Céolin René, Tamarit Josep-Lluis, Barrio Maria, López David O, Nicolaï Béatrice, Veglio Nestor, Perrin Marc-Antoine, Espeau Philippe
Department de Física i Enginyeria Nuclear, Laboratori de Caracterizació de Materials, ETSEIB, Diagonal 647, 08028 Barcelona, Catalunya, Spain.
J Pharm Sci. 2008 Sep;97(9):3927-41. doi: 10.1002/jps.21285.
The melt from the usual monoclinic phase (Phase I) of biclotymol (T(fusI) = 400.5 +/- 1.0 K, Delta(fus)H(I) = 36.6 +/- 0.9 kJ mol(-1)) recrystallizes into another phase, Phase II, that melts at T(fusII) = 373.8 +/- 0.2 K (Delta(fus)H(II) = 28.8 +/- 1.0 kJ mol(-1)). The transformation of Phase II into Phase I is found to be exothermic upon heating either as a direct process at 363 K or through a melting-recrystallization process (II --> liquid --> I). The melting curves, obtained from differential thermal analyses at various pressures ranging from 0 to 85 MPa, diverge as the pressure increases ((dP/dT)(fusI) = 2.54 +/- 0.07 MPa K(-1), (dP/dT)(fusII) = 5.14 +/- 0.85 MPa K(-1)). A topological P-T diagram with no stable phase region for Phase II, and similar to the 4th case of the P-T state diagrams formerly published by Bakhuis Roozeboom, is drawn, thus illustrating the overall monotropic behavior of Phase II.
比克罗托酚通常的单斜晶相(I相)(T(fusI)=400.5±1.0K,Δ(fus)H(I)=36.6±0.9kJ mol⁻¹)的熔体再结晶形成另一个相,即II相,其熔点为T(fusII)=373.8±0.2K(Δ(fus)H(II)=28.8±1.0kJ mol⁻¹)。发现II相转变为I相在加热时是放热的,无论是在363K作为直接过程还是通过熔化-再结晶过程(II→液体→I)。从0至85MPa的各种压力下的差示热分析获得的熔化曲线随着压力增加而发散((dP/dT)(fusI)=2.54±0.07MPa K⁻¹,(dP/dT)(fusII)=5.14±0.85MPa K⁻¹)。绘制了一个拓扑P-T图,其中II相没有稳定相区域,并且类似于Bakhuis Roozeboom先前发表的P-T状态图的第4种情况,从而说明了II相的整体单向行为。