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Views of the cellulose I crystal packing with the (1 f 4) linkage directed out of the page for (a) parallel down and (b) parallel up packing. 

Views of the cellulose I crystal packing with the (1 f 4) linkage directed out of the page for (a) parallel down and (b) parallel up packing. 

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The crystal structure of Valonia cellulose I is determined by X-ray fiber diffraction analysis. A careful reanalysis of two existing X-ray diffraction data sets for Valonia cellulose I leads to a consistent, definitive structure of the -phase. The results resolve ambiguities in existing X-ray analyses between "parallel up" and "parallel down" packi...

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... interesting question is "why does cellulose pack in the parallel up, rather than the parallel down, arrangement"? Parts a and b of Figure 2 show the parallel up and parallel down packing, respectively, displayed such that the polarities of the molecular chains are the same. Defining the unit cells this way means that γ ≈ 83° and γ ≈ 97° in parts a and b, respectively ( Figure 2). ...
Context 2
... a and b of Figure 2 show the parallel up and parallel down packing, respectively, displayed such that the polarities of the molecular chains are the same. Defining the unit cells this way means that γ ≈ 83° and γ ≈ 97° in parts a and b, respectively ( Figure 2). Hence, relative to the molecules, parallel down and parallel up packings correspond to γ ≈ 83° and γ ≈ 97°, respectively. ...
Context 3
... question posed above can then be recast as "why does cellulose pack with γ ≈ 97° rather than γ ≈ 83°"? Or more generally as "why does cellulose pack with γ ≈ 97°, rather than some other value of γ"? Referring to Figure 2, what γ determines, together with w, is the relative position with which the two sheets of cellulose molecules pack. Two calculations were made to shed some light on the answer to this question. ...

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... To study the effects of different silane coupling agents that modify cellulose and different concentrations of KH1631, molecular dynamics simulations (MS) were conducted with Materials Studio 6.0 using the COMPASS Force Field. A Nosé-Hoover thermostat was used to maintain the temperature at 298 K and 405 K. MS first involved geometric optimization of silane coupling agent chain and cellulose crystal models (Finkenstadt and Millane 1998), after which dynamic analysis was carried out. ...
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... Figures 3 a and b show the wide-angle X-ray fiber diffraction patterns of the four different crystalline cotton cellulose. The XRD patterns of cellulose I β (Finkenstadt and Millane 1998), II (Langan et al. 1999), III I (Wada et al. 2004), and IV I (Gardiner and Sarko 1985) simulated based on cif files are also provided in Fig. 3 a and (105) crystal planes of cellulose I, respectively. Therefore, the crystal lattice of cellulose in cotton fibers has not been destroyed during the waste cotton recycling process. ...
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... The unit cell of cellulose is monoclinic (P21) with lattice parameters of a = 7.78 Å, b = 8.20 Å, c = 10.38 Å, α = β = 90°, γ = 96.5° [3,24]. Cellulose bundles perform a significant role in reinforcing the plant cell wall attributing to intermolecular hydrogen bonding network between adjacent chains [21]. ...
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... The wide angle X-ray fiber diffraction profiles of cotton fibers before and after TiO 2 loading are shown in Fig. 3. The simulated XRD patterns of cellulose I β (Finkenstadt and Millane 1998), II (Langan et al. 1999), III I (Wada et al. 2004a) and IV I (Gardiner and Sarko 1985) cif files and the standard XRD pattern of anatase TiO 2 (JCPDS No.21-1272) are also provided for comparison and analysis. As illustrated in Fig. 3a, the diffraction peaks at 2θ = 14.8°, 16.7°, 20.6°, 22.9°, 27.9°, 34.5°, 41.9° and 45.0° in the C-I and T-C-I fibers are well correlated with the (1-10), (110), (102), (200), (013), (004), (204) and (105) crystal planes of cellulose I β , respectively (French 2014). ...
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... The physical properties of the cellulose, among which are swelling, adsorption and accessibility for chemical modification Intra-and intermolecular hydrogen bonds within a cellulose structure [44] are influenced by these crystalline structures [47]. The first study work giving details of the crystalline structure, and the packing of native celluloses was reported by Meyer et al. [48] The report proposed that ramie cellulose has a structure with a monoclinic unit cell. The unit cell is made of two anti-parallel polysaccharide chains with dimensions a = 0.835 nm, b = 0.79 nm. ...
... The unit cell is made of two anti-parallel polysaccharide chains with dimensions a = 0.835 nm, b = 0.79 nm. Where c is the fiber axis, equal to 1.03 nm, and γ = 84° [48] A different model of the native crystalline structure of alga Valonia having a triclinic unit cell was reported by Finkenstadt and Millane [49]. ...
... This movement rapidly forms an intermediary complex by protonation of the glycosidic linkage, as shown in Figure 4 [40]. The protonation of the β-1,4-glucosidic bonds results in the slowly scissioning of the bond, thereby producing fragments of rod-like CWs [48]. The slitting of the hydrolytic cleavage of the glycosidic linkage bond is the ratedetermining step of the process. ...
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... Cellulose is insoluble in most organic solvents and water. Therefore, there has been significant effort to find ways to process cellulose using new solvents and reagents 42 , dating back to the viscose method that uses carbon disulphide 43 After cellulose xylan is the second most abundant biopolymer, on earth 45 . Xylan is found in the cell walls of plants and comes in a wide range of structures, where this diversity in structures is correlated with their functions in the plants they are found. ...
Chapter
Solutions of xylan and xylose in 1-ethyl-3-methylimidazolium acetate [C2mim] [OAc], a room temperature ionic liquid, were examined across a range of temperatures (20°C–70 °C) using: NMR spectroscopy; diffusion; low-field (20 MHz) spin–lattice and spin–spin relaxation times; and rheological measurements through the zero shear rate viscosity. The addition of xylose and xylan affect the mobility of the ions, with a decrease occurring when the carbohydrate concentration is increased. The ratio of the diffusion coefficients for the anion to the cation remained constant upon the addition of both xylan and xylose, showing that the anion and cation were equally affected by the presence of the carbohydrate. The translational diffusion motion of the ions in the xylose solutions were similar in value to published results for cellobiose, which we explain in terms of the number of available carbohydrate OH groups that the ions are interacting with. We observe from the various NMR results that the dissolving mechanism of xylan in [C2mim] [OAc] is similar to that for cellulose.
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