Fm 100

Fermium (Fm)

actinide
주기: 7 블록: f

Solid

표준 원자량

[257]

전자 배치

[Rn] 5f12 7s2

녹는점

1526.85 °C

끓는점

해당 없음

밀도

9700 kg/m³

산화 상태

+2, +3

전기 음성도(Pauling)

1.3

제1 이온화 에너지

6.5 eV

발견 연도

1952

원자 반지름

해당 없음

상세 정보

이름의 유래 Named in honor of the scientist Enrico Fermi.
발견 국가 United States
발견자 Argonne, Los Alamos, U of Calif

Fermium is a synthetic actinide and the element with atomic number 100. It is produced only in minute amounts in high-neutron-flux reactions and is studied mainly by radiochemical and nuclear methods. Its chemistry is dominated by the +3 oxidation state, broadly resembling that of other late actinides and lanthanides. No macroscopic metallic sample has been prepared, and most measured properties are isotope- or solution-specific.

Fermium does not occur naturally in the Earth’s crust. It was first identified in December 1952 by American scientists from the Argonne National Laboratory near Chicago, Illinois, the Los Alamos National Laboratory in Los Alamos, New Mexico, and The University of California Laboratory in Berkeley, California in the debris of thermonuclear weapons (Fig. IUPAC.100.1). The element was named for Enrico Fermi, who built the first man-made nuclear reactor. 255Fm (with a half-life of 20 h) was the first fermium isotope identified. Fermium is the heaviest element that can be formed by neutron bombardment of lighter elements and is thus the heaviest element that can be synthesized in macroscopic quantities [632], [633].

Fermium is of interest in particle physics research, but it has no commercial applications. 253Fm was one of the decay products used to confirm synthesis of copernicium in a particle accelerator experiment [634].

Fermium is the heaviest synthetic element that can be formed by neutron bombardment of lighter elements, and hence the heaviest element that can be prepared in macroscopic quantities. The chemical properties of fermium have been studied solely using tracer amounts and innovative experimental techniques are required. Fermium metal has not been prepared, however measurements have been made on fermium alloys with rare earth metals and a number of predictions have been made. It was deduced that fermium metal prefers a divalent state but with modest compression can form a trivalent state. Other measurements on mixed fermium alloys and compounds include the magnetic moment, inner-shell binding energies, x-ray energies, sublimation enthalpy, etc.

The chemistry of fermium is typical of the late actinides, with a dominance of the +3 oxidation state but also a tendency toward an accessible +2 oxidation state. In the solid state no pure fermium compounds have been prepared, however Fm(III) has been studied by co-crystallization techniques as a trace component in a rare earth matrix with the same charge. Fermium co-precipitates with rare earth fluorides and hydroxides. In aqueous solution, fermium exists in solution as the Fm3+ ion, which has a hydration number of 16.9 and an acid dissociation constant of 1.6 × 10-4 (pKa = 3.8). Fm3+ forms complexes with a wide variety of organic ligands with hard donor atoms such as oxygen, and these complexes are usually more stable than those of the lighter actinides. It also forms complexes with ligands such as chloride or nitrate and, again, these complexes appear to be more stable than those formed by einsteinium or californium. Bonding in the heavier actinides is mostly ionic in character and the ionic radius of the Fm3+ ion is smaller than the preceding An3+ ions because of the actinide contraction. This is the result of a higher effective nuclear charge of fermium, and thus fermium forms shorter and stronger metal–ligand bonds. In the heavier actinides there is an increasing tendency to form a divalent ion that emerges at einsteinium. Fm3+ can be readily reduced to stable Fm2+ using moderately strong reducing agents such as samarium(II) chloride. In aqueous media, the Fm(III)/Fm(III) redox couple has been investigated via radio-electrochemistry and other techniques. The electrode potentials have been estimated to be similar to that of the ytterbium redox couple. The redox potentials for the various fermium couples have been measured and/or estimated by various workers: Fm3+ → Fm2+ (- 1.15 V); Fm2+ → Fm0 (-2.37 V), all versus the Normal Hydrogen Electrode.

Fermium was discovered by a team of scientists led by Albert Ghiorso in 1952 while studying the radioactive debris produced by the detonation of the first hydrogen bomb. The isotope they discovered, fermium-255, has a half-life of about 20 hours and was produced by combining 17 neutrons with uranium-238, which then underwent eight beta decays. Today, fermium is produced though a lengthy chain of nuclear reactions that involves bombarding each isotope in the chain with neutrons and then allowing the resulting isotope to undergo beta decay. Fermium's most stable isotope, fermium-257, has a half-life of about 100.5 days. It decays into californium-253 through alpha decay or decays through spontaneous fission.

Fermium, element 100, is the eighth transuranium element of the actinide series and is named after the Italian physicist and Nobel Laureate Enrico Fermi. Element 100 was first discovered in 1952 in the fallout from the 10-megaton "Ivy Mike" nuclear test in the south Pacific the first successful test of a hydrogen fusion bomb. Researchers identified a new Pu-244 isotope found on filter papers on drone aircraft flown through the fallout. They determined that it could only have formed by the unexpected absorption of six neutrons by uranium-238 followed by successive beta-decays. At the time, the absorption of neutrons by a heavy nucleus was thought to be a rare process, but the identification of Pu-244 raised the possibility that still more neutrons could have been absorbed by the uranium nuclei leading to additional new elements.

Element 99, einsteinium was discovered almost immediately on other filter papers by Albert Ghiorso and co-workers at the Lawrence Berkeley Laboratory in collaboration with Argonne and Los Alamos National Laboratories, demonstrating that 15 neutrons were captured by U-238! The subsequent discovery of fermium required more material, as the yield of element 100 was expected to be at least an order of magnitude lower than that of einsteinium. So, contaminated coral from ground zero on Eniwetok atoll was shipped to Berkeley for processing and analysis. About two months after the Ivy-Mike test, a new activity was isolated emitting high-energy α-particles (7.1 MeV) with a half-life of about 1 day. It was the β- decay daughter of an isotope of einsteinium, and it had to be an isotope of element 100. : It was identified as 255Fm (half-life 20.07 hours). The discovery of the new elements, and the new data on neutron capture, was kept secret on the orders of the U.S. Military until 1955 due to Cold War tensions. Later the Berkeley team was able to prepare elements 99 and 100 in the lab by neutron bombardment of Pu-239 in a cyclotron. They published this work in 1954, with the disclaimer that these were not the first studies that had been carried out on the element. The 'Ivy Mike' studies were later declassified and published in 1955. Meanwhile, a group at the Nobel Institute for Physics in Stockholm independently claimed discovery of element 100 by producing an isotope with a 30-minute half-life and published their work in May 1954. Nevertheless, the historical precedence of the Berkeley team was generally recognized, and with it the prerogative to name the new element in honor of the recently deceased Enrico Fermi, the developer of the first artificial self-sustained nuclear reactor.

이미지

특성

물리적 특성

반데르발스 반지름
245 pm 모든 원소의 반데르발스 반지름 비교 →
밀도
9700 kg/m³ 모든 원소의 밀도 비교 →
STP에서의 상
고체 모든 원소의 STP에서의 상 비교 →
녹는점
1526.85 °C 모든 원소의 녹는점 비교 →

화학적 특성

전기 음성도(Pauling)
1.3 모든 원소의 전기 음성도(Pauling) 비교 →
전자 친화도
0.339 eV
제1 이온화 에너지
6.5 eV 모든 원소의 제1 이온화 에너지 비교 →
제2 이온화 에너지
12.400043 eV 모든 원소의 제2 이온화 에너지 비교 →
제3 이온화 에너지
23.20008 eV 모든 원소의 제3 이온화 에너지 비교 →
제4 이온화 에너지
39.300135 eV 모든 원소의 제4 이온화 에너지 비교 →
제5 이온화 에너지
55.000189 eV 모든 원소의 제5 이온화 에너지 비교 →
산화 상태
+2, +3 모든 원소의 산화 상태 비교 →
원자가 전자
3 모든 원소의 원자가 전자 비교 →
전자 배치
[Rn] 5f12 7s2

열역학적 특성

승화열
4.145722 eV
원자화열
4.145722 eV

핵 특성

양성자 수
100 모든 원소의 양성자 수 비교 →
중성자 수
157 모든 원소의 중성자 수 비교 →
알려진 동위원소 수
20 모든 원소의 알려진 동위원소 수 비교 →
안정 동위원소 수
0 모든 원소의 안정 동위원소 수 비교 →
질량수(가장 안정한 동위원소)
257
가장 안정한 동위원소
Fm-257
발견 연도
1952

존재비

해당 없음

결정 구조

해당 없음

전자 구조

전자껍질별 전자 수
2, 8, 18, 32, 30, 8, 2 모든 원소의 전자껍질별 전자 수 비교 →

식별자

CAS 등록 번호
7440-72-4 모든 원소의 CAS 등록 번호 비교 →
항 기호
3H6
InChI
InChI=1S/Fm
InChI 키
MIORUQGGZCBUGO-UHFFFAOYSA-N

전자 배치 측정값

이온 전하
양성자 100
전자 100
전하 중성
배치 Fm: 5f¹² 7s²
전자 배치
측정값
[Rn] 5f¹² 7s²
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f¹² 7s²
오비탈 도표
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
12/14 2↑
총 전자 수: 100 홀전자: 2 ?

원자 모형

양성자 100
중성자 143
전자 100
질량수 243
안정성 방사성

동위원소에 따라 중성자 수, 질량, 안정성은 달라지지만, 중성 원자의 전자 배치는 달라지지 않습니다.

개략적인 원자 모형이며 실제 비율과 다릅니다.

원자 지문

방출 / 흡수 스펙트럼

0 / 0 (0 세기 정보가 있는 선 0개)
측정값
방출 가시광선: 380–750 nm

동위원소 분포

안정 동위원소가 없습니다.

질량수원자 질량(u)천연 존재비반감기
242 방사성242.07343 ± 0.00043해당 없음800 us
241 방사성241.07421 ± 0.00032해당 없음730 us
258 방사성258.09708 ± 0.00022해당 없음370 us
243 방사성243.07446 ± 0.00023해당 없음231 ms
256 방사성256.0917745 ± 0.0000078해당 없음157.1 분
측정값

상 / 상태

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

이유: 승화점(1526.85 °C)보다 1501.8 °C 낮음

승화점 1526.85 °C
0 K 현재 온도: 25 °C 6000 K
상 변화 도표

개략도이며 실제 비율과 다름

고체
기체
승화점
25°C
고체
액체
기체
현재

상전이점

승화점 문헌값
1526.85 °C
현재 상 계산값
고체

전이 에너지

승화열 문헌값
4.145722 eV

승화점에서 1 mol을 승화시키는 데 필요한 에너지

밀도

기준 밀도 문헌값
9700 kg/m³

표준 조건에서

현재 밀도 계산값
9700 kg/m³

표준 조건에서

원자 스펙트럼

전체 100개 중 10개를 표시합니다. 이온 전하순으로 정렬되었습니다(오름차순).

보유 에너지 준위 데이터 ?

이온전하준위
Fm I 02
Fm II +12
Fm III +22
Fm IV +32
Fm V +42
Fm VI +52
Fm VII +62
Fm VIII +72
Fm IX +82
Fm X +92
NIST 보유 에너지 준위 데이터 →
100 Fm 257

Fermium — 원자 오비탈 시각화 도구

[Rn] 5f12 7s2
에너지 준위 2 8 18 32 30 8 2
산화 상태 +2, +3
HOMO 5f n=5 · l=3 · m=-3
Fermium — 원자 오비탈 시각화 도구 미리보기
Three.js는 요청할 때만 불러옵니다
100 Fm 257

Fermium — 결정 구조 시각화 도구

결정 구조 데이터 없음

이온 반지름

전하배위스핀반지름
+39해당 없음110.5 pm

화합물

Fm
257.095 u
Fm
255.090 u
Fm
254.087 u
Fm
257.095 u
Fm
252.082 u
Fm
253.085 u

동위원소 (5)

A total of 21 known isotopes of fermium exist with atomic weights from 242 to 260, including 2 that are metastable. Fermium-257 is the longest-lived with a half-life of 100.5 days. Other relatively long-lived isotopes include Fm-253 (3 days), Fm-252 (25.4 hours) and Fm-255 (~20 hours). Fm-250, with a half-life of 30 minutes, was shown to be a decay product of nobelium, element 102 and the chemical identification of the isotope 250Fm confirmed the production and discovery of element 102. All the remaining isotopes of fermium have half-lives ranging from 30 minutes to less than a millisecond. The neutron-capture product of fermium-257, 258Fm, undergoes spontaneous fission with a half-life of just 370 microseconds; 259Fm and 260Fm are also unstable with respect to spontaneous fission (t½ = 1.5 s and 4 ms respectively). This means that the neutron capture production chain essentially terminates at mass number 257 because of the very short spontaneous fission half-lives of the heavier isotopes.

질량수원자 질량(u)천연 존재비반감기붕괴 방식
242 방사성242.07343 ± 0.00043해당 없음800 us
SF ≈100%α ?
241 방사성241.07421 ± 0.00032해당 없음730 us
SF =?α<14% β+<12%
258 방사성258.09708 ± 0.00022해당 없음370 us
SF ≈100%α ?
243 방사성243.07446 ± 0.00023해당 없음231 ms
α =91±0.3%SF =9±0.3%β+ ?
256 방사성256.0917745 ± 0.0000078해당 없음157.1 분
SF =91.9±0.3%α =8.1±0.3%
242 방사성
원자 질량(u) 242.07343 ± 0.00043
천연 존재비 해당 없음
반감기 800 us
붕괴 방식
SF ≈100%α ?
241 방사성
원자 질량(u) 241.07421 ± 0.00032
천연 존재비 해당 없음
반감기 730 us
붕괴 방식
SF =?α<14% +1
258 방사성
원자 질량(u) 258.09708 ± 0.00022
천연 존재비 해당 없음
반감기 370 us
붕괴 방식
SF ≈100%α ?
243 방사성
원자 질량(u) 243.07446 ± 0.00023
천연 존재비 해당 없음
반감기 231 ms
붕괴 방식
α =91±0.3%SF =9±0.3% +1
256 방사성
원자 질량(u) 256.0917745 ± 0.0000078
천연 존재비 해당 없음
반감기 157.1 분
붕괴 방식
SF =91.9±0.3%α =8.1±0.3%

확장 특성

공유 결합 반지름(확장)

공유 결합 반지름(Pyykkö)
167 pm

반데르발스 반지름

UFF
328.6 pm

번호 척도

Mendeleev
36
Pettifor
37
Glawe
44

전기 음성도 척도

Ghosh
0

분극률 및 분산

쌍극자 분극률
113 a.u.
쌍극자 분극률(불확도)
20 a.u.

상전이 및 동소체

녹는점1800.15 K

산화 상태 분류

+2 extended
+3 main

심화 참고 데이터

결정 반지름 상세 정보 (1)
전하CN스핀rcrystal (pm)기원
3IX—124.5
동위원소 붕괴 방식 (46)
동위원소모드세기
241SF—
241A14%
241B+12%
242SF100%
242A—
243A91%
243SF9%
243B+—
244SF97%
244B+2%

추가 데이터

Production

Production of this element (from raw materials or other compounds containing the element).

Because of the short half-life of all fermium isotopes, all that may have been present on the Earth during its formation has long since decayed away. Einsteinium and fermium did occur in the natural nuclear fission reactor at Oklo, but no longer exist. Fermium is produced as the result of multiple neutron captures in lighter elements, such as uranium and curium, followed by successive beta decays. The probability of such events increases with increased neutron flux, and nuclear explosions are the most powerful neutron sources on Earth. Fermium is also produced by the bombardment of lighter actinides with neutrons in nuclear reactors or accelerators. Fermium-257 is the heaviest isotope that is obtained via neutron capture, and can only be produced in nanogram quantities. The major source is the 85 MW High Flux Isotope Reactor (HFIR) at the Oak Ridge National Laboratory in Tennessee, USA. In a HFIR "campaign", tens of grams of curium are irradiated to produce heavier actinides and picogram quantities of fermium. The quantities of fermium produced in 20–200 kiloton thermonuclear explosions are believed to be of the order of milligrams, although it is mixed in with a huge quantity of debris. Forty picograms of 257Fm were recovered from 10 kilograms of debris from the 'Hutch' nuclear test in 1969. After production, fermium must be separated from debris and a host of other actinides and lanthanide fission products by solvent extraction, ion exchange, etc.). The annual reactor production of fermium-257 is in the picogram range. However, pure 255Fm (half-life 20 hours) can be easily isolated by "milking" the beta-decay daughter of pure 255Es (half-life 39.8 days).

참고 문헌 (1)

참고 문헌

(9)
2 Atomic Mass Data Center (AMDC), International Atomic Energy Agency (IAEA)
Fm

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)
Fermium

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.

라이선스 안내: 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
Fermium

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/

라이선스 안내: Please see citation and linking information: https://education.jlab.org/faq/index.html
6 Los Alamos National Laboratory, U.S. Department of Energy
Fermium

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
Fermium

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
Fermium

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

9 PubChem Elements
Fermium

The element property data was retrieved from publications.

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