How to Approach the Prandtl Boundary Layer Equation for Steady Laminar Flow?

In summary, the conversation discusses the use of the Bernoulli equation for approaching a problem, but it is noted that this equation is only valid for inviscid flow and cannot account for a boundary layer. Instead, the conversation suggests using boundary layer theory in the free stream.
  • #1
sakif
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1
Homework Statement
Prove the following statement
Relevant Equations
Prandtl boundary layer equation for a two dimensional steady laminar flow of incompressible fluid over a semi infinite plate
I have tried to approach in the following way
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I am stuck. How should I approach this next.please help
 

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  • #2
I see you try to use the Bernoulli equation. But that is never going to work since that equation is only valid for inviscid flow. And in an inviscid flow no boundary layer can exist.
 
  • #3
Arjan82 said:
I see you try to use the Bernoulli equation. But that is never going to work since that equation is only valid for inviscid flow. And in an inviscid flow no boundary layer can exist.
Far from the boundary, in the free stream, it is valid to use the Bernoulli equation. That's what boundary layer theory is all about.
 

FAQ: How to Approach the Prandtl Boundary Layer Equation for Steady Laminar Flow?

What is the Prandtl boundary layer equation?

The Prandtl boundary layer equation is a simplified form of the Navier-Stokes equations that describe the flow of fluid near a solid boundary. It specifically addresses the behavior of the flow in the thin region called the boundary layer where viscous forces are significant. For a two-dimensional steady laminar flow, the equation can be written as:

\[ u \frac{\partial u}{\partial x} + v \frac{\partial u}{\partial y} = \nu \frac{\partial^2 u}{\partial y^2} \]

where \( u \) and \( v \) are the velocity components in the \( x \) and \( y \) directions respectively, and \( \nu \) is the kinematic viscosity of the fluid.

What assumptions are made in deriving the Prandtl boundary layer equation?

Several key assumptions are made in deriving the Prandtl boundary layer equation:1. The flow is steady and laminar.2. The flow is two-dimensional.3. The boundary layer is thin compared to the characteristic length scale of the problem.4. The pressure gradient in the direction normal to the boundary is negligible.5. The velocity component normal to the boundary is much smaller than the velocity component parallel to the boundary.

How does the boundary layer thickness vary along a flat plate?

The boundary layer thickness \(\delta(x)\) on a flat plate increases with the distance \( x \) from the leading edge of the plate. For a laminar boundary layer, the thickness can be estimated using the Blasius solution, which gives \(\delta(x) \approx 5 \sqrt{\frac{\nu x}{U_\infty}}\), where \( U_\infty \) is the free-stream velocity and \( \nu \) is the kinematic viscosity.

What is the significance of the Reynolds number in boundary layer theory?

The Reynolds number \( Re \) is a dimensionless quantity that characterizes the relative importance of inertial forces to viscous forces in a fluid flow. In boundary layer theory, it is defined as \( Re = \frac{U_\infty x}{\nu} \). A low Reynolds number indicates laminar flow, while a high Reynolds number indicates turbulent flow. The transition from laminar to turbulent flow in the boundary layer typically occurs at a critical Reynolds number around \( Re \approx 5 \times 10^5 \).

How can the Prandtl boundary layer equation be solved?

The Prandtl boundary layer equation can be solved using analytical methods for simple cases, such as the Blasius solution for a flat plate. For more complex geometries or flow conditions, numerical

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