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Straight simulation mode

The rates of relaxation of the first and the third modes of macromolecule of length M = 25Me (x = 0.04, B = 429, ip = 8.27). The results calculated from analytical correlation function (4.29) are depicted by solid lines. By straight dashed lines, the values of the relaxation times due to the Doi-Edwards model are presented. The circles (for the first mode) and squares (for the third mode) depict the results of simulation for above values of parameters ip and B and values of parameters of local anisotropy ae = 0.3, cq = 0.06. Adapted from Pokrovskii (2006). [Pg.75]

Abstract This chapter deals with capillary instability of straight free liquid jets moving in air. It begins with linear stability theory for small perturbations of Newtonian liquid jets and discusses the unstable modes, characteristic growth rates, temporal and spatial instabilities and their underlying physical mechanisms. The linear theory also provides an estimate of the main droplet size emerging from capillary breakup. Formation of satellite modes is treated in the framework of either asymptotic methods or direct numerical simulations. Then, such additional effects like thermocapiUarity, or swirl are taken into account. In addition, quasi-one-dimensional approach for description of capillary breakup is introduced and illustrated in detail for Newtonian and rheologically complex liquid jets (pseudoplastic, dilatant, and viscoelastic polymeric liquids). [Pg.3]

To help understand and quantitatively evaluate the secondary movement shown above, Debbaut et al. [75, 77] augmented this experimental work with a three-dimensional flow simulation that incorporated viscoelastic effects. The finite element method, using a 4-mode Giesekus model as the viscoelastic constitutive equation, was used for the simulation. The polymer used for the experiment and simulation was a low-density polyethylene. Figures 12.20 and 12.21 show the experimental observations and the numerical predictions of the deformations of the interface for the rectangular straight channel [78], and for the teardrop channel [75], respectively. [Pg.891]


See other pages where Straight simulation mode is mentioned: [Pg.246]    [Pg.246]    [Pg.60]    [Pg.55]    [Pg.55]    [Pg.398]    [Pg.226]    [Pg.5]    [Pg.121]    [Pg.302]   


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