75
Re
Rhenium
Atomic Mass 186.207
Electron Configuration [Xe]6s24f145d5
Oxidation States +7, +6, +4
Year Discovered 1925

Identifiers

Element Name Rhenium
Element Symbol Re
InChI InChI=1S/Re
InChIKey WUAPFZMCVAUBPE-UHFFFAOYSA-N

Properties

Atomic Weight

186.207(1)

186.207

186.2

186.207(1)

Electron Configuration

[Xe]6s24f145d5

Atomic Radius

Van der Waals Atomic Radius : 217 pm (Van der Waals)

Empirical Atomic Radius : 135pm (Empirical)

Covalent Atomic Radius : 151(7) pm (Covalent)

Oxidation States

+7, +6, +4

7, 6, 5, 4, 3, 2, 1, 0, -1, -3 ​(a mildly acidic oxide)

Ground Level

6S5/2

Ionization Energy

7.88 eV

7.83352 ± 0.00011 eV

Electronegativity

Pauling Scale Electronegativity : 1.9(Pauling Scale)

Allen Scale Electronegativity : 1.6(Allen Scale)

Electron Affinity

0.15eV

0.38eV

Atomic Spectra

Lines Holdings

Levels Holdings

Physical Description

Solid

Element Classification

Metal

Element Period Number

6

Element Group Number

7

Density

20.8 grams per cubic centimeter

Melting Point

3459 K (3186°C or 5767°F)

3186°C

Boiling Point

5869 K (5596°C or 10105°F)

5630°C

Estimated Crustal Abundance

7×10-4 milligrams per kilogram

Estimated Oceanic Abundance

4×10-6 milligrams per liter

History

The name derives from the Latin rhenus for the Rhine river in Germany. Rhenium was discovered by x-ray spectroscopy in 1925 by German chemists Walter Noddack, Ida Tacke, and Otto Berg.

Rhenium was discovered by the German chemists Ida Tacke-Noddack, Walter Noddack and Otto Carl Berg in 1925. They detected rhenium spectroscopically in platinum ores and in the minerals columbite ((Fe, Mn, Mg)(Nb, Ta)2O6), gadolinite ((Ce, La, Nd, Y)2FeBe2Si2O10) and molybdenite (MoS2). Rhenium is present in these materials only in trace amounts. In 1928, Noddack and Berg were able to extract 1 gram of rhenium from 660 kilograms of molybdenite. Today, rhenium is obtained as a byproduct of refining molybdenum and copper.

Discovery of rhenium is generally attributed to Noddack, Tacke, and Berg, who announced in 1925 they had detected the element in platinum ore and columbite. They also found the element in gadolinite and molybdenite. By working up 660 kg of molybdenite in 1928 they were able to extract 1 g of rhenium.

Historical Atomic Weights

Year Atomic Weight (uncertainty) [u] Reference
1973 186.207(1) https://doi.org/10.1351/pac197437040589
1969 186.2(1) https://doi.org/10.1351/pac197021010091
1961 186.2 https://doi.org/10.1021/ja00881a001
1955 186.22 https://doi.org/10.1021/ja01595a001
1931 186.31 https://doi.org/10.1039/JR9310001617

Historical Isotopic Abundances

Year Isotope Abundance (uncertainty) Reference
2013 185Re 0.3740(5) https://doi.org/10.1515/pac-2015-0503
2013 187Re 0.6260(5) https://doi.org/10.1515/pac-2015-0503
1979 185Re 0.3740(2) https://doi.org/10.1351/pac198052102349
1979 187Re 0.6260(2) https://doi.org/10.1351/pac198052102349
1975 185Re 0.374 https://doi.org/10.1351/pac197647010075
1975 187Re 0.626 https://doi.org/10.1351/pac197647010075

Description

The element is silvery white with a metallic luster; its density is exceeded only by that of platinum, iridium, and osmium, and its melting point is exceeded only by that of tungsten and carbon.

The usual commercial form of the element is powder, but it can be consolidated by pressing and resistance-sintering in a vacuum or hydrogen atmosphere. This process produces a compact shape in excess of 90 percent of the density of the metal.

Annealed rhenium is very ductile, and can be bent, coiled, or rolled. Rhenium is used as an additive to tungsten and molybdenum -based alloys to impart useful properties.

Users

Rhenium is used in flash lamps for photography and for filaments in mass spectrographs and ion gages, but is most frequently used as an alloying agent in tungsten and molybdenum and as a catalyst for performing certain reactions to a type of hydrocarbon known as an olefin.

It is widely used as filaments for mass spectrographs and ion gauges. Rhenium-molybdenum alloys are superconductive at 10 K.

Rhenium is also used as an electrical contact material because it has good wear resistance and withstands arc corrosion. Thermocouples made of Re-W are used for measuring temperatures up to 2200C, and rhenium wire is used in photoflash lamps for photography.

Rhenium catalysts are exceptionally resistant to poisoning from nitrogen, sulfur, and phosphorus, and are used for hydrogenation of fine chemicals.

Sources

Rhenium does not occur free in nature or as a compound in a distinct mineral species. It is, however, widely spread throughout the earth's crust to the extent of about 0.001 ppm. Commercial rhenium in the U.S. today is obtained from molybdenum roaster-flue dusts obtained from copper-sulfide ores mined in the vicinity of Miami, Arizona and elsewhere in Arizona and in Utah.

Some molybdenum contains from 0.002% to 0.2% rhenium. More than 150,000 troy ounces of rhenium are now being produced yearly in the United States. The total estimated Free World reserve of rhenium metal is 3500 tons. Rhenium metal is prepared by reducing ammonium perrhentate with hydrogen at elevated temperatures.

Compounds

See more information at the Rhenium compound page.

Element Forms

CID Name Formula SMILES Molecular Weight
23947 rhenium Re [Re] 186.207
161105 rhenium-186 Re [186Re] 185.954989
161062 rhenium-187 Re [187Re] 186.955752
167082 rhenium-188 Re [188Re] 187.958114
177020 rhenium-177 Re [177Re] 176.9503
177539 rhenium-181 Re [181Re] 180.9501
25087171 rhenium-185 Re [185Re] 184.952958
177157 rhenium-182 Re [182Re] 181.951
177533 rhenium-184 Re [184Re] 183.95253
177675 rhenium-189 Re [189Re] 188.95923
25087175 rhenium-183 Re [183Re] 182.95082
177019 rhenium-178 Re [178Re] 177.9510
44154623 rhenium-180 Re [180Re] 179.9508

Isotopes

Stable Isotope Count 1
Summary Natural rhenium is a mixture of two stable isotopes. Twenty six other unstable isotopes are recognized.

Isotopes in Geochronology

The rhenium-osmium dating method is of special interest for the dating of rhenium-bearing ores, gold deposits, copper-nickel deposits, and meteorites. This method is based on the beta-decay of 187Re (having a half-life of 41.6×109 years) to 187Os, an example of which appears in Fig. IUPAC.75.1 [515].

Fig. IUPAC.75.1: Cross plot of n(¹⁸⁷Os)/n(¹⁸⁸Os) isotope-amount ratio and n(¹⁸⁷Re)/n(¹⁸⁸Os) amount ratio of marine and non-marine organic-rich sediments and coals from Egypt (modified from [515]). The Maghara area (about 200 km east of Cairo) has middle-Jurassic coal beds (about 165×10⁶ years old, identified by the green dotted line). The age of marine black shales in the Red Sea area was previously estimated as 74×10⁶ years old, identified by the blue dotted line. ¹⁸⁷Os is produced by decay of ¹⁸⁷Re. Samples from an older formation will have proportionally more ¹⁸⁷Os because of the longer accumulation time for ¹⁸⁷Os; thus, the slope of the line for the Maghara coals (turquoise triangles), having an age of 165×10⁶ years, is substantially higher than the slope of the Red Sea specimens. Note the analytical challenges in obtaining isotope-amount values that plot near the 165- and 74-million-year isochrons. Many of the values plot between the isochrons.

[515] H. M. Baioumy, L. B. Eglinton, B. Peucker-Ehrenbrink. Chem. Geol.285, 70 (2011).

Isotopes in Medicine

186Re (with a half-life of 89 h) is a beta-emitting radioisotope that is used for cancer treatment, in particular for pain relief in bone cancer and in rheumatoid arthritis (see radiosynovectomy). It is produced from the stable isotope 185Re via the 185Re (n, γ) 186Re reaction [188]. 186Re is also used for radiolabeling of cancer therapeutic agents [188]. 188Re (with a half-life of 17 h) is used to irradiate coronary arteries with beta particles during insertion of an angioplasty balloon (a tiny balloon that is inserted into an artery and inflated to flatten plaque build-up and improve blood flow) and in palliative therapy, particularly for bone metastases. The beta irradiation can decrease scar tissue formation after the overstretching of arteries by angioplasty.

[188] S. J. Adelstein, F. J. Manning. Isotopes for Medicine and the Life Sciences, pp. 20–25, National Academy Press, Washington DC (1995).

Isotope Mass and Abundance

Isotope Atomic Mass (uncertainty) [u] Abundance (uncertainty)
185Re 184.952 958(6) 0.3740(5)
187Re 186.955 752(5) 0.6260(5)
Isotope Atomic Mass (uncertainty) [u] Abundance (uncertainty)
185Re 184.9529545(13) 0.3740(2)
187Re 186.9557501(16) 0.6260(2)

Atomic Mass, Half Life, and Decay

Nuclide Atomic Mass and Uncertainty [u] Half Life and Uncertainty Discovery Year Decay Modes, Intensities and Uncertainties [%]
159Re 158.984106 ± 0.000327 [Estimated] 40 us [Estimated] 2006 p ?; α ?
159Rem 158.984106 ± 0.000327 [Estimated] 20 us ± 4 2006 p=92.5±3.5%; α=7.5±3.5%
160Re 159.981880 ± 0.000322 [Estimated] 611 us ± 7 1992 p=89±0.1%; α=11±0.1%
160Rem 159.981880 ± 0.000322 [Estimated] 2.8 us ± 0.1 2011 IT=100%
161Re 160.977624313 ± 0.00016093 440 us ± 1 1979 p≈100%; α ?
161Rem 160.977624313 ± 0.00016093 14.7 ms ± 0.3 1979 α=93.0±0.3%; p=7.0±0.3%
162Re 161.975896 ± 0.000215 [Estimated] 107 ms ± 13 1979 α=94±0.6%; β+ ?
162Rem 161.975896 ± 0.000215 [Estimated] 77 ms ± 9 1979 α=91±0.5%; β+ ?
163Re 162.972085434 ± 0.000019897 390 ms ± 70 1979 β+ ?; α=32±0.3%
163Rem 162.972085434 ± 0.000019897 214 ms ± 5 1979 α=66±0.4%; β+ ?
164Re 163.970507122 ± 0.000058566 719 ms ± 89 1979 α=?; β+ ?
164Rem 163.970507122 ± 0.000058566 890 ms ± 130 2009 β+ ?; α=3±0.1%
165Re 164.967085831 ± 0.000025328 1.6 s ± 0.6 1981 β+=86±0.8%; α=14±0.8%
165Rem 164.967085831 ± 0.000025328 1.74 s ± 0.06 1978 β+=87±0.1%; α=13±0.1%
166Re 165.965821216 ± 0.000094731 2.25 s ± 0.21 1978 β+=88±0.7%; α=12±0.7%
166Rep 165.965821216 ± 0.000094731 3 s [Estimated] β+ ?; α ?; IT ?
167Re 166.962604 ± 0.000043 [Estimated] 3.4 s ± 0.4 1992 α≈100%; β+=?
167Rem 166.962604 ± 0.000043 [Estimated] 5.9 s ± 0.3 1984 β+ ?; α=?
168Re 167.961572607 ± 0.000033087 4.4 s ± 0.1 1992 β+≈100%; α≈0.005%
169Re 168.958765979 ± 0.000012204 8.1 s ± 0.5 1978 β+=?; α=0.005±0.3%
169Rem 168.958765979 ± 0.000012204 15.1 s ± 1.5 1984 β+ ?; α= ?; IT ?
170Re 169.958234844 ± 0.000012267 >1 s [Estimated] 1974 β+=100%
170Rem 169.958234844 ± 0.000012267 9.2 s ± 0.2 1974 β+=?; IT ?
170Ren 169.958234844 ± 0.000012267 130 ns ± 10 1974 IT=100%
171Re 170.955716000 ± 0.00003 15.2 s ± 0.4 1987 β+=100%
172Re 171.955376165 ± 0.000038183 55 s ± 5 1977 β+=100%
172Rem 171.955376165 ± 0.000038183 15 s ± 3 1972 β+=100%
173Re 172.953243000 ± 0.00003 2.0 m ± 0.3 1986 β+=100%
174Re 173.953115000 ± 0.00003 2.40 m ± 0.04 1972 β+=100%
174Rem 173.953115000 ± 0.00003 1 m >1us [Estimated] 2012 IT ?; β+ ?
175Re 174.951381000 ± 0.00003 5.89 m ± 0.05 1967 β+=100%
176Re 175.951623000 ± 0.00003 5.3 m ± 0.3 1967 β+=100%
177Re 176.950328000 ± 0.00003 14 m ± 1 1957 β+=100%
177Rem 176.950328000 ± 0.00003 >100 ns IT=100%
177Ren 176.950328000 ± 0.00003 50 us ± 10 1972 IT=100%
178Re 177.950989000 ± 0.00003 13.2 m ± 0.2 1957 β+=100%
179Re 178.949989686 ± 0.00002645 19.5 m ± 0.1 1960 β+=100%
179Rem 178.949989686 ± 0.00002645 95 us ± 25 1972 IT=100%
179Ren 178.949989686 ± 0.00002645 408 ns ± 12 1972 IT=100%
179Rep 178.949989686 ± 0.00002645 466 us ± 15 1989 IT=100%
180Re 179.950791568 ± 0.000022965 2.46 m ± 0.03 1955 β+=100%
180Rem 179.950791568 ± 0.000022965 >1 us [Estimated] 2005 IT≈100%; β+ ?
180Ren 179.950791568 ± 0.000022965 9.0 us ± 0.7 2005 IT=100%
181Re 180.950061507 ± 0.000013471 19.9 h ± 0.7 1957 β+=100%
181Rem 180.950061507 ± 0.000013471 156.7 ns ± 1.9 1967 IT=100%
181Ren 180.950061507 ± 0.000013471 250 ns ± 10 1974 IT=100%
181Rep 180.950061507 ± 0.000013471 11.5 us ± 0.9 2000 IT=100%
181Req 180.950061507 ± 0.000013471 1.2 us ± 0.2 2000 IT=100%
182Re 181.951211560 ± 0.000109483 64.2 h ± 0.5 1950 β+=100%
182Rem 181.951211560 ± 0.000109483 14.14 h ± 0.45 1950 β+=100%
182Ren 181.951211560 ± 0.000109483 585 ns ± 30 1969 IT=100%
182Rep 181.951211560 ± 0.000109483 780 ns ± 90 1984 IT=100%
183Re 182.950821306 ± 0.000008625 70.0 d ± 1.4 1950 ε=100%
183Rem 182.950821306 ± 0.000008625 1.04 ms ± 0.04 1966 IT=100%
184Re 183.952528073 ± 0.00000459 35.4 d ± 0.7 1940 β+=100%
184Rem 183.952528073 ± 0.00000459 169 d ± 8 1964 IT=74.5±0.8%; ε=25.5±0.8%
185Re 184.952958320 ± 0.000000879 Stable 1931 IS=37.40±0.5%
185Rem 184.952958320 ± 0.000000879 200 ns ± 4 1997 IT=100%
186Re 185.954989172 ± 0.00000088 3.7185 d ± 0.0005 1939 β-=92.53±1%; ε=7.47±1%
186Rem 185.954989172 ± 0.00000088 ~200 ky 1972 IT≈100%; β- ?
187Re 186.955752217 ± 0.000000791 41.6 Gy ± 0.02 1931 IS=62.60±0.5%; β-=100%; α=0%
187Rem 186.955752217 ± 0.000000791 555.3 ns ± 1.7 1949 IT=100%
187Ren 186.955752217 ± 0.000000791 354 ns ± 62 2003 IT=100%
188Re 187.958113658 ± 0.000000792 17.005 h ± 0.003 1939 β-=100%
188Rem 187.958113658 ± 0.000000792 18.59 m ± 0.04 1953 IT=100%
189Re 188.959227764 ± 0.000008793 24.3 h ± 0.4 1963 β-=100%
189Rem 188.959227764 ± 0.000008793 2 us [Estimated] IT ?
189Ren 188.959227764 ± 0.000008793 223 us ± 14 2016 IT=100%
190Re 189.961800064 ± 0.000005227 3.0 m ± 0.2 1955 β-=100%
190Rem 189.961800064 ± 0.000005227 3.1 h ± 0.2 1962 β-=54.4±2%; IT=45.6±2%
191Re 190.963123322 ± 0.000011019 9.8 m ± 0.5 1963 β-=100%
191Rem 190.963123322 ± 0.000011019 20 us [Estimated] IT ?
191Ren 190.963123322 ± 0.000011019 50.6 us ± 3.5 2011 IT=100%
192Re 191.966088000 ± 0.000076 15.4 s ± 0.5 1965 β-=100%
192Rem 191.966088000 ± 0.000076 88 us ± 8 2005 IT=100%
192Ren 191.966088000 ± 0.000076 <500 ms 2012 β- ?; IT ?
193Re 192.967545000 ± 0.000042 3 m >300ns [Estimated] 1999 β- ?
193Rem 192.967545000 ± 0.000042 69 us ± 6 2005 IT=100%
194Re 193.970735 ± 0.000215 [Estimated] 5 s ± 1 1999 β-=100%
194Rem 193.970735 ± 0.000215 [Estimated] 45 us ± 18 2011 IT=100%
194Ren 193.970735 ± 0.000215 [Estimated] 25 s ± 8 2012 β-=100%
194Rep 193.970735 ± 0.000215 [Estimated] 100 s ± 10 2012 β-=100%
195Re 194.972560 ± 0.000322 [Estimated] 6 s ± 1 2008 β-=100%
196Re 195.975996 ± 0.000322 [Estimated] 2.4 s ± 1.5 2008 β- ?
196Rem 195.975996 ± 0.000322 [Estimated] 3.6 us ± 0.6 2009 IT=100%
197Re 196.978153 ± 0.000322 [Estimated] 400 ms >300ns [Estimated] 2009 β- ?
198Re 197.981760 ± 0.000429 [Estimated] 1 s >300ns [Estimated] 2009 β- ?; β-n ?
199Re 198.984187 ± 0.000429 [Estimated] 250 ms >300ns [Estimated] 2012 β- ?

Information Sources

  1. 1.  PubChem
  2. 2.  Atomic Mass Data Center (AMDC), International Atomic Energy Agency (IAEA)
  3. 3.  IUPAC Commission on Isotopic Abundances and Atomic Weights (CIAAW)
  4. 4.  Jefferson Lab, U.S. Department of Energy
    LICENSE
    Please see citation and linking information https https://www.jlab.org/privacy-and-security-notice
  5. 5.  Los Alamos National Laboratory, U.S. Department of Energy
  6. 6.  NIST Physical Measurement Laboratory
  7. 7.  IUPAC Periodic Table of the Elements and Isotopes (IPTEI)
    LICENSE
    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.
    https://creativecommons.org/licenses/by-nc-nd/4.0/
  8. 8.  PubChem Elements
    Rhenium

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