The relaxation of helical structures very close to equilibrium is observed via transient 2D IR spectroscopy. An initial distribution of synthetically distorted helices having an unnatural bridge linking the 10th and 12th residues of an alanine-rich α-helix is released to evolve into the equilibrium distribution of α-helix conformations. The bridge constrains the structure to be slightly displaced from the full α-helix equilibrium near these residues, yet the peptide is not unfolded completely. The release is accomplished by a subpicosecond pulse of UV irradiation. The resulting 2D IR signals are used to obtain snapshots of the ∼100-ps helical conformational reorganization of the distorted dihedral angle and distance between amide units at chemical bond length-scale resolution. The decay rates of the angle between the dipoles, dihedral angles, and distance autocorrelations obtained from molecular dynamics simulations support the experiments, providing evidence that the final helix collapse conforms to linear response theory.synthetic peptides | tetrazines | helix dynamics T he concept of a rugged free energy surface and the mechanism of how a protein explores that space are longstanding questions (1-3) influencing all aspects of conformational dynamics, ranging from ligand exchange and enzyme activity to protein folding and unfolding. Although in principle one may imagine defining answers from molecular dynamics (MD) simulations to questions regarding specific local steps along such surfaces, there are few experimental approaches that can directly measure the time evolution of distributions of microscopic structural parameters throughout such explorations. Nonetheless, the dominant principles of protein dynamics are beautifully illustrated by an immense theoretical effort that was summarized (4) and exposed recently by experiments on ligand recombination dynamics (5-7), fluctuations in enzyme activity (8), singlemolecule FRET experiments (9, 10), and downhill folding (11), all of which measure some coarse-grained aspect of the microscopic fluctuations.The helix-coil transition is one of the most basic examples of peptide folding; therefore, considerable experimental and theoretical investigation already has been dedicated to investigating such structural searches (12-16). Qualitatively, helix formation is predicted to initiate from infrequently formed single-helix turn structures, which promote rapid development of the remaining turns of the helix (12-15, 17, 18). The equilibrium folding kinetics thus is dominated by the mean existence time of states that have failed to initiate. The current work provides a direct measure of a feature of α-helix conformation dynamics that is independent of the intrusive rate-determining nucleation period involved in helix folding. Prior helix folding experiments demonstrated that helix relaxation occurs with exponential time constants on the order of hundreds of nanoseconds, which may be affected by peptide length, temperature, viscosity, ionic strength, and steric effects of sid...