SYNOPSISIn a previous paper [Ng and McKinley (2008)], we demonstrated that gluten gels can best be understood as a polymeric network with a power-law frequency response that reflects the fractal structure of the gluten network. Large deformation tests in both transient shear and extension show that in the absence of rigid starch fillers these networks are also time-strain factorizable up to very large strain amplitudes ( ). In the present work, we further explore the non-linear rheological behavior of these critical gels by considering the material response obtained in large amplitude oscillatory shear (LAOS) over a wide range of strains and frequencies. We use a Lissajous representation to compare the measured material response with the predictions of a network theory that is consistent with the proposed molecular structure of gluten gels. In the linear viscoelastic regime, the Lissajous figures are elliptical as expected and can be quantitatively described by the same power-law relaxation parameters determined independently 2 from earlier experiments. In the non-linear regime, the Lissajous curves show two prominent additional features. Firstly a gradual softening of the network indicated by the rotation of the major axis. This feature is accounted for in the model by the inclusion of a simple non-linear network destruction term that reflects the reduction in network connectivity as the polymer chains are increasingly stretched. Secondly, a distinct upturn in the viscoelastic stress is discernable at large strains. We show that this phenomenon can be modeled by considering the effects of finitely extensible segments in the elastic network. We apply this model to other large amplitude transient flows such as the start-up of steady shear and extension. In addition to quantitative prediction of the evolution of stress in the gluten gel, we find that the onset of strongly non-linear unsteady phenomena such as edge instability in shear and sample rupture during extension can be understood as consequences of the finite extensibility and increased dissociation of the network filaments. (2008)] have shown that under small amplitude oscillatory conditions, as well as in large deformations in either shear or extension, the gluten gel can best be understood as consisting of flexible/semi-flexible segments that are interconnected to form a gel network. The interstitial spaces are filled with water but have minimal direct effect on the rheology as little or no solvent contribution to the total stress can be detected. For time scales that are greater than the Rouse relaxation time of the polymeric network segments, we also demonstrated that the quasi-linear behavior in an unfilled gluten gel is time-strain separable up to large strains and can be welldescribed by the generalized gel equation:
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I INTRODUCTIONwhere is the finger strain tensor. The expression can also be rewritten in terms of the finite strain rate tensor in the following way:( 2) where [Bird et al. (1987a)].Our previous studies also showed that in start-up ...