We propose a theory for the penetration depth (T) of superconducting bilayers and multilayers, which are composed of two dissimilar superconducting layers S and SЈ with arbitrary coupling strength, and with the S layer thickness (T c,S ϾT c,S Ј ) less than or comparable to its coherence length. Within the framework of the theory, we discuss the influences of the SЈ layer parameters, and of the coupling strength between the SЈ and S layers. We show that their variations lead to a variety of temperature dependences of (T). Many of the basic features observed experimentally in conventional SSЈ structures have been reproduced. The theory begins with an extension of the proximity-effect model developed by Golubov et al. ͓Phys. Rev. B 51, 1073 ͑1995͔͒, which is based on the Usadel equations. It therefore applies to the dirty SSЈ system, and provides a description of the superconducting properties over the entire temperature range below T c , the transition temperature of the system. We shall compare our model with a phenomenological model developed within the proximity-effect theory which is applicable near T c . A brief discussion on the highly anisotropic systems in connection with the intrinsically layered high-T c superconductors is also presented.