In a nuclear reactor, a neutron of high speed `(~~10^(7)ms^(-1))` must be slowed down to `10^(3)ms^(-1)` so that it can have a high probality of interacting with isotipe `_92U^(235)` and causing it to fission. Show that a neutron can lose most of its K.E. in an elastic collision with a light nuclei like deuterium or carbon which has a mass of only a fewe times the neutron mass. The material making up the light nuclei usually heavy water `(D_(2)O)` or graphite is called modertaor.
Initial K.E. of neutron is
`K_(1)=(1)/(2)m_(1)u_(1)^(2)`
Velocity of neutron after collision with deuterium, `upsilon_(1)=((m_(1)-m_(2))u_(1))/(m_(1)+m_(2))`
Final K.E. of neutron is
`K_(2)=(1)/(2)m_(1)upsilon_(1)^(2)=(1)/(2)m_(1)((m_(1)-m_(2))/(m_(1)+m_(2)))^(2)u_(1)^(2)`
`:.` Frational K.E. retained by neutron is
`f_(1)=(K_(2))/(K_(1))=((m_(1)-m_(2))/(m_(1)+m_(2)))^(2)`
For deuterium, `m_(2)=2m_(1) :. f_(1)=(1)/(9)`,
Fractional K.E. lost by neutron
`f_(2)=1-f_(1)=1-(1)/(9)=(8)/(9)=90%`
This is the fractional K.E. gained by moderating nuclei.
Therefore, almost `90% ` of neutron energy is transferred to deuterium. Similarly, in case of carbon, we can show that `f_(1)=28.4%` and `f_(2)=71.6%`.