Abstraet. Molecular dynamics of three derivatives of 1,2,4-benzothiadiazine-l,l-dioxide, hydrochlorothiazide (HCTZ), althiazide (ATZ) and chlorotbiazide (CTZ), was studied by 35C1 nuclear quadrupole resonance (NQR) spectroscopy. The temperature dependence of the resonance frequency was analyzed within the 6 known standard models. The activation energies estimated from the temperature dependence of the 3~C1 NQR frequency assuming the Bayer model were 1.07, 2.35 and 2.76 kJ/mot for HCTZ, ATZ and CTZ respectivety, wbich confirms that HCTZ is Iess rigid than CTZ and ATZ is much more rigid than HCTZ, and suggests that the mechanism of relaxation is based on small amplitude librations. The characteristic temperatures estimated from the Bayer model, with that for CTZ (332.5 K) being much higher than for HCTZ (132.1 K), mean that the intermolecular interactions in CTZ are much stronger than in HCTZ, as suggested by the melting point of CTZ being higher than that for HCTZ. For ATZ the characteristic temperature (288 K) takes an intermediate value, which suggests that the intermolecular interactions in this compound are stronger than in HCTZ and weaker than in CTZ. A significant narrowing of the resonance 3~C1 NQR line observed for all these compounds at room temperature, relative to that at the liquid nitrogen temperature, suggests an averaging of dipolar interactions asa result of fast rotation of nonquadrupole nuclei in the vicinity of the quadrupote nuclei, when 2nv~r~ 87 1 (a rotation of the -NH z group in the direct neighborhood of the chlorine nuclei) or a change in the gradient o¡ with its value preserved (which is equivalent to rotation of the quadrupole nucleus CI). The influence of the rotations of the -NH~ and -CH2SCH2CH=CH z groups (ATZ) or -CHCI z group (TCTZ) on the 3~C1 NQR frequency was modelled by the B3LYP/6-31G" method. The frequencies of the libration vibrations calculated from the temperature dependence of the NQR resonance frequency were compared with experimental ones and those implied by the density functional theory, infrared and Raman spectra. For HCTZ the anomalies in the temperature dependence of the 35C1 NQR frequency, the lack of hysteresis and small but notable changes in the slope and the jump in the frequency observed at 253 K which does not exceed 0.05 MHz suggest a second-order phase transition at 253 K.