Consider heat transfer in fission and fusion re-
actors. In today’s typical light-water reactor
(LWR), there is generated by fission in fuel
pins containing uranium. The heat is then
transferred to the coolant at the surfaces of a
relatively large number of small diameter pins.
This arrangement provides a larger surface area
to transfer heat than, say, a single large fuel cyl-
inder. Indeed, by decreasing the diameter of
the pins even further (but increasing their
number to keep the amount of uranium un-
changed), the total surface area available to
transfer heat would be further increased. Thus,
the actual heat-transfer rate through any given
square inch of surface on a fuel rod is not criti-
cal. Suffcient heat can always be removed
merely by increasing the total area.
This strategy does not work in a fusion reactor.
The heat-transfer surface is limited to the in-
side of the wall surrounding the plasma, and
the relatively small surface area of this wall
cannot be increased without further increasing
the size of the reactor. In fact, bigger reactors
need larger heat-transfer rates. Thus, the actual
heat-transfer rate per square inch must be ex-
tremely large and cannot simply be reduced by
a design change.
Suppose a fission reactor and a fusion reactor
were built with equivalent heat-transfer rates.
Knowing this, one can calculate two other
critical engineering factors: the flux of neu-
trons at the heat-transfer surface, and the
overall power density of the reactor. The neu-
tron flux should, of course, be as low as possi-
ble, because it damages the reactor structure
and makes it radioactive. And the power den-
sity should, as mentioned, be as high as possi-
ble, so that a reasonable amount of power will
be produced in a reactor of a given size.
On these counts, a comparison between cur-
rent LWR fission reactors and the somewhat
optimistic fusion designs produced by the
DOE studies yields a devastating critique of
fusion. For equal heat-transfer rates, the criti-
cal inner wall of the fusion reactor is subject to
ten times greater neutron flux than the fuel in
a fission reactor. Worse, the neutrons striking
the first wall of the fusion reactor are far more
energetic — and thus more damaging — than
those encountered by components of fission
reactors. ...