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(a) Calculate the radius of\(^{{\rm{58}}}{\rm{Ni}}\), one of the most tightly bound stable nuclei. (b) What is the ratio of the radius of\(^{{\rm{58}}}{\rm{Ni}}\)to that of\(^{{\rm{258}}}{\rm{Ha}}\), one of the largest nuclei ever made? Note that the radius of the largest nucleus is still much smaller than the size of an atom.

Short Answer

Expert verified
  1. The radius of the \(^{{\rm{58}}}{\rm{Ni}}\) particle is obtained as: \(4.645 \times {10^{ - 15}}\,{\rm{m}}\).
  2. The ratio is obtained as: \(0.608\).

Step by step solution

01

Define Radioactivity

The spontaneous emission of radiation in the form of particles or high-energy photons as a result of a nuclear process is known as radioactivity.

02

Evaluating the radius

a)The atomic mass number of the \(^{{\rm{58}}}{\rm{Ni}}\) particle is:

\(A = 58\)

The radius of \(^{{\rm{58}}}{\rm{Ni}}\) particle is:

\({R_o} = 1.2 \times {10^{ - 15}}\,{\rm{m}}\)

Using the following relation to obtain the value of radius as:

\(\begin{align}R &= \;{R_o}{A^{\frac{1}{3}}}\\ &= 1.2 \times {10^{ - 15}}\,m \times {(58)^{\frac{1}{3}}}\\ &= {\rm{ }}4.645 \times {10^{ - 15}}\,m\end{align}\)

Therefore, the radius is: \(4.645 \times {10^{ - 15}}\,{\rm{m}}\).

03

Evaluating the ratio

b) The atomic mass number of the \(^{{\rm{258}}}{\rm{Ha}}\) particle is:

\(A = 258\)

The radius of \(^{{\rm{258}}}{\rm{Ha}}\) particle is:

\({R_o} = 1.2 \times {10^{ - 15}}\,{\rm{m}}\)

Using the following relation to obtain the value of radius as:

\(\begin{align}R &= \;{R_o}{A^{\frac{1}{3}}}\\ &= 1.2 \times {10^{ - 15}}\,m \times {(258)^{\frac{1}{3}}}\\ &= {\rm{ }}7.639 \times {10^{ - 15}}\,m\end{align}\)

Dividing both the radius to obtain the ratio as:

\(\begin{align}\frac{{{R_{Ni}}}}{{{R_{Ha}}}} &= \frac{{4.645 \times {{10}^{ - 15}}\,m}}{{7.639 \times {{10}^{ - 15}}\,m}}\\ &= 0.608\end{align}\)

Therefore, the ration is: \(0.608\).

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Most popular questions from this chapter

An old campfire is uncovered during an archaeological dig. Its charcoal is found to contain less than \(1/1000\) the normal amount of \({}^{{\rm{14}}}{\rm{C}}\). Estimate the minimum age of the charcoal, noting that \({2^{10}} = 1024\).

a) Calculate the energy released in the \({\rm{\alpha }}\) decay of \({}^{{\rm{238}}}{\rm{U}}\) . (b) What fraction of the mass of a single \({}^{{\rm{238}}}{\rm{U}}\) is destroyed in the decay? The mass of \({}^{{\rm{234}}}{\rm{Th}}\) is \(234.043593\,{\rm{u}}\). (c) Although the fractional mass loss is large for a single nucleus, it is difficult to observe for an entire macroscopic sample of uranium. Why is this?

To obtain the most precise value of\({\rm{BE}}\)from the equation\({\rm{BE = (ZM}}{{\rm{(}}^{\rm{1}}}{\rm{H) + N}}{{\rm{m}}_{\rm{n}}}{\rm{)}}{{\rm{c}}^{\rm{2}}}{\rm{ - m}}{{\rm{(}}^{\rm{A}}}{\rm{X)}}{{\rm{c}}^{\rm{2}}}\), we should take into account the binding energy of the electrons in the neutral atoms. Will doing this produce a larger or smaller value for\({\rm{BE}}\)? Why is this effect usually negligible?

What is the source of the energy emitted in radioactive decay? Identify an earlier conservation law, and describe how it was modified to take such processes into account.

The ceramic glaze on a red-orange Fiesta ware plate is \({{\rm{U}}_{\rm{2}}}{{\rm{O}}_{\rm{3}}}\)and contains \({\rm{50}}{\rm{.0}}\)grams of \(^{{\rm{238}}}{\rm{U}}\), but very little \(^{{\rm{235}}}{\rm{U}}\). (a)

  1. What is the activity of the plate?
  2. Calculate the total energy that will be released by the \(^{{\rm{238}}}{\rm{U}}\)decay.
  3. If energy is worth \({\rm{12}}{\rm{.0}}\)cents per\({\rm{kW \times h}}\), what is the monetary value of the energy emitted? (These plates went out of production some 30 years ago, but are still available as collectibles.)
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