1 n + 235U → [236U] → 92Kr + 141Ba + 3 nThe above equation informs us that one energetic neutron properly striking an atom of uranium, isotope 235, produces, first and temporarily, an ordinarily stable atom of uranium, isotope 236.
However, the 236 isotope of uranium is not entirely stable, and the kinetic energy provided by a fast-moving neutron, combined with the energy within the nucleus itself, puts the total energy in the nucleus “over the top” so that the atom of 236U splits into the lighter elements written above, namely krypton gas and barium metal.
The decay in producing these elements, does not balance without the release of three neutrons and an amazing amount of energy. Since the reaction is initiated with only one neutron, but winds up producing three, there are two high-energy neutrons left to “get into trouble”.
This suggests that, given the correct conditions, a chain reaction can be made to occur. If the quantity of uranium atoms used is sufficiently above a certain critical mass, the end result can be the release of enormous energy in a violent explosion. If the reaction is prevented from surpassing the critical mass level, the energy can be put to practical use, instead of destructive use.
This All Sounds Convincing But…Can one achieve a chain reaction from a chunk of ordinary uranium metal, the mixture of isotopes as it occurs in nature, with its tiny fraction of a percent of 235U in its makeup?
The answer is, no. The 235 isotope needs to be isolated and enough gathered to reach critical mass. What is critical mass? A very simple online definition reads: the minimum amount of fissile material needed to maintain a nuclear chain reaction.
Notice critical mass is required to maintain a fission chain reaction. In fact, at least for the production of an atomic weapons, supercritical mass, that is an amount of mass over critical mass, must be achieved.
Just How Much is Critical Mass?In order to keep the fission reaction going, at least one of the three neutrons is required to initiate the next reaction sequence if a chain is to begin. Up to two of the three neutrons produced by each fission reaction may be “wasted”, not more, if one is to establish a chain.
There are a number of parameters or factors that determine precisely what critical mass is for any given fissionable (fissile) material. Among them are the shape of the mass and its density. The more spherical the shape and the greater the density, the better. A neutron-reflective shield that surrounds the mass lessens the quantity of required material. There are other manipulative factors that help minimize the required mass.
If the bare minimum of critical mass is achieved, after some of the fissionable “fuel” is used up, the critical mass then becomes a subcritical mass. Some fission continues, but fades. On the other hand, an amount of material greater than critical mass is said to be a supercritical mass. This enables initiation of fusion, but also allows the sustaining of a chain reaction.
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