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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...
Types of Fluids01:27

Types of Fluids

Fluids can be classified into Newtonian and non-Newtonian fluids based on their response to shear stress. Newtonian fluids have a linear relationship between shear stress and the shear strain rate, following Newton's law of viscosity. Their viscosity remains constant regardless of the shear rate, making their behavior predictable and easier to analyze. Common examples include water, air, oil, and gasoline.
In contrast, non-Newtonian fluids do not follow Newton's law of viscosity, and their...
Elastic Strain Energy for Shearing Stresses01:20

Elastic Strain Energy for Shearing Stresses

As discussed in previous lessons, strain energy in a material is the energy stored when it is elastically deformed, a concept crucial in materials science and mechanical engineering. This energy results from the internal work done against the cohesive forces within the material. When a material undergoes shearing stress and corresponding shearing strain, the strain energy density, which is the energy stored per unit volume, is calculated. Within the elastic limit, where the stress is...
Shearing Stress01:18

Shearing Stress

Shearing stress, denoted by the Greek letter tau (τ), is stress caused by forces acting transversely on an object. These forces create internal ones within the entity in the plane where the external forces are applied. The resultant of these internal forces is the shear in the section.
The average shearing stress can be calculated by dividing the shear by the area of the cross-section.
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...
Dimensionless Groups in Fluid Mechanics01:15

Dimensionless Groups in Fluid Mechanics

Dimensionless groups in fluid mechanics provide simplified ratios that help analyze fluid behavior without relying on specific units. The Reynolds number (Re), which represents the ratio of inertial to viscous forces, distinguishes between laminar and turbulent flows, making it essential in the design of pipelines and aerodynamic surfaces. The Froude number (Fr), the ratio of inertial to gravitational forces, is particularly useful in predicting wave formation and hydraulic jumps in...

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Related Experiment Video

Updated: May 13, 2026

Studying Large Amplitude Oscillatory Shear Response of Soft Materials
06:07

Studying Large Amplitude Oscillatory Shear Response of Soft Materials

Published on: April 25, 2019

Transient shear banding in time-dependent fluids.

Xavier Illa1, Antti Puisto, Arttu Lehtinen

  • 1Departament d'Estructura i Constituents de la Matèria, Facultat de Física, Universitat de Barcelona, Diagonal, 647, E-08028 Barcelona, Catalonia, Spain.

Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|March 19, 2013
PubMed
Summary

This study explains transient shear banding in fluids using a simple rheological model. A positive feedback loop between flow and viscosity drives nonhomogeneous shear distribution, clarifying dynamic effects in time-dependent fluids.

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Area of Science:

  • Fluid dynamics
  • Rheology
  • Material science

Background:

  • Shear banding is a common phenomenon in complex fluids.
  • Understanding its dynamics is crucial for material processing and applications.
  • Previous models often simplified the interplay between local structure and flow.

Purpose of the Study:

  • To investigate the dynamics of shear-band formation and evolution.
  • To explain transient shear banding in time-dependent fluids.
  • To provide a simple rheological model for these phenomena.

Main Methods:

  • Utilized a simple rheological model coupled with local structure and viscosity.
  • Employed the Couette geometry for detailed analysis.
  • Solved the model iteratively with the Navier-Stokes equation.
  • Obtained time evolution of local velocity and viscosity fields.

Main Results:

  • Identified nonhomogeneous shear distribution as the cause of dynamic effects.
  • Demonstrated a positive feedback mechanism between flow field and shear-thinning fluid viscosity.
  • Successfully explained transient shear banding observations.

Conclusions:

  • The proposed model offers a straightforward explanation for transient shear banding.
  • The findings are applicable to various time-dependent fluids.
  • The model can be extended to more complex rheological systems.