Related Experiment Video
Updated: May 7, 2026

06:42
Magnetically Induced Rotating Rayleigh-Taylor Instability
Published on: March 3, 2017
9.2K
Minimal model for zero-inertia instabilities in shear-dominated non-Newtonian flows
S Boi1, A Mazzino, J O Pralits
1Physics Department, University of Genova, Via Dodecaneso 33, 16146 Genova, Italy.
Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|October 16, 2013
Summary
Fluid instabilities emerge in rheopectic fluids due to shear-induced viscosity changes. This study investigates these instabilities in Kolmogorov flow at low Reynolds numbers, offering insights for microfluidic applications.
Area of Science:
- Fluid dynamics
- Non-Newtonian fluid mechanics
- Rheology
Background:
- Fluid instabilities are crucial for mixing, but often inhibited in low-inertia systems like microfluidics.
- Kolmogorov flow, a benchmark system, is examined for instability emergence near zero Reynolds number.
- Non-Newtonian fluid behavior, specifically finite-time viscosity changes, is key to instability onset.
Purpose of the Study:
- Investigate the emergence of fluid instabilities in Kolmogorov flow at vanishing fluid inertia (low Reynolds number).
- Identify the critical role of finite-time shear-induced microstructural transitions and viscosity changes in instability formation.
- Determine the conditions under which instabilities emerge in different classes of non-Newtonian fluids.
Main Methods:
- Renormalized perturbative expansions (multiple-scale expansions) were employed.
- Energy-based arguments on linearized equations of motion were utilized.
- Numerical analysis of eigenvalue problems from linear stability analysis provided key data.
Main Results:
- Instabilities emerge in rheopectic fluids due to finite-time, shear-induced order-disorder transitions and viscosity increases.
- No instabilities were observed in shear-thinning or shear-thickening fluids with instantaneous viscosity adjustments.
- Thixotropic fluids, despite finite viscosity adjustment times, also did not exhibit instabilities at low Reynolds numbers.
Conclusions:
- Finite-time viscosity changes are essential for hydrodynamic instabilities in low-inertia flows.
- Non-Newtonian fluids offer potential solutions for triggering mixing in microfluidic applications.
- The findings open new avenues for research in smart fluid materials and hydrodynamic control.
More Related Videos
Related Concept Videos
Newtonian Fluid: Problem Solving
1.1K
Newtonian fluids exhibit a constant viscosity, meaning their shear stress and shear strain rate are directly proportional. This property ensures a predictable and stable response to applied forces, maintaining a linear relationship between force and flow. Examples include water, air, and light oils, consistently demonstrating this proportional behavior regardless of external conditions.
A velocity gradient forms within the fluid when a Newtonian fluid is placed between two parallel plates, with...
A velocity gradient forms within the fluid when a Newtonian fluid is placed between two parallel plates, with...
1.1K
Irrotational Flow
1.3K
Irrotational flow is characterized by fluid motion where particles do not rotate around their axes, resulting in zero vorticity. For a flow to be irrotational, the curl of the velocity field must be zero. This imposes specific conditions on velocity gradients. For instance, to maintain zero rotation about the z-axis, the gradient condition:
1.3K
Navier–Stokes Equations
2.8K
For incompressible Newtonian fluids, where density remains constant, stresses show a linear relationship with the deformation rate, defined by normal and shear stresses. Normal stresses depend on the pressure exerted on the fluid and the rate of deformation in specific directions, which determines how fluid flows under varying pressures. Shear stresses, on the other hand, act tangentially across fluid layers. They explain how adjacent fluid layers slide relative to one another, connecting...
2.8K
Euler's Equations of Motion
1.1K
In fluid mechanics, shear stresses arise from viscosity, which represents a fluid's internal resistance to deformation. For low-viscosity fluids, like water, these stresses are minimal, simplifying flow analysis by allowing the fluid to be treated as inviscid, or frictionless. In an inviscid fluid, shear stresses are absent, leaving only normal stresses, which act perpendicularly to fluid elements. Notably, pressure — defined as the negative of the normal stress — remains uniform...
1.1K
Steady, Laminar Flow Between Parallel Plates
1.1K
Understanding steady, laminar flow between parallel plates is essential for analyzing and designing flow in narrow rectangular channels, commonly found in various water conveyance and drainage systems. The Navier-Stokes equations govern fluid motion and are generally challenging to solve due to their nonlinearity. However, simplifications are possible in certain cases, like the steady laminar flow between parallel plates. For this scenario, we assume steady, incompressible, laminar flow.
1.1K
Typical Model Studies
870
Fluid mechanics model studies often utilize scaled-down systems to predict fluid behavior in full-scale environments, such as river flows, dam spillways, and structures interacting with open surfaces. Maintaining Froude number similarity in river models is crucial, as it replicates surface flow features like wave patterns and velocities.
870

