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Bk 97

Berkelium (Bk)

actinide
Période: 7 Bloc: f

Solid

Masse atomique relative standard

[247]

Configuration électronique

[Rn] 7s2 5f9

Point de fusion

1049,85 °C

Point d’ébullition

N/D

Masse volumique

1,4e+4 kg/m³

États d’oxydation

+2, +3, +4, +5

Électronégativité (Pauling)

1,3

Énergie d’ionisation (1re)

6,19785 eV

Année de découverte

1949

Rayon atomique

N/D

Détails

Origine du nom Named after Berkeley, California the city of its discovery.
Pays de découverte United States
Découvreurs 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

Images

Propriétés

Propriétés chimiques

Électronégativité (Pauling)
1,3 Comparer : Électronégativité (Pauling) de tous les éléments →
Affinité électronique
-0,5 eV (valeur négative — l'atome ne devrait pas lier d'électron supplémentaire)
Énergie d’ionisation (1re)
6,19785 eV Comparer : Énergie d’ionisation (1re) de tous les éléments →
Énergie d’ionisation (2e)
11,900041 eV Comparer : Énergie d’ionisation (2e) de tous les éléments →
Énergie d’ionisation (3e)
21,600074 eV Comparer : Énergie d’ionisation (3e) de tous les éléments →
Énergie d’ionisation (4e)
36,000124 eV Comparer : Énergie d’ionisation (4e) de tous les éléments →
Énergie d’ionisation (5e)
56,000193 eV Comparer : Énergie d’ionisation (5e) de tous les éléments →
États d’oxydation
+2, +3, +4, +5 Comparer : États d’oxydation de tous les éléments →
Électrons de valence
3 Comparer : Électrons de valence de tous les éléments →
Allotropes
["\u03b2 form"]
Configuration électronique
[Rn] 7s2 5f9

Propriétés thermodynamiques

Enthalpie de sublimation
3,938436 eV
Enthalpie d’atomisation
3,938436 eV
Enthalpie d’atomisation
3,212935 eV

Propriétés nucléaires

Protons
97 Comparer : Protons de tous les éléments →
Neutrons
150 Comparer : Neutrons de tous les éléments →
Isotopes connus
22 Comparer : Isotopes connus de tous les éléments →
Isotopes stables
0 Comparer : Isotopes stables de tous les éléments →
Nombre de masse (isotope le plus stable)
247
Isotope le plus stable
Bk-247
Année de découverte
1949

Abondance

N/D

Structure cristalline

N/D

Structure électronique

Électrons par couche
2, 8, 18, 32, 27, 8, 2 Comparer : Électrons par couche de tous les éléments →

Identifiants

Numéro CAS
7440-40-6 Comparer : Numéro CAS de tous les éléments →
Symbole de terme
6H°15/2
InChI
InChI=1S/Bk
Clé InChI
PWVKJRSRVJTHTR-UHFFFAOYSA-N

Configuration électronique Mesuré

Charge ionique
Protons 97
Électrons 97
Charge Neutre
Configuration Bk: 5f⁹ 7s²
Configuration électronique
Mesuré
[Rn] 5f⁹ 7s²
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f⁹ 7s²
Diagramme d’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↑
Nombre total d’électrons: 97 Non appariés: 5 ?

Modèle atomique

Protons 97
Neutrons 152
Électrons 97
Nombre de masse 249
Stabilité Radioactif

Les isotopes diffèrent par leur nombre de neutrons, leur masse et leur stabilité — pas par la configuration électronique de l’atome neutre.

Modèle atomique schématique, non à l’échelle.

Empreinte atomique

Spectre d’émission / d’absorption

0 / 0 (0 0 avec intensité)
Mesuré
Émission Visible : 380–750 nm

Distribution isotopique

Aucun isotope stable.

Nombre de masseMasse atomique (u)Abondance naturelleDemi-vie
249 Radioactif249,0749877 ± 0,0000027N/D327.2 jours
239 Radioactif239,05824 ± 0,00022N/D100 secondes
253 Radioactif253,08688 ± 0,00039N/D60 minutes
251 Radioactif251,080762 ± 0,000012N/D55.6 minutes
233 Radioactif233,056652 ± 0,00025N/D40 secondes
Mesuré

Phase / État

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

Explication: 1024,8 °C en dessous du point de sublimation (1049,85 °C)

Point de sublimation 1049,85 °C
0 K Température actuelle: 25 °C 6000 K
Échelle des phases

Schématique, non à l’échelle

Solide
Gaz
Sublimation
25°C
Solide
Liquide
Gaz
Actuel

Points de transition de phase

Point de sublimation Littérature scientifique
1049,85 °C
Phase actuelle Calculé
Solide

Énergies de transition

Enthalpie de sublimation Littérature scientifique
3,938436 eV

Énergie nécessaire pour sublimer 1 mol au point de sublimation

Masse volumique

Masse volumique de référence Littérature scientifique
1,4e+4 kg/m³

Dans les conditions standard

Masse volumique actuelle Calculé
1,4e+4 kg/m³

Dans les conditions standard

Spectres atomiques

Affichage de 10 sur 97. Tri par charge ionique croissante.

Raies répertoriées ?

IonChargeNombre total de raiesProbabilités de transitionDésignations des niveaux
Bk I 012000
Bk II +14800
Raies répertoriées par le NIST →

Niveaux répertoriés ?

IonChargeNiveaux
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
Niveaux répertoriés par le NIST →
97 Bk 247

Berkelium — Visualiseur d’orbitales atomiques

[Rn]7s25f9
Niveaux d’énergie 2 8 18 32 27 8 2
États d’oxydation +2, +3, +4, +5
HOMO 5f n=5 · l=3 · m=-3
Berkelium — Aperçu du visualiseur d’orbitales atomiques
Three.js se charge uniquement à la demande
97 Bk 247

Berkelium — Visualiseur de structure cristalline

Données de structure cristalline indisponibles

Rayons ioniques

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

Composés

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

Isotopes (5)

Nombre de masseMasse atomique (u)Abondance naturelleDemi-vieMode de désintégration
249 Radioactif249,0749877 ± 0,0000027N/D327.2 jours
β- ≈100%α =0.00145±0.8%SF =47e-9±0.2%
239 Radioactif239,05824 ± 0,00022N/D100 secondes
β+ ≈100%α<0.01% SF<0.01%
253 Radioactif253,08688 ± 0,00039N/D60 minutes
β- ?
251 Radioactif251,080762 ± 0,000012N/D55.6 minutes
β- =100%
233 Radioactif233,056652 ± 0,00025N/D40 secondes
α ≈82%β+ ?
249 Radioactif
Masse atomique (u) 249,0749877 ± 0,0000027
Abondance naturelle N/D
Demi-vie 327.2 jours
Mode de désintégration
β- ≈100%α =0.00145±0.8% +1
239 Radioactif
Masse atomique (u) 239,05824 ± 0,00022
Abondance naturelle N/D
Demi-vie 100 secondes
Mode de désintégration
β+ ≈100%α<0.01% +1
253 Radioactif
Masse atomique (u) 253,08688 ± 0,00039
Abondance naturelle N/D
Demi-vie 60 minutes
Mode de désintégration
β- ?
251 Radioactif
Masse atomique (u) 251,080762 ± 0,000012
Abondance naturelle N/D
Demi-vie 55.6 minutes
Mode de désintégration
β- =100%
233 Radioactif
Masse atomique (u) 233,056652 ± 0,00025
Abondance naturelle N/D
Demi-vie 40 secondes
Mode de désintégration
α ≈82%β+ ?

Propriétés étendues

Rayons covalents (données étendues)

Rayon covalent (Pyykkö)
168 pm
Rayon covalent (Pyykkö, liaison double)
139 pm

Rayons de van der Waals

Alvarez
340 pm
UFF
333,9 pm

Échelles de numérotation

Mendeleev
30
Pettifor
40
Glawe
41

Échelles d’électronégativité

Ghosh
0

Polarisabilité et dispersion

Polarisabilité dipolaire
125 a.u.
Polarisabilité dipolaire (incertitude)
25 a.u.

Transitions de phase et allotropes

β form
Point de fusion1259,15 K

Catégories d’états d’oxydation

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

Données de référence avancées

Détail des rayons cristallins (4)
ChargeCNSpinrcrystal (pm)Origine
3VI110from r^3 vs V plots,
4VI97from r^3 vs V plots,
4VIII107from r^3 vs V plots,
3IX—127,7
Modes de désintégration des isotopes (46)
IsotopeModeIntensité
233A82%
233B+—
234A80%
234B+20%
235B+—
235A—
236B+100%
236A—
236B+SF0%
237B+—

Données complémentaires

Références

(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.

Note sur la licence: 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/

Note sur la licence: 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.

Dernière mise à jour:

Données vérifiées:

Le contenu est vérifié au regard des dernières données scientifiques.