A scaling theory and simulation results are presented for fragmentation of percolation clusters by random bond dilution. At the percolation threshold, scaling forms describe the average number of fragmenting bonds and the distribution of cluster masses produced by fragmentation.A relationship between the scaling exponents and standard percolation exponents is verified in one dimension, on the Bethe lattice, and for Monte Carlo simulations on a square lattice. These results further describe the structure of percolation clusters and provide kernels relevant to rate equations for fragmentation. The structure of percolation clusters has received considerable attention in recent years because of the desire to understand transport properties through random media.For this reason, much of the recent eA'ort has focused on the structure of clusters at and near the percolation threshold p, where the infinite cluster dominates the behavior of the system. In particular, the link, node, and blob picture of the infinite cluster has helped to clarify the conduction of electricity through random networks and the flow of water through random porous materials [3,4]. Since the backbone of the infinite cluster carries current across the cluster, the structure and connectivity of the backbone has been examined carefully [5][6][7].Comparatively little effort has been spent, however, on characterizing overall cluster connectivity, an important issue for fragmentation.In this spirit, we ask about the consequences of removing a bond of mass 1 from a percolation cluster of finite mass s, given by the number of bonds, at the percolation threshold p, . Is