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To illustrate the concept of a decay series, consider the decay of Th-232 series ( [link] ). The neutron number, N , is plotted on the vertical y -axis, and the atomic number, Z , is plotted on the horizontal x -axis, so Th-232 is found at the coordinates ( N , Z ) = ( 142 , 90 ) . Th-232 decays by α emission with a half-life of 1.39 × 10 10 years. Alpha decay decreases the atomic number by 2 and the mass number by 4, so we have

90 232 T h 88 228 R a + 2 4 H e .

The neutron number for Radium-228 is 140, so it is found in the diagram at the coordinates ( N , Z ) = ( 140 , 88 ) . Radium-228 is also unstable and decays by β emission with a half-life of 5.76 years to Actinum-228. The atomic number increases by 1, the mass number remains the same, and the neutron number decreases by 1. Notice that in the graph, α emission appears as a line sloping downward to the left, with both N and Z decreasing by 2. Beta emission, on the other hand, appears as a line sloping downward to the right with N decreasing by 1, and Z increasing by 1. After several additional alpha and beta decays, the series ends with the stable nucleus Pb-208.

The relative frequency of different types of radioactive decays (alpha, beta, and gamma) depends on many factors, including the strength of the forces involved and the number of ways a given reaction can occur without violating the conservation of energy and momentum. How often a radioactive decay occurs often depends on a sensitive balance of the strong and electromagnetic forces. These forces are discussed in Particle Physics and Cosmology .

A graph of neutron number N = A – Z versus atomic number Z is shown. Alpha decay is shown by red arrows pointing downward left, thus showing decrease in both N and Z. Beta decay is shown by blue arrows pointing downward right, indicating a decrease in N and increase in Z. The decay is shown as follows: Alpha decay from 232 Th to 228 Ra in 1.39 into 10 to the power 10 years. Beta decay from 228 Ra to 228 Ac in 5.76 years and from 228 Ac to 228 Th in 6.15 hours. Alpha decay from 228 Th to 224 Ra in 1.91 years, from 224 Ra to 220 Rn in 3.66 days, from 220 Rn to 216 Po in 55.6 seconds and from 216 Po to 212 Pb in 0.15 seconds. Beta decay from 212 Pb to 212 Bi in 10.6 hours and from 212 Bi to 212 Po in 60.6 minutes. Alpha decay from 212 Po to 208 Pb in 0.3 into 10 to the power minus 6 seconds.
In the thorium 90 232 T h decay series, alpha ( α ) decays reduce the atomic number, as indicated by the red arrows. Beta ( β ) decays increase the atomic number, as indicated by the blue arrows. The series ends at the stable nucleus Pb-208.

As another example, consider the U-238 decay series shown in [link] . After numerous alpha and beta decays, the series ends with the stable nucleus Pb-206. An example of a decay whose parent nucleus no longer exists naturally is shown in [link] . It starts with Neptunium-237 and ends in the stable nucleus Bismuth-209. Neptunium is called a transuranic element    because it lies beyond uranium in the periodic table. Uranium has the highest atomic number ( Z = 92 ) of any element found in nature. Elements with Z > 92 can be produced only in the laboratory. They most probably also existed in nature at the time of the formation of Earth, but because of their relatively short lifetimes, they have completely decayed. There is nothing fundamentally different between naturally occurring and artificial elements.

A graph of neutron number N = A – Z versus atomic number Z is shown. Alpha decay is shown by red arrows pointing downward left, thus showing decrease in both N and Z. Beta decay is shown by blue arrows pointing downward right, indicating a decrease in N and increase in Z. The decay is shown as follows: Alpha decay from 238 U to 234 Th in 4.46 into 10 to the power 9 years. Beta decay from 234 Th to 234 Pa in 24.1 days and from 234 Pa to 234 U in 6.66 hours. Alpha decay from 234 U to 230 Th in 2.48 into 10 to the power 5 years, from 230 Th to 226 Ra in 7.54 into 10 to the power 4 years, from 226 Ra to 222 Rn in 1600 years, from 222 Rn to 218 Po in 3.82 days, and from 218 Po to 214 Pb in 3.05 minutes. Beta decay from 214 Pb to 214 Bi in 26 minutes and from 214 Bi to 214 Po in 19.9 minutes. Alpha decay from 214 Bi to 210 Tl in 26 minutes and from 214 Po to 210 Pb in 1.64 into 10 to the power minus 4 seconds. Beta decay from 210 Tl to 210 Pb in 1.3 minutes, from 210 Pb to 210 Bi in 22.6 years and from 210 Bi to 210 Po in 5.01 days. Alpha decay from 210 Po to 206 Pb in 138 days.
In the Uranium-238 decay series, alpha ( α ) decays reduce the atomic number, as indicated by the red arrows. Beta ( β ) decays increase the atomic number, as indicated by the blue arrows. The series ends at the stable nucleus Pb-206.

Notice that for Bi (21), the decay may proceed through either alpha or beta decay.

A graph of neutron number N = A – Z versus atomic number Z is shown. Alpha decay is shown by red arrows pointing downward left, thus showing decrease in both N and Z. Beta decay is shown by blue arrows pointing downward right, indicating a decrease in N and increase in Z. The decay is shown as follows: Alpha decay from 237 Np to 233 Pa in 2.14 into 10 to the power 6 years. Beta decay from 233 Pa to 233 U in 27 days. Alpha decay from 233 U to 229 Th in 1.59 into 10 to the power 5 years and from 229 Th to 225 Ra in 7900 years. Beta decay from 225 Ra to 225 Ac in 14.8 days. Alpha decay from 225 Ac to 221 Fr in 10 days, from 221 Fr to 217 At in 4.8 minutes and from 217 At to 213 Bi in 0.032 seconds. Beta decay from 213 Bi to 213 Po in 45.6 minutes. Alpha decay from 213 Po to 209 Pb in 4 into 10 to the power minus 6 seconds. Beta decay from 209 Pb to 209 Bi in 3.25 hours.
In the Neptunium-237 decay series, alpha ( α ) decays reduce the atomic number, as indicated by the red arrows. Beta ( β ) decays increase the atomic number, as indicated by the blue arrows. The series ends at the stable nucleus Bi-209.

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Source:  OpenStax, University physics volume 3. OpenStax CNX. Nov 04, 2016 Download for free at http://cnx.org/content/col12067/1.4
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