We consider an important class of self-assembly problems, and using the formalism of stochastic thermodynamics, we derive a set of design principles for growing controlled assemblies far from equilibrium. The design principles constrain the set of configurations that can be obtained under nonequilibrium conditions. Our central result provides intuition for how equilibrium self-assembly landscapes are modified under finite nonequilibrium drive.self-assembly | nonequilibrium self-assembly | pattern formation | stochastic thermodynamics | second law of thermodynamics T he fields of colloidal and nanoscale self-assembly have seen dramatic progress in the last few years. Indeed experimental and theoretical work has elucidated design principles for the assembly of complex 3D structures (1-4). Most of these advances, however, are based on an equilibrium thermodynamic framework: the target configuration minimizes a thermodynamic free energy (5). Understanding the principles governing self-assembly and organization in far-from equilibrium systems remains one of the central challenges of nonequilibrium statistical mechanics (6-13). In this report, we show that design principles can be derived for a broad class of nonequilibrium driven self-assembly processes. Our central result constrains the set of possible configurations that can be achieved under a nonequilibrium drive.Imagine a self-assembly process in which interactions among the various monomers are described by a set of energies E eq . The ratio of association and dissociation rates is set by a combination of interaction energies and chemical potentials {. . . µi . . .} of the monomers. This generic setup is sufficient to describe many selfassembly processes. Examples include growth of crystals from solution by nucleation (9), growth dynamics of cell walls (14), growth of multicomponent assemblies (4), and growth dynamics of biological polymers and filaments (15). The chemical potential controls the growth of the assembly. If the chemical potential is tuned to a coexistence value such that the assembly grows at an infinitesimally slow rate, then the configuration of the assembly can be predicted by computing the equilibrium partition function and free energy G eq appropriate to the set of interaction energies. For values of the chemical potentials more favorable than the coexistence chemical potential, the assembly grows at a nonzero rate. In such instances, the growing assembly might not have sufficient time to relax to values characteristic of the equilibrium partition function (9,16,17). Defects are accumulated as the assembly grows at a nonzero rate. The time taken for a defect to anneal increases rapidly with distance from the interface of the growing configuration. Due to the resulting kinetically trapped states, the crystal can assume configurations very different from those representative of the equilibrium state (9,16,17).By applying the second law of thermodynamics and the formalism of stochastic thermodynamics, we derive a surprising thermodynamic relati...