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Bk 97

Berkelium (Bk)

actinide
Periode: 7 Block: f

Solid

Standardatomgewicht

[247]

Elektronenkonfiguration

[Rn] 7s2 5f9

Schmelzpunkt

1049,85 °C

Siedepunkt

N/A

Dichte

1,4e+4 kg/m³

Oxidationszustände

+2, +3, +4, +5

Elektronegativität (Pauling)

1,3

Ionisierungsenergie (1.)

6,19785 eV

Entdeckungsjahr

1949

Atomradius

N/A

Details

Namensherkunft Named after Berkeley, California the city of its discovery.
Entdeckungsland United States
Entdecker 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

Bilder

Eigenschaften

Physikalisch

Van-der-Waals-Radius
244 pm Vergleiche Van-der-Waals-Radius aller Elemente →
Dichte
1,4 × 104 kg/m³ Vergleiche Dichte aller Elemente →
Aggregatzustand bei Standardbedingungen
Fest Vergleiche Aggregatzustand bei Standardbedingungen aller Elemente →
Schmelzpunkt
1049,85 °C Vergleiche Schmelzpunkt aller Elemente →

Chemisch

Elektronegativität (Pauling)
1,3 Vergleiche Elektronegativität (Pauling) aller Elemente →
Elektronenaffinität
-0,5 eV (negativer Wert — das Atom bindet voraussichtlich kein zusätzliches Elektron)
Ionisierungsenergie (1.)
6,19785 eV Vergleiche Ionisierungsenergie (1.) aller Elemente →
Ionisierungsenergie (2.)
11,900041 eV Vergleiche Ionisierungsenergie (2.) aller Elemente →
Ionisierungsenergie (3.)
21,600074 eV Vergleiche Ionisierungsenergie (3.) aller Elemente →
Ionisierungsenergie (4.)
36,000124 eV Vergleiche Ionisierungsenergie (4.) aller Elemente →
Ionisierungsenergie (5.)
56,000193 eV Vergleiche Ionisierungsenergie (5.) aller Elemente →
Oxidationszustände
+2, +3, +4, +5 Vergleiche Oxidationszustände aller Elemente →
Valenzelektronen
3 Vergleiche Valenzelektronen aller Elemente →
Allotrope
["\u03b2 form"]
Elektronenkonfiguration
[Rn] 7s2 5f9

Thermodynamisch

Sublimationswärme
3,938436 eV
Atomisierungswärme
3,938436 eV
Atomisierungsenthalpie
3,212935 eV

Nuklear

Protonen
97 Vergleiche Protonen aller Elemente →
Neutronen
150 Vergleiche Neutronen aller Elemente →
Bekannte Isotope
22 Vergleiche Bekannte Isotope aller Elemente →
Stabile Isotope
0 Vergleiche Stabile Isotope aller Elemente →
Massenzahl (stabilstes)
247
Stabilstes Isotop
Bk-247
Entdeckungsjahr
1949

Häufigkeit

N/A

Kristallstruktur

N/A

Elektronische Struktur

Elektronen pro Schale
2, 8, 18, 32, 27, 8, 2 Vergleiche Elektronen pro Schale aller Elemente →

Identifikatoren

CAS-Nummer
7440-40-6 Vergleiche CAS-Nummer aller Elemente →
Termsymbol
6H°15/2
InChI
InChI=1S/Bk
InChI-Key
PWVKJRSRVJTHTR-UHFFFAOYSA-N

Elektronenkonfiguration Gemessen

Ionenladung
Protonen 97
Elektronen 97
Ladung Neutral
Konfiguration Bk: 5f⁹ 7s²
Elektronenkonfiguration
Gemessen
[Rn] 5f⁹ 7s²
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f⁹ 7s²
Orbitaldiagramm
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↑
Gesamtelektronen: 97 Ungepaart: 5 ?

Atommodell

Protonen 97
Neutronen 152
Elektronen 97
Massenzahl 249
Stabilität Radioaktiv

Isotope ändern die Neutronenzahl, Masse und Stabilität — nicht die Elektronenkonfiguration eines neutralen Atoms.

Schematisches Atommodell, nicht maßstabsgetreu.

Atomarer Fingerabdruck

Emissions- / Absorptionsspektrum

0 / 0 (0 0 mit Intensität)
Gemessen
Emission Sichtbar: 380–750 nm

Isotopenverteilung

Keine stabilen Isotope.

MassenzahlAtommasse (u)Natürliche HäufigkeitHalbwertszeit
249 Radioaktiv249,0749877 ± 0,0000027N/A327.2 Tage
239 Radioaktiv239,05824 ± 0,00022N/A100 Sekunden
253 Radioaktiv253,08688 ± 0,00039N/A60 Minuten
251 Radioaktiv251,080762 ± 0,000012N/A55.6 Minuten
233 Radioaktiv233,056652 ± 0,00025N/A40 Sekunden
Gemessen

Phase / Zustand

1 atm / 101.325 kPa
Fest 25 °C (298,15 K)

Grund: 1024,8 °C unter Sublimationspunkt (1049,85 °C)

Sublimationspunkt 1049,85 °C
0 K Aktuelle Temperatur: 25 °C 6000 K
Phasenzeitlinie

Schematisch, nicht maßstabsgetreu

Fest
Gas
Sublimation
25°C
Fest
Flüssig
Gas
Aktuell

Phasenübergangspunkte

Sublimationspunkt Literatur
1049,85 °C
Aktuelle Phase Berechnet
Fest

Übergangsenergien

Sublimationswärme Literatur
3,938436 eV

Energie benötigt, um 1 mol am Sublimationspunkt zu sublimieren

Dichte

Referenzdichte Literatur
1,4e+4 kg/m³

Bei Standardbedingungen

Aktuelle Dichte Berechnet
1,4e+4 kg/m³

Bei Standardbedingungen

Atomspektren

10 von 97 angezeigt. Sortiert nach Ionenladung (aufsteigend).

Liniendaten ?

IonLadungGesamtlinienÜbergangswahrscheinlichkeitenNiveau-Bezeichnungen
Bk I 012000
Bk II +14800
NIST Liniendaten →

Niveaudaten ?

IonLadungNiveaus
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
NIST Niveaudaten →
97 Bk 247

Berkelium — Atomorbital-Visualisierer

[Rn]7s25f9
Energieniveaus 2 8 18 32 27 8 2
Oxidationszustände +2, +3, +4, +5
HOMO 5f n=5 · l=3 · m=-3
Berkelium — Atomorbital-Visualisierer Vorschau
Three.js lädt nur auf Anfrage
97 Bk 247

Berkelium — Kristallstruktur-Visualisierer

Kristallstrukturdaten nicht verfügbar

Ionenradien

LadungKoordinationSpinRadius
+36N/A96 pm
+39N/A113.7 pm
+46N/A83 pm
+48N/A93 pm

Verbindungen

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

Isotope (5)

MassenzahlAtommasse (u)Natürliche HäufigkeitHalbwertszeitZerfallsart
249 Radioaktiv249,0749877 ± 0,0000027N/A327.2 Tage
β- ≈100%α =0.00145±0.8%SF =47e-9±0.2%
239 Radioaktiv239,05824 ± 0,00022N/A100 Sekunden
β+ ≈100%α<0.01% SF<0.01%
253 Radioaktiv253,08688 ± 0,00039N/A60 Minuten
β- ?
251 Radioaktiv251,080762 ± 0,000012N/A55.6 Minuten
β- =100%
233 Radioaktiv233,056652 ± 0,00025N/A40 Sekunden
α ≈82%β+ ?
249 Radioaktiv
Atommasse (u) 249,0749877 ± 0,0000027
Natürliche Häufigkeit N/A
Halbwertszeit 327.2 Tage
Zerfallsart
β- ≈100%α =0.00145±0.8% +1
239 Radioaktiv
Atommasse (u) 239,05824 ± 0,00022
Natürliche Häufigkeit N/A
Halbwertszeit 100 Sekunden
Zerfallsart
β+ ≈100%α<0.01% +1
253 Radioaktiv
Atommasse (u) 253,08688 ± 0,00039
Natürliche Häufigkeit N/A
Halbwertszeit 60 Minuten
Zerfallsart
β- ?
251 Radioaktiv
Atommasse (u) 251,080762 ± 0,000012
Natürliche Häufigkeit N/A
Halbwertszeit 55.6 Minuten
Zerfallsart
β- =100%
233 Radioaktiv
Atommasse (u) 233,056652 ± 0,00025
Natürliche Häufigkeit N/A
Halbwertszeit 40 Sekunden
Zerfallsart
α ≈82%β+ ?

Erweiterte Eigenschaften

Kovalente Radien (Erweitert)

Kovalenzradius (Pyykkö)
168 pm
Kovalenzradius (Pyykkö, doppelt)
139 pm

Van-der-Waals-Radien

Alvarez
340 pm
UFF
333,9 pm

Nummerierungsskalen

Mendeleev
30
Pettifor
40
Glawe
41

Elektronegativitätsskalen

Ghosh
0

Polarisierbarkeit & Dispersion

Dipolpolarisierbarkeit
125 a.u.
Dipolpolarisierbarkeit (Uns.)
25 a.u.

Phasenübergänge & Allotrope

β form
Schmelzpunkt1259,15 K

Oxidationszustands-Kategorien

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

Erweiterte Referenzdaten

Kristallradien-Details (4)
LadungCNSpinrcrystal (pm)Herkunft
3VI110from r^3 vs V plots,
4VI97from r^3 vs V plots,
4VIII107from r^3 vs V plots,
3IX—127,7
Isotopenzerfallsarten (46)
IsotopModusIntensität
233A82%
233B+—
234A80%
234B+20%
235B+—
235A—
236B+100%
236A—
236B+SF0%
237B+—

Zusätzliche Daten

Referenzen

(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.

Lizenzhinweis: 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/

Lizenzhinweis: 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.

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