88
Ra
Radium
Atomic Mass 226
Electron Configuration [Rn]7s2
Oxidation States +2
Year Discovered 1898

Identifiers

Element Name Radium
Element Symbol Ra
InChI InChI=1S/Ra
InChIKey HCWPIIXVSYCSAN-UHFFFAOYSA-N

Properties

Atomic Weight

226

226

[226]

Electron Configuration

[Rn]7s2

Atomic Radius

Van der Waals Atomic Radius : 283 pm (Van der Waals)

Empirical Atomic Radius : 215pm (Empirical)

Covalent Atomic Radius : 221(2) pm (Covalent)

Oxidation States

+2

2

Ground Level

1S0

Ionization Energy

5.279 eV

5.2784239 ± 0.0000025 eV

Electronegativity

Pauling Scale Electronegativity : 0.9(Pauling Scale)

Allen Scale Electronegativity : 0.89(Allen Scale)

Electron Affinity

0eV

Atomic Spectra

Lines Holdings

Levels Holdings

Physical Description

Solid

Element Classification

Metal

Element Period Number

7

Element Group Number

2 - Alkaline Earth Metal

Density

5 grams per cubic centimeter

Melting Point

973 K (700°C or 1292°F)

700°C

Boiling Point

1413 K (1140°C or 2084°F)

1737°C

Estimated Crustal Abundance

9×10-7 milligrams per kilogram

Estimated Oceanic Abundance

8.9×10-11 milligrams per liter

History

Radium was discovered by Marie Sklodowska Curie, a Polish chemist, and Pierre Curie, a French chemist, in 1898. Marie Curie obtained radium from pitchblende, a material that contains uranium, after noticing that unrefined pitchblende was more radioactive than the uranium that was separated from it. She reasoned that pitchblende must contain at least one other radioactive element. Curie needed to refine several tons of pitchblende in order to obtain tiny amounts of radium and polonium, another radioactive element discovered by Curie. One ton of uranium ore contains only about 0.14 grams of radium. Today, radium can be obtained as a byproduct of refining uranium and is usually sold as radium chloride (RaCl2) or radium bromide (RaBr2) and not as a pure material. Radium's most stable isotope, radium-226, has a half-life of about 1600 years. It decays into radon-222 through alpha decay or into lead-212 by ejecting a carbon-14 nucleus.

Radium was discovered in 1898 by Madame Curie in the pitchblende or uraninite of North Bohemia, where it occurs. There is about 1 g of radium in 7 tons of pitchblende. The element was isolated in 1911 by Mme. Curie and Debierne by the electrolysis of a solution of pure radium chloride employing a mercury cathode; on distillation in an atmosphere of hydrogen, this amalgam yielded the pure metal.

Historical Atomic Weights

Year Atomic Weight (uncertainty) [u] Reference
1983 n/a https://doi.org/10.1351/pac198456060653
1969 226.0254(1) https://doi.org/10.1351/pac197021010091
1936 226.05 https://doi.org/10.1039/JR9370001893
1931 225.97 https://doi.org/10.1039/JR9310001617
1925 225.95 https://doi.org/10.1039/CT9252700913
1909 226.4 https://doi.org/10.1021/ja01931a001
1903 225 https://doi.org/10.1021/ja02003a001

Description

Radium is obtained commercially as bromide and chloride; it is doubtful if any appreciable stock of the isolated element now exists. The pure metal is brilliant white when freshly prepared, but blackens on exposure to air, probably due to formation of the nitride. It exhibits luminescence, as do its slats; it decomposes in water and is somewhat more volatile than barium. It is a member of the alkaline-earth group of metals. Radium imparts a carmine red color to a flame. Radium emits alpha, beta, and gamma rays and when mixed with beryllium produce neutrons. One gram of 226Ra undergoes 3.7 x 1010 disintegrations per second. The curie is defined as that amount of radioactivity which has the same disintegration rate as 1 g of 226Ra. Twenty five isotopes are now known; radium 226, the common isotope, has a half-life of 1600 years.

Users

The Curie, a unit used to describe the activity of a radioactive substance, is based on radium-226. It is equal to the number of atoms in a one gram sample of radium-226 that will decay in one second, or 37,000,000,000 decays per second.

Radium had been used to make self-luminous paints for watches, aircraft instrument dials and other instrumentation, but has largely been replaced by cobalt-60, a less dangerous radioactive source. A mixture of radium and beryllium will emit neutrons and is used as a neutron source. Radium is used to produce radon, a radioactive gas used to treat some types of cancer. A single gram of radium-226 will produce 0.000l milliliters of radon a day.

Radium is about one million times more active than uranium. The lab notebooks used by the Curies are too highly contaminated to be safely handled today.

One gram of radium produces about 0.0001 ml (stp) of emanation, or radon gas, per day. This is purged from the radium and sealed in minute tubes, which are used in the treatment of cancer and other diseases. Radium was used in the producing of self-luminous paints, neutron sources, and in medicine for the treatment of disease. Other radioisotopes, such as 60Co, are now being used in place of radium. Some of these sources are much more powerful, and others are safer to use. Radium loses about 1% of its activity in 25 years, being transformed into elements of lower atomic weight. Lead is a final product of disintegration. Stored radium and radium-containing products or minerals should be ventilated to prevent build-up of radon.

Sources

Originally, radium was obtained from the rich pitchblende ore found in Joachimsthal, Bohemia. The carnotite sands of Colorado furnish some radium, but richer ores are found in the Republic of Zaire and the Great Lake region of Canada. Radium is present in all uranium minerals, and could be extracted, if desired, from the extensive wastes of uranium processing. Large uranium deposits are located in Ontario, New Mexico, Utah, Australia, and elsewhere.

Compounds

See more information at the Radium compound page.

Element Forms

CID Name Formula SMILES Molecular Weight
9877911 radium-226 Ra [226Ra] 226.02541
6328144 radium Ra [Ra] 226.02541
6328553 radium-228 Ra [228Ra] 228.03107
6328538 radium-224 Ra [224Ra] 224.02021
6335825 radium-223 Ra [223Ra] 223.01850
6336607 radium-225 Ra [225Ra] 225.02361
6337591 radium-227 Ra [227Ra] 227.02918
25000466 radium-222 Ra [222Ra] 222.01537
6337593 radium-220 Ra [220Ra] 220.01103
6452485 radium-230 Ra [230Ra] 230.0371
10262582 radium-212 Ra [212Ra] 211.9998
90480252 radium-233 Ra [233Ra] 233.04759

Handling And Storage

Inhalation, injection, or body exposure to radium can cause cancer and other body disorders. The maximum permissible border in the total body for 226Ra is 7400 becquerel.

Isotopes

Stable Isotope Count 0

Isotopes in Earth/Planetary Science

The radioactive isotopes 223Ra (with a half-life of 275 h), 224Ra (with a half-life of 88 h), 226Ra (with a half-life of 1600 years), and 228Ra (with a half-life of 5.75 years) are used as tracers to determine water flow rates. They are ideal environmental tracers because they behave conservatively once released into a water mass (meaning only mixing and decay processes affect their distribution) [578]. The activity ratios A(224Ra)/A(223Ra), A(223Ra)/A(226Ra), A(224Ra)/A(228Ra), and A(228Ra)/A(226Ra) have been used in lake studies to monitor and detect water inflow and mixing, to determine sources of inflowing water, and to monitor introduced water masses as they move within a body of water (i.e. a lake) [578], [579]. For example, submarine groundwater discharge is an important pathway that transports dissolved substances from aquifers below a seabed to the coastal ocean. Submarine groundwater discharge can be difficult to quantify because it is both spatially and temporally variable. As a result, its relative importance in coastal ocean chemical budgets is commonly poorly known. Peterson et al. [572] used an hourly time series of measurements of multiple radium isotopes 223Ra, 224Ra, and 226Ra to quantify submarine groundwater discharge. They also used 222Rn (with a half-life of 3.8 days) measurements to independently quantify submarine groundwater discharge.

[572] R. N. Peterson, W. C. Burnett, M. Taniguchi, J. Chen, I. R. Santos, T. Ishitobi. J. Geophys. Res.113, C09021 (2008).
[578] United States Geological Survey. Resources on Isotopes-Periodic Table-Radium, U.S. Geological Survey (2014), Feb. 25; http://wwwrcamnl.wr.usgs.gov/isoig/period/ra_iig.html.
[579] T. F. Kraemer. Limnol. Oceanogr.50, 158 (2005).

Isotopes in Geochronology

226Ra and 228Ra can be used for dating materials up to a few thousand years in age because the half-lives of 226Ra and 228Ra are 1600 years and 5.75 years, respectively, even though the long-lived 226Ra is found in nature as a result of its continuous production by the decay of 238U. For example, long-lived 226Ra has been used to date a limestone cave in central Switzerland, corals in the Indian Ocean, and Pleistocene gravel terraces [580]. The activity ratio A(224Ra)/A(223Ra) is a potential age calculator for old lake water because the low 223Ra and 224Ra activities in old lake water are relatively unaffected by mixing [579].

[579] T. F. Kraemer. Limnol. Oceanogr.50, 158 (2005).
[580] J. Eikenberg. “Radium isotope systematics in nature: applications in geochronology and hydrogeochemistry”, in Habilitation Thesis, Earth Science Department.

Isotopes in Medicine

226Ra is used in brachytherapy (Fig. IUPAC.88.1), which is a method of localized treatment of various types of cancer. A sealed implant (such as a rod, seed, or needle) containing the radioactive isotope 226Ra is inserted into or near a patient’s tumor to apply a high dose of radiation to the tumor. The sealed implant is inserted by a physician or by an automated device (called a remote afterloader), and it is removed from the patient once the tumor is destroyed [75], [581].

Fig. IUPAC.88.1: Brachytherapy seeds shown with a penny (19-mm diameter) for scale (modified from [582]).

[75] J. Peterson, M. McDonell, L. Haroun, F. Monette, R. D. Hildebrand, A. Taboas. Radiological and Chemical Fact Sheets to Support Health Risk Analyses for Contaminated Areas, Prepared by Argonne National Laboratory Environmental Science Division in collaboration with U.S. Department of Energy, Richland Operations Office and Chicago Operations Office (2014), Feb. 22; http://www.remm.nlm.gov/ANL_ContaminantFactSheets_All_070418.pdf.
[581] United States Nuclear Regulatory Commission (U.S. NRC). Frequently Asked Questions (FAQs) Regarding Radium-226 Overview, United States Nuclear Regulatory Commission (U.S. NRC) (2017), April 8; https://scp.nrc.gov/narmtoolbox/radium%20faq102008.pdf.
[582] Oak Ridge Associated Universities. Seeds (ca. 1940s–1960s), Oak Ridge Associated Universities (2014), Feb. 25; http://www.orau.org/ptp/collection/brachytherapy/seeds.htm.

Isotope Mass and Abundance

Isotope Atomic Mass (uncertainty) [u] Abundance (uncertainty)
223Ra 223.0185023(27)
224Ra 224.0202120(23)
226Ra 226.0254103(25)
228Ra 228.0310707(26)

Atomic Mass, Half Life, and Decay

Nuclide Atomic Mass and Uncertainty [u] Half Life and Uncertainty Discovery Year Decay Modes, Intensities and Uncertainties [%]
201Ra 201.012814699 ± 0.000021794 20 ms ± 30 2005 α=100%
201Ram 201.012814699 ± 0.000021794 6 ms ± 5 2005 α=100%
202Ra 202.009742305 ± 0.000016122 4.1 ms ± 1.1 2005 α=100%
203Ra 203.009233907 ± 0.0000104 36 ms ± 13 1996 α≈100%; β+ ?
203Ram 203.009233907 ± 0.0000104 25 ms ± 5 1996 α≈100%; β+ ?
204Ra 204.006506855 ± 0.00000958 60 ms ± 9 1995 α≈100%; β+ ?
205Ra 205.006230692 ± 0.000024446 220 ms ± 50 1987 α≈100%; β+ ?
205Ram 205.006230692 ± 0.000024446 180 ms ± 50 1995 α≈100%; IT ?; β+ ?
206Ra 206.003827842 ± 0.000019332 240 ms ± 20 1967 α≈100%; β+ ?
207Ra 207.003772420 ± 0.000062572 1.38 s ± 0.18 1967 α≈86%; β+ ?
207Ram 207.003772420 ± 0.000062572 57 ms ± 8 1987 IT=85%[Estimated]; α=?; β+ ?
208Ra 208.001855012 ± 0.000009686 1.110 s ± 0.045 1967 α=87±0.3%; β+ ?
208Ram 208.001855012 ± 0.000009686 263 ns ± 17 1998 IT=100%
209Ra 209.001994902 ± 0.000006169 4.71 s ± 0.08 1967 α≈100%; β+ ?
209Ram 209.001994902 ± 0.000006169 117 us ± 5 2008 α≈90%; β+≈10%
210Ra 210.000475406 ± 0.000009868 4.0 s ± 0.1 1967 α≈100%; β+ ?
210Ram 210.000475406 ± 0.000009868 2.29 us ± 0.03 1998 IT=100%
211Ra 211.000893049 ± 0.000005331 12.6 s ± 1.2 1967 α≈100%; β+ ?
211Ram 211.000893049 ± 0.000005331 9.5 us ± 0.3 2004 IT=100%
212Ra 211.999786619 ± 0.000011007 13.0 s ± 0.2 1967 α=?; β+ ?
212Ram 211.999786619 ± 0.000011007 9.3 us ± 0.9 1986 IT=100%
212Ran 211.999786619 ± 0.000011007 850 ns ± 130 1986 IT=100%
213Ra 213.000370971 ± 0.00001054 2.73 m ± 0.05 1955 α=87±0.2%; β+=13±0.2%
213Ram 213.000370971 ± 0.00001054 2.20 ms ± 0.05 1976 IT≈99%; α=0.6±0.4%
214Ra 214.000099560 ± 0.000005636 2.437 s ± 0.016 1967 α=99.941±0.4%; β+=0.059±0.4%
214Ram 214.000099560 ± 0.000005636 118 ns ± 7 2004 IT=100%
214Ran 214.000099560 ± 0.000005636 67.3 us ± 1.5 1971 IT=99.91±0.7%; α=0.09±0.7%
214Rap 214.000099560 ± 0.000005636 295 ns ± 7 1979 IT=100%
214Raq 214.000099560 ± 0.000005636 279 ns ± 4 1979 IT=100%
214Rar 214.000099560 ± 0.000005636 225 ns ± 4 1979 IT=100%
214Rax 214.000099560 ± 0.000005636 128 ns ± 4 1992 IT=100%
215Ra 215.002718208 ± 0.00000773 1.669 ms ± 0.009 1967 α=100%
215Ram 215.002718208 ± 0.00000773 7.31 us ± 0.13 1983 IT=100%
215Ran 215.002718208 ± 0.00000773 1.39 us ± 0.07 1998 IT=100%
215Rap 215.002718208 ± 0.00000773 555 ns ± 10 1987 IT=100%
216Ra 216.003533534 ± 0.000008592 172 ns ± 7 1972 α=100%; ε<1e-8%
217Ra 217.006322676 ± 0.000007564 1.95 us ± 0.12 1970 α=100%
218Ra 218.007134297 ± 0.000010528 25.91 us ± 0.14 1970 α=100%
219Ra 219.010084715 ± 0.000007315 9 ms ± 2 1952 α=100%
219Ram 219.010084715 ± 0.000007315 10 ms ± 3 2018 α≈100%; IT ?
220Ra 220.011027542 ± 0.000008153 18.1 ms ± 1.2 1949 α=100%
221Ra 221.013917293 ± 0.00000497 25 s ± 4 1949 α=100%; 14C=1.2e-10±0.9%
222Ra 222.015373371 ± 0.000004781 33.6 s ± 0.4 1948 α=100%; 14C=3.0e-8±1%
223Ra 223.018500648 ± 0.000002243 11.4352 d ± 0.0010 1905 α=100%; 14C=8.9e-8±0.4%
224Ra 224.020210361 ± 0.000001944 3.6316 d ± 0.0014 1902 α=100%; 14C=4.0e-9±1.2%
225Ra 225.023610502 ± 0.000002786 14.82 d ± 0.19 1947 β-=100%
226Ra 226.025408186 ± 0.000002068 1.600 ky ± 0.007 1898 α=100%; 14C=2.6e-9±0.6%; 2β- ?
227Ra 227.029176205 ± 0.000002089 42.2 m ± 0.5 1953 β-=100%
228Ra 228.031068574 ± 0.000002141 5.75 y ± 0.03 1907 β-=100%
229Ra 229.034956703 ± 0.000016576 4.0 m ± 0.2 1975 β-=100%
230Ra 230.037054776 ± 0.000011053 93 m ± 2 1978 β-=100%
231Ra 231.041027085 ± 0.000012206 104 s ± 1 1983 β-=100%
231Ram 231.041027085 ± 0.000012206 ~53 us 2001 IT=100%
232Ra 232.043475267 ± 0.000009823 4.0 m ± 0.3 1983 β-=100%
233Ra 233.047594570 ± 0.000009235 30 s ± 5 1990 β-=100%
234Ra 234.050382100 ± 0.000009 30 s ± 10 1990 β-=100%; β-SF ?
235Ra 235.054890 ± 0.000322 [Estimated] 5 s [Estimated] 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.  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/
  5. 5.  Jefferson Lab, U.S. Department of Energy
    LICENSE
    Please see citation and linking information https https://www.jlab.org/privacy-and-security-notice
  6. 6.  Los Alamos National Laboratory, U.S. Department of Energy
  7. 7.  NIST Physical Measurement Laboratory
  8. 8.  PubChem Elements
    Radium

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