  We calculate the Lamb, fine and hyperfine shifts in $b\bar b$ with $n=2$,
$l=0,1$. Radiative corrections as well as leading nonperturbative corrections
(known to be due to the gluon condensate) are taken into account. The
calculation is parameter-free, as we take $\Lambda$, ${\langle \alpha_s G^2
\rangle}$ from independent sources. Agreement with experiment is found at the
expected level $\sim 30\%$. Particularly interesting is a prediction for the
hyperfine splitting, $M_{\rm average}(2^3P)-M(2^1P_1) = 1.7 \pm 0.9\, {\rm
MeV}$, opposite in sign to the $c\bar c$ one ($\approx -0.9\, {\rm MeV}$), and
where the nonzero value of ${\langle \alpha_s G^2 \rangle}$ plays a leading
role.
