1.2 Dynamic Flexibility

The dynamics of the transition from the t to g- and g+ states is determined by the activation barrier separating them, ΔE. In analogy to the structural or spatial counterpart, we may think in terms of a persistence time, τp

τp = τ0exp(ΔE ∕kT)
(2)

where τ0 is an attempt frequency.

On timescales smaller than τp (at high frequencies, ω > 1∕τp), the chain looks inflexible - its conformation doesn’t change.
On longer timescales, or smaller frequencies, the chain appears flexible as it is able to sample many different conformational states during the time of observation.