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Poly calculations

The reports were that water condensed from the vapor phase into 10-100-/im quartz or pyrex capillaries had physical properties distinctly different from those of bulk liquid water. Confirmations came from a variety of laboratories around the world (see the August 1971 issue of Journal of Colloid Interface Science), and it was proposed that a new phase of water had been found many called this water polywater rather than the original Deijaguin term, anomalous water. There were confirming theoretical calculations (see Refs. 121, 122) Eventually, however, it was determined that the micro-amoimts of water that could be isolated from small capillaries was always contaminated by salts and other impurities leached from the walls. The nonexistence of anomalous or poly water as a new, pure phase of water was acknowledged in 1974 by Deijaguin and co-workers [123]. There is a mass of fascinating anecdotal history omitted here for lack of space but told very well by Frank [124]. [Pg.248]

Of particular interest has been the study of the polymer configurations at the solid-liquid interface. Beginning with lattice theories, early models of polymer adsorption captured most of the features of adsorption such as the loop, train, and tail structures and the influence of the surface interaction parameter (see Refs. 57, 58, 62 for reviews of older theories). These lattice models have been expanded on in recent years using modem computational methods [63,64] and have allowed the calculation of equilibrium partitioning between a poly-... [Pg.399]

A great many polymers appear to form films having a flat molecular configuration. Thus various polyesters [7] gave extrapolated areas of about 2.5 m /mg corresponding to about the calculated 60-70 area per segment, or mono-layer Sickness of 3-5 A. A similar behavior was noted for poly(vinyl acetate)... [Pg.539]

At 25°C, the Mark-Houwink exponent for poly(methyl methacrylate) has the value 0.69 in acetone and 0.83 in chloroform. Calculate (retaining more significant figures than strictly warranted) the value of that would be obtained for a sample with the following molecular weight distribution if the sample were studied by viscometry in each of these solvents ... [Pg.69]

The equimolar copolymer of ethylene and tetrafluoroethylene is isomeric with poly(vinyhdene fluoride) but has a higher melting point (16,17) and a lower dielectric loss (18,19) (see Fluorine compounds, organic-poly(VINYLIDENE fluoride)). A copolymer with the degree of alternation of about 0.88 was used to study the stmcture (20). Its unit cell was determined by x-ray diffraction. Despite irregularities in the chain stmcture and low crystallinity, a unit cell and stmcture was derived that gave a calculated crystalline density of 1.9 g/cm. The unit cell is befleved to be orthorhombic or monoclinic (a = 0.96 nm, b = 0.925 nm, c = 0.50 nm 7 = 96%. [Pg.365]

A solubihty parameter of 24.5-24.7 MPa / [12.0-12.1 (cal/cm ) ] has been calculated for PVF using room temperature swelling data (69). The polymer lost solvent to evaporation more rapidly than free solvent alone when exposed to air. This was ascribed to reestabUshment of favorable dipole—dipole interactions within the polymer. Infrared spectral shifts for poly(methyl methacrylate) in PVF have been interpreted as evidence of favorable acid—base interactions involving the H from CHF units (70). This is consistent with the greater absorption of pyridine than methyl acetate despite a closer solubihty parameter match with methyl acetate. [Pg.380]

MO calculations, 2, 99 in photography, 1, 389 reactions with poly(styrene), 1, 309 structure, 2, 102 Bipyrimidines synthesis, 3, 103... [Pg.569]

Step 1. Calculate the poly tropic exponent using Equation 2.71. [Pg.166]

Using the new poly tropic exponent, calculate the discharge temperature using Equation 5.16. [Pg.169]

It was found that the amount of chlorine that could be removed (84-87%) was in close agreement to that predicted by Flory on statistical grounds for structure Figure 12.10(a). It is of interest to note that similar statistical calculations are of relevance in the cyclisation of natural rubber and in the formation of the poly(vinyl acetals) and ketals from poly(vinyl alcohol). Since the classical work of Marvel it has been shown by diverse techniques that head-to-tail structures are almost invariably formed in addition polymerisations. [Pg.319]

Fig. 4.55. Experimental and calculated (dashed line) RAIR-spectra for poly(methyl methacrylate) films 3270 + 100 nm, 362 30 nm, and 78 + 15 nm thick (a) p-polarized light incident at 60° (b) s-polarized light incident at 60°, after [4.266]. Fig. 4.55. Experimental and calculated (dashed line) RAIR-spectra for poly(methyl methacrylate) films 3270 + 100 nm, 362 30 nm, and 78 + 15 nm thick (a) p-polarized light incident at 60° (b) s-polarized light incident at 60°, after [4.266].
FIGURE 6.18 Poly(Gly-Pro-Pro), a collagen-like right-handed triple helix composed of three left-handed helical chains. (Adaptedfrom Miller Scheraga, H. A., 1976, Calculation of the... [Pg.176]

Model calculations have indicated that/3-poly(L-ma-late) displays a certain degree of isosterism with the pho-sphodeoxyribose backbone of DNA (and probably with the backbone of RNA) regarding the distance between the negative charges [22]. It is, therefore, possible that /3-poly(L-malate) mimicks DNA in many of its activities. [Pg.100]

Two Hell UPS spectra of poly(3-hexylthiophene), or P3HT, compared with the DOVS derived from VEH band structure calculations 83], arc shown in Figure 5-14. The general chemical structure of poIy(3-a ky thiophcne) is sketched in Figure 5-4. The two UPS spectra, were recorded at two different temperatures, +190°C and -60 "C, respectively, and the DOVS was derived from VEH calculations on a planar conformation of P3HT. Compared to unsubslitutcd polythio-phene, the main influence in the UPS spectra due to the presence of the hexyl... [Pg.80]

Boys, S. F., Proc. Roy. Soc. (London) A217, 235, Electronic wave functions. X. A calculation of eight variational poly-detor wave functions for B and C. [Pg.334]

Moreover, calculations on the evaporation rate of bromine from the complex phase were carried out assuming a worst-case scenario, namely a complete spill age of the total bromine inventory (as poly bromide complex) of a fully charge (100% SOC) 15 kWh module which means -32.5 kg of available Br2, forming a 10 m2... [Pg.189]

Fig. 18. Time profiles of transient absorbance at 602 nm due to MV+ for the poly (A/St/Phen)-MV2+ system [Phen](residue) = 0.66 mM [MV2+] = 5mM ( ), 10mM (a). The solid lines represent the best-fit curves calculated from Eq. 10 with the use of the parameters given in Table 6 [120]... Fig. 18. Time profiles of transient absorbance at 602 nm due to MV+ for the poly (A/St/Phen)-MV2+ system [Phen](residue) = 0.66 mM [MV2+] = 5mM ( ), 10mM (a). The solid lines represent the best-fit curves calculated from Eq. 10 with the use of the parameters given in Table 6 [120]...
CTC formation is accompanied by a volume contraction129. Thus, poly(schiff base)s having no side groups give complexes with a density 10—15% higher than that calculated on an additivity assumption. [Pg.34]


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See also in sourсe #XX -- [ Pg.349 ]




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