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34
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3342884562
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note
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14b is not correct in detail. In addition, there are other discrepancies between the calculated and experimental X-ray diffraction patterns; there are unwanted Okl equatorial diffraction signals in the region between the 010 and 020, and there is poor agreement with the observed hoo intensities.
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85086290359
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note
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4,5
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36
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3342940102
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note
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The appearance of the first few orders of the 3.2 nm on the equator indicates that the lamellae are stacking reasonably well at the stacking periodicity of 3.2 nm. In a number of crystal preparations, only a diffuse first order at spacing 3.6 nm (12% greater) was observed. This is consistent with poorly stacked lamellae.
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37
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3342988371
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note
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There are two possible sequences for the γ-turns, either GAG or AGA. Since we know a priori that the resolution of the experimental data will not allow us to delineate the fine details of the fold geometry, we chose the GAG γ-turn as the basis of our model.
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38
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3342888000
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note
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With regard to the stacking of the polar apβ-sheets, there are two possibilities if like surfaces are to be in contact, either a rotation, π, about the a-axis, or a rotation, π, about the c-axis. The former structure was favored since it results in a chain-folded lamellar crystal with both surfaces equally populated with the two types of fold conformations. These considerations are discussed in more detail in ref 5.
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39
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3342898483
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note
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14a it may be that little, if any, chain folding occurred. No low-angle diffraction features were reported.
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submitted for publication
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Cantor, E. J.; Atkins, E. D. T.; Cooper, S. J.; Fournier, M. J.; Mason, T. L.; Tirrell, D. A., submitted for publication.
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Cantor, E.J.1
Atkins, E.D.T.2
Cooper, S.J.3
Fournier, M.J.4
Mason, T.L.5
Tirrell, D.A.6
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