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Radioactive decay

Radioactive decay (also known as nuclear decay, radioactivity, radioactive disintegration, or nuclear disintegration) is the process by which an unstable atomic nucleus loses energy by radiation. A material containing unstable nuclei is considered radioactive. Three of the most common types of decay are alpha, beta, and gamma decay. The weak force is the mechanism that is responsible for beta decay, while the other two are governed by the electromagnetism and nuclear force.[1]

"Radioactive" and "Radioactivity" redirect here. For other uses, see Radioactive (disambiguation) and Radioactivity (disambiguation).

Radioactive decay is a random process at the level of single atoms. According to quantum theory, it is impossible to predict when a particular atom will decay, regardless of how long the atom has existed.[2][3][4] However, for a significant number of identical atoms, the overall decay rate can be expressed as a decay constant or as half-life. The half-lives of radioactive atoms have a huge range; from nearly instantaneous to far longer than the age of the universe.


The decaying nucleus is called the parent radionuclide (or parent radioisotope[note 1]), and the process produces at least one daughter nuclide. Except for gamma decay or internal conversion from a nuclear excited state, the decay is a nuclear transmutation resulting in a daughter containing a different number of protons or neutrons (or both). When the number of protons changes, an atom of a different chemical element is created.


There are 28 naturally occurring chemical elements on Earth that are radioactive, consisting of 35 radionuclides (seven elements have two different radionuclides) that date before the time of formation of the Solar System. These 35 are known as primordial radionuclides. Well-known examples are uranium and thorium, but also included are naturally occurring long-lived radioisotopes, such as potassium-40.

The , t1/2, is the time taken for the activity of a given amount of a radioactive substance to decay to half of its initial value.

half-life

The , λ "lambda", the reciprocal of the mean lifetime (in s−1), sometimes referred to as simply decay rate.

decay constant

The , τ "tau", the average lifetime (1/e life) of a radioactive particle before decay.

mean lifetime

The decay rate, or activity, of a radioactive substance is characterized by the following time-independent parameters:


Although these are constants, they are associated with the statistical behavior of populations of atoms. In consequence, predictions using these constants are less accurate for minuscule samples of atoms.


In principle a half-life, a third-life, or even a (1/√2)-life, can be used in exactly the same way as half-life; but the mean life and half-life t1/2 have been adopted as standard times associated with exponential decay.


Those parameters can be related to the following time-dependent parameters:


These are related as follows:


where N0 is the initial amount of active substance — substance that has the same percentage of unstable particles as when the substance was formed.

The activity: A = λN.

The : n = N/NA.

amount of substance

The : m = Mn = MN/NA.

mass

Theoretical basis[edit]

The neutrons and protons that constitute nuclei, as well as other particles that approach close enough to them, are governed by several interactions. The nuclear force (also known as residual strong force), not observed at the familiar macroscopic scale, is the most powerful force over subatomic distances. The electrostatic force is almost always significant, and, in the case of beta decay, the weak nuclear force is also involved.


The combined effects of these forces produces a number of different phenomena in which energy may be released by rearrangement of particles in the nucleus, or else the change of one type of particle into others. These rearrangements and transformations may be hindered energetically so that they do not occur immediately. Radioactive decay half-life of nuclides has been measured over timescales of 54 orders of magnitude, from 8.6(6)×10−23 seconds (for hydrogen-5) to 7.10(28)×1031 seconds (for tellurium-128).[26] The limits of these timescales are set by the sensitivity of instrumentation only, and there are no known natural limits to how brief or long a decay half-life for radioactive decay of a radionuclide may be. A radioactive nucleus (or any excited system in quantum mechanics) is unstable, and can, thus, spontaneously stabilize to a less-excited system. The resulting transformation alters the structure of the nucleus and results in the emission of either a photon or a high-velocity particle that has mass (such as an electron, alpha particle, or other type).[55]

The trefoil symbol used to warn of presence of radioactive material or ionising radiation

The trefoil symbol used to warn of presence of radioactive material or ionising radiation

2007 ISO radioactivity hazard symbol intended for IAEA Category 1, 2 and 3 sources defined as dangerous sources capable of death or serious injury[56]

2007 ISO radioactivity hazard symbol intended for IAEA Category 1, 2 and 3 sources defined as dangerous sources capable of death or serious injury[56]

One of several dangerous goods transport classification signs for radioactive materials

One of several dangerous goods transport classification signs for radioactive materials

Encyclopædia Britannica. 2006. Encyclopædia Britannica Online. December 18, 2006

"Radioactivity"

Radio-activity by Ernest Rutherford Phd,

Encyclopædia Britannica Eleventh Edition

– Contains tabulated information on radioactive decay types and energies.

The Lund/LBNL Nuclear Data Search

Nomenclature of nuclear chemistry

.

Specific activity and related topics

The Live Chart of Nuclides – IAEA

Archived 10 October 2018 at the Wayback Machine

Interactive Chart of Nuclides

Health Physics Society Public Education Website

Beach, Chandler B., ed. (1914). . The New Student's Reference Work . Chicago: F. E. Compton and Co.

"Becquerel Rays" 

Archived 7 October 2010 at the Wayback Machine

Annotated bibliography for radioactivity from the Alsos Digital Library for Nuclear Issues

Archived 13 August 2011 at the Wayback Machine by Wolfgang Bauer

Stochastic Java applet on the decay of radioactive atoms

by David M. Harrison

Stochastic Flash simulation on the decay of radioactive atoms

"Henri Becquerel: The Discovery of Radioactivity", Becquerel's 1896 articles online and analyzed on [click 'à télécharger' for English version].

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"Radioactive change", Rutherford & Soddy article (1903), online and analyzed on [click 'à télécharger' for English version]

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