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Radioactive Decay

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Half-lives are unaffected by the nuclei's surroundings and only depend on what ... Since the 14C decays, after 5730 years, half of it will be gone ... – PowerPoint PPT presentation

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Title: Radioactive Decay


1
Radioactive Decay
  • The number of atoms in a sample that decay
    depends on the total number of atoms in the
    sample!!
  • This fact yields a rate of decay called an
    exponential decay
  • Exponential decay has a simple picture

2
Exponential Decay
Decay of 226Ra
3
Half-Life
  • There are a large range of half-lives seen in
    nature
  • Half-lives are unaffected by the nucleis
    surroundings and only depend on what goes on
    inside the nucleus
  • 238U has a half-life of 4.5 billion years

4
Half-Life
  • To summarize, one-half of the sample will decay
    in one half-fife
  • One-half of that one-half will decay in the next
    half life
  • One-half of that one-fourth will decay in the
    next half life

5
Half-Life
6
Transmutations
  • The changing of one element to another is called
    transmutation
  • This occurs whenever there is an alpha decay or a
    beta decay
  • Remember, that for a gamma decay, the nucleus
    just changes internal energy levels, but doesnt
    change the identity of nucleons

7
Transmutations
  • Consider an alpha decay
  • 238U - 234Th alpha (4He)
  • Have to count the number of protons and neutrons
  • Protons U-92, Th-90, He-2 Balance!!
  • Neutrons U-146, Th-144, He-2 Balance!!
  • Mass No. U-238, Th-234, He-4 Balance!!

8
Transmutations
  • Consider a beta decay
  • 234Th - 234Pa beta
  • This means a neutron changed into a proton
  • So mass number stays the same
  • Proton number increases by one and the thorium
    changes into protactinium
  • Actually an anti-neutrino appears also

9
Transmutations
10
Artificial Transmutation
  • First example was Rutherford bombarding nitrogen
    with alpha particles
  • 4He 14N - 17O 1H
  • He viewed the reaction with a cloud chamber
  • The particles left a vapor trail in the mist

11
Cloud Chamber
When you pull the piston down suddenly, you
reduce the air pressure in the chamber. This
means vapor is now super-saturated. A charged
particle acts as a nucleation seed to condense
the liquid from the vapor. This is the same
principle as cloud-seeding to make it rain.
12
Isotopic Dating
  • Cosmic rays (mostly high energy protons) strike
    upper atmosphere and cause transmutations that
    result in many protons and neutrons being sprayed
    out
  • Protons tend to grab electrons from other atoms
    and become simple hydrogen
  • Neutrons keep going and smash into other atoms

13
Isotopic Dating
  • When a neutron strikes nitrogen
  • 1n 14N - 14C 1H
  • In the atmosphere, 14C is about 1 part in 1011
  • Reacts with plants just like 12C
  • 14C decays via beta emission
  • 14C - 14N beta half life of 5730 years

14
Carbon Dating
  • When a plant dies, it stops the intake of carbon
  • Since the 14C decays, after 5730 years, half of
    it will be gone
  • We can just weigh a piece of dead wood, calculate
    how much 14C it originally had and measure to how
    much it has now to get the age

15
Uranium Dating
  • We know the half -life of 238U and 235U
  • They have series that end in 206Pb and 207Pb
  • Compare how much U vs. special lead and calculate
    the age of the rock!!
  • Carbon dating only good for about 50,000 years
  • Uranium rock dating good for millions of years

16
Nuclear Fission
1n 235U - 91Kr 142Ba 31n
17
Chain Reaction
18
Chain Reaction
  • The key to keeping the reaction going is that at
    least one of the neutrons given off, must cause
    another fission
  • Controlled reaction in a nuclear reactor
  • If two or three cause fissions, you can get a
    bomb!
  • Idea of critical mass

19
Critical Mass
20
Atom Bomb
21
Nuclear Reactor
22
Mass-Energy Relationship
  • Einsteins famous equation E mc2
  • A nucleus is measured to have less mass than the
    sum of its parts
  • 12C has a mass exactly 12.00000 amu
  • Six protons have mass 6 x 1.00728 amu
  • Six neutrons have mass 6 x 1.00867 amu
  • Parts have mass 12.09570 amu

23
Mass-Energy Relationship
  • So, where does the mass go?
  • It is the binding energy that is holding the
    nucleus together
  • Interesting to look at the mass per nucleon as we
    change the atomic number (change which element we
    look at)

24
Mass-Energy Relationship
25
Nuclear Fission
26
Nuclear Fusion
27
Nuclear Energy
28
Fusion Reactions
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