The hell bombLaurence, William L. (William Leonard)
Philosophy
The hell bomb
Laurence, William L. (William Leonard)
Hydrogen bomb
The same formula also reveals the time it would take liquid deuterium to
ignite at higher temperatures, the increase of which shortens the
ignition time. These figures show that the ignition time for liquid
deuterium at 75,000,000 degrees centigrade is 40 microseconds. At
100,000,000 degrees the time is 30 microseconds; at 150,000,000 degrees,
15 microseconds; and at 200,000,000 degrees on the centigrade scale,
about 4.8 millionths of a second. Doubling the temperature speeds up the
ignition time for liquid deuterium by a factor of about six.
The problem thus is a dual one: to raise the temperature at which the
A-bomb explodes, and to extend the time before the A-bomb flies apart.
It is also obvious that if the liquid deuterium is to be ignited at all,
it must be done before the bomb has disintegrated—that is, during the
incredibly short time interval before it expands into a cloud of vapor
and gas, since by then the deuterium would no longer be liquid.
Can we increase the A-bomb’s temperature fourfold to 200,000,000 degrees
and literally make time stand still while it holds together for nearly
five millionths of a second? To get a better understanding of the
problem we must take a closer look at what takes place inside the A-bomb
during the infinitesimal interval in which it comes to life.
This life history of the A-bomb is an incredible tale, from the time its
inner mechanisms are set in motion until its metamorphosis into a great
ball of fire. As explained earlier, the A-bomb’s explosion takes place
through a process akin to spontaneous combustion as soon as a certain
minimum amount (critical mass) of either one of two fissionable
(combustible) elements—uranium 235 or plutonium—is assembled in one
unit. The most obvious way it takes place is by bringing together two
pieces of uranium 235 (U-235), or plutonium, each less than a critical
mass, firing one of these into the other with a gun mechanism, thus
creating a critical mass at the last minute. If, for example, the
critical mass at which spontaneous combustion takes place is ten
kilograms (the actual figure is a top secret), then the firing of a
piece of one kilogram into another of nine kilograms would bring
together a critical mass that would explode faster than the eye could
wink—in fact, some thousands of times faster than TNT.
Public-domain text, read in full here on John Shaqi.
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