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Bk 97

Berkelium (Bk)

actinide
Periodo: 7 Bloque: f

Solid

Peso atómico estándar

[247]

Configuración electrónica

[Rn] 7s2 5f9

Punto de fusión

1049,85 °C

Punto de ebullición

N/D

Densidad

1,4e+4 kg/m³

Estados de oxidación

+2, +3, +4, +5

Electronegatividad (Pauling)

1,3

Energía de ionización (1.ª)

6,19785 eV

Año de descubrimiento

1949

Radio atómico

N/D

Detalles

Origen del nombre Named after Berkeley, California the city of its discovery.
País de descubrimiento United States
Descubridores 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

Imágenes

Propiedades

Químicas

Electronegatividad (Pauling)
1,3 Comparar Electronegatividad (Pauling) de todos los elementos →
Afinidad electrónica
-0,5 eV (valor negativo: se predice que el átomo no capta un electrón adicional)
Energía de ionización (1.ª)
6,19785 eV Comparar Energía de ionización (1.ª) de todos los elementos →
Energía de ionización (2.ª)
11,900041 eV Comparar Energía de ionización (2.ª) de todos los elementos →
Energía de ionización (3.ª)
21,600074 eV Comparar Energía de ionización (3.ª) de todos los elementos →
Energía de ionización (4.ª)
36,000124 eV Comparar Energía de ionización (4.ª) de todos los elementos →
Energía de ionización (5.ª)
56,000193 eV Comparar Energía de ionización (5.ª) de todos los elementos →
Estados de oxidación
+2, +3, +4, +5 Comparar Estados de oxidación de todos los elementos →
Electrones de valencia
3 Comparar Electrones de valencia de todos los elementos →
Alótropos
["\u03b2 form"]
Configuración electrónica
[Rn] 7s2 5f9

Termodinámicas

Calor de sublimación
3,938436 eV
Calor de atomización
3,938436 eV
Entalpía de atomización
3,212935 eV

Nucleares

Protones
97 Comparar Protones de todos los elementos →
Neutrones
150 Comparar Neutrones de todos los elementos →
Isótopos conocidos
22 Comparar Isótopos conocidos de todos los elementos →
Isótopos estables
0 Comparar Isótopos estables de todos los elementos →
Número másico (isótopo más estable)
247
Isótopo más estable
Bk-247
Año de descubrimiento
1949

Abundancia

N/D

Estructura cristalina

N/D

Estructura electrónica

Electrones por capa
2, 8, 18, 32, 27, 8, 2 Comparar Electrones por capa de todos los elementos →

Identificadores

Número CAS
7440-40-6 Comparar Número CAS de todos los elementos →
Símbolo del término
6H°15/2
InChI
InChI=1S/Bk
Clave InChI
PWVKJRSRVJTHTR-UHFFFAOYSA-N

Configuración electrónica Medido

Carga del ion
Protones 97
Electrones 97
Carga Neutro
Configuración Bk: 5f⁹ 7s²
Configuración electrónica
Medido
[Rn] 5f⁹ 7s²
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f⁹ 7s²
Diagrama de orbitales
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 electrones: 97 Desapareados: 5 ?

Modelo atómico

Protones 97
Neutrones 152
Electrones 97
Número másico 249
Estabilidad Radiactivo

Los isótopos cambian el número de neutrones, la masa y la estabilidad, pero no la configuración electrónica de un átomo neutro.

Modelo atómico esquemático, no a escala.

Huella atómica

Espectro de emisión / absorción

0 / 0 (0 0 con intensidad)
Medido
Emisión Visible: 380–750 nm

Distribución isotópica

No hay isótopos estables.

Número másicoMasa atómica (u)Abundancia naturalPeriodo de semidesintegración
249 Radiactivo249,0749877 ± 0,0000027N/D327.2 días
239 Radiactivo239,05824 ± 0,00022N/D100 segundos
253 Radiactivo253,08688 ± 0,00039N/D60 minutos
251 Radiactivo251,080762 ± 0,000012N/D55.6 minutos
233 Radiactivo233,056652 ± 0,00025N/D40 segundos
Medido

Fase / Estado

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

Motivo: 1024,8 °C por debajo del punto de sublimación (1049,85 °C)

Punto de sublimación 1049,85 °C
0 K Temperatura actual: 25 °C 6000 K
Secuencia de fases

Esquemático, no a escala

Sólido
Gas
Sublimación
25°C
Sólido
Líquido
Gas
Actual

Puntos de transición de fase

Punto de sublimación Bibliografía
1049,85 °C
Fase actual Calculado
Sólido

Energías de transición

Calor de sublimación Bibliografía
3,938436 eV

Energía necesaria para sublimar 1 mol en el punto de sublimación

Densidad

Densidad de referencia Bibliografía
1,4e+4 kg/m³

En condiciones estándar

Densidad actual Calculado
1,4e+4 kg/m³

En condiciones estándar

Espectros atómicos

Se muestran 10 de 97. Ordenado por carga del ion (ascendente).

Líneas disponibles ?

IonCargaTotal de líneasProbabilidades de transiciónDesignaciones de los niveles
Bk I 012000
Bk II +14800
Líneas disponibles en el NIST →

Niveles disponibles ?

IonCargaNiveles
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
Niveles disponibles en el NIST →
97 Bk 247

Berkelium — Visualizador de orbitales atómicos

[Rn]7s25f9
Niveles de energía 2 8 18 32 27 8 2
Estados de oxidación +2, +3, +4, +5
HOMO 5f n=5 · l=3 · m=-3
Berkelium — Vista previa del visualizador de orbitales atómicos
Three.js solo se carga cuando se solicita
97 Bk 247

Berkelium — Visualizador de estructuras cristalinas

No hay datos disponibles sobre la estructura cristalina

Radios iónicos

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

Compuestos

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 másicoMasa atómica (u)Abundancia naturalPeriodo de semidesintegraciónModo de desintegración
249 Radiactivo249,0749877 ± 0,0000027N/D327.2 días
β- ≈100%α =0.00145±0.8%SF =47e-9±0.2%
239 Radiactivo239,05824 ± 0,00022N/D100 segundos
β+ ≈100%α<0.01% SF<0.01%
253 Radiactivo253,08688 ± 0,00039N/D60 minutos
β- ?
251 Radiactivo251,080762 ± 0,000012N/D55.6 minutos
β- =100%
233 Radiactivo233,056652 ± 0,00025N/D40 segundos
α ≈82%β+ ?
249 Radiactivo
Masa atómica (u) 249,0749877 ± 0,0000027
Abundancia natural N/D
Periodo de semidesintegración 327.2 días
Modo de desintegración
β- ≈100%α =0.00145±0.8% +1
239 Radiactivo
Masa atómica (u) 239,05824 ± 0,00022
Abundancia natural N/D
Periodo de semidesintegración 100 segundos
Modo de desintegración
β+ ≈100%α<0.01% +1
253 Radiactivo
Masa atómica (u) 253,08688 ± 0,00039
Abundancia natural N/D
Periodo de semidesintegración 60 minutos
Modo de desintegración
β- ?
251 Radiactivo
Masa atómica (u) 251,080762 ± 0,000012
Abundancia natural N/D
Periodo de semidesintegración 55.6 minutos
Modo de desintegración
β- =100%
233 Radiactivo
Masa atómica (u) 233,056652 ± 0,00025
Abundancia natural N/D
Periodo de semidesintegración 40 segundos
Modo de desintegración
α ≈82%β+ ?

Propiedades ampliadas

Radios covalentes (ampliados)

Radio covalente (Pyykkö)
168 pm
Radio covalente (Pyykkö, enlace doble)
139 pm

Radios de van der Waals

Alvarez
340 pm
UFF
333,9 pm

Escalas de numeración

Mendeleev
30
Pettifor
40
Glawe
41

Escalas de electronegatividad

Ghosh
0

Polarizabilidad y dispersión

Polarizabilidad dipolar
125 a.u.
Polarizabilidad dipolar (incert.)
25 a.u.

Transiciones de fase y alótropos

β form
Punto de fusión1259,15 K

Categorías de estados de oxidación

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

Datos de referencia avanzados

Detalle de los radios cristalinos (4)
CargaCNEspínrcrystal (pm)Origen
3VI110from r^3 vs V plots,
4VI97from r^3 vs V plots,
4VIII107from r^3 vs V plots,
3IX—127,7
Modos de desintegración de los isótopos (46)
IsótopoModoIntensidad
233A82%
233B+—
234A80%
234B+20%
235B+—
235A—
236B+100%
236A—
236B+SF0%
237B+—

Datos adicionales

Referencias

(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 la licencia: 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 la licencia: 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 actualización:

Datos verificados:

El contenido se revisa conforme a los datos científicos más recientes.