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Abstracts - KTH Mechanics

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Modelling Shear Flow Effects on the Fibre Orientation<br />

Distribution Function in a Planar Contraction<br />

M. Hyensjö ∗ and Anders Dahlkild †<br />

The effect of turbulence generating vanes and its location in a planar contraction<br />

on fibre orientation anisotropy was studied by mathematical modelling. We use single<br />

phase CFD modelling as an input for the fibre orientation dispersion model to study<br />

the effect of shear flow and turbulence in an accelerated fluid flow on fibre orientation<br />

anisotropy. The fibre dispersion model is based on a Fokker-Planck equation 1 ,which<br />

describes the evolution of the fibre orientation probability distribution function in a<br />

flow field. We consider a plane case, for one orientation angle in the symmetry plane 2<br />

of the contraction, and also the case of a 3D fibre orientation described with two<br />

orientation angles. The rotational angular velocities are based on the flow around a<br />

fibre with high aspect ratio, but without spatial extension 3 . The two models have<br />

been compared to experimental data 4 . For different streamlines in the contracting<br />

channel, the fibre orientation distribution function is obtained numerically, and the<br />

fibre orientation anisotropy could be studied along streamlines near the vane wall<br />

and vane tip and further away downstream. In figure 1 (a), (b) and (c) example on<br />

outlet fibre orientation distributions are shown for a wake, a undisturbed region and<br />

a wall boundary layer respectively. A higher degree of orientation can be seen in the<br />

undisturbed region, i.e. cf. figure 1 (b). In the wake region, cf. figure 1 (a), for a<br />

plane γ=0, the preferred orientation angle is shifted towards β values smaller than π<br />

/2, i.e. fibres are oriented upwards, the opposite effect is shown for the wall boundary<br />

layer, cf. figure 1 (c). For the wake region of the outlet profile of the contraction<br />

the fibre orientation anisotropy was decreased by moving the vane tip closer to the<br />

outlet.<br />

Figure 1: (a) The wake region. (b) The undisturbed region. (c) The boundary layer<br />

∗ Metso Paper Karlstad AB, SE-651 15 Karlstad, Sweden.<br />

† <strong>KTH</strong> <strong>Mechanics</strong> OB 18, SE-100 44 Stockholm, Sweden.<br />

1 Advani and Tucker, Journal of Rheology, 31(8) (1987).<br />

2 Hyensjö, Krochak, Olson, Hämäläinen and Dahlkild, In Proc. ICMF’04, Yokohama, (2004).<br />

3 Jeffrey, Proc. R. Soc., 102(A) (1922).<br />

4 Asplund and Norman, Journal of Pulp and Paper Science, 30(8) (2004).<br />

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