Activated processes are of central importance to many biochemical phenomena, including ligand binding and enzyme catalysis [1,2]. A simple model for such processes, provided by the rotation ('flipping') of' aromatic amino acid sidechains in the interior of globular protein has been studied intensively by experimental [3][4][5][6][7][8] and theoretical techniques [9][10][11][12]. Energy minimization [9,10] and activated trajectory [11,12] calculations have demonstrated that the nature of the rotational transition and its effective barrier are determined by the positions and fluctuations of the protein matrix atoms surrounding the aromatic ring. The importance of frictional effects for the ring motion and for other processes involving fluctuations in the protein interior has been pointed out [11][12][13][14][15].Recently, Wagner [ 16,17] has determined the hydrostatic pressure dependence of the aromatic ring rotation rates in the bovine pancreatic trypsin inhibitor (PTI). Over the measured range (1-1200 atm), interpretation of the rate data for two of the rings (Phe 45 and Tyr 35) in terms of transition state theory [ 18 ]:yielded activation volumes, At/C, of about 50 A3; the positive sign of A l/~ corresponds to a decrease of the rate with increasing pressure. The observed magnitude of the activation volume, on the order of that associated with protein denaturation [19,20], provides an important test for the theoretical interpretation of the ring rotation process given previously [9][10][11][12]. For motion in the interior of a protein, as for solution reactions [21] in general, the pressure dependence of the rate constant is not related directly to a physical volume change between the reactant and transition state. Instead, it can be dominated by the interactions between the reacting species and the solvent environment, which in the case of the ring rotations is provided by the surrounding protein atoms. To analyze the factors involved, we make use of the Kramers formulation for an activated process in the diffusive limit [21][22][23][24]; this is an approximation since dynamical calculations [ 11,12] suggest that the ring motion is in the intermediate damping regime [22,23]. Considering the ring flipping as a one-dimensi0nal problem defined by the ring rotation angle, we can write the rate constant as [24]:where J is the effective activation enthalpy, ~i and ~ts are the vibrational frequencies in the initial well and at the top of the inverted barrier, respectively, and fr and I r are the rotational friction coefficient and moment of inertia of the aromatic ring. Previous studies have shown that except for the moment of inertia, all of the parameters in eqn 2 are determined by interactions between the aromatic ring and the surrounding protein matrix; the intrinsic torsional potential of the ring is negligible [9][10][11][12]. Since compression of the protein will tend to decrease the distances between the ring and the matrix atoms, a pressure dependence for the rate constant is expected from eqn 2. The changes...