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Two points of general interest in structural refinement of polymers based on internal coordinates are discussed: the chain orientation and the chain continuity. Using a proprietary computer program, based on revised approaches to these questions, the structure of polyisobutene has been reconsidered, using new X-ray diffraction measurements (Fuji image plate) and performing a structure refinement based on internal coordinates. Three refinement schemes, with a decreasing number of degrees of freedom, have been considered, with the conclusion that the distortion from the 83 regular helix, claimed by Tadokoro [(1979). Structure of Crystalline Polymers, p. 136. New York: Wiley-Interscience], is confirmed, though lower than supposed. The new procedures implemented for chain orientation and chain continuity work excellently.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0021889806044955/db5009sup1.cif
Contains datablock yill

CCDC reference: 660871

Computing details top

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
(yill) top
Crystal data top
?β = 90°
Mr = ?γ = 90°
?, &unitsp;V = ? Å3
a = 6.880 ÅZ = ?
b = 11.910 Å? radiation, λ = ? Å
c = 18.600 Å × × mm
α = 90°
Data collection top
h = ??l = ??
k = ??
Refinement top
Crystal data top
?β = 90°
Mr = ?γ = 90°
?, &unitsp;V = ? Å3
a = 6.880 ÅZ = ?
b = 11.910 Å? radiation, λ = ? Å
c = 18.600 Å × × mm
α = 90°
Data collection top
Refinement top
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzBiso*/Beq
C10.34210.05400.0442
C20.32560.03720.1261
C30.14530.02770.1748
C40.20670.03070.2544
C50.36400.03620.2948
C60.32710.03050.3764
C70.28340.07060.4254
C80.28370.03350.5047
C90.27160.17280.0246
c100.55570.03980.0212
C110.04010.08370.1591
C120.00740.12670.1593
C130.56510.01410.2780
C140.35800.15960.2702
C150.08250.11900.4062
C160.44030.16120.4141
H170.39620.09950.1458
H180.39510.03140.1348
H190.08920.01360.2799
H200.24230.10770.2623
H210.44190.06310.3970
H220.21800.07950.3836
H230.26080.10180.5307
H240.41440.00820.5127
H250.34910.22800.0489
H260.13820.18210.0386
H270.28220.18440.0263
H280.63560.09390.0456
H290.56780.05070.0297
H300.60040.03420.0332
H310.07260.09050.1892
H320.12550.14580.1685
H330.00020.08630.1097
H340.10560.12160.1894
H350.03260.12530.1099
H360.07240.19650.1688
H370.66430.02700.3029
H380.56950.09120.2930
H390.59000.01050.2273
H400.45560.20220.2951
H410.38190.16420.2194
H420.23280.19140.2803
H430.05380.18210.4364
H440.01590.06280.4129
H450.08100.14300.3569
H460.41440.22470.4444
H470.44060.18540.3649
H480.56600.13140.4258

Experimental details

Crystal data
Chemical formula?
Mr?
Crystal system, space group?, &unitsp;
Temperature (K)?
a, b, c (Å)6.880, 11.910, 18.600
α, β, γ (°)90, 90, 90
V3)?
Z?
Radiation type?, λ = ? Å
µ (mm1)?
Crystal size (mm) × ×
Data collection
Diffractometer?
Absorption correction?
No. of measured, independent and
observed (?) reflections
?, ?, ?
Rint?
Refinement
R[F2 > 2σ(F2)], wR(F2), S ?, ?, ?
No. of reflections?
No. of parameters?
No. of restraints?
Δρmax, Δρmin (e Å3)?, ?

 

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