ENTHALPY, ENTROPY, AND STRUCTURAL RELAXATION BEHAVIORS OF A-DNA AND B-DNA IN THEIR VITRIFIED STATES AND THE EFFECT OF WATER ON THE DYNAMICSOF B-DNA

The A and B forms of NaDNA with hydration level of between 0.15 and 0. 64 (g of water)/(g of NaDNA) have been vitrified by cooling at rates b etween 4 and similar to 2700 K min(-1), and their thermal behavior on reheating was studied from similar to 120 to 300 K by differential sca nning calorimetry (DSC). The effects of the annealing time, t(a), for two different hydration levels at a fixed temperature and of the annea ling temperature, T-a, for a fitted t(a) have been investigated, and t he effects of various T-a and t(a) on the enthalpy and entropy relaxat ions and recovery were ascertained. From these effects we evaluate tau (a), the characteristic structural relaxation time, E, the activation energy, tau(0), the preexponential factor, and beta < 1 as an empiric al parameter for apparent distribution of relaxation times. No DSC fea tures of significance that may be attributed to the onset of molecular motions are found for A-DNA or when the water content is low, but for B-DNA and high water content, endothermic features resembling the ons et of molecular motions, or glass --> liquid transition, are observed from similar to 153 K to similar to 263 K. This corresponds to a slowe r increase in the heat capacity with temperature than is observed for most glass --> liquid transitions, and it is attributed to the sum of a large number of relaxation modes of different parts with closely spa ced single relaxation times. This is also seen as equivalent to a very broad distribution of structural relaxation times or of energy barrie rs separating the conformational and other substates corresponding to the various modes of local motions in a picture of multiple energy bar riers, These local modes of motions involve both DNA segments and the water attached to them. Annealing vitrified B-DNA at temperatures from similar to 153 K to similar to 263 K causes its structure's net energ y or enthalpy (and by implication its entropy) to decrease. The magnit ude of this decrease has been measured by using the DSC difference sca ns in which the enthalpy lost on annealing is recovered on reheating b ut at a temperature higher than that of annealing. This recovered enth alpy increases with t(a) according to the stretched exponential relati on, Delta H(t(a)) proportional to 1 - exp[-(t(a)/tau(a))(beta)]. tau(a ) seems to remain constant with t(a) but changes with T-a in much the same manner as for synthetic amorphous polymers. The peak temperature of the endotherm observed during the recovery of the lost enthalpy, T- p, also increases according to a relation, T-p(2) proportional to 1 - exp[-(t(a) tau(a))(beta)], with the same values of beta and tau(a) as for the increase in Delta H(t(a)). It is concluded that the molecular segmental motions of B-DNA and of the water attached to it are attribu table to a broad distribution of energy barriers between conformationa l substates.