This term corrects the underestimation of \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\rm S} (L -{\rm S} (L -{\rmend{document} S}(L ) - S (L - 1 ) for large lengths L [ 56].
Small angle neutron scattering on isolated chicken erythrocyte nuclei revealed DNA power-law relations between the scattering intensity and the scattering vector, thus indicating a fractal organization with a dimension of 2.4 between 15 and 400 nm and 2.9 for larger length scales.
However, different results could be obtained for larger lengths of the drying cycles.
Average night time power densities as high as 30 W/cm2 are possible if the system is designed with a small PCM length (10 cm) to operate just a few hours after sun-set, but running times longer than 72 h (3 days) are possible for larger lengths (50 cm) at the expense of a lower average power density of about 14 W/cm2.
Furthermore, for the case of pure in-plane bending, the nonlocal effects are relatively more than other cases (other load factors) and the difference in the effect of small scale between this case and other cases is significant even for larger lengths.
According to cut-off points in either direction of selection, plants with lower values for LIBR were randomly mated to obtain the first cycle for short-length of the internode basal ring (Short_LIBR) and plants with higher values for LIBR were randomly mated to obtain the first cycle for large-length of the internode basal ring (Large_LIBR).
We are aware that induced fields, with amplitudes of a few nT, are associated with Sq variations (Olsen et al. 2005a), but these essentially consist of large length-scale patterns that should be accounted for through the global large length-scale fit.
The agreement between the theory and the Rouse modes does not depend markedly on the temperature with some improvement for the first modes (large length scales).
MD simulations revealed that the diffusivity decreases with the constriction length and approaches a constant value for large constriction length.
In the horizontal components, modulations with the solar cycle are observed for the large length-scale field at mid- to low latitudes (more obvious in the X direction), and for periodic signals, in horizontal components at high latitudes.
