What is the difference between strain rate and velocity gradient?

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Strain rate and velocity gradient in a Newtonian fluid are equivalent and directly proportional to shear stress, linked by the second viscosity coefficient. The normal shear stress in the x-direction can be expressed with the equation τ_{xx} = λ(∇·V) + 2μ(∂u/∂x), highlighting the velocity gradient's role. The coefficient λ, which is challenging to measure, is often approximated using Stoke's Hypothesis, where λ is assumed to be -2/3μ. This relationship is crucial for understanding fluid dynamics and the behavior of Newtonian fluids under shear. Overall, the discussion emphasizes the mathematical connection between strain rate, velocity gradient, and shear stress in fluid mechanics.
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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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