Human POT1 Unfolds G-Quadruplexes by Conformational Selection

The reaction mechanism by which shelterin protein POT1 (Protection of Telomeres) unfolds human telomeric G-quadruplex structures is not fully understood. We report here kinetic, thermodynamic, hydrodynamic and computational studies that show that a conformational selection mechanism, in which POT1 binding is coupled to an obligatory unfolding reaction, is the most plausible mechanism. We show that binding of the single-strand oligonucleotide d[TTAGGGTTAG] to POT1 is fast, with an apparent relaxation time of 80.0 {+/-} 0.4 ms, and strong, with a binding free energy of -10.1 {+/-} 0.3 kcal mol-1. That favourable free energy arises from a large favourable enthalpy contribution of -38.2 {+/-} 0.3 kcal mol-1. In sharp contrast, the binding of POT1 to an initially folded 24 nt G-quadruplex structure is slow, with an average relaxation time of 2000-3000 s. Fluorescence, circular dichroism and analytical ultracentrifugation studies show that POT1 binding is coupled to quadruplex unfolding with a final stoichiometry of 2 POT1 molecules bound per 24 nt DNA. The binding isotherm for the POT1-quadruplex binding interaction is sigmoidal, indicative of a complex reaction. A conformational selection model that includes equilibrium constants for both G-quadruplex unfolding and POT1 binding to the resultant single-strand provides an excellent quantitative fit to the experimental binding data. The overall favourable free energy of the POT1-quadruplex interaction is -7.1 kcal mol-1, which arises from a balance between unfavourable free energy of +3.4 kcal mol-1 for quadruplex unfolding and a large, favorable free energy of -10.5 kcal mol-1 for POT1 binding. We show that POT1 can unfold and bind to any conformational form of human telomeric G-quadruplex (antiparallel, hybrid or parallel), but will not interact with duplex DNA or with a parallel G-quadruplex structure formed by a c-myc promoter sequence. Finally, molecular dynamics simulations provide a detailed structural model of a 2:1 POT1:DNA complex that is fully consistent with experimental biophysical results.