In a \({\rm{3 \times 1}}{{\rm{0}}^{\rm{9}}}\)-year-old rock that originally contained some\(^{{\rm{238}}}{\rm{U}}\)which has a half-life of \({\rm{4}}{\rm{.5 \times 1}}{{\rm{0}}^{\rm{9}}}\) years, we expect to find some \(^{{\rm{238}}}{\rm{U}}\)remaining in it. Why are \(^{{\rm{226}}}{\rm{Ra}}{{\rm{,}}^{{\rm{222}}}}{\rm{Rn, and}}{{\rm{ }}^{{\rm{210}}}}{\rm{Po}}\) also found in such a rock, even though they have much shorter half-lives (1600 years, 3.8 days, and 138 days, respectively)?

Short Answer

Expert verified

The decay series starting from \(^{238}U\)produces \(^{226}Ra\)and \(^{210}{\rm{Po}}\)that are radioactive isotopes.

Step by step solution

01

Definition of Alpha and Beta decay

The process of radioactive decay known as "alpha decay," in which an atomic nucleus produces an alpha particle and changes into a separate atomic nucleus with a mass number that is reduced by four and an atomic number that is reduced by two, is known as radioactive decay.

Beta decay is a type of radioactive decay in nuclear physics in which a beta particle is emitted from an atomic nucleus, converting the original nuclide to an isobar of that nuclide.

02

Explanation

The time required for the original number of nuclei to decay to half is defined as the half-life. Some nuclides are stable and live indefinitely. Unstable nuclides decay and produce stable nuclides after various decays. The products of decay are referred to as daughters, while the original nuclide is referred to as the parent nuclide. \(^{238}U\) Decay into another unstable nuclide, resulting in decay where each nuclide decays to form a stable nuclide.

The decay series begins with\(^{238}U\)and ends with\(^{226}Ra\)and\(^{210}{\rm{Po}}\)both of which are radioactive isotopes.\(^{222}Rn\)is also generated. As a result, radioactive isotopes with shorter half-lives are found in such rock.

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Most popular questions from this chapter

Arrange the following according to their ability to act as radiation shields, with the best first and worst last. Explain your ordering in terms of how radiation loses its energy in matter.

(a) A solid material with low density composed of low-mass atoms.

(b) A gas composed of high-mass atoms.

(c) A gas composed of low-mass atoms.

(d) A solid with high density composed of high-mass atoms.

If a \(1.50\,{\rm{cm}}\)-thick piece of lead can absorb \({\rm{90}}{\rm{.0 \% }}\) of the \({\rm{\gamma }}\) rays from a radioactive source, how many centimeters of lead are needed to absorb all but \({\rm{0}}{\rm{.100 \% }}\) of the \({\rm{\gamma }}\) rays?

(a) Write the complete \({\rm{\alpha }}\) decay equation for \(^{249}Cf\).

(b) Find the energy released in the decay.

Calculate the energy released in the\({{\rm{\beta }}^{\rm{ + }}}\)decay of\({}^{{\rm{22}}}{\rm{Na}}\), the equation for which is given in the text. The masses of\({}^{{\rm{22}}}{\rm{Na}}\)and\({}^{{\rm{22}}}{\rm{Ne}}\)are\({\rm{21}}{\rm{.994434}}\)and\({\rm{21}}{\rm{.991383u}}\), respectively.

Suppose a particle of ionizing radiation deposits\(1.0\,{\rm{MeV}}\)in the gas of a Geiger tube, all of which goes to creating ion pairs. Each ion pair requires\(30.0\,{\rm{eV}}\)of energy. (a) The applied voltage sweeps the ions out of the gas in\(1.00\,{\rm{\mu s}}\). What is the current? (b) This current is smaller than the actual current since the applied voltage in the Geiger tube accelerates the separated ions, which then create other ion pairs in subsequent collisions. What is the current if this last effect multiplies the number of ion pairs by\({\rm{900}}\)?

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