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"In thermonuclear weapons, radiation from a fission explosive can be contained and used to transfer energy to compress and ignite a physically separate component containing thermonuclear fuel."

			The 3 basic concepts of thermonuclear devices,
			U.S. DOE, Sept 1980, Duane Sewell,
			Assistant Secretary of Energy for Defense,
			Official Declassification Act.


Under solar conditions (high temps of about 100 millions degrees C, 1 milion megabars pressure), H atoms fuse into He. Three isotopes of H exist:

	H1 (P)	protium
	H2 (D)	deuterium
	H3 (T)	tritium.

Protium reacts too slowly even in the sun so deuterium and tritium are used. Under solar conditions, the H atoms gain enough kinetic enery to overcome the electrostatic repulsion of their positive charges. The electrons which are normally found surrounding H nuclei have already been ionised. You have a plasma of positive nuclei. He is formed in a H-H reaction, releasing energy.

Sources of D and T

Heavy water (D2O) is present at 1 part in 6700 in normal tap water. You can separate the heavy water, and then obtain deuterium gas. D2 gas is obtained via electrolysis.

Tritium is radioactive, and is obtained via bombardment of Li6 with thermal (slow) neutrons. It beta decays like: T → He3 + e

T fuses with D at a temperature an order of mag lower than for D-D fusion, hence its usefulness in a weapon.


The lightest of metals, only 1/2 as dense as water. Found combined with other elements in igneous rocks and mineral spring water. Li7 is separated electrolytically from Li7Cl. Has several isotopes: Li5 to Li9. Li6 and Li7 are used in weapons, and are naturally occuring. Li5, Li8, and Li9 are man-made radioisotopes.

Li6 is present as 7.5% of all naturally occuring Li. Separation methods include electrolysis, distillation, chemical exchange, or EM methods. Li bonds with H to form the solid Li6D.

Back to the Story

Since the mass of the resultant He is less than the mass of the separate H, the excess energy is converted into radiation and kinetic energy of neutrons. The energy of these fast neutrons is high enough to split normal U-238. Slow neutrons only transmute U-238 into Np-239 (which then beta decays into Pu-239).

One cubic metre of gaseous deuterium, when fused into helium, yields the equivalent of about 10 megatons of TNT.

Deuterium and tritium are gases at room temperature, so their storage in a weapon would be cumbersome. Instead, a substance called lithium deuteride (Li6D or Li7D) is used. This material has the property of being a whitish, slightly-blue powdery light salt-solid (which is extremely hygroscopic) at room temperature. It is made by heating metal lithium in a vessel, into which deuterium gas is injected. It is then pressed and shaped into a ceramic.

When a neutron is absorbed by a LiD molecule, the molecule breaks up into a He, H3, and a deuterium. The D can then reacts with the T in fusion. This releases enormous amounts of energy, much greater than you would get in a fission reaction. The end products include a free n, and a He. Schematically:

U-238 fission releases fast neutrons and heat (thermal kinetic energy of neutrons).

	Li6 + n -> He4 + T + 4.7 MeV


	  D + T ->  He4 + n + 17.6 MeV.
      n + U-238 -> neutrons + fission products + energy

These reactions occur in under 1/10-6 secs. Additional reactions are:

	Li6 + D -> 2(He4) + 22.4 MeV
	    Li6 -> 2(He4) + n
	Li6 + P -> He4 + He3 + 4.0 MeV
	Li7 + P -> 2(He4) + 17.3 MeV
	Li7 + D -> Li8 + P
	Li7 + n -> He4 + T + n
	D + Li7 -> Be8 + n + 15.1 MeV
	D + D	-> T + H + 4.0 MeV
	D + D	-> He3 + n + 3.25 MeV
	D + D	-> He4 + 23 MeV
	T + T	-> He4 + 2n + 12.2 MeV
	He3 + D	-> He4 + H + 18.3 MeV
	D + n	-> T

Beryllium is useful in the core of a fission mass since you can use it to increase the neutron flux:

	Be9 + n	-> Be8 + 2n
	Be9 + D	-> Be8 + T + 4.53 MeV

For a thermonuclear reaction, you have to compress the Li6D solid to 15-30 times it's original uncompressed density at RTP (15lbs/foot^3). Compression is needed to:

(1) increase fusion *probability*. You pack the molecules closer together. In the process, you pave the way to overcoming the electrostatic repulsion of the H atoms in the Li6D.

(2) increase fusion *rate*, since you get quicker reactions when the reactants are packed closely together than far apart. The *time* for a reaction is inversely proportional to fuel density. Denser fuels mean shorter reaction times, and hence more chance of a larger number of reactions. The *rate* of reaction, on the other hand, is proportional to the square of the fuel density. Increase the density by a factor of 30, and your rate increases by a factor of 900.

Compression is a form of inertial confinement fusion (ICF). You are in effect counteracting the explosive forces released in the fusion, by giving the reactants an inwardly directed momentum. So the whole mass of fuel stays together. It's collapsing in on itself; at the same time it wants to tear itself apart.

PS, 1994

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