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Turbulent flow of non-Newtonian liquids through an axisymmetric sudden expansion Rob Poole Department of Engineering, University of Liverpool Osborne Reynolds.

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Presentation on theme: "Turbulent flow of non-Newtonian liquids through an axisymmetric sudden expansion Rob Poole Department of Engineering, University of Liverpool Osborne Reynolds."— Presentation transcript:

1 Turbulent flow of non-Newtonian liquids through an axisymmetric sudden expansion Rob Poole Department of Engineering, University of Liverpool Osborne Reynolds Seminar 30th April 2003

2 Introduction Osborne Reynolds Seminar 30th April 2003 Osborne Reynolds (1883,1895) Newtonian flows - large literature exists Non-Newtonian - Few previous studies [Pak et al (1990)] –Experimental: flow visualisation Aims of this study –Use of LDA to provide quantitative data –Investigate effect on reattachment length –Database for CFD validation

3 Osborne Reynolds Seminar 30th April 2003 Experimental rig Fully developed pipe flow d= 26 mmD=52 mm R = D 2 / d 2 = 4

4 Osborne Reynolds Seminar 30th April 2003 Working fluids Water Three concentrations of polyacrylamide (PAA) –0.02%, 0.05% and 0.1% –Shear thinning to various degrees –Increasing viscoelasticity with concentration –Large extensional viscosities –Highly drag reducing –Optically transparent

5 Osborne Reynolds Seminar 30th April 2003 Working fluids cont… Rheological data obtained –Shear viscosity vs shear rate –First normal stress difference vs shear stress N1N1

6 Osborne Reynolds Seminar 30th April 2003 Rheological data 0.02% PAA 0.05% PAA 0.1% PAA

7 Osborne Reynolds Seminar 30th April 2003 Rheological data cont … 0.1% PAA

8 Osborne Reynolds Seminar 30th April 2003 Estimation of Reynolds number Difficulty - no single value for the viscosity characterises the fluid. Method adopted - estimate the maximum shear rate at ‘inlet’ (x/h=1). Example 0.02% PAA

9 Osborne Reynolds Seminar 30th April 2003 Estimation of Reynolds number This shear rate is then used to obtain a viscosity from the Carreau-Yasuda model: μ C  2.82 x10 -3 Pa.s Hence a Reynolds number of

10 Mean axial velocity profiles Osborne Reynolds Seminar 30th April 2003 0.02% PAA Water

11 Streamlines Water -0.08<  <0 [0.02 steps] 0<  <0.35 [0.05 steps] 0.02% PAA -0.09<  <-0.01 [0.02 steps] 0<  <0.3 [0.05 steps] Osborne Reynolds Seminar 30th April 2003

12 Axial Reynolds stresses (u) Osborne Reynolds Seminar 30th April 2003 0.02% PAA Water

13 Radial Reynolds stresses (v) Osborne Reynolds Seminar 30th April 2003 0.02% PAA Water

14 Osborne Reynolds Seminar 30th April 2003 0.1% PAA Re  4000 X R  32 Mean axial velocity profiles No recirculation

15 Osborne Reynolds Seminar 30th April 2003 Concluding remarks Turbulent flow through an axisymmetric sudden expansion of area expansion ratio (i.e. D 2 /d 2 ) 4. Water and two lowest conc. of PAA - axisymmetric. Reattachment lengths were Water X R  10 step heights 0.02% and 0.05% PAA X R  20 step heights

16 Osborne Reynolds Seminar 30th April 2003 Concluding remarks cont… Increase in X R caused by modifications to turbulence structure with large reductions in v and w resulting in reduced transverse transfer of axial momentum. At highest conc. of PAA axisymmetric flow could not be achieved. This could be due to an elastic instability or a slight geometric imperfection that is accentuated by viscoelasticity.


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