Enantiomer crystal structures

While wild-type PAMO was unable to convert 2-phenylcyclohexanone efficiently, all deletion mutants readily accepted this ketone as substrate. All mutants also displayed a similar thermostability when compared with the parent enzyme. The most active mutant (deletion of S441 and A442) was used for examining its enantioselective properties. It was found that the mutant preferably formed the (/ )-enantiomer of the corresponding lactone E = 100). While CHMO also shows a similar enantioselective behavior, this PAMO deletion mutant is a better candidate for future applications due to its superior stability. This clearly demonstrates that PAMO can be used as parent enzyme to design thermostable BVMO variants. It also illustrates that the available crystal structure of PAMO will be of great help for BVMO redesign efforts. ... 

P212121 Z = 8 Dx = 1.419 R = 0.068 for 1,373 intensities. The crystal structure contains two symmetry-independent molecules having slightly different conformations. The pyranoside conformations are 1C4 with Q = 57,60 pm, 0=173,177°. The nitro and acetate groups are oriented approximately normal to the mean plane of the pyranoside ring. The atomic coordinates refer to the d enantiomer. The hydrogen-atom positions were not reported. 

C16H2207 l,5-Anhydro-2,3,4-tri-0-benzoylxylitol (ATBXYL10)114 PI Z = 2 Dx = 1.32 R = 0.053 for 3,536 intensities. The crystal structure contains centrosymmetrically related d and l enantiomers. The pyranoid conformation is an almost ideal (d) [1C4(l)]i withQ = 60 pm, 0=1°, with normal bond-lengths and valence-angles. The benzoyl groups are equatorial, with their planes approximately normal to the mean plane of the pyranoid ring. 

X-Ray crystal structural studies32) (Fig. 13 and Scheme 8 which refers to the crystal structure) showed that one molecule of 93 is held in a fixed conformation determined by two hydrogen bonds and by neighboring host molecules which prevent free rotation about the CO—CO single bond in 93. Free rotation about this bond would enable the production of the two possible enantiomers. The fixed conformation of the guest molecule by the chiral host molecule causes the least molecular motion during the photocyclization reaction and the high enantioselectivity. 

Crystals composed of the R and S enantiomers of the same racemic mixture must be related by mirror symmetry in terms of both their internal structure and external shape. Enantiomorphous crystals may be sorted visually only if the crystals develop recognizable hemihedral faces. [Opposite (hid) and (hkl) crystal faces are hemihedral if their surface structures are not related to each other by symmetry other than translation, in which case the crystal structure is polar along a vector joining the two faces. Under such circumstances the hemihedral (hkl) and (hkl) faces may not be morphologically equivalent.] It is well known that Pasteur s discovery of enantiomorphism through die asymmetric shape of die crystals of racemic sodium ammonium tartrate was due in part to a confluence of favorable circumstances. In the cold climate of Paris, Pasteur obtained crystals in the form of conglomerates. These crystals were large and exhibited easily seen hemihedral faces. In contrast, at temperatures above 27°C sodium ammonium tartrate forms a racemic compound. 

Finally, reference must be made to the important and interesting chiral crystal structures. There are two classes of symmetry elements those, such as inversion centers and mirror planes, that can interrelate. enantiomeric chiral molecules, and those, like rotation axes, that cannot. If the space group of the crystal is one that has only symmetry elements of the latter type, then the structure is a chiral one and all the constituent molecules are homochiral the dissymmetry of the molecules may be difficult to detect but, in principle, it is present. In general, if one enantiomer of a chiral compound is crystallized, it must form a chiral structure. A racemic mixture may crystallize as a racemic compound, or it may spontaneously resolve to give separate crystals of each enantiomer. The chemical consequences of an achiral substance crystallizing in a homochiral molecular assembly are perhaps the most intriguing of the stereochemical aspects of solid-state chemistry. 

The crystals of both compounds contain pairs of (A)- and (A)-enantiomers. Selected geometric parameters for 88 and 89 are listed in Table XIV. Similar crystal structures were observed for the corresponding oxygen analogs 53 and 77, respectively (see Sections III,D and III, E). As can be seen from the Si-O [1.7600(14)-1.815(4) A], Si-S [2.144(2)-2.1638(9) A], and Si-C distances [1.900(5)-1.906(2) A], the Si02S2C frameworks of 88 and 89 are best described as being built up by five normal covalent bonds rather than a bonding system in the sense of a 4+1 coordination. The Si-S distances are very similar to those observed for tetracoordinate silicon compounds with Si-S bonds. 

Some chiral compounds exhibit a different crystal structure for each pure enantiomer and their mixture the difference can be used to distinguish them. Again, the use of cascading libraries allows pure compounds to be distinguished from compounds contaminated with relatively small amounts of the other chiral forms. 

A second example of the use of optically pure coordinatoclathrate hosts in controlling the enantioselectivity of photochemical reactions in the crystalline state is found in the case of the a-oxoamide derivative 13, which forms a crystalline 1 1 complex with host (S,S)-8 [18,19]. Irradiation of these crystals led to the P-lactam derivative (-)-14 in 90% yield and a reported ee of 100% (Scheme 3). The X-ray crystal structure of the complex showed that oxoamide 13 adopts a helical conformation that favors the formation of a single enantiomer of photoproduct 14. The reaction is thus conformationally controlled in a way exactly analogous to the examples discussed earlier in the review. 

Since the enantiomers of the carboxylic acid 42-H can easily be separated via its diastereomeric salts (Scheme 10) [59], many of the other bicyclopropylidene derivatives can also be obtained in enantiomerically pure form by transformations of the acids (R)- and (S)-42-H. The absolute configuration of (i )-42-H was proved by an X-ray crystal structure analysis of its (f )-a-phenylethylamide [59]. 

Using the crystal structures of two related RED enzymes of lignan biosynthesis, a provisional molecular model has been produced for the M. sativa IFR. A smaller binding pocket in the protein, in comparison to the other enzymes, is suggested to account for the specific enantiomer binding and processing of IFR. 

Structure of the lithio derivatives (84CC853) The crystal structure of a THF solvate of the lithium derivative of racemic bislactim ether (derived from two molecules of alanine) has been determined. In the solid state, the lithium derivative exists as a dimer in which the two lithium atoms are nonequivalent (189). The two organic moieties in each dimer are homo-chiral this means that the crystal contains equal number of enantiomers. The Li Li distance is 2.61 A. In THF solution at - 108°C, the compound seems to exist as an equilibrium mixture of monomer and dimer in the ratio 5 1. It is not clear at the moment whether the reacting species is the monomer or the dimer. 

The term Molecular Clip has been coined for molecules of type 2. That these molecules do indeed possess the geometric features of a clip is apparent from the X-ray structure of the tetramethoxy derivative 3a (Fig. 2) [lla,b]. The o-xylylene moieties of this molecule define a tapering cavity, the walls of which are at an angle of 39.5 with the centers of the benzene rings 6.67 A apart. The carbonyl groups of the glycoluril moiety, which are hydrogen-bond acceptor sites, are separated by 5.52 A. It was also possible to obtain a crystal structure of the chiral dibromo-derivative 4 of clip 3 (Fig. 3). This compound was separated into its enantiomers by HPLC on a chiral stationary phase [12]. 

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