← Voltar à tabela periódica
Bk 97

Berkelium (Bk)

actinide
Período: 7 Bloco: f

Solid

Peso atômico padrão

[247]

Configuração eletrônica

[Rn] 7s2 5f9

Ponto de fusão

1049,85 °C

Ponto de ebulição

N/D

Densidade

1,4e+4 kg/m³

Estados de oxidação

+2, +3, +4, +5

Eletronegatividade (Pauling)

1,3

Energia de ionização (1ª)

6,19785 eV

Ano da descoberta

1949

Raio atômico

N/D

Detalhes

Origem do nome Named after Berkeley, California the city of its discovery.
País da descoberta United States
Descobridores G.T.Seaborg, S.G.Tompson, A.Ghiorso

Berkelium is a synthetic transuranium actinide with no stable isotopes. It is produced in nuclear reactors by neutron capture in lighter actinides and is normally handled in microgram to milligram research quantities. Its chemistry is mainly that of a trivalent actinide, but berkelium is notable because the +4 state is comparatively accessible in solution and solids. The isotope ²⁴⁹Bk is the most important for chemical work because its half-life permits separation, shipment, and target fabrication.

Berkelium does not occur naturally in the Earth’s crust. It was first synthesized in December 1949 by Stanley G. Thompson, Glenn T. Seaborg, and Albert Ghiorso at the University of California in Berkeley using the nuclear reaction 241Am (4He, 2n) 243Bk in the Berkeley 60-inch cyclotron. The element was named for the town in California where it was first synthesized. The first isotope of berkelium produced from this experiment had a mass number of 243 and a half-life of 4.5 h. 247Bk has a half-life of 1.4×103 years, which makes it one of the least radioactive isotopes of berkelium. 249Bk has a half-life of 320 days, which makes it possible to isolate and study on a macroscopic scale, although studies have found that the radiation given off from berkelium creates health hazards. For example, lengthy exposure to the radiation from berkelium has been shown to cause an accumulation of berkelium in the skeletal system of rats. The radiation is also unfavorable to the formation of red blood cells [620], [621], [622], [623], [624]. Berkelium has no known isotopic applications aside from scientific research, in which it served as a target for the production of tennessine (Fig. IUPAC.97.1).

Berkelium was first produced by Stanley G. Thompson, Glenn T. Seaborg, Kenneth Street, Jr. and Albert Ghiorso working at the University of California, Berkeley, in December, 1949. They bombarded an isotope of americium, americium-241, with alpha particles with a device called a cyclotron. This created berkelium-243 and two free neutrons. Berkelium's most stable isotope, berkelium-247, has a half-life of about 1,380 years. It decays into americium-243 through alpha decay.

The first visible amounts of a berkelium compound, berkelium chloride (BkCl3) was produced in 1962 and weighed about 3 billionths of a gram (0.000000003 grams). Berkelium oxychloride (BkOCl), berkelium fluoride (BkF3), berkelium dioxide (BkO2) and berkelium trioxide (BkO3) have been identified and studied with a method known as X-ray diffraction.

Since only small amounts of berkelium have ever been produced, there are no known uses for berkelium and its compounds outside of basic scientific research.

Berkelium, the eighth member of the actinide transition series, was first produced in 1949 by Thompson, Ghiorso, and Seaborg via accelerator bombardment of 241Am with high energy alpha particles. This generated a new electron-capture activity eluting on a chromatography column just ahead of curium. This activity was assigned to an isotope of element 97 with mass number 243. It was named berkelium after Berkeley, California, the city of its discovery. Initial investigation of its chemical properties were limited to tracer experiments (ion exchange and co-precipitation) but these were sufficient to establish the stability of Bk(III) and the accessibility of Bk(IV) ions in aqueous solution and provide an estimate of the electrochemical potential of the Bk(IV)/Bk(III) couple.

A complete study of an element is not possible by tracer methods alone, so a campaign was initiated in 1952 for long-term irradiation of about 8 grams of 239Pu in a nuclear reactor in Arco, Idaho to provide macro amounts of berkelium. In 1958 about 0.6 micrograms of 249Bk with a half-life of 330 days was recovered, separated, and purified by Cunningham et al. who determined the absorption spectrum in aqueous solution and measured the magnetic susceptibility of Bk(III). The first structural determination of a berkelium compound was in 1962. Four X-ray diffraction lines were obtained from 4 nanograms of berkelium-249 dioxide and indexed as face centered cubic. The first bulk (> 1 microgram) samples of berkelium metal were prepared in 1969 by reduction of BkF3 with lithium metal vapor at 1300 K by Haire and Peterson et al. Bk metal issilvery in appearance, easily soluble in dilute mineral acids, and rapidly oxidized by air or oxygen at elevated temperatures to form the oxide. The metal exhibits two crystal forms: double hexagonal closest packed (dhcp) and face centered cubic (fcc). Numerous alloys and compounds of berkelium have been prepared and studied including hydrides, oxides, halides, chalcogenides, pnictides, oxalates, oxychlorides, organometallic, and coordination compounds to name a few. Berkelium oxidation states Bk(0), Bk(III), and Bk(IV) are known in bulk and some evidence has been offered for the existence of Bk(II) but there is only speculation on the possible existence of Bk(V) ions.

Fourteen isotopes of berkelium are now known and have been synthesized from mass number 238 to 251. As with other actinide elements, berkelium tends to accumulate in the skeletal system. Because of its rarity, berkelium presently has no commercial use, however, with its relatively long half-life and availability in microgram quantities, Bk-249 is used extensively as a target to synthesize heavier elements by charged particle bombardment. Berkelium is the first member of the second half of the actinide series and as such, studies of the physicochemical properties of this element enables more accurate extrapolations to the behavior of the heavier elements for which studies are severely limited by scarcity of material, very short half-lives, and intense radioactivity.

Further reading: D. E. Hobart and J. R. Peterson (2006) "Berkelium," Chapter 10 in The Chemistry of the Actinide and Transactinide Elements, Third Edition, L. R. Morss, J. Fuger, and N. M. Edelstein, Eds, Springer Publishers.

This element reviewed and Updated by David Hobart, Los Alamos National Laboratory 2011

Imagens

Propriedades

Química

Eletronegatividade (Pauling)
1,3 Comparar Eletronegatividade (Pauling) de todos os elementos →
Afinidade eletrônica
-0,5 eV (valor negativo — prevê-se que o átomo não capte um eletrão adicional)
Energia de ionização (1ª)
6,19785 eV Comparar Energia de ionização (1ª) de todos os elementos →
Energia de ionização (2ª)
11,900041 eV Comparar Energia de ionização (2ª) de todos os elementos →
Energia de ionização (3ª)
21,600074 eV Comparar Energia de ionização (3ª) de todos os elementos →
Energia de ionização (4ª)
36,000124 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
+2, +3, +4, +5 Comparar Estados de oxidação de todos os elementos →
Elétrons de valência
3 Comparar Elétrons de valência de todos os elementos →
Alótropos
["\u03b2 form"]
Configuração eletrônica
[Rn] 7s2 5f9

Termodinâmica

Calor de sublimação
3,938436 eV
Calor de atomização
3,938436 eV
Entalpia de atomização
3,212935 eV

Nuclear

Prótons
97 Comparar Prótons de todos os elementos →
Nêutrons
150 Comparar Nêutrons de todos os elementos →
Isótopos conhecidos
22 Comparar Isótopos conhecidos de todos os elementos →
Isótopos estáveis
0 Comparar Isótopos estáveis de todos os elementos →
Número de massa (mais estável)
247
Isótopo mais estável
Bk-247
Ano da descoberta
1949

Abundância

N/D

Estrutura cristalina

N/D

Estrutura eletrônica

Elétrons por camada
2, 8, 18, 32, 27, 8, 2 Comparar Elétrons por camada de todos os elementos →

Identificadores

Número CAS
7440-40-6 Comparar Número CAS de todos os elementos →
Símbolo de termo
6H°15/2
InChI
InChI=1S/Bk
Chave InChI
PWVKJRSRVJTHTR-UHFFFAOYSA-N

Configuração eletrônica Medido

Carga do íon
Prótons 97
Elétrons 97
Carga Neutro
Configuração Bk: 5f⁹ 7s²
Configuração eletrônica
Medido
[Rn] 5f⁹ 7s²
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f⁹ 7s²
Diagrama de orbitais
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
9/14 5↑
Total de elétrons: 97 Desemparelhados: 5 ?

Modelo atômico

Prótons 97
Nêutrons 152
Elétrons 97
Número de massa 249
Estabilidade Radioativo

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

0 / 0 (0 0 com intensidade)
Medido
Emissão Visível: 380–750 nm

Distribuição isotópica

Sem isótopos estáveis.

Número de massaMassa atômica (u)Abundância naturalMeia-vida
249 Radioativo249,0749877 ± 0,0000027N/D327.2 dias
239 Radioativo239,05824 ± 0,00022N/D100 segundos
253 Radioativo253,08688 ± 0,00039N/D60 minutos
251 Radioativo251,080762 ± 0,000012N/D55.6 minutos
233 Radioativo233,056652 ± 0,00025N/D40 segundos
Medido

Fase / Estado

1 atm / 101,325 kPa
Sólido 25 °C (298,15 K)

Motivo: 1024,8 °C abaixo do ponto de sublimação (1049,85 °C)

Ponto de sublimação 1049,85 °C
0 K Temperatura atual: 25 °C 6000 K
Linha do tempo das fases

Esquemático, sem escala

Sólido
Gás
Sublimação
25°C
Sólido
Líquido
Gás
Atual

Pontos de transição de fase

Ponto de sublimação Literatura
1049,85 °C
Fase atual Calculado
Sólido

Energias de transição

Calor de sublimação Literatura
3,938436 eV

Energia necessária para sublimar 1 mol no ponto de sublimação

Densidade

Densidade de referência Literatura
1,4e+4 kg/m³

Em condições padrão

Densidade atual Calculado
1,4e+4 kg/m³

Em condições padrão

Espectros atômicos

Mostrando 10 de 97. Ordenado por carga do íon (ordem crescente).

Dados de linhas disponíveis ?

ÍonCargaTotal de linhasProbabilidades de transiçãoDesignações dos níveis
Bk I 012000
Bk II +14800
Dados de linhas disponíveis no NIST →

Dados de níveis disponíveis ?

ÍonCargaNíveis
Bk I 02
Bk II +12
Bk III +22
Bk IV +32
Bk V +42
Bk VI +52
Bk VII +62
Bk VIII +72
Bk IX +82
Bk X +92
Dados de níveis disponíveis no NIST →
97 Bk 247

Berkelium — Visualizador de orbitais atômicos

[Rn]7s25f9
Níveis de energia 2 8 18 32 27 8 2
Estados de oxidação +2, +3, +4, +5
HOMO 5f n=5 · l=3 · m=-3
Berkelium — Prévia do visualizador de orbitais atômicos
O Three.js é carregado apenas quando solicitado
97 Bk 247

Berkelium — Visualizador de estruturas cristalinas

Dados de estrutura cristalina indisponíveis

Raios iônicos

CargaCoordenaçãoSpinRaio
+36N/D96 pm
+39N/D113.7 pm
+46N/D83 pm
+48N/D93 pm

Compostos

Bk
247,070 u
Bk
249,075 u
Bk
247,070 u
Bk
250,078 u
Bk
246,069 u
Bk
245,066 u

Isótopos (5)

Número de massaMassa atômica (u)Abundância naturalMeia-vidaModo de decaimento
249 Radioativo249,0749877 ± 0,0000027N/D327.2 dias
β- ≈100%α =0.00145±0.8%SF =47e-9±0.2%
239 Radioativo239,05824 ± 0,00022N/D100 segundos
β+ ≈100%α<0.01% SF<0.01%
253 Radioativo253,08688 ± 0,00039N/D60 minutos
β- ?
251 Radioativo251,080762 ± 0,000012N/D55.6 minutos
β- =100%
233 Radioativo233,056652 ± 0,00025N/D40 segundos
α ≈82%β+ ?
249 Radioativo
Massa atômica (u) 249,0749877 ± 0,0000027
Abundância natural N/D
Meia-vida 327.2 dias
Modo de decaimento
β- ≈100%α =0.00145±0.8% +1
239 Radioativo
Massa atômica (u) 239,05824 ± 0,00022
Abundância natural N/D
Meia-vida 100 segundos
Modo de decaimento
β+ ≈100%α<0.01% +1
253 Radioativo
Massa atômica (u) 253,08688 ± 0,00039
Abundância natural N/D
Meia-vida 60 minutos
Modo de decaimento
β- ?
251 Radioativo
Massa atômica (u) 251,080762 ± 0,000012
Abundância natural N/D
Meia-vida 55.6 minutos
Modo de decaimento
β- =100%
233 Radioativo
Massa atômica (u) 233,056652 ± 0,00025
Abundância natural N/D
Meia-vida 40 segundos
Modo de decaimento
α ≈82%β+ ?

Propriedades ampliadas

Raios covalentes (dados ampliados)

Raio covalente (Pyykkö)
168 pm
Raio covalente (Pyykkö, ligação dupla)
139 pm

Raios de van der Waals

Alvarez
340 pm
UFF
333,9 pm

Escalas de numeração

Mendeleev
30
Pettifor
40
Glawe
41

Escalas de eletronegatividade

Ghosh
0

Polarizabilidade e dispersão

Polarizabilidade dipolar
125 a.u.
Polarizabilidade dipolar (incerteza)
25 a.u.

Transições de fase e alótropos

β form
Ponto de fusão1259,15 K

Categorias de estados de oxidação

+3 main
+4 extended
+5 extended
+2 extended

Dados de referência avançados

Detalhes dos raios cristalinos (4)
CargaCNSpinrcrystal (pm)Origem
3VI110from r^3 vs V plots,
4VI97from r^3 vs V plots,
4VIII107from r^3 vs V plots,
3IX—127,7
Modos de decaimento dos isótopos (46)
IsótopoModoIntensidade
233A82%
233B+—
234A80%
234B+20%
235B+—
235A—
236B+100%
236A—
236B+SF0%
237B+—

Dados adicionais

Referências

(9)
2 Atomic Mass Data Center (AMDC), International Atomic Energy Agency (IAEA)
Bk

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)
Berkelium

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.

Nota sobre a licença: 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
Berkelium

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/

Nota sobre a licença: Please see citation and linking information: https://education.jlab.org/faq/index.html
6 Los Alamos National Laboratory, U.S. Department of Energy
Berkelium

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
Berkelium

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
Berkelium

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

9 PubChem Elements
Berkelium

The element property data was retrieved from publications.

Última atualização:

Dados verificados:

O conteúdo é revisado com base nos dados científicos mais recentes.