The Society of Rheology 88th Annual Meeting

February 12-16, 2017 - Tampa, Florida


NF24 


Non-Newtonian Fluid Mechanics & Instabilities


Quantitative predictions of the breakup times of inviscid-elastic filaments of dilute polymer solutions


February 16, 2017 (Thursday) 10:50


Track 2 / Audubon A

(Click on name to view author profile)

  1. Shahid, Taisir (KU Leuven, Department of Chemical Engineering)
  2. Mathues, Wouter (KU Leuven, Department of Chemical Engineering)
  3. Van Ruymbeke, Evelyne (Université catholique de Louvain, Bio and Soft Matter, Inst. on Cond. Matter and Nano-science)
  4. Clasen, Christian (KU Leuven, Department of Chemical Engineering)

(in printed abstract book)
Taisir Shahid1, Wouter Mathues1, Evelyne Van Ruymbeke2, and Christian Clasen1
1Department of Chemical Engineering, KU Leuven, Heverlee 3001, Belgium; 2Bio and Soft Matter, Inst. on Cond. Matter and Nano-science, Université catholique de Louvain, Louvain-la-Neuve B-1348, Belgium


Clasen, Christian


The applicability of dilute polymer solutions in free surface flow processes that involve a strong extensional component depends to a large extend on the longevity of the filament that forms after the development of a Rayleigh instability on an initial liquid bridge and that connects two consecutively forming droplets. Based on the analysis of V. Entov and J. Hinch [1], the stability and thinning dynamics of this liquid bridge has been described theoretically in great detail, and the predicted dynamics have been confirmed experimentally in several publications. In particular, a recent publication by C. Wagner et al. [2] describes an analytical solution for this elastocapillary (EC) balance regime, that allows a quantitative description of the breakup time for a known relaxation time and finite extensibility of the polymer in solutions, once the onset point of this EC regime I known. However, their analysis for the description of this onset point was based on the assumption of a viscid fluid. Since many dilute polymer in practical applications involve solvents that behave inviscid during filament thinning, we present in this paper an analytical solution for the evolution of the polymer stretch in an inviscid solvent, based on the FENE-P model, that allows us to quantitatively predict the breakup time of inviscid-elastic filaments. Predictions of this model are compared to experimental results for a number of model polymer solutions that span the relevant range of intrinsic Deborah and Elastocapillary numbers for actual applications.

[1] V.M. Entov, E.J. Hinch, JNNFM 72 (1997), 31-53. [2] C. Wagner, L. Bourouiba, G.H. McKinley, JNNFM 218 (2015), 53-61.