The variable-coefficient two-dimensional Korteweg-de Vries (KdV) model is of considerable significance in describing many physical situations such as in canonical and cylindrical cases, and in the propagation of surface waves in large channels of varying width and depth with nonvanishing vorticity. Under investigation hereby is a generalized variable-coefficient two-dimensional KdV model with various external-force terms. With the extended bilinear method, this model is transformed into a variable-coefficient bilinear form, and then a Bäcklund transformation is constructed in bilinear form. Via symbolic computation, the associated inverse scattering scheme is simultaneously derived on the basis of the aforementioned bilinear Bäcklund transformation. Certain constraints on coefficient functions are also analyzed and finally some possible cases of the external-force terms are discussed. Among the most important models of nonlinear evolution equations (NLEEs), constant-coefficient Korteweg-de Vries (KdV) and KdV-type equations are encountered in many apparently unrelated phenomena in different physical areas such as shallow water waves, plasmas, fluids and lattice vibrations of a crystal at low temperatures [1]. In all of these applications, the physical situations described via the KdV (or KdVtype) models tend to be highly idealized, owing to the assumption of constant coefficients. Considering the inhomogeneities of media, nonuniformities of boundaries and external forces, the variable-coefficient models are much more powerful and realistic than their constant-coefficient counterparts in describing various 0932-0784 / 09 / 0300-0222 $ 06.00 c 2009 Verlag der Zeitschrift für Naturforschung, Tübingen · http://znaturforsch.com situations, e. g., in the coastal waters of oceans, space and laboratory plasmas, superconductors and opticalfiber communications [2 -6].In the past decades, it has been shown that various physical phenomena in nature, actual physics and engineering can be described by the variable-coefficient KdV model with perturbed, dissipative and externalforce terms as [7] where v(x,t) is a function of the variables x and t, µ 1 (t) = 0, µ 2 (t) = 0, µ 3 (t), µ 4 (t) and µ 5 (t) represent the coefficients of the nonlinear, dispersive, dissipative, perturbed and external-force terms, respectively, all of which are real functions. In recent studies, of physical and mechanical interests, many important examples of (1), among others, can be listed [8]:Unauthenticated Download Date | 5/8/18 5:12 AM