Lecture 4 Flashcards
The neutron spectrum averaged cross sections in a fast reactor are substantially _____ than those in a thermal system
smaller
In a fast reactor, the spatial distribution of the flux will be ____ across the cross section of the cell
K infinite equation as a function of enrichment for fast reactors
In the thermal and intermediate neutron energy ranges, cross sections generally are ___ than for higher energy neutrons.
larger
Thermal reactor coolant and moderator region dimensions are typically ___ than those of the coolant channels in fast reactors
larger
In thermal reactors the flux (will/will not) differ significantly
will
k infinite for thermal reactors
What is the four factor formula?
k infinite = εpfη
Define ε
fast fission factor, the ratio of fast neutrons produced by fissions at all energies to the number of fast neutrons produced in thermal fission
ε =
1 + probable number of collisions in fast neutron spectrum * nu / probable number of collisions in thermal neutron spectrum * nu
define p
the probablity that a neutron will be slowed to thermal energy and escape resonance capture
p =
numer of neutrons that reach thermal energies/numer of fast neutrons that start to slow down
Increasing the temperature ____ the self-shielding at the resonance peak, and this _____ the absorption as temp increases
decreases
increases
The resonance integral eqn
integral of absorption probablity in fuel/scattering dE
Seperation of fuel from moderator causes resonance escape probablity to
increase