Lr 103

Lawrencium (Lr)

actinide
Period: 7 Group: 3 Block: s

Solid

Standard Atomic Weight

[262]

Electron configuration

[Rn] 7s2 5f14 6d1

Melting point

1626.85 °C (1900 K)

Boiling point

N/A

Density

1.560000e+4 kg/m³

Oxidation states

+3

Electronegativity (Pauling)

N/A

Ionization energy (1st)

Discovery year

1961

Atomic radius

N/A

Details

Name origin Named in honor of Ernest O. Lawrence, inventor of the cyclotron.
Discovery country United States
Discoverers A.Ghiorso, T.Sikkeland, A.E.Larsh, R.M.Latimer

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

Van der Waals radius 246 pm
Density
Phase at STP solid
Melting point 1626.85 °C

Chemical

Electron affinity
Ionization energy (1st)
Ionization energy (2nd)
Ionization energy (3rd)
Ionization energy (4th)
Ionization energy (5th)
Oxidation states +3
Valence electrons 3
Electron configuration
Electron configuration (semantic)

Thermodynamic

Heat of sublimation 4.249365 eV
Heat of atomization 4.249365 eV

Nuclear

Stable isotopes 0
Mass number (most stable) 262
Discovery year 1961

Abundance

N/A

Reactivity

N/A

Crystal Structure

N/A

Electronic Structure

Electrons per shell 2, 8, 18, 32, 32, 8, 3

Identifiers

CAS number 22537-19-5
Term symbol
InChI InChI=1S/Lr
InChI Key CNQCVBJFEGMYDW-UHFFFAOYSA-N

Electron Configuration Measured

Ion charge
Protons 103
Electrons 103
Charge Neutral
Configuration Lr: 5f¹⁴ 7s² 7p¹
Electron configuration
Measured
[Rn] 5f¹⁴ 7s² 7p¹
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f¹⁴ 7s² 7p¹
Orbital diagram
1s
2/2
2s
2/2
2p
6/6
3s
2/2
3p
6/6
4s
2/2
3d
10/10
4p
6/6
5s
2/2
4d
10/10
5p
6/6
6s
2/2
4f
14/14
5d
10/10
6p
6/6
7s
2/2
5f
14/14
7p
1/6 1↑
Total electrons: 103 Unpaired: 1 ?

Atomic model

Protons 103
Neutrons 150
Electrons 103
Mass number 253
Stability Radioactive

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

0 / 0 (0 with intensity)
Measured
Emission Visible: 380–750 nm

Isotope Distribution

No stable isotopes.

Mass numberAtomic mass (u)Natural abundanceHalf-life
253 Radioactive253.09509 ± 0.00022N/A632 ms
252 Radioactive252.09526 ± 0.00026N/A369 ms
251 Radioactive251.09418 ± 0.00032N/A300 us
261 Radioactive261.10688 ± 0.00022N/A39 minutes
255 Radioactive255.096562 ± 0.000019N/A31.1 seconds
Measured

Phase / State

1 atm / 101.325 kPa
Solid 25 °C (298.15 K)

Reason: 1601.8 °C below sublimation point (1626.85 °C)

Sublimation point 1626.85 °C
0 K Current temperature: 25 °C 6000 K
Phase timeline

Schematic, not to scale

Solid
Gas
Sublimation
25°C
Solid
Liquid
Gas
Current

Phase transition points

Sublimation point Literature
1626.85 °C
Current phase Calculated
Solid

Transition energies

Heat of sublimation Literature
4.249365 eV

Energy required to sublime 1 mol at sublimation point

Density

Reference density Literature
1.560000e+4 kg/m³

At standard conditions

Current density Calculated
1.560000e+4 kg/m³

At standard conditions

Atomic Spectra

Showing 10 of 103 Atomic Spectra. Sorted by ion charge (ascending).

Levels Holdings ?

IonChargeLevels
Lr I 02
Lr II +12
Lr III +22
Lr IV +32
Lr V +42
Lr VI +52
Lr VII +62
Lr VIII +72
Lr IX +82
Lr X +92
NIST Levels Holdings →
103 Lr 262

Lawrencium — Atomic Orbital Visualizer

[Rn]7s25f146d1
Energy levels 2 8 18 32 32 9 2
Oxidation states +3
HOMO 6d n=6 · l=2 · m=-2
Lawrencium — Atomic Orbital Visualizer Preview
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103 Lr 262

Lawrencium — Crystal Structure Visualizer

Crystal structure data not available

Ionic Radii

ChargeCoordinationSpinRadius
+39N/A107.4 pm

Compounds

Lr
266.120 u

Isotopes (5)

Mass numberAtomic mass (u)Natural abundanceHalf-lifeDecay mode
253 Radioactive253.09509 ± 0.00022N/A632 ms
α =90±1%SF =1.0±0.6%β+ ?
252 Radioactive252.09526 ± 0.00026N/A369 ms
α ≈98%SF ≈2%β+ ?
251 Radioactive251.09418 ± 0.00032N/A300 us
β+ ?α ?
261 Radioactive261.10688 ± 0.00022N/A39 minutes
SF ≈100%α ?
255 Radioactive255.096562 ± 0.000019N/A31.1 seconds
α =99.7±0.1%β+ =0.3±0.1%SF ?
253 Radioactive
Atomic mass (u) 253.09509 ± 0.00022
Natural abundance N/A
Half-life 632 ms
Decay mode
α =90±1%SF =1.0±0.6% +1
252 Radioactive
Atomic mass (u) 252.09526 ± 0.00026
Natural abundance N/A
Half-life 369 ms
Decay mode
α ≈98%SF ≈2% +1
251 Radioactive
Atomic mass (u) 251.09418 ± 0.00032
Natural abundance N/A
Half-life 300 us
Decay mode
β+ ?α ?
261 Radioactive
Atomic mass (u) 261.10688 ± 0.00022
Natural abundance N/A
Half-life 39 minutes
Decay mode
SF ≈100%α ?
255 Radioactive
Atomic mass (u) 255.096562 ± 0.000019
Natural abundance N/A
Half-life 31.1 seconds
Decay mode
α =99.7±0.1%β+ =0.3±0.1% +1

Extended Properties

Covalent Radii (Extended)

Covalent radius (Pyykkö)  
Covalent radius (Pyykkö, double)  

Van der Waals Radii

UFF  

Numbering Scales

Mendeleev
Pettifor
Glawe

Electronegativity Scales

Ghosh

Polarizability & Dispersion

Dipole polarizability  
Dipole polarizability (unc.)  

Phase Transitions & Allotropes

Melting point1900.15 K

Oxidation State Categories

+3 main

Advanced Reference Data

Crystal Radii Detail (1)
ChargeCNSpinrcrystal (pm)Origin
3IX121.4
Isotope Decay Modes (38)
IsotopeModeIntensity
251B+
251A
252A98%
252SF2%
252B+
253A90%
253SF1%
253B+
254A71.7%
254B+28.3%

Additional Data

References

(8)
2 Atomic Mass Data Center (AMDC), International Atomic Energy Agency (IAEA)
Lr

The half-life and atomic mass data was provided by the Atomic Mass Data Center at the International Atomic Energy Agency.

3 IUPAC Commission on Isotopic Abundances and Atomic Weights (CIAAW)
Lawrencium

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.

4 IUPAC Periodic Table of the Elements and Isotopes (IPTEI)

The information are cited from Pure Appl. Chem. 2018; 90(12): 1833-2092, https://doi.org/10.1515/pac-2015-0703.

License note: Copyright (c) 2020 International Union of Pure and Applied Chemistry. The International Union of Pure and Applied Chemistry (IUPAC) contribution within Pubchem is provided under a CC-BY-NC-ND 4.0 license, unless otherwise stated.
5 Jefferson Lab, U.S. Department of Energy
Lawrencium

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/

License note: Please see citation and linking information: https://education.jlab.org/faq/index.html
6 Los Alamos National Laboratory, U.S. Department of Energy
Lawrencium

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.

7 NIST Physical Measurement Laboratory
Lawrencium

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

8 PubChem Elements
Lawrencium

This section provides all form of data related to element Lawrencium.

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