• UNIT 4:ATOMIC NUCLEI AND RADIOACTIVE DECAY

    Fig.4. 1: Sign of radiation precaution

    Key unit competence: Analyse atomic nuclei and radioactivity decay
    My goals
    • Define atomic mass and atomic number
    • Identify the constituents of a nucleus
    • Explain Einstein’s mass-energy relation.
    • Define nuclear fusion and fission.
    • Analyze determinations of a mass of nuclei by using Bainbridge mass
    spectrometer.
    • Derive the relationship between decay constant and half-life.
    • Determine the stability of a nuclei.
    • Describe properties of different radiations.
    • Describe creation of artificial isotopes.
    • Identify the application of radioactivity in life.
    • Plot a graph of binding energy against nucleon and explain its features.
    • Calculate the decay rate of unstable isotopes.
    • Appreciate the safety precautions to be taken when handling radioactive
    materials.
    • Appreciate that the nucleus of an atom and quantum system has discrete

    energy levels.

    INTRODUCTORY ACTIVITY


    In different places like industries, hospitals, and other sensitive places, there
    are different posts that caution someone about dangerous substances one
    may encounter if care is not taken. Among the reasons why these places bare
    such instruction is because of chemicals and radiations that are used in such
    places which may be harmful if not handled with care.
    1. Discuss some of the safety signs you have ever seen in any hospitals or
    industry if you have ever visited one.
    2. Why do you think there is a need to put those signs in such places?
    3. It is believed that there are some of diseases that are treated using
    radioactive substances. Can you state some of the radiations used to
    treat some diseases.
    4. There are natural men made radioactive substances. All of these are
    used for different purposes. What are some of negative effects of these
    radiations to (i) man , (ii) environment
    5. Some countries like Iran are affected by these radiations. Imagine you
    were a resident of that country, what would you do to protect yourself

    from such effects of radioactive substances.

    4.1 ATOMIC NUCLEI-NUCLIDE
    4.1.1 Standard representation of the atomic nucleus

    ACTIVITY 4.1: Investigating the stable and unstable nicleus


    Fig.4. 2 The standard representation of an atom nucleus
    Observe the Fig.4.1 above of an atom and answer to the questions that
    follow:
    1. What do numbers A and Z stand for?
    2. Describe the relation between the two numbers and their meanings.
    3. When do we say that an atom is stable or unstable?
    4. Explain clearly the meaning of isotopes. Give an example of isotopes

    you know.

    A nucleus is composed of two types of particles: protons and neutrons. The
    only exception is the ordinary hydrogen nucleus, which is a single proton. We
    describe the atomic nucleus by the number of protons and neutrons it contains,
    using the following quantities:
    a. The atomic number or the number of protons Z in the nucleus (sometimes
    called the charge number).
    b. The neutron number or the number of neutrons N in the nucleus.
    c. The mass number or the number of nucleons in the nucleus,
                                          A = Z + N.                         (4.01)
    In representing nuclei, it is convenient to use the symbol AZ
    to show how many
    protons and neutrons are present in the nucleus. X represents the chemical
    symbol of the element. For example, 5626 Fe nucleus has mass number 56 and
    atomic number 26. It therefore, contains 26 protons and 30 neutrons.
    When no confusion is likely to arise, we omit the subscript Z because the
    chemical symbol can always be used to determine Z. Therefore, 5626 Fe is the same
    as 56 Fe and can also be expressed as “iron-56.” Each type of atom that contains

    a unique combination of protons and neutrons is called nuclide.

    4.1.2 Classification
    Depending on the combinations of protons and neutrons in the nucleus,
    nuclides can be classified in the following 3 categories:
    a. Isotopes: These are nuclei of a particular element that contain the same
    number of protons but different numbers of neutrons. Most elements
    have a few stable isotopes and several unstable, radioactive isotopes.

    Example of isotopes:

    Therefore, the chemical properties of different isotopes of an element are
    identical but they will often have great differences in nuclear stability. For
    stable isotopes of light elements, the number of protons will be almost equal to
    the number of neutrons. Physical properties of different isotopes of the same
    element are different and therefore they cannot be separated by chemical
    methods i.e. only physics methods such as the centrifugation method can be
    used to separate different isotopes of an element.
    b. Isobars: these are nuclei which have the same mass number but different

    number of protons Z or neutrons N.

    c. Isotones: these are nuclei in which the number of neutrons is the same

    but the mass number A and the atomic number Z differ

    4.1.3 Units and dimensions in nuclear physics
    The standard SI units used to measure length, mass, energy etc. are too large
    to use conveniently on an atomic scale. Instead appropriate units are chosen.
    • The length: The unit of length in nuclear physics is the femtometer.
    1 fm =10−15 m
    This unit is called Fermi in the honor of the Italian Americano physicists who

    did a lot of pioneering work in nuclear physics.

    • The mass: The unit used to measure the mass of an atom is called the
    atomic mass unit, abbreviated “amu or u” and is defined as a1⁄12 the
    mass of an atom of carbon-12. Since mass in grams of one carbon-12

    atom is its atomic mass (12) divided by Avogadro’s number gives.

    • Nuclear masses can be specified in unified atomic mass units (u).
    On this scale:
    • A neutral 126 C atom is given the exact value 12.000000 u.
    • A neutron then has a measured mass of 1.008665 u,
    • A proton 1.007276 u,
    • A neutral hydrogen 11H
     atom (proton plus electron) 1.007825 u
    Energy: the SI unit used for energy that is Joule is too large. In nuclear physics
    the appropriate unit used for energy is an electronvolt (eV). An electron volt
    (eV) isdefined as the energy transferred to a free electron when it is accelerated
    trough a potential difference of one volt. This means that
    1eV =1.6022×10−19 C×1V =1.6022×10−19 J
    It is also a common practice in nuclear physics to quote the rest mass energy
    calculated using ,
                                                      E = mc2                                                                        (4.02)
    Since the mass of a proton is mp =1.67262  ×10 −27kg =1.007276 u, then 1 u is equal to

    This is equivalent to energy in MeV of   

    • The time: the time involved in nuclear phenomena is of the order of
    10-20s to million or billion years.
    • Nuclear radius: various types of scattering experiments suggest that
    nuclei are roughly spherical and appear to have the same density. The

    data are summarized in the expression called Fermi model.

    Where r0  =12 fm  =1.2 × 10−15 m  and A is the mass number of the nucleus
    The assumption of a constant density leads to the estimate of the mass density

    which is obtained by considering.

    This high density can explain why ordinary particles cannot go through the
    nucleus as highlighted by Rutherford experiments. The same density was only
    observed in neutron stars. The nuclear mass can be determined using a mass
    spectrometer.
    4.1.4 Working principle a mass spectrometer
    The figure below highlights the working principle of a typical mass spectrometer
    used to separate charges of different masses. It can be used to differentiate

    isotopes of a certain element.

    Fig.4. 3: Bainbridge mass spectrometer

    Ions are formed in ionization chamber and accelerated towards the cathode.
    The beam passes through the cathode and is focused by the collimating slits S1
    and S2. The beam is then passed through a velocity selector in which electric
    and magnetic fields are applied perpendicular to each other. The ion moves in
    straight line path for which both the forces acting on it are equal
                                 qE = qvB
    The velocity of ion which passes un-deflected through the velocity selector is

    then given by   

    The ions then reach the vacuum chamber where they are affected by the
    magnetic field  alone and then move in circular paths; the lighter ions
    having the larger path radius. If the mass of an ion is m, its charge q and its

    velocity v then

    The radius of the path in the deflection chamber is directly proportional to the
    mass of the ion. The detection is done by photographic plate when the ions fall
    on it. The fig. 4.5 shows the recorded mass spectrum for a gas containing three
    isotopes. Note the wider line for the mass m1, showing its relatively greater

    abundance.

    4.1.5 Checking my progress



    4.2 MASS DEFECT AND BINDING ENERGY
    4.2.1 Mass defect
    ACTIVITY 5.2: Select the words in the following puzzle
    Observe the puzzle below:
    1. Discover 8 different words related to particle Physics hidden in the
    puzzle below, and write them in your notebook.

    2. Use them to formulate a meaningful sentence


    3. Complete the sentences below using the words you discovered in
    the puzzle
    a. An …….is the SI unit of energy
    c. The ………..of nucleons is greater than the mass of a nucleus.
    d. The atom releases ………when its nucleus is formed from its
    constituent particles
    e. The binding energy per nucleon gives an indication of the …………
    of the nucleus.
    f. The surprising suggestion that energy and mass are equivalent
    was made by ……in 1905.
    4. Discuss and explain the meaning of the following expression as used in
    physics
    a. Mass defect c. Electronvolt

    b. Biding energy d. Stable nuclides

    The nucleus is composed of protons that are positively charged and neutrons
    that are neutral. The question is what is holding these particles together in
    this tiny space?
    Experiences have demonstrated that the mass of a nucleus as a whole is always
    less than the sum of the individual masses of protons and neutrons composing
    that nucleus.
    The difference between the two measurements is called mass defect Δm . For a

    nucleus  

    4.2.2 Einstein mass-energy relation
    In 1905, while developing his special theory of relativity, Einstein made the
    surprising suggestion that energy and mass are equivalent. He predicted that if
    the energy of a body changes by an amount of energy E, its mass changes by an
    amount m given by the equation
                                                    E = mc2                                                                                  (4.09)
    Where c is the speed of light and m mass of a body
    Everyday examples of energy gain are much too small to produce detectable
    changes of mass.
    4.2.3 Binding energy
    The mass of a nucleus is less than the combined mass of its protons and
    neutrons (nucleons). The missing mass is called the mass defect. This observed
    mass defect represent a certain amount of energy in the nucleus known as the
    binding energy b E and calculated using the Einstein formula as:
                                                    ΔE = Δmc                                        (4.10)
    where c is the speed of light and Δm the mass defect.

    The binding energy for a nucleus containing Z protons and N neutrons is defined as

    The binding energy is the energy released when a nucleus is formed from its
    constituent particles or the energy required to break up (to split) the nucleus
    into protons and neutrons. Protons and electrons are held together in the
    nucleus of an atom by the strong nuclear force. So if we imagine splitting a
    nucleus up into its separate protons and neutrons, it would require energy,
    because we would need to overcome the strong nuclear force.
    4.2.4 Binding energy per nucleon and stability
    Instead of looking at the total binding energy of a nucleus, it is often more useful
    to consider the binding energy per nucleon. This is the total biding energy

    divided by the total number of nucleons.

    A plot of binding energy per nucleon Eb/A as a function of mass number A for

    various stable nuclei is shown on Fig. 5.6.

    Fig.4. 5: The graph of binding energy per nucleon of the known elements (Giancoli D. C., 2005)

    The nuclear binding energy per nucleon for light element increases with the
    mass number until a certain maximum is reached at around A = 56 and then
    after it almost saturate. The fact that there is a peak in the binding energy per
    nucleon curve means that either the breaking of heavier nucleus (fission) or
    the combination of lighter nuclei (fusion) will yield the product nuclei with
    greater binding energy per nucleon and therefore more stable.
    As an example if a nucleus like is 23892U split into two fragments of nearly equal
    masses, the two fragments will have higher binding energy per nucleon than
    the original. The excess energy is released as useful energy and this process
    called fission is the basis of electricity production in a nucleus plant.
    If two light elements combine their nuclei in one nucleus, the formed nucleus

    will have a greater binding energy per nucleon than the originals.


    This process is called nuclear fusion and can only take place at a very high
    temperature. It is the source of energy in the sun and other stars. The fusion is
    more energetic than the fission.
    The binding energy per nucleon therefore gives an indication of the stability
    of the nucleus. A high binding energy per nucleon indicates a high degree of

    stability – it would require a lot of energy to take these nucleons apart.

    4.2.5 Checking my Progress


    4.3 RADIOACTIVITY AND NUCLEAR STABILITY
    ACTIVITY 4.3: Investigating radioactivity
    During the World War II, its final stage was marked by the atomic bombing
    on Nagasaki and Hiroshima towns in Japan (Fig.5.6). Observe the image and

    read the text provided below before answering the following questions.


    Fig.4. 6: The atomic bomb in Nagasaki (Japan in 1945)

    In August 1945, after four years of world war, united States B-29 bomber,
    dropped the atomic bomb over the cities of Hiroshima on August 6th 1945.
    70.000 people died in 9 seconds, and the city of Hiroshima was leveled. 3 days
    after as second bomb was dropped in Nagasaki, Japan with the same devastating
    results. The bombing killed over 129.000 people.
    The bomb released cataclysmic load of energy. The ones who were close enough
    to see the blast lost their eyes. It was the last thing they ever saw. The bright
    light of what the blinded them. The black of their eyes, the retina, melted away.
    The radiation received by the body is equivalent today’s thousands of x-rays.
    The human body can’t absorb unlimited radiation. It falls apart because the
    cells are dying of radiation poisoning, if the radiation is intense enough, it looks
    like a urn. Layers of the skin begin to fall off. The body vital functioning began
    to slow down until it stops.
    1. Describe and discuss the phenomena happening on two images.
    2. From the text, show that the atomic bomb of Hiroshima was very harmful
    to human body.
    3. What are the types of radiations should be there?
    4. Stable isotopes do not emit radiations. What is the name of materials which
    emit radiations? Describe them.
    5. What are the possible main radioisotopes used to produce energy in figure
    above?
    6. Which processes are used to generate such heavy energy? Describe any one
    of your choice
    Radioactivity is one of the dynamic properties of nuclei, in this process the
    system makes a transition from a high energy state to a low energy by emitting
    α and β-particles or γ-rays. This process happens naturally and is not affected by
    any external agent such as pressure, temperature or electric and magnetic fields.
    The α-particles are Helium nuclei and can be stopped by a piece of paper while
    β-particles are either electron or positron. There are high energetic particles
    and can pass through one cm thick aluminum sheet. γ-rays are electromagnetic
    radiations and can be stopped by several inches of lead.
    4.3.1 Radioactive decay of a single parent
    Nucleus decay is a random process and the rate of disintegration is proportional
    to the number of available radioactive nuclides. Let us analyses the simple case
    where the first daughter nuclide is stable. Suppose that at time t, there are N
    radioactive nuclide and dN is the number of nuclide disintegrating within a
    time dt. As the rate of disintegration is proportional to the number of nuclides
    present in the radioactive substance, we get

    where λ, the proportionality constant, is called the radioactive constant.
    This constant depends on the nature of the radioactive substance. The negative
    sign shows that an increase in disintegration rate will decrease the number of
    radioactive nuclides which are present. From this we can establish the formula

    of radioactive decay:


    where it assumed that the initial number of radioactive nuclide is equal to N0.


    Fig.4. 7: Illustration of the radioactive decay law

    If we consider the activity A of a radioactive sample which is the number of
    decay events in a unit time we obtain a similar expression for the radioactive

    decay law but expressed in terms of activity of the radioactive substance:


    where A0 is the initial activity of the radioactive source. Another parameter
    useful in characterizing nuclear decay is the half-life T1⁄2 .
    The half-life of a radioactive substance is the time interval during which half

    of a given number of radioactive nuclei decay. Therefore the half time period is


    Finally,one shows that the mean-life of a nuclide or the average life period of a

    nuclide is related to the radioactive constant by


    In general, after n half-lives, the number of un-decayed radioactive nuclei

    remaining is 



    4.3.2 Characteristics of radioactive substances
    Radioactive substances (nuclides) present one or more of the following features
    • The atom of radioactive elements are continually decaying into simpler
    atoms as a result of emitting radiation
    • The radiations from radioactive elements produce bright flashes of
    light when they strike certain compounds. The compound fluoresce.
    For example, rays from radium cause zinc sulphide to give off light in
    the dark. For this reason, a mixture of radium and zinc sulphide is used
    to make luminous paints.
    • They cause ionization of air molecules. The radiations from radioactive
    substances knock out electrons from molecules of air. This leaves the
    gas molecules with a positive charge.
    • Radiations from radioactive substances can penetrate the heavy black
    wrapping around a photographic film. When the film is developed, it
    appears black where the radiations struck the film.
    • Radiations from radioactive substances can destroy the germinating
    power of plants seeds, kill bacteria or burn or kill animals and plants.
    Radiations can also kill cancers.
    A. Properties of emitted radiations

    Some of their properties are summarized and shown in the table below:


    Table 4. 3 Properties of different types of radiations

    a. Alpha decay ( 42He )
    If one element changes into another by alpha decay, the process is called
    transmutation. For alpha emission to occur, the mass of the parent must be
    greater than the combined mass of the daughter and the alpha particle.
    In the decay process, this excess of mass is converted into energy of other forms
    and appears in the form of kinetic energy of both the daughter nucleus and
    the alpha particle. Most of kinetic energy is carried away by the alpha particle
    because it is much less massive than the daughter nucleus. The momentum is
    conserved in this process.
    The isotope whose natural radioactive decay involves the emission of alpha
    particles usually have a relative atomic mass greater than 210 (Ar>210). They
    have too much mass to be stable and give out alpha particles to form smaller

    and more stable atoms.

    b. Beta decay
    The isotopes whose radioactive decay involves the emission of beta particles
    often have a relative atomic mass less than 210 (Ar < 210). Beta particles are
    usually emitted from heavier nuclei that have too many neutrons compared
    with the number of protons.
    I. Negative β-decay

    In this process of negative β-decay an electron and an antineutrino are emitted.

    The emitted electron results from the following reaction where a neutron
    changes into a proton and an electron is emitted from the nucleus as a beta

    particle:

    The conservation of charges and mass number is maintained. The daughter

    nuclide may be in an excited state and will become stable after emitting a γ-ray.

    II. Positive β-decay

    In this process the positron and the neutrino are emitted.

    This positive decay is different from an electron capture which takes place
    when an electron that is close to the nucleus recombines with a proton in the

    nucleus producing a neutron and a neutrino:

    The equation of decay of the electron capture is:

    The daughter nuclide is seem to be the same as that we could have been
    produced if a positron has been emitted. The rearrangement of the remaining
    Z-1electrons will lead to emission of characteristic x-ray of the daughter
    nucleus. In few case both positron and electron capture may happen.
    C. Gamma decay (Y)
    Very often a nucleus that undergoes radioactive decay is left in an excited
    energy state. The nucleus can then undergo a second decay to a lower energy
    state by emitting one or more photons. Unlike α and β decay, γ decay results
    in the production of photons that have zero mass and no electric charge. The
    photons, emitted in such process, are called gamma rays and they have very
    high energy.
    If an atom of a material Y emits a γ ray (γ photon), then the nuclear reaction can

    be represented symbolically as  

    Gamma emission does not result in any change in either Z or A.
    Notes:
    • A transmutation does not occur in gamma decay. When an alpha
    particles and beta particles are emitted, gamma rays are often emitted
    at the same time. When a radioisotope emits gamma rays, it become
    more stable because it loses energy.
    • In both alpha and beta decay, the new element formed is called the

    daughter isotope.

    • Gamma rays are like X-rays. Typical gamma rays are of a higher
    frequency and thus higher energy than X-rays.
    • Deviations of alpha, beta and gamma radiations due to electric field and
    magnetic field ( See Fig.4.9). It can be seen unlike gamma-rays, alpha
    and -particles are affected by the presence of electric and magnetic
    fields since these particles are charged. Gamma-rays are not affected

    by these fields.


    Fig.4. 8: Deviation of radiation particles in an electric field

    4.3.3 Nuclear fission and Fusion
    a. Nuclear fission
    Heavy unstable nuclides can be broken up to produce energy in a process
    called nuclear fission. When uranium decays naturally, alpha and beta particles
    are emitted. However, when uranium-235 is bombarded by neutrons it forms
    uranium-236. Uranium-236 is unstable and breaks down, splitting into two
    large particles and emitting three neutrons. The fission of 235U by thermal

    neutrons can be represented by the reaction


    where 236U∗ is an intermediate excited state that lasts for approximately10-12s
    before splitting into medium-mass nuclei X and Y, and these are called fission

    fragments.

    Fig.4. 9: Fission diagram illustration

    When the exact masses of the final products are added together, the sum is
    found to be appreciably less than the exact masses of the uranium-235 and the
    original neutron. This difference in mass Δm appears as energy given by
    Δm = Δmc2
    Another important point arises! The three neutrons released may collide with
    other nuclides and split them also resulting in cascade reactions. In this way,
    chain reactions occur and as a result, the quantity of energy released can be
    very large. A few kilogram of uranium can produce as much heat energy as
    thousands of tons of coal.
    Advantages and disadvantages of nuclear fission
    The nuclear fission produces a huge amount of energy. This energy can
    be released in a controlled manner in nuclear power station and be used in
    driving steam turbines that produce electric power. However, when produced
    in uncontrolled manner it will result in the fabrication of atomic bomb that may
    release a large amount of heat energy and damaging radiations. The emitted
    radiations have both short term and long term effect on the living things.
    b. Nuclear fusion
    When lighter nuclides merge together in a process called fusion, energy is

    produced and mass is lost. For example: 


    These reactions occur in the core of a star and are responsible for the outpouring
    of energy from the star.
    The sum of the exact masses of the helium atom is less than the sum of exact
    masses of the four hydrogen atoms. This lost mass is released as energy. It is
    thought that the sun’s energy is produced by nuclear fusion.
    4.3.4 Radiation detectors
    ACTIVITY 4.4: Smoke detector bellow
    Observe the diagram of a smoke detector bellow then answer to the

    questions that follow:

    Fig.4. 10: illustration diagram of a smoke detector

    1. Name the components labeled A, B, C and D on the smoke detector
    above?
    2. What is meant by smoke detector?
    3. Describe a functioning of a smoke detector.
    4. Design an inventory of other radiation detectors you know
    Experiments in Nuclear and Particle Physics depend upon the detection of
    primary radiation/particle and that of the product particles if any. The detection
    is made possible by the interaction of nuclear radiation with atomic electrons
    directly or indirectly.
    a. Classification of radiation detectors
    There are a variety of other radioactive detectors that we may conveniently

    classify into two classes: Electrical and Optical detectors.



    Table4. 1 Classification of radiation detectors

    b. Working principle of an ionization chamber
    Conventionally, the term “ionization chamber” is used exclusively to describe
    those detectors which collect all the charges created by direct ionization within
    the gas through the application of an electric field. Ionization chamber is filled
    with inert gases at low pressure. In the chamber there are two electrodes,
    namely, the cathode and the anode which are maintained at a high potential

    difference as shown on the figure below


    Fig,4.11: visualization of ion chamber operation

    When radiation enters the chamber, it ionizes the gas atoms creating negative
    and positive charges. The negative charges or electrons are attracted by the
    anode while positive ions are attracted by the cathode; this produces the current
    in the outside circuit depending on the strength and the type of radiation. The
    current produced is quite small and dc amplified electrometers are used to

    measure such small currents.

    4.3.5 Checking my progress
    In the following exercises (1 to 4), choose the best answer and explain your
    choice
    1. Which of the following is an electron?
    a. Neutrino c. Photon
    b. Gamma particle d. Beta particle
    2..Which of the following most accurately describe radioactive decay?
    a. Molecules spontaneously break apart to produce energy
    b. Atoms spontaneously break apart to produce energy beta decay, alpha
    decay and positron emission are all forms of radioactive decay. Energy is
    released because the atoms are converted to a more stable energy
    c. Protons and neutrons spontaneously break apart to produce energy
    d. Electrons spontaneously break apart to produce energy
    3. Which of the following is true concerning the ratio neutrons to protons in
    stable atoms?
    a. The ratio for all stable atoms is 1:1.
    b. The ratio for small stable atoms is 1:1, and the ratio for large stable atom is
    greater than 1:1. As atomic weight goes up, the ratio of neutrons to protons
    for stable atoms increases up to as much as 1.8:1 ratio.
    c. The ratio for large stable atom is 1:1, and the ratio for small stable atoms
    is greater than 1:1.
    d. There is no correlation between the stability of the atom and its neutron
    to proton ratio.
    4. Polonium-218 undergoes one alpha decay and two beta decays to make
    a. Polonium-214 c. Bismuth-214
    b. Plomb-214 d. Plomb-210
    5. a) Compare (i) the charge possessed by alpha, beta and gamma radiations
    (ii) The penetrating power of these radiations
    6. a.What is meant by the term (i) radioactive decay? (ii) Half-life of a radioactive
    substance?
    b. A 32 g sample of radioactive material was reduced to 2 g in 96 days. What is its
    half-life? How much of it will remain after another 96 days?
    7. 212Be Decays to 208Th by α-emission in 34% of the disintegration and to212Ra
    by β-emission in 66% of the disintegration. If the total half value period is 60.5
    minutes, find the decay constants for alpha and beta and the total emission.
    8. If a radioactive material initially contains 3.0milligrams of Uranium234U , how
    much it will contain after 150,000 years? What will be its activity at the end of

    this time?

    4.4 APPLICATION OF RADIOACTIVITY

    ACTIVITY 5.5: Use of nuclear energy to generate electricity


    Fig.4. 12: Nuclear power plant functioning mechanism diagram.

    Many people disagree to the use of nuclear power to generate our
    electricity, even though the safety record of nuclear industry is extremely
    good. Observe clearly the image diagram of the nuclear power plant
    (Fig.4.12) and answer to the questions that follow
    1. Why do you think people disagree to the use of nuclear power
    station?
    2. What are the main parts of the power plant station observed in
    Fig.5.12?
    3. Analyze and explain the steps of energy transformation from reactor
    to generator
    4. Write a brief explanation on the advantages and disadvantages of
    using nuclear energy as a source of electricity if any.
    5. Use internet and your library or any other resources to find out
    about the other application of radionuclides in our daily life
    People would not have fear of radiations when controlled in certain manner.
    Radioisotopes and nuclear power process have been used and produced
    improvement in various sectors. These includes: consumer products, food and
    agriculture, industry, medicine and scientific research, transport, water
    resources and the environment. The following are some descriptive examples
    among others.
    4.4.1 Industry
    Different materials we use at home are manufactured in industry and made of
    different radioactive materials. The dosage of use of radioactive substance is
    thus controlled so that they are not harmful to human body.
    Gamma radiation and beta radiation from radio-isotopes can be used to
    monitor the level of the material inside the container. The penetrating power
    of gamma rays is used to detect hidden flow in metal castings. Beta rays are
    used to measure the thickness of various flat objects (the mass absorbed by the
    object is proportional to its thickness).
    In the textile industries, irradiation with beta radiations fixes various chemicals
    onto cotton fibers. This produces for instance permanent press clothing. Again,
    radioactive materials can be used as tracers to investigate the flow of liquids in

    chemical factories.

    Fig.4. 13 Testing the level of a liquid in a container using radiations

    If there is a sudden decrease in the amount of radiation reaching the detector,
    which will happen when the container is full, then this can be used as a signal
    to switch off the flow of substance into the container. A similar method is used
    to monitor the thickness of sheets of plastic, metal and paper in production.
    4.4.2 Tracer studies
    Tracer techniques can be used to track where substances go to and where leaks
    may have occurred. Leaks in gas pipes or oil pipes can be detected by using this
    technique. Tracer techniques are also used in medicine to treat thyroid glands
    which can be underactive or over active. The activity of the thyroid gland can
    be monitored by the patient being injected with or asked to drink radioactive
    iodine. The radioactivity in the vicinity of the thyroid gland is then checked to
    see how much of the radioactive iodine has settled in the area around the gland.
    4.4.3 Nuclear power stations
    Nuclear power stations control a large amounts of energy released when
    Uranium-235undergoes nuclear fission. The energy released by this controlled
    chain reaction, is then used to produce electricity.
    4.4.4 Nuclear fusion
    In nuclear fusion, the nuclei of elements with a very low atomic number are fused
    together to make heavier elements. When this takes place, it is accompanied by
    a very large release of energy. In the sun, hydrogen nuclei are fusing together
    all the time to make helium nuclei. This is also the process by which a hydrogen
    bomb works.
    4.4.5 Medicine
    ACTIVITY 4.6: Radionuclides in Medicine

    Observe the figure below and suggest answers to the question below

    Fig.4. 14: A gamma camera assembly. The photons emitted in the patients are detected
    by the photomultiplier tubes. A computer monitor displays the image computed from

    the photomultiplier signals.

    1. Who is this person (a man or a woman)?
    2. Where is he?
    3. What does the image on the right represent?
    4. What do you think the patient is suffering from?
    5. Using the knowledge acquired in optics, what kind of light
    propagation observed there?
    6. Does the imaging use reflection or refraction? Why?

    7. What should be the name of radiation being used in this imaging?

    Nuclear medicine has revolved treatment of different disease of the century. It
    consists on the use of nuclear properties of radioactive substances in diagnosis,
    therapy and research to evaluate metabolic, physiologic and pathologic
    conditions of human body. Today, nuclear medicine is currently used in the
    diagnosis, treatment and prevention of many serious sicknesses.
    Cancer cells are more easily killed by radiation than healthy cells. In medicine,
    penetrating gamma rays of cobalt-60 sources are used for this purpose. Other
    cancers such as skin cancers are treated by less penetrating beta radiation from
    strontium-90 source. Surgical instruments can also be sterilized using gamma
    radiation.
    4.4.6 Food preservation
    The preservation of food uses gamma rays is spreading worldwide. Treating
    food with gamma rays can:
    • Slow down the ripening of some fruits and the sprouting of potatoes.
    In both cases, this helps storage and increases the half-life of the food.
    • Kill highly dangerous micro-organisms such as salmonella
    • Kill micro-organisms that spoil food
    4.4.7 Radiocarbon dating
    There are three isotopes of carbon: carbon-12, carbon-13 and carbon-14. The
    isotope carbon-14 is radioactive and has half-life of 5760 years. To estimate
    the age of a biological sample, radiocarbon146C is used as a radioactive
    nuclide. Nucleus decay is independent of the physical or chemical condition
    imposed on the elements. This can be used to measure the ages of biological
    samples by considering the ratio of 146Cwhich is radioactive and 126C in dead
    species. Radioactive carbon is produced when cosmic rays interact with

    air atoms to produce neutrons and these neutrons interact with nitrogen

    The half-life period of 146Cis equal to 5760 years. The carbon reacts with oxygen
    to produce CO2 and plants combine this CO2 with water in the process of
    photosynthesis to manufacture their food. Therefore plants and animals are
    radioactive. When plants or animals die, the 146Cin them keeps on decaying
    without any new intake. The ratio of 146C and 126C will therefore be different in
    dead and leaving plants and animals. The age of the dead plant or animal can be

    estimated by measuring this ratio.

    4.4.8 Agricultural uses
    In agriculture, radionuclides are used as tracers for studying plants, insect
    and animals. For example, phosphorus-32 can be added to plant fertilizer.
    Phosphorus is absorbed by plants and its distribution can be measured.
    Radiation has been used in South American to detect and control the screw
    worm fly pest. A large number of the male of the species were exposed to
    gamma radiation. When the males were released back into the wild and mated
    with wild females, sterile eggs resulted and no new flies were born.
    The points of photosynthesis in a leaf are revealed by growing it in air containing
    carbon-14. The presence of this radioactive nuclide in the leaf is the revealed
    by putting the leaf onto a photographic plate and letting it take its own picture.

    4.4.9 Checking my progress

    1. Suggest different uses of radionuclides in (i) Medicine (ii) food and
    agriculture
    2. In our daily life, we are exposed to radiations of different types mainly
    in materials we use.
    a. Make an inventory of all of the devices in your home that may have
    (contain) a radioactive substance.
    b. What is the origin of these radiations in the materials highlighted
    above?
    c. Explain the purpose of radioactive material in the device.
    d. Then make research to find out how the objects shown in Fig.5.15 use

    radiation in their manufacture.


    Fig.4. 15

    4.5 HAZARDS AND SAFETY PRECAUTIONS OF WHEN
    HANDLING RADIATIONS

    ACTIVITY 4.7: Investigating the safety in a place with radiations


    Fig.4. 16: Radiation effects on human body according to the exposure.

    The image above (Fig.4.16) shows different side effects of radiation on
    human body according to the exposure time taken. With reference to
    section 4.3 and activity 4.3, answer to the following questions:
    1. What are the dangers of radiations you may observe?
    2. Analyze measures should be taken for radiation users?
    4.5.1 Dangers of radioactivity
    • Both beta particles and gamma rays can pass easily in the skin and can
    easily destroy or even kill cells, causing illness.
    • They can cause mutations in a cell’s DNA, which means that it cannot
    reproduce properly, which may lead to diseases such as cancer.
    • Alpha particles cannot pass through the skin. However, they are
    extremely dangerous when they get inside your body. This can happen
    if you inhale radioactive material.
    4.5.2 Safety precautions when Handling Radiations
    The precautions taken by workers who deal with radioactive materials are:
    • Wearing protective suits
    • Wearing radiation level badges
    • Checking the radiation level regularly
    • Using thick lead-walled containers for transporting radioactive
    materials
    • Using remote control equipment from behind thick glass or lead walls
    to handle radioactive material
    • They should be held with forceps and never touched with hands.
    • No eating, drinking or smoking where radioactive materials are in use
    • Wash your hands thoroughly after exposure of to any radioactive
    materials
    • Any cuts in the body should be covered before using radioactive sources
    • Arrange the source during experiments such that the radiation window
    points away from your body

    • There are ten golden rules for working safely with radioactivity.

    END UNIT ASSESSMENT 4
    A. Multiple choice questions
    Instructions: Write number 1 to 5 in your notebook. Beside each
    number, write the letter corresponding to the best choice
    1. Radionuclides
    a. Are those nuclides having more neutrons than protons
    b. May emit X-rays.
    c. Decay exponentially
    d. May be produced in a cyclotron
    2. Concerning Compton Effect:
    a. There is interaction between a photon and a free electron.
    b. The larger the angle through which the photon is scatted, the
    more energy it loses.
    c. The wavelength change produced depends upon the
    scattering material.
    d. High energy radiation is scatted more than lower energy
    radiations.
    e. The amount of scattering that occurs depends on the electron
    density of the scattering material.
    3. Classical physics offered a satisfactory explanation for
    a. The diffraction of electrons by crystals
    b. The deflection of charged particles in an electric field
    c. The intensity spectrum of black body radiation
    d. The photoelectric effect
    e. Matter waves
    4. When investigating β decay, the neutrino was postulated to explain
    a. Conservation of the number of nucleons
    b. Counteracting the ionizing effect of radiation
    c. Conservation of energy and momentum
    d. The production of antiparticles
    e. The energy to carry away the β particles.
    5. Gamma radiations differ from α and β emissions in that
    a. It consist in photons rather than particles having nonzero
    rest mass
    b. It has almost no penetrating ability
    c. Energy is not conserved in the nuclear decays producing it
    d. Momentum is not conserved in the nuclear decays producing it
    e. It is not produced in the nucleus
    6. The process represented by the nuclear equation is 
    a. Annihilation c. β decay e. γ decay
    b. α decay d. pair production
    7. Write number (i) to (iii) in your note book. Indicate beside each number
    whether the corresponding statement is true (T) or false (F). If it is false,
    write a corrected version.
    I. An alpha particle is also called a hydrogen nucleus
    II. The neutrino was suggested to resolve the problem of conserving
    energy and momentum in β decay.
    III. The amount of energy released in a particular α or β decay is found
    by determining the mass difference between the products and the
    parent. A mass-energy equivalence calculation then gives the energy.
    IV. The average biding energy per nucleon decreases with the increasing
    atomic mass number
    8. A radioactive source emits radiations alpha, beta and gamma a shown
    below:

    Fig.4. 17 Absorption of radiation
    The main radiation(s) in the beam at X and Y are

    9. The energy released by the nuclear bomb that destroyed Hiroshima was
    equivalent to 12.4 kilotons of TNT. This is equivalent to 9.1 × 1026 MeV.
    The mass that was Converted into energy in this explosion was (Convert

    MeV in Joules, use E=mc2)

    10. In the decay scheme (Conserve charge and electron lepton number) the

    blanks should contain

    11. Complete the following sentences by using a word, number and an
    equation where necessary

    a. The half-life in years of the decay represented by the graph in fig.4.18

    Fig.4. 18 Half life carve

    b. When an animal or plant dies, no more _______________is taken in and
    that which is present undergoes radioactive decay. If we measure the
    amount of carbon-14 left, it is possible to determine the________ of the
    sample.
    c. If an atom of material Y emits a gamma ray (gamma photon), then the

    nuclear reaction can be represented symbolically as_________________

    B. Structured questions
    12. Prepare a table summarizing the three types of radioactive emission.
    Classify each type under the following headings: Type of Emission,
    Mass, Charge, penetrating Power and Ionization Ability.
    13. Copy the following table in your notebook and answer the questions

    that follow

    14. Give the value of x and y in each of the following equations

    15. Give the value of x and y in each of the reaction classify each as α , β ,

    or γ decay

    16. The half-life of carbon14 is 5730 years the mass of certain sample of
    this isotope is800 μg . Graph the activity for the first 5 half-lives.
    17. Beams of a, b- and g radiation of approximately the same energy pass

    through electric and magnetic fields as shown below.

    a. Show the path taken by each particle in the two fields. Why do
    they follow these paths?
    b. Which particle is the most penetrating? Explain your answer.
    c. Which has the highest ionizing power?
    d. How are β + and electrons different?
    e. How are x-rays, y rays and photons different?
    18. We are exposed to radiation all the time, indoors and outdoors. This is
    called background radiation.
    a. Give two examples of sources of this background radiation.
    b. Which organ generally receives the most background radiation, and
    why?
    c. There is some concern at the moment that pilots and flight attendants
    may have significantly higher exposures to radiation than the normal
    exposure rates for the general public.
    d. Why do pilots have a higher exposure to radiation than most other
    people?
    19. Nuclei can decay by emitting particles which can change the energy, mass
    and charge of the nucleus.
    a. How is α decay possible when the α particle must pass an energy
    barrier which is greater than the energy of the particle? Describe the
    process involved.
    b. If isotope A emits α particles with greater energy than isotope B (of
    the same element), which will have the longer half-life?
    c. How can a nucleus change its charge without emitting a charged

    particle?

    C. Question of research
    21. Using the information in radioactivity and making an internet search
    or/ and using other sources of information, consolidate your skills in
    other hazardous materials you may meet in your area. Then complete

    the table below (not exhaustive):

    Table 4. 7 Precaution signs

    UNIT 3 FOSSIL AND NON-FOSSIL FUEL AND POWER PRODUCTIONUNIT 5 APPLICATIONS OF OPTICAL FIBER IN TELECOMMUNICATION SYSTEMS.