A simple model is presented to account for the Yohkoh Rare observation
s of Feldman et al. (1994), and Masuda (1994). Electrons accelerated b
y the flare are assumed to encounter the dense, small regions observed
by Feldman et al, at the tops of impulsively flaring coronal magnetic
loops. The values of electron density and volume inferred by Feldman
et al. imply that these dense regions present an intermediate thick-th
in target to the energised electrons. Specifically, they present a thi
ck (thin) target to electrons with energy much less (greater) than E(c
) where 15 keV < E(c) < 40 keV. The electrons are either stopped at th
e loop top or precipitate down the field lines of the loop to the foot
points. Collisional losses of the electrons at the loop top produce th
e heating observed by Feldman et al. and also some hard X-rays. It is
argued that this is the mechanism for the loop-top hard X-ray sources
observed in limb flares by Masuda. Adopting a simple model for the ene
rgy losses of electrons traversing the dense region and the ambient lo
op plasma, hard X-ray spectra are derived for the loop-top source, the
footpoint sources and the region between the loop top and footpoints.
These spectra are compared with the observations of Masuda. The model
spectra are found to qualitatively agree with the data, and in partic
ular account for the observed steepening of the loop-top and footpoint
spectra between 14 and 53 keV and the relative brightnesses of the lo
op-top and footpoint sources.