Wall shear stress definitions Good afternoon everyone.
In defining the shear velocity at the wall $u_\tau=\sqrt{\frac{\tau_w}{\rho}}$ for the incompressible turbulence, $w$ being the wall, I found in some literature that this relation holds:
$$\tau_w=\mu \frac{\partial U}{\partial y}|_{y=0}= -\frac{\partial p_w}{\partial x}$$
$p$ being the pressure, $\mu$ the dynamic viscosity and $x$ the direction of the flow velocity $U$.
However I don't know neither if the second equality is correct or where it comes from. Could anyone help?
 A: I'm trying to show the second equality, what I've done so far:
From Navier-Stokes (incompressible) in the x direction (take z also along the wall and y orthogonal to them, assuming no field forces) and let $\mathbf{u} = u \mathbf{i} + v \mathbf{j} + w \mathbf{k}$:
$$\rho \frac{D u}{Dt} = \mu \Delta u - \frac{\partial p}{\partial x} + \rho g_x$$
notice that the particle is stopped (zero constant velocity and partial derivatives of it along x and z) along the wall ("no slip") and therefore, from the Lagrangian frame, it has zero (material) derivative. It will reduce to:
$$\mu \frac{\partial^2 u}{\partial y^2} = \frac{\partial p}{\partial x}$$
but I don't know what to do from here. Maybe the sign will be reversed since the shear stress in the fluid is a reaction to the shear stress in the wall?
Edit: checking the dimensions, could it happen that something is wrong with the equality? Since the first two terms evaluate to Pa, and the final one to Pa/m.
Using the reasoning above, could it be something like $$\frac{\partial \tau_w}{\partial y} = -\frac{\partial p_w}{\partial x}$$?
