Geometric Interpretation of Turbulence

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Discussion Overview

The discussion centers around the geometric interpretation of turbulence, specifically in the context of Poiseuille flow. Participants explore the relationship between the velocity profile of the flow and the behavior of fluid particles, including concepts of rotation and vorticity, while examining the conditions under which turbulence may arise.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • One participant suggests that in Poiseuille flow, the velocity profile resembles a parabolic shape, leading to sideways rotation of particles due to the profile's slope.
  • Another participant asserts that laminar flow, such as Poiseuille flow, does not exhibit turbulence and questions the initial interpretation.
  • Some participants clarify that while there is vorticity in the flow, it is distinct from turbulence, and that vorticity can exist even when flow velocity vectors are parallel.
  • It is noted that many turbulence models incorporate flow gradients as a source of turbulence, but this is not universally applicable, as certain flows with velocity gradients do not lead to turbulence under all conditions.
  • Participants discuss the importance of distinguishing between rotational flow and vorticity, with some acknowledging terminology mistakes in their contributions.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between velocity gradients and turbulence, with some arguing that gradients can lead to turbulence while others caution that this is not always the case. There is no consensus on the validity of the initial intuition regarding turbulence in Poiseuille flow.

Contextual Notes

Participants highlight that Poiseuille flow is defined as laminar and that the presence of velocity gradients does not guarantee turbulence. The discussion includes nuances regarding the definitions of rotation and vorticity, which remain unresolved.

George444fg
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TL;DR
Geometric Interpretation of Turbulence
I would like to give a geometric interpretation to turbulence. Let's take into consideration for example a Poiseuille flow. The velocity profile resembles a parabolic bullet. As the particles are pushed by other layers of particles, then it must be that in addition to their translation, they would rotate sideways due to the shape of the profile. While as far away the particles are from the centre of the tube the greater the slope of the paraboloid would be and therefore the greater the turbulence. Is my intuition valid?
 
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Laminar flow has no turbulence. So your interpretations must be incorrect. Turbulence is characterized by rapid and chaotic temporal fluctuations of the velocity components; such rapid temporal fluctuations are not present in laminar flow.
 
George444fg said:
Summary:: Geometric Interpretation of Turbulence

I would like to give a geometric interpretation to turbulence. Let's take into consideration for example a Poiseuille flow. The velocity profile resembles a parabolic bullet. As the particles are pushed by other layers of particles, then it must be that in addition to their translation, they would rotate sideways due to the shape of the profile. While as far away the particles are from the centre of the tube the greater the slope of the paraboloid would be and therefore the greater the turbulence. Is my intuition valid?
Why would particles need to be pushed in the way you describe? The velocity vector does not point normal to the profile you seem to describe. The fluid particles simply move horizontally with a velocity that, when plotted, is parabolic (in the case of Poiseuille flow that you cite).

If you want a "geometric" interpretation, the best I can do for you is to cite a 1922 limerick by Lewis Fry Richardson:
Big whorls have little whorls
Which feed on their velocity,
And little whorls have lesser whorls
And so on to viscosity
 
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George444fg said:
Let's take into consideration for example a Poiseuille flow. The velocity profile resembles a parabolic bullet. As the particles are pushed by other layers of particles, then it must be that in addition to their translation, they would rotate sideways due to the shape of the profile. While as far away the particles are from the centre of the tube the greater the slope of the paraboloid would be and therefore the greater the turbulence. Is my intuition valid?

Not sure what you mean by "rotate sideways", but if a test body floats in the Poiseuille flow, it will be rotated by the gradient. The vorticity (curl of the velocity field) can be non-zero, even if the flow velocity vectors are all parallel. But vorticity is different from turbulence.

https://en.wikipedia.org/wiki/Vorticity#Examples

 
A.T. said:
Not sure what you mean by "rotate sideways", but if a test body floats in the Poiseuille flow, it will be rotated by the gradient. The vorticity (curl of the velocity field) can be non-zero, even if the flow velocity vectors are all parallel. But vorticity is different from turbulence.

https://en.wikipedia.org/wiki/Vorticity#Examples


True, though it should be pointed out that while turbulence is inherently vortical, the converse is not true.
 
George444fg said:
Summary:: Geometric Interpretation of Turbulence

I would like to give a geometric interpretation to turbulence. Let's take into consideration for example a Poiseuille flow. The velocity profile resembles a parabolic bullet. As the particles are pushed by other layers of particles, then it must be that in addition to their translation, they would rotate sideways due to the shape of the profile. While as far away the particles are from the centre of the tube the greater the slope of the paraboloid would be and therefore the greater the turbulence. Is my intuition valid?

Allthough, Poiseuille flow is by definition laminar indeed. Also, there is not really rotation in the flow. But as @A.T. already mentioned, there is vorticity in the flow, i.e. draw am off-center rectangle in the flow and compute the integrated tangential velocity, this is not zero. This is a 'kind of' rotation, but only if you subtract the mean flow.

All that said, there is some validity to your intuition. Many turbulence models, used in viscous flow computations (CFD) use the gradient in the flow as a source of turbulence (together with some more complex parameters and modelling). So, the higher the gradient (as is true when you get closer to the wall) the higher the turbulence generation. This is not the entire story, because flow velocity, among others, also plays its part, but it is true to some extent.
 
Arjan82 said:
All that said, there is some validity to your intuition. Many turbulence models, used in viscous flow computations (CFD) use the gradient in the flow as a source of turbulence (together with some more complex parameters and modelling). So, the higher the gradient (as is true when you get closer to the wall) the higher the turbulence generation. This is not the entire story, because flow velocity, among others, also plays its part, but it is true to some extent.

One example of gradient in the flow as a source of turbulence:

https://en.wikipedia.org/wiki/Kelvin–Helmholtz_instability



 
You have to be very careful suggesting that velocity gradients lead to turbulence, because it is not universally true. The Blasius boundary layer, Poiseuille flow, Couette flow, and many others (including the superposed fluids subject to Kelvin-Helmholtz posted above) have velocity gradients but are only unstable under certain conditions. In other words, the existence of a velocity gradient is not a sufficient condition for the generation of turbulence.
 
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Arjan82 said:
Allthough, Poiseuille flow is by definition laminar indeed. Also, there is not really rotation in the flow. But as @A.T. already mentioned, there is vorticity in the flow, i.e. draw am off-center rectangle in the flow and compute the integrated tangential velocity, this is not zero. This is a 'kind of' rotation, but only if you subtract the mean flow.

All that said, there is some validity to your intuition. Many turbulence models, used in viscous flow computations (CFD) use the gradient in the flow as a source of turbulence (together with some more complex parameters and modelling). So, the higher the gradient (as is true when you get closer to the wall) the higher the turbulence generation. This is not the entire story, because flow velocity, among others, also plays its part, but it is true to some extent.
Excuse me I used the wrong term. We have rotational flow.
 
  • #10
boneh3ad said:
You have to be very careful suggesting that velocity gradients lead to turbulence, because it is not universally true. The Blasius boundary layer, Poiseuille flow, Couette flow, and many others (including the superposed fluids subject to Kelvin-Helmholtz posted above) have velocity gradients but are only unstable under certain conditions. In other words, the existence of a velocity gradient is not a sufficient condition for the generation of turbulence.
Excuse me I used the wrong term. I meant rotational flow, not turbulent
 
  • #11
Do you mean rotational flow (large scale structures rotating around some center) or vorticity (local flow parameter, or point value, like velocity and pressure)?
 
  • #12
Arjan82 said:
Do you mean rotational flow (large scale structures rotating around some center) or vorticity (local flow parameter, or point value, like velocity and pressure)?
Yep exactly that, I made a mistake
 
  • #13
George444fg said:
Yep exactly that, I made a mistake
exactly what? rotation or vorticity?
 
  • #14
Arjan82 said:
exactly what? rotation or vorticity?
rotation
 

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