Lawrencium (Lr)
actinideSolid
Peso atômico padrão
[262]Configuração eletrônica
[Rn] 7s2 5f14 6d1Ponto de fusão
1626,85 °CPonto de ebulição
N/DDensidade
1,56e+4 kg/m³Estados de oxidação
+3Eletronegatividade (Pauling)
N/DEnergia de ionização (1ª)
4,96 eVAno da descoberta
1961Raio atômico
N/DDetalhes
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.
No macroscopic sample of lawrencium has been prepared, and its visible appearance has not been observed. The pure metal’s color, texture, density, melting behavior, and other bulk properties are therefore unknown or only theoretically estimated.
Lawrencium has no practical use outside scientific research. Its isotopes are produced to study nuclear structure, heavy-element synthesis, decay chains, and the chemical behavior at the end of the actinide series. Individual atoms have also been used in chromatography and related experiments to test periodic trends, especially the stability and complexing behavior of Lr³⁺. It has no commercial, medical, industrial, or consumer application.
Since only tiny amounts of lawrencium have ever been produced, there are currently no uses for it outside of basic scientific research.
No weighable compound of lawrencium has been isolated. The established chemistry is dominated by the +3 oxidation state in aqueous solution, where Lr³⁺ is the important species. Atom-at-a-time studies have examined its adsorption and complex formation with mineral acids and organic complexants. Simple compounds such as lawrencium trichloride, LrCl₃, or lawrencium oxide, Lr₂O₃, are chemically plausible by analogy, but their bulk structures and properties have not been measured directly. Higher oxidation states are not established under ordinary chemical conditions.
See more information at the Lawrencium compound page.
All known lawrencium isotopes are radioactive, and safety concerns are radiological rather than ordinary chemical exposure hazards. The amounts produced are extremely small, but work with lawrencium occurs in facilities equipped for heavy-ion reactions and actinide radiochemistry. Isotope-specific half-lives and decay modes matter for handling, shielding, contamination control, and waste management. There is no known biological role.
Lawrencium has no confirmed natural environmental cycle. Any atoms produced on Earth are artificial and decay before dispersal could resemble the behavior of stable elements. In the environment, hypothetical lawrencium would be expected to follow trivalent actinide chemistry to some extent, but this has not been observed at environmental concentrations. Its ecological relevance is therefore limited to controlled laboratory production and radioactive waste from experiments.
Lawrencium has no commodity market, no bulk production, and no recycling stream. It is made only for research by bombarding heavy actinide targets, such as isotopes of californium or berkelium, with accelerated ions. Production yields are very low, often only atoms suitable for immediate detection or chemistry. The limiting factors are accelerator access, rare target materials, radiochemical separation speed, and detector capability rather than ordinary raw-material demand.
Produced by bombarding californium with boron ions.
Lawrencium is not expected to have a persistent cosmic abundance. Its known isotopes decay too rapidly to survive from stellar nucleosynthesis or the formation of the Solar System. Very short-lived lawrencium nuclei could in principle be formed in extreme neutron-rich or heavy-ion processes, but no extraterrestrial occurrence has been detected. Any natural presence would be transient and atomically scarce.
- Lawrencium chemistry is performed one atom at a time.
- Its electron configuration is anomalous, with a 7p electron in the neutral atom’s ground state.
- The element helps test where the actinide series ends and how group 3 should be described.
- Lr³⁺ is more chemically relevant than the neutral metal for experiments.
- No lawrencium compound has been isolated in visible quantity.
Imagens
Propriedades
Física
- Raio de van der Waals
- 246 pm Comparar Raio de van der Waals de todos os elementos →
- Densidade
- 1,56 × 104 kg/m³ Comparar Densidade de todos os elementos →
- Fase nas CNTP
- Sólido Comparar Fase nas CNTP de todos os elementos →
- Ponto de fusão
- 1626,85 °C Comparar Ponto de fusão de todos os elementos →
Química
- Afinidade eletrônica
- 0,315 eV
- Energia de ionização (1ª)
- 4,96 eV Comparar Energia de ionização (1ª) de todos os elementos →
- Energia de ionização (2ª)
- 14,54005 eV Comparar Energia de ionização (2ª) de todos os elementos →
- Energia de ionização (3ª)
- 21,800075 eV Comparar Energia de ionização (3ª) de todos os elementos →
- Energia de ionização (4ª)
- 43,60015 eV Comparar Energia de ionização (4ª) de todos os elementos →
- Energia de ionização (5ª)
- 56,000193 eV Comparar Energia de ionização (5ª) de todos os elementos →
- Estados de oxidação
- +3 Comparar Estados de oxidação de todos os elementos →
- Elétrons de valência
- 3 Comparar Elétrons de valência de todos os elementos →
- Configuração eletrônica
- [Rn] 7s2 5f14 6d1
Termodinâmica
- Calor de sublimação
- 4,249365 eV
- Calor de atomização
- 4,249365 eV
Nuclear
- Prótons
- 103 Comparar Prótons de todos os elementos →
- Nêutrons
- 163 Comparar Nêutrons de todos os elementos →
- Isótopos conhecidos
- 16 Comparar Isótopos conhecidos de todos os elementos →
- Isótopos estáveis
- 0 Comparar Isótopos estáveis de todos os elementos →
- Número de massa (mais estável)
- 262
- Isótopo mais estável
- Lr-266
- Ano da descoberta
- 1961
Abundância
N/D
Estrutura cristalina
N/D
Estrutura eletrônica
- Elétrons por camada
- 2, 8, 18, 32, 32, 8, 3 Comparar Elétrons por camada de todos os elementos →
Identificadores
- Número CAS
- 22537-19-5 Comparar Número CAS de todos os elementos →
- Símbolo de termo
- 2P°1/2
- InChI
- InChI=1S/Lr
- Chave InChI
- CNQCVBJFEGMYDW-UHFFFAOYSA-N
Configuração eletrônica Medido
Lr: 5f¹⁴ 7s² 7p¹[Rn] 5f¹⁴ 7s² 7p¹1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f¹⁴ 7s² 7p¹Modelo atômico
Os isótopos alteram o número de nêutrons, a massa e a estabilidade — não a configuração eletrônica de um átomo neutro.
Modelo atômico esquemático, sem escala.
Assinatura atômica
Espectro de emissão / absorção
Distribuição isotópica
Sem isótopos estáveis.
| Número de massa | Massa atômica (u) | Abundância natural | Meia-vida |
|---|---|---|---|
| 253 Radioativo | 253,09509 ± 0,00022 | N/D | 632 ms |
| 252 Radioativo | 252,09526 ± 0,00026 | N/D | 369 ms |
| 251 Radioativo | 251,09418 ± 0,00032 | N/D | 300 us |
| 261 Radioativo | 261,10688 ± 0,00022 | N/D | 39 minutos |
| 255 Radioativo | 255,096562 ± 0,000019 | N/D | 31.1 segundos |
Fase / Estado
Motivo: 1601,8 °C abaixo do ponto de sublimação (1626,85 °C)
Esquemático, sem escala
Pontos de transição de fase
Energias de transição
Energia necessária para sublimar 1 mol no ponto de sublimação
Densidade
Em condições padrão
Em condições padrão
Espectros atômicos
Mostrando 10 de 103. Ordenado por carga do íon (ordem crescente).
Dados de níveis disponíveis ?
| Íon | Carga | Níveis |
|---|---|---|
| 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 |
Dados de estrutura cristalina indisponíveis
Raios iônicos
| Carga | Coordenação | Spin | Raio |
|---|---|---|---|
| +3 | 9 | N/D | 107.4 pm |
Compostos
Isótopos (5)
| Número de massa | Massa atômica (u) | Abundância natural | Meia-vida | Modo de decaimento | |
|---|---|---|---|---|---|
| 253 Radioativo | 253,09509 ± 0,00022 | N/D | 632 ms | α =90±1%SF =1.0±0.6%β+ ? | |
| 252 Radioativo | 252,09526 ± 0,00026 | N/D | 369 ms | α ≈98%SF ≈2%β+ ? | |
| 251 Radioativo | 251,09418 ± 0,00032 | N/D | 300 us | β+ ?α ? | |
| 261 Radioativo | 261,10688 ± 0,00022 | N/D | 39 minutos | SF ≈100%α ? | |
| 255 Radioativo | 255,096562 ± 0,000019 | N/D | 31.1 segundos | α =99.7±0.1%β+ =0.3±0.1%SF ? |
Propriedades ampliadas
Raios covalentes (dados ampliados)
- Raio covalente (Pyykkö)
- 161 pm
- Raio covalente (Pyykkö, ligação dupla)
- 141 pm
Raios de van der Waals
- UFF
- 323,6 pm
Escalas de numeração
- Mendeleev
- 42
- Pettifor
- 34
- Glawe
- 47
Escalas de eletronegatividade
- Ghosh
- 0
Polarizabilidade e dispersão
- Polarizabilidade dipolar
- 320 a.u.
- Polarizabilidade dipolar (incerteza)
- 20 a.u.
Transições de fase e alótropos
| Ponto de fusão | 1900,15 K |
Categorias de estados de oxidação
Dados de referência avançados
Detalhes dos raios cristalinos (1)
| Carga | CN | Spin | rcrystal (pm) | Origem |
|---|---|---|---|---|
| 3 | IX | — | 121,4 |
Modos de decaimento dos isótopos (38)
| Isótopo | Modo | Intensidade |
|---|---|---|
| 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% |
Dados adicionais
Estimated Crustal Abundance
The estimated element abundance in the earth's crust.
Not Applicable
Referências (1)
- [5] Lawrencium https://education.jlab.org/itselemental/ele103.html
Estimated Oceanic Abundance
The estimated element abundance in the earth's oceans.
Not Applicable
Referências (1)
- [5] Lawrencium https://education.jlab.org/itselemental/ele103.html
Referências
(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.
