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Outline
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Nuclear Reactions
  • Fission and Fusion
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A brief history…
  • 1919:  Ernest Rutherford experimented with bombarding nitrogen gas molecules with alpha particles emitted from bismuth-214
  • Discovery:  faster moving particles were produced, and these could travel farther than the alpha particles!
  • “New” particles also deflected in a magnetic field like a positive particle
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A brief history…
  • Conclusion:  The faster moving particles were protons
  • Artificial Transmutation:
    • The change of one element to another through the bombardment of a nucleus


  • More experiments to determine exact nature of the particles and how they were “created” done with a cloud chamber…
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Cloud Chambers
  • Invented ~1911 by a Scottish Atmospheric Physicist (C.T.R. Wilson) to experiment with rain clouds.
    • Enclosed environment made to be supersaturated (originally with water vapor, now commonly ethanol)
    • Ions introduced to this environment would attract water molecules (which are polar), forming clouds…
  • Earned a share in the
  • 1927 Nobel Prize in
  • Physics for the invention…
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Cloud Chambers
  • Why would this be useful for Rutherford?
    • Water vapor condenses around ions
    • An alpha particle is ionizing radiation, thus leave a LOT of ions in its path
    • Water vapor would condense around these ions, leaving a vapor trail showing where an alpha particle had been…
  • Video


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Rutherford’s Theories…
  • If proton was simply “chipped off” the Nitrogen nucleus by the alpha particle, there should be 4 visible tracks in the cloud chamber:
      • The original alpha particle BEFORE collision
      • The alpha particle AFTER the collision
      • The “chipped off” proton
      • The Nitrogen nucleus, now charged, as it recoiled after the collision
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Rutherford’s Theories…
  • If alpha particle was absorbed, and that caused the proton to be pushed out, then there should be 3 visible tracks:
      • The alpha particle before collision
      • The proton emitted after the collision
      • The path of the recoiling Nitrogen nucleus
  • This theory was proven true in 1925
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Balancing Nuclear Equations:
  • Note:  Deuteron = Hydrogen-2 atom, a.k.a Deuterium
  • Example problem:
    • A sample of Oxygen-16 is bombarded with neutrons.  If one of the resulting products is a deuteron, what is the resulting nucleus?

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Unified Mass Unit (u)
  • A unit adopted by scientists that is  more appropriate for masses along the order of magnitude of atomic masses
  • 1 u = 1.66 x 10-27 kg
  • Mass of an electron (me) = 0.000549 u
  • Mass of a proton (mp) = 1.007277 u
  • Mass of a neutron (mn) = 1.008665 u
  • Mass of 1 H atom (mH) = 1.007825 u
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Mass-energy equivalence
  • Einstein hypothesized a relationship between mass and energy in 1905
  • Many years later, data from nuclear reactions showed that his hypothesis was indeed true


  • c = 3.00 x 108 m·s-1
  • m = mass (kg)
  • E = Energy (J)
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Mass-energy equivalence


  • Used to calculate the Rest Energy of a mass
  • Used to calculate the amount of energy released in nuclear reactions
  • For Example:
  • Calculate the amount of energy released when 1.00 kg of fuel is used up in a nuclear reactor…


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Binding Energy
  • All atomic nuclei have a total mass that is lower than the sum of the masses of each individual particle
    • For example:  The EXPECTED mass of an atom of Helium would be the sum of the mass of 2 neutrons, 2 protons, and 2 electrons:
  • 2(0.000549 u) + 2(1.007277 u) + 2(1.008665 u) = 4.032982 u
  • The MEASURED mass of an atom of helium has been found to be 4.002602 u
  • àa difference of 0.03038 u
  • This difference is known as the Mass Defect of the atom
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Binding Energy
  • …a measure of the energy needed to keep a nucleus together
  • Binding Energy is the energy equivalent of the mass defect
  • E = mc2
  • E = (1.66 x 10-27 kg)(3.00 x 108 m·s-1)2
  • E = 1.49 x 10-10 J = 931 MeV
  • (Since 1 eV = 1.6 x 10-19 J)



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Binding Energy Example:
  • Calculate the binding energy of Oxygen-16.  The measured mass of Oxygen-16 is 15.994915 u
  • 8 protons+8 electrons+8 neutrons


  • 8mH + 8mn = mexpected
  • = 8(1.007825 u) + 8(1.008665 u)
  • = 8.062600 u + 8.069320 u
  • = 16.131920 u


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Binding Energy Example:
  • Calculate the binding energy of Oxygen-16.  The measured mass of Oxygen-16 is 15.994915 u
  • mdefect = mexpected – mmeasured
  • = 16.131920 u – 15.994915 u
  • = 0.137005 u


  • Eb = mdefect · (931 MeV·u-1)
  • Eb = (0.137005)(931)
  • = 127 MeV


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Nuclear Reactions
  • Fission:  A reaction that involves the splitting of a large, unstable nucleus into 2 or more smaller, more stable nuclei




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Nuclear Reactions

  • Fusion: A reaction that joins two very light nuclei to form a heavier nucleus









  • Picture source:  www.atomicarchive.com
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Nuclear Reactions and Binding Energy
  • Nuclei with higher amounts of binding energy per nucleon are more stable than those with lower amounts of binding energy per nucleon.
  • Fission and fusion processes each release large amounts of energy as the nuclei join or split to form more stable products.
  • To predict how much energy can result from a nuclear reaction, we use a binding energy curve…
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Binding Energy Curve
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Binding Energy Curve
  • Example:  Use the binding energy curve to predict the amount of energy released when Uranium-235 undergoes fission to produce two Palladium-117 fragments.
  • Eb for 235U = 7.6 MeV/nucleon
  • Eb for 117Pd = 8.4 MeV/nucleon
  • The difference between these values, multiplied by the total number of nucleons, is equal to the amount of energy released in the reaction:
  • (0.8 MeV/nucleon) x (235 Nucleons) = 188 MeV
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Nuclear Fission
  • Only takes place in certain very heavy elements, such as Uranium-235
  • Fissile Uranium-235 is used in nuclear reactions:
      • Nucleus bombarded with a neutron to begin a chain reaction…



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Fission Reactions
  • Self-sustaining (chain) reactions:  when enough neutrons are produced to naturally enable the reaction to continue until all fissile material is gone
    • Examples:  Nuclear Reactors in Power Plants; Bombs dropped on Hiroshima and Nagasaki in WWII
  • Critical Mass:  The amount of fissile material required to sustain a fission reaction


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Nuclear Fusion Reactions
  • Conditions required for fusion reactions:
      • Very high temperatures (because nuclei need very high kinetic energies)
      • Very densely packed (to ensure that enough collisions will occur), therefore:
      • Very high pressures
  • Problems with creating fusion on Earth:
      • Containment is a huge problem
      • At temps required, atoms would ionize and technically would become a plasma
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Nuclear Fusion Reactions
  • Proton-Proton Cycle = the fusion reaction that is the source of energy in young/cool stars such as the sun:






  • The first two reactions in the cycle must occur twice
  • Total energy released = 24.7 MeV
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Fusion Example
  • Calculate the energy released when a proton and a deuteron undergo fusion to produce helium-3.