A revised structure and hydrogen-bonding system in cellulose II from a neutron fiber diffraction analysis

Citation
P. Langan et al., A revised structure and hydrogen-bonding system in cellulose II from a neutron fiber diffraction analysis, J AM CHEM S, 121(43), 1999, pp. 9940-9946
Citations number
44
Categorie Soggetti
Chemistry & Analysis",Chemistry
Journal title
JOURNAL OF THE AMERICAN CHEMICAL SOCIETY
ISSN journal
00027863 → ACNP
Volume
121
Issue
43
Year of publication
1999
Pages
9940 - 9946
Database
ISI
SICI code
0002-7863(19991103)121:43<9940:ARSAHS>2.0.ZU;2-D
Abstract
The crystal and molecular structure and hydrogen bonding system in cellulos e II have been revised using new neutron diffraction data extending to 1.2 Angstrom resolution collected from two highly crystalline fiber samples of mercerized flax, Mercerization was achieved in NaOH/H2O for one sample and in NaOD/D2O for the other, corresponding to the labile hydroxymethyl moieti es being hydrogenated and deuterated, respectively. Fourier difference maps were calculated in which neutron difference amplitudes were combined with phases calculated from two revised X-ray models of cellulose II, A and B'. The revised phasing models were determined by refinement against the X-ray data set of Kolpak and Blackwell,(8) using the LALS methadology.(37) Both m odels A and B' have two antiparallel chains organized in a P2(1) space grou p and unit cell parameters: a = 8.01 Angstrom; b = 9.04 Angstrom, c = 10.36 Angstrom, and gamma = 117.1 degrees.(15) Model A has equivalent backbone c onformations for both chains but different conformations for the hydroxymet hyl moieties: gt for the origin chain and fg for the center chain. Model B' , based on the recent crystal structures of cellotetraose,(21-23) has diffe rent conformations for the two chains but nearly equivalent conformations f or the hydroxymethyl moieties. On the basis of the X-ray data alone, model A and model B' could not be differentiated. From the neutron Fourier differ ence maps, possible labile hydrogen atom positions were identified for each model and refined using LALS. We were able to eliminate model A in favor o f model B'. The hydrogen-bonding scheme identified for model B' is signific antly different from previous proposals based on the crystal structures of cellotetraose,(21-23) MD simulations of cellulose II,(25),and any potential hydrogen-bonding network in the structure of cellulose II determined in ea rlier X-ray fiber diffraction studies.(7,8) The exact localization of the l abile hydrogen atoms involved in this bonding, together with their donor an d acceptor characteristics, is presented and discussed. This study provides , for the first time, the coordinates of all of the atoms in cellulose II.