So then, for the free-body diagram, how come we don't have to
consider six planes ? the positive and negative z planes, the positive and negative
y planes, and the positive and negative x planes ?
Ok. So considering the free body diagram,
how come we don't consider all six faces?
(i.e. are we considering a rectangular prism
of water or is it more of a cylinder with shells? )
I
I'm familiar with shear stress.
I've just been introduced to viscocity.
At the wall of the pipe, I'd imagine that the velocity would be almost zero.
I would imagine that u(r) increases as it moves closer to the center of the pipe.
Unfortunately, I only have access to Fluid Mechanics (seventh edition) by Frank White.
I looked up the Navier Stokes equations there and all I'm getting are a bunch of general-case partial
derivative equations (e.g. du/dx + dv/dy = 0 ).
I must not be getting it; can someone please either...
Ok, Thanks. So, do the Navier Stokes equations include this specific equation?
Or am I supposed to derive the u(r) equation using the Stokes equations ?
By the way, my textbook is Fluid Mechanics by Frank M. White, so if possible, could somebody tell me which chapter this type of problem is...
Homework Statement
For low-speed(laminar) , steady flow through a circular pipe, the velocity u varies with radius and takes what form? Please see this link for picture of the pipe...