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Related Concept Videos

Newtonian Fluid: Problem Solving01:18

Newtonian Fluid: Problem Solving

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...
Navier–Stokes Equations01:28

Navier–Stokes Equations

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...
Euler's Equations of Motion01:28

Euler's Equations of Motion

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 across...
Symmetry in Maxwell's Equations01:28

Symmetry in Maxwell's Equations

Once the fields have been calculated using Maxwell's four equations, the Lorentz force equation gives the force that the fields exert on a charged particle moving with a certain velocity. The Lorentz force equation combines the force of the electric field and of the magnetic field on the moving charge. Maxwell's equations and the Lorentz force law together encompass all the laws of electricity and magnetism. The symmetry that Maxwell introduced into his mathematical framework may not be...
Differential Form of Maxwell's Equations01:17

Differential Form of Maxwell's Equations

James Clerk Maxwell (1831–1879) was one of the significant contributors to physics in the nineteenth century. He is probably best known for having combined existing knowledge of the laws of electricity and the laws of magnetism with his insights to form a complete overarching electromagnetic theory, represented by Maxwell's equations. The four basic laws of electricity and magnetism were discovered experimentally through the work of physicists such as Oersted, Coulomb, Gauss, and Faraday.
Steady, Laminar Flow Between Parallel Plates01:17

Steady, Laminar Flow Between Parallel Plates

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.

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Updated: Jul 6, 2026

Magnetically Induced Rotating Rayleigh-Taylor Instability
06:42

Magnetically Induced Rotating Rayleigh-Taylor Instability

Published on: March 3, 2017

Shear-induced chaos in nonlinear Maxwell-model fluids.

Chris Goddard1, Ortwin Hess, Alexander G Balanov

  • 1Advanced Technology Institute, School of Electronics and Physical Sciences, University of Surrey, Guildford, GU2 7XH, United Kingdom. c.goddard@surrey.ac.uk

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|March 21, 2008
PubMed
Summary

This study explores complex fluid dynamics in non-Newtonian fluids, revealing nonlinear responses and deterministic chaos under specific flow conditions. Researchers mapped chaotic behaviors using Lyapunov exponents and bifurcation analysis, identifying key stability loss mechanisms.

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Studying Large Amplitude Oscillatory Shear Response of Soft Materials
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Magnetically Induced Rotating Rayleigh-Taylor Instability
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Area of Science:

  • Fluid Dynamics
  • Non-Newtonian Fluid Mechanics
  • Chaos Theory

Background:

  • Non-Newtonian fluids exhibit complex stress tensor behavior.
  • Understanding their dynamics is crucial for various industrial applications.
  • Previous models often simplify these complex responses.

Purpose of the Study:

  • To investigate a generalized model for stress tensor behavior in non-Newtonian fluids.
  • To analyze nonlinear responses and deterministic chaos in plane Couette flow.
  • To identify parameters and mechanisms driving complex fluid dynamics.

Main Methods:

  • Utilized a generalized model for stress tensor analysis.
  • Simulated spatially homogeneous plane Couette flow.
  • Employed largest Lyapunov exponent for chaos mapping.
  • Conducted bifurcation diagrams and stability analysis.

Main Results:

  • Observed a variety of nonlinear responses and deterministic chaos.
  • Identified shear rate and temperature/density as key parameters influencing chaos.
  • Revealed rich dynamics through bifurcation and stability analyses.
  • Identified Hopf, saddle-node, and period-doubling bifurcations as stability loss mechanisms.

Conclusions:

  • The generalized model effectively captures complex dynamics in non-Newtonian fluids.
  • Nonlinear responses and chaos are inherent in these systems under specific conditions.
  • Bifurcation analysis provides insights into the transition to chaotic behavior.