(a) Calculate the activity \({\rm{R}}\) in curies of \(1.00\,{\rm{g}}\) of \({}^{{\rm{226}}}{\rm{Ra}}\). (b) Discuss why your answer is not exactly \(1.00\,{\rm{Ci}}\), given that the curie was originally supposed to be exactly the activity of a gram of radium.

Short Answer

Expert verified

(a) The activity \({\rm{R}}\) is \(0.989\,{\rm{Ci}}\).

(b) We now know more about the half-life than we did when the unit was initially formed.

Step by step solution

01

Define radioactivity

Radioactivity is a phenomenon in which a few substances spontaneously release energy and subatomic particles. The nuclear instability of an atom causes radioactivity.

02

Evaluating the activity R

(a) The number of nuclei is computed using the formula \(N = \frac{m}{M}{N_A}\)

Where\({\rm{m}}\)is the mass of\({}^{{\rm{226}}}{\rm{Ra}}\),\({\rm{M}}\)is the molar mass of\({}^{{\rm{226}}}{\rm{Ra}}\), and\({{\rm{N}}_{\rm{A}}}\)is the Avogadro number, the number of atoms may be computed as follows,

\(\begin{array}{c}N = (1.00\,{\rm{g}})\left( {\frac{{{\rm{mol}}}}{{226\,{\rm{g}}}}} \right)\frac{{6.022 \times {{10}^{23}}\,{\rm{atoms}}}}{{{\rm{mol}}}}\\ = 2.6646 \times {10^{21}}\,{\rm{atoms}}\end{array}\)

By the equation\(R = \frac{{0.693}}{{{t_{1/2}}}}\), where we know that\({}^{{\rm{226}}}{\rm{Ra}}\)has a half-life of\(1.6 \times {10^3}\,{\rm{y}}\).

\(\begin{array}{c}R = \frac{{\left( {0.693} \right)\left( {2.6646 \times {{10}^{21}}} \right)}}{{1.6 \times {{10}^3}\,{\rm{y}}}} \times \frac{{1\,{\rm{y}}}}{{3.156 \times {{10}^7}\,{\rm{s}}}}\\ = 3.66 \times {10^{10}}\,{\rm{Bq}}\left( {\frac{{1\,{\rm{Ci}}}}{{3.70 \times {{10}^{10}}\,{\rm{Bq}}}}} \right)\\ = 0.989\,{\rm{Ci}}\end{array}\)

Therefore, the activity \({\rm{R}}\) is \(0.989\,{\rm{Ci}}\).

03

Explanation

(b) We now have a better understanding of the half-life of\({}^{{\rm{226}}}{\rm{Ra}}\) than we had when the\({\rm{Ci}}\) unit was first established.

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Most popular questions from this chapter

Large amounts of depleted uranium \({{\rm{(}}^{{\rm{238}}}}{\rm{U)}}\)are available as a by-product of uranium processing for reactor fuel and weapons. Uranium is very dense and makes good counter weights for aircraft. Suppose you have a \(4000\,{\rm{kg}}\)block of\(^{{\rm{238}}}{\rm{U}}\).

  1. Find its activity.
  2. How many calories per day are generated by thermalization of the decay energy?
  3. Do you think you could detect this as heat? Explain.

The detail observable using a probe is limited by its wavelength. Calculate the energy of a\({\rm{\gamma }}\)-ray photon that has a wavelength of\(1 \times {10^{ - 16}}\,{\rm{m}}\), small enough to detect details about one-tenth the size of a nucleon. Note that a photon having this energy is difficult to produce and interacts poorly with the nucleus, limiting the practicability of this probe.

Confirm that charge, electron family number, and the total number of nucleons are all conserved by the rule for α decay given in the equation\(_Z^A{X_N} \to _{Z - 2}^{A - 4}{Y_{N - 2}} + _2^4H{e_2}\). To do this, identify the values of each before and after the decay.

The relatively scarce naturally occurring calcium isotope \(^{48}{\rm{Ca}}\) has a half-life of about \(2 \times {10^{16}}{\rm{y}}\). (a) A small sample of this isotope is labeled as having an activity of \(1.0\)Ci. What is the mass of the \(^{48}{\rm{Ca}}\)in the sample?

(b) What is unreasonable about this result?

(c) What assumption is responsible?

Unreasonable Results

A frazzled theoretical physicist reckons that all conservation laws are obeyed in the decay of a proton into a neutron, positron, and neutrino (as in\({\beta ^ + }\)decay of a nucleus) and sends a paper to a journal to announce the reaction as a possible end of the universe due to the spontaneous decay of protons. (a) What energy is released in this decay?

(b) What is unreasonable about this result?

(c) What assumption is responsible?

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