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Encyclopedia > Elimination half life

The half-life of a radioactive substance is the time required for half of a sample to undergo radioactive decay. Radioactive decay is the set of various processes by which unstable atomic nuclei (nuclides) emit subatomic particles. ...


More generally, for a quantity subject to exponential decay, the half-life is the time required for the quantity to fall to half of its initial value. (This article is a narrow discussion of half-life. For phenomena where half-life is applied, see "Related topics" below.) A quantity is said to be subject to exponential decay if it decreases at a rate proportional to its value. ...

After # of
Half-lives
Percent of quantity
remaining
0 100%
1 50
2 25
3 12.5
4 6.25
5 3.125
6 1.5625
7 0.78125%

The table at right shows the reduction of the quantity in terms of the number of half-lives elapsed.


Quantities subject to exponential decay are commonly denoted by the symbol N. (This convention suggests a decaying number of discrete items. This interpretation is valid in many, but not all, cases of exponential decay.) If the quantity is denoted by the symbol N, the value of N at a time t is given by the formula:

N(t) = N_0 e^{-lambda t} ,

where

  • N0 is the initial value of N (at t=0)
  • λ is a positive constant (the decay constant).

When t=0, the exponential is equal to 1, and N(t) is equal to N0. As t approaches infinity, the exponential approaches zero.


In particular, there is a time t_{1/2} , such that:

N(t_{1/2}) = N_0cdotfrac{1}{2}

Substituting into the formula above, we have:

N_0cdotfrac{1}{2} = N_0 e^{-lambda t_{1/2}} ,
e^{-lambda t_{1/2}} = frac{1}{2} ,
- lambda t_{1/2} = ln frac{1}{2} = - ln{2} ,
t_{1/2} = frac{ln 2}{lambda} ,

Thus the half-life is 69.3% of the mean lifetime. Given an assembly of elements, the number of which decreases ultimately to zero, the lifetime (also called the mean lifetime) is a certain number that characterizes the rate of reduction (decay) of the assembly. ...


Decay by two or more processes

A radioactive element may decay via two or more different processes. These processes may have different probabilities of occuring, and thus there is also a different half-life associated with each process.


As an example, for two decay modes, the ammount of substance left after time t is given by

N(t) = N_0 e^{-lambda _1 t} e^{-lambda _2 t} = N_0 e^{-(lambda _1 + lambda _2) t}

In a fashion similar to the previous section, we can calculate the new total half-life T _{1/2} , and we'll find it to be

T_{1/2} = frac{ln 2}{lambda _1 + lambda _2} ,

or, in terms of the two half-lives

T_{1/2} = frac{t _1 t _2}{t _1 + t_2} ,

Where t _1 , is the half-life of the first process, and t _2 , is the half life of the second process.


Related topics


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