Bk 97

Berkelium (Bk)

actinide
Period: 7 Block: s

Solid

Standard Atomic Weight

[247]

Electron configuration

[Rn] 7s2 5f9

Melting point

1049.85 °C (1323 K)

Boiling point

N/A

Density

1.400000e+4 kg/m³

Oxidation states

+2, +3, +4, +5

Electronegativity (Pauling)

1.3

Ionization energy (1st)

Discovery year

1949

Atomic radius

N/A

Details

Name origin Named after Berkeley, California the city of its discovery.
Discovery country United States
Discoverers 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

Properties

Physical

Van der Waals radius 244 pm
Density
Phase at STP solid
Melting point 1049.85 °C

Chemical

Electronegativity (Pauling) 1.3
Electron affinity
Ionization energy (1st)
Ionization energy (2nd)
Ionization energy (3rd)
Ionization energy (4th)
Ionization energy (5th)
Oxidation states +2, +3, +4, +5
Valence electrons 3
Allotropes ["\u03b2 form"]
Electron configuration
Electron configuration (semantic)

Thermodynamic

Heat of sublimation 3.938436 eV
Heat of atomization 3.938436 eV
Atomization enthalpy

Nuclear

Stable isotopes 0
Mass number (most stable) 247
Discovery year 1949

Abundance

N/A

Reactivity

N/A

Crystal Structure

N/A

Electronic Structure

Electrons per shell 2, 8, 18, 32, 27, 8, 2

Identifiers

CAS number 7440-40-6
Term symbol
InChI InChI=1S/Bk
InChI Key PWVKJRSRVJTHTR-UHFFFAOYSA-N

Electron Configuration Measured

Ion charge
Protons 97
Electrons 97
Charge Neutral
Configuration Bk: 5f⁹ 7s²
Electron configuration
Measured
[Rn] 5f⁹ 7s²
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f⁹ 7s²
Orbital diagram
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 electrons: 97 Unpaired: 5 ?

Atomic model

Protons 97
Neutrons 152
Electrons 97
Mass number 249
Stability Radioactive

Isotopes change neutron count, mass, and stability — not the electron configuration of a neutral atom.

Schematic atomic model, not to scale.

Atomic Fingerprint

Emission / Absorption Spectrum

0 / 0 (0 with intensity)
Measured
Emission Visible: 380–750 nm

Isotope Distribution

No stable isotopes.

Mass numberAtomic mass (u)Natural abundanceHalf-life
249 Radioactive249.0749877 ± 0.0000027N/A327.2 days
239 Radioactive239.05824 ± 0.00022N/A100 seconds
253 Radioactive253.08688 ± 0.00039N/A60 minutes
251 Radioactive251.080762 ± 0.000012N/A55.6 minutes
233 Radioactive233.056652 ± 0.00025N/A40 seconds
Measured

Phase / State

1 atm / 101.325 kPa
Solid 25 °C (298.15 K)

Reason: 1024.8 °C below sublimation point (1049.85 °C)

Sublimation point 1049.85 °C
0 K Current temperature: 25 °C 6000 K
Phase timeline

Schematic, not to scale

Solid
Gas
Sublimation
25°C
Solid
Liquid
Gas
Current

Phase transition points

Sublimation point Literature
1049.85 °C
Current phase Calculated
Solid

Transition energies

Heat of sublimation Literature
3.938436 eV

Energy required to sublime 1 mol at sublimation point

Density

Reference density Literature
1.400000e+4 kg/m³

At standard conditions

Current density Calculated
1.400000e+4 kg/m³

At standard conditions

Atomic Spectra

Showing 10 of 97 Atomic Spectra. Sorted by ion charge (ascending).

Lines Holdings ?

IonChargeTotal linesTransition probabilitiesLevel designations
Bk I 012000
Bk II +14800
NIST Lines Holdings →

Levels Holdings ?

IonChargeLevels
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 Levels Holdings →
97 Bk 247

Berkelium — Atomic Orbital Visualizer

[Rn]7s25f9
Energy levels 2 8 18 32 27 8 2
Oxidation states +2, +3, +4, +5
HOMO 5f n=5 · l=3 · m=-3
Berkelium — Atomic Orbital Visualizer Preview
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97 Bk 247

Berkelium — Crystal Structure Visualizer

Crystal structure data not available

Ionic Radii

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

Compounds

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)

Mass numberAtomic mass (u)Natural abundanceHalf-lifeDecay mode
249 Radioactive249.0749877 ± 0.0000027N/A327.2 days
β- ≈100%α =0.00145±0.8%SF =47e-9±0.2%
239 Radioactive239.05824 ± 0.00022N/A100 seconds
β+ ≈100%α<0.01% SF<0.01%
253 Radioactive253.08688 ± 0.00039N/A60 minutes
β- ?
251 Radioactive251.080762 ± 0.000012N/A55.6 minutes
β- =100%
233 Radioactive233.056652 ± 0.00025N/A40 seconds
α ≈82%β+ ?
249 Radioactive
Atomic mass (u) 249.0749877 ± 0.0000027
Natural abundance N/A
Half-life 327.2 days
Decay mode
β- ≈100%α =0.00145±0.8% +1
239 Radioactive
Atomic mass (u) 239.05824 ± 0.00022
Natural abundance N/A
Half-life 100 seconds
Decay mode
β+ ≈100%α<0.01% +1
253 Radioactive
Atomic mass (u) 253.08688 ± 0.00039
Natural abundance N/A
Half-life 60 minutes
Decay mode
β- ?
251 Radioactive
Atomic mass (u) 251.080762 ± 0.000012
Natural abundance N/A
Half-life 55.6 minutes
Decay mode
β- =100%
233 Radioactive
Atomic mass (u) 233.056652 ± 0.00025
Natural abundance N/A
Half-life 40 seconds
Decay mode
α ≈82%β+ ?

Extended Properties

Covalent Radii (Extended)

Covalent radius (Pyykkö)  
Covalent radius (Pyykkö, double)  

Van der Waals Radii

Alvarez  
UFF  

Numbering Scales

Mendeleev
Pettifor
Glawe

Electronegativity Scales

Ghosh

Polarizability & Dispersion

Dipole polarizability  
Dipole polarizability (unc.)  

Phase Transitions & Allotropes

β form
Melting point1259.15 K

Oxidation State Categories

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

Advanced Reference Data

Crystal Radii Detail (4)
ChargeCNSpinrcrystal (pm)Origin
3VI110from r^3 vs V plots,
4VI97from r^3 vs V plots,
4VIII107from r^3 vs V plots,
3IX127.7
Isotope Decay Modes (46)
IsotopeModeIntensity
233A82%
233B+
234A80%
234B+20%
235B+
235A
236B+100%
236A
236B+SF0%
237B+

Additional Data

References

(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.

License note: 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/

License note: 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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