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Macromolecules magic angle” spinning

Asakura, T., Kuzuhara, A., Tabeta, R., and Saito, H. (1985). Conformation characteriz-tion of Bombyx mod silk fibroin in the solid state by high-frequency 13C cross polarization-magic angle spinning NMR, x-ray diffraction, and infrared spectroscopy. Macromolecules 18, 1841-1845. [Pg.43]

In this section, initial spectral data on several polymers are reported to illustrate the utility of variable-temperature magic-angle spinning (VT-MAS) for the study of macromolecules in the solid state. [Pg.202]

Stoever HDH, Frechet JMJ, Direct polarization 13C and 1H magic angle spinning NMR in the characterization of solvent-swollen gels, Macromolecules, 22 1574-1576, 1989. [Pg.266]

MD Poliks, J Schaefer. Microscopic dynamics in chloral polycarbonate by crosspolarization magic-angle spinning carbon-13 NMR. Macromolecules 23 2682-2686, 1990. [Pg.512]

H. Saito, R. Tabeta, T. Asakura, Y. Iwanaga, A. Shoji, T. Ozaki, I. Ando, High-resolution C-13 NMR-study of silk fibroin in the solid-state by the cross-polarization magic angle spinning method—conformational characterization of silk-I and silk-II type forms of Bombyx mori fibroin by the conformation-dependent C-13 chemical-shifts. Macromolecules 17 (1984) 1405-1412. [Pg.379]

H.R. Kricheldorf, D. Muller, Secondary structure of peptides.3. C-13 NMR cross polarization magic angle spinning spectroscopic characterization of solid polypeptides, Macromolecules 16 (1983) 615-623. [Pg.380]

Shefer, A., Shefer, S., Kost, J. and Langer, R. (1992) Structural characterization of starch networks in tlic solid state by cro.s.s-polarization magic-angle spinning 13C NMR spectroscopy and wide angle X-rav diffraction. Macromolecules, 25, 6756-6760. [Pg.295]

Fyfe CA, Rudin A, Tchir WJ. Application of High-Resolution C NMR Spectroscopy Using Magic Angle Spinning Techniques to the Direct Investigation of Solid Cured Phenolic Resins. Macromolecules 1980 13 1320. [Pg.149]

Bryson RL, Hatfield GR, Early TA, Palmer AR, MAciel GE. Carbon-13 NMR studies of solid phenolic resins using cross polarization and magic-angle spinning. Macromolecules... [Pg.149]

Figure 6 MAS image of the polybutadiene fraotion of a poly-butadiene/polystyrene blend cast as a film from toluene. MAS alone at 5 kHz spinning Is not suffioient to narrow the polystyrene NMR resonanoe. The in-plane resolution Is SOxSOpm. Figure reproduoed with permission from Cory DG, de Boer JC and Vee-man WS (1989) Magic angle spinning H NMR imaging of poly-butadiene/polystyrene blends. Macromolecules 22 1618. Figure 6 MAS image of the polybutadiene fraotion of a poly-butadiene/polystyrene blend cast as a film from toluene. MAS alone at 5 kHz spinning Is not suffioient to narrow the polystyrene NMR resonanoe. The in-plane resolution Is SOxSOpm. Figure reproduoed with permission from Cory DG, de Boer JC and Vee-man WS (1989) Magic angle spinning H NMR imaging of poly-butadiene/polystyrene blends. Macromolecules 22 1618.
W.L. Earl, D.L. Vanderhart, Observations in solid polyethylenes by C-13 nuclear magnetic-resonance with magic angle sample spinning. Macromolecules 12 (1979) 762-767. [Pg.371]


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See also in sourсe #XX -- [ Pg.271 ]




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