1967
DOI: 10.1002/polc.5070160405
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Dynamic birefringence of poly(methyl methacrylate)

Abstract: The dynamic modulus, strain‐optical coefficient, and stress‐optical coefficient have been measured for conventional poly(methyl methacrylate) (PMMA) in the frequency range 16–10−2.5 cps and at temperatures between −130 and +140°C. Both the α (glass–rubber) relaxation and the β relaxation have been detected in plots of each of these observables, or the appropriate phase angles, against temperature or frequency. The extremely broad mechanical β relaxation suggests a wide distribution of relaxation frequencies. T… Show more

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Cited by 21 publications
(15 citation statements)
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“…The contribution of the ester group to the optical anisotropy of a statistical segment depends on the orientation of the -COO-plane with respect to the axis of the segment. Calculations of the optical anisotropy by Tsvetkov et al [11] and Read [17] based upon the additivity of bond polarizabilities show that the values of the optical anisotropy differ for different positions of the -COOplane. In the case of a fixed trans-position where the -COO-plane is perpendicular to the axis of the segment the optical anisotropy of a monomer unit is negative.…”
Section: Hindered Side Group Rotation and Associationsmentioning
confidence: 99%
“…The contribution of the ester group to the optical anisotropy of a statistical segment depends on the orientation of the -COO-plane with respect to the axis of the segment. Calculations of the optical anisotropy by Tsvetkov et al [11] and Read [17] based upon the additivity of bond polarizabilities show that the values of the optical anisotropy differ for different positions of the -COOplane. In the case of a fixed trans-position where the -COO-plane is perpendicular to the axis of the segment the optical anisotropy of a monomer unit is negative.…”
Section: Hindered Side Group Rotation and Associationsmentioning
confidence: 99%
“…2 Dynamic measurements on polymers far above and well below the glass transition temperature have been interpreted in terms of a C that is independent of stress and test frequency. [14][15][16][17][18][19][20][21][22] In rubbers, a direct proportionality between stress and birefringence implies that both have the same physical originsorientation of the segments comprising the polymer chains. 2,3,23 Four departures from the stress optical law are known: (i) When the orientation of the bond vectors (responsible for the intrinsic birefringence) is no longer proportional to the orientation of the chain end-to-end vector (responsible for the mechanical stress).…”
Section: Introductionmentioning
confidence: 99%
“…(ii) Behavior in the softening zone of the viscoelastic spectrum ostensibly violates the stress optical law; however, the stress optical coefficient obtained from dynamic mechanical experiments in this regime can be decomposed into a glassy and rubbery component, both conforming to eq 1. [14][15][16][17][18][19][20][21][22] (iii) While the intrinsic birefringence is proportional to the stress, the form birefringence, arising from spatial variations of the dielectric constant, is not. Significant for phase-separated blends and semicrystalline polymers, 2,24 the form birefringence is negligible in homogeneous materials.…”
Section: Introductionmentioning
confidence: 99%
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“…If all positions of the side group have the same probability, the calculated optical anisotropy of the monomer unit is positive ("free rotating" side group). If the side group is in a perpendicular position to the main chain (~ = z/2) Aam is negative [6,7]. The actual mean position of the side group and consequently Aam are functions of the temperature.…”
Section: Introductionmentioning
confidence: 99%