We study the existence and stability of spherical membranes in curved
space-times. For Dirac membranes in the Schwarzschild-de Sitter backgr
ound we find that there exists an equilibrium solution. By fine-tuning
the dimensionless parameter Lambda M(2), the static membrane can be a
t any position outside the black hole event horizon, even at the stret
ched horizon, but the solution is unstable. We show that modes having
l = 0 (and for Lambda M(2) < 16/243 also l = 1) are responsible for th
e instability. We also find that spherical higher order membranes (mem
branes with extrinsic curvature corrections), contrary to what happens
in flat Minkowski space, do have equilibrium solutions in a general c
urved background and, in particular, also in the ''plain'' Schwarzschi
ld geometry (while Dirac membranes do not have equilibrium solutions t
here). These solutions, however, are also unstable. We shah discuss a
way of bypassing these instability problems, and we also relate our re
sults to the recent ideas of representing the black hole event horizon
as a relativistic bosonic membrane.