Berkelium (Bk)
actinideSolid
Peso atomico standard
[247]Configurazione elettronica
[Rn] 7s2 5f9Punto di fusione
1049,85 °CPunto di ebollizione
N/DDensità
1,4e+4 kg/m³Stati di ossidazione
+2, +3, +4, +5Elettronegatività (Pauling)
1,3Energia di ionizzazione (1ª)
6,19785 eVAnno della scoperta
1949Raggio atomico
N/DDettagli
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
Fresh berkelium metal has been reported as a silvery actinide metal, but only very small samples have been prepared. It oxidizes readily in air, and most practical observations involve compounds or solutions rather than bulk metal pieces.
Berkelium has no commercial use. Its principal value is in actinide chemistry, nuclear-structure studies, and preparation of targets for heavy-element synthesis. ²⁴⁹Bk was used as the target material in experiments that produced element 117, now named tennessine. Small amounts also serve as tracers or sources in specialized studies of transplutonium separations, redox chemistry, and radiation effects, where its behavior helps compare the later actinides.
It has no significant commercial applications.
Berkelium most often forms Bk³⁺ salts, broadly resembling other trivalent actinides and lanthanides. The +4 state is unusually important for this part of the actinide series and appears in compounds such as berkelium dioxide, BkO₂, and in oxidized aqueous complexes. Representative trivalent compounds include berkelium(III) chloride, BkCl₃, berkelium(III) fluoride, BkF₃, and berkelium(III) oxide, Bk₂O₃. Berkelium(IV) fluoride, BkF₄, is known, but the chemistry is constrained by radioactivity, scarcity, and self-irradiation of samples.
See more information at the Berkelium compound page.
All berkelium isotopes are radioactive, and hazards depend strongly on isotope, chemical form, and activity. ²⁴⁹Bk decays mainly by beta emission but also produces daughter nuclides that can add radiological complications. Inhalation, ingestion, or wound contamination by soluble or finely divided berkelium compounds would be serious internal exposure risks. Work is confined to shielded radiochemical facilities with contamination control.
Berkelium has no significant natural environmental cycle. Any environmental presence is artificial and associated with nuclear-weapons debris, reactor materials, or accidental releases, generally at extremely low levels compared with more abundant actinides. In soils and waters it would be expected to behave as a particle-reactive trivalent or tetravalent actinide, with mobility controlled by oxidation state, complexing ligands, colloids, and sorption to minerals.
Berkelium is not a traded commodity and has no ordinary industrial supply chain. Usable amounts are made by prolonged neutron irradiation of curium, americium, or plutonium targets in high-flux reactors, followed by demanding radiochemical separation from a mixture of transplutonium elements and fission products. Production is episodic, expensive in facility time, and limited by isotope decay, target availability, and the need for specialized hot-cell handling. Recycling is possible only within research programs that recover residues from targets or separations.
Some compounds have been made and studied. Made by bombarding americium with alpha particles.
Berkelium is not a primordial cosmic element because all of its known isotopes are too short-lived on geological and astronomical time scales. It can be formed transiently in intense neutron-capture environments, but it decays before it can accumulate. Any extraterrestrial berkelium would be temporary and detectable only as part of recent nuclear processes, not as a stable planetary constituent.
- Berkelium was first identified in 1949 at Berkeley, California.
- The isotope ²⁴⁹Bk is favored for research because it is long-lived enough to handle but still highly radioactive.
- Berkelium helped make the first confirmed atoms of tennessine.
- The accessible +4 state distinguishes berkelium from several neighboring transplutonium elements.
- Self-irradiation can damage berkelium solids and complicate measurements on stored samples.
Immagini
Proprietà
Fisiche
- Raggio di van der Waals
- 244 pm Confronta Raggio di van der Waals di tutti gli elementi →
- Densità
- 1,4 × 104 kg/m³ Confronta Densità di tutti gli elementi →
- Fase in condizioni STP
- Solido Confronta Fase in condizioni STP di tutti gli elementi →
- Punto di fusione
- 1049,85 °C Confronta Punto di fusione di tutti gli elementi →
Chimiche
- Elettronegatività (Pauling)
- 1,3 Confronta Elettronegatività (Pauling) di tutti gli elementi →
- Affinità elettronica
- -0,5 eV (valore negativo — l'atomo non dovrebbe legare un elettrone extra)
- Energia di ionizzazione (1ª)
- 6,19785 eV Confronta Energia di ionizzazione (1ª) di tutti gli elementi →
- Energia di ionizzazione (2ª)
- 11,900041 eV Confronta Energia di ionizzazione (2ª) di tutti gli elementi →
- Energia di ionizzazione (3ª)
- 21,600074 eV Confronta Energia di ionizzazione (3ª) di tutti gli elementi →
- Energia di ionizzazione (4ª)
- 36,000124 eV Confronta Energia di ionizzazione (4ª) di tutti gli elementi →
- Energia di ionizzazione (5ª)
- 56,000193 eV Confronta Energia di ionizzazione (5ª) di tutti gli elementi →
- Stati di ossidazione
- +2, +3, +4, +5 Confronta Stati di ossidazione di tutti gli elementi →
- Elettroni di valenza
- 3 Confronta Elettroni di valenza di tutti gli elementi →
- Allotropi
- ["\u03b2 form"]
- Configurazione elettronica
- [Rn] 7s2 5f9
Termodinamiche
- Calore di sublimazione
- 3,938436 eV
- Calore di atomizzazione
- 3,938436 eV
- Entalpia di atomizzazione
- 3,212935 eV
Nucleari
- Protoni
- 97 Confronta Protoni di tutti gli elementi →
- Neutroni
- 150 Confronta Neutroni di tutti gli elementi →
- Isotopi noti
- 22 Confronta Isotopi noti di tutti gli elementi →
- Isotopi stabili
- 0 Confronta Isotopi stabili di tutti gli elementi →
- Numero di massa (isotopo più stabile)
- 247
- Isotopo più stabile
- Bk-247
- Anno della scoperta
- 1949
Abbondanza
N/D
Struttura cristallina
N/D
Struttura elettronica
- Elettroni per guscio
- 2, 8, 18, 32, 27, 8, 2 Confronta Elettroni per guscio di tutti gli elementi →
Identificativi
- Numero CAS
- 7440-40-6 Confronta Numero CAS di tutti gli elementi →
- Simbolo di termine
- 6H°15/2
- InChI
- InChI=1S/Bk
- Chiave InChI
- PWVKJRSRVJTHTR-UHFFFAOYSA-N
Configurazione elettronica Misurato
Bk: 5f⁹ 7s²[Rn] 5f⁹ 7s²1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f⁹ 7s²Modello atomico
Gli isotopi modificano il numero di neutroni, la massa e la stabilità — non la configurazione elettronica di un atomo neutro.
Modello atomico schematico, non in scala.
Impronta atomica
Spettro di emissione / assorbimento
Distribuzione isotopica
Nessun isotopo stabile.
| Numero di massa | Massa atomica (u) | Abbondanza naturale | Emivita |
|---|---|---|---|
| 249 Radioattivo | 249,0749877 ± 0,0000027 | N/D | 327.2 giorni |
| 239 Radioattivo | 239,05824 ± 0,00022 | N/D | 100 secondi |
| 253 Radioattivo | 253,08688 ± 0,00039 | N/D | 60 minuti |
| 251 Radioattivo | 251,080762 ± 0,000012 | N/D | 55.6 minuti |
| 233 Radioattivo | 233,056652 ± 0,00025 | N/D | 40 secondi |
Fase / Stato
Motivo: 1024,8 °C sotto il punto di sublimazione (1049,85 °C)
Schema non in scala
Punti di transizione di fase
Energie di transizione
Energia necessaria per sublimare 1 mol al punto di sublimazione
Densità
In condizioni standard
In condizioni standard
Spettri atomici
Sono visualizzati 10 di 97. Ordinamento per carica ionica crescente.
Righe disponibili ?
| Ione | Carica | Righe totali | Probabilità di transizione | Designazioni dei livelli |
|---|---|---|---|---|
| Bk I | 0 | 120 | 0 | 0 |
| Bk II | +1 | 48 | 0 | 0 |
Livelli disponibili ?
| Ione | Carica | Livelli |
|---|---|---|
| Bk I | 0 | 2 |
| Bk II | +1 | 2 |
| Bk III | +2 | 2 |
| Bk IV | +3 | 2 |
| Bk V | +4 | 2 |
| Bk VI | +5 | 2 |
| Bk VII | +6 | 2 |
| Bk VIII | +7 | 2 |
| Bk IX | +8 | 2 |
| Bk X | +9 | 2 |
Dati sulla struttura cristallina non disponibili
Raggi ionici
| Carica | Coordinazione | Spin | Raggio |
|---|---|---|---|
| +3 | 6 | N/D | 96 pm |
| +3 | 9 | N/D | 113.7 pm |
| +4 | 6 | N/D | 83 pm |
| +4 | 8 | N/D | 93 pm |
Composti
Isotopi (5)
| Numero di massa | Massa atomica (u) | Abbondanza naturale | Emivita | Modalità di decadimento | |
|---|---|---|---|---|---|
| 249 Radioattivo | 249,0749877 ± 0,0000027 | N/D | 327.2 giorni | β- ≈100%α =0.00145±0.8%SF =47e-9±0.2% | |
| 239 Radioattivo | 239,05824 ± 0,00022 | N/D | 100 secondi | β+ ≈100%α<0.01% SF<0.01% | |
| 253 Radioattivo | 253,08688 ± 0,00039 | N/D | 60 minuti | β- ? | |
| 251 Radioattivo | 251,080762 ± 0,000012 | N/D | 55.6 minuti | β- =100% | |
| 233 Radioattivo | 233,056652 ± 0,00025 | N/D | 40 secondi | α ≈82%β+ ? |
Proprietà estese
Raggi covalenti (dati estesi)
- Raggio covalente (Pyykkö)
- 168 pm
- Raggio covalente (Pyykkö, legame doppio)
- 139 pm
Raggi di van der Waals
- Alvarez
- 340 pm
- UFF
- 333,9 pm
Scale di numerazione
- Mendeleev
- 30
- Pettifor
- 40
- Glawe
- 41
Scale di elettronegatività
- Ghosh
- 0
Polarizzabilità e dispersione
- Polarizzabilità dipolare
- 125 a.u.
- Polarizzabilità dipolare (inc.)
- 25 a.u.
Transizioni di fase e allotropi
| Punto di fusione | 1259,15 K |
Categorie degli stati di ossidazione
Dati di riferimento avanzati
Dettaglio dei raggi cristallini (4)
| Carica | CN | Spin | rcrystal (pm) | Origine |
|---|---|---|---|---|
| 3 | VI | 110 | from r^3 vs V plots, | |
| 4 | VI | 97 | from r^3 vs V plots, | |
| 4 | VIII | 107 | from r^3 vs V plots, | |
| 3 | IX | — | 127,7 |
Modalità di decadimento degli isotopi (46)
| Isotopo | Modalità | Intensità |
|---|---|---|
| 233 | A | 82% |
| 233 | B+ | — |
| 234 | A | 80% |
| 234 | B+ | 20% |
| 235 | B+ | — |
| 235 | A | — |
| 236 | B+ | 100% |
| 236 | A | — |
| 236 | B+SF | 0% |
| 237 | B+ | — |
Dati aggiuntivi
Estimated Crustal Abundance
The estimated element abundance in the earth's crust.
Not Applicable
Riferimenti (1)
- [5] Berkelium https://education.jlab.org/itselemental/ele097.html
Estimated Oceanic Abundance
The estimated element abundance in the earth's oceans.
Not Applicable
Riferimenti (1)
- [5] Berkelium https://education.jlab.org/itselemental/ele097.html
Riferimenti
(9)
Data deposited in or computed by PubChem
The half-life and atomic mass data was provided by the Atomic Mass Data Center at the International Atomic Energy Agency.
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.
The information are cited from Pure Appl. Chem. 2018; 90(12): 1833-2092, https://doi.org/10.1515/pac-2015-0703.
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/
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.
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
This section provides all form of data related to element Berkelium.
The element property data was retrieved from publications.
