Chapter 14: Nuclear and Particle Physics — Review and Exercises
Chapter contents: Chapter 14: Nuclear and Particle Physics
Glossary
activity
the expected number of radioactive decays per unit time in a sample; also called decay rate
alpha decay
type of radioactive decay in which an atomic nucleus emits an alpha particle
alpha ray
a component of nuclear radioactivity; consists of two protons and two neutrons
Anger camera
a common medical imaging device that uses a scintillator connected to a series of photomultipliers
antielectron
another name for the positron, the electron’s antiparticle
antimatter
composed of antiparticles
atomic mass
the mass of an atom, including the effects of the binding of its constituents; it is less than the sum of the masses of its separated protons, neutrons, and electrons
atomic number
number of protons in a nucleus
baryon number
a quantum number equal to +1 for baryons, −1 for antibaryons, and zero for mesons and leptons; in the quark model, one third of the number of quarks minus antiquarks
baryons
hadrons whose simplest quark structure consists of three quarks bound together; antibaryons consist of three antiquarks
becquerel
SI unit for rate of decay of a radioactive material
beta decay
type of radioactive decay in which an atomic nucleus emits a beta particle
beta ray
an electron or positron emitted in nuclear beta decay
boson
particle with an integer value of intrinsic spin
break-even
equality of fusion energy output and a specified energy input; the boundary used to count input energy must be stated
breeder reactors
reactors designed to produce more fissile material than they consume
breeding
production of new fissile material from fertile material by neutron capture and subsequent nuclear transformations
carbon-14 dating
a radioactive dating technique based on the radioactivity of carbon-14
chart of the nuclides
a table comprising stable and unstable nuclei
conservation of total baryon number
the rule that total baryon number remains unchanged in a reaction or decay; no violation has been observed
conservation of total electron family number
equality of the total electron family number before and after a process; applicable to the decay examples here, but not a universal law because of neutrino oscillations
conservation of total muon family number
equality of the total muon family number before and after a process; applicable to the decay examples here, but not a universal law because of neutrino oscillations
critical mass
the minimum mass of fissile material needed for a self-sustaining chain reaction under specified conditions of composition, shape, density, and surroundings
criticality
the condition in which each generation of fissions produces, on average, one succeeding generation of the same size
curie
a unit of activity equal to exactly 3.7 × 1010 becquerels (decays per second), originally based on the activity of one gram of radium-226
daughter
the nucleus obtained when parent nucleus decays and produces another nucleus following the rules and the conservation laws
decay
a spontaneous transformation of an unstable particle or nucleus; nuclear decay produces a different nucleus or a lower-energy nuclear state
decay constant
the probability per unit time that an undecayed nucleus will decay; the constant determining the exponential decay rate
decay series
process whereby subsequent nuclides decay until a stable nuclide is produced
effective dose
the sum of organ and tissue equivalent doses multiplied by tissue weighting factors; used in radiation protection to compare long-term risks and measured in sieverts (Sv) or rem
electron antineutrino
antiparticle of the electron neutrino
electron capture
the process in which a proton-rich nuclide absorbs an inner atomic electron and simultaneously emits a neutrino
electron family number
the number of electron-family leptons minus their antiparticles, with other particles contributing zero
electron neutrino
the electrically neutral lepton of electron flavor, associated with the electron in weak interactions
electroweak theory
the unified theory describing electromagnetic and weak interactions
equivalent dose
the average absorbed doses to an organ or tissue from each radiation type, multiplied by their radiation weighting factors and added; measured in sieverts (Sv) or rem
fermion
particle with a half-integer value of intrinsic spin
Feynman diagram
a diagram representing a contribution to the calculation of a quantum interaction
fission fragments
the daughter nuclei produced when a heavy nucleus undergoes fission
gamma camera
another name for an Anger camera
gamma decay
a nuclear transition to a lower-energy state by emission of a gamma-ray photon, without changing the numbers of protons or neutrons
gauge boson
a particle associated with a gauge field; the Standard Model gauge bosons are the photon, gluons, and W and Z bosons
Geiger tube
a gas-filled radiation detector in which ionizing radiation triggers an electrical discharge that can be registered as a count
gluons
the eight types of particles that carry the strong interaction between quarks. Gluons themselves carry color charge and can interact with one another
grand unified theory
a proposed theory that places the strong and electroweak interactions within a single framework
gray (Gy)
the SI unit of absorbed dose; 1 Gy = 1 J/kg = 100 rad
hadrons
composite particles whose constituents are bound by the strong interaction
half-life
the time in which there is a 50% chance that a nucleus will decay
Higgs boson
an elementary particle with zero spin associated with the Higgs field, discovered in 2012; its discovery supports the mechanism by which the W and Z bosons acquire mass
high dose
an absorbed dose greater than 1 Gy (100 rad) for X-rays and gamma rays
hormesis
a term used to describe generally favorable biological responses to low exposures of toxins or radiation
ignition
fusion conditions in which heating by fusion products sustains the hot fuel against energy losses
inertial confinement
brief confinement of rapidly compressed fusion fuel by its own inertia before it expands
ionizing radiation
a radiation that produces ionization; examples include alpha rays, beta rays, gamma rays, and X-rays
isotopes
nuclei having the same and different s
leptons
elementary particles that do not participate in the strong interaction, including electrons, muons, taus, neutrinos, and their antiparticles
linear hypothesis
the model that additional cancer risk is proportional to radiation dose, with no threshold below which the risk is zero
liquid drop model
a model that treats a nucleus as a drop of nuclear matter to describe collective properties such as binding and deformation
low dose
an absorbed dose less than 0.1 Gy (10 rad) for X-rays and gamma rays
magic numbers
a number that indicates a shell structure for the nucleus in which closed shells are more stable
magnetic confinement
a technique in which charged particles are trapped in a small region because of difficulty in crossing magnetic field lines
mass number
number of nucleons in a nucleus
meson
a hadron whose simplest quark structure consists of a quark and an antiquark bound together
moderate dose
an absorbed dose from 0.1 to 1 Gy (10 to 100 rad) for X-rays and gamma rays
muon family number
the number of muon-family leptons minus their antiparticles, with other particles contributing zero
neutrino
an electrically neutral elementary lepton that participates in the weak interaction; neutrinos occur in electron, muon, and tau flavors
neutron
an electrically neutral particle found in atomic nuclei; a free neutron is unstable and undergoes beta decay
neutron activation
the production of radioactive isotopes through interactions of neutrons with atomic nuclei
neutron-induced fission
fission that is initiated after the absorption of neutron
nuclear fission
reaction in which a nucleus splits
nuclear fusion
a reaction in which two nuclei are combined, or fused, to form a larger nucleus
nuclear radiation
radiation that originate in the nuclei of atoms; alpha, beta, and gamma rays are among most common forms; also see “radioactivity”
nuclear reaction energy
the energy released or required in a nuclear reaction, determined by the difference between the total initial and final rest energies
nucleons
protons and neutrons, the constituents of atomic nuclei
nucleus
a region consisting of protons and neutrons at the center of an atom
nuclide
a type of atom whose nucleus has specific numbers of protons and neutrons
parent
the original state of nucleus before decay
photomultiplier tube
a device that converts faint light into an electrical signal and amplifies it through successive stages of electron multiplication
positron
the antiparticle of the electron, with the same mass and a positive electric charge; also called an antielectron
positron decay
type of beta decay in which a proton is converted to a neutron, releasing a positron and a neutrino
positron emission tomography (PET)
tomography technique that uses emitters and detects the two annihilation rays, aiding in source localization
proton-proton cycle
a sequence of fusion reactions whose net effect is to convert four protons into a helium-4 nucleus, with positrons, electron neutrinos, and released energy
quality factor
a factor used to weight absorbed dose in dose-equivalent quantities for radiation monitoring; distinct from RBE
quantum chromodynamics
the theory of the strong interaction between quarks and gluons, based on color charge
quantum electrodynamics
the theory of electromagnetism on the particle scale
rad
an older unit of absorbed dose; 1 rad = 0.01 Gy = 0.01 J/kg
radiation detector
a device that registers radiation through its interaction with matter
radiation weighting factor
a standardized factor used to weight absorbed dose for radiation type when calculating equivalent dose
radioactive
a substance or object that emits nuclear radiation
radioactive dating
an application of radioactive decay in which the age of a material is determined by the amount of radioactivity of a particular type that occurs
radioactivity
spontaneous transformation of an unstable nucleus into a different nucleus or a lower-energy nuclear state
radiopharmaceutical
a preparation containing a radionuclide and used for medical diagnosis or treatment
range of radiation
the distance radiation travels through a material; alpha and beta particles have stopping ranges, while gamma rays are attenuated without a definite stopping range
relative biological effectiveness (RBE)
the ratio of absorbed doses of a reference radiation and the radiation being studied that produce the same specified biological effect
roentgen equivalent man (rem)
an older unit of equivalent dose and effective dose; 1 rem = 0.01 Sv
scintillators
materials that emit brief flashes of light when they absorb energy from ionizing radiation
shielding
a technique to limit radiation exposure
sievert
the SI unit of equivalent dose and effective dose; 1 Sv = 100 rem
single-photon-emission computed tomography (SPECT)
tomography performed with -emitting radiopharmaceuticals
solid-state radiation detectors
semiconductors fabricated to directly convert incident radiation into electrical current
Standard Model
the theory describing known elementary particles and their strong, weak, and electromagnetic interactions; it includes quarks, leptons, force-carrier particles, and the Higgs boson, but does not include gravity
strangeness
a quantum number equal to the number of strange antiquarks minus the number of strange quarks in a particle. Total strangeness is conserved in strong and electromagnetic interactions but can change in weak interactions
supercriticality
the condition in which the fission chain reaction grows because each generation produces more fissions in the next
superstring theory
a proposed theoretical framework in which fundamental particles correspond to different vibrational states of strings and which incorporates supersymmetry
tagged
process of attaching a radioactive substance to a chemical compound
tau family number
the number of tau-family leptons minus their antiparticles, with other particles contributing zero
Section Summary
14.2: Nuclear Radioactivity
- Some nuclei are radioactive—they spontaneously decay destroying some part of their mass and emitting energetic rays, a process called nuclear radioactivity.
- Nuclear radiation, like X-rays, is ionizing radiation, because energy sufficient to ionize matter is emitted in each decay.
- The range (or distance traveled in a material) of ionizing radiation is affected by the charge of the emitted particle and its energy. Greater electric charge and lower energy lead to shorter ranges; less electric charge and higher energy lead to longer ranges.
- Radiation detectors are based directly or indirectly upon the ionization created by radiation, as are the effects of radiation on living and inert materials.
14.3: Radiation Detection and Detectors
- Radiation detectors are based directly or indirectly upon the ionization created by radiation, as are the effects of radiation on living and inert materials.
14.4: Substructure of the Nucleus
- Two particles, both called nucleons, are found inside nuclei. The two types of nucleons are protons and neutrons; they are very similar, except that the proton is positively charged while the neutron is neutral. Some of their characteristics are given in Table 14.4.1 and compared with those of the electron. A mass unit convenient to atomic and nuclear processes is the unified atomic mass unit (u), defined to be
.
- A nuclide is a specific combination of protons and neutrons, denoted by
or simply , where is the number of protons or atomic number, X is the symbol for the element, is the number of neutrons, and is the mass number or the total number of protons and neutrons,
.(14.4.4)
- Nuclides having the same but different are isotopes of the same element.
- The radius of a nucleus, , is approximately
where . Nuclear volumes are proportional to . There are two nuclear forces, the weak and the strong. Systematics in nuclear stability seen on the chart of the nuclides indicate that there are shell closures in nuclei for values of and equal to the magic numbers, which correspond to highly stable nuclei.,(14.4.6)
14.5: Nuclear Decay and Conservation Laws
- When a parent nucleus decays, it produces a daughter nucleus following rules and conservation laws. There are three major types of nuclear decay, called alpha , beta , and gamma . The decay equation is .(14.5.3)
- Nuclear decay releases an amount of energy related to the mass destroyed by.(14.5.4)
- There are three forms of beta decay. The decay equation is
.(14.5.6)
- The decay equation is .(14.5.8)
- The electron capture equation is .(14.5.11)
- is an electron, is an antielectron or positron, represents an electron neutrino, and is an electron antineutrino. In addition to all previously known conservation laws, two new ones arise— conservation of electron family number and conservation of the total number of nucleons. The decay equation is is a high-energy photon originating in a nucleus.(14.5.12)
14.6: Half-Life and Activity
- Half-life is the time in which there is a 50% chance that a nucleus will decay. The number of nuclei as a function of time iswhere is the number present at , and is the decay constant, related to the half-life by,(14.6.2).(14.6.3)
- One of the applications of radioactive decay is radioactive dating, in which the age of a material is determined by the amount of radioactive decay that occurs. The rate of decay is called the activity :.(14.6.4)
- The SI unit for is the becquerel (Bq), defined by.(14.6.5)
- is also expressed in terms of curies (Ci), where
.(14.6.6)
- The activity of a source is related to and by.(14.6.7)
- Since has an exponential behavior as in the equation , the activity also has an exponential behavior, given bywhere is the activity at .,(14.6.8)
14.7: Medical Imaging and Diagnostics
- Radiopharmaceuticals are compounds that are used for medical imaging and therapeutics.
- The process of attaching a radioactive substance is called tagging.
- Table 14.7.1 lists selected diagnostic uses of radiopharmaceuticals, with named preparations and adult activity ranges.
- One common imaging device is the Anger camera, which consists of a lead collimator, radiation detectors, and an analysis computer.
- Tomography performed with -emitting radiopharmaceuticals is called SPECT and has the advantages of x-ray CT scans coupled with organ- and function-specific drugs.
- PET is a similar technique that uses emitters and detects the two annihilation rays, which aid to localize the source.
14.8: Biological Effects of Ionizing Radiation
- The biological effects of ionizing radiation are due to two effects it has on cells: interference with cell reproduction, and destruction of cell function.
- A radiation dose unit called the rad is defined in terms of the ionizing energy deposited per kilogram of tissue:
.(14.8.1)
- The SI unit for radiation dose is the gray (Gy), which is defined to be .
- To account for radiation type in radiation protection, we use the radiation weighting factors in Table 14.8.1. For one radiation type, equivalent dose H is average absorbed dose D to the organ or tissue multiplied by its radiation weighting factor:(14.8.3)
- Effective dose also accounts for the different sensitivities of organs and tissues by applying tissue weighting factors to their equivalent doses and adding the results. Equivalent and effective doses are measured in sieverts (Sv) or rem:.(14.8.4)
- For X-rays and gamma rays, absorbed doses below 0.1 Gy are called low, those from 0.1 to 1 Gy moderate, and those above 1 Gy high. Some effects of acute whole-body radiation exposure are given in Table 14.8.3. The linear hypothesis assumes that cancer risk is proportional to dose. The estimated additional lifetime risk of dying from radiation-induced cancer is about 300 in a million per rem of whole-body exposure, within an order of magnitude. Heritable effects have not been demonstrated in the offspring of Hiroshima and Nagasaki survivors. Background radiation doses and sources are given in Table 14.8.4. World-wide average annual effective dose from natural sources, including radon, is about 3 mSv, or 300 mrem. Radiation protection utilizes time, distance, and shielding to limit exposure.
14.9: Fusion
- Nuclear fusion is a reaction in which two nuclei are combined to form a larger nucleus. It releases energy when light nuclei are fused to form medium-mass nuclei.
- Fusion is the source of energy in stars, with the proton-proton cycle,
(14.9.1)(14.9.2)(14.9.3)being the principal sequence of energy-producing reactions in our Sun.
- The overall effect of the proton-proton cycle is
,(14.9.4)where the 26.7 MeV includes the energy of the positrons emitted and annihilated.
- Attempts to utilize controlled fusion as an energy source on Earth are related to deuterium and tritium, and the reactions play important roles.
- Ignition occurs when energy deposited by fusion products sustains the fuel’s heating against its losses. Break-even compares fusion output with a specified energy input. NIF has achieved ignition and output greater than the laser energy delivered to its target; this does not mean the facility produces net useful electrical energy.
- Magnetic confinement and inertial confinement are the two methods being developed for heating fuel to sufficiently high temperatures, at sufficient density, and for sufficiently long times to achieve ignition. Magnetic confinement uses magnetic fields. In laser-driven inertial confinement, expanding hot plasma compresses the fuel, whose inertia keeps it dense briefly before it expands.
14.10: Fission
- Nuclear fission is a reaction in which a nucleus is split.
- Fission releases energy when heavy nuclei are split into medium-mass nuclei.
- Self-sustained fission is possible, because neutron-induced fission also produces neutrons that can induce other fissions, , where and are the two daughter nuclei, or fission fragments, and x is the number of neutrons produced.
- A minimum mass, called the critical mass, should be present to achieve criticality.
- More than a critical mass can produce supercriticality.
- The production of new or different isotopes (especially ) by nuclear transformation is called breeding, and reactors designed for this purpose are called breeder reactors.
14.11: Nuclear Weapons
- There are two types of nuclear weapons—fission bombs use fission alone, whereas thermonuclear bombs use fission to ignite fusion.
- Both types of weapons produce huge numbers of nuclear reactions in a very short time.
- Energy yields are measured in kilotons or megatons of equivalent conventional explosives and range from 0.1 kT to more than 20 MT.
- Nuclear bombs are characterized by far more thermal output and nuclear radiation output than conventional explosives.
14.12: The Four Basic Forces
- The four basic forces and their carrier particles are summarized in the Table 14.12.1.
- Feynman diagrams represent contributions to quantum interaction calculations. Lines represent particles or their propagation, and vertices represent interactions; the lines are not measured trajectories.
- The theory of electromagnetism on the particle scale is called quantum electrodynamics (QED).
14.13: Particles, Patterns, and Conservation Laws
- All particles of matter have an antimatter counterpart that has the opposite charge and certain other quantum numbers as seen in Table 14.13.1. These matter-antimatter pairs are otherwise very similar but will annihilate when brought together. Known particles can be divided into three major groups—leptons, hadrons, and carrier particles (gauge bosons).
- Leptons do not feel the strong nuclear force and are further divided into three groups—electron family designated by electron family number ; muon family designated by muon family number ; and tau family designated by tau family number . The family numbers are not universally conserved due to neutrino oscillations.
- Hadrons are particles that feel the strong nuclear force and are divided into baryons, with the baryon family number being conserved, and mesons.
14.14: GUTs: The Unification of Forces
- Electroweak theory unifies the electromagnetic and weak interactions. Grand unified theories propose a further unification with the strong interaction.
- Eight types of gluons carry the strong interaction described by quantum chromodynamics (QCD). QCD and electroweak theory together form the Standard Model, which describes elementary particles and their strong, weak, and electromagnetic interactions.
- Further unification remains unconfirmed. Some grand unified theories predict proton decay, with lifetimes and decay modes that depend on the model. Searches have found no convincing evidence of proton decay and constrain these theories.
Questions and Exercises
14.2: Nuclear Radioactivity
Exercise 1
What characteristics of radioactivity show it to be nuclear in origin and not atomic?
Exercise 2
(a) Identify the particles emitted as radiation, radiation, radiation, and radiation.
(b) An particle of a given energy has a quoted range of 2.0 mm in a material. Does every such particle stop at exactly 2.0 mm? Explain.
Exercise 3
Match each description to , , , or radiation: (a) a helium-4 nucleus, (b) an electron, (c) a positron, and (d) a high-energy photon. Give the electric charge of each in units of the positive elementary charge.
Exercise 4
particles, particles, particles, and rays travel horizontally between two plates. The upper plate is positively charged and the lower plate is negatively charged. Which beams deflect upward, which deflect downward, and which continue straight? Explain using their charges.
Exercise 5
What is the difference between rays and characteristic X-rays? Is either necessarily more energetic than the other? Which can be the most energetic?
Exercise 6
For typical radioactive-source energies, explain why paper can stop particles, a suitable thickness of plastic can stop beta particles, and much thicker shielding is usually needed to substantially reduce radiation. Why does “reducing the intensity” describe shielding more accurately than “stopping every photon”?
Exercise 7
For each source below, suggest a suitable shielding material and explain your choice: (a) a source of particles, (b) a source of particles, and (c) a source of rays. Why must the particle energy and shield thickness also be considered?
Exercise 8
In an idealized narrow-beam measurement, each 1.50-cm layer of lead transmits 10.0% of the rays incident on that layer. What percentage of the original beam remains after two layers? After three? What total thickness leaves 0.100%?
Exercise 9
Workers handling radioactive contamination may wear disposable coveralls and gloves. Explain what these prevent. Why do such garments provide little shielding against penetrating rays?
Exercise 10
Where does the energy released in radioactive decay come from? Explain how the total rest mass of the products can be smaller than that of the parent while total energy is conserved.
14.3: Radiation Detection and Detectors
Exercise 11
What does it mean to ionize an atom or molecule? Explain how ionizing radiation can damage living cells even when the incident radiation is electrically neutral.
Exercise 12
Explain why ionizing radiation can damage living cells. In your answer, describe what ionization does to an atom or molecule and how this can affect DNA or other cell structures. Does the radiation itself need to carry an electric charge to cause this damage?
Exercise 13
A gas detector requires an average of 30 eV of deposited energy per ion pair produced. A particle deposits 0.60 MeV in the gas. Estimate the number of ion pairs produced. Use .
Exercise 14
Is it possible for light emitted by a scintillator to be too low in frequency to be used in a photomultiplier tube? Explain.
14.4: Substructure of the Nucleus
Exercise 15
Explain the relationships among the terms nucleus, nucleon, proton, neutron, and nuclide. Is a neutrino a nucleon? Explain.
Exercise 16
For helium-4 (), carbon-14 (), cobalt-60 (), and uranium-235 (), give the numbers of protons, neutrons, and total nucleons. Which number identifies the element?
Exercise 17
Give the numbers of protons and neutrons in carbon-12, carbon-14, cobalt-60, cesium-137, and uranium-238. The atomic numbers are 6 for carbon, 27 for cobalt, 55 for cesium, and 92 for uranium. Which two listed nuclides are isotopes of the same element, and how do you know?
Exercise 18
What are isotopes? Why do different isotopes of the same element have similar chemistries?
Exercise 19
Protons repel one another electrically. What interaction helps bind protons and neutrons into nuclei, and why does its short range matter? Which interaction is responsible for beta decay?
Exercise 20
Which statements correctly describe the interaction that binds protons and neutrons in ordinary nuclei? Explain each choice.
(a) It is effective only over very short distances.
(b) It acts only between protons.
(c) It can overcome electric repulsion between neighboring protons.
(d) It is the same inverse-square force that binds electrons to nuclei.
14.5: Nuclear Decay and Conservation Laws
Exercise 21
Polonium-210 () undergoes decay. Write the complete decay equation and identify the daughter; lead has . Check the total charge and number of nucleons.
Exercise 22
Tritium, hydrogen-3 (), undergoes decay. Write the complete decay equation, including the electron and electron antineutrino. Identify the daughter; helium has .
Exercise 23
A free neutron undergoes decay: . Check electric charge and nucleon number before and after the decay. Using for the electron and −1 for the electron antineutrino, check electron-family number as well.
Exercise 24
An electron and a positron initially at rest annihilate into two photons. Explain why the photons travel in opposite directions and have equal energies. What supplies their energy?
Exercise 25
Manganese-50 () undergoes decay. Write the complete decay equation, including the positron and electron neutrino. Identify the daughter; chromium has .
Exercise 26
Beryllium-7 () captures an electron. Write the complete reaction equation, including the electron neutrino. Identify the daughter; lithium has .
Exercise 27
In electron capture, a proton in a nucleus and an electron become a neutron and an electron neutrino. Show that electric charge is conserved. Using for an electron and for an electron neutrino, explain why the emitted neutrino is consistent with electron-family-number conservation in this reaction.
Exercise 28
For decay, decay, and electron capture, describe how a neutron or proton changes and how and change. How do those changes differ from decay? What happens to and in emission?
14.6: Half-Life and Activity
Exercise 29
Many samples each initially contain 100 nuclei of the same radioactive isotope. After one half-life, the remaining radioactive nuclei in each sample are counted. Describe what you would expect to find when comparing the samples. How would the results change if each sample initially contained one million radioactive nuclei? Discuss the fraction remaining as well as the number.
Exercise 30
In a -year-old rock that originally contained some , which has a half-life of
years, we expect to find some remaining in it. Why are , , and also found in such a rock, even though they have much shorter half-lives (1600 years, 3.8 days, and 138 days, respectively)?
Exercise 31
Carbon-14 has a half-life of 5700 years. Assume a closed sample initially contained 8000 carbon-14 atoms and now contains about 1000. How many half-lives have passed, and what age does this suggest? Explain why this is an estimate rather than an exact clock for each atom.
Exercise 32
Carbon-14 has a half-life of 5700 years. Assume that a closed sample initially contains 1600 carbon-14 atoms.
(a) About how many remain after 11,400 years?
(b) If about 200 remain, how much time has passed?
Exercise 33
A sealed source has an initial activity of 800 Bq and a half-life of 5.0 years.
(a) What activity is expected after 15 years?
(b) How long until the expected activity is 50 Bq? Assume the daughter contributes no measured activity and the measurement conditions remain unchanged.
14.7: Medical Imaging and Diagnostics
Exercise 34
Which of these imaging methods use ionizing radiation: conventional X-ray imaging, CT, PET, MRI, and ultrasound? For each, identify the kind of radiation or physical signal used. Explain why “does not use ionizing radiation” does not mean that an imaging method has no safety considerations.
Exercise 35
Consider a conventional X-ray image, a CT scan, a PET scan, an MRI scan, and an ultrasound image.
(a) Which use ionizing radiation?
(b) Which of these uses a radioactive substance administered to the patient?
(c) Does receiving an X-ray image ordinarily make the patient radioactive? Explain.
Exercise 36
In terms of radiation dose, what is the major difference between medical diagnostic uses of radiation and medical therapeutic uses?
Exercise 37
Why can a short physical half-life help limit the time a diagnostic radiopharmaceutical remains radioactive? Why must its half-life still be long enough for preparation and imaging?
Exercise 38
Molybdenum-99 () undergoes decay to technetium-99, often in the metastable state technetium-99m. Write the equation including the electron antineutrino. When technetium-99m emits a photon, do its proton and neutron counts change?
Exercise 39
In PET imaging, a positron emitted by a radiopharmaceutical annihilates with an electron. Explain why detecting two photons at nearly the same time on opposite sides of the patient helps locate the event. What does the location of the two detectors tell you about where the annihilation occurred, and what remains undetermined?
14.8: Biological Effects of Ionizing Radiation
Exercise 40
Why can an -emitting material be much more hazardous when inhaled or swallowed than when it is outside intact skin? Explain why radiation can contribute to exposure even when its source remains outside the body.
Exercise 41
Why is radon more closely associated with inducing lung cancer than other types of cancer?
Exercise 42
Suppose a person swallows some radioactive material by accident. What information is needed to be able to assess possible damage?
Exercise 43
Describe how each change can reduce exposure to a radiation source: (a) spending less time near it, (b) working farther away, and (c) placing suitable shielding between it and the worker. Why must the shielding material and thickness be chosen for the radiation involved?
Exercise 44
A worker must briefly handle equipment near a sealed -ray source. Suggest one change involving time, one involving distance, and one involving shielding that could reduce exposure. Explain why a pair of ordinary disposable gloves cannot substitute for these measures against the rays.
14.9: Fusion
Exercise 45
Why does the fusion of light nuclei into heavier nuclei release energy?
Exercise 46
Energy input is required to fuse medium-mass nuclei, such as iron or cobalt, into more massive nuclei. Explain why.
Exercise 47
The net conversion in the proton–proton chain, including positron annihilation, can be written , where is the released energy. Check electric charge and nucleon number. If is +1 for an electron and an electron neutrino, check electron-family number too.
Exercise 48
Light nuclei can release energy when they fuse. Why is it nevertheless difficult to start and sustain fusion? Explain the roles of electric repulsion, high temperature, and keeping the reacting nuclei together long enough.
14.10: Fission
Exercise 49
Explain why the fission of heavy nuclei releases energy. Similarly, why is it that energy input is required to fission light nuclei?
Exercise 50
A heavy nucleus splits into two smaller nuclei in one reaction; two light nuclei combine in another.
(a) Name the two processes.
(b) Which powers the Sun?
(c) Can both release energy?
(d) When either releases energy, how does the total rest mass of the products compare with that of the reactants?
Exercise 51
In the fission reaction , determine x by conserving nucleon number. Check electric charge using for U, 36 for Kr, and 56 for Ba. How can the emitted neutrons help sustain a chain reaction?
Exercise 52
Radioactivity depends on the nucleus and not the atom or its chemical state. Why, then, is one kilogram of uranium more radioactive than one kilogram of uranium hexafluoride containing uranium of the same isotopic composition?
Exercise 53
In a steady fission chain reaction, about how many neutrons from each fission must, on average, cause another fission? Explain how neutron absorption and leakage affect whether the chain reaction dies away, stays steady, or grows. How do control rods help regulate it?
Exercise 54
Fission commonly leaves radioactive fission products. Does that mean a fusion facility would necessarily produce no radioactive material? Discuss how neutrons from some fusion reactions can affect surrounding materials.
Exercise 55
Control rods stop the self-sustaining fission chain reaction in a nuclear reactor, but the reactor still requires cooling. Explain the source of the continuing energy release and why inserting the control rods does not stop it.
Exercise 56
Why is a commercial power reactor not a nuclear bomb? Distinguish an explosive nuclear-weapon chain reaction from steam or chemical explosions that can occur in a reactor accident.
14.11: Nuclear Weapons
Exercise 57
An event releases of nuclear energy—an amount comparable to the electrical energy used throughout the city of Alameda in the San Francisco Bay Area in about two weeks. Using and , find the corresponding decrease in rest mass in grams.
Exercise 58
The measured activity of a radioactive contaminant at a particular site can fall faster than radioactive decay alone predicts. Give two physical processes that could cause this. Does a fall in activity at that site necessarily mean the radioactive nuclei have decayed?
14.12: The Four Basic Forces
Exercise 59
Identify the interaction chiefly responsible for each: (a) Earth’s orbit around the Sun, (b) the attraction between an electron and a nucleus, (c) binding protons and neutrons into a nucleus, and (d) beta decay. Which of these interactions have a short range at nuclear or subnuclear scales?
14.13: Particles, Patterns, and Conservation Laws
Exercise 60
An antihydrogen atom contains an antiproton and a positron. How could annihilation when it encounters ordinary matter help distinguish antihydrogen from hydrogen? If its positron annihilates with an electron, with both initially approximately at rest, two photons are emitted. Explain why the photons have equal energies and calculate the energy of each in MeV. Use .
Exercise 61
What lifetime do you expect for an antineutron isolated from normal matter?
Exercise 62
In , check electric charge, electron-family number, and muon-family number. Use +1 for a lepton in its family, −1 for its antiparticle, and zero for particles outside that family.
Exercise 63
Early solar-neutrino experiments detected fewer electron neutrinos than solar models predicted. Explain how neutrino flavor change resolves this discrepancy. Why was a measurement sensitive to all three active neutrino flavors an important test?
Exercise 64
In ordinary nuclear reactions without baryon–antibaryon production, how does baryon-number conservation account for conservation of the total number of nucleons? Why does this not require the total rest mass to remain unchanged?
Exercise 65
(a) Classify the electron, muon, electron neutrino, pion, kaon, proton, neutron, photon, and gluon as leptons, mesons, baryons, or gauge bosons. You may use the particle table.
(b) Which categories in this list contain hadrons?
(c) Describe the valence-quark content of an ordinary meson and an ordinary baryon. Why does mass alone not determine these categories?
Exercise 66
Using the particle table and the quark model, classify each of these as a lepton, meson, baryon, or gauge boson: electron, tau, muon neutrino, pion, kaon, proton, neutron, photon, and gluon. Which of these are composite particles? Explain why “heavier particle” is not a reliable definition of baryon.
Exercise 67
Measurements of beta decay showed that the daughter nucleus and emitted electron did not account for all the initial energy and momentum. Explain how an additional, electrically neutral particle could account for these observations. Why was the missing energy and momentum evidence for such a particle, but not by itself conclusive proof of its existence?
14.14: GUTs: The Unification of Forces
Exercise 68
Which interactions are described by the Standard Model? Which is left out? How does a proposed grand unified theory differ from the already established electroweak theory?
Exercise 69
Does the discovery of the Higgs boson mean that it replaces the W and Z bosons as the carrier of the weak interaction? Explain your response.
Exercise 70
If a deeper theory successfully unifies all four forces, it will still be correct to say that the orbit of the moon is determined by the gravitational force. Explain why.
Source sections: Nuclear Radioactivity, Radiation Detection and Detectors, Substructure of the Nucleus, Nuclear Decay and Conservation Laws, Half-Life and Activity, Medical Imaging and Diagnostics, Biological Effects of Ionizing Radiation, Fusion, Fission, Nuclear Weapons, The Four Basic Forces, Particles, Patterns, and Conservation Laws, GUTs: The Unification of Forces. Credits and licenses appear with each source section.