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For a related paper on the crystalline transitions and related physical properties of poly(dichlorophosphazene) see H. R. Allcock and R. A. Arcus
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85022836827
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unpublished results.
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H. R. Allcock and E. G. Stroh, unpublished results.
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Interscience, New York
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E. Giglio, F. Pompa, and A. Ripamonti, J. Polym. Sci., 59, 293 (1962).
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SUNY at Stony Brook, modified by M. J. Bennett and B. M
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Foxman
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C. T. Prewitt, SFLS5A, SUNY at Stony Brook, modified by M. J. Bennett and B. M. Foxman.
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Lawrence Berkeley Laboratory, University of California, modified by G. Hamilton and J. A
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Ibers
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A. Zalkin, FORDAP, Lawrence Berkeley Laboratory, University of California, modified by G. Hamilton and J. A. Ibers.
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Zalkin, A.1
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The conformational energy calculation method is described in detail in H. R. Allcock, R. W. Allen, and J. J. Meister
-
The potential used was a 6-12 Lennard-Jones potential together with a Coulombic term of the type Djj = (kQiQf)/(erA. The partial charges, Q., were +0.70 for phosphorus, -0.32 for nitrogen, and -0.19 for chlorine. No intrinsic backbone torsional potential was applied for the reasons discussed in the article referenced above.
-
The conformational energy calculation method is described in detail in H. R. Allcock, R. W. Allen, and J. J. Meister, Macromolecules, 9, 950 (1976). The potential used was a 6-12 Lennard-Jones potential together with a Coulombic term of the type Djj = (kQiQf)/(erA. The partial charges, Q., were +0.70 for phosphorus, -0.32 for nitrogen, and -0.19 for chlorine. No intrinsic backbone torsional potential was applied for the reasons discussed in the article referenced above.
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The Annals of the Computation Laboratory at Harvard University; Tables of Bessel Functions
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Elsevier, New York
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Wagner, A.J.1
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0000372661
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The equations for these calculations were derived from those reported by T. Miyazawa
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The equations for these calculations were derived from those reported by T. Miyazawa, J. Polym. Sci., 55, 215 (1961).
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