Title: Mass Defect, Binding Energy, Fission and Fusion
1Mass Defect, Binding Energy, Fission and Fusion
- Edward A. Mottel
- Department of Chemistry
- Rose-Hulman Institute of Technology
2Nuclear Energy
- Mass Defect
- Binding Energy
- Nuclear Fission
- Nuclear Fusion
- Comparisons of various forms of energy
3Mass Defect
- The nucleus
- is composed of protons and neutrons
- the actual mass is less than the mass of the
separate particles. - The "missing" mass is in the form of energy
holding the nucleus together.
4Uranium-238
The nuclear mass of uranium-238 is 238.0003 amu
238U
92
A proton is 1.00728 amu
A neutron is 1.00867 amu
What mass is expected for the nucleus of 238U?
5Uranium-238
(92)(1.00728) 92.6698
92 protons
(146)(1.00867) 147.2658
146 neutrons
predicted mass 239.9356
actual mass 238.0003
mass defect 1.9353 amu
6Masses of Atoms
The nuclear mass of 238U is 238.0003
Why does the Handbook of Chemistry and
Physics list the mass of uranium238 as 238.0508?
(92)(0.0005488) 238.0003 238.0508
7Binding Energy
- The mass defect indicates the total energy
involved in holding the nucleus together. - To determine the stability of the nucleus, the
binding energy per nuclear particle is a better
measure.
8Binding Energy of 238U
1.9353 amu
DE Dmc2 931.5 MeV/amu
What is the binding energy per nucleon of 238U?
9Binding Energy of 238U
10Binding Energy
11Nuclear Fission
- Fissionable materials
- Daughter products
- Energy release
- Nuclear chain reactions
- Nuclear reactors
- Control rods
- Breeder reactor
12Nuclear Fission
- Nuclear process in which the nucleus of the atom
breaks into two large fragments. - Fissionable materials
- undergo spontaneous fission or
- can be converted into a fissionable isotope
- Neutron capture can result in daughter products
which are more fissionable.
13Fissionable Materials
Fissionable
Non-Fissionable
235U
238U
239Pu
207Pb
12C
14Fissionable Materials
Natural abundance 235U 0.7 238U 99.3
What is the percentage of 235U in a commercial
sample of UO2?
235U _at_ 0.0
15Fission Daughter Products
Spontaneous fission is a statistical
process resulting in several different daughter
isotopes.
235U 1n 236U 140Ba 94Kr 2 1n
energy 141Ba 92Kr 3 1n energy 137Te
97Zr 2 1n energy 144Cs 90Rb 2 1n
energy 146La 87Br 3 1n energy
16Nuclear Chain Reaction
- In the previous disintegration process there are
an average of 2.3 neutrons generated per
disintegration. - If one neutron is captured for each nuclear
disintegration that occurs, the reaction is
self-sustaining.
17Nuclear Chain Reaction
fissionable material
18Nuclear Chain Reaction
19Nuclear Chain Reaction
20Nuclear Chain Reaction
21Nuclear Chain Reaction
22Nuclear Chain Reaction
23Nuclear Chain Reaction
24Nuclear Chain Reaction
25Nuclear Chain Reaction
26Nuclear Chain Reaction
27Nuclear Chain Reaction
28Nuclear Chain Reaction
29Nuclear Chain Reaction
30Nuclear Chain Reaction
31Control Rods
Control rods regulate the rate of reaction by
controlling the neutron flux.
What kind of material would be used as a control
rod?
32Thermal Neutron Capture Cross-Section
0.00051 0.00001 b
2H
0.5 0.2 b
10B
0.0034 0.0003 b
12C
20000 300 b
113Cd
680 2 b
235U
2.720 0.025 b
238U
Which of these elements would limit excess
neutrons?
33Nuclear Reactor
34Nuclear Reactor
35Breeder Reactor
- Converts non-fissionable material into
fissionable material
Non-fissionable
Fissionable
36Nuclear Fusion
- Process by which lighter nuclei combine to form
heavier nuclei. - 4 1H 2 e 4He2
- Dm 0.02758 gmol1
- The energy source of stars.
37Nuclear Mechanismsproton-proton mechanism
- ( 1H 1H 2H b ) x2
- ( 2H 1H 3He g ) x2
- 3He 3He 4He 2 1H
- ( b e 2 g ) x2
2 e 6 1H 2 3He 4He 2 3He 6 g 2 1H
Whats the overall net nuclear reaction?
38Nuclear Mechanismscarbon cycle mechanism
- 12C 1H 13N g
- 13N 13C b
- 13C 1H 14N g
- 14N 1H 15O g
- 15O 15N b
- 15N 1H 12C 4He
- ( b e 2 g ) x2
-
2 e 4 1H 4He 7 g
39Reaction Conditions
- For two nuclei to react, they must be moving at
high velocities to overcome the coulombic
repulsion of two positive charges. - Typical thermal energies of _at_107 K in a star.
40Laboratory Attempts
- Laser Fusion
- 3H 2H 4He 1H
- Frozen sample heated to 106 K by laser
- Cold Fusion
- Room temperature process involving deuterium
dissolved in a metal matrix - 2H 2H 4He g
41Energy Comparison
C O
products
2
235
1
10
7
U
n
products
1.7 x 10
7.1 x 10
9
8
1
4
H
products
2.4 x 10
5.9 x 10
42On Line File of Nuclide Data
- http//necs01.dne.bnl.gov/CoN/
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