Lr 103

Lawrencium (Lr)

actinide
周期: 7 族: 3 区: f

Solid

标准原子量

[262]

电子排布

[Rn] 7s2 5f14 6d1

熔点

1626.85 °C

沸点

暂无

密度

1.56e+4 kg/m³

氧化态

+3

电负性(鲍林)

暂无

第一电离能

4.96 eV

发现年份

1961

原子半径

暂无

详细信息

名称来源 Named in honor of Ernest O. Lawrence, inventor of the cyclotron.
发现国家 United States
发现者 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.

图片

性质

物理性质

范德华半径
246 pm 比较所有元素的范德华半径 →
密度
1.56 × 104 kg/m³ 比较所有元素的密度 →
标准温度和压力下的物相
固态 比较所有元素的标准温度和压力下的物相 →
熔点
1626.85 °C 比较所有元素的熔点 →

化学性质

电子亲和能
0.315 eV
第一电离能
4.96 eV 比较所有元素的第一电离能 →
第二电离能
14.54005 eV 比较所有元素的第二电离能 →
第三电离能
21.800075 eV 比较所有元素的第三电离能 →
第四电离能
43.60015 eV 比较所有元素的第四电离能 →
第五电离能
56.000193 eV 比较所有元素的第五电离能 →
氧化态
+3 比较所有元素的氧化态 →
价电子
3 比较所有元素的价电子 →
电子排布
[Rn] 7s2 5f14 6d1

热力学性质

升华热
4.249365 eV
原子化热
4.249365 eV

核性质

质子
103 比较所有元素的质子 →
中子
163 比较所有元素的中子 →
已知同位素
16 比较所有元素的已知同位素 →
稳定同位素
0 比较所有元素的稳定同位素 →
质量数(最稳定同位素)
262
最稳定同位素
Lr-266
发现年份
1961

丰度

暂无

晶体结构

暂无

电子结构

各电子层电子数
2, 8, 18, 32, 32, 8, 3 比较所有元素的各电子层电子数 →

标识符

CAS登记号
22537-19-5 比较所有元素的CAS登记号 →
谱项符号
2P°1/2
InChI
InChI=1S/Lr
InChI Key
CNQCVBJFEGMYDW-UHFFFAOYSA-N

电子排布 实测值

离子电荷
质子 103
电子 103
电荷 中性
电子排布 Lr: 5f¹⁴ 7s² 7p¹
电子排布
实测值
[Rn] 5f¹⁴ 7s² 7p¹
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f¹⁴ 7s² 7p¹
轨道图
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↑
电子总数: 103 未配对: 1 ?

原子模型

质子 103
中子 150
电子 103
质量数 253
稳定性 放射性

不同同位素的中子数、质量和稳定性不同,但中性原子的电子排布不变。

原子模型示意图,未按比例绘制。

原子指纹

发射 / 吸收光谱

0 / 0 (0 0条具有强度数据)
实测值
发射 可见光:380–750 nm

同位素分布

无稳定同位素。

质量数原子质量(u)天然丰度半衰期
253 放射性253.09509 ± 0.00022暂无632 ms
252 放射性252.09526 ± 0.00026暂无369 ms
251 放射性251.09418 ± 0.00032暂无300 us
261 放射性261.10688 ± 0.00022暂无39 分钟
255 放射性255.096562 ± 0.000019暂无31.1 秒
实测值

物相 / 状态

1 atm / 101.325 kPa
固态 25 °C (298.15 K)

原因: 低于升华点(1626.85 °C)1601.8 °C

升华点 1626.85 °C
0 K 当前温度: 25 °C 6000 K
物相变化轴

示意图,未按比例绘制

固态
气态
升华
25°C
固态
液态
气态
当前

相变点

升华点 文献值
1626.85 °C
当前物相 计算值
固态

相变能

升华热 文献值
4.249365 eV

在升华点升华1 mol物质所需的能量

密度

参考密度 文献值
1.56e+4 kg/m³

标准条件下

当前密度 计算值
1.56e+4 kg/m³

标准条件下

原子光谱

已显示10项,共103项。 按离子电荷升序排列。

收录能级 ?

离子电荷能级
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
NIST收录能级 →
103 Lr 262

Lawrencium — 原子轨道可视化工具

[Rn]7s25f146d1
能级 2 8 18 32 32 9 2
氧化态 +3
HOMO 6d n=6 · l=2 · m=-2
Lawrencium — 原子轨道可视化预览
Three.js仅在需要时加载
103 Lr 262

Lawrencium — 晶体结构可视化工具

暂无晶体结构数据

离子半径

电荷配位自旋半径
+39暂无107.4 pm

化合物

Lr
266.120 u

同位素 (5)

质量数原子质量(u)天然丰度半衰期衰变方式
253 放射性253.09509 ± 0.00022暂无632 ms
α =90±1%SF =1.0±0.6%β+ ?
252 放射性252.09526 ± 0.00026暂无369 ms
α ≈98%SF ≈2%β+ ?
251 放射性251.09418 ± 0.00032暂无300 us
β+ ?α ?
261 放射性261.10688 ± 0.00022暂无39 分钟
SF ≈100%α ?
255 放射性255.096562 ± 0.000019暂无31.1 秒
α =99.7±0.1%β+ =0.3±0.1%SF ?
253 放射性
原子质量(u) 253.09509 ± 0.00022
天然丰度 暂无
半衰期 632 ms
衰变方式
α =90±1%SF =1.0±0.6% +1
252 放射性
原子质量(u) 252.09526 ± 0.00026
天然丰度 暂无
半衰期 369 ms
衰变方式
α ≈98%SF ≈2% +1
251 放射性
原子质量(u) 251.09418 ± 0.00032
天然丰度 暂无
半衰期 300 us
衰变方式
β+ ?α ?
261 放射性
原子质量(u) 261.10688 ± 0.00022
天然丰度 暂无
半衰期 39 分钟
衰变方式
SF ≈100%α ?
255 放射性
原子质量(u) 255.096562 ± 0.000019
天然丰度 暂无
半衰期 31.1 秒
衰变方式
α =99.7±0.1%β+ =0.3±0.1% +1

扩展性质

共价半径(扩展)

共价半径(Pyykkö)
161 pm
共价半径(Pyykkö,双键)
141 pm

范德华半径

UFF
323.6 pm

编号标度

Mendeleev
42
Pettifor
34
Glawe
47

电负性标度

Ghosh
0

极化率与色散

偶极极化率
320 a.u.
偶极极化率(不确定度)
20 a.u.

相变与同素异形体

熔点1900.15 K

氧化态分类

+3 main

高级参考数据

晶体半径详情 (1)
电荷CN自旋rcrystal (pm)来源
3IX—121.4
同位素衰变方式 (38)
同位素模式强度
251B+—
251A—
252A98%
252SF2%
252B+—
253A90%
253SF1%
253B+—
254A71.7%
254B+28.3%

补充数据

参考文献

(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.

许可证说明: 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/

许可证说明: 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.

最后更新:

数据已核实:

内容已依据最新科学数据进行审核。