Lawrencium (Lr)

Lawrencium is a synthetic, highly radioactive actinide metal. It was first produced in 1961 by a team led by Albert Ghiorso at the University of California, Berkeley, and is named after Ernest O. Lawrence.

Atomic Number
103
Atomic Mass
262
Category
Actinides
Phase (STP)
Solid
Block
F
Electronegativity (Pauling)
1.3

Bohr Atomic Model

Protons
103
Neutrons
103
Electrons
103
Identity
Atomic Number103
SymbolLr
NameLawrencium
GroupActinides
Period7
Position
Period7
Group Label
Grid X18
Grid Y1
Physical Properties
Atomic Mass (u)262
Density (g/cm³)
Melting Point (K)1900 K null °C
Boiling Pointnull K null °C
Phase at STPSolid
CategoryActinides
Liquid Density (g/cm³)
Molar Volume (cm³/mol)
Emission Spectrum (nm)
Discovery
English NameLawrencium
English Pronunciationlor-REN-see-um
Latin Name
Latin Pronunciation
Year1965
DiscovererGeorgy Flerov and colleagues and at Dubna, near Moscow, Russia, and independently by Albert Ghiorso and colleagues at Berkeley, California, USA
CountryUnited States
CAS Number22537-19-5
CID Number
RTECS Number
Atomic Properties
Electron Shell
Electron Configuration[Rn] 5f^1^47s^27p^1
Oxidation States+3 +1
Ion ChargeLr3+, Lr+
Ionization Potential (eV)4.9
Electronegativity (Pauling)1.3
Electron Affinity (kJ/mol)
Electrons103
Protons103
Neutrons
ValenceIII
BlockF
Atomic Radius (pm)
Covalent Radius (pm)161
van der Waals Radius (pm)246
Thermodynamic Properties
PhaseSOLID
Heat of Fusion (kJ/mol)
Specific Heat (J/g·K)
Thermal Expansion (1/K)
Heat of Vaporization (kJ/mol)
Mechanical Properties
Brinell Hardness
Mohs Hardness
Vickers Hardness
Bulk Modulus (GPa)
Young's Modulus (GPa)
Shear Modulus (GPa)
Poisson Ratio
Sound Speed (m/s)
Refractive Index
Thermal Conductivity (W/m·K)
Electromagnetic Properties
Electrical Conductivity (S/m)
Electrical Type
Magnetic Type
Volume Magnetic Susceptibility
Mass Magnetic Susceptibility
Molar Magnetic Susceptibility
Resistivity (Ω·m)
Superconducting Point (K)
Crystal Properties
Structure
System
Space Group
a (Å)
b (Å)
c (Å)
α (°)
β (°)
γ (°)
Debye Temperature (K)
Nuclear Properties
RadioactiveNo
Half-lifeLongest-lived isotope Lr-266 has a half-life of about 11 hours.
Lifetime
Neutron Cross-section (barn)
Safety Information
Health HazardRadioactive; handle only in specialized facilities
Reactivity Hazard
Specific HazardRadioactive
Prevalence
Universe0
Sun0
Oceans0
Human Body0
Earth Crust0
Meteorites


FAQs about Lawrencium

Lawrencium (Lr) is a man-made actinide with atomic number 103, located at the end of the actinide series (period 7, f-block), after nobelium (No) and before the transactinides. It is produced atom-by-atom in accelerators and studied at tracer levels.

Lr was discovered (1961) by bombarding heavy actinide targets with light ions and then rapidly separating products radiochemically. A stylized production route is:

\(^{249}\mathrm{Cf}(^{11}\mathrm{B},\,4n)\,^{256}\mathrm{Lr}\)

Other target–projectile combinations (e.g., curium or americium with oxygen/carbon beams) also yield short-lived Lr isotopes.

Commonly observed isotopes include Lr-256, Lr-257, Lr-258, and Lr-260 (half-lives from seconds to minutes). Most decay by alpha emission and sometimes spontaneous fission:

\(^{256}\mathrm{Lr} \;\to\; ^{252}\mathrm{Md} + \alpha\)

In solution, Lr(III) is the dominant state, forming hydrated cations akin to other trivalent actinides. Under strongly reducing conditions, Lr(II) can be accessed transiently for separations. The trivalent aqua ion can be represented generically as:

\(\mathrm{[Lr(H_2O)_n]^{3+}}\; (n\approx 8\text{–}9)\)

Modern spectroscopic/relativistic analyses support a ground-state configuration close to [Rn] 5f14 7s2 7p1, which helps explain some distinctive chemical behavior at the end of the actinide series.

Atoms are swept out of the target by a gas jet, then passed through rapid chromatography or on-line ion-exchange. Identification uses alpha-decay chains and characteristic energies, time correlations, and daughter products rather than bulk physical measurements.

No routine applications exist. Because only a few atoms are produced at a time and the half-lives are short, Lr is used exclusively for fundamental research in nuclear structure and late-actinide chemistry.

Yes. Lr is a radiotoxic heavy metal, but experiments use atom-to-picogram quantities. Even so, work is done with remote handling, hot cells or glove boxes, HEPA-filtered ventilation, dosimetry, and compliant radioactive-waste procedures.

At tracer scale, Lr(III) forms halides (e.g., LrCl3) and coordinates with oxygen-donor ligands (nitrates, phosphates). Redox tuning to transient Lr(II) assists in separating Lr from neighboring trivalent actinides during rapid chromatographic runs.

One illustrative production–decay sequence is:

  • Production (stylized):

    \(^{243}\mathrm{Am}(^{18}\mathrm{O},\,5n)\,^{256}\mathrm{Lr}\)

  • Decay:

    \(^{257}\mathrm{Lr} \;\to\; ^{253}\mathrm{Md} + \alpha\)

Chains continue via successive \(\alpha\)/\(\beta\) steps toward longer-lived daughters.