8 Nuclear Instability (Transmutation)

download 8 Nuclear Instability (Transmutation)

of 14

Transcript of 8 Nuclear Instability (Transmutation)

  • 7/28/2019 8 Nuclear Instability (Transmutation)

    1/14

    Nuclear Instability

    (Transmutation)

  • 7/28/2019 8 Nuclear Instability (Transmutation)

    2/14

    Contents

    Basic Radioactivity Inverse Square Law of Gamma Radiation

    Exponential Law of Decay

    Probing Matter

  • 7/28/2019 8 Nuclear Instability (Transmutation)

    3/14

    Basic RadioactivityRadiation is the decay of an unstable parent nucleus to a more

    stable daughter nucleus by emitting particles and/or energy

    Transmutation is the process in which the unstable nucleus decays to form

    another nucleus of a different atom. If this new nucleus is unstable, it willdecay again, and this is known as a decay chain.

    The decay chain be very long or very short. Some elements decay overthousands of years, some after microseconds.

  • 7/28/2019 8 Nuclear Instability (Transmutation)

    4/14

    Basic Radioactivity

    Isotopes of different elements may be radioactive. These

    radioactive versions are called radioisotopes.

    There are three types of radiation:

    Radiation Description Penetration Ionisation Effect of E or Bfield

    Alpha ()Helium nucleus

    2p + 2nQ = + 2 e

    Few cm airThin paper

    Intense, about 104ion pairs per mm.

    Slight deflection asa positive charge

    Beta ()

    High speed

    electronQ = -1 e

    Few mm of

    aluminium

    Less intense than

    a, about 102

    ionpairs per mm.

    Strong deflection

    in oppositedirection to a.

    Gamma ()Very short

    wavelength emradiation

    Several cm lead,couple of m of

    concrete

    Weak interactionabout 1 ion pair

    per mm.No effect.

  • 7/28/2019 8 Nuclear Instability (Transmutation)

    5/14

    Inverse Square Law of Gamma Radiation

    To measure the variation of gamma ray intensity with distance, the aboveexperiment is used.

    If Count Rate against 1/Distance2 isplotted, a straight line is achieved.

    The origin of the line is below zerodistance because the gamma source

    is deep within its housing.

    It is found that the counts per second, intensity, decreases with the square of thedistance, meaning if the distance is doubled, the intensity reduces by four times.

  • 7/28/2019 8 Nuclear Instability (Transmutation)

    6/14

    Inverse Square Law of Gamma RadiationThe inverse square relationship is therefore:

    Where: I intensity I0 intensity at the source k constant x the distance from the source

    Background Radiation must be measured and taken into account whenperforming radiation experiments. It comes in the following forms: Cosmic rays Radioactive material in the bricks of the building. Small amounts from medical and industrial uses. People (contain Carbon-14 amongst other radioisotopes)

    It is more common to calculate counts from two points, ifl0 is unknown:

    &

    When combined and rearranged gives:

  • 7/28/2019 8 Nuclear Instability (Transmutation)

    7/14

    Exponential Law of DecayRadioactive decay is entirely randomand unpredictable.

    Chemical reactions involve the outer shell of electrons, BUTradioactive decay involves the nucleus of an atom.

    The rate of decay of any nuclide at a given time is directlyproportional to the number of atoms left at that time:

    (The minus sign indicates that Ndecreases as time increases)

    (The d/dt gives the rate of change)

    Incorporating the radioactive decay constant, , into this

    equation gives:

    The radioactive decay constant is the fraction of the total number of nuclei present

    that decays per unit time, provided that the time interval is small

  • 7/28/2019 8 Nuclear Instability (Transmutation)

    8/14

    Exponential Law of DecayThe units ofis s-1 (per second), but often the Becquerel is used:

    1 Bq = 1 count per secondOver long time periods, the equation becomes:

    Where: N no of nuclei N0 original number of nuclei

    e exponential number

    - decay constant t time(s)

    This relationship is knownas exponential decay, andthe graph of this is shownhere

    The rate of decay is theactivity, measured inBecquerels, Bq

  • 7/28/2019 8 Nuclear Instability (Transmutation)

    9/14

    Exponential Law of DecayHalf-lifeDefined as the time taken for the activity of a sample to decreaseto half of some initial value So:

    After 1 half life Activity=50%After 2 half lives Activity=25%After 3 half lives Activity=12.5%

    etc...

    Half-life can be related to the decay constant:By definition:- and:-

    Therefore:-

    Half-life is useful for ascertaining methods of storing radioactive waste.

    The decay equations are useful for radioactive dating, using radioisotopes

    such as carbon-14, rubidium-87, and hydrogen-3

  • 7/28/2019 8 Nuclear Instability (Transmutation)

    10/14

    Probing MatterMethods of probing matter:

    Rutherford scattering(described in Particles, Radiation & Quantum Phenomena)

    Electron diffraction tube

    Electrons can be shown to have simple wave properties by using an electrondiffraction tube as shown above. A slice of carbon is placed in a beam of electronsso that the electrons diffract, producing diffraction ringswhich show their wave-like

    properties

  • 7/28/2019 8 Nuclear Instability (Transmutation)

    11/14

    Probing Matter X-Ray Diffraction

    A sample of the material isplaced in the beam of X-rays,and the resulting scatteringpattern is picked up on aphotographic plate. The X raysare diffracted in a cone. It is

    useful tool to discover thestructure of solid materials.

    Using a simple equation, the separation of layers of atoms can be determined:

    n = 2dsin

    where: norder of diffraction - de Broglie wavelength of the x-raysd the distance from source to screen- diffraction angle (cone angle for this case)

  • 7/28/2019 8 Nuclear Instability (Transmutation)

    12/14

    Probing Matter Nuclear Radius

    Rutherford estimated the radiusof a nucleus from his scatteringexperiments, and using CoulombsLaw, to be ~ 3.0x10-14 m

    The particle is repelled at point P.It has zero Kinetic Energy, as it isstationary; all its energy is potential.

    Using electrostatic potential energy equations, the distance can be calculated:

    Ep

    = potential at P charge of the alpha particle:

    Rearrange: Therefore: rc= 3.25x10-14 m

  • 7/28/2019 8 Nuclear Instability (Transmutation)

    13/14

    Probing Matter Electron Scattering

    Electrons interact with the nucleus by electromagnetic interaction unlike the alphaparticles which interact by strong nuclear interaction.

    A reasonable estimate can be obtained with a fairly simple equation:

    where:

    - de Broglie wavelength of the high-energy electrons

    - angle of diffractionR - nuclear radius

    This gives a result of the radius being: 2.65 10-15 m

    However, the radius depends on the nucleon number via a simple relationship:

    R= r0A1/3r0- a constant, value: 1.410

    -15 m

    A - nucleon number

    The graph represents thisrelationship between nuclear

    radius and nucleon number

    Nuclear radius is different toatomic radius.Atomic radius is similarwhether the element is light orheavy.Nuclear radius can vary

    largely, depending on element

  • 7/28/2019 8 Nuclear Instability (Transmutation)

    14/14

    Summary

    Basic Radioactivity Inverse Square Law of Gamma Radiation

    Exponential Law of Decay

    Probing Matter