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Macromolecules, star-branched

As already outlined, star branched macromolecules resemble their linear chain analogues. The behavior becomes evident when for a given number of arms f the... [Pg.137]

Fig. 13. Chain length dependence of the second virial coefficient A2 for some star branched macromolecule, according to Casassa (full line). The data points correspond to measurements [89] (triangles 3-arm, circles 12-arm and rhombus 18-arm stars. Reprinted with permission from [89]. Copyright [1984] American Society... Fig. 13. Chain length dependence of the second virial coefficient A2 for some star branched macromolecule, according to Casassa (full line). The data points correspond to measurements [89] (triangles 3-arm, circles 12-arm and rhombus 18-arm stars. Reprinted with permission from [89]. Copyright [1984] American Society...
The Schulz-Zimm distribution would be found for/end-to-end coupled linear chains which obey the most probable distribution, as well as for/of such chains which are coupled onto a star center. This behavior demonstrates once more the quasi-linear behavior of star branched macromolecules. In fact, to be sure of branching, other structural quantities have to be measured in addition to the molar mass distribution. [Pg.155]

In contrast to star-branched macromolecules, this relationship differs now from that of the non-fractionated samples... [Pg.163]

Fig. 22. KMHS relationships for the fractions of end-linked 3-arm star-branched polystyrene molecules and of linear polystyrene fractions. The data refer to three samples of different in the pregel state and one from the sol fraction of a gel. The curves for the branched macromolecules coincide within experimental error in the high molar mass region. The deviations at lowM result from a different amount of non-reacted end-functionalized stars. The exponents of the end-linked and linear PS chains are a =0.42 0.02 while that of linear chains is 0.70 0.01 [95,120,123,124]. Reprinted with permission from [95]. Copyright [1997] American Society... Fig. 22. KMHS relationships for the fractions of end-linked 3-arm star-branched polystyrene molecules and of linear polystyrene fractions. The data refer to three samples of different in the pregel state and one from the sol fraction of a gel. The curves for the branched macromolecules coincide within experimental error in the high molar mass region. The deviations at lowM result from a different amount of non-reacted end-functionalized stars. The exponents of the end-linked and linear PS chains are a =0.42 0.02 while that of linear chains is 0.70 0.01 [95,120,123,124]. Reprinted with permission from [95]. Copyright [1997] American Society...
Fig. 24. Contraction factors for star-branched macromolecules as a function of the number of arms. The full line represents strictly regular stars, the dashed line one that for stars with polydisperse arms (MyM =2), the dotted line according to Daoud and Cotton [29]. The symbols represent the data from the literature. The deviation at large / represents the stretching of the arms due to overcrowding... Fig. 24. Contraction factors for star-branched macromolecules as a function of the number of arms. The full line represents strictly regular stars, the dashed line one that for stars with polydisperse arms (MyM =2), the dotted line according to Daoud and Cotton [29]. The symbols represent the data from the literature. The deviation at large / represents the stretching of the arms due to overcrowding...
Thus a simple power law behavior with an exponent of 1.5 would result if 0"= 1 [125]. Zimm and Kilb [128] made a first attempt to calculate g for star branched macromolecules on the basis of the Kirkwood-Riseman approximation for the hydrodynamic interaction. They came to the conclusion that... [Pg.167]

Fig. 25. The viscosity contraction factor g as a function of the geometric contraction factor g for star-branched macromolecules ( 3-128). No distinction was made between the chemical nature of the various arms and between the thermodynamic quality of the solvents used. See Table 3... Fig. 25. The viscosity contraction factor g as a function of the geometric contraction factor g for star-branched macromolecules ( 3-128). No distinction was made between the chemical nature of the various arms and between the thermodynamic quality of the solvents used. See Table 3...
In some case, however, only a flattening of the osmotic modulus curve is observed. Such a case is found with star-branched macromolecules. This observation has rather comprehensively been investigated by Roovers et al. with stars of 64 and 128 arms [172]. The authors give the following explanation. At the point of coil overlap and at somewhat higher concentrations the stars feel the interaction as a quasi colloidal particle. Hence, a steeper increase of the osmotic mod-... [Pg.188]

Tian D, Dubois P, Jerome R, Teyssie P (1994) Macromolecular engineering of polylactones and polylactides. 18. Synthesis of star-branched aliphatic polyesters bearing various functional end-groups. Macromolecules 27 4134 144... [Pg.216]

Figure 2. Robust super high-spin oiganic macromolecules with linear and star-branched topologies. Figure 2. Robust super high-spin oiganic macromolecules with linear and star-branched topologies.
In 1965, Milkovich (. ) reported that divinylbenzene could be utilized for the formation of star-branched macromolecules. Later, Rempp and coworkers (2, 3, 4) successfully applied this method for the synthesis of star-branched polystyrenes. Moreover, Fetters and coworkers (54 ) used this procedure for the synthesis of multi-arm star-branched polyisoprene homopolymers and poly-... [Pg.557]

Fig. 29. Zimm-plot and Kratky-plot from a star-branched macromolecule. Star centre nodule of densely cross-linked polydivinyl benzene rays monodisperse polystyrene chains. Measurement in toluene at 20 °C and with the three wavelengths 20 = 546, 436 and 365 nm"1... Fig. 29. Zimm-plot and Kratky-plot from a star-branched macromolecule. Star centre nodule of densely cross-linked polydivinyl benzene rays monodisperse polystyrene chains. Measurement in toluene at 20 °C and with the three wavelengths 20 = 546, 436 and 365 nm"1...
A larger reduction in the mean square unperturbed dimensions can be achieved by rearrangement of the n + 1 atoms into an /-functional star-branched polymer. In this architecture, the macro molecule contains / branches (f> 2), each with n/f bonds, that emanate from a common atom. The same terminology is frequently used for branched macromolecules with very large/if the branches emanate from a collection of atoms that are constrained to remain close together, so that the origin of all of the branches is clustered in a volume much smaller than (s2)m. The influence of the star-branched architecture on the mean square dimensions is traditionally designated by a factor g that is defined as ... [Pg.7]

Equation (1.20) suggests that the mean square dimensions of the macrocycle are approximated by the star-branched polymer with five arms, for which g = 0.52. It also suggests that a macromolecule with a closer approach to the condensed state could be obtained by using f>5. [Pg.7]

The intrinsic viscosity [ry] of both linear and branched macromolecules and the branching parameter values of the star-branched copolymers were also calculated by the GPC software and are reported in Table IV. The ratio [vlhAvlim, between the intrinsic viscosity of the... [Pg.176]

Utracki, L.A. Roovers, J.E.L. Viscosity and normal stresses of linear and star branched polystyrene solution. I. Application of corresponding states principle to zero-shear viscosities. Macromolecules 1973, 6 (3), 366-372. [Pg.265]

Burchard W, Schmidt M, Stockmayer WH. Influence of hydrodynamic preaveraging on quasi-elastic scattering from flexible linear and star-branched macromolecules. Macromolecules 1980 13 580-587. [Pg.57]

The experimental evidence to-date suggests that the effects on stability arising from these higher order terms are negligible. This would not necessarily be the case, however, with star-branched macromolecules as stabilizers. Even in free solution, such polymers apparently display anom-... [Pg.136]

The nonlinear branched topology is expected to introduce novel specific features in the collapse transition of individual charged macromolecules, due to the interplay between intra- and interbranch Coulomb repulsion. Conformations of intrinsically hydrophobic star-branched PE have been studied experimentally in the past decade [50, 51]. Recently synthesized PDMAEMA stars responsive to both pH and temperature [47, 48] are expected to undergo an intramolecular collapse transition as a response to the increase in temperature. The latter provokes a decrease in the solubility of the monomers in the star arms. [Pg.46]

Dong, T., Dubois, P., Jdrdme, R., and Teyssie, P., 1994, Macromolecular Engineering of Polylactones and Polylactides. 18. Synthesis of Star-Branched Aliphatic Polyesters Bearing Various Functional End Groups. Macromolecules, 27 4134... [Pg.193]

F. Wang, M. S. Wilson, R. D. Rauh, P. Schottland, B. C. Thompson and J. R. Reynolds, Electrochromic linear and star branched poly(3,4-ethylenedioxythiophene-didodecyloxybenzene) polymers. Macromolecules, 33, 2083-2091 (2000). [Pg.141]


See other pages where Macromolecules, star-branched is mentioned: [Pg.240]    [Pg.218]    [Pg.667]    [Pg.115]    [Pg.146]    [Pg.181]    [Pg.558]    [Pg.240]    [Pg.4]    [Pg.87]    [Pg.697]    [Pg.167]    [Pg.172]    [Pg.288]    [Pg.620]    [Pg.625]    [Pg.191]    [Pg.620]    [Pg.625]    [Pg.72]    [Pg.3]    [Pg.10]    [Pg.122]    [Pg.161]    [Pg.189]    [Pg.71]    [Pg.1917]    [Pg.47]   
See also in sourсe #XX -- [ Pg.557 ]




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Branched macromolecules

Star macromolecule

Star-branched

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