The elastic interactions between dislocations in a finite lamellar sys
tem of N layers are calculated as a function of the size of the system
, surface tension and lamellar elastic constants. For large surface te
nsion the in-plane interactions are repulsive for like dislocations an
d attractive for opposite ones, decaying exponentially with the decay
length proportional to square-root N. Their strength is inversely prop
ortional to square-root N. For small surface tension the elastic inter
actions are attractive at large distances for like dislocations and re
pulsive for opposite ones. In thin films with small surface tension li
ke dislocations are stabilized at finite separations (approximately sq
uare-root N), while in thick films they unbind due to Helfrich forces.
The unbinding transition is extremely sensitive to the surface tensio
n and surface bending elastic constant.