Curie (unit)

Last updated
Curie
Radium226.jpg
A sample of radium, the element which was used in the original definition of the curie.
General information
Unit of Activity
SymbolCi
Named after Pierre Curie and Marie Curie
Conversions
1 Ci in ...... is equal to ...
    rutherfords    37000  Rd
    SI derived unit    37  GBq
    SI base unit    3.7×1010  s −1
Sample of cobalt-60 that emits 1 mCi (microcurie) of radioactivity; i.e. 37,000 decays per second. Cobalt-60.jpg
Sample of cobalt-60 that emits 1 μCi (microcurie) of radioactivity; i.e. 37,000 decays per second.

The curie (symbol Ci) is a non-SI unit of radioactivity originally defined in 1910. According to a notice in Nature at the time, it was to be named in honour of Pierre Curie, [1] but was considered at least by some to be in honour of Marie Curie as well, [2] and is in later literature considered to be named for both. [3]

Contents

It was originally defined as "the quantity or mass of radium emanation in equilibrium with one gram of radium (element)", [1] but is currently defined as 1 Ci = 3.7×1010 decays per second [4] after more accurate measurements of the activity of 226Ra (which has a specific activity of 3.66×1010 Bq/g [5] ).

In 1975 the General Conference on Weights and Measures gave the becquerel (Bq), defined as one nuclear decay per second, official status as the SI unit of activity. [6] Therefore:

1 Ci = 3.7×1010 Bq = 37 GBq

and

1 Bq ≅ 2.703×10−11 Ci ≅ 27 pCi

While its continued use is discouraged by the National Institute of Standards and Technology (NIST) [7] and other bodies, the curie is still widely used throughout government, industry and medicine in the United States and in other countries.

At the 1910 meeting, which originally defined the curie, it was proposed to make it equivalent to 10  nanograms of radium (a practical amount). But Marie Curie, after initially accepting this, changed her mind and insisted on one gram of radium. According to Bertram Boltwood, Marie Curie thought that "the use of the name 'curie' for so infinitesimally small [a] quantity of anything was altogether inappropriate". [2]

The power emitted in radioactive decay corresponding to one curie can be calculated by multiplying the decay energy by approximately 5.93  mW  /  MeV.

A radiotherapy machine may have roughly 1000 Ci of a radioisotope such as caesium-137 or cobalt-60. This quantity of radioactivity can produce serious health effects with only a few minutes of close-range, unshielded exposure.

Radioactive decay can lead to the emission of particulate radiation or electromagnetic radiation. Ingesting even small quantities of some particulate emitting radionuclides may be fatal. For example, the median lethal dose (LD-50) for ingested polonium-210 is 240 μCi; about 53.5 nanograms. However, millicurie quantities of electromagnetic emitting radionuclides are routinely used in nuclear medicine.

The typical human body contains roughly 0.1 μCi (14 mg) of naturally occurring potassium-40. A human body containing 16 kg (35 lb) of carbon (see Composition of the human body ) would also have about 24 nanograms or 0.1 μCi of carbon-14. Together, these would result in a total of approximately 0.2 μCi or 7400 decays per second inside the person's body (mostly from beta decay but some from gamma decay).

As a measure of quantity

Units of activity (the curie and the becquerel) also refer to a quantity of radioactive atoms. Because the probability of decay is a fixed physical quantity, for a known number of atoms of a particular radionuclide, a predictable number will decay in a given time. The number of decays that will occur in one second in one gram of atoms of a particular radionuclide is known as the specific activity of that radionuclide.

The activity of a sample decreases with time because of decay.

The rules of radioactive decay may be used to convert activity to an actual number of atoms. They state that 1 Ci of radioactive atoms would follow the expression

N (atoms) × λ (s−1) = 1 Ci = 3.7 × 1010 Bq,

and so

N = 3.7 × 1010 Bq / λ,

where λ is the decay constant in s−1.

Here are some examples, ordered by half-life:

IsotopeHalf-lifeMass of 1 curieSpecific activity (Ci/g)
209Bi 1.9×1019 years11.1 billion tonnes9.01×10−17
232Th 1.405×1010 years9.1 tonnes1.1×10−7 (110,000 pCi/g, 0.11 μCi/g)
238U 4.471×109 years2.977 tonnes3.4×10−7 (340,000 pCi/g, 0.34 μCi/g)
40K 1.25×109 years140 kg7.1×10−6 (7,100,000 pCi/g, 7.1 μCi/g)
235U 7.038×108 years463 kg2.2×10−6 (2,160,000 pCi/g, 2.2 μCi/g)
129I 15.7×106 years5.66 kg0.00018
99Tc 211×103 years58 g0.017
239Pu 24.11×103 years16 g0.063
240Pu 6563 years4.4 g0.23
14C 5730 years0.22 g4.5
226Ra 1601 years1.01 g0.99
241Am 432.6 years0.29 g3.43
238Pu 88 years59 mg17
137Cs 30.17 years12 mg83
90Sr 28.8 years7.2 mg139
241Pu 14 years9.4 mg106
3H 12.32 years104 μg9,621
228Ra 5.75 years3.67 mg273
60Co 1925 days883 μg1,132
210Po 138 days223 μg4,484
131I 8.02 days8 μg125,000
123I 13 hours518 ng1,930,000
212Pb 10.64 hours719 ng1,390,000
223Fr 22 minutes26 ng38,000,000
212Po 299 nanoseconds5.61 ag1.78×1017

The following table shows radiation quantities in SI and non-SI units:

Ionizing radiation related quantities
QuantityUnitSymbolDerivationYear SI equivalent
Activity (A) becquerel Bqs−11974SI unit
curie Ci3.7 × 1010 s−119533.7×1010 Bq
rutherford Rd106 s−119461,000,000 Bq
Exposure (X) coulomb per kilogram C/kgC⋅kg−1 of air1974SI unit
röntgen R esu / 0.001293 g of air19282.58 × 10−4 C/kg
Absorbed dose (D) gray Gy J⋅kg−11974SI unit
erg per gramerg/gerg⋅g−119501.0 × 10−4 Gy
rad rad100 erg⋅g−119530.010 Gy
Equivalent dose (H) sievert SvJ⋅kg−1 × WR 1977SI unit
röntgen equivalent man rem100 erg⋅g−1 × WR 19710.010 Sv
Effective dose (E) sievert SvJ⋅kg−1 × WR × WT 1977SI unit
röntgen equivalent man rem100 erg⋅g−1 × WR × WT 19710.010 Sv

See also

Related Research Articles

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Po
is 166 TBq/g, i.e., 1.66 × 1014 Bq/g. At the same time, 210Po is not readily detected by common radiation detectors, because its gamma rays have a very low energy. Therefore, 210
Po
can be considered as a quasi-pure alpha emitter.

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γ
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or 4
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2
He
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References

  1. 1 2 Rutherford, Ernest (6 October 1910). "Radium Standards and Nomenclature". Nature. 84 (2136): 430–431. Bibcode:1910Natur..84..430R. doi: 10.1038/084430a0 .
  2. 1 2 Frame, Paul (1996). "How the Curie Came to Be". Health Physics Society Newsletter. Archived from the original on 20 March 2012. Retrieved 3 July 2015.
  3. United States Atomic Energy Commission (1951). Semiannual Report of the Atomic Energy Commission, Volume 9. p. 93.
  4. "Resolution 7 of the 12th CGPM". International Bureau of Weights and Measures (BIPM). 1964. Archived from the original on 2021-02-19.
  5. Delacroix, D. (2002). "Radionuclide and Radiation Protection Data Handbook 2002". Radiation Protection Dosimetry. 98 (1). Nuclear Technology Publishing: 147. doi:10.1093/oxfordjournals.rpd.a006705. PMID   11916063. Archived from the original on 2016-03-05.
  6. "SI units for ionizing radiation: becquerel". Resolutions of the 15th CGPM (Resolution 8). 1975. Retrieved 3 July 2015.
  7. NIST Special Publication 811, paragraph 5.2 (Report). NIST. 28 January 2016. Retrieved 22 March 2016.