Radionuclide





A radionuclide (radioactive nuclide, radioisotope or radioactive isotope) is an atom that has excess nuclear energy, making it unstable. This excess energy can be used in one of three ways: emitted from the nucleus as gamma radiation; transferred to one of its electrons to release it as a conversion electron; or used to create and emit a new particle (alpha particle or beta particle) from the nucleus. During those processes, the radionuclide is said to undergo radioactive decay.[1] These emissions are considered ionizing radiation because they are powerful enough to liberate an electron from another atom. The radioactive decay can produce a stable nuclide or will sometimes produce a new unstable radionuclide which may undergo further decay. Radioactive decay is a random process at the level of single atoms: it is impossible to predict when one particular atom will decay.[2][3][4][5] However, for a collection of atoms of a single element the decay rate, and thus the half-life (t1/2) for that collection can be calculated from their measured decay constants. The range of the half-lives of radioactive atoms have no known limits and span a time range of over 55 orders of magnitude.


Radionuclides occur naturally or are artificially produced in nuclear reactors, cyclotrons, particle accelerators or radionuclide generators. There are about 730 radionuclides with half-lives longer than 60 minutes (see list of nuclides). Thirty-two of those are primordial radionuclides that were created before the earth was formed. At least another 60 radionuclides are detectable in nature, either as daughters of primordial radionuclides or as radionuclides produced through natural production on Earth by cosmic radiation. More than 2400 radionuclides have half-lives less than 60 minutes. Most of those are only produced artificially, and have very short half-lives. For comparison, there are about 253 stable nuclides. (In theory, only 146 of them are stable, and the other 107 are believed to decay (alpha decay or beta decay or double beta decay or electron capture or double electron capture))


All chemical elements can exist as radionuclides. Even the lightest element, hydrogen, has a well-known radionuclide, tritium. Elements heavier than lead, and the elements technetium and promethium, exist only as radionuclides. (In theory, elements heavier than dysprosium exist only as radionuclides, but the half-life for some such elements (e.g. gold and platinum) are too long to found)


Unplanned exposure to radionuclides generally has a harmful effect on living organisms including humans, although low levels of exposure occur naturally without harm. The degree of harm will depend on the nature and extent of the radiation produced, the amount and nature of exposure (close contact, inhalation or ingestion), and the biochemical properties of the element; with increased risk of cancer the most usual consequence. However, radionuclides with suitable properties are used in nuclear medicine for both diagnosis and treatment. An imaging tracer made with radionuclides is called a radioactive tracer. A pharmaceutical drug made with radionuclides is called a radiopharmaceutical.




Contents






  • 1 Origin


    • 1.1 Natural


    • 1.2 Nuclear fission


    • 1.3 Synthetic




  • 2 Uses


  • 3 Examples


    • 3.1 Household smoke detectors




  • 4 Impacts on organisms


  • 5 Summary table for classes of nuclides, "stable" and radioactive


  • 6 List of commercially available radionuclides


    • 6.1 Gamma emission only


    • 6.2 Beta emission only


    • 6.3 Alpha emission only


    • 6.4 Multiple radiation emitters




  • 7 See also


  • 8 Notes


  • 9 References


  • 10 Further reading


  • 11 External links





Origin



Natural


On Earth, naturally occurring radionuclides fall into three categories: primordial radionuclides, secondary radionuclides, and cosmogenic radionuclides.



  • Radionuclides are produced in stellar nucleosynthesis and supernova explosions along with stable nuclides. Most decay quickly but can still be observed astronomically and can play a part in understanding astronomic processes. Primordial radionuclides, such as uranium and thorium, exist in the present time because their half-lives are so long (>100 million years) that they have not yet completely decayed. Some radionuclides have half-lives so long (many times the age of the universe) that decay has only recently been detected, and for most practical purposes they can be considered stable, most notably bismuth-209: detection of this decay meant that bismuth was no longer considered stable. It is possible decay may be observed in other nuclides adding to this list of primordial radionuclides.

  • Secondary radionuclides are radiogenic isotopes derived from the decay of primordial radionuclides. They have shorter half-lives than primordial radionuclides. They arise in the decay chain of the primordial isotopes thorium-232, uranium-238 and uranium-235. Examples include the natural isotopes of polonium and radium.


  • Cosmogenic isotopes, such as carbon-14, are present because they are continually being formed in the atmosphere due to cosmic rays.[6]


Many of these radionuclides exist only in trace amounts in nature, including all cosmogenic nuclides. Secondary radionuclides will occur in proportion to their half-lives, so short-lived ones will be very rare. Thus polonium can be found in uranium ores at about 0.1 mg per metric ton (1 part in 1010).[7][8] Further radionunclides may occur in nature in virtually undetectable amounts as a result of rare events such as spontaneous fission or uncommon cosmic ray interactions.



Nuclear fission


Radionuclides are produced as an unavoidable result of nuclear fission and thermonuclear explosions. The process of nuclear fission creates a wide range of fission products, most of which are radionuclides. Further radionuclides can be created from irradiation of the nuclear fuel (creating a range of actinides) and of the surrounding structures, yielding activation products. This complex mixture of radionuclides with different chemistries and radioactivity makes handling nuclear waste and dealing with nuclear fallout particularly problematic.



Synthetic





Artificial nuclide americium-241 emitting alpha particles inserted into a cloud chamber for visualisation


Synthetic radionuclides are deliberately synthesised using nuclear reactors, particle accelerators or radionuclide generators:



  • As well as being extracted from nuclear waste, radioisotopes can be produced deliberately with nuclear reactors, exploiting the high flux of neutrons present. These neutrons activate elements placed within the reactor. A typical product from a nuclear reactor is iridium-192. The elements that have a large propensity to take up the neutrons in the reactor are said to have a high neutron cross-section.

  • Particle accelerators such as cyclotrons accelerate particles to bombard a target to produce radionuclides. Cyclotrons accelerate protons at a target to produce positron-emitting radionuclides, e.g. fluorine-18.

  • Radionuclide generators contain a parent radionuclide that decays to produce a radioactive daughter. The parent is usually produced in a nuclear reactor. A typical example is the technetium-99m generator used in nuclear medicine. The parent produced in the reactor is molybdenum-99.



Uses


Radionuclides are used in two major ways: either for their radiation alone (irradiation, nuclear batteries) or for the combination of chemical properties and their radiation (tracers, biopharmaceuticals).



  • In biology, radionuclides of carbon can serve as radioactive tracers because they are chemically very similar to the nonradioactive nuclides, so most chemical, biological, and ecological processes treat them in a nearly identical way. One can then examine the result with a radiation detector, such as a Geiger counter, to determine where the provided atoms were incorporated. For example, one might culture plants in an environment in which the carbon dioxide contained radioactive carbon; then the parts of the plant that incorporate atmospheric carbon would be radioactive. Radionuclides can be used to monitor processes such as DNA replication or amino acid transport.

  • In nuclear medicine, radioisotopes are used for diagnosis, treatment, and research. Radioactive chemical tracers emitting gamma rays or positrons can provide diagnostic information about internal anatomy and the functioning of specific organs, including the human brain.[9][10][11] This is used in some forms of tomography: single-photon emission computed tomography and positron emission tomography (PET) scanning and Cherenkov luminescence imaging. Radioisotopes are also a method of treatment in hemopoietic forms of tumors; the success for treatment of solid tumors has been limited. More powerful gamma sources sterilise syringes and other medical equipment.

  • In food preservation, radiation is used to stop the sprouting of root crops after harvesting, to kill parasites and pests, and to control the ripening of stored fruit and vegetables.

  • In industry, and in mining, radionuclides are used to examine welds, to detect leaks, to study the rate of wear, erosion and corrosion of metals, and for on-stream analysis of a wide range of minerals and fuels.

  • In spacecraft and elsewhere, radionuclides are used to provide power and heat, notably through radioisotope thermoelectric generators (RTGs).

  • In astronomy and cosmology radionuclides play a role in understanding stellar and planetary process.

  • In particle physics, radionuclides help discover new physics (physics beyond the Standard Model) by measuring the energy and momentum of their beta decay products.[12]

  • In ecology, radionuclides are used to trace and analyze pollutants, to study the movement of surface water, and to measure water runoffs from rain and snow, as well as the flow rates of streams and rivers.

  • In geology, archaeology, and paleontology, natural radionuclides are used to measure ages of rocks, minerals, and fossil materials.



Examples


The following table lists properties of selected radionuclides illustrating the range of properties and uses.



























































































































































































































































































Isotope Z N half life DM DE
keV
Mode of formation Comments

Tritium (3H)
1 2 12.3 y β
19 Cosmogenic lightest radionuclide, used in artificial nuclear fusion, also used for radioluminescence and as oceanic transient tracer. Synthesized from neutron bombardment of lithium-6 or deuterium

Beryllium-10
4 6 1,387,000 y β
556
Cosmogenic used to examine soil erosion, soil formation from regolith, and the age of ice cores

Carbon-14
6 8 5,700 y β
156
Cosmogenic used for radiocarbon dating

Fluorine-18
9 9 110 min β+, EC
633/1655
Cosmogenic positron source, synthesised for use as a medical radiotracer in PET scans.

Aluminium-26
13 13 717,000 y β+, EC
4004
Cosmogenic exposure dating of rocks, sediment

Chlorine-36
17 19 301,000 y β, EC
709
Cosmogenic exposure dating of rocks, groundwater tracer

Potassium-40
19 21 1.24×109 y β, EC
1330 /1505
Primordial used for potassium-argon dating, source of atmospheric argon, source of radiogenic heat, largest source of natural radioactivity

Calcium-41
20 21 102,000 y EC
Cosmogenic exposure dating of carbonate rocks

Cobalt-60
27 33 5.3 y β
2824
Synthetic produces high energy gamma rays, used for radiotherapy, equipment sterilisation, food irradiation

Strontium-90
38 52 28.8 y β
546
Fission product
medium-lived fission product; probably most dangerous component of nuclear fallout

Technetium-99
43 56 210,000 y β
294
Fission product commonest isotope of the lightest unstable element, most significant of long-lived fission products

Technetium-99m
43 56 6 hr γ,IC 141
Synthetic most commonly used medical radioisotope, used as a radioactive tracer

Iodine-129
53 76 15,700,000 y β
194
Cosmogenic longest lived fission product; groundwater tracer

Iodine-131
53 78 8 d β
971
Fission product most significant short term health hazard from nuclear fission, used in nuclear medicine, industrial tracer

Xenon-135
54 81 9.1 h β
1160
Fission Product strongest known "nuclear poison" (neutron-absorber), with a major effect on nuclear reactor operation.

Caesium-137
55 82 30.2 y β
1176
Fission Product other major medium-lived fission product of concern

Gadolinium-153
64 89 240 d EC
Synthetic Calibrating nuclear equipment, bone density screening

Bismuth-209
83 126 1.9×1019y α 3137
Primordial long considered stable, decay only detected in 2003

Polonium-210
84 126 138 d α 5307
Decay Product Highly toxic, used in poisoning of Alexander Litvinenko

Radon-222
86 136 3.8d α 5590
Decay Product gas, responsible for the majority of public exposure to ionizing radiation, second most frequent cause of lung cancer

Thorium-232
90 142 1.4×1010 y α 4083
Primordial basis of thorium fuel cycle

Uranium-235
92 143 7×108y α 4679
Primordial
fissile, main nuclear fuel

Uranium-238
92 146 4.5×109 y α 4267
Primordial Main Uranium isotope

Plutonium-238
94 144 87.7 y α 5593
Synthetic used in radioisotope thermoelectric generators (RTGs) and radioisotope heater units as an energy source for spacecraft

Plutonium-239
94 145 24110 y α 5245
Synthetic used for most modern nuclear weapons

Americium-241
95 146 432 y α 5486
Synthetic used in household smoke detectors as an ionising agent

Californium-252
98 154 2.64 y α/SF 6217
Synthetic undergoes spontaneous fission (3% of decays), making it a powerful neutron source, used as a reactor initiator and for detection devices

Key: Z = no of protons; N = no of Neutrons; DM = Decay Mode; DE = Decay Energy; EC = Electron Capture



Household smoke detectors




Americium-241 container in a smoke detector.




Americium-241 capsule as found in smoke detector. The circle of darker metal in the center is americium-241; the surrounding casing is aluminium.


Radionuclides are present in many homes as they are used inside the most common household smoke detectors. The radionuclide used is americium-241, which is created by bombarding plutonium with neutrons in a nuclear reactor. It decays by emitting alpha particles and gamma radiation to become neptunium-237. Smoke detectors use a very small quantity of 241Am (about 0.29 micrograms per smoke detector) in the form of americium dioxide. 241Am is used as it emits alpha particles which ionise the air in the detector's ionization chamber. A small electric voltage is applied to the ionised air which gives rise to a small electric current. In the presence of smoke some of the ions are neutralized, thereby decreasing the current, which activates the detector's alarm.[13][14]



Impacts on organisms


Radionuclides that find their way into the environment may cause harmful effects as radioactive contamination. They can also cause damage if they are excessively used during treatment or in other ways exposed to living beings, by radiation poisoning. Potential health damage from exposure to radionuclides depends on a number of factors, and "can damage the functions of healthy tissue/organs. Radiation exposure can produce effects ranging from skin redness and hair loss, to radiation burns and acute radiation syndrome. Prolonged exposure can lead to cells being damaged and in turn lead to cancer. Signs of cancerous cells might not show up until years, or even decades, after exposure."[15]



Summary table for classes of nuclides, "stable" and radioactive


Following is a summary table for the total list of nuclides with half-lives greater than one hour. Ninety of these 989 nuclides are theoretically stable, except to proton-decay (which has never been observed). About 253 nuclides have never been observed to decay, and are classically considered stable.


The remaining 662 radionuclides have half-lives longer than 1 hour, and are well-characterized (see list of nuclides for a complete tabulation). They include 28 nuclides with measured half-lives longer than the estimated age of the universe (13.8 billion years[16]), and another 4 nuclides with half-lives long enough (> 100 million years) that they are radioactive primordial nuclides, and may be detected on Earth, having survived from their presence in interstellar dust since before the formation of the solar system, about 4.6 billion years ago. Another 60+ short-lived nuclides can be detected naturally as daughters of longer-lived nuclides or cosmic-ray products. The remaining known nuclides are known solely from artificial nuclear transmutation.


Numbers are not exact, and may change slightly in the future, as "stable nuclides" are observed to be radioactive with very long half-lives.


This is a summary table[17] for the 988 nuclides with half-lives longer than one hour (including those that are stable), given in list of nuclides.



















































Stability class
Number of nuclides

Running total
Notes on running total
Theoretically stable to all but proton decay
90
90
Includes first 40 elements. Proton decay yet to be observed.
Theoretically stable to alpha decay, beta decay, isomeric transition, and double beta decay but not spontaneous fission, which is possible for "stable" nuclides ≥ niobium-93
56
146
All nuclides that are possible completely stable (spontaneous fission has never been observed for nuclides with mass number < 232).
Energetically unstable to one or more known decay modes, but no decay yet seen. All considered "stable" until decay detected.
107
253
Total of classically stable nuclides.
Radioactive primordial nuclides.
33
286
Total primordial elements include uranium, thorium, bismuth, rubidium-87, potassium-40, tellurium-128 plus all stable nuclides.
Radioactive nonprimordial, but naturally occurring on Earth.
61
347

Carbon-14 (and other isotopes generated by cosmic rays) and daughters of radioactive primordial elements, such as radium, polonium, etc. 41 of these have a half life of greater than one hour.
Radioactive synthetic half-life ≥ 1.0 hour). Includes most useful radiotracers.
662
989
These 989 nuclides are listed in the article List of nuclides.
Radioactive synthetic (half-life < 1.0 hour).
>2400
>3300
Includes all well-characterized synthetic nuclides.


List of commercially available radionuclides



This list covers common isotopes, most of which are available in very small quantities to the general public in most countries. Others that are not publicly accessible are traded commercially in industrial, medical, and scientific fields and are subject to government regulation.



Gamma emission only































































Isotope

Activity
Half-life
Energies (keV)

Barium-133
9694 TBq/kg (262 Ci/g)
10.7 years
81.0, 356.0

Cadmium-109
96200 TBq/kg (2600 Ci/g)
453 days
88.0

Cobalt-57
312280 TBq/kg (8440 Ci/g)
270 days
122.1

Cobalt-60
40700 TBq/kg (1100 Ci/g)
5.27 years
1173.2, 1332.5

Europium-152
6660 TBq/kg (180 Ci/g)
13.5 years
121.8, 344.3, 1408.0

Manganese-54
287120 TBq/kg (7760 Ci/g)
312 days
834.8

Sodium-22
237540 Tbq/kg (6240 Ci/g)
2.6 years
511.0, 1274.5

Zinc-65
304510 TBq/kg (8230 Ci/g)
244 days
511.0, 1115.5

Technetium-99m

7007195000000000000♠1.95×107 TBq/kg (5.27 × 105 Ci/g)
6 hours
140


Beta emission only

































Isotope
Activity
Half-life
Energies (keV)

Strontium-90
5180 TBq/kg (140 Ci/g)
28.5 years
546.0

Thallium-204
17057 TBq/kg (461 Ci/g)
3.78 years
763.4

Carbon-14
166.5 TBq/kg (4.5 Ci/g)
5730 years
49.5 (average)

Tritium (Hydrogen-3)
357050 TBq/kg (9650 Ci/g)
12.32 years
5.7 (average)


Alpha emission only





















Isotope
Activity
Half-life
Energies (keV)

Polonium-210
166500 TBq/kg (4500 Ci/g)
138.376 days
5304.5

Uranium-238
12580 KBq/kg (0.00000034 Ci/g)
4.468 billion years
4267


Multiple radiation emitters
























Isotope
Activity
Half-life
Radiation types
Energies (keV)

Caesium-137
3256 TBq/kg (88 Ci/g)
30.1 years
Gamma & beta
G: 32, 661.6 B: 511.6, 1173.2

Americium-241
129.5 TBq/kg (3.5 Ci/g)
432.2 years
Gamma & alpha
G: 59.5, 26.3, 13.9 A: 5485, 5443


See also




  • List of nuclides shows all radionuclides with half-life > 1 hour

  • Hyperaccumulators table – 3

  • Radioactivity in biology

  • Radiometric dating

  • Radionuclide cisternogram

  • Uses of radioactivity in oil and gas wells



Notes





  1. ^ R.H. Petrucci, W.S. Harwood and F.G. Herring, General Chemistry (8th ed., Prentice-Hall 2002), p.1025–26


  2. ^ "Decay and Half Life". Retrieved 2009-12-14..mw-parser-output cite.citation{font-style:inherit}.mw-parser-output q{quotes:"""""""'""'"}.mw-parser-output code.cs1-code{color:inherit;background:inherit;border:inherit;padding:inherit}.mw-parser-output .cs1-lock-free a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/6/65/Lock-green.svg/9px-Lock-green.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output .cs1-lock-limited a,.mw-parser-output .cs1-lock-registration a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/d/d6/Lock-gray-alt-2.svg/9px-Lock-gray-alt-2.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output .cs1-lock-subscription a{background:url("//upload.wikimedia.org/wikipedia/commons/thumb/a/aa/Lock-red-alt-2.svg/9px-Lock-red-alt-2.svg.png")no-repeat;background-position:right .1em center}.mw-parser-output .cs1-subscription,.mw-parser-output .cs1-registration{color:#555}.mw-parser-output .cs1-subscription span,.mw-parser-output .cs1-registration span{border-bottom:1px dotted;cursor:help}.mw-parser-output .cs1-hidden-error{display:none;font-size:100%}.mw-parser-output .cs1-visible-error{font-size:100%}.mw-parser-output .cs1-subscription,.mw-parser-output .cs1-registration,.mw-parser-output .cs1-format{font-size:95%}.mw-parser-output .cs1-kern-left,.mw-parser-output .cs1-kern-wl-left{padding-left:0.2em}.mw-parser-output .cs1-kern-right,.mw-parser-output .cs1-kern-wl-right{padding-right:0.2em}


  3. ^ Stabin, Michael G. (2007). "3". Radiation Protection and Dosimetry: An Introduction to Health Physics (Submitted manuscript). Springer. doi:10.1007/978-0-387-49983-3. ISBN 978-0387499826.


  4. ^ Best, Lara; Rodrigues, George; Velker, Vikram (2013). "1.3". Radiation Oncology Primer and Review. Demos Medical Publishing. ISBN 978-1620700044.


  5. ^ Loveland, W.; Morrissey, D.; Seaborg, G.T. (2006). Modern Nuclear Chemistry. Modern Nuclear Chemistry. Wiley-Interscience. p. 57. Bibcode:2005mnc..book.....L. ISBN 978-0-471-11532-8.


  6. ^ Eisenbud, Merril; Gesell, Thomas F (1997-02-25). Environmental Radioactivity: From Natural, Industrial, and Military Sources. p. 134. ISBN 9780122351549.


  7. ^ Bagnall, K. W. (1962). "The Chemistry of Polonium". Advances in Inorganic Chemistry and Radiochemistry 4. New York: Academic Press. pp. 197–226. doi:10.1016/S0065-2792(08)60268-X.
    ISBN 0-12-023604-4. Retrieved June 14, 2012., p. 746



  8. ^ Bagnall, K. W. (1962). "The Chemistry of Polonium". Advances in Inorganic Chemistry and Radiochemistry 4. New York: Academic Press., p. 198


  9. ^ Ingvar, David H.; Lassen, Niels A. (1961). "Quantitative determination of regional cerebral blood-flow in man". The Lancet. 278 (7206): 806–807. doi:10.1016/s0140-6736(61)91092-3.


  10. ^ Ingvar, David H.; Franzén, Göran (1974). "Distribution of cerebral activity in chronic schizophrenia". The Lancet. 304 (7895): 1484–1486. doi:10.1016/s0140-6736(74)90221-9.


  11. ^ Lassen, Niels A.; Ingvar, David H.; Skinhøj, Erik (October 1978). "Brain Function and Blood Flow" (PDF). Scientific American. 239 (4): 62–71. Bibcode:1978SciAm.239d..62L. doi:10.1038/scientificamerican1078-62.


  12. ^ Severijns, Nathal; Beck, Marcus; Naviliat-Cuncic, Oscar (2006). "Tests of the standard electroweak model in nuclear beta decay". Reviews of Modern Physics. 78 (3): 991–1040. arXiv:nucl-ex/0605029. Bibcode:2006RvMP...78..991S. doi:10.1103/RevModPhys.78.991.


  13. ^ "Smoke Detectors and Americium". world-nuclear.org. Archived from the original on 2010-11-12.


  14. ^ Office of Radiation Protection – Am 241 Fact Sheet – Washington State Department of Health Archived 2011-03-18 at the Wayback Machine.


  15. ^ "Ionizing radiation, health effects and protective measures". World Health Organization. November 2012. Retrieved January 27, 2014.


  16. ^ "Cosmic Detectives". The European Space Agency (ESA). 2013-04-02. Retrieved 2013-04-15.


  17. ^ Table data is derived by counting members of the list; see WP:CALC. References for the list data itself are given below in the reference section in list of nuclides




References




  • Carlsson, J.; Forssell Aronsson, E; Hietala, SO; Stigbrand, T; Tennvall, J; et al. (2003). "Tumour therapy with radionuclides: assessment of progress and problems". Radiotherapy and Oncology. 66 (2): 107–117. doi:10.1016/S0167-8140(02)00374-2. PMID 12648782.


  • "Radioisotopes in Industry". World Nuclear Association.


  • Martin, James (2006). Physics for Radiation Protection: A Handbook. p. 130. ISBN 978-3527406111.



Further reading



  • Luig, H.; Kellerer, A. M.; Griebel, J. R. (2011). "Radionuclides, 1. Introduction". Ullmann's Encyclopedia of Industrial Chemistry. doi:10.1002/14356007.a22_499.pub2. ISBN 978-3527306732.


External links








  • EPA – Radionuclides – EPA's Radiation Protection Program: Information.


  • FDA – Radionuclides – FDA's Radiation Protection Program: Information.


  • Interactive Chart of Nuclides – A chart of all nuclides


  • National Isotope Development Center – U.S. Government source of radionuclides – production, research, development, distribution, and information

  • The Live Chart of Nuclides – IAEA











這個網誌中的熱門文章

Tangent Lines Diagram Along Smooth Curve

Yusuf al-Mu'taman ibn Hud

Zucchini