. Can. J. Chem. 52, 2421 (1974).Wide line n.m.r. studies of the n-alkylammonium chlorides C,,-C,,show a nonreversible behavior which parallels that observed using differential scanning calorimetry. For samples which have been heated above the nonreversible transition the temperature dependence of the line width and second moment resemble that of the shorter chain compounds of this series: one transition due to the onset of chain rotation and a second higher temperature transition due to more extended motion probably of a translational nature. A change in crystal structure is proposed in order to explain the nonreversibility. Chem. 52, 2421Chem. 52, (1974.Les etudes de la bande large en r.ni.n. des chlorures de ti-alkylanimoni~~n~ C,,--C,, montrent un comporternent non-reversible qui est du meme type que celui observe par calorimetrie a balayage differentiel. La dependance de la largeur de bande et du moment secondaire par rapport a la ternperat~ire pour les echantillons chauffks au-dessus de la transition non-reversible resemble a ce qui a etC observe pour les co~nposes a chaine plus courte de cette serie: une premiere transition est due au debut de rotation de la chaine et Line deuxieme est d~~e a un mouveinent plus developpe probablement de nature translationnelle. On propose un changelnent dans la structure cristalline en vue d'expliquer la non-reversibilite.[Traduit par le joitrnal] Introduction Fragmentary evidence for the existence of solid-solid phase transitions in the homologous series of n-alkylammonium halides has existed for inany years but there have been few systematic investigations of the nature of these transitions (1-3). The reported X-ray structural studies are limited almost entirely to room temperature measurements of the (001) long spacings (4-8), and only n-propyl-and npentylamnioniu~i~ chlorides (9, 10) and t1-dodecylamrnoni~~m bromide (7) appear to have been s t~~d i e d in any greater detail. In general the chlorides are tetragonal up to a chain length of about 10 carbon atoms and either monoclinic (C,,,C,,,C,,,C,,) or orthorhombic (C, ,,C,,) thcreafter. Differential scanning calorimetric (d.s.c.) studies (2) showed that several thermal transitions exist for each co~npound and that these occur below room temperature for chain lengths up to C, and abo\e room temperature for the longer members of the series. On the basis of this evidence it seems orobable tha: one of the thermal transitions involves a change from, at low temperature, a monoclinic or orthorhombic forin to a tetragonal structure at higher temperature. Such a transition has been