curie said:
Btw, I would be interested to read your input on the questions you posed on the example scenarios.
curie,
Since Emfuser took a pass at answering the questions i posed; I'll do so for you.
In regards to the core of the Little Boy device sitting there without any neutrons:
Is Little Boy critical? Yes - in fact the assembled Little Boy core is super-critical.
Even though there are no neutrons, the "k" of Little Boy is defined; and it is greater than
unity. The "k" and the "criticality" are properties of the geometry and materials;
irrespective of whether there are neutrons in the device at the time.
As I explained in my previous response to Emfuser, one of the physical properties
of the super-critical assembly is the probability that a neutron introduced at a given
position, with a given energy, and going in a given direction will lead to a chain reaction,
as opposed to immediately being absorbed, or having the chain reaction start and then
die out. It turns out that the probability that the neutron will cause a runaway chain
reaction is a function of the "k" the assembly [ in addition to the properties of the added
neutron].
Under Emfuser's understanding [ or in actuality lack thereof ]; there would be no "k"
defined because his "understanding" requires neutrons to be present. The super-critical
Little Boy assembly has a physical property every bit as REAL as any other physical
property - namely this probability - but we can't characterize it without the value of "k".
Evidently Emfuser is also ignorant of the concept of "neutron importance". You need
the concept of neutron importance when you define reactivity. Neutron importance
will properly account for the fact that a given number of neutron introduced into the
core will have differing effects on the reactivity based on the position, energy, and
direction of the incident neutrons.
The neutron importance is the solution to the adjoint transport equation. However,
unlike the forward transport equation which solves for a physical quantity - namely
the distribution of neutrons in phase space - there are no "adjoint neutrons". So
Emfuser would contend that it isn't "real".
As another analogy, consider the suspension system on your car. This suspension
system can either be underdamped, overdamped, or "critically damped". [ If your
"shocks" are worn - it will be underdamped. ] This property of the car's suspension
system EXISTS and is WELL DEFINED - independent of whether the suspension
system is actually moving at the time. The car's suspension is either underdamped,
overdamped, or critically dampded; even if it is not moving. Likewise, a reactor is
sub-critical, super-critical, or exactly critical; independent of whether there are actually
neutrons in the reactor multiplying or attenuating.
Emfuser knows only basic Reactor Theory 101. Fortunately, I would assume the
people that actually designed the reactor he works on have a more comprehensive
knowledge of Nuclear Reactor Theory.
The question about putting a pulse into an exactly critical reactor:
Putting a pulse of neutrons into the reactor DOESN'T CHANGE the criticality.
Likewise, putting a pulse of neutrons in the reactor DOESN'T CHANGE the "k" of the
reacor. [ Assuming no heating that would alter the material properties. There will be
an insignificant amount of heating - depending on the magnitude of the pulse ].
The reactivity is different. The reactivity DOES DEPEND on the distribution of neutrons
in the reactor.
Before the pulse. the exactly critical reactor had a reactivity of ZERO. The reactivity
vanishes because the geometry and materials are in an exactly critical configuration,
AND I also premised the question with the fact that the neutron population present was
the fundamental mode. Under those conditions, the reactivity vanishes identically.
However, when I add the pulse of neutrons; I'm augmenting the neutron population with
a bunch of neutrons that are NOT in the same distribution as the fundamental mode.
With the addition of this neutron pulse; the reactor will go through a transient on its way
to a new steady-state. During this transition the reactivity is NOT ZERO!
When the reactor reaches a new steady state with an increased neutron population; that
new population will be a multiple of the fundamental mode; so that the neutron population
is once again in the fundamental mode and the reactivity vanishes exactly.
[This is all modulo the assumption of constant material properties; i.e. insignificant heating
or the assumption that the cooling system removes any excess heat ]
This is EXACTLY the type of questions one would expect in a graduate program in
nuclear engineering; in a reactor theory or transport theory course.
Dr. Gregory Greenman
Physicist