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Rf 104

Rutherfordium (Rf)

transition-metal
Periode: 7 Golongan: 4 Blok: d

Solid

Bobot Atom Standar

263 u

Konfigurasi elektron

[Rn] 7s2 5f14 6d2

Titik lebur

2126,85 °C

Titik didih

5526,85 °C

Massa jenis

2,33e+4 kg/m³

Bilangan oksidasi

+3, +4

Keelektronegatifan (Pauling)

Tidak tersedia

Energi ionisasi (ke-1)

6,02 eV

Tahun penemuan

1964

Jari-jari atom

150 pm

Detail

Asal nama Named in honor of Ernest Rutherford
Negara penemuan United States
Penemu A. Ghiorso, et al

Rutherfordium is a synthetic transactinide element and the first member of the 6d transition-metal series. All confirmed isotopes are radioactive and short-lived, so its chemistry is studied atom by atom. Chemical experiments show behavior broadly consistent with a group 4 element, analogous to hafnium and zirconium, with the +4 oxidation state dominant in aqueous and halide systems. Relativistic effects and nuclear instability make direct measurements difficult.

Rutherfordium does not occur naturally in the Earth’s crust. Credit for the first synthesis of this element 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. The element is named for Ernest Rutherford (Fig. IUPAC.104.1), who won the Nobel Prize for developing the theory of radioactive transformations [645].

Rutherfordium is of interest in particle physics research, but it has no commercial applications. 261Rf was one of the decay products used to confirm the synthesis of copernicium in a particle accelerator experiment [634].

Rutherfordium named after Ernest Rutherford.

Scientists working at the Joint Institute for Nuclear Research in Dubna, Russia, first reported the production of rutherfordium in 1964. They bombarded atoms of plutonium-242 with ions of neon-22, forming what they believed to be atoms of rutherfordium-260 and four free neutrons. In 1969, a group of scientists working at the Lawrence Radiation Laboratory, now known as the Lawrence Berkeley Laboratory, in Berkeley, California, attempted to confirm the Dubna group's discovery. Lacking the equipment needed to accelerate neon ions, the Berkeley group, led by Albert Ghiorso, bombarded atoms of californium-248 and californium-249 with ions of carbon-12 and carbon-13, producing atoms of rutherfordium-257, rutherfordium-258, rutherfordium-259 and rutherfordium-261. They were, however, unable to produce the same isotope as the Dubna group. Credit for the discovery of rutherfordium is still under debate. Rutherfordium's most stable isotope, rutherfordium-263, has a half-life of about 10 minutes and decays through spontaneous fission.

In 1964, workers at the Joint Nuclear Research Institute at Dubna (U.S.S.R.) bombarded plutonium with accelerated 113 to 115 MeV neon ions. By measuring fission tracks in a special glass with a microscope, they detected an isotope that decays by spontaneous fission. They suggested that this isotope, which had a half-life of 0.3 +/- 0.1 s might be 260-104, produced by the following reaction: 242Pu + 22Ne >260Rf +4n.

Element 104, the first transactinide element, is expected to have chemical properties similar to those of hafnium. It would, for example, form a relatively volatile compound with chlorine (a tetrachloride).

The Soviet scientists have performed experiments aimed at chemical identification, and have attempted to show that the 0.3-s activity is more volatile than that of the relatively nonvolatile actinide trichlorides. This experiment does not fulfill the test of chemically separating the new element from all others, but it provides important evidence for evaluation. Data issued by Soviet scientists reduced the half-life of the isotope they worked with from 0.3 to 0.15 s.

Gambar

Sifat

Fisika

Jari-jari atom (empiris)
150 pm Bandingkan Jari-jari atom (empiris) semua unsur →
Massa jenis
2,33 × 104 kg/m³ Bandingkan Massa jenis semua unsur →
Fase pada STP
Padat Bandingkan Fase pada STP semua unsur →
Titik lebur
2126,85 °C Bandingkan Titik lebur semua unsur →
Titik didih
5526,85 °C Bandingkan Titik didih semua unsur →

Kimia

Afinitas elektron
0,65 eV
Energi ionisasi (ke-1)
6,02 eV Bandingkan Energi ionisasi (ke-1) semua unsur →
Energi ionisasi (ke-2)
14,350049 eV Bandingkan Energi ionisasi (ke-2) semua unsur →
Energi ionisasi (ke-3)
23,840082 eV Bandingkan Energi ionisasi (ke-3) semua unsur →
Energi ionisasi (ke-4)
31,87011 eV Bandingkan Energi ionisasi (ke-4) semua unsur →
Energi ionisasi (ke-5)
64,00022 eV Bandingkan Energi ionisasi (ke-5) semua unsur →
Bilangan oksidasi
+3, +4 Bandingkan Bilangan oksidasi semua unsur →
Elektron valensi
4 Bandingkan Elektron valensi semua unsur →
Konfigurasi elektron
[Rn] 7s2 5f14 6d2

Termodinamika

Tidak tersedia

Nuklir

Proton
104 Bandingkan Proton semua unsur →
Neutron
162 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)
267
Isotop paling stabil
Rf-266
Tahun penemuan
1964

Kelimpahan

Tidak tersedia

Struktur Kristal

Tidak tersedia

Struktur Elektronik

Elektron per kulit
2, 8, 18, 32, 32, 10, 2 Bandingkan Elektron per kulit semua unsur →

Pengenal

Nomor CAS
53850-36-5 Bandingkan Nomor CAS semua unsur →
Simbol term
3F2
InChI
InChI=1S/Rf
Kunci InChI
YGPLJIIQQIDVFJ-UHFFFAOYSA-N

Konfigurasi Elektron Diprediksi

Muatan ion
Proton 104
Elektron 104
Muatan Netral
Konfigurasi Rf: 5f¹⁴ 6d² 7s²
Konfigurasi elektron
Diprediksi
[Rn] 5f¹⁴ 6d² 7s²
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f¹⁴ 6d² 7s²
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
6d
2/10 2↑
Total elektron: 104 Tidak berpasangan: 2 ?

Model atom

Proton 104
Neutron 154
Elektron 104
Nomor massa 258
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
262 Radioaktif262,10992 ± 0,00024Tidak tersedia250 ms
254 Radioaktif254,10005 ± 0,0003Tidak tersedia22.9 us
260 Radioaktif260,10644 ± 0,00022Tidak tersedia21 ms
253 Radioaktif253,10044 ± 0,00044Tidak tersedia13 ms
258 Radioaktif258,103428 ± 0,000034Tidak tersedia12.5 ms
Diukur

Fase / Wujud

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

Alasan: 2101,8 °C di bawah titik lebur (2126,85 °C)

Titik lebur 2126,85 °C
Titik didih 5526,85 °C
Di bawah titik lebur sebesar 2101,8 °C
0 K Suhu saat ini: 25 °C 6000 K
Linimasa fase

Skematis, tidak sesuai skala

Padat
Cair
Gas
Peleburan
Pendidihan
25°C
Padat
Cair
Gas
Saat ini

Titik transisi fase

Titik lebur Diprediksi
2126,85 °C
Titik didih Diprediksi
5526,85 °C
Fase saat ini Diprediksi
Padat

Massa jenis

Massa jenis referensi Diprediksi
2,33e+4 kg/m³

Pada kondisi standar

Massa jenis saat ini Diprediksi
2,33e+4 kg/m³

Pada kondisi standar

Spektrum Atom

Menampilkan 10 dari 93. Diurutkan berdasarkan muatan ion (menaik).

Data Tingkat Energi ?

IonMuatanTingkat energi
Rf I 02
Rf II +12
Rf III +22
Rf IV +32
Rf V +42
Rf VI +52
Rf VII +62
Rf VIII +72
Rf IX +82
Rf X +92
Data Tingkat Energi NIST →
104 Rf 263

Rutherfordium — Visualisasi Orbital Atom

[Rn]7s25f146d2
Tingkat energi 2 8 18 32 32 10 2
Bilangan oksidasi +3, +4
HOMO 6d n=6 · l=2 · m=-2
Rutherfordium — Pratinjau Visualisasi Orbital Atom
Three.js hanya dimuat saat diminta
104 Rf 263

Rutherfordium — Visualisasi Struktur Kristal

Data struktur kristal tidak tersedia

Senyawa

Rf
267,122 u

Isotop (5)

In 1969 Ghiorso, Nurmia, Harris, K.A.Y. Eskola, and P.L. Eskola of the University of California at Berkeley reported that they had positively identified two, and possibly three isotopes of Element 104. The group indicated that, after repeated attempts, they produced isotope 260104 reported by the Dubna groups in 1964.

Nomor massaMassa atom (u)Kelimpahan alamiWaktu paruhMode peluruhan
262 Radioaktif262,10992 ± 0,00024Tidak tersedia250 ms
SF ≈100%
254 Radioaktif254,10005 ± 0,0003Tidak tersedia22.9 us
SF ≈100%α<1.5%
260 Radioaktif260,10644 ± 0,00022Tidak tersedia21 ms
SF ≈100%α ?β+ ?
253 Radioaktif253,10044 ± 0,00044Tidak tersedia13 ms
SF ≈100%α ?
258 Radioaktif258,103428 ± 0,000034Tidak tersedia12.5 ms
SF =95.1±1.6%α =4.9±1.6%
262 Radioaktif
Massa atom (u) 262,10992 ± 0,00024
Kelimpahan alami Tidak tersedia
Waktu paruh 250 ms
Mode peluruhan
SF ≈100%
254 Radioaktif
Massa atom (u) 254,10005 ± 0,0003
Kelimpahan alami Tidak tersedia
Waktu paruh 22.9 us
Mode peluruhan
SF ≈100%α<1.5%
260 Radioaktif
Massa atom (u) 260,10644 ± 0,00022
Kelimpahan alami Tidak tersedia
Waktu paruh 21 ms
Mode peluruhan
SF ≈100%α ? +1
253 Radioaktif
Massa atom (u) 253,10044 ± 0,00044
Kelimpahan alami Tidak tersedia
Waktu paruh 13 ms
Mode peluruhan
SF ≈100%α ?
258 Radioaktif
Massa atom (u) 258,103428 ± 0,000034
Kelimpahan alami Tidak tersedia
Waktu paruh 12.5 ms
Mode peluruhan
SF =95.1±1.6%α =4.9±1.6%

Sifat Lanjutan

Jari-jari Kovalen (Lanjutan)

Jari-jari kovalen (Pyykkö)
157 pm
Jari-jari kovalen (Pyykkö, ikatan rangkap dua)
140 pm
Jari-jari kovalen (Pyykkö, ikatan rangkap tiga)
131 pm

Skala Penomoran

Mendeleev
46

Polarizabilitas & Dispersi

Polarizabilitas dipol
112 a.u.
Polarizabilitas dipol (ketidakpastian)
10 a.u.

Kategori Bilangan Oksidasi

+3 extended
+4 main

Data Referensi Lanjutan

Mode Peluruhan Isotop (33)
IsotopModeIntensitas
253SF100%
253A—
254SF100%
254A1,5%
255A52,8%
255SF47,2%
255B+6%
256SF99,7%
256A0,3%
257A89,3%

Data Tambahan

Referensi

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

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)
Rutherfordium

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
Rutherfordium

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
Rutherfordium

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
Rutherfordium

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
Rutherfordium

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

Terakhir diperbarui:

Data terverifikasi:

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