Moggach Stephen A, Allan David R, Morrison Carole A, Parsons Simon, Sawyer Lindsay
School of Chemistry and Centre for Science at Extreme Conditions, The University of Edinburgh, King's Buildings, West Mains Road, Edinburgh EH9 3JJ, Scotland.
Acta Crystallogr B. 2005 Feb;61(Pt 1):58-68. doi: 10.1107/S0108768104031787. Epub 2005 Jan 19.
The crystal structure of L-serine has been determined at room temperature at pressures between 0.3 and 4.8 GPa. The structure of this phase (hereafter termed L-serine-I), which consists of the molecules in their zwitterionic tautomer, is orthorhombic, space group P212121. The least compressible cell dimension (c), corresponds to chains of head-to-tail NH...carboxylate hydrogen bonds. The most compressible direction is along b, and the pressure-induced distortion in this direction takes the form of closing up voids in the middle of R-type hydrogen-bonded ring motifs. This occurs by a change in the geometry of hydrogen-bonded chains connecting the hydroxyl groups of the -CH2OH side chains. These hydrogen bonds are the longest conventional hydrogen bonds in the system at ambient pressure, having an O...O separation of 2.918 (4) A and an O...O...O angle of 148.5 (2) degrees ; at 4.8 GPa these parameters are 2.781 (11) and 158.5 (7) degrees . Elsewhere in the structure one NH...O interaction reaches an N...O separation of 2.691 (13) A at 4.8 GPa. This is amongst the shortest of this type of interaction to have been observed in an amino acid crystal structure. Above 4.8 GPa the structure undergoes a single-crystal-to-single-crystal phase transition to a hitherto uncharacterized polymorph, which we designate L-serine-II. The OH...OH hydrogen-bonded chains of L-serine-I are replaced in L-serine-II by shorter OH...carboxyl interactions, which have an O...O separation of 2.62 (2) A. This phase transition occurs via a change from a gauche to an anti conformation of the OH group, and a change in the NCalphaCO torsion angle from -178.1 (2) degrees at 4.8 GPa to -156.3 (10) degrees at 5.4 GPa. Thus, the same topology appears in both crystal forms, which explains why it occurs from one single-crystal form to another. The transition to L-serine-II is also characterized by the closing-up of voids which occur in the centres of other R-type motifs elsewhere in the structure. There is a marked increase in CH...O hydrogen bonding in both phases relative to L-serine-I at ambient pressure.
已在室温下、0.3至4.8吉帕的压力范围内测定了L-丝氨酸的晶体结构。该相(以下称为L-丝氨酸-I)的结构由两性离子互变异构体中的分子组成,为正交晶系,空间群P212121。最难压缩的晶胞尺寸(c)对应于头对头NH…羧酸盐氢键链。最易压缩的方向沿b轴,该方向上压力诱导的畸变表现为R型氢键环基序中间的空隙闭合。这是通过连接-CH2OH侧链羟基的氢键链几何形状的变化而发生的。这些氢键是常压下该体系中最长的常规氢键,O…O间距为2.918(4)Å,O…O…O角为148.5(2)度;在4.8吉帕时,这些参数分别为2.781(11)和158.5(7)度。在结构的其他位置,一个NH…O相互作用在4.8吉帕时N…O间距达到2.691(13)Å。这是在氨基酸晶体结构中观察到的此类相互作用中最短的之一。在4.8吉帕以上,该结构经历单晶到单晶的相变,转变为一种迄今未表征的多晶型物,我们将其命名为L-丝氨酸-II。L-丝氨酸-I中OH…OH氢键链在L-丝氨酸-II中被较短的OH…羧基相互作用取代,O…O间距为2.62(2)Å。这种相变是通过OH基团从gauche构象变为anti构象以及NCalphaCO扭转角从4.8吉帕时的-178.1(2)度变为5.4吉帕时的-156.3(10)度而发生的。因此,两种晶体形式中出现了相同拓扑结构,这解释了为什么它会从一种单晶形式转变为另一种单晶形式。向L-丝氨酸-II的转变还表现为结构中其他位置的其他R型基序中心出现的空隙闭合。相对于常压下的L-丝氨酸-I,两个相中的CH…O氢键都有显著增加。