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Lr 103

Lawrencium (Lr)

actinide
Periode: 7 Golongan: 3 Blok: f

Solid

Bobot Atom Standar

[262]

Konfigurasi elektron

[Rn] 7s2 5f14 6d1

Titik lebur

1626,85 °C

Titik didih

Tidak tersedia

Massa jenis

1,56e+4 kg/m³

Bilangan oksidasi

+3

Keelektronegatifan (Pauling)

Tidak tersedia

Energi ionisasi (ke-1)

4,96 eV

Tahun penemuan

1961

Jari-jari atom

Tidak tersedia

Detail

Asal nama Named in honor of Ernest O. Lawrence, inventor of the cyclotron.
Negara penemuan United States
Penemu A.Ghiorso, T.Sikkeland, A.E.Larsh, R.M.Latimer

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.

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

Muatan ion
Proton 103
Elektron 103
Muatan Netral
Konfigurasi Lr: 5f¹⁴ 7s² 7p¹
Konfigurasi elektron
Diukur
[Rn] 5f¹⁴ 7s² 7p¹
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f¹⁴ 7s² 7p¹
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
14/14
7p
1/6 1↑
Total elektron: 103 Tidak berpasangan: 1 ?

Model atom

Proton 103
Neutron 150
Elektron 103
Nomor massa 253
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
253 Radioaktif253,09509 ± 0,00022Tidak tersedia632 ms
252 Radioaktif252,09526 ± 0,00026Tidak tersedia369 ms
251 Radioaktif251,09418 ± 0,00032Tidak tersedia300 us
261 Radioaktif261,10688 ± 0,00022Tidak tersedia39 menit
255 Radioaktif255,096562 ± 0,000019Tidak tersedia31.1 detik
Diukur

Fase / Wujud

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

Alasan: 1601,8 °C di bawah titik sublimasi (1626,85 °C)

Titik sublimasi 1626,85 °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
1626,85 °C
Fase saat ini Dihitung
Padat

Energi transisi

Kalor sublimasi Literatur
4,249365 eV

Energi yang diperlukan untuk menyublimkan 1 mol pada titik sublimasi

Massa jenis

Massa jenis referensi Literatur
1,56e+4 kg/m³

Pada kondisi standar

Massa jenis saat ini Dihitung
1,56e+4 kg/m³

Pada kondisi standar

Spektrum Atom

Menampilkan 10 dari 103. Diurutkan berdasarkan muatan ion (menaik).

Data Tingkat Energi ?

IonMuatanTingkat energi
Lr I 02
Lr II +12
Lr III +22
Lr IV +32
Lr V +42
Lr VI +52
Lr VII +62
Lr VIII +72
Lr IX +82
Lr X +92
Data Tingkat Energi NIST →
103 Lr 262

Lawrencium — Visualisasi Orbital Atom

[Rn]7s25f146d1
Tingkat energi 2 8 18 32 32 9 2
Bilangan oksidasi +3
HOMO 6d n=6 · l=2 · m=-2
Lawrencium — Pratinjau Visualisasi Orbital Atom
Three.js hanya dimuat saat diminta
103 Lr 262

Lawrencium — Visualisasi Struktur Kristal

Data struktur kristal tidak tersedia

Jari-jari Ion

MuatanKoordinasiSpinJari-jari
+39Tidak tersedia107.4 pm

Senyawa

Lr
266,120 u

Isotop (5)

Nomor massaMassa atom (u)Kelimpahan alamiWaktu paruhMode peluruhan
253 Radioaktif253,09509 ± 0,00022Tidak tersedia632 ms
α =90±1%SF =1.0±0.6%β+ ?
252 Radioaktif252,09526 ± 0,00026Tidak tersedia369 ms
α ≈98%SF ≈2%β+ ?
251 Radioaktif251,09418 ± 0,00032Tidak tersedia300 us
β+ ?α ?
261 Radioaktif261,10688 ± 0,00022Tidak tersedia39 menit
SF ≈100%α ?
255 Radioaktif255,096562 ± 0,000019Tidak tersedia31.1 detik
α =99.7±0.1%β+ =0.3±0.1%SF ?
253 Radioaktif
Massa atom (u) 253,09509 ± 0,00022
Kelimpahan alami Tidak tersedia
Waktu paruh 632 ms
Mode peluruhan
α =90±1%SF =1.0±0.6% +1
252 Radioaktif
Massa atom (u) 252,09526 ± 0,00026
Kelimpahan alami Tidak tersedia
Waktu paruh 369 ms
Mode peluruhan
α ≈98%SF ≈2% +1
251 Radioaktif
Massa atom (u) 251,09418 ± 0,00032
Kelimpahan alami Tidak tersedia
Waktu paruh 300 us
Mode peluruhan
β+ ?α ?
261 Radioaktif
Massa atom (u) 261,10688 ± 0,00022
Kelimpahan alami Tidak tersedia
Waktu paruh 39 menit
Mode peluruhan
SF ≈100%α ?
255 Radioaktif
Massa atom (u) 255,096562 ± 0,000019
Kelimpahan alami Tidak tersedia
Waktu paruh 31.1 detik
Mode peluruhan
α =99.7±0.1%β+ =0.3±0.1% +1

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 lebur1900,15 K

Kategori Bilangan Oksidasi

+3 main

Data Referensi Lanjutan

Detail Jari-jari Kristal (1)
MuatanCNSpinrcrystal (pm)Asal
3IX—121,4
Mode Peluruhan Isotop (38)
IsotopModeIntensitas
251B+—
251A—
252A98%
252SF2%
252B+—
253A90%
253SF1%
253B+—
254A71,7%
254B+28,3%

Data Tambahan

Referensi

(8)
2 Atomic Mass Data Center (AMDC), International Atomic Energy Agency (IAEA)
Lr

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)
Lawrencium

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
Lawrencium

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
Lawrencium

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
Lawrencium

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
Lawrencium

This section provides all form of data related to element Lawrencium.

Terakhir diperbarui:

Data terverifikasi:

Konten ditinjau berdasarkan data ilmiah terbaru.