Nuclear Power. Source: Uranium-235 Process: – An unstable uranium nucleus is bombarded with a...
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Transcript of Nuclear Power. Source: Uranium-235 Process: – An unstable uranium nucleus is bombarded with a...
![Page 1: Nuclear Power. Source: Uranium-235 Process: – An unstable uranium nucleus is bombarded with a neutron and splits into two smaller nuclei and some neutrons.](https://reader035.fdocuments.us/reader035/viewer/2022081603/56649cc15503460f94989221/html5/thumbnails/1.jpg)
Nuclear Power
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• Source: Uranium-235• Process: – An unstable uranium nucleus is bombarded with a
neutron and splits into two smaller nuclei and some neutrons
– Rest mass of products is less than reactants so some matter is converted into energy
– Released neutrons strike other uranium nuclei causing further fissions
![Page 3: Nuclear Power. Source: Uranium-235 Process: – An unstable uranium nucleus is bombarded with a neutron and splits into two smaller nuclei and some neutrons.](https://reader035.fdocuments.us/reader035/viewer/2022081603/56649cc15503460f94989221/html5/thumbnails/3.jpg)
235 1 141 92 192 0 56 36 03U n Ba Kr n+ → + +
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• . The energy released by one atom of carbon-12 during combustion is approximately 4 eV. The energy released by one atom of uranium-235 during fission is approximately 180 MeV.
a) Based on this information, determine the ratio of the energy density of uranium-235 to that of carbon-12.
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23
25
= x molar mass
1mass = x .235 kg
6.02 10
mass=3.90x10
A
Nmass
N
x
kg−
23
26
= x molar mass
1mass = x .012 kg
6.02 10
mass=1.99x10
A
Nmass
N
x
kg−
6 1911180 10 1.60 10
2.88 101 1
x eV x Jx J
eV
−−⎛ ⎞⎛ ⎞
=⎜ ⎟⎜ ⎟⎝ ⎠⎝ ⎠
19194 1.60 10
6.40 101 1
eV x Jx J
eV
−−⎛ ⎞⎛ ⎞ =⎜ ⎟⎜ ⎟
⎝ ⎠⎝ ⎠
1113
25
7
2.88 107.38 10 /
3.90 10
7.38 10 /
e
x JD x J kg
x kg
x MJ kg
−
−= =
=
197
26
6.40 103.22 10 /
1.99 10
32.2 /
e
x JD x J kg
x kg
MJ kg
−
−= =
=7
6 U-235 7.38 102.3 10
C-12 32.2e
e
D xx
D= =
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b. With this information, explain an advantage of using U-235, instead of coal.
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Naturally Occurring Isotopes of Uranium
Uranium-238: most abundant (99.3%) but not used for fuel since it has a very small probability of fissioning when it captures a neutron.
Uranium-235: rare (0.3%) but used for fuel since
it has a much greater probability of fissioning when captures a neutron but must be a low-energy neutron (thermal neutron).
![Page 8: Nuclear Power. Source: Uranium-235 Process: – An unstable uranium nucleus is bombarded with a neutron and splits into two smaller nuclei and some neutrons.](https://reader035.fdocuments.us/reader035/viewer/2022081603/56649cc15503460f94989221/html5/thumbnails/8.jpg)
• Thermal Neutron: low-energy neutron (≈1eV) that favors fission reactions – energy comparable to gas particles at normal temperatures
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• Fuel Enrichment: process of increasing proportion of uranium-235 in a sample of uranium
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Fuel Enrichment• formation of gaseous uranium (uranium hexafluoride) from
uranium ores
• separated in gas centrifuges by spinning – heavier U-238 moves to outside
• increases proportion of U-235 to about 3-5% of total (low
enrichment) • This low enriched hex is compressed and turned into solid
uranium-oxide fuel pellets which are packed into tubes called fuel rods which will be used in the core of a nuclear reactor.
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• Advantage: More uranium is available for fission and a chain reaction can be sustained in a reactor to produce nuclear energy.
• Disadvantage: If the fuel is enriched to a high level (90% = weapons grade) it can be used in the core of a nuclear weapon. Possession of nuclear weapons is seen by many to be a threat to world peace.
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• Controlled nuclear fission: nuclear power production • Some material (control rod) absorbs excess neutrons
before they strike another nucleus. • This leaves only one neutron from each reaction to
produce another reaction. • If the total mass of uranium used is too small, too
many neutrons will escape without causing further fissions so the reaction cannot be sustained.
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• Uncontrolled Nuclear Fission: Nuclear weapons. – Fuel is enriched to a high level.– Reaction is an exponential, chain reaction. – Releases immense amounts of energy.
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Nuclear Reactor Model
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• Moderator: A substance, usually water or graphite, that is used to slow down the neutron to “thermal” levels. (a thermal neutron-1eV)
• Control Rods: Speed up or slow down the fission process. Neutron absorbing materials, like Cadmium or Boron. Rods move to capture more or less neutrons and control the speed of the reaction.
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• Coolant: frequently the same as the moderator. Heated in the reactor core, and flows through closed pipes (primary loop), through the exchanger, where it cools
• Heat Exchanger: Thermal energy of the hot coolant is transferred to cooler water, in a secondary loop. That water is turned to steam, which spins fan blades, that turns a magnet through a coil of wire, to generate electricity.
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• Sankey Diagram
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• Suppose the average power consumption for a household is 500 W per day. Estimate the amount of uranium-235 that would have to undergo fission to supply the household with electrical energy for a year.
• Assume plant is 100% efficient• Assume 200 MeV per fission
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Plutonium
• In a uranium-fueled reactor, as the U-235 depletes over time, the amount of Pu-239 increases. This plutonium is then extracted (by reprocessing of the uranium fuel rods) for use in a plutonium reactor or in a nuclear warhead.
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Nuclear Waste
• Atoms formed during nuclear reactions are still radioactive (not stable).
• Those atoms need to be disposed of, but will go through radioactive decay, releasing radiation.
• The radiation released causes damage to healthy cells, prenatal mutations, and cancer.
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Storage of Nuclear waste
Low-level waste: Radioactive material from mining, enrichment and operation of a plant must be disposed of. It’s often left encased in concrete.
• High-level waste: a major problem is the disposal of spent fuel rods. Some isotopes have ½ lives of thousands of years. Plutonium’s is 240,000 years.
• Some are stored under water at the reactor site for several years to cool off then sealed in steel cylinders and buried underground.
• Some are reprocessed to remove any plutonium and useful uranium. The remaining isotopes have shorter ½ lives and the long-term storage need is reduced.