Neptunium (Np)
actinideSolid
Bobot Atom Standar
[237]Konfigurasi elektron
[Rn] 7s2 5f4 6d1Titik lebur
643,85 °CTitik didih
3901,85 °CMassa jenis
2,025e+4 kg/m³Bilangan oksidasi
+2, +3, +4, +5, +6, +7Keelektronegatifan (Pauling)
1,36Energi ionisasi (ke-1)
6,265608 eVTahun penemuan
1940Jari-jari atom
175 pmDetail
Neptunium is a radioactive actinide and the first transuranium element. It is produced mainly by neutron reactions involving uranium in nuclear reactors and occurs naturally only in minute amounts from neutron capture and decay processes in uranium ores. Its chemistry bridges uranium and plutonium, with several accessible oxidation states in solution. The isotope ²³⁷Np is the most important for handling and study because of its long half-life and availability as a reactor by-product.
Neptunium metal buttons (photo courtesy Lawrence Berkeley National Laboratory)
Neptunium was first produced by Edwin M. McMillian and Philip H. Abelson, working at the University of California, Berkeley, in 1940. They produced neptunium-239, an isotope of neptunium with a half-life of about 2.4 days, by bombarding uranium with slow moving neutrons.
Named for the planet Neptune (named after the Roman god of the sea), the next planet out from the Sun after Uranus. There were many early false reports of the discovery of neptunium. The most significant was by Enrico Fermi who believed that bombarding uranium with neutrons followed by beta decay would lead to the formation of element 93. In 1934, he bombarded uranium atoms with neutrons and reported that he had produced elements 93 and 94. As it turned out, Fermi had actually fissioned or split uranium atoms into many fragment radioisotopes. The explanation and announcement of the discovery of fission was later published by Hahn and Strassman, although it was their co-worker Lisa Meitner who had correctly interpreted the results of the experiments. In 1940, with excitement about fission reaching the University of California at Berkeley, Professor Edwin McMillan and graduate student Philip Abelson bombarded uranium with cyclotron-produced moderated (slow) neutrons, resulting not in “fission” but "fusion" of the reactants forming the new element 93, which they named "neptunium":
23892U + 10n → 23992U → 23993Np + β-
Neptunium-239 was the first transuranium element produced synthetically and the first actinide series transuranium element discovered. This isotope has a beta-decay half-life of 2.3565 days, which forms daughter product plutonium-239 with a half-life of 24,000 years.
Metallic neptunium has been prepared in visible quantities. Fresh metal is silvery, dense, and chemically reactive, but it tarnishes in air as oxide layers form. It has several solid allotropes, and bulk physical measurements are limited by radioactivity, scarcity, and self-heating.
Neptunium has no broad commercial use as an element. ²³⁷Np is used in research on actinide chemistry, nuclear fuel cycles, and long-lived radioactive waste behavior. It is also the principal target material for producing ²³⁸Pu by neutron irradiation; ²³⁸Pu is then used in radioisotope heat sources and power systems. Small quantities of neptunium compounds have been used as analytical standards and in radiochemical method development.
Neptunium's most stable isotope, neptunium-237, has a half-life of about 2,144,000 years. It decays into protactinium-233 through alpha decay. Neptunium-237, which is produced in gram quantities as a by-product of the production of plutonium in nuclear reactors, is used in neutron detectors.
Once considered to be completely artificial, extremely small amounts of neptunium are produced naturally in uranium ores through the interaction of atoms of uranium in the ore with neutrons produced by the decay of other atoms of uranium in the ore.
Isotopes in Industry
237Np (with a half-life of 2.14×106 years) is fissionable, meaning that neptunium can be bombarded with neutrons and, as a result, create more neutrons that are free to interact with nearby material and can be used in fast neutron reactors or in nuclear weapons (Fig. IUPAC.93.1) [75] J. Peterson, M. McDonell, L. Haroun, F. Monette, R. D. Hildebrand, A. Taboas. Radiological and Chemical Fact Sheets to Support Health Risk Analyses for Contaminated Areas, Prepared by Argonne National Laboratory Environmental Science Division in collaboration with U.S. Department of Energy, Richland Operations Office and Chicago Operations Office (2014), Feb. 22; http://www.remm.nlm.gov/ANL_ContaminantFactSheets_All_070418.pdf., [603] P. Weiss. Science News.162, 259 (2002)., [604] T. Kenna. J. Anal. At. Spectrom.17, 1471 (2002).. 237Np is used in neutron detection instruments [75] J. Peterson, M. McDonell, L. Haroun, F. Monette, R. D. Hildebrand, A. Taboas. Radiological and Chemical Fact Sheets to Support Health Risk Analyses for Contaminated Areas, Prepared by Argonne National Laboratory Environmental Science Division in collaboration with U.S. Department of Energy, Richland Operations Office and Chicago Operations Office (2014), Feb. 22; http://www.remm.nlm.gov/ANL_ContaminantFactSheets_All_070418.pdf..
Isotopes Used as a Source of Radioactive Isotope(s)
237Np is used in the production of 238Pu (with a half-life of 87.7 years), which is an emitter of alpha particles used in thermoelectric generators and radioisotope-heater units. When 237Np captures a neutron, it becomes 238Np, with a half-life of 2.117 days, which decays to 238Pu [75] J. Peterson, M. McDonell, L. Haroun, F. Monette, R. D. Hildebrand, A. Taboas. Radiological and Chemical Fact Sheets to Support Health Risk Analyses for Contaminated Areas, Prepared by Argonne National Laboratory Environmental Science Division in collaboration with U.S. Department of Energy, Richland Operations Office and Chicago Operations Office (2014), Feb. 22; http://www.remm.nlm.gov/ANL_ContaminantFactSheets_All_070418.pdf..
Neptunium forms compounds in oxidation states from +3 to +7, with +4, +5, and +6 especially important in aqueous chemistry. The neptunyl ion NpO₂⁺ is a characteristic +5 species and is often relatively mobile in oxidizing waters, while NpO₂²⁺ represents +6 chemistry. Neptunium dioxide NpO₂ is a stable refractory oxide and an important solid phase. Halides such as neptunium tetrachloride NpCl₄ and neptunium hexafluoride NpF₆ illustrate the element’s actinide-like coordination and redox behavior.
See more information at the Neptunium compound page.
All neptunium isotopes are radioactive, and hazards depend strongly on isotope, chemical form, and exposure route. ²³⁷Np emits mainly alpha radiation with associated gamma emissions from decay products, so ingestion, inhalation, or contamination of wounds is the principal concern. Finely divided metal and soluble compounds require strict radiological containment. External dose rates can be significant for some samples because of accompanying gamma-emitting impurities or daughters.
Natural neptunium is extremely scarce, but anthropogenic neptunium occurs in spent nuclear fuel, reprocessing wastes, and fallout residues. Environmental behavior is controlled by oxidation state, complexation, mineral sorption, and reducing conditions. Np(V) as NpO₂⁺ can migrate more readily than many tetravalent actinides, whereas Np(IV) tends to form less soluble solids or strongly sorbed species. Its long half-life makes it important in repository performance assessments.
Neptunium is not traded as a commodity and has no ordinary industrial supply chain. Recoverable ²³⁷Np is generated as a by-product in irradiated uranium fuel and can be separated only in specialized nuclear facilities under heavy regulation. Demand is small and centered on research inventories and on target preparation for ²³⁸Pu production. Costs are dominated by radiochemical separation, safeguards, licensing, waste management, and secure storage rather than by ore mining or conventional refining.
Produced by bombarding uranium with slow neutrons.
Neptunium has no stable isotopes, so any primordial neptunium has decayed away. It can be formed in trace amounts by neutron capture in uranium-bearing materials and in nuclear explosions or reactors, and transient neptunium isotopes may occur in astrophysical rapid neutron-capture processes. Its extraterrestrial abundance is effectively negligible compared with long-lived actinides such as uranium and thorium.
- Neptunium was named after Neptune, following uranium’s naming after Uranus.
- ²³⁷Np has a half-life of about 2.14 million years.
- Neptunium was the first element beyond uranium to be identified.
- NpF₆ is volatile, a property relevant to actinide fluoride chemistry.
- The common aqueous Np(V) ion is linear neptunyl, NpO₂⁺.
- Separated neptunium metal darkens on exposure to air.
Gambar
Sifat
Fisika
- Jari-jari atom (empiris)
- 175 pm Bandingkan Jari-jari atom (empiris) semua unsur →
- Jari-jari kovalen
- 190 pm Bandingkan Jari-jari kovalen semua unsur →
- Jari-jari van der Waals
- 221 pm Bandingkan Jari-jari van der Waals semua unsur →
- Massa jenis
- 2,025 × 104 kg/m³ Bandingkan Massa jenis semua unsur →
- Volume molar
- 0,0211 L/mol
- Fase pada STP
- Padat Bandingkan Fase pada STP semua unsur →
- Titik lebur
- 643,85 °C Bandingkan Titik lebur semua unsur →
- Titik didih
- 3901,85 °C Bandingkan Titik didih semua unsur →
- Struktur kristal
- Ortorombik Bandingkan Struktur kristal semua unsur →
Kimia
- Keelektronegatifan (Pauling)
- 1,36 Bandingkan Keelektronegatifan (Pauling) semua unsur →
- Afinitas elektron
- 0,48 eV
- Energi ionisasi (ke-1)
- 6,265608 eV Bandingkan Energi ionisasi (ke-1) semua unsur →
- Energi ionisasi (ke-2)
- 11,50004 eV Bandingkan Energi ionisasi (ke-2) semua unsur →
- Energi ionisasi (ke-3)
- 19,700068 eV Bandingkan Energi ionisasi (ke-3) semua unsur →
- Energi ionisasi (ke-4)
- 33,800116 eV Bandingkan Energi ionisasi (ke-4) semua unsur →
- Energi ionisasi (ke-5)
- 48,000165 eV Bandingkan Energi ionisasi (ke-5) semua unsur →
- Bilangan oksidasi
- +2, +3, +4, +5, +6, +7 Bandingkan Bilangan oksidasi semua unsur →
- Elektron valensi
- 3 Bandingkan Elektron valensi semua unsur →
- Konfigurasi elektron
- [Rn] 7s2 5f4 6d1
Termodinamika
- Kalor peleburan
- 0,10364305 eV Bandingkan Kalor peleburan semua unsur →
- Kalor penguapan
- 3,482407 eV Bandingkan Kalor penguapan semua unsur →
- Kalor sublimasi
- 4,33228 eV
- Kalor atomisasi
- 4,33228 eV
- Entalpi atomisasi
- 4,817329 eV
Nuklir
- Proton
- 93 Bandingkan Proton semua unsur →
- Neutron
- 144 Bandingkan Neutron semua unsur →
- Isotop yang diketahui
- 27 Bandingkan Isotop yang diketahui semua unsur →
- Isotop stabil
- 0 Bandingkan Isotop stabil semua unsur →
- Nomor massa (paling stabil)
- 237
- Isotop paling stabil
- Np-237
- Tahun penemuan
- 1940
Kelimpahan
Tidak tersedia
Struktur Kristal
- Konstanta kisi a
- 472 pm
Struktur Elektronik
- Elektron per kulit
- 2, 8, 18, 32, 22, 9, 2 Bandingkan Elektron per kulit semua unsur →
Pengenal
- Nomor CAS
- 7439-99-8 Bandingkan Nomor CAS semua unsur →
- Simbol term
- 6L11/2
- InChI
- InChI=1S/Np
- Kunci InChI
- LFNLGNPSGWYGGD-UHFFFAOYSA-N
Konfigurasi Elektron Diukur
Np: 5f⁴ 6d¹ 7s²[Rn] 5f⁴ 6d¹ 7s²1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f⁴ 6d¹ 7s²Model atom
Isotop mengubah jumlah neutron, massa, dan kestabilan — bukan konfigurasi elektron atom netral.
Model atom skematis, tidak sesuai skala.
Sidik Jari Atom
Spektrum Emisi / Absorpsi
Distribusi Isotop
Tidak memiliki isotop stabil.
| Nomor massa | Massa atom (u) | Kelimpahan alami | Waktu paruh |
|---|---|---|---|
| 219 Radioaktif | 219,03143 ± 0,00021 | Tidak tersedia | 570 us |
| 227 Radioaktif | 227,034957 ± 0,000078 | Tidak tersedia | 510 ms |
| 222 Radioaktif | 222,0333 ± 0,00021 | Tidak tersedia | 480 ns |
| 235 Radioaktif | 235,0440635 ± 0,0000021 | Tidak tersedia | 396.1 hari |
| 236 Radioaktif | 236,04657 ± 0,000054 | Tidak tersedia | 153 ky |
Fase / Wujud
Alasan: 618,9 °C di bawah titik lebur (643,85 °C)
Skematis, tidak sesuai skala
Titik transisi fase
Energi transisi
Energi yang diperlukan untuk meleburkan 1 mol pada titik lebur
Energi yang diperlukan untuk menguapkan 1 mol pada titik didih
Energi yang diperlukan untuk menyublimkan 1 mol pada titik sublimasi
Massa jenis
Pada kondisi standar
Pada kondisi standar
Spektrum Atom
Menampilkan 10 dari 93. Diurutkan berdasarkan muatan ion (menaik).
Data Garis Spektrum ?
| Ion | Muatan | Total garis | Probabilitas transisi | Penamaan tingkat energi |
|---|---|---|---|---|
| Np I | 0 | 96 | 0 | 0 |
Data Tingkat Energi ?
| Ion | Muatan | Tingkat energi |
|---|---|---|
| Np I | 0 | 2 |
| Np II | +1 | 2 |
| Np III | +2 | 2 |
| Np IV | +3 | 2 |
| Np V | +4 | 2 |
| Np VI | +5 | 2 |
| Np VII | +6 | 2 |
| Np VIII | +7 | 2 |
| Np IX | +8 | 2 |
| Np X | +9 | 2 |
Jari-jari Ion
| Muatan | Koordinasi | Spin | Jari-jari |
|---|---|---|---|
| +2 | 6 | Tidak tersedia | 110.00000000000001 pm |
| +3 | 6 | Tidak tersedia | 101 pm |
| +3 | 9 | Tidak tersedia | 117.8 pm |
| +4 | 6 | Tidak tersedia | 87 pm |
| +4 | 8 | Tidak tersedia | 98 pm |
| +5 | 6 | Tidak tersedia | 75 pm |
| +6 | 6 | Tidak tersedia | 72 pm |
| +7 | 6 | Tidak tersedia | 71 pm |
Senyawa
Isotop (5)
There are 25 known radioactive isotopes of neptunium ranging in atomic weights from 225 to 244 with 5 of those as metastable isotopes. The most stable are Np-237 with a half-life of 2.14 million years; Np-236 with a half-life of 154,000 years; and Np-235 with a half-life of 396 days. All of the remaining isotopes have half-lives less than 4.5 days, with most less than 50 minutes. The primary decay mode for isotopes lighter than 237Np is by electron capture with a great deal of alpha emission. The products are mostly isotopes of uranium. The primary decay mode for Np-237 is by alpha-decay forming protactinium. The primary decay mode for the isotopes heavier than Np-237 is by beta-decay, forming plutonium. Neptunium-237, after decaying to protactinium then to uranium, eventually decays to form bismuth-209 and thallium-205. Unlike most other common heavy nuclei which decay to make isotopes of lead this decay chain is known as the neptunium series.
| Nomor massa | Massa atom (u) | Kelimpahan alami | Waktu paruh | Mode peluruhan | |
|---|---|---|---|---|---|
| 219 Radioaktif | 219,03143 ± 0,00021 | Tidak tersedia | 570 us | α =100% | |
| 227 Radioaktif | 227,034957 ± 0,000078 | Tidak tersedia | 510 ms | α ≈100%β+ ? | |
| 222 Radioaktif | 222,0333 ± 0,00021 | Tidak tersedia | 480 ns | α =100% | |
| 235 Radioaktif | 235,0440635 ± 0,0000021 | Tidak tersedia | 396.1 hari | ε =99.99740±1.3%α =0.00260±1.3% | |
| 236 Radioaktif | 236,04657 ± 0,000054 | Tidak tersedia | 153 ky | ε =86.3±0.8%β- =13.5±0.8%α =0.16±0.4% |
Sifat Lanjutan
Jari-jari Kovalen (Lanjutan)
- Jari-jari kovalen (Pyykkö)
- 171 pm
- Jari-jari kovalen (Pyykkö, ikatan rangkap dua)
- 136 pm
- Jari-jari kovalen (Pyykkö, ikatan rangkap tiga)
- 116 pm
Jari-jari van der Waals
- Alvarez
- 282 pm
- UFF
- 342,4 pm
- MM3
- 252 pm
Jari-jari Atom & Logam
- Jari-jari atom (Rahm)
- 281 pm
Skala Penomoran
- Mendeleev
- 22
- Pettifor
- 44
- Glawe
- 37
Skala Keelektronegatifan
- Ghosh
- 0
Polarizabilitas & Dispersi
- Polarizabilitas dipol
- 151 a.u.
- Polarizabilitas dipol (ketidakpastian)
- 20 a.u.
Transisi Fase & Alotrop
| Titik lebur | 917,15 K |
Kategori Bilangan Oksidasi
Data Referensi Lanjutan
Detail Jari-jari Kristal (8)
| Muatan | CN | Spin | rcrystal (pm) | Asal |
|---|---|---|---|---|
| 2 | VI | 124 | ||
| 3 | VI | 115 | from r^3 vs V plots, | |
| 4 | VI | 101 | from r^3 vs V plots, | |
| 4 | VIII | 112 | from r^3 vs V plots, | |
| 5 | VI | 89 | ||
| 6 | VI | 86 | from r^3 vs V plots, | |
| 7 | VI | 85 | Ahrens (1952) ionic radius, | |
| 3 | IX | — | 131,8 |
Mode Peluruhan Isotop (44)
| Isotop | Mode | Intensitas |
|---|---|---|
| 219 | A | 100% |
| 220 | A | 100% |
| 221 | A | — |
| 222 | A | 100% |
| 223 | A | 100% |
| 224 | A | 100% |
| 225 | A | 100% |
| 225 | B+ | — |
| 226 | A | 100% |
| 226 | B+ | — |
Data Tambahan
Estimated Crustal Abundance
The estimated element abundance in the earth's crust.
Not Applicable
Referensi (1)
- [5] Neptunium https://education.jlab.org/itselemental/ele093.html
Estimated Oceanic Abundance
The estimated element abundance in the earth's oceans.
Not Applicable
Referensi (1)
- [5] Neptunium https://education.jlab.org/itselemental/ele093.html
Referensi
(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 Neptunium.
The element property data was retrieved from publications.