In physics, shear rate is the rate at which a progressive shear strain is applied to some material, causing shearing to the material. Shear rate is a measure of how the velocity changes with distance.
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
\gamma |
=
v | |
h |
,
where:
\gamma |
Or:
\gamma |
ij=
\partialvi | |
\partialxj |
+
\partialvj | |
\partialxi |
.
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".[1] However, when modelling fluids in 3D, it is common to consider a scalar value for the shear rate by calculating the second invariant of the strain-rate tensor
\gamma |
=\sqrt{2\varepsilon:\varepsilon}
The shear rate at the inner wall of a Newtonian fluid flowing within a pipe[2] is
\gamma |
=
8v | |
d |
,
where:
\gamma |
The linear fluid velocity is related to the volumetric flow rate by
v=
Q | |
A |
,
where is the cross-sectional area of the pipe, which for an inside pipe radius of is given by
A=\pir2,
thus producing
v=
Q | |
\pir2 |
.
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 :
\gamma |
=
8v | |
d |
=
| |||||
2r |
,
which simplifies to the following equivalent form for wall shear rate in terms of volumetric flow rate and inner pipe radius :
\gamma |
=
4Q | |
\pir3 |
.
For a Newtonian fluid wall, shear stress can be related to shear rate by
\tauw=
\gamma |
x\mu