A priori crystal structure prediction of native celluloses

The packing of β‐1,4‐glucopyranose chains has been modeled to further elaborate the molecular structures of native cellulose microfibrils. A chain pairing procedure was implemented that evaluates the optimal interchain distance and energy for all possible settings of the two chains. Starting with a...

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Veröffentlicht in:Biopolymers 2000-10, Vol.54 (5), p.342-354
Hauptverfasser: Viëtor, Remco J., Mazeau, Karim, Lakin, Miles, Pérez, Serge
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creator Viëtor, Remco J.
Mazeau, Karim
Lakin, Miles
Pérez, Serge
description The packing of β‐1,4‐glucopyranose chains has been modeled to further elaborate the molecular structures of native cellulose microfibrils. A chain pairing procedure was implemented that evaluates the optimal interchain distance and energy for all possible settings of the two chains. Starting with a rigid model of an isolated chain, its interaction with a second chain was studied at various helix‐axis translations and mutual rotational orientations while keeping the chains at van der Waals separation. For each setting, the sum of the van der Waals and hydrogen‐bonding energy was calculated. No energy minimization was performed during the initial screening, but the energy and interchain distances were mapped to a three‐dimensional grid, with evaluation of parallel settings of the cellulose chains. The emergence of several energy minima suggests that parallel chains of cellulose can be paired in a variety of stable orientations. A further analysis considered all possible parallel arrangements occurring between a cellulose chain pair and a further cellulose chain. Among all the low‐energy three‐chain models, only a few of them yield closely packed three‐dimensional arrangements. From these, unit‐cell dimensions as well as lattice symmetry were derived; interestingly two of them correspond closely to the observed allomorphs of crystalline native cellulose. The most favorable structural models were then optimized using a minicrystal procedure in conjunction with the MM3 force field. The two best crystal lattice predictions were for a triclinic (P1) and a monoclinic (P21) arrangement with unit cell dimensions a = 0.63, b = 0.69, c = 1.036 nm, α = 113.0, β = 121.1, γ = 76.0°, and a = 0.87, b = 0.75, c = 1.036 nm, γ = 94.1°, respectively. They correspond closely to the respective lattice symmetry and unit‐cell dimensions that have been reported for cellulose Iα and cellulose Iβ allomorphs. The suitability of the modeling protocol is endorsed by the agreement between the predicted and experimental unit‐cell dimensions. The results provide pertinent information toward the construction of macromolecular models of microfibrils. © 2000 John Wiley & Sons, Inc. Biopoly 54: 342–354, 2000
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A chain pairing procedure was implemented that evaluates the optimal interchain distance and energy for all possible settings of the two chains. Starting with a rigid model of an isolated chain, its interaction with a second chain was studied at various helix‐axis translations and mutual rotational orientations while keeping the chains at van der Waals separation. For each setting, the sum of the van der Waals and hydrogen‐bonding energy was calculated. No energy minimization was performed during the initial screening, but the energy and interchain distances were mapped to a three‐dimensional grid, with evaluation of parallel settings of the cellulose chains. The emergence of several energy minima suggests that parallel chains of cellulose can be paired in a variety of stable orientations. A further analysis considered all possible parallel arrangements occurring between a cellulose chain pair and a further cellulose chain. Among all the low‐energy three‐chain models, only a few of them yield closely packed three‐dimensional arrangements. From these, unit‐cell dimensions as well as lattice symmetry were derived; interestingly two of them correspond closely to the observed allomorphs of crystalline native cellulose. The most favorable structural models were then optimized using a minicrystal procedure in conjunction with the MM3 force field. The two best crystal lattice predictions were for a triclinic (P1) and a monoclinic (P21) arrangement with unit cell dimensions a = 0.63, b = 0.69, c = 1.036 nm, α = 113.0, β = 121.1, γ = 76.0°, and a = 0.87, b = 0.75, c = 1.036 nm, γ = 94.1°, respectively. They correspond closely to the respective lattice symmetry and unit‐cell dimensions that have been reported for cellulose Iα and cellulose Iβ allomorphs. The suitability of the modeling protocol is endorsed by the agreement between the predicted and experimental unit‐cell dimensions. The results provide pertinent information toward the construction of macromolecular models of microfibrils. © 2000 John Wiley &amp; Sons, Inc. 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A chain pairing procedure was implemented that evaluates the optimal interchain distance and energy for all possible settings of the two chains. Starting with a rigid model of an isolated chain, its interaction with a second chain was studied at various helix‐axis translations and mutual rotational orientations while keeping the chains at van der Waals separation. For each setting, the sum of the van der Waals and hydrogen‐bonding energy was calculated. No energy minimization was performed during the initial screening, but the energy and interchain distances were mapped to a three‐dimensional grid, with evaluation of parallel settings of the cellulose chains. The emergence of several energy minima suggests that parallel chains of cellulose can be paired in a variety of stable orientations. A further analysis considered all possible parallel arrangements occurring between a cellulose chain pair and a further cellulose chain. Among all the low‐energy three‐chain models, only a few of them yield closely packed three‐dimensional arrangements. From these, unit‐cell dimensions as well as lattice symmetry were derived; interestingly two of them correspond closely to the observed allomorphs of crystalline native cellulose. The most favorable structural models were then optimized using a minicrystal procedure in conjunction with the MM3 force field. The two best crystal lattice predictions were for a triclinic (P1) and a monoclinic (P21) arrangement with unit cell dimensions a = 0.63, b = 0.69, c = 1.036 nm, α = 113.0, β = 121.1, γ = 76.0°, and a = 0.87, b = 0.75, c = 1.036 nm, γ = 94.1°, respectively. They correspond closely to the respective lattice symmetry and unit‐cell dimensions that have been reported for cellulose Iα and cellulose Iβ allomorphs. The suitability of the modeling protocol is endorsed by the agreement between the predicted and experimental unit‐cell dimensions. The results provide pertinent information toward the construction of macromolecular models of microfibrils. © 2000 John Wiley &amp; Sons, Inc. 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A chain pairing procedure was implemented that evaluates the optimal interchain distance and energy for all possible settings of the two chains. Starting with a rigid model of an isolated chain, its interaction with a second chain was studied at various helix‐axis translations and mutual rotational orientations while keeping the chains at van der Waals separation. For each setting, the sum of the van der Waals and hydrogen‐bonding energy was calculated. No energy minimization was performed during the initial screening, but the energy and interchain distances were mapped to a three‐dimensional grid, with evaluation of parallel settings of the cellulose chains. The emergence of several energy minima suggests that parallel chains of cellulose can be paired in a variety of stable orientations. A further analysis considered all possible parallel arrangements occurring between a cellulose chain pair and a further cellulose chain. Among all the low‐energy three‐chain models, only a few of them yield closely packed three‐dimensional arrangements. From these, unit‐cell dimensions as well as lattice symmetry were derived; interestingly two of them correspond closely to the observed allomorphs of crystalline native cellulose. The most favorable structural models were then optimized using a minicrystal procedure in conjunction with the MM3 force field. The two best crystal lattice predictions were for a triclinic (P1) and a monoclinic (P21) arrangement with unit cell dimensions a = 0.63, b = 0.69, c = 1.036 nm, α = 113.0, β = 121.1, γ = 76.0°, and a = 0.87, b = 0.75, c = 1.036 nm, γ = 94.1°, respectively. They correspond closely to the respective lattice symmetry and unit‐cell dimensions that have been reported for cellulose Iα and cellulose Iβ allomorphs. The suitability of the modeling protocol is endorsed by the agreement between the predicted and experimental unit‐cell dimensions. The results provide pertinent information toward the construction of macromolecular models of microfibrils. © 2000 John Wiley &amp; Sons, Inc. Biopoly 54: 342–354, 2000</abstract><cop>New York</cop><pub>John Wiley &amp; Sons, Inc</pub><pmid>10935974</pmid><doi>10.1002/1097-0282(20001015)54:5&lt;342::AID-BIP50&gt;3.0.CO;2-O</doi><tpages>13</tpages></addata></record>
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subjects 4-glucopyranose chains
Carbohydrate Conformation
Cellulose - chemistry
Computer Simulation
crystal structure prediction
Crystallography
Models, Chemical
Models, Molecular
molecular structure
native cellulose microfibrils
packing
Thermodynamics
β-1
β‐1,4‐glucopyranose chains
title A priori crystal structure prediction of native celluloses
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