The upper layer, which is moving faster,
tries to draw the lower slowly moving layer along with it
by means of a force F along the direction of flow
on this layer. Similarly, the lower layer tries to retard
the upper one, according to Newton's third law, with an
equal and opposite force F on it (Figure 1.6).
Such a fluid flow where x-direction velocities, for
example, change with y-coordinate is called shear flow
of the fluid.
Thus, the dragging effect of one layer
on the other is experienced by a tangential force F
on the respective layers. If F acts over an
area of contact A, then the shear stress
τ is defined as