The presence of macromolecules in cells geometrically restricts the available space for poplypeptide chains. To study the effects of macromolecular crowding on folding thermodynamics and kinetics, we used an off-lattice model of the all-β-sheet WW domain in the presence of large spherical particles whose interaction with the polypeptide chain is purely repulsive. At all volume fractions, ϕ c , of the crowding agents the stability of the native state is enhanced. Remarkably, the refolding rates, which are larger than the value at ϕ c = 0, increase nonmonotonically as ϕ c increases, reaching a maximum at [12pt]{minimal} {amsmath} {wasysym} {amsfonts} {amssymb} {amsbsy} {mathrsfs} {}{-69pt} {document} {equation*}{φ}_{{c}}={φ}_{{c}}*{equation*}{document} . At high values of ϕ c , the depletion-induced intramolecular attraction produces compact structures with considerable structure in the denatured state. Changes in native state stability and folding kinetics at ϕ c can be quantitatively mapped onto confinement in a volume-fraction-dependent spherical pore with radius R s ≈ (4π/3ϕ c ) 1/3 R c ( R c is the radius of the crowding particles) as long as [12pt]{minimal} {amsmath} {wasysym} {amsfonts} {amssymb} {amsbsy} {mathrsfs} {}{-69pt} {document} {equation*}{φ}_{{c}}{≤}{φ}_{{c}}*{equation*}{document} . We show that the extent of native state stabilization at finite ϕ c is comparable with that in a spherical pore. In both situations, rate enhancement is due to destabilization of the denatured states with respect to ϕ c = 0.
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Cheung et al. (2005) studied this question.
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