Protactinium (Pa)
actinideSolid
Masse atomique relative standard
231,03588 uConfiguration électronique
[Rn] 7s2 5f2 6d1Point de fusion
1571,85 °CPoint d’ébullition
N/DMasse volumique
1,537e+4 kg/m³États d’oxydation
+2, +3, +4, +5Électronégativité (Pauling)
1,5Énergie d’ionisation (1re)
5,89 eVAnnée de découverte
1913Rayon atomique
180 pmDétails
Protactinium is a dense, silvery actinide metal with atomic number 91. It lies between thorium and uranium and is chemically notable for the stability of the +5 oxidation state, although +4 compounds are also known. All isotopes are radioactive. Natural protactinium occurs only in trace amounts, chiefly as ²³¹Pa in the ²³⁵U decay series and as short-lived products in other decay chains, so it has little technological role outside nuclear and geochemical research.
Protactinium metal is a dense, silvery-gray material with a bright metallic luster which it retains for some time in air but it does readily react with oxygen, water vapor and inorganic acids to form various compounds. In solid compounds protactinium is most stable in the oxidation state +5, but it also exists in the +4, +3 and +2 oxidation states. In solution the +5 state rapidly hydrolyzes by combining with hydroxide ions to form soluble or insoluble hydroxy-oxide solids which have a tendency to stick to the surfaces of vessels in which it is contained. A number of protactinium compounds are known, some of which are colored. The element is superconductive below 1.4K.
The name derives from the Greek protos (first) for preceding the element actinium, because its most common isotope (231Pa) decays to 227Ac by loss of an alpha particle.
In 1913 the German chemists K. Fajans and O. H. Gohring identified the first isotope of protactinium, 234Pa, and proposed the name brevium because of that isotope's short half-life of 6.7 h. 231Pa, with a longer half-life of 3.25(1)×104 a, was identified in 1918 by the German chemist O. Hahn and the Austrian physicist L. Meitner; and, independently in Britain, by F. Soddy and J. A. Cranston.
Protactinium was first identified by Kasimir Fajans and O.H. Göhring in 1913 while studying uranium's decay chain. The particular isotope they found, protactinium-234m, has a half-life of about 1.17 minutes. They named the element brevium, meaning brief, and then continued with their studies. Protactinium's existence was confirmed in 1918 when another isotope, protactinium-231, was independently discovered and studied by two groups of scientists, Otto Hahn and Lise Meitner of Germany and Frederick Soddy and John Cranston of Great Britain. Protactinium was first isolated by Aristid V. Grosse in 1934. Protactinium is a rare, poisonous and expensive element that is present in uranium ores in very small amounts. In 1961, the Great Britain Atomic Energy Authority was able to produce 125 grams of 99.9% pure protactinium, although they had to process about 55,000 kilograms of ore and spend about $500,000 to get it.
Protactinium's most stable isotope, protactinium-231, has a half-life of about 32,760 years. It decays into actinium-227 through alpha decay.
The name "protactinium" comes from adding the Greek protos meaning first, before the word "actinium." In 1871, Dmitri Mendeleevpredicted the existence of an element between thorium and uranium. In 1900, William Crookes isolated protactinium from uraniu. It was an intensely radioactive material, however, he could not characterize it as a new chemical element and thus named it uranium-X. In 1913 the first isotope of element 91, 234Pa, was discovered by K. Fajans and O.H. Gohring. It was a very short-lived member of the naturally occurring 238U decay series and as such they named it "brevium." In 1917/18, two groups of scientists, Otto Hahn and Lise Meitner of Germany and Frederick Soddy and John Cranston of Great Britain, independently discovered another isotope of protactinium, 231Pa having much longer half-life of about 32,000 years. The name was changed to proto-actinium as being more consistent with the longer-lived characteristics of the most abundant isotope. In 1927, Grosse prepared 2 mg of a white powder, which was shown to be Pa2O5. In 1934 he isolated the element from 0.1 g of pure Pa2O5 by two methods, one of which was by converting the oxide to an iodide and "cracking" it in a high vacuum by an electrically heated filament by the reaction: 2PaI5 > 2Pa + 5I2. In 1949, the name protoactinium was shortened by the IUPAC who officially named it protactinium and confirmed Hahn and Meitner as co-discoverers. The new name meant "parent of actinium" and reflected the fact that actinium is a decay product of the radioactive decay of protactinium.
Fresh protactinium metal has been reported as a bright, silvery-gray solid. Macroscopic samples are extremely rare because of radioactivity, scarcity, and self-heating from decay. The metal tarnishes in air and is normally handled only in specialized radiochemical facilities.
Protactinium has no significant commercial use. Its main applications are scientific: ²³¹Pa is used in geochemistry and paleoceanography, especially with thorium isotopes, to study particle scavenging and past ocean circulation. Protactinium has also been investigated in nuclear chemistry because ²³³Pa is an intermediate in the breeding of ²³³U from ²³²Th. Such work is primarily research or process-control chemistry rather than a use of the element as a bulk material.
Due to its scarcity, high radioactivity and toxicity, there are currently no uses for protactinium outside of basic scientific research.
Because of its scarcity, high radioactivity and high toxicity, there are currently no practical uses for protactinium other than that of basic scientific research, and for this purpose, protactinium is generally extracted from spent nuclear fuel.
Isotopes in Earth/Planetary Science
231Pa (with a half-life of 3.25×104 years) and 230Th (with a half-life of 7.56×104 years) are produced in seawater by radioactive decay of 235U and 234U. The amount ratio of radioactive production of 231Pa and 230Th, n(231Pa)/n(230Th), is 0.093. 230Th is removed from seawater in settling particulates more efficiently than 231Pa, while 231Pa tends to be transported farther in ocean currents. Therefore, the amount ratio n(231Pa)/n(230Th) in settling particulates tends to be less than the production ratio of 0.093 unless the water mass is stationary and allows both products to settle out. Thus, sedimentary records of excess n(231Pa)/n(230Th) amount ratios can provide information for changes in the relative magnitude of major ocean circulation (Fig. IUPAC.91.1) [593] K. A. Roberts, C. Xu, C. C. Hung, M. H. Conte, P. H. Santschi. Earth. Planet. Sci. Lett.286, 131 (2009)., [594] J. F. McManus, R. Francois, J. M. Gherardi, L. D. Keigwin, S. Brown-Leger. Nature428, 834 (2004)..
Isotopes in Geochronology
231Pa is a natural radiogenic isotope produced by alpha decay of 235U to 231Th, followed by beta emission to form 231Pa. Although its behavior in the environment as a transient member of the U-series decay chain may be complex, measurements and modeling of 231Pa in relation to the isotopes of uranium and thorium have been used in a variety of geochronologic applications on time scales of 103 to 105 years [596] H. Cheng, R. L. Edwards, M. T. Murrell, T. M. Benjamin. Geochim. Cosmochim. Acta62 (21-22), 3437 (1998)., [597] R. L. Edwards, C. D. Gallup, H. Cheng. Rev. Mineral. Geochem.52, 363 (2003).. Studies include movement of water masses and particles in the oceans, rates of magma melting and movement beneath volcanoes, and ages of carbonate mineral deposits, including corals, in relation to climate change.
Protactinium chemistry is dominated by Pa(V), which readily forms oxo and halide complexes and is strongly hydrolyzed in aqueous solution. Protactinium(V) oxide, Pa₂O₅, is a representative oxide, and protactinium(IV) oxide, PaO₂, is also known. Halides include protactinium(V) chloride, PaCl₅, protactinium(IV) chloride, PaCl₄, protactinium(V) fluoride, PaF₅, and protactinium(IV) fluoride, PaF₄. In water, polymeric and adsorbed species complicate simple speciation.
See more information at the Protactinium compound page.
Protactinium is hazardous because all of its isotopes are radioactive and because actinide compounds can be retained in the body if inhaled or ingested. ²³¹Pa has a long half-life and emits alpha radiation with associated decay products. External exposure, contamination spread, and internal uptake are the main practical concerns. Handling requires radiochemical containment, shielding appropriate to the isotope mixture, and strict contamination control.
Natural protactinium is produced continuously in uranium-bearing minerals and sediments by radioactive decay. It is present at very low concentrations and is not known to have a biological role. In seawater, protactinium is particle-reactive and is removed to sediments more readily than uranium but differently from thorium, making its distribution useful as a tracer. Human releases are generally limited to nuclear and laboratory contexts.
Protactinium has no commodity market. It is one of the rarest naturally occurring elements that can be isolated, and gram-scale work is exceptional. Historically, ²³¹Pa has been recovered from uranium-processing residues or from materials in the actinium decay series, but separation is difficult because of intense radioactivity, low concentration, and complex aqueous chemistry. Supply is therefore institutional and research-driven, with substitution usually meaning avoidance of protactinium rather than replacement in a product.
Protactinium is one of the rarest and most expensive naturally occurring elements. The average concentrations of protactinium in the Earth's crust is typically on the order of a few parts per trillion, but may reach up to a few parts per million in some uraninite ore deposits. The element occurs in pitchblende to the extent of about 1 part 231Pa to 10 million parts of ore. Ores from Zaire have about 3 ppm. In 1959 and 1961, it was announced that the Great Britain Atomic Energy Authority extracted by a 12-stage process 125 g of 99.9% protactinium, the world's only stock of the metal for many years following. The extraction was made from 60 tons of waste material at a cost of about $500,000.
Protactinium is cosmically scarce because it has no stable isotopes. Any primordial protactinium has long since decayed. In nature it is mainly a transient daughter in uranium and thorium decay chains, so its abundance follows the presence of those long-lived actinides. It may be produced in small amounts by neutron-capture and decay processes in stellar or explosive nucleosynthesis, but it does not accumulate on astronomical timescales.
- The name refers to its position as the parent of actinium in the decay chain.
- ²³¹Pa has a half-life of about 32,760 years, long enough for environmental tracing but short on geologic timescales.
- Protactinium was once called protoactinium; the spelling was later shortened.
- Its aqueous chemistry is unusually difficult because Pa(V) hydrolyzes and adsorbs strongly to surfaces.
- ²³³Pa is important in thorium fuel-cycle chemistry because it decays to fissile ²³³U.
Images
Propriétés
Propriétés physiques
- Rayon atomique (empirique)
- 180 pm Comparer : Rayon atomique (empirique) de tous les éléments →
- Rayon covalent
- 200 pm Comparer : Rayon covalent de tous les éléments →
- Rayon de van der Waals
- 243 pm Comparer : Rayon de van der Waals de tous les éléments →
- Masse volumique
- 1,537 × 104 kg/m³ Comparer : Masse volumique de tous les éléments →
- Volume molaire
- 0,015 L/mol
- Phase aux CNTP
- Solide Comparer : Phase aux CNTP de tous les éléments →
- Point de fusion
- 1571,85 °C Comparer : Point de fusion de tous les éléments →
- Structure cristalline
- Quadratique Comparer : Structure cristalline de tous les éléments →
Propriétés chimiques
- Électronégativité (Pauling)
- 1,5 Comparer : Électronégativité (Pauling) de tous les éléments →
- Affinité électronique
- 0,123 eV
- Énergie d’ionisation (1re)
- 5,89 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)
- 18,600064 eV Comparer : Énergie d’ionisation (3e) de tous les éléments →
- Énergie d’ionisation (4e)
- 30,900106 eV Comparer : Énergie d’ionisation (4e) de tous les éléments →
- Énergie d’ionisation (5e)
- 44,300152 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 →
- Configuration électronique
- [Rn] 7s2 5f2 6d1
Propriétés thermodynamiques
- Enthalpie de fusion
- 0,15546458 eV Comparer : Enthalpie de fusion de tous les éléments →
- Enthalpie de vaporisation
- 4,974867 eV Comparer : Enthalpie de vaporisation de tous les éléments →
- Enthalpie de sublimation
- 6,291133 eV
- Enthalpie d’atomisation
- 6,291133 eV
- Enthalpie d’atomisation
- 5,835104 eV
Propriétés nucléaires
- Protons
- 91 Comparer : Protons de tous les éléments →
- Neutrons
- 140 Comparer : Neutrons de tous les éléments →
- Isotopes connus
- 31 Comparer : Isotopes connus de tous les éléments →
- Isotopes stables
- 0 Comparer : Isotopes stables de tous les éléments →
- Isotope le plus stable
- Pa-231
- Année de découverte
- 1913
Abondance
- Abondance (croûte terrestre)
- 1,4e-6 mg/kg Comparer : Abondance (croûte terrestre) de tous les éléments →
- Abondance (océan)
- 5 × 10−11 mg/L Comparer : Abondance (océan) de tous les éléments →
Structure cristalline
- Paramètre de maille a
- 392 pm
Structure électronique
- Électrons par couche
- 2, 8, 18, 32, 20, 9, 2 Comparer : Électrons par couche de tous les éléments →
Identifiants
- Numéro CAS
- 7440-13-3 Comparer : Numéro CAS de tous les éléments →
- Symbole de terme
- 4K11/2
- InChI
- InChI=1S/Pa
- Clé InChI
- XLROVYAPLOFLNU-UHFFFAOYSA-N
Configuration électronique Mesuré
Pa: 5f² 6d¹ 7s²[Rn] 5f² 6d¹ 7s²1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f² 6d¹ 7s²Modèle atomique
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
Distribution isotopique
Aucun isotope stable.
| Nombre de masse | Masse atomique (u) | Abondance naturelle | Demi-vie |
|---|---|---|---|
| 224 Radioactif | 224,0256176 ± 0,0000082 | N/D | 844 ms |
| 218 Radioactif | 218,020059 ± 0,00002 | N/D | 108 us |
| 216 Radioactif | 216,019109 ± 0,000057 | N/D | 105 ms |
| 219 Radioactif | 219,019904 ± 0,000055 | N/D | 56 ns |
| 227 Radioactif | 227,0288054 ± 0,000008 | N/D | 38.3 minutes |
Phase / État
Explication: 1546,8 °C en dessous du point de fusion (1571,85 °C)
Schématique, non à l’échelle
Points de transition de phase
Énergies de transition
Énergie nécessaire pour faire fondre 1 mol au point de fusion
Énergie nécessaire pour vaporiser 1 mol au point d’ébullition
Énergie nécessaire pour sublimer 1 mol au point de sublimation
Masse volumique
Dans les conditions standard
Dans les conditions standard
Spectres atomiques
Affichage de 10 sur 91. Tri par charge ionique croissante.
Raies répertoriées ?
| Ion | Charge | Nombre total de raies | Probabilités de transition | Désignations des niveaux |
|---|---|---|---|---|
| Pa I | 0 | 55 | 0 | 0 |
| Pa II | +1 | 33 | 0 | 0 |
Niveaux répertoriés ?
| Ion | Charge | Niveaux |
|---|---|---|
| Pa I | 0 | 2 |
| Pa II | +1 | 2 |
| Pa III | +2 | 2 |
| Pa IV | +3 | 2 |
| Pa V | +4 | 2 |
| Pa VI | +5 | 2 |
| Pa VII | +6 | 2 |
| Pa VIII | +7 | 2 |
| Pa IX | +8 | 2 |
| Pa X | +9 | 2 |
Rayons ioniques
| Charge | Coordinence | Spin | Rayon |
|---|---|---|---|
| +3 | 6 | N/D | 104 pm |
| +3 | 9 | N/D | 119.9 pm |
| +4 | 6 | N/D | 90 pm |
| +4 | 8 | N/D | 101 pm |
| +5 | 6 | N/D | 78 pm |
| +5 | 8 | N/D | 91 pm |
| +5 | 9 | N/D | 95 pm |
Composés
Isotopes (5)
Twenty-nine radioisotopes of protactinium have been discovered. Nearly all naturally occurring protactinium is 231Pa with a half-life of 32,700 years. It is an alpha emitter and is formed by the decay of uranium-235, whereas the beta radiating protactinium-234 with a half-life of 6.74 hours is produced as a result of uranium-238 decay. Nearly all uranium-238 (99.8%) decays first to the 234mPa isomer and then to 234Pa. Smaller trace amounts of the short-lived nuclear isomer protactinium-234m occur in the decay chain of uranium-238. Protactinium-233 results from the decay of thorium-233 as part of the chain of events used to produce uranium-233 by neutron irradiation of thorium-232.
| Nombre de masse | Masse atomique (u) | Abondance naturelle | Demi-vie | Mode de désintégration | |
|---|---|---|---|---|---|
| 224 Radioactif | 224,0256176 ± 0,0000082 | N/D | 844 ms | α ≈100%β+ ? | |
| 218 Radioactif | 218,020059 ± 0,00002 | N/D | 108 us | α =100% | |
| 216 Radioactif | 216,019109 ± 0,000057 | N/D | 105 ms | α ≈100%β+ ? | |
| 219 Radioactif | 219,019904 ± 0,000055 | N/D | 56 ns | α =100%β+ ? | |
| 227 Radioactif | 227,0288054 ± 0,000008 | N/D | 38.3 minutes | α =85±0.2%ε =15±0.2% |
Propriétés étendues
Rayons covalents (données étendues)
- Rayon covalent (Pyykkö)
- 169 pm
- Rayon covalent (Pyykkö, liaison double)
- 138 pm
- Rayon covalent (Pyykkö, liaison triple)
- 129 pm
Rayons de van der Waals
- Alvarez
- 288 pm
- UFF
- 342,4 pm
- MM3
- 264 pm
Rayons atomiques et métalliques
- Rayon atomique (Rahm)
- 285 pm
Échelles de numérotation
- Mendeleev
- 18
- Pettifor
- 46
- Glawe
- 35
Échelles d’électronégativité
- Ghosh
- 0
Polarisabilité et dispersion
- Polarisabilité dipolaire
- 154 a.u.
- Polarisabilité dipolaire (incertitude)
- 20 a.u.
Transitions de phase et allotropes
| Point de fusion | 1845,15 K |
Catégories d’états d’oxydation
Données de référence avancées
Détail des rayons cristallins (7)
| Charge | CN | Spin | rcrystal (pm) | Origine |
|---|---|---|---|---|
| 3 | VI | 118 | estimated, | |
| 4 | VI | 104 | from r^3 vs V plots, | |
| 4 | VIII | 115 | ||
| 5 | VI | 92 | ||
| 5 | VIII | 105 | ||
| 5 | IX | 109 | ||
| 3 | IX | — | 133,9 |
Modes de désintégration des isotopes (51)
| Isotope | Mode | Intensité |
|---|---|---|
| 211 | A | 100% |
| 211 | B+ | — |
| 211 | p | — |
| 212 | A | 100% |
| 213 | A | 100% |
| 214 | A | 100% |
| 215 | A | 100% |
| 216 | A | 100% |
| 216 | B+ | — |
| 217 | A | 100% |
Facteurs de diffusion des rayons X (516)
| Énergie (eV) | f₁ | f₂ |
|---|---|---|
| 10 | — | 1,75788 |
| 10,1617 | — | 1,76101 |
| 10,3261 | — | 1,76414 |
| 10,4931 | — | 1,76728 |
| 10,6628 | — | 1,73466 |
| 10,8353 | — | 1,69295 |
| 11,0106 | — | 1,65224 |
| 11,1886 | — | 1,61457 |
| 11,3696 | — | 1,58512 |
| 11,5535 | — | 1,5562 |
Données complémentaires
Estimated Crustal Abundance
The estimated element abundance in the earth's crust.
1.4×10-6 milligrams per kilogram
Références (1)
- [5] Protactinium https://education.jlab.org/itselemental/ele091.html
Estimated Oceanic Abundance
The estimated element abundance in the earth's oceans.
5×10-11 milligrams per liter
Références (1)
- [5] Protactinium https://education.jlab.org/itselemental/ele091.html
Sources
Sources of this element.
Protactinium is one of the rarest and most expensive naturally occurring elements. The average concentrations of protactinium in the Earth's crust is typically on the order of a few parts per trillion, but may reach up to a few parts per million in some uraninite ore deposits. The element occurs in pitchblende to the extent of about 1 part 231Pa to 10 million parts of ore. Ores from Zaire have about 3 ppm. In 1959 and 1961, it was announced that the Great Britain Atomic Energy Authority extracted by a 12-stage process 125 g of 99.9% protactinium, the world's only stock of the metal for many years following. The extraction was made from 60 tons of waste material at a cost of about $500,000.
Références (1)
- [6] Protactinium https://periodic.lanl.gov/91.shtml
Références
(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 Protactinium.
The element property data was retrieved from publications.

