 # Shear rate

Shear rate is the rate at which a progressive shearing deformation is applied to some material.

## Simple shear

The shear rate for a fluid flowing between two parallel plates, one moving at a constant speed and the other one stationary (Couette flow), is defined by

${\dot {\gamma }}={\frac {v}{h}},$ where:

• is the shear rate, measured in reciprocal seconds;
• v is the velocity of the moving plate, measured in meters per second;
• h is the distance between the two parallel plates, measured in meters.

Or:

${\dot {\gamma }}_{ij}={\frac {\partial v_{i}}{\partial x_{j}}}+{\frac {\partial v_{j}}{\partial x_{i}}}.$ For the simple shear case, it is just a gradient of velocity in a flowing material. The SI unit of measurement for shear rate is s−1, expressed as "reciprocal seconds" or "inverse seconds".

The shear rate at the inner wall of a Newtonian fluid flowing within a pipe is

${\dot {\gamma }}={\frac {8v}{d}},$ where:

• is the shear rate, measured in reciprocal seconds;
• v is the linear fluid velocity;
• d is the inside diameter of the pipe.

The linear fluid velocity v is related to the volumetric flow rate Q by

$v={\frac {Q}{A}},$ where A is the cross-sectional area of the pipe, which for an inside pipe radius of r is given by

$A=\pi r^{2},$ thus producing

$v={\frac {Q}{\pi r^{2}}}.$ Substituting the above into the earlier equation for the shear rate of a Newtonian fluid flowing within a pipe, and noting (in the denominator) that d = 2r:

${\dot {\gamma }}={\frac {8v}{d}}={\frac {8\left({\frac {Q}{\pi r^{2}}}\right)}{2r}},$ which simplifies to the following equivalent form for wall shear rate in terms of volumetric flow rate Q and inner pipe radius r:

${\dot {\gamma }}={\frac {4Q}{\pi r^{3}}}.$ For a Newtonian fluid wall, shear stress (τw) can be related to shear rate by τw = xμ, where μ is the dynamic viscosity of the fluid. For non-Newtonian fluids, there are different constitutive laws depending on the fluid, which relates the stress tensor to the shear rate tensor.

This page was last updated at 2021-03-22 20:18, View original page

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