The normal mode spectrum for the linearized MHD equations is investiga
ted for a simple cylindrical equilibrium. This spectrum is examined fo
r zero and non-zero scalar resistivity. Particular attention is paid t
o the thermal sub-spectrum. It is shown that when resistivity is inclu
ded, a 'dissipative' layer forms at the location of the singularity as
sociated with the thermal continuum. For the most unstable 'quasi-cont
inuum modes', the thickness of this dissipative layer is proportional
to the 1/4 power of the magnetic Reynolds number. This generates lengt
h scales that are of the same order of magnitude as those reported for
the fine-scale structure seen in prominences. It is therefore conclud
ed that dissipation due to resistivity may be relevant for the formati
on of prominence fine-scale structure.