Fluid Mechanics: 2D Laminar Flow

AI Thread Summary
The discussion focuses on the analysis of a two-dimensional incompressible laminar boundary layer on a flat surface. The boundary layer approximation is given by a specific velocity profile equation, with δ defined as a function of the distance along the surface. Participants clarify the application of the continuity equation and the need for a derivative term dδ/dx in the x-component of velocity. The chain rule is identified as the method to derive this term, emphasizing its relevance in differentiating functions of multiple variables. Understanding these concepts is crucial for solving problems related to laminar flow in fluid mechanics.
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Homework Statement


A reasonable approximation for the two-dimensional incompressible laminar boundary layer on the flat surface in Fig. P4.17 is

u ≈ U(2*(y/δ) - 6*(y34) + y44)

δ = Cx1/2 where C is a constant

y ≤ δ

Homework Equations

The Attempt at a Solution


Incompressible so density is constant, 2D flow so no z component, continuity equation reduces to
∂u/∂x + ∂v/∂y = 0For the x component, I got [ (-2y/δ2) + (6*y34) - (4*y45) ]

But there is supposed to be a dδ/dx term attached to each term. Where does this term come from? Is it some kind of chain rule thing? Thanks!
 
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jdawg said:
U(2*(y/δ) - 6*(y34) + y44)
I assume you mean 6(y33).
jdawg said:
Is it some kind of chain rule thing?
Yes. ∂/∂x of f(y, z) where z is a function of x is given by ∂f/∂z dz/dx.
 
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