Recent observations of the X-ray and EUV emission of non-supergiant B
stars are summarised. As compared with O stars, the X-rays of most of
the near-main-sequence B stars are soft, and the stars show a departur
e from the L(x) = 10(-7) L(bot) relation. Using line driven wind model
s to provide an estimate of the density distribution, it is concluded
that a major fraction of the wind emission measure is hot, whereas in
shocked wind theory less than 10 percent of the wind emission measure
should be hot. The X-ray observations suggest that all of the B stars
are X-ray emitters with a basal X-ray luminosity of about 10 10(-8.5)
L(bol). A hard component dominates the X-ray emission of tau Sco, and
possible causes are discussed. For the Be stars, the X-ray emission is
that which is expected from a normal B-star wind coming from the pole
s, as in the Wind Compressed Disk (WCD) model of Be stars. None of the
stars, including the beta Cep stars, show noticeable variability in t
heir X-rays. EUVE observations of epsilon CMa B2 II, find it to be the
brightest object in the EUV sky at 500 to 700 A. It shows a Lyman con
tinuum flux that is a factor of 30 higher than line blanketed model at
mospheres. The continuum is seen on both sides of the He I 504 Angstro
m edge, and the discrepancy with model atmospheres is even greater sho
rtward of 504 Angstrom. The EUVE spectra show emission lines both from
high stages of ionization (Fe IX to Fe XVI) and from low stages (HeII
and O III). The He II Lyman alpha results from recombination followin
g X-ray photoionization in the wind, and the O III resonance line is f
ound to be present because of the Bowen fluorescence mechanism. Thus,
there is and interesting coupling between the wind production by the E
UV photospheric emission, the production of X-ray and line EUV emissio
n by winds, and the production of fluorescence by recombination in the
wind; all of these processes are now observable in B stars.