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A Monte Carlo study of the excluded-volume effect on the amylosic chain conformation

✍ Scribed by Shinichi Kitamura; Takahiro Okamoto; Yasushi Nakata; Takeshi Hayashi; Takashi Kuge


Publisher
Wiley (John Wiley & Sons)
Year
1987
Tongue
English
Weight
562 KB
Volume
26
Category
Article
ISSN
0006-3525

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✦ Synopsis


A Monte Carlo procedure was used to determine the effect of excluded volume on the conformational dimensions of amyloaic chains. The excluded volume was introduced into the model by assuming that hard spheres, which cannot overlap each other, exist at the center of mees of each glucose unit in the chain sequence. Monte Carlo chains, which were generated to be distributed consistent with the potential energy of nonbonded nearest-neighbor interactions, underwent self-intersections, and the attrition rate in the generation of self-avoiding chains was found to obey an exponential decay law with increasing chain length x. Thus, in order to generate effectively a large number of self-avoiding chains with long sequences, we used the Wall-Erpenbeck s-p method of chain enrichment [F. T. W a l l and J. J. Erpenbeck (1959) J . C h m .

Phys. 30,634-6373. By examinatim of the radial distribution of the end-to-end distance and the chain-length dependence of the quantity ( r 2 ) / d 2 ((r') is the mean square end-to-end distance and I ie the virtual bond length), it was found that unperturbed amylkc chains change in overall conformation from a non-Gaueeian chain having a helical character to Gaussian as x is increased, whereas perturbed chains do not show Gaussian behavior even at x = 500. For the perturbed chains, (r') can be expresaed by the equation ( r 2 ) = atb in the range of 100 5 x < 500, where a and b > 1 are constants From comparisons of the persistence vectors and perspective drawings of representative unperturbed and perturbed chains, we felt the local conformation of the amyloeic chains, i.e., the local helical character, is also afhted by the long-range excluded-volume interaction.

shown only for energies less than 5.0 kcal mol-', where solid contours are given at intervals of 1 kcal mol-* for energiea 2 -1 kcal mol-' and dashed contours at 0.2 kcal mol-' for energies < -1 kcal mol-'.


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