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Bk 97

Berkelium (Bk)

actinide
Periode: 7 Blok: f

Solid

Bobot Atom Standar

[247]

Konfigurasi elektron

[Rn] 7s2 5f9

Titik lebur

1049,85 °C

Titik didih

Tidak tersedia

Massa jenis

1,4e+4 kg/m³

Bilangan oksidasi

+2, +3, +4, +5

Keelektronegatifan (Pauling)

1,3

Energi ionisasi (ke-1)

6,19785 eV

Tahun penemuan

1949

Jari-jari atom

Tidak tersedia

Detail

Asal nama Named after Berkeley, California the city of its discovery.
Negara penemuan United States
Penemu 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

Gambar

Sifat

Fisika

Jari-jari van der Waals
244 pm Bandingkan Jari-jari van der Waals semua unsur →
Massa jenis
1,4 × 104 kg/m³ Bandingkan Massa jenis semua unsur →
Fase pada STP
Padat Bandingkan Fase pada STP semua unsur →
Titik lebur
1049,85 °C Bandingkan Titik lebur semua unsur →

Kimia

Keelektronegatifan (Pauling)
1,3 Bandingkan Keelektronegatifan (Pauling) semua unsur →
Afinitas elektron
-0,5 eV (nilai negatif — atom tidak diprediksi mengikat elektron tambahan)
Energi ionisasi (ke-1)
6,19785 eV Bandingkan Energi ionisasi (ke-1) semua unsur →
Energi ionisasi (ke-2)
11,900041 eV Bandingkan Energi ionisasi (ke-2) semua unsur →
Energi ionisasi (ke-3)
21,600074 eV Bandingkan Energi ionisasi (ke-3) semua unsur →
Energi ionisasi (ke-4)
36,000124 eV Bandingkan Energi ionisasi (ke-4) semua unsur →
Energi ionisasi (ke-5)
56,000193 eV Bandingkan Energi ionisasi (ke-5) semua unsur →
Bilangan oksidasi
+2, +3, +4, +5 Bandingkan Bilangan oksidasi semua unsur →
Elektron valensi
3 Bandingkan Elektron valensi semua unsur →
Alotrop
["\u03b2 form"]
Konfigurasi elektron
[Rn] 7s2 5f9

Termodinamika

Kalor sublimasi
3,938436 eV
Kalor atomisasi
3,938436 eV
Entalpi atomisasi
3,212935 eV

Nuklir

Proton
97 Bandingkan Proton semua unsur →
Neutron
150 Bandingkan Neutron semua unsur →
Isotop yang diketahui
22 Bandingkan Isotop yang diketahui semua unsur →
Isotop stabil
0 Bandingkan Isotop stabil semua unsur →
Nomor massa (paling stabil)
247
Isotop paling stabil
Bk-247
Tahun penemuan
1949

Kelimpahan

Tidak tersedia

Struktur Kristal

Tidak tersedia

Struktur Elektronik

Elektron per kulit
2, 8, 18, 32, 27, 8, 2 Bandingkan Elektron per kulit semua unsur →

Pengenal

Nomor CAS
7440-40-6 Bandingkan Nomor CAS semua unsur →
Simbol term
6H°15/2
InChI
InChI=1S/Bk
Kunci InChI
PWVKJRSRVJTHTR-UHFFFAOYSA-N

Konfigurasi Elektron Diukur

Muatan ion
Proton 97
Elektron 97
Muatan Netral
Konfigurasi Bk: 5f⁹ 7s²
Konfigurasi elektron
Diukur
[Rn] 5f⁹ 7s²
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f⁹ 7s²
Diagram orbital
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 elektron: 97 Tidak berpasangan: 5 ?

Model atom

Proton 97
Neutron 152
Elektron 97
Nomor massa 249
Kestabilan Radioaktif

Isotop mengubah jumlah neutron, massa, dan kestabilan — bukan konfigurasi elektron atom netral.

Model atom skematis, tidak sesuai skala.

Sidik Jari Atom

Spektrum Emisi / Absorpsi

0 / 0 (0 0 dengan intensitas)
Diukur
Emisi Tampak: 380–750 nm

Distribusi Isotop

Tidak memiliki isotop stabil.

Nomor massaMassa atom (u)Kelimpahan alamiWaktu paruh
249 Radioaktif249,0749877 ± 0,0000027Tidak tersedia327.2 hari
239 Radioaktif239,05824 ± 0,00022Tidak tersedia100 detik
253 Radioaktif253,08688 ± 0,00039Tidak tersedia60 menit
251 Radioaktif251,080762 ± 0,000012Tidak tersedia55.6 menit
233 Radioaktif233,056652 ± 0,00025Tidak tersedia40 detik
Diukur

Fase / Wujud

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

Alasan: 1024,8 °C di bawah titik sublimasi (1049,85 °C)

Titik sublimasi 1049,85 °C
0 K Suhu saat ini: 25 °C 6000 K
Linimasa fase

Skematis, tidak sesuai skala

Padat
Gas
Sublimasi
25°C
Padat
Cair
Gas
Saat ini

Titik transisi fase

Titik sublimasi Literatur
1049,85 °C
Fase saat ini Dihitung
Padat

Energi transisi

Kalor sublimasi Literatur
3,938436 eV

Energi yang diperlukan untuk menyublimkan 1 mol pada titik sublimasi

Massa jenis

Massa jenis referensi Literatur
1,4e+4 kg/m³

Pada kondisi standar

Massa jenis saat ini Dihitung
1,4e+4 kg/m³

Pada kondisi standar

Spektrum Atom

Menampilkan 10 dari 97. Diurutkan berdasarkan muatan ion (menaik).

Data Garis Spektrum ?

IonMuatanTotal garisProbabilitas transisiPenamaan tingkat energi
Bk I 012000
Bk II +14800
Data Garis Spektrum NIST →

Data Tingkat Energi ?

IonMuatanTingkat energi
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
Data Tingkat Energi NIST →
97 Bk 247

Berkelium — Visualisasi Orbital Atom

[Rn]7s25f9
Tingkat energi 2 8 18 32 27 8 2
Bilangan oksidasi +2, +3, +4, +5
HOMO 5f n=5 · l=3 · m=-3
Berkelium — Pratinjau Visualisasi Orbital Atom
Three.js hanya dimuat saat diminta
97 Bk 247

Berkelium — Visualisasi Struktur Kristal

Data struktur kristal tidak tersedia

Jari-jari Ion

MuatanKoordinasiSpinJari-jari
+36Tidak tersedia96 pm
+39Tidak tersedia113.7 pm
+46Tidak tersedia83 pm
+48Tidak tersedia93 pm

Senyawa

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

Isotop (5)

Nomor massaMassa atom (u)Kelimpahan alamiWaktu paruhMode peluruhan
249 Radioaktif249,0749877 ± 0,0000027Tidak tersedia327.2 hari
β- ≈100%α =0.00145±0.8%SF =47e-9±0.2%
239 Radioaktif239,05824 ± 0,00022Tidak tersedia100 detik
β+ ≈100%α<0.01% SF<0.01%
253 Radioaktif253,08688 ± 0,00039Tidak tersedia60 menit
β- ?
251 Radioaktif251,080762 ± 0,000012Tidak tersedia55.6 menit
β- =100%
233 Radioaktif233,056652 ± 0,00025Tidak tersedia40 detik
α ≈82%β+ ?
249 Radioaktif
Massa atom (u) 249,0749877 ± 0,0000027
Kelimpahan alami Tidak tersedia
Waktu paruh 327.2 hari
Mode peluruhan
β- ≈100%α =0.00145±0.8% +1
239 Radioaktif
Massa atom (u) 239,05824 ± 0,00022
Kelimpahan alami Tidak tersedia
Waktu paruh 100 detik
Mode peluruhan
β+ ≈100%α<0.01% +1
253 Radioaktif
Massa atom (u) 253,08688 ± 0,00039
Kelimpahan alami Tidak tersedia
Waktu paruh 60 menit
Mode peluruhan
β- ?
251 Radioaktif
Massa atom (u) 251,080762 ± 0,000012
Kelimpahan alami Tidak tersedia
Waktu paruh 55.6 menit
Mode peluruhan
β- =100%
233 Radioaktif
Massa atom (u) 233,056652 ± 0,00025
Kelimpahan alami Tidak tersedia
Waktu paruh 40 detik
Mode peluruhan
α ≈82%β+ ?

Sifat Lanjutan

Jari-jari Kovalen (Lanjutan)

Jari-jari kovalen (Pyykkö)
168 pm
Jari-jari kovalen (Pyykkö, ikatan rangkap dua)
139 pm

Jari-jari van der Waals

Alvarez
340 pm
UFF
333,9 pm

Skala Penomoran

Mendeleev
30
Pettifor
40
Glawe
41

Skala Keelektronegatifan

Ghosh
0

Polarizabilitas & Dispersi

Polarizabilitas dipol
125 a.u.
Polarizabilitas dipol (ketidakpastian)
25 a.u.

Transisi Fase & Alotrop

β form
Titik lebur1259,15 K

Kategori Bilangan Oksidasi

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

Data Referensi Lanjutan

Detail Jari-jari Kristal (4)
MuatanCNSpinrcrystal (pm)Asal
3VI110from r^3 vs V plots,
4VI97from r^3 vs V plots,
4VIII107from r^3 vs V plots,
3IX—127,7
Mode Peluruhan Isotop (46)
IsotopModeIntensitas
233A82%
233B+—
234A80%
234B+20%
235B+—
235A—
236B+100%
236A—
236B+SF0%
237B+—

Data Tambahan

Referensi

(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.

Catatan lisensi: 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/

Catatan lisensi: 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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