In some prior speculation about the possibility of designing
an environmentally acceptable and safe uranium fission
reactor, which employs direct thermal to electric conversion
and depends on "makeup" neutrons in the form of fully
shrunken hydrinos, an idea was present by Robin van
Spaandonk which is intriguing in the context of a particular
manufacturing technique. Robin writes,

"It seems to me that the overall efficiency would be higher
if you just used
the electrons freed by the fission fragments directly [snip]
This avoids losses involved in producing coherent light, and
in transferring the energy of that light to free electrons."

At first, this idea seemed attractive but did not seem
possible in actual practice... at least not for the
situation were a high multiplication ratio in a subcritical
reactor must be maintained using only natural uranium. Even
if several pounds of hydrinos can be produced in situ per
day and an acceptable percentage of those result in virtual
neutrons, one would still need several thousand pounds of
unenriched uranium to achieve a high multiplication ratio.
How do you get that much uranium thin enough and still use
it as a cathode?

Here is the Energy (in MeV) distribution in typical fission
reactions

Kinetic energy of fission fragments    161 MeV
Prompt gamma                                         9
Kinetic energy of fission neutrons           8
Delayed Gamma  (fission products)       8
Beta decay of fission products                7
Antineutrinos                                              7

total
200 MeV per fission

The fission fragements are both around half the mass of the
original uranium, therfore even with about 80 MeV each, they
will not travel far in a solid fuel rod. I would suspect the
the free-path would be submicron. If one wanted to engineer
a situation where a substanial number of the fragments (or
at least the electrons displaced by them) were to be able
geometrically to actually exit the cathode of a thermionic
fuel rod, then the prospect looks hopeless... at first it
did anyway. How does one convert several thousand pounds of
natural uranium into a form thin enough but with structural
integrity for use in a thermionic situation at 2000 K or
higher ?

Here is a partial answer based upon a particular
manufacturing techniuqe... which is close to some which are
in use today in metal fabrication factories, but is not
itself exactly like anything which has been done before.
First, realize that pure U is very malleable and ductile,
bur very reactive with O2. It can be rolled as thin as
aluminum foil and stamped using common metal working
equipment so long as this is done in a very dry and O2
reduced environment. IOW it is difficult but not impossible.
It can then be easily anodized or nitrided into a very heat
resistent ceramic, using normal nitriding techniques. This
alos binds the layers into a structural unit. In mass
production, therefore, one can imagine that a tubular
cathode of U ceramic with a high porosity can be
manufactured ( 70-90 % porosity and not just random
porosity, but micro-channeled so that all the channels are
aligned radial to the fuel pipe axis.

It would involve rolling, stamping, stacking and annodizing
very thin disks of uranium robotically. The resulting
cathode pipe would have porous channels all radiating out
from the central axis in the direction of an accelerating
grid but OTOH it would also be a one-piece heat resistent
structural cathode.

What this might allow, in terms of added efficency could be
very promising... but who knows... The $64 question is - in
a geometry in which a high proportion of all fissions result
in the expelling of ballistic electrons, due to the kinetics
of the fission fragments, can this be highly efficent even
without high-probability coupling of the emitted electrons
to semi-coherent IR from the fuel pipe?

I don't think any of the garage experimenters on vortex are
equiped to find out the answer, but I wonder if the "not
invented here" syndrome extends all the way throught the
entrenched nuclear bureaucracy?

A curious note. Uranium is the second most dense element, so
even if it is manufactured in a form with a porous solid
with a gazzillion aligned microchannels, so that it has a
porosity of say 85% (IOW 85 percent open space and 15
percent cermet)  it will still be as dense as solid
aluminum.

Jones


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