Complex Fluids Research
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Research Interests

  • Fluid Mechanics

  • Complex Flows

  • Interfacial Flows

  • Non-Newtonian Fluids

  • Highlighted Current Research

    Here you can find out about some of our recent research directions. For more, click on our publication page or contact us via email. We always seek new ideas and collaborations!

      Buoyant miscible displacement flows in rectangular channels

      Abstract: Buoyant displacement flows of two miscible fluids in rectangular channels are studied, theoretically and experimentally. The scenario considered involves the displacement of a fluid by a slightly heavier one in nearly-horizontal channel inclinations, where inertial effects are weak and laminar stratified flows may be expected. In the theoretical part, a lubrication approximation model is developed to simplify the displacement flow governing equations and furnish a semi-analytical solution for the heavy and light fluid flux functions. Three key dimensionless parameters govern the fluid flow motion, i.e., a buoyancy number, the viscosity ratio and the channel cross section aspect ratio. When these parameters are specified, the reduced model can deliver the interface propagation in time, leading and trailing front heights, shapes and speeds, cross sectional velocity fields, etc. In addition, the model can be exploited to provide various classifications such as single or multiple fronts as well as main displacement flow regimes at long times such as no-sustained-backflows, stationary interface flows and sustained-backflows. Focusing on the variation of the buoyancy number, a large number of iso-viscous displacement experiments are performed in a square duct and the results are compared with those of the lubrication model. Qualitative displacement flow features observed in the theory and experiments are in good agreement, in particular, in terms of the main displacement flow regimes. The quantitative comparisons are also reasonable for small and moderate imposed displacement flow velocities. However, at large flow rates, a deviation of the experimental results from the model results is observed, which may be due to the presence of non-negligible inertial effects.

      Sample publication: S.M. Taghavi, R. Mollaabbasi and Y. St-Hilaire. Buoyant miscible displacement flows in rectangular channels. Journal of Fluid Mechanics 826, 676-713 (2017). [doi]

      Displacement flows in moving geometry

      Abstract: In the present work, we experimentally study displacement flows of two Newtonian, miscible fluids in a long, vertical moving pipe while comparing the results with the corresponding displacement flows in a stationary pipe. When in motion, the pipe slowly oscillates like an inverted pendulum. The two fluids have a small density difference and a nearly-identical viscosity. The denser displacing fluid is placed above the displaced fluid. Overall, our buoyant displacement flows in a moving pipe are at least controlled by three dimensionless groups, namely the Reynolds number, the densimetric Froude number, and the Rossby number. Experimental images of the penetrating front of the heavy displacing fluid into the light displaced one have been analyzed for a wide range of the dimensionless groups. In particular, three different flow regimes are observed for displacement flows in a moving pipe: a stable flow that is non-diffusive (for Re/Ro ≲ O(102) & Re/Fr2<35), a stable-diffusive flow (for Re/Ro≳ O(102) & Re/Fr2<35) and an unstable-diffusive flow (for Re/Fr2 >35).

      Collaborators: Professor F. Larachi at Université Laval.

      Sample publication: A. Amiri, F. Larachi and S.M. Taghavi. Displacement flows in periodically moving pipe: Understanding multiphase flows hosted in oscillating geometry {Invited Article}. Chemical Engineering Science 170, 437-450 (2017). [doi]

      Buoyant displacement flows in slightly non-uniform channels

      Abstract: We consider displacement flows in slightly diverging or converging plane channels. The two fluids are miscible and buoyancy is significant. We assume that the channel is oriented close to horizontal. Employing a classical lubrication approximation, we simplify the governing equations to furnish a semi-analytical solution for the flux functions. Then, we demonstrate how the non-uniformity of the displacement flow geometry can affect the propagation of the interface between the heavy and light fluids in time, for various parameters studied, e.g. the viscosity ratio, a buoyancy number and rheological features. By setting diffusion effects to zero, certain solution behaviours at longer times can be practically predicted through the associated hyperbolic problem, using which it becomes possible to directly compute the interfacial features of interest, e.g. leading and trailing front heights and speeds.

      Sample publication: R. Mollaabbasi and S.M. Taghavi. Buoyant displacement flows in slightly non-uniform channels. Journal of Fluid Mechanics 795, 876-913 (2016). [doi]

      A model for nanofibre formation in centrifugal spinning methods

      Abstract: We develop a general regularized thin-fibre (string) model to predict the properties of non-Newtonian fluid fibres generated by centrifugal spinning. In this process the fibre emerges from a nozzle of a spinneret that rotates rapidly around its axis of symmetry, in the presence of centrifugal, Coriolis, inertial, viscous/shear-thinning, surface tension and gravitational forces. We analyse the effects of five important dimensionless groups, namely, the Rossby number (Rb), the Reynolds number (Re), the Weber number (We), the Froude number (Fr) and a power-law index (m), on the steady state trajectory and thinning of fibre radius. In particular, we find that the gravitational force mainly affects the fibre vertical angle at small arc lengths as well as the fibre trajectory. We show that for small Rb, which is the regime of nanofibre formation in centrifugal spinning methods, rapid thinning of the fibre radius occurs over small arc lengths, which becomes more pronounced as Re increases or m decreases. At larger arc lengths, a relatively large We results in a spiral trajectory regime, where the fibre eventually recovers a corresponding inviscid limit with a slow thinning of the fibre radius as a function of the arc length. Viscous forces do not prevent the fibre from approaching the inviscid limit, but very strong surface tension forces may do so as they could even result in a circular trajectory with an almost constant fibre radius. We divide the spiral and circular trajectories into zones of no thinning, intense thinning and slow or ceased thinning, and for each zone we provide simple expressions for the fibre radius as a function of the arc length.

      Collaborators: Professor R.G. Larson at The University of Michigan and Dr. W. Arne at Fraunhofer Institute for Industrial Mathematics.

      Sample publication: Noroozi, H. Alamdari, W. Arne, R.G. Larson and S.M. Taghavi. Regularized string model for nanofibre formation in centrifugal spinning methods. Journal of Fluid Mechanics 822, 202-234 (2017). [doi]

      Viscous fingering regimes in elasto-visco-plastic fluids

      Abstract: We experimentally study the Saffman-Taylor instability of air invasion into a non-Newtonian fluid (i.e., Carbopol solution) in a rectangular Hele-Shaw cell. In addition to viscous features, the non-Newtonian fluid used exhibits yield stress, shear-thinning as well as elastic behaviors. The key dimensionless parameters that govern the various flow regimes are the Bingham number (Bn), the capillary number (Ca), the Weber number (We), the Weissenberg number (Wi), the channel aspect ratio (δ ≫ 1), and the shear- thinning power-law index (n). Three main flow regimes are observed, i.e., a yield stress regime, a viscous regime and an elasto-inertial regime. We present a detailed description for each regime and quantify their transition boundaries versus dimensionless groups. Some of the secondary flow aspects, e.g., the wall residual layer thickness and a network structure regime, have been also studied.

      Sample publication: A. Eslami and S.M. Taghavi. Viscous fingering regimes in elasto-visco-plastic fluids. Journal of Non-Newtonian Fluid Mechanics 243, 79-94 (2017). [doi]

      A microfluidic model for non-intrusive biofilm viscosity measurements

      Abstract: Straight, low-aspect ratio micro flow cells are used to support biofilm attachment and preferential accumulation at the short side-wall, which progressively reduces the effective channel width. The biofilm shifts downstream at measurable velocities under the imposed force from the constant laminar co-flowing nutrient stream. The dynamic behaviour of the biofilm viscosity is modeled semi-analytically, based on experimental measurements of biofilm dimensions and velocity as inputs. The technique advances the study of biofilm mechanical properties by strongly limiting biases related to non-Newtonian biofilm properties (e.g., shear dependent viscosity) with excellent time resolution. To demonstrate the proof of principle, young Pseudomonas sp. biofilms were analyzed under different nutrient concentrations and constant micro-flow conditions. The striking results show that large initial differences in biofilm viscosities grown under different nutrient concentrations become nearly identical in less than one day, followed by a continuous thickening process. The technique verifies that in 50 h from inoculation to early maturation stages, biofilm viscosity could grow by over 2 orders of magnitude. The approach opens the way for detailed studies of mechanical properties under a wide variety of physiochemical conditions, such as ionic strength, temperature, and shear stress.

      Collaborators: Professor J. Greener at Université Laval.

      Sample publication: J. Greener, M. Parvinzadeh Gashti, A. Eslami, M.P. Zarabadi, S.M. Taghavi. A microfluidic method and custom model for continuous, non-intrusive biofilm viscosity measurements under different nutrient conditions. Biomicrofluidics 10 (6), 064107 (2016). [doi]