The hell bombLaurence, William L. (William Leonard)
Philosophy
The hell bomb
Laurence, William L. (William Leonard)
Hydrogen bomb
Here must be mentioned another form of hydrogen, named tritium. It has
long ago disappeared from nature but it is now being re-created in
ponderable amounts in our atomic furnaces. Tritium, the nucleus of which
is known as a triton, weighs three times as much as the lightest form of
hydrogen. It has an energy content nearly twice that of deuterium. But
it is very difficult to make and is extremely expensive. Its cost per
kilogram at present AEC prices is close to a billion dollars, as
compared with no more than $4,500 for a kilogram of deuterium. A
combination of deuterons and tritons would release the greatest energy
of all, 3.5 times the energy of deuterons alone. It would reduce the
amount of tritons required to half the volume and three fifths of the
weight required in a pure triton bomb, thus making the cost considerably
lower.
But why bother with such fantastically costly tritons when we can get
all the deuterium we want at no more than $4,500 a kilogram, while we
can make up the difference in energy by merely incorporating two to
three and a half times as much deuterium? Here we are dealing with what
is probably the most ticklish question in the design of the H-bomb.
To light a fire successfully, it is not enough merely to have a match.
The match must burn for a time long enough for its flame to act. If you
try to light a cigarette in a strong wind, the wind may blow out your
match so fast that your cigarette will not light. The same question
presents itself here, but on a much greater scale. The match for
lighting deuterium—namely, the A-bomb—burns only for about a hundred
billionths of a second. Is this time long enough to light the
“cigarette” with this one and only “match”?
It is known that the time is much too slow for lighting deuterium in its
gaseous form. But it is also known that the inflammability is much
faster when the gas is compressed to its liquid form, at which its
density is 790 times greater. At this density it would take only seven
liters (about 7.4 quarts) per one kilogram (2.2 pounds), as compared
with 5,555 liters for gaseous deuterium. And it catches fire in a much
shorter time.
Is this time long enough? On the answer to this question will depend
whether the hydrogen bomb will consist of deuterium alone or of
deuterium and tritium, for it is known that the deuteron-triton
combination catches fire much faster than deuterons or tritons alone.
Public-domain text, read in full here on John Shaqi.
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