Deuterons are bosons and as such, under proper conditions, will Bose c
ondense. A configuration which permits this phenomenon is described in
which deuterons are weakly bound at interstitial sites of the metal p
alladium. It is argued that at a moderate value of the deuterium-to-pa
lladium concentration ratio, a magnetically driven current in a single
-crystal loop of this material will become ''class B'' superconducting
at the critical temperature, T(c), where ''class B'' denotes heavy-bo
son charge flow. Two distinct regimes are examined in which the deuter
on kinetic energy, E, is large or small compared to the activation ene
rgy, E(a). In the domain E< E(a), stemming from the London criterion f
or Bose-condensation and the tunneling matrix element, an expression f
or T(c) is obtained which, for deuteron propagation in palladium, is n
oted to be infinitesimally small, rendering the proposed phenomenon un
feasible. In the domain E > E., first-order estimates of the nearly-fr
ee-particle model, together with the London criterion, give the critic
al value T(c) almost-equal-to 9.1 K. It is shown that the condition E
> E(a) may be established for sufficiently short rise time of an impos
ed magnetic field. A calculation is included which indicates that at t
hese low temperatures, phonon effects in the present model are minimal
. Metallurgical limitations on obtaining a single-crystal loop of pall
adium, with the fcc structure continuously maintained, imply the condi
tion rho greater-than-or-equal-to 1.75 X 10(3)b, where rho is the radi
us of curvature of the palladium current loop and b is its diameter.