¹1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f¹⁴ 7s² 7p¹Atomic model
Isotopes change neutron count, mass, and stability — not the electron configuration of a neutral atom.
Schematic atomic model, not to scale.
Atomic Fingerprint
Emission / Absorption Spectrum
Isotope Distribution
No stable isotopes.
| Mass number | Atomic mass (u) | Natural abundance | Half-life |
|---|---|---|---|
| 253 Radioactive | 253.09509 ± 0.00022 | N/A | 632 ms |
| 252 Radioactive | 252.09526 ± 0.00026 | N/A | 369 ms |
| 251 Radioactive | 251.09418 ± 0.00032 | N/A | 300 us |
| 261 Radioactive | 261.10688 ± 0.00022 | N/A | 39 minutes |
| 255 Radioactive | 255.096562 ± 0.000019 | N/A | 31.1 seconds |
Phase / State
Reason: 1601.8 °C below sublimation point (1626.85 °C)
Schematic, not to scale
Phase transition points
Transition energies
Energy required to sublime 1 mol at sublimation point
Density
At standard conditions
At standard conditions
Atomic Spectra
Showing 10 of 103 Atomic Spectra. Sorted by ion charge (ascending).
Levels Holdings ?
| Ion | Charge | Levels |
|---|---|---|
| Lr I | 0 | 2 |
| Lr II | +1 | 2 |
| Lr III | +2 | 2 |
| Lr IV | +3 | 2 |
| Lr V | +4 | 2 |
| Lr VI | +5 | 2 |
| Lr VII | +6 | 2 |
| Lr VIII | +7 | 2 |
| Lr IX | +8 | 2 |
| Lr X | +9 | 2 |
Crystal structure data not available
Ionic Radii
| Charge | Coordination | Spin | Radius |
|---|---|---|---|
| +3 | 9 | N/A | 107.4 pm |
Compounds
Isotopes (5)
| Mass number | Atomic mass (u) | Natural abundance | Half-life | Decay mode | |
|---|---|---|---|---|---|
| 253 Radioactive | 253.09509 ± 0.00022 | N/A | 632 ms | α =90±1%SF =1.0±0.6%β+ ? | |
| 252 Radioactive | 252.09526 ± 0.00026 | N/A | 369 ms | α ≈98%SF ≈2%β+ ? | |
| 251 Radioactive | 251.09418 ± 0.00032 | N/A | 300 us | β+ ?α ? | |
| 261 Radioactive | 261.10688 ± 0.00022 | N/A | 39 minutes | SF ≈100%α ? | |
| 255 Radioactive | 255.096562 ± 0.000019 | N/A | 31.1 seconds | α =99.7±0.1%β+ =0.3±0.1%SF ? |
Extended Properties
Covalent Radii (Extended)
Van der Waals Radii
Numbering Scales
Electronegativity Scales
Polarizability & Dispersion
Phase Transitions & Allotropes
| Melting point | 1900.15 K |
Oxidation State Categories
Advanced Reference Data
Crystal Radii Detail (1)
| Charge | CN | Spin | rcrystal (pm) | Origin |
|---|---|---|---|---|
| 3 | IX | — | 121.4 |
Isotope Decay Modes (38)
| Isotope | Mode | Intensity |
|---|---|---|
| 251 | B+ | — |
| 251 | A | — |
| 252 | A | 98% |
| 252 | SF | 2% |
| 252 | B+ | — |
| 253 | A | 90% |
| 253 | SF | 1% |
| 253 | B+ | — |
| 254 | A | 71.7% |
| 254 | B+ | 28.3% |
Additional Data
Estimated Crustal Abundance
The estimated element abundance in the earth's crust.
Not Applicable
References (1)
- [5] Lawrencium https://education.jlab.org/itselemental/ele103.html
Estimated Oceanic Abundance
The estimated element abundance in the earth's oceans.
Not Applicable
References (1)
- [5] Lawrencium https://education.jlab.org/itselemental/ele103.html
References
(8)
Data deposited in or computed by PubChem
The half-life and atomic mass data was provided by the Atomic Mass Data Center at the International Atomic Energy Agency.
Element data are cited from the Atomic weights of the elements (an IUPAC Technical Report). The IUPAC periodic table of elements can be found at https://iupac.org/what-we-do/periodic-table-of-elements/. Additional information can be found within IUPAC publication doi:10.1515/pac-2015-0703 Copyright © 2020 International Union of Pure and Applied Chemistry.
The information are cited from Pure Appl. Chem. 2018; 90(12): 1833-2092, https://doi.org/10.1515/pac-2015-0703.
Thomas Jefferson National Accelerator Facility (Jefferson Lab) is one of 17 national laboratories funded by the U.S. Department of Energy. The lab's primary mission is to conduct basic research of the atom's nucleus using the lab's unique particle accelerator, known as the Continuous Electron Beam Accelerator Facility (CEBAF). For more information visit https://www.jlab.org/
The periodic table at the LANL (Los Alamos National Laboratory) contains basic element information together with the history, source, properties, use, handling and more. The provenance data may be found from the link under the source name.
The periodic table contains NIST's critically-evaluated data on atomic properties of the elements. The provenance data that include data for atomic spectroscopy, X-ray and gamma ray, radiation dosimetry, nuclear physics, and condensed matter physics may be found from the link under the source name. Ref: https://www.nist.gov/pml/atomic-spectra-database
This section provides all form of data related to element Lawrencium.
