Secondary processes of poly(methyl methacrylate) and their activation energies as determined by shear and tensile creep compliance measurements

1968 ◽  
Vol 6 (3) ◽  
pp. 433-449 ◽  
Author(s):  
Edward V. Thompson
2009 ◽  
Vol 47 (17) ◽  
pp. 1713-1727 ◽  
Author(s):  
Hau-Nan Lee ◽  
Keewook Paeng ◽  
Stephen F. Swallen ◽  
M. D. Ediger ◽  
Rebecca A. Stamm ◽  
...  

1996 ◽  
Vol 11 (10) ◽  
pp. 2403-2405 ◽  
Author(s):  
Sanboh Lee

The effect of thickness on methanol transport in fourteen-year-old crosslinked poly(methyl methacrylate) was investigated. The samples studied here are from the same primary source of those used by a study made fourteen years earlier. The sample was encapsulated by a plastic bag and maintained in a desiccator at room temperature. Four thicknesses, 0.6, 1.0, 1.5, and 1.9 mm, were examined. Methanol sorption data were fit to a model in which the mass sorption is a combination of case I, case II, and anomalous sorption. The diffusion coefficient for case I transport increases with increasing thickness, but the velocity for case II transport does the opposite. The diffusion coefficient for case I transport and the velocity for case II transport exhibit the Arrhenius behavior. The activation energies for case II transport are 18.9, 16.3, 14.6, and 13.4 kcal/mole, corresponding to the thicknesses 0.6, 1.0, 1.5, and 1.9 mm, respectively. The activation energies for case I transport are 24.7, 24.2, 21.7, and 21.9 kcal/mole, corresponding to the thicknesses 0.6, 1.0, 1.5, and 1.9 mm, respectively. For thickness 1.5 mm the activation energies for case I and case II transport are 21.7 and 14.6 kcal/mole for this study and 24.9 and 17.3 kcal/mole obtained fourteen years ago.


2007 ◽  
Vol 340-341 ◽  
pp. 1091-1096 ◽  
Author(s):  
Wen Bo Luo ◽  
Chu Hong Wang ◽  
Rong Guo Zhao

The uniaxial tensile creep of a commercial grade Poly(methyl methacrylate) was measured for 4000 seconds under various temperatures and stress levels ranging from 14 oC to 26 oC and 6 MPa to 32 MPa. The resultant creep compliance curves depart from each other for stresses beyond a critical value which varies with temperature, indicating nonlinear viscoelastic behavior. The time-temperature-stress superposition principle (TTSSP) was used to construct a smooth master compliance curve with a much longer time-scale interval from the short-term tests at higher stresses and temperatures. It is shown that the master curve covers a period of over 290 days, which is nearly 3.9 decades longer than the test duration. Moreover, it is verified that the time-temperature shift factors are dependent on stresses at which the shifts are applied, and that the time-stress shift factors are dependent on reference temperatures.


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