We find that the optimal helical angle of the SWNT varies with its length f
or the fixed number of carbon hexagons along the tubular perimeter. The lon
ger the tube is, the larger the helical angle is, in which the helical angl
e is defined with respect to the zigzag configuration. The armchair is the
optimal helical configuration of the SWNT when its length is long enough. (
C) 2001 Elsevier Science B.V. All rights reserved.