We address the stability of multicharged finite systems driven by Coulomb forces beyond the Rayleigh instability limit. Our exploration of the nuclear dynamics of heavily charged Morse clusters enabled us to vary the range of the pair potential and of the fissibility parameter, which results in distinct fragmentation patterns and in the angular distributions of the fragments. The Rayleigh instability limit separates between nearly binary (or tertiary) spatially unisotropic fission and spatially isotropic Coulomb explosion into a large number of small, ionic fragments. Implications are addressed for a broad spectrum of dynamics in chemical physics, radiation physics of ultracold gases, and biophysics, involving the fission of clusters and droplets, the realization of Coulomb explosion of molecular clusters, the isotropic expansion of optical molasses, and the Coulomb instability of ''isolated'' proteins.T he fragmentation of multiply charged finite systems driven by long-range Coulomb forces (1-33) or their analogue (34), i.e., nuclei (1-4), clusters (5-29), droplets (30-33), and optical molasses (34), raises some interesting questions regarding the energetics and dynamics of dissociation. How does a finite system respond to a large excess charge (1-33) or effective charge (34)? What are the topography and topology of the multidimensional energy landscape (4, 35) that guide the system's shape evolution and fragmentation? What are the fragmentation channels and under what conditions are they realized? What is the interplay between fission, i.e., instability toward dissociation, of the finite system into two (or a small number of) fragments and Coulomb explosion (17-29) into a large number ϳn (where n is the number of constituents) of ionic species? On the basis of molecular dynamics simulations of the fragmentation patterns of heavily charged Morse clusters we established that the Rayleigh instability limit (30) separates between nearly binary (or tertiary) spatially unisotropic fission and spatially isotropic Coulomb explosion into a large number of ionic fragments.The ubiquity of fission phenomena of droplets (30-33), nuclei (1-4), and clusters (5-16) was traditionally described by the liquid drop model (LDM) of Lord Rayleigh (30), Meitner and Frisch (2), and Wheeler and Bohr (1), where a classical charged drop deforms through elongated shapes to form separate droplets. The fissibility parameter X ϭ E(Coulomb)͞2E(surface) characterizes the relative contribution of repulsive (Coulomb) and cohesive (surface) energies to the fission barrier, separating between the bound initial states and the fission products. For X Ͻ 1, thermally activated fission over the barrier prevails. At the Rayleigh instability limit of X ϭ 1, the barrier height is zero (1, 30). Many features of nuclear and metal cluster fission go beyond the physics of a classical liquid droplet and require the incorporation of quantum shell structure and dynamics (4, 10). Nevertheless, the simple LDM expression X ϭ Z 2 e 2 ͞16␥R 3 ϭ (Z 2 ͞n)͞(Z 2 ͞n) cr w...