Lawrencium (Lr)
actinideSolid
Bobot Atom Standar
[262]Konfigurasi elektron
[Rn] 7s2 5f14 6d1Titik lebur
1626,85 °CTitik didih
Tidak tersediaMassa jenis
1,56e+4 kg/m³Bilangan oksidasi
+3Keelektronegatifan (Pauling)
Tidak tersediaEnergi ionisasi (ke-1)
4,96 eVTahun penemuan
1961Jari-jari atom
Tidak tersediaDetail
Lawrencium is a synthetic, highly radioactive actinide and the last element of the actinide series. It has been made only in minute numbers of atoms in nuclear reactions, so its chemistry is known from rapid, atom-at-a-time experiments and theoretical calculations. Its most stable known isotopes are short-lived on ordinary laboratory timescales. In solution it behaves chiefly as a trivalent metal, Lr³⁺, broadly resembling late actinides and some trivalent lanthanides.
Lawrencium does not occur naturally in the Earth’s crust. Credit for the first synthesis of this element in 1971 is given jointly to Albert Ghiorso and his team at the University of California in Berkeley and Georgi Flerov and his team at the Joint Institute for Nuclear Research (JINR) in Dubna, Russia (Fig. IUPAC.103.1). The element is named for Ernest O. Lawrence (Fig. IUPAC.103.2), who developed the cyclotron. The chemical symbol for lawrencium was originally proposed as Lw. At the IUPAC General Assembly in 1963, lawrencium was officially accepted by IUPAC, but the symbol was changed to Lr because the Commission on Inorganic Nomenclature determined that the letter ‘w’ presented a problem in languages other than English [636], [640], [641], [642]. There are no known isotopic applications for lawrencium outside of scientific research.
Lawrencium behaves differently from dipositive nobelium and more like the tripositive elements earlier in the actinide series.
Lawrencium was created by four American scientists, Albert Ghiorso, Torbjørn Sikkeland, Almon E. Larsh and Robert M. Latimer, in March, 1961. Working at the Lawrence Radiation Laboratory in Berkeley, California, the scientists placed three micrograms (0.000003 grams) of californium in the target chamber of a device called a linear accelerator. The scientists used the accelerator to bombard the californium with boron ions. Several different isotopes of lawrencium were created and there is some confusion as to which isotope the group actually detected. Today, the Lawrence Radiation Laboratory is known as the Lawrence Berkeley Laboratory. Lawrencium's most stable isotope, lawrencium-262, has a half-life of about 4 hours. It decays into nobelium-262 through electron capture, mendelevium-258 through alpha decay or through spontaneous fission.
Named after Lawrence, inventor of the cyclotron. This member of the 5f transition elements (actinide series) was discovered in March 1961 by A. Ghiorso, T. Sikkeland, A.E. Larsh, and R.M. Latimer. A 3-Mg californium target, consisting of a mixture of isotopes of mass number 249, 250, 251, and 252, was bombarded with either 10B or 11B. The electrically charged transmutation nuclei recoiled with an atmosphere of helium and were collected on a thin copper conveyor tape which was then moved to place collected atoms in front of a series of solid-state detectors. The isotope of element 103 produced in this way decayed by emitting an 8.6 MeV alpha particle with a half-life of 8 s.
In 1967, Flerov and associates at the Dubna Laboratory reported their inability to detect an alpha emitter with a half-life of 8 s which was assigned by the Berkeley group to 257103. This assignment has been changed to 258Lr or 259Lr.
In 1965, the Dubna workers found a longer-lived lawrencium isotope, 256Lr, with a half-life of 35 s. In 1968, Thiorso and associates at Berkeley used a few atoms of this isotope to study the oxidation behavior of lawrencium. Using solvent extraction techniques and working very rapidly, they extracted lawrencium ions from a buffered aqueous solution into an organic solvent completing each extraction in about 30 s.
No macroscopic sample of lawrencium has been prepared, and its visible appearance has not been observed. The pure metal’s color, texture, density, melting behavior, and other bulk properties are therefore unknown or only theoretically estimated.
Lawrencium has no practical use outside scientific research. Its isotopes are produced to study nuclear structure, heavy-element synthesis, decay chains, and the chemical behavior at the end of the actinide series. Individual atoms have also been used in chromatography and related experiments to test periodic trends, especially the stability and complexing behavior of Lr³⁺. It has no commercial, medical, industrial, or consumer application.
Since only tiny amounts of lawrencium have ever been produced, there are currently no uses for it outside of basic scientific research.
No weighable compound of lawrencium has been isolated. The established chemistry is dominated by the +3 oxidation state in aqueous solution, where Lr³⁺ is the important species. Atom-at-a-time studies have examined its adsorption and complex formation with mineral acids and organic complexants. Simple compounds such as lawrencium trichloride, LrCl₃, or lawrencium oxide, Lr₂O₃, are chemically plausible by analogy, but their bulk structures and properties have not been measured directly. Higher oxidation states are not established under ordinary chemical conditions.
See more information at the Lawrencium compound page.
All known lawrencium isotopes are radioactive, and safety concerns are radiological rather than ordinary chemical exposure hazards. The amounts produced are extremely small, but work with lawrencium occurs in facilities equipped for heavy-ion reactions and actinide radiochemistry. Isotope-specific half-lives and decay modes matter for handling, shielding, contamination control, and waste management. There is no known biological role.
Lawrencium has no confirmed natural environmental cycle. Any atoms produced on Earth are artificial and decay before dispersal could resemble the behavior of stable elements. In the environment, hypothetical lawrencium would be expected to follow trivalent actinide chemistry to some extent, but this has not been observed at environmental concentrations. Its ecological relevance is therefore limited to controlled laboratory production and radioactive waste from experiments.
Lawrencium has no commodity market, no bulk production, and no recycling stream. It is made only for research by bombarding heavy actinide targets, such as isotopes of californium or berkelium, with accelerated ions. Production yields are very low, often only atoms suitable for immediate detection or chemistry. The limiting factors are accelerator access, rare target materials, radiochemical separation speed, and detector capability rather than ordinary raw-material demand.
Produced by bombarding californium with boron ions.
Lawrencium is not expected to have a persistent cosmic abundance. Its known isotopes decay too rapidly to survive from stellar nucleosynthesis or the formation of the Solar System. Very short-lived lawrencium nuclei could in principle be formed in extreme neutron-rich or heavy-ion processes, but no extraterrestrial occurrence has been detected. Any natural presence would be transient and atomically scarce.
- Lawrencium chemistry is performed one atom at a time.
- Its electron configuration is anomalous, with a 7p electron in the neutral atom’s ground state.
- The element helps test where the actinide series ends and how group 3 should be described.
- Lr³⁺ is more chemically relevant than the neutral metal for experiments.
- No lawrencium compound has been isolated in visible quantity.
Gambar
Sifat
Fisika
- Jari-jari van der Waals
- 246 pm Bandingkan Jari-jari van der Waals semua unsur →
- Massa jenis
- 1,56 × 104 kg/m³ Bandingkan Massa jenis semua unsur →
- Fase pada STP
- Padat Bandingkan Fase pada STP semua unsur →
- Titik lebur
- 1626,85 °C Bandingkan Titik lebur semua unsur →
Kimia
- Afinitas elektron
- 0,315 eV
- Energi ionisasi (ke-1)
- 4,96 eV Bandingkan Energi ionisasi (ke-1) semua unsur →
- Energi ionisasi (ke-2)
- 14,54005 eV Bandingkan Energi ionisasi (ke-2) semua unsur →
- Energi ionisasi (ke-3)
- 21,800075 eV Bandingkan Energi ionisasi (ke-3) semua unsur →
- Energi ionisasi (ke-4)
- 43,60015 eV Bandingkan Energi ionisasi (ke-4) semua unsur →
- Energi ionisasi (ke-5)
- 56,000193 eV Bandingkan Energi ionisasi (ke-5) semua unsur →
- Bilangan oksidasi
- +3 Bandingkan Bilangan oksidasi semua unsur →
- Elektron valensi
- 3 Bandingkan Elektron valensi semua unsur →
- Konfigurasi elektron
- [Rn] 7s2 5f14 6d1
Termodinamika
- Kalor sublimasi
- 4,249365 eV
- Kalor atomisasi
- 4,249365 eV
Nuklir
- Proton
- 103 Bandingkan Proton semua unsur →
- Neutron
- 163 Bandingkan Neutron semua unsur →
- Isotop yang diketahui
- 16 Bandingkan Isotop yang diketahui semua unsur →
- Isotop stabil
- 0 Bandingkan Isotop stabil semua unsur →
- Nomor massa (paling stabil)
- 262
- Isotop paling stabil
- Lr-266
- Tahun penemuan
- 1961
Kelimpahan
Tidak tersedia
Struktur Kristal
Tidak tersedia
Struktur Elektronik
- Elektron per kulit
- 2, 8, 18, 32, 32, 8, 3 Bandingkan Elektron per kulit semua unsur →
Pengenal
- Nomor CAS
- 22537-19-5 Bandingkan Nomor CAS semua unsur →
- Simbol term
- 2P°1/2
- InChI
- InChI=1S/Lr
- Kunci InChI
- CNQCVBJFEGMYDW-UHFFFAOYSA-N
Konfigurasi Elektron Diukur
Lr: 5f¹⁴ 7s² 7p¹[Rn] 5f¹⁴ 7s² 7p¹1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f¹⁴ 7s² 7p¹Model 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 |
|---|---|---|---|
| 253 Radioaktif | 253,09509 ± 0,00022 | Tidak tersedia | 632 ms |
| 252 Radioaktif | 252,09526 ± 0,00026 | Tidak tersedia | 369 ms |
| 251 Radioaktif | 251,09418 ± 0,00032 | Tidak tersedia | 300 us |
| 261 Radioaktif | 261,10688 ± 0,00022 | Tidak tersedia | 39 menit |
| 255 Radioaktif | 255,096562 ± 0,000019 | Tidak tersedia | 31.1 detik |
Fase / Wujud
Alasan: 1601,8 °C di bawah titik sublimasi (1626,85 °C)
Skematis, tidak sesuai skala
Titik transisi fase
Energi transisi
Energi yang diperlukan untuk menyublimkan 1 mol pada titik sublimasi
Massa jenis
Pada kondisi standar
Pada kondisi standar
Spektrum Atom
Menampilkan 10 dari 103. Diurutkan berdasarkan muatan ion (menaik).
Data Tingkat Energi ?
| Ion | Muatan | Tingkat energi |
|---|---|---|
| Lr I | 0 | 2 |
| Lr II | +1 | 2 |
| Lr III | +2 | 2 |
| Lr IV | +3 | 2 |
| Lr V | +4 | 2 |
| Lr VI | +5 | 2 |
| Lr VII | +6 | 2 |
| Lr VIII | +7 | 2 |
| Lr IX | +8 | 2 |
| Lr X | +9 | 2 |
Data struktur kristal tidak tersedia
Jari-jari Ion
| Muatan | Koordinasi | Spin | Jari-jari |
|---|---|---|---|
| +3 | 9 | Tidak tersedia | 107.4 pm |
Senyawa
Isotop (5)
| Nomor massa | Massa atom (u) | Kelimpahan alami | Waktu paruh | Mode peluruhan | |
|---|---|---|---|---|---|
| 253 Radioaktif | 253,09509 ± 0,00022 | Tidak tersedia | 632 ms | α =90±1%SF =1.0±0.6%β+ ? | |
| 252 Radioaktif | 252,09526 ± 0,00026 | Tidak tersedia | 369 ms | α ≈98%SF ≈2%β+ ? | |
| 251 Radioaktif | 251,09418 ± 0,00032 | Tidak tersedia | 300 us | β+ ?α ? | |
| 261 Radioaktif | 261,10688 ± 0,00022 | Tidak tersedia | 39 menit | SF ≈100%α ? | |
| 255 Radioaktif | 255,096562 ± 0,000019 | Tidak tersedia | 31.1 detik | α =99.7±0.1%β+ =0.3±0.1%SF ? |
Sifat Lanjutan
Jari-jari Kovalen (Lanjutan)
- Jari-jari kovalen (Pyykkö)
- 161 pm
- Jari-jari kovalen (Pyykkö, ikatan rangkap dua)
- 141 pm
Jari-jari van der Waals
- UFF
- 323,6 pm
Skala Penomoran
- Mendeleev
- 42
- Pettifor
- 34
- Glawe
- 47
Skala Keelektronegatifan
- Ghosh
- 0
Polarizabilitas & Dispersi
- Polarizabilitas dipol
- 320 a.u.
- Polarizabilitas dipol (ketidakpastian)
- 20 a.u.
Transisi Fase & Alotrop
| Titik lebur | 1900,15 K |
Kategori Bilangan Oksidasi
Data Referensi Lanjutan
Detail Jari-jari Kristal (1)
| Muatan | CN | Spin | rcrystal (pm) | Asal |
|---|---|---|---|---|
| 3 | IX | — | 121,4 |
Mode Peluruhan Isotop (38)
| Isotop | Mode | Intensitas |
|---|---|---|
| 251 | B+ | — |
| 251 | A | — |
| 252 | A | 98% |
| 252 | SF | 2% |
| 252 | B+ | — |
| 253 | A | 90% |
| 253 | SF | 1% |
| 253 | B+ | — |
| 254 | A | 71,7% |
| 254 | B+ | 28,3% |
Data Tambahan
Estimated Crustal Abundance
The estimated element abundance in the earth's crust.
Not Applicable
Referensi (1)
- [5] Lawrencium https://education.jlab.org/itselemental/ele103.html
Estimated Oceanic Abundance
The estimated element abundance in the earth's oceans.
Not Applicable
Referensi (1)
- [5] Lawrencium https://education.jlab.org/itselemental/ele103.html
Referensi
(8)
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 Lawrencium.
