Understanding the effects of confinement on protein stability and folding kinetics is important for describing protein folding in the cellular environment. We have investigated the effects of confinement on two structurally distinct proteins as a function of the dimension d c and characteristic size R of the confining boundary. We find that the stabilization of the folded state relative to bulk conditions is quantitatively described by R ؊␥ c, where the exponent ␥c is Ϸ5/3 independent of the dimension of confinement dc (cylindrical, planar, or spherical). Moreover, we find that the logarithm of the folding rates also scale as R ؊␥ c, with deviations only being seen for very small confining geometries, where folding is downhill; for both stability and kinetics, the dominant effect is the change in the free energy of the unfolded state. A secondary effect on the kinetics is a slight destabilization of the transition state by confinement, although the contacts present in the confined transition state are essentially identical to the bulk case. We investigate the effect of confinement on the position-dependent diffusion coefficients D(Q) for dynamics along the reaction coordinate Q (fraction of native contacts). The diffusion coefficients only change in the unfolded state basin, where they are increased because of compaction. macromolecular crowding ͉ course-grained simulation ͉ energy landscape ͉ diffusion P rotein folding in the cell occurs in a crowded, heterogeneous environment, a perturbation that may alter both the thermodynamics and kinetics of folding relative to observations made in dilute solutions. Experimental and theoretical studies have shown that effects arising from excluded volume interactions either due to macromolecular crowding (1-15) or localization (confinement) of the protein in a small volume (16-31), such as the ribosome tunnel (32) or a chaperonin cavity (33-35), can indeed have significant effects on folding. In the limit where the crowding particles are much bigger and heavier than the protein, the macromolecular crowding effects can be approximated by confinement; the shape and dimensions of the cavity will depend on the crowding concentration. This approach was shown to be applicable for a range of conditions in an insightful study by Cheung, Klimov, and Thirumalai (9). Specifically, they showed that the effect of crowding on protein-folding kinetics can be mimicked by confining the protein within a spherical cavity. The effect of crowding at low concentrations will be different from encapsulation in a spherical cavity and may be better represented by the weaker confining environment within a cylinder or between two planes. Because all of these confinement configurations may also appear naturally (e.g., cylindrical confinement for protein passage through a ribosome tunnel and planar confinement for proteins at interfaces or near surfaces), it is instructive to study the effects of varying the reduced dimensions due to confinement (d c ϭ 1, 2, and 3 for planar, cylindrical, and spherical...