Figure 42-16 gives the activities of three radioactive samples versus time. Rank the samples according to their (a) half-life and (b) disintegration constant, greatest first. (Hint:For (a), use a straightedge on the graph.)

Short Answer

Expert verified
  1. The rank of the samples according to their half-life is C > B > A.
  2. The rank of the samples according to their disintegration constant is A > B > C.

Step by step solution

01

Given data

Figure 42-16 gives the activities of three radioactive samples versus time is given.

02

Understanding the concept of decay  

Half-life is the time required for a quantity to reduce to half of its initial value during the radioactive decay process.

The disintegration constant of a radioactive substance is defined as the ratio of its instantaneous rate of disintegration to the number of nuclides present at that time.

The half-life and disintegration constant of a nuclide are inversely proportional to each other.

Formulae:

The disintegration constant,λ=ln2Tv2............(1)

Where,Tv2is the half-life of the substance,

The rate of decay, R=λN........(2)

03

a) Calculation for the rank of the samples according to their half-lives

From the graph, we can see that the rate of.decay of the samples at half of their time decay is in the order of: A > B > C

Thus, from equations (1) and (2), we can see that the rate of decay is inversely proportional to their half-lives,R=ln@Tv2N.

Hence, the rank of the samples according to their half-lives is given by C > B > A.

04

b) Calculation of the rank of the samples according to their disintegration constants

Now, from part (a) calculations, the rank according to half-lives is given as: C > B > A

Thus, from equation (1), we see that disintegration constant is inversely proportional to the half-life.

Hence, the ranking of the samples according to disintegration constant is A > B > C.

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Most popular questions from this chapter

A certain radionuclide is being manufactured in a cyclotron at a constant rate R. It is also decaying with disintegration constantλ. Assume that the production process has been going on for a time that is much longer than the half-life of the radionuclide. (a) Show that the numbers of radioactive nuclei present after such time remains constant and is given byN=Rλ. (b) Now show that this result holds no matter how many radioactive nuclei were present initially. The nuclide is said to be in secular equilibriumwith its source; in this state its decay rate is just equal to its production rate.

Two radioactive materials that alpha decay,U238and T232h, and one that beta decaysK40, are sufficiently abundant in granite to contribute significantly to the heating of Earth through the decay energy produced. The alpha-decay isotopes give rise to decay chains that stop when stable lead isotopes are formed. The isotopeK40has single beta decay. (Assume this is the only possible decay of that isotope.) Here is the information:

In the table Qis the totalenergy released in the decay of one parent nucleus to the finalstable endpoint and fis the abundance of the isotope in kilograms per kilogram of granite;means parts per million. (a) Show that these materials produce energy as heat at the rate of1.0×10-8Wfor each kilogram of granite. (b) Assuming that there is2.7×1022kgof granite in a 20-km-thick spherical shell at the surface of Earth, estimate the power of this decay process over all of Earth. Compare this power with the total solar power intercepted by Earth,1.7×1017W1.

Is the mass excess of an alpha particle (use a straightedge on Fig. 42-13) greater than or less than the particle’s total binding energy (use the binding energy per nucleon from Fig. 42-7)?

How much energy is released when a 238nucleus decays by emitting (a) an alpha particle and (b) a sequence of neutron, proton, neutron, and proton? (c) Convince yourself both by reasoned argument and by direct calculation that the difference between these two numbers is just the total binding energy of the alpha particle. (d) Find that binding energy. Some needed atomic and particle masses are

U238238.05079uT234h234.04363uU237237.04873uH4e4.00260uU236236.04891uH11.00783uU235235.04544un1.00866u

Figure 42-17 shows the curve for the binding energy per nucleonEbenversus mass number A. Three isotopes are indicated. Rank them according to the energy required to remove a nucleon from the isotope, greatest first.

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