The structure of Boc-(L-Val-D-Val),-OMe has been determined by x-ray single-crystal diffraction analysis. The octapepti+ crystallizes in the trigonal system, space group P3,21 with a = b = 12.760 A, c = 63.190 A and Z = 6. The independent unit is represented by one octapeptide chain. The structure h
The structure of the left-handed antiparallel amylose double helix: Theoretical studies
β Scribed by Wolfgang Schulz; Heinz Sklenar; Winfried Hinrichs; Wolfram Saenger
- Publisher
- Wiley (John Wiley & Sons)
- Year
- 1993
- Tongue
- English
- Weight
- 864 KB
- Volume
- 33
- Category
- Article
- ISSN
- 0006-3525
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β¦ Synopsis
we have calculated a theoretical counterpart of this idealized double helix by constraining the helical twist and rise to their experimental values ( -45' and 2.33 A, respectively). Applying the same constraints to the parallel-stranded duplex, this also leads to a low-energy structure with wide central cavity. It is considered as an alternative model to accommodate iodine as observed in the starch-iodine complex.
Release of the helical constraints leads to left-handed antiparallel-and parallel-stranded double helices, respectively, with narrow central cavities. Both structures have very similar helix parameters and correspond, in their main characteristics, to the experimentally derived parallel-stranded structure of amylose in starch ( 6 residues per turn and a pitch height of about 21 A). The intramolecular energy calculated for the optimized antiparallel-stranded amylose double helix is comparable to that of the parallel-stranded structure. This result raises the question why parallel-stranded amylose seems to be favored in nature. 0 1992 John Wiley & Sons, Inc.
π SIMILAR VOLUMES
The crystal structure of Boc-(L-Phe-D-Phe),-OMe has been determined by x-ray diffracti2n analysis. peptide cry@llizes in the triclinic system, space group P1 with a = 15.290 A, b = 15.163 A, c = 19.789 A, a = 102.49', 8 = 96.59", y = 74.22", and Z = 2. The structure has been solved by coupling of t
The Lifson-Roig and Zimm-Bragg theories of t,he helix-coil transition ill polypeptides are generalized to include both right-and left-handed a-helical states. The partition functions for these more general theories are formulated in terms of the parameters u, V R , V L , W R , and W L for t,he gener