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College Physics for APĀ® Courses

Irina Lyublinskaya, Gregg Wolfe, Douglas Ingram , Liza Pujji

Chapter 32

Medical Applications of Nuclear Physics - all with Video Answers

Educators

SL

Chapter Questions

02:01

Problem 1

A neutron generator uses an $\alpha$ source, such as radium, to bombard beryllium, inducing the reaction
$^{4} \mathrm{He}+^{9} \mathrm{Be} \rightarrow^{12} \mathrm{C}+n .$ Such neutron sources are called
RaBe sources, or PuBe sources if they use plutonium to get the $\alpha$ s. Calculate the energy output of the reaction in MeV.

Hebe Lee
Hebe Lee
Numerade Educator
03:21

Problem 2

Neutrons from a source (perhaps the one discussed in the preceding problem) bombard natural molybdenum, which is 24 percent $^{98}$ Mo. What is the energy output of the reaction
$98 \mathrm{Mo}+n \rightarrow^{99} \mathrm{Mo}+\gamma ?$ The mass of 98 $\mathrm{Mo}$ is given in

SL
Sin Lin
Numerade Educator
01:41

Problem 3

The purpose of producing 99 Mo (usually by neutron activation of natural molybdenum, as in the preceding problem) is to produce $99 \mathrm{~m} \mathrm{Tc}$. Using the rules, verify that the $\beta^{-}$ decay of $99 \mathrm{Mo}$ produces $99 \mathrm{~m} \mathrm{Tc} .$ (Most $99 \mathrm{~m} \mathrm{Tc}$
nuclei produced in this decay are left in a metastable excited state denoted ${ }^{99 \mathrm{~m}} \mathrm{Tc} .$.)

Hebe Lee
Hebe Lee
Numerade Educator
04:22

Problem 4

(a) Two annihilation $\gamma$ rays in a PET scan originate at the same point and travel to detectors on either side of the patient. If the point of origin is 9.00 $\mathrm{cm}$ closer to one of the detectors, what is the difference in arrival times of the photons? (This could be used to give position information, but
the time difference is small enough to make it difficult.)
(b) How accurately would you need to be able to measure arrival time differences to get a position resolution of 1.00 $\mathrm{mm} ?$

SL
Sin Lin
Numerade Educator
01:50

Problem 5

Table 32.1 indicates that 7.50 $\mathrm{mCi}$ of 99 $\mathrm{m}$ Tc is used in a
brain scan. What is the mass of technetium?

Hebe Lee
Hebe Lee
Numerade Educator
02:41

Problem 6

The activities of ${ }^{131} \mathrm{I}$ and $123 \mathrm{I}$ used in thyroid scans are given in Table 32.1 to be 50 and $70 \mu \mathrm{Ci}$, respectively. Find
and compare the masses of ${ }^{131} \mathrm{I}$ and ${ }^{123} \mathrm{I}$ in such scans, given their respective half-lives are $8.04 \mathrm{~d}$ and $13.2 \mathrm{~h}$. The masses are so small that the radioiodine is usually mixed with stable iodine as a carrier to ensure normal chemistry and distribution in the body.

Hebe Lee
Hebe Lee
Numerade Educator
02:28

Problem 7

(a) Neutron activation of sodium, which is 100$\%$ 23 $\mathrm{Na}$ produces $^{24} \mathrm{Na},$ which is used in some heart scans, as seen in Table 32.1 . The equation for the reaction is $^{23} \mathrm{Na}+n \rightarrow^{24} \mathrm{Na}+\gamma .$ Find its energy output, given the
mass of 24 $\mathrm{Na}$ is 23.990962 $\mathrm{u}$ . (b) What mass of $^{24} \mathrm{Na}$ produces the needed 5.0 -mci activity, given its half-life is 15.0 $\mathrm{h}$ ?

Hebe Lee
Hebe Lee
Numerade Educator
01:35

Problem 8

What is the dose in mSv for: (a) a 0.1 Gy x-ray? (b) 2.5 mGy of neutron exposure to the eye? (c) 1.5 mGy of $\alpha$ exposure?

Hebe Lee
Hebe Lee
Numerade Educator
01:01

Problem 9

Find the radiation dose in Gy for: (a) A 10 -mSv fluoroscopic. X-ray series. (b) 50 $\mathrm{mSv}$ of skin exposure by an $\alpha$ emitter. (c) 160 $\mathrm{mSv}$ of $\beta^{-}$ and $\gamma$ rays from the $^{40} \mathrm{K}$ in your body.

Hebe Lee
Hebe Lee
Numerade Educator
00:30

Problem 10

How many Gy of exposure is needed to give a cancerous tumor a dose of 40 Sv if it is exposed to $\alpha$ activity?

Hebe Lee
Hebe Lee
Numerade Educator
00:28

Problem 11

What is the dose in Sv in a cancer treatment that exposes the patient to 200 Gy of $\gamma$ rays?

Hebe Lee
Hebe Lee
Numerade Educator
02:13

Problem 12

One half the $\gamma$ rays from 99 $\mathrm{m}$ Tc are absorbed by a 0.170 -mm-thick lead shielding. Half of the $\gamma$ rays that pass through the first layer of lead are absorbed in a second layer of equal thickness. What thickness of lead will absorb all but one in 1000 of these $\gamma$ rays?

SL
Sin Lin
Numerade Educator
01:39

Problem 13

A plumber at a nuclear power plant receives a whole-body dose of 30 msv in 15 minutes while repairing a crucial valve. Find the radiation-induced yearly risk of death from cancer and the chance of genetic defect from this maximum allowable exposure.

Hebe Lee
Hebe Lee
Numerade Educator
03:08

Problem 14

In the 1980 s, the term picowave was used to describe food irradiation in order to overcome public resistance by playing on the well-known safety of microwave radiation. Find the energy in MeV of a photon having a wavelength of a picometer.

Hebe Lee
Hebe Lee
Numerade Educator
02:01

Problem 15

Find the mass of 239 $\mathrm{Pu}$ that has an activity of 1.00$\mu \mathrm{Ci}$

Hebe Lee
Hebe Lee
Numerade Educator
02:11

Problem 16

A beam of 168 -MeV nitrogen nuclei is used for cancer therapy. If this beam is directed onto a $0.200-\mathrm{kg}$ tumor and gives it a 2.00 -Sv dose, how many nitrogen nuclei were stopped? (Use an RBE of 20 for heavy ions.)

Hebe Lee
Hebe Lee
Numerade Educator
03:35

Problem 17

(a) If the average molecular mass of compounds in food is 50.0 g, how many molecules are there in 1.00 $\mathrm{kg}$ of food? (b) How many ion pairs are created in 1.00 $\mathrm{kg}$ of food, if it is
exposed to 1000 $\mathrm{Sv}$ and it takes 32.0 $\mathrm{eV}$ to create an ion pair? (c) Find the ratio of ion pairs to molecules. (d) If these ion pairs recombine into a distribution of 2000 new
compounds, how many parts per billion is each?

Hebe Lee
Hebe Lee
Numerade Educator
01:42

Problem 18

Calculate the dose in Sv to the chest of a patient given an x-ray under the following conditions. The x-ray beam intensity is $1.50 \mathrm{W} / \mathrm{m}^{2},$ the area of the chest exposed is $0.0750 \mathrm{m}^{2}, 35.0 \%$ of the $x$ -rays are absorbed in 20.0 $\mathrm{kg}$ of tissue, and the exposure time is 0.250 $\mathrm{s}$ .

Hebe Lee
Hebe Lee
Numerade Educator
02:26

Problem 19

(a) $A$ cancer patient is exposed to $\gamma$ rays from a $5000-C i$ 60 Co transillumination unit for 32.0 s. The $\gamma$ rays are collimated in such a manner that only 1.00$\%$ of them strike
the patient. Of those, 20.0$\%$ are absorbed in a tumor having a mass of 1.50 $\mathrm{kg}$ . What is the dose in rem to the tumor, if the average $\gamma$ energy per decay is 1.25 $\mathrm{MeV}$ ? None of the $\beta$ from the decay reach the patient. (b) Is the dose consistent with stated therapeutic doses?

Hebe Lee
Hebe Lee
Numerade Educator
02:18

Problem 20

What is the mass of 60 Co in a cancer therapy transillumination unit containing 5.00 $\mathrm{kCi}$ of $^{60} \mathrm{Co} ?$

Hebe Lee
Hebe Lee
Numerade Educator
02:00

Problem 21

Large amounts of $^{65} \mathrm{Zn}$ are produced in copper exposed to accelerator beams. While machining contaminated copper, a physicist ingests 50.0$\mu \mathrm{Ci}$ of $^{65} \mathrm{Zn} .$ Each 65 $\mathrm{Zn}$ decay emits an average $\gamma$ -ray energy of $0.550 \mathrm{MeV}, 40.0 \%$ of which is absorbed in the scientist's 75.0 -kg body. What dose in mSv is caused by this in one day?

Hebe Lee
Hebe Lee
Numerade Educator
03:47

Problem 22

Naturally occurring 40 $\mathrm{K}$ is listed as responsible for 16 mrem/y of background radiation. Calculate the mass of 40 that must be inside the $55-\mathrm{kg}$ body of a woman to produce this dose. Each 40 $\mathrm{K}$ decay emits a 1.32 -MeV $\beta$ , and 50$\%$ of the energy is absorbed inside the body.

Hebe Lee
Hebe Lee
Numerade Educator
04:19

Problem 23

(a) Background radiation due to ${ }^{226} \mathrm{Ra}$ averages only 0.01 mSvly, but it can range upward depending on where a person lives. Find the mass of $^{226}$ Ra in the 80.0 -kg body of a man who receives a dose of 2.50 -mev/y from it, noting that each $^{226}$ Ra decay emits a $4.80-$ Mev $\alpha$ particle. You may
neglect dose due to daughters and assume a constant amount, evenly distributed due to balanced ingestion and bodily elimination. (b) Is it surprising that such a small mass could cause a measurable radiation dose? Explain.

Hebe Lee
Hebe Lee
Numerade Educator
04:37

Problem 24

The annual radiation dose from $^{14} \mathrm{C}$ in our bodies is normal $12 \mathrm{C},$ and assuming the body is 13$\%$ carbon, estimate the fraction of the decay energy absorbed. (The rest
escapes, exposing those close to you.)

Hebe Lee
Hebe Lee
Numerade Educator
01:22

Problem 25

If everyone in Australia received an extra 0.05 msv per year of radiation, what would be the increase in the number of cancer deaths per year? (Assume that time had elapsed for the effects to become apparent.) Assume that there are $200 \times 10^{-4}$ deaths per Sv of radiation per year. What
$200 \times 10^{-4}$ deaths per Sv of radiation per year. What percent of the actual number of cancer deaths recorded is this?

Hebe Lee
Hebe Lee
Numerade Educator
03:26

Problem 26

Verify that the total number of nucleons, total charge, and electron family number are conserved for each of the fusion reactions in the proton-proton cycle in $$^{1} \mathrm{H}+^{1} \mathrm{H} \rightarrow^{2} \mathrm{H}+e^{+}+v_{\mathrm{e}},^{1} \mathrm{H}+^{2} \mathrm{H} \rightarrow^{3} \mathrm{He}+\gamma.$$ and $$^{3} \mathrm{He}+^{3} \mathrm{He} \rightarrow^{4} \mathrm{He}+^{1} \mathrm{H}+^{1} \mathrm{H}.$$ (List the value of each of the conserved quantities before and after each of the reactions.)

Hebe Lee
Hebe Lee
Numerade Educator
02:50

Problem 27

Calculate the energy output in each of the fusion reactions in the proton-proton cycle, and verify the values given in the above summary.

Hebe Lee
Hebe Lee
Numerade Educator
02:11

Problem 28

Show that the total energy released in the proton-proton cycle is 26.7 MeV, considering the overall effect in $^{1} \mathrm{H}+^{1} \mathrm{H} \rightarrow^{2} \mathrm{H}+e^{+}+v_{\mathrm{e}},^{1} \mathrm{H}+^{2} \mathrm{H} \rightarrow^{3} \mathrm{He}+\gamma,$ and
$^{3} \mathrm{He}+^{3} \mathrm{He} \rightarrow^{4} \mathrm{He}+^{1} \mathrm{H}+^{1} \mathrm{H}$ and being certain to include the annihilation energy.

Hebe Lee
Hebe Lee
Numerade Educator
01:49

Problem 29

Verify by listing the number of nucleons, total charge, and electron family number before and after the cycle that these quantities are conserved in the overall proton-proton cycle in
$2 e^{-}+4^{1} \mathrm{H} \rightarrow^{4} \mathrm{Hc}+2 v_{\mathrm{e}}+6 \gamma$

Hebe Lee
Hebe Lee
Numerade Educator
01:12

Problem 30

The energy produced by the fusion of a 1.00 -kg mixture of deuterium and tritium was found in Example Calculating Energy and Power from Fusion. Approximately how many kilograms would be required to supply the annual energy use in the United States?

Hebe Lee
Hebe Lee
Numerade Educator
01:10

Problem 31

Tritium is naturally rare, but can be produced by the reaction $n+^{2} \mathrm{H} \rightarrow^{3} \mathrm{H}+\gamma .$ How much energy in Mev is released in this neutron capture?

Hebe Lee
Hebe Lee
Numerade Educator
02:03

Problem 32

Two fusion reactions mentioned in the text are
$n+^{3} \mathrm{He} \rightarrow^{4} \mathrm{He}+\gamma$
and
$n+\mathrm{H} \rightarrow^{2} \mathrm{H}+\gamma$
Both reactions release energy, but the second also creates more fuel. Confirm that the energies produced in the reactions are 20.58 and 2.22 MeV, respectively. Comment on which product nuclide is most tightly bound, "He or $^{2} \mathrm{H}$ .

Hebe Lee
Hebe Lee
Numerade Educator
06:41

Problem 33

a) Calculate the number of grams of deuterium in an $80,000$ -L swimming pool, given deuterium is 0.0150$\%$ of natural hydrogen. (b) Find the energy released in joules if this deuterium is
fused via the reaction $^{2} \mathrm{H}+^{2} \mathrm{H} \rightarrow^{3} \mathrm{He}+n$
(c) Could the neutrons be used to create more energy?
(d) Discuss the amount of this type of energy in a swimming pool as compared to that in, say, a gallon of gasoline, also taking into consideration that water is far more abundant.

Hebe Lee
Hebe Lee
Numerade Educator
02:12

Problem 34

How many kilograms of water are needed to obtain the 198.8 mol of deuterium, assuming that deuterium is 0.01500$\%$ (by number) of natural hydrogen?

Hebe Lee
Hebe Lee
Numerade Educator
04:15

Problem 35

The power output of the Sun is $4 \times 10^{26} \mathrm{W}$ .
(a) If 90$\%$ of this is supplied by the proton-proton cycle, how many protons are consumed per second?
(b) How many neutrinos per second should there be per square meter at the Earth from this process? This huge number is indicative of how rarely a neutrino interacts, since large detectors observe very few per day.

Hebe Lee
Hebe Lee
Numerade Educator
02:47

Problem 36

Another set of reactions that result in the fusing of hydrogen into helium in the Sun and especially in hotter stars is called the carbon cycle. It is $\begin{aligned}{ }^{12} \mathrm{C}+{ }^{1} \mathrm{H} & \rightarrow{ }^{13} \mathrm{~N}+\gamma \\{ }^{13} \mathrm{~N} \quad & \rightarrow{ }^{13} \mathrm{C}+e^{+}+v_{e} \\{ }^{13} \mathrm{C}+{ }^{1} \mathrm{H} & \rightarrow{ }^{14} \mathrm{~N}+\gamma \\{ }^{14} \mathrm{~N}+{ }^{1} \mathrm{H} & \rightarrow{ }^{15} \mathrm{O}+\gamma \\{ }^{15} \mathrm{O} \quad &{ }^{15} \mathrm{~N}+e^{+}+v_{e}, \\{ }^{15} \mathrm{~N}+{ }^{1} \mathrm{H} & \rightarrow \quad{ }^{12} \mathrm{C}+{ }^{4} \mathrm{He} \end{aligned}$
Write down the overall effect of the carbon cycle (as was
done for the proton-proton cycle in $\left.2 e^{-}+4^{1} \mathrm{H} \rightarrow{ }^{4} \mathrm{He}+2 v_{e}+6 \gamma\right)$. Note the number of protons $\left({ }^{1} \mathrm{H}\right)$ required and assume that the positrons $\left(e^{+}\right)$
annihilate electrons to form more $\gamma$ rays.

Hebe Lee
Hebe Lee
Numerade Educator
02:03

Problem 37

(a) Find the total energy released in MeV in each carbon cycle (elaborated in the above problem) including the annihilation energy.
(b) How does this compare with the proton-proton cycle output?

Hebe Lee
Hebe Lee
Numerade Educator
04:49

Problem 38

Verify that the total number of nucleons, total charge, and electron family number are conserved for each of the fusion reactions in the carbon cycle given in the above problem. (List the value of each of the conserved quantities before and after each of the reactions.)

Hebe Lee
Hebe Lee
Numerade Educator
06:02

Problem 39

Integrated Concepts
The laser system tested for inertial confinement can produce
a 100 -kJ pulse only 1.00 ns in duration. (a) What is the power output of the laser system during the brief pulse?
(b) How many photons are in the pulse, given their wavelength is 1.06$\mu \mathrm{m} ?$
(c) What is the total momentum of all these photons?
(d) How does the total photon momentum compare with that of a single 1.00 MeV deuterium nucleus?

Hebe Lee
Hebe Lee
Numerade Educator
07:39

Problem 40

Integrated Concepts
Find the amount of energy given to the $^{4}$ He nucleus and to the $\gamma$ ray in the reaction $n+^{3} \mathrm{He} \rightarrow^{4} \mathrm{He}+\gamma,$ using the conservation of momentum principle and taking the reactants to be initially at rest. This should confirm the contention that
most of the energy goes to the $\gamma$ ray.

Hebe Lee
Hebe Lee
Numerade Educator
07:24

Problem 41

(a) What temperature gas would have atoms moving fast enough to bring two $^{3}$ He nuclei into contact? Note that, because both are moving, the average kinetic energy only needs to be half the electric potential energy of these doubly charged nuclei when just in contact with one another.
(b) Does this high temperature imply practical difficulties for doing this in controlled fusion?

Hebe Lee
Hebe Lee
Numerade Educator
03:11

Problem 42

(a) Estimate the years that the deuterium fuel in the oceans could supply the energy needs of the world. Assume world energy consumption to be ten times that of the United States which is $8 \times 10^{19}$ J/y and that the deuterium in the oceans could be converted to energy with an efficiency of 32$\%$ . You
must estimate or look up the amount of water in the oceans and take the deuterium content to be 0.015$\%$ of natural hydrogen to find the mass of deuterium available. Note that approximate energy yield of deuterium is $3.37 \times 10^{14}$ Jikg.
(b) Comment on how much time this is by any human measure. ( It is not an unreasonable result, only an impressive one.)

Hebe Lee
Hebe Lee
Numerade Educator
03:23

Problem 43

(a) Calculate the energy released in the neutron-induced fission (similar to the spontaneous fission in Example 32.3$)$
$n+^{238} \mathrm{U} \rightarrow^{96} \mathrm{Sr}+^{140} \mathrm{Xe}+3 n$
given $m\left(^{96} \mathrm{Sr}\right)=95.921750 \mathrm{u}$ and
$m(140 \mathrm{Xe})=139.92164 .$ (b) This result is about 6 $\mathrm{MeV}$
greater than the result for spontaneous fission. Why? (c) Confirm that the total number of nucleons and total charge are conserved in this reaction

Hebe Lee
Hebe Lee
Numerade Educator
03:05

Problem 44

(a) Calculate the energy released in the neutron-induced fission reaction
$n+^{235} \mathrm{U} \rightarrow^{92} \mathrm{Kr}+^{142} \mathrm{Ba}+2 n$
given $m\left(^{92} \mathrm{Kr}\right)=91.926269 \mathrm{u}$ and
$m\left(^{142} \mathrm{Ba}\right)=141.916361 \mathrm{u}$
(b) Confirm that the total number of nucleons and total charge are conserved in this reaction.

Hebe Lee
Hebe Lee
Numerade Educator
02:49

Problem 45

(a) Calculate the energy released in the neutron-induced fission reaction $n+^{239} \mathrm{Pu} \rightarrow^{96} \mathrm{Sr}+^{140} \mathrm{Ba}+4 n$
given $m\left(^{96} \mathrm{Sr}\right)=95.921750 \mathrm{u}$ and
$m(140 \mathrm{Ba})=139.910581 \mathrm{u}$
(b) Confirm that the total number of nucleons and total charge are conserved in this reaction.

Hebe Lee
Hebe Lee
Numerade Educator
02:57

Problem 46

Confirm that each of the reactions listed for plutonium breeding just following Example 32.4 conserves the total number of nucleons, the total charge, and electron family number.

Hebe Lee
Hebe Lee
Numerade Educator
02:51

Problem 47

Breeding plutonium produces energy even before any plutonium is fissioned. (The primary purpose of the four nuclear reactors at Chernobyl was breeding plutonium for weapons. Electrical power was a by-product used by the civilian population.) Calculate the energy produced in each of the reactions listed for plutonium breeding just following Example $32.4 .$ The pertinent masses are $m\left({ }^{239} \mathrm{U}\right)=239.054289 \mathrm{u}, m\left({ }^{239} \mathrm{~Np}\right)=239.052932 \mathrm{u}$ and $m\left({ }^{239} \mathrm{Pu}\right)=239.052157 \mathrm{u}$

Hebe Lee
Hebe Lee
Numerade Educator
05:51

Problem 48

The naturally occurring radioactive isotope 232 Th does not make good fission fuel, because it has an even number of neutrons; however, it can be bred into a suitable fuel (much as $^{238} \mathrm{U}$ is bred into 239 $\mathrm{P}$ ).
(a) What are $Z$ and $N$ for 232 Th?
(b) Write the reaction equation for neutron captured by 232 Th and identify the nuclide $A X$ produced in
$n+232 \mathrm{Th} \rightarrow^{A} X+\gamma$
(c) The product nucleus $\beta^{-}$ decays, as does its daughter Write the decay equations for each, and identify the final nucleus.
(d) Confirm that the final nucleus has an odd number of neutrons, making it a better fission fuel.
(e) Look up the half-life of the final nucleus to see if it lives long enough to be a useful fuel.

Colton Wang
Colton Wang
Numerade Educator
03:15

Problem 49

The electrical power output of a large nuclear reactor facility is 900 $\mathrm{MW} .$ It has a 35.0$\%$ efficiency in converting nuclear power to electrical.
(a) What is the thermal nuclear power output in megawatts?
(b) How many 235 U nuclei fission each second, assuming the average fission produces 200 Mev?
(c) What mass of 235 U is fissioned in one year of full-power operation?

Hebe Lee
Hebe Lee
Numerade Educator
01:48

Problem 50

A large power reactor that has been in operation for some months is turned off, but residual activity in the core still produces 150 $\mathrm{MW}$ of power. If the average energy per decay of the fission products is $1.00 \mathrm{MeV},$ what is the core activity in curies?

Hebe Lee
Hebe Lee
Numerade Educator
01:18

Problem 51

Find the mass converted into energy by a $12.0-\mathrm{kT}$ bomb.

Hebe Lee
Hebe Lee
Numerade Educator
00:49

Problem 52

What mass is converted into energy by a 1.00 -MT bomb?

Hebe Lee
Hebe Lee
Numerade Educator
01:09

Problem 53

Fusion bombs use neutrons from their fission trigger to create tritium fuel in the reaction $n+^{6} \mathrm{Li} \rightarrow^{3} \mathrm{H}+^{4} \mathrm{He}$ What is the energy released by this reaction in MeV?

Hebe Lee
Hebe Lee
Numerade Educator
01:27

Problem 54

It is estimated that the total explosive yield of all the nuclear bombs in existence currently is about $4,000 \mathrm{MT}$ .
(a) Convert this amount of energy to kilowatt-hours, noting that $1 \mathrm{kW} \cdot \mathrm{h}=3.60 \times 10^{6} \mathrm{J}$ .
(b) What would the monetary value of this energy be if it could be converted to electricity costing 10 cents per kw-h?

Hebe Lee
Hebe Lee
Numerade Educator
01:40

Problem 55

A radiation-enhanced nuclear weapon (or neutron bomb) can have a smaller total yield and still produce more prompt radiation than a conventional nuclear bomb. This allows the use of neutron bombs to kill nearby advancing enemy forces with radiation without blowing up your own forces with the blast. For a 0.500 -kT radiation-enhanced weapon and a 1.00-kT conventional nuclear bomb: (a) Compare the blast
yields. (b) Compare the prompt radiation yields.

Hebe Lee
Hebe Lee
Numerade Educator
01:44

Problem 56

(a) How many 239 Pu nuclei must fission to produce a 20.0 -kT yield, assuming 200 MeV per fission? (b) What is the mass of this much 239 $\mathrm{Pu}$ ?

Hebe Lee
Hebe Lee
Numerade Educator
04:33

Problem 57

Assume one-fourth of the yield of a typical $320-\mathrm{kT}$ strategic bomb comes from fission reactions averaging 200 MeV and the remainder from fusion reactions averaging 20 MeV.
(a) Calculate the number of fissions and the approximate mass of uranium and plutonium fissioned, taking the average atomic mass to be $238 .$
(b) Find the number of fusions and calculate the approximate mass of fusion fuel, assuming an average total atomic mass of the two nuclei in each reaction to be $5 .$
(c) Considering the masses found, does it seem reasonable that some missiles could carry 10 warheads? Discuss, noting that the nuclear fuel is only a part of the mass of a warhead.

Hebe Lee
Hebe Lee
Numerade Educator
01:37

Problem 58

This problem gives some idea of the magnitude of the energy yield of a small tactical bomb. Assume that half the energy of a $1.00-\mathrm{kT}$ nuclear depth charge set off under an aircraft carrier goes into lifting it out of the water-that is, into gravitational potential energy. How high is the carrier lifted if its mass is 90,000 tons?

Hebe Lee
Hebe Lee
Numerade Educator
01:53

Problem 59

It is estimated that weapons tests in the atmosphere have deposited approximately 9 MCi of $^{90}$ Sr on the surface of the earth. Find the mass of this amount of 90 Sr.

Hebe Lee
Hebe Lee
Numerade Educator
02:46

Problem 60

A 1.00 -MT bomb exploded a few kilometers above the ground deposits 25.0$\%$ of its energy into radiant heat.
(a) Find the calories per $\mathrm{cm}^{2}$ at a distance of 10.0 $\mathrm{km}$ by assuming a uniform distribution over a spherical surface of that radiurs
(b) If this heat falls on a person's body, what temperature increase does it cause in the affected tissue, assuming it is absorbed in a layer 1.00-cm deep?

Hebe Lee
Hebe Lee
Numerade Educator
01:26

Problem 61

One scheme to put nuclear weapons to nonmilitary use is to explode them underground in a geologically stable region and extract the geothermal energy for electricity production. There was a total yield of about $4,000$ MT in the combined arsenals in $2006 .$ If 1.00 MT per day could be converted to electricity with an efficiency of $10.0 \% :$.
(a) What would the average electrical power output be?
(b) How many years would the arsenal last at this rate?

Hebe Lee
Hebe Lee
Numerade Educator