Time Travel Research Center
© 2005 Cetin BAL - GSM:+90 05366063183 - Turkey / Denizli
Schematic Design of a Fusion (Hydrogen)
Bomb
Evolution of Explosion
Assume 10 kt trigger / 20 Mt total yield
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Detonation of HE
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Implosion and initiation of fission trigger (t = 0)
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t = 1/2 microsecond: ~50 generations, E ~ 108 calories
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t = 1 microsecond: fission stops
E ~ 1013 calories
T ~ 20 x 106 K
80% of energy in thermal X-rays
Pressure P ~ 10 6 atmospheres
-
Radiation and plasma compress and heat LiD
-
LiD fuses, releases energetic neutrons + ~10Mt
-
Neutrons cause fission in U-238 blanket + ~10Mt
-
Weapon innards and casing vaporized, forming fireball (still has not
moved much)
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80%
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photons
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Yield ~
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15%
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debris
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5%
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prompt nuclear radiation
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-
Fireball expands
At first, vexp ~ 107 cm/s ~ 100 miles/sec
(Lecture addendum: In class was a mock-up of a MK 12A reentry
vehicle with a 335 kt warhead. It was roughly man-sized. Its yield would
break down as follows: primary ~20 kt, secondary ~150 kt, casing ~150kt)
Energy From a Single Fission
n + (fissile nucleus) --> (fission fragments) + (2 or 3 n)
Energy Distribution (MeV)
Kinetic energy of fission fragments |
~ 165 |
* |
Energy of prompt gamma-rays |
7 |
* |
KE of prompt neutrons |
5 |
|
KE of beta-rays from fragments |
7 |
|
E of gamma-rays from fragments |
6 |
|
E of neutrinos from fragments |
6 |
|
Total
|
~ 200
|
|
* Only this 172 MeV is counted in the explosive "yield" of nuclear
weapons
Fusion Reactions
Thermonuclear
|
|
+
|
|
-->
|
|
+
|
|
+
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Energy
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Probability: |
1.
|
D
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+
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D
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-->
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3He
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+
|
n
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+
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3.2 MeV
|
Int. |
2.
|
D
|
+
|
D
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-->
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T
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+
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1H
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+
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4.0 MeV
|
Int. |
3.
|
T
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+
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D
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-->
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4He
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+
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n
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+
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17.6 MeV
|
High |
4.
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T
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+
|
T
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-->
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4He
|
+
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2n
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+
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11.3 MeV
|
Low |
Need T ~ 20 x 106 K to react
Most energy comes off in neutron kinetic energy
==> can cause fission of U-238 ("fission blanket" concept)
Typically, yield is 50% fission / 50% fusion
Yields
Reactions 1+2+3: 5D (10 amu) yield 24.8 MeV
Recall: 1 fission (235 amu) yields 200 MeV
Fusion = 24.8/10 ~ 3 x 200/235 ~ 3 x fission yield per kg
Catalysis--
6Li + n --> 4He + T + 4.8 MeV
--> Fusion of 20 g of deuterium yields 1 kt <--
Terrorist Nuclear Bombs
Some problems confronting terrorist organizations wishing to construct a
nuclear explosive --
-
Assembling a team of technical personnel
-
Substantial financial costs
-
Radiation and chemical hazards
-
Possibility of detection
-
Acquisition of fissile material
Requirements for Making a Fission
Bomb
-
Know nuclear physics of fission
-
Have needed data on the physical and chemical properties of weapon
materials
-
Build technical facilities to fabricate and test devices and
components of the chosen design
All these requirements are now met in any significantly
industrialized country
-
Obtain the needed fissile material
-
Allocate the necessary resources
Thermonuclear Weapons
Use deuterium (D) and tritium (T) - almost as plentiful as water!
The trick is to ignite them...
"Boosted" fission weapons
Add a small amount of D and T; get D-D and D-T fusion
Fusion contributes little to yield, but many fast neutrons
n + 238U --> (fission products) + energy
Increases efficiency of fission weapon |
|
True fusion weapons
- First attempts
-
Used liquid D ("Mike", 1952)
Experiments, not yet bombs
- "Improved" method
-
Catalyze D-T burning with 6Li
(Natural Li is ~7.5% 6Li
6Li + n --> 4He + T + 4.8 MeV
Usually use solid LiD; then get:
6LiD + n --> 4He + T + D + 4.8 MeV
T + D --> 4He + n + 17.6 MeV
Net effect is:
6LiD + n --> 2 4He + n + 22.4 MeV
Alıntı:
http://wug.physics.uiuc.edu/courses/phys180/spring98/lectures/07/slide05.html
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