We study theoretically the dewetting of a liquid film intercalated bet
ween a flat solid and a weakly crosslinked rubber. The rubber is chara
cterised by a static shear modulus, mu(0) a high frequency modulus, mu
(infinity)(>>mu 0) and a relaxation time, T. The film dewets by nuclea
tion and growth of a dry contact zone (radius R(t) at time i) surround
ed by a liquid rim collecting the liquid. We expect three regimes: a)
at short times (R < R-c1), the rubber behaves like a hard elastic soli
d (mu = mu(infinity)) and the dissipation is dominated by the liquid r
im. We call this fast elastic dewetting. b) at intermediate times (R-c
1 < R < R-c2), the rubber behaves like an ultra-viscous liquid. We cal
l this ''mixed viscous dewetting'' because both components dissipate.
c) at long times (R > R-c2) the rubber behaves like a soft solid (mu =
mu(0)) and the liquid dissipation is again dominant. We call this slo
w elastic dewetting.