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Matter

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Title: Matter


1
Matter Radiation 4Particles and antiparticles
  • Unit 1.1a4
  • Breithaupt chapter 1.4
  • pages 10 to 12

2
AS specification
  • Candidates should know that for every type of
    particle, there is a corresponding antiparticle.
    They should know that the positron, the
    antiproton, the antineutron and the antineutrino
    are the antiparticles of the electron, the
    proton, the neutron and the neutrino
    respectively.
  • Comparison of particle and antiparticle masses,
    charge and rest energy in MeV.
  • Knowledge of annihilation and pair production
    processes and the respective energies involved.
    The use of E mc2 is not required in
    calculations.

3
Antimatter
  • Most particles of normal matter, such as protons,
    neutrons and electrons have a corresponding
    particle that
  • has the same mass
  • has opposite charge (if the normal particle is
    charged)
  • will undergo annihilation with the normal
    particle if they meet
  • Examples
  • an antiproton is negatively charged
  • an anti-electron, normally called a positron, has
    a positive charge

LHC Rap
4
Further notes on antimatter
  • Other particle properties are also reversed in
    antimatter allowing the existence of uncharged
    antiparticles such as the antineutron.
  • Two particles that have the same mass and
    opposite charges are not necessarily a particle
    and an antiparticle pair.
  • The antineutrino produced in beta-minus decay is
    an example of antimatter.
  • Most examples of antimatter have a symbol that
    adds a bar above the normal matter symbol e.g.
  • Certain man-made isotopes are made in order to
    provide a source of antimatter. e.g. positrons
    are needed for PET scans (see page 10).

5
Annhilation
  • When a particle and its corresponding
    antiparticle meet together annihilation occurs.
  • All of their mass and kinetic energy is converted
    into two photons of equal frequency that move off
    in opposite directions.

6
Pair production
  • The opposite of annihilation.
  • The energy of one photon can be used to create a
    particle and its corresponding antiparticle.
  • The proton ceases to exist afterwards

7
The electron-volt (eV) and MeV
  • The electron-volt (symbol eV) is a very small
    unit of energy equal to 1.6 x 10-19 J
  • The electron-volt is equal to the kinetic energy
    gained by an electron when it is accelerated by a
    potential difference of one volt
  • Also 1 MeV (megaelectron-volt) 1.6 x 10-13 J
  • Question Calculate the energy in electron-volts
    of a photon of orange light of frequency 4.5 x
    1014 Hz
  • E h x f (6.63 x 10-34 Js) x (4.5 x 1014 Hz)
  • 2.98 x 10-19 J
  • energy in eV energy in joules / 1.6 x
    10-19
  • 1.86 eV

8
Particle rest energy
  • Using Einsteins relation E mc2 the energy
    equivalent of mass can be calculated. The masses
    of sub-atomic particles are commonly quoted in
    energy terms using the unit MeV.
  • Example the mass of a proton is 1.67 x 10-27 kg
  • E mc2 (1.67 x 10-27 kg) x (3.0 x 108 ms-1)2
  • 1.50 x 10-10 J
  • This is normally expressed in terms of MeV where
    1 MeV 1.6 x 10-13 J
  • And so the mass-energy of a proton in MeV (1.50
    x 10-10 J) / (1.6 x 10-13 J)
  • 938 MeV
  • This will be the energy of a stationary proton
    having no kinetic energy and as such is referred
    to as the rest energy of a proton
  • Other (and more precise) rest energies in MeV
    (from page 245)
  • proton 938.257 neutron 939.551 electron
    0.510999 photon 0
  • Mass is sometimes quoted using the unit GeV/c2
    (1000 MeV/c2 1 GeV/c2 )
  • for example proton rest mass 0.938 GeV/c2

9
Annihilation calculation
  • Calculate the minimum energies of the photons
    produced by the annihilation of a proton and
    antiproton.
  • The minimum energies occur when the pair of
    particles have initially insignificant kinetic
    energy.
  • rest energy of a proton in MeV 938MeV
  • rest energy of an antiproton also 938MeV
  • total mass converted into electromagnetic
    radiation in the form of two photons 1876 MeV
  • therefore each photon has an energy of 938 MeV
  • Further question What would be the wavelength of
    these photons?
  • 938MeV 1.50 x 10-10 J
  • E hc / ? becomes ? E / hc
  • and so ? (1.50 x 10-10 J) / ((6.63 x 10-34 Js)
    x (3.0 x 108 ms-1))
  • 7.54 x 10-18 m (gamma radiation)

10
Pair production calculation
  • Calculate the minimum photon energy required to
    produce an electron-positron pair.
  • The minimum energy will produce two stationary
    particles (which would then annihilate each other
    again!)
  • rest energy of an electron in MeV 0.511 MeV
  • rest energy of a positron also 0.511MeV
  • therefore minimum energy required 2 x 0.511
  • 1.022 MeV
  • Further question What would be the frequency of
    this photon?
  • 1.022 MeV 1.64 x 10-13 J
  • E hf becomes f E / h
  • and so f (1.64 x 10-13 J) / (6.63 x 10-34 Js)
  • 2.47 x 1020 Hz (gamma radiation)

11
Notes from Breithaupt pages 10 to 12
  • What is anitimatter? How does antimatter compare
    in mass and charge with normal matter?
  • State what is meant by annihilation and
    pair-production in the context of antimatter.
  • What is (a) an electron-volt (b) MeV?
  • Explain how the rest energy of a proton can be
    stated as 938MeV
  • Explain why a photon must have a minimum energy
    of 1.022MeV in order to produce an
    electro-positron pair.
  • How was the positron first discovered? How are
    positrons used in PET scans?
  • Try the summary questions on page 12

12
Answers to the summary questions
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