Laminar Pipe Flow: Displacement, and Momentum Thicknesses

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SUMMARY

This discussion focuses on the calculation of displacement and momentum thicknesses in laminar pipe flow and their relation to flow over flat plates. The displacement thickness for fully developed laminar flow in pipes is equivalent to the pipe radius (R), as the boundary layer penetrates to the center of the pipe. The conversation highlights that while displacement thickness is significant in the entrance region, it becomes less relevant in fully developed flow due to the established velocity profile. Key equations for displacement and momentum thicknesses are provided, emphasizing their derivation from fluid dynamics principles.

PREREQUISITES
  • Understanding of laminar flow dynamics
  • Familiarity with boundary layer theory
  • Knowledge of fluid mechanics equations
  • Basic calculus for integration of flow profiles
NEXT STEPS
  • Study the derivation of boundary layer equations in fluid mechanics
  • Learn about the velocity profile in fully developed laminar flow
  • Explore the concept of boundary layer thickness in different flow conditions
  • Investigate the effects of pipe curvature on flow characteristics
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Students and professionals in fluid dynamics, mechanical engineers, and researchers focusing on hydrodynamics and pipe flow analysis.

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Hello. I'm new to the forums. I apologize if I have posted this in the wrong topic area.

I'm new to this hydrodynamics area and I'm trying to learn the concepts of boundary layer thicknesses. My question is about laminar pipe flow and calculating displacement and momentum thicknesses. I was wondering if finding the displacement and momentum thicknesses in a pipe flow is the same as finding them in flow over a flat-plate.

I found the displacement thickness over a flat plate to be:
## \delta_1 = \int_0^\infty (1-\frac{u\rho}{u_{\infty}\rho_{\infty}})dy ##

And the momentum thickness is:
## \delta_2 = \int_0^\infty \frac{\rho u}{\rho_{\infty}u_{\infty}} (1-\frac{u\rho}{u_{\infty}\rho_{\infty}})dy ##

Thank you.
 
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In the region where the thicknesses are small compared to the radius of the pipe, you can treat flow in the entrance region to a pipe as flow over a flat plate. However, as the thicknesses become greater, neglect of the curvature becomes less acceptable.

Chet
 
Hello Sir,
I just want to know further in this topic that
"Can we calculate displacement thickness for fully developed laminar flow in pipes"
 
cabon7969 said:
Hello Sir,
I just want to know further in this topic that
"Can we calculate displacement thickness for fully developed laminar flow in pipes"
For fully developed laminar flow in pipes, the boundary layer has penetrated to the center of the pipe, and the displacement thickness is R.

Chet
 
Hello Sir ,
I did not understand how the displacement thickness becomes R.
According to me, displacement thickness is the distance by which streamline get deflected due to effect of boundary layer and also it can be stated as imaginary increase in thickness of wall due to boundary layer.
But for the fully developed laminar flow this thickness will be constant, but i don't know what it will be ?
 
For a fully-developed pipe flow, why do you feel the need to define a displacement thickness in the first place? Once the flow is fully-developed, the concept of a boundary layer is somewhat meaningless. There is already a well-defined, well-predicted velocity profile.
 

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