What is the difference between strain rate and velocity gradient?

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SUMMARY

The discussion clarifies that for a Newtonian fluid, strain rate and velocity gradient are equivalent and directly proportional to shear stress, governed by the second viscosity coefficient. The equation for normal shear stress in the x-direction is expressed as τxx = λ (∇·V) + 2μ(∂u/∂x), highlighting the velocity gradient's role. It is noted that λ is challenging to measure, leading to the application of Stoke's Hypothesis, which simplifies λ to -2/3μ for practical calculations.

PREREQUISITES
  • Understanding of Newtonian fluid dynamics
  • Familiarity with shear stress concepts
  • Knowledge of viscosity coefficients
  • Basic grasp of vector calculus
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  • Study the implications of Stoke's Hypothesis in fluid dynamics
  • Explore the measurement techniques for viscosity coefficients
  • Learn about the mathematical derivation of shear stress equations
  • Investigate the differences between Newtonian and non-Newtonian fluids
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Fluid dynamics engineers, researchers in material science, and students studying rheology will benefit from this discussion.

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What is the difference between strain rate and velocity gradient of a Newtonian fluid?
 
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For a Newtonian fluid, they are the same, which is proportional to the the shear stress. They are proportional by the second viscosity coefficient. For example, the normal shear stress in the x-direction is given by:

\tau_{xx} = \lambda (\vec{\nabla}\cdot\vec{V})+2\mu\frac{\partial u}{\partial x}
You can see the velocity gradient term in there, with the leading coefficient being the proportional part. Do note that \lambda is hard to measure, and this is where Stoke's Hypothesis (see number fudge so the equations can be solved) comes into play, where we just assume that:
\lambda = -\frac{2}{3}\mu
 

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