Energy that comes from a source and travels through matter or space
Two types of radiation:
Electromagnetic - Includes light, gamma rays, and X-rays
Particulate - Mass given off from unstable atoms with the energy of motion
Ionizing radiation
Radiation of either type that can produce charged particles in matter
Radioactivity
Radioactive decay
The spontaneous emission of electromagnetic or other types of radiation
Radioactive atoms
Unstable atoms that give off excess matter, energy, or both as ionizing radiation
Nucleons
General term used to describe nuclear particles, protons, and neutrons
Remember:
\(Z\) signifies the atomic number, the number of protons in the nucleus of an atom
\(N\) signifies the neutron number, the number of neutrons in the nucleus of an atom
Sum of \(N\) and \(Z\) is \(A\) (\(N+Z = A\)), the mass number
Nuclides
Remember, isotopes are:
Atoms with the same atomic number \(Z\), but different neutron numbers \(N\) and mass numbers \(A\)
Nuclides
Isotopes that exist for a measurable length of time and have a defined energy state
An atom of a particular atomic number, mass number and neutron number
Band of Stability
Of the more than 3,000 nuclides known, about 250 are stable
The rest decompose over a period of time, emitting radiation in the process of creating new nuclides
The stable nuclides have approximately equal numbers of protons and neutrons (\(N/Z\) ratio = 1) in the lighter elements (\(Z\) = 1 to 20) and more neutrons than protons in the heavier elements (\(N/Z\) ratio > 1).
Radiation
In a nuclear reaction, an emission of radiation usually accompanies changes in the composition of the nucleus.
Natural radiation associated with radioactive decay can be placed into three classes:
Alpha particles
Beta particles
Gamma rays
Properties of Types of Radiation
Type
Notation
Mass
Charge
Penetration into Al
Alpha
\(\chem{{}^4_2\alpha},\, \chem{{}^4_2He^{2+}}\)
4
2+
0.01 mm
Beta (electron)
\(\chem{{}_{-1}^0\beta^-}\)
~0
1-
0.5-1.0 mm
Beta (positron)
\(\chem{{}_1^0\beta^+}\)
~0
1+
(Reacts with electrons)
Gamma
\(\chem{\gamma}\)
0
0
50-110 mm
Types of Radiation
Alpha particles
Nuclei of helium-4 atoms
Contain 2 protons and 2 neutrons
Least harmful to animal and human tissue
Gamma rays
High energy electromagnetic radiation: energy without charge or mass
Highest energy and most penetrating type of radiation
Types of Radiation (cont.)
Beta particles
Small, charged particle that can be emitted from unstable atoms at speeds approaching the speed of light
Penetrate through skin into tissue
2 types of beta particles:
Positron - Same mass as an electron with an opposite charge
Electron
Nuclear Reactions
Two conditions must be met to balance a nuclear equation:
When a nucleus emits an alpha particle, it loses 2 protons and 2 neutrons, so its atomic number decreases by 2 and its mass number decreases by 4.
\[ \chem{{}^{232}_{90}Th \rightarrow {}^{228}_{88}Ra + {}^4_2\alpha} \]
Beta Particle (Electron) Emission
When a nucleus emits a beta particle (electron), its atomic number increases by 1 and its mass number remains unchanged.
\[ \chem{{}^{231}_{90}Th \rightarrow {}^{231}_{91}Pa + {}^0_{-1}\beta^-} \]
Beta Particle (Positron) Emission
When a nucleus emits a beta particle (positron), its atomic number decreases by 1 and its mass number remains unchanged.
\[ \chem{{}^{23}_{12}Mg \rightarrow {}^{23}_{11}Na + {}^0_{1}\beta^+} \]
Electron Capture
A proton and an electron combine to form a neutron. The mass number stays the same, but the atomic number decreases by 1.
Very few nuclides undergo this transformation.
\[ \chem{{}_4^7Be + {}^0_{-1}e^- \rightarrow {}_3^7Li} \]
Gamma Ray Emission
In all nuclear reactions, the nucleus changes from a state of higher energy to a state of lower energy.
Gamma rays are pure electromagnetic energy.
Results in no change in mass or atomic number.
\[ \chem{{}^{99m}Tc \rightarrow {}^{99}Tc + \gamma} \]
Nuclear Bombardment Reactions
Nuclei are hit with a beam of nuclei or nuclear particles to trigger a nuclear reaction
Occurs when a nuclear reaction is not spontaneous and is produced intentionally by artificial means
Used to synthesize transuranium elements, those following uranium on the periodic table
Particle accelerators are used for nuclear bombardment reactions.
The synchroton, perhaps the most successful accelerator, uses a circular path for the accelerating particles.
Sponeaneous Nuclear Decay Reactions
The tendency for the neutron/proton (\(N/Z\)) ratio to move toward the band of stability, explains the nuclear reactions of naturally radioactive nuclides.
For every process except \(\gamma\) emission, the change that occurs for an unstable nuclide takes it closer to the observed band of stability.
Radioactive nuclides convert spontaneously over time to form stable nuclides.
Nuclear Instability
Reason for Nuclear Instability
Radioactive Process
Emitted Radiation
Change in \(N/Z\) Ratio
Excess Mass
Alpha decay
\(\chem{{}^4_2\alpha}\)
Slight increase
\(N/Z\) too high
Beta decay
\(\chem{{}^0_{-1}\beta^-}\)
Decrease
\(N/Z\) too low
Positron emission
\(\chem{^0_1\beta^+}\)
Increase
\(N/Z\) too low
Electron capture
-
Increase
Energetically excited
Gamma emission
\(\chem{\gamma}\) ray
None
Radioactive Decay Series
In heavier elements, often the product of radioactive decay is itself radioactive.
In such cases, a series of alpha and beta decay steps ultimately leads to a stable nuclide.
Accounts for most of the radioactive decay among elements 83 through 92.
Rates of Radioactive Decay
Detecting Radiation
Various instruments have been developed to give speedier and more accurate measures of radiation intensity:
Geiger-Muller counter
Scintillation counter
Half-Life
The time required for half of a sample of a nuclide to decay to a different nuclide
It takes the same time for a fresh sample to decay to one-half the original number of atoms of that nuclide as it does one-half to decay to one-fourth and so on.
The shorter the half-life of a nuclide, the more intense the radiation that it emits.
Archeological Dating
Radio-carbon dating
Using carbon-14 to measure time on an archeological scale
As long as a plant or animal is alive, its carbon-14 content should match that in the atmosphere
After it dies, its carbon-14 content decreases through beta decay:
\[ \chem{{}^{14}_6C \rightarrow {}^{14}_7N + {}^0_{-1}\beta^-} \]
The half-life of the process is 5730 years.
Medical Applications of Isotopes
Many medical applications exists that use radioactivity:
Power generators
Example: \(\chem{{}^{238}Pu}\) is used to power pacemakers
Medical diagnoses
Radioactive nuclides are used as tracers to track movements of substances in chemical or biological systems
Example: \(\chem{{}^{99m}Tc}\) is used to help doctors locate tumors
Medical Applications
Positron Emission Topography
A PET scan detects abnormalities in living tissues without disrupting the tissue.
Medical Applications (cont.)
Cancer therapy
Radioactive nuclides, in much higher doses than those used for imaging, are used to treat cancerous tumors
Cancer cells absorb nutrients containing gamma-emitting components, the gamma radiation becomes concentrated in the cancerous cells, destroying them in greater numbers than normal cells.
Examples: \(\chem{{}^{131}I}\) destroys thyroid tumors, \(\chem{{}^{198}Au}\) used to treat lung cancer, \(\chem{{}^{32}P}\) used for eye tumors
Biological Effects of Radiation
Radiation can have one of four effects on the functioning of a cell:
The radiation can pass through the cell with no damage.
The cell can absorb the radiation and be damaged, but it can subsequently repair the damage and resume normal functioning.
The cell can be damaged so severely that it cannot repair itself. New cells formed from this cell will be abnormal. This mutant cell can ultimately cause cancer if it continues to proliferate.
The cell can be so severely damaged that it dies.
Biological Effects of Radiation - Radon
A rare noble gas which has also been implicated as a possible cause of lung cancer
Accumulates in houses from particular kinds of soils or rock strata
The Fear of Nuclear Energy...
Before and After...
Comparison
Nuclear Energy
Fission
Splitting of a heavy nucleus into two or more lighter nuclei and some number of neutrons
A reaction in which the product of one step is the reactant in another step
In order for a chain reaction to sustain itself, the amount and shape of the sample of fissionable material must be such that the neutrons will not escape due to energy that is higher than optimum for inducing further fission
A chain reaction should maintain a constant rate
Critical mass - The smallest amount of fissionable material necessary to support a continuing chain reaction
Fission Reactors
Nuclear power plants use fission to produce electric energy
If the chain reaction is going too quickly, movable control rods made of these elements are inserted into a core of uranium fuel in fission reactors
Fusion Reactions
Combination of light nuclei to form heavier nuclei
A major fusion reaction occurs continuously in the Sun and other stars:
\[ \chem{4{}^1_1H \rightarrow {}^4_2He + 2 {}^0_1\beta^+} \]
This process occurs in several steps:
\[ \chem{{}^1_1H + {}^1_1H \rightarrow {}^2_1H + {}^0_1\beta^+} \]
\[ \chem{{}^1_1H + {}^2_1H \rightarrow {}^3_2He} \]
\[ \chem{{}^1_1H + {}^3_2He \rightarrow {}^4_2He + {}^0_1\beta^+} \]
Fusion Reaction Terms
Ignition temperature - Temperature required to initiate a fusion reaction
Breeder reactors - A reactor that produces fuel that can be used in other reactors
Plasma
An ionized gas that must be created and controlled at temperatures of about \(10^8\, K\)
Melts most container material
Until recently, fusion in reactors required more energy than was given off
In order to achieve fusion, the gaseous reactants must be condensed to a small volume at high temperatures.