Significance of the viscous stress tensor

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Discussion Overview

The discussion revolves around the physical interpretation of the viscous stress tensor components in the context of the Navier-Stokes equations, particularly focusing on the normal stress components and their relationship to pressure. Participants explore the implications of turbulent flow on viscous stresses and the averaging of stress components.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants question the physical interpretation of the normal stress components ##\tau_{xx}##, ##\tau_{yy}##, and ##\tau_{zz}##, suggesting that viscous stresses are typically associated with shear components (##\tau_{ij}## where ##i≠j##).
  • There is a discussion about whether it is reasonable to consider fluctuations of the viscous stress tensor to be zero in turbulent flow, with some arguing that the time-averaged values are not zero.
  • Participants express uncertainty about the implications of averaging the Navier-Stokes equations and whether certain components of the turbulent stress tensor can be simplified to zero.
  • One participant asserts that the normal components of the stress tensor can be non-zero, depending on the coordinate system used, while another emphasizes that in certain flow conditions, these components may indeed be zero.
  • There is a mention of the Cauchy stress tensor's symmetry and whether this property applies to the viscous stress tensor as well.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the interpretation of the viscous stress tensor components, particularly regarding the normal stresses and their relationship to pressure. Multiple competing views remain on the treatment of turbulent stresses and the implications of averaging in turbulent flow.

Contextual Notes

Some claims depend on specific flow conditions and assumptions about the coordinate system. The discussion highlights the complexity of relating viscous stresses to pressure and the nuances involved in averaging stress components in turbulent flows.

dRic2
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Hi,

when working with NS equations the stress tensor can be written as ##\nabla \tau = - \nabla P + \nabla \tau_{v}##, where ##\tau_{v} ## is
\begin{pmatrix}
\tau_{xx} & \tau_{xy} & \tau_{xz} \\
\tau_{xy} & \tau_{yy} & \tau_{yz} \\
\tau_{zx} & \tau_{zy} & \tau_{zz}
\end{pmatrix}

This question was stuck in my mind since last years, but I used to forget to ask: what is the physical interpretation of ##\tau_{xx}##, ##\tau_{yy}##, ##\tau_{zz}##? I know where they come from "mathematically", but I don't get the difference with pressure... I thought viscous stresses could only be like ##\tau_{ij}## with ##i≠j##.

PS: Out of the blue: In a very turbulent flow is it ok to consider ##\tau_{ij} = 0## with ##i≠j##?

Thanks
Ric
 
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dRic2 said:
Hi,

when working with NS equations the stress tensor can be written as ##\nabla \tau = - \nabla P + \nabla \tau_{v}##, where ##\tau_{v} ## is
\begin{pmatrix}
\tau_{xx} & \tau_{xy} & \tau_{xz} \\
\tau_{xy} & \tau_{yy} & \tau_{yz} \\
\tau_{zx} & \tau_{zy} & \tau_{zz}
\end{pmatrix}

This question was stuck in my mind since last years, but I used to forget to ask: what is the physical interpretation of ##\tau_{xx}##, ##\tau_{yy}##, ##\tau_{zz}##? I know where they come from "mathematically", but I don't get the difference with pressure... I thought viscous stresses could only be like ##\tau_{ij}## with ##i≠j##.
Why do you wonder about the difference with pressure? Regarding the i,j thing, why did you think this?
PS: Out of the blue: In a very turbulent flow is it ok to consider ##\tau_{ij} = 0## with ##i≠j##?

Thanks
Ric
In turbulent flow, the time averaged values of the viscous stresses are definitely not equal to zero.
 
Chestermiller said:
Why do you wonder about the difference with pressure? Regarding the i,j thing, why did you think this?

##\tau_xx## (for example) is a normal vector respect to ##zy## surface. I thought viscous stress can only be tangent vectors (like ##\tau_{xy}##) because of Newton's law ##\tau = -\mu \frac {\partial v_x} {\partial y} ##.
 
Chestermiller said:
In turbulent flow, the time averaged values of the viscous stresses are definitely not equal to zero.
Sorry, I'm so dumb...

I don't know how I came up this...

What I really meant is: "In a turbulent flow is it ok to consider the fluctuations of ##\tau## to be zero? I mean if I average NS equations I get ##\tau = \tau_{v} + \tau_{t}## where ##\tau_{t}## is:

\begin{pmatrix}
\bar v'^2_{xx} & \bar {v'_xv'_y} & \bar {v'_xv'_z} \\
\bar v'^2_{yx} & \bar {v'^2_y} & \bar {v'_yv'_z} \\
\bar v'^2_{zx} & \bar {v'_zv'_y} & \bar {v'^2_z}
\end{pmatrix}

Is it ok to do this:

\begin{pmatrix}
\bar v'^2_{xx} & 0& 0\\
0 & \bar {v'^2_y} &0 \\
0& 0 & \bar {v'^2_z}
\end{pmatrix}

?
 
dRic2 said:
##\tau_xx## (for example) is a normal vector respect to ##zy## surface. I thought viscous stress can only be tangent vectors (like ##\tau_{xy}##) because of Newton's law ##\tau = -\mu \frac {\partial v_x} {\partial y} ##.
That's only the simplified version for a specific type of flow situation. The 3D version of the law is what is required so that law is independent of the coordinate system used by the observer. You are aware that, even for the state of stress you have indicated, if the coordinate axes were rotated, the components of the stress tensor in the new coordinate system will contain normal stresses, correct?
 
dRic2 said:
Sorry, I'm so dumb...

I don't know how I came up this...

What I really meant is: "In a turbulent flow is it ok to consider the fluctuations of ##\tau## to be zero? I mean if I average NS equations I get ##\tau = \tau_{v} + \tau_{t}## where ##\tau_{t}## is:

\begin{pmatrix}
\bar v'^2_{xx} & \bar {v'_xv'_y} & \bar {v'_xv'_z} \\
\bar v'^2_{yx} & \bar {v'^2_y} & \bar {v'_yv'_z} \\
\bar v'^2_{zx} & \bar {v'_zv'_y} & \bar {v'^2_z}
\end{pmatrix}

Is it ok to do this:

\begin{pmatrix}
\bar v'^2_{xx} & 0& 0\\
0 & \bar {v'^2_y} &0 \\
0& 0 & \bar {v'^2_z}
\end{pmatrix}

?
Sure. These are called the turbulent stresses.
 
Thanks for the quick replies, I'm in kind of a hurry now. I'll be back later/tomorrow! :)
 
Chestermiller said:
You are aware that, even for the state of stress you have indicated, if the coordinate axes were rotated, the components of the stress tensor in the new coordinate system will contain normal stresses, correct?

Do you mean something like this?
204771-39640136e6f7a29a73ce33239b091d02.jpg


I think it is clear. But it is different: here you "create" the normal components by rotating the axis. Consider a chunk of fluid flowing in rectangular pipe (so we won't bother changing coordinates). Let's set the origin of the axis in one of the corner of the pipe (no rotation). What is the meaning of ##\tau_{ii}##?

Ps: I remember the Cauchy stress tensor for a rigid (static) body has to be symmetric because of conservation of momentum. Does this apply also to viscous stress tensor?
 

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Chestermiller said:
Sure. These are called the turbulent stresses.

Why ##\bar {v'_iv'_j} = 0## is reasonable ?
 
  • #10
dRic2 said:
Why ##\bar {v'_iv'_j} = 0## is reasonable ?
It's not, and the average of the product of these fluctuations isn't zero.
 
  • #11
dRic2 said:
Do you mean something like this?
204771-39640136e6f7a29a73ce33239b091d02.jpg


I think it is clear. But it is different: here you "create" the normal components by rotating the axis. Consider a chunk of fluid flowing in rectangular pipe (so we won't bother changing coordinates). Let's set the origin of the axis in one of the corner of the pipe (no rotation). What is the meaning of ##\tau_{ii}##?
For this flow, it is zero. If you want to see the full derivation showing why the normal components can be non-zero, see chapters 1 and 2 in Transport Phenomena by Bird, Stewart, and Lightfoot
Ps: I remember the Cauchy stress tensor for a rigid (static) body has to be symmetric because of conservation of momentum. Does this apply also to viscous stress tensor?
Yes.
 
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  • #12
Chestermiller said:
For this flow, it is zero. If you want to see the full derivation showing why the normal components can be non-zero, see chapters 1 and 2 in Transport Phenomena by Bird, Stewart, and Lightfoot

Things are coming together in my mind, thank you!
 
  • #13
Chestermiller said:
It's not, and the average of the product of these fluctuations isn't zero.

I might have misunderstood your previous answer:

Chestermiller said:
Sure. These are called the turbulent stresses.

I thought it was referred to this:

dRic2 said:
Sorry, I'm so dumb...

I don't know how I came up this...

What I really meant is: "In a turbulent flow is it ok to consider the fluctuations of ##\tau## to be zero? I mean if I average NS equations I get ##\tau = \tau_{v} + \tau_{t}## where ##\tau_{t}## is:

\begin{pmatrix}
\bar v'^2_{xx} & \bar {v'_xv'_y} & \bar {v'_xv'_z} \\
\bar v'^2_{yx} & \bar {v'^2_y} & \bar {v'_yv'_z} \\
\bar v'^2_{zx} & \bar {v'_zv'_y} & \bar {v'^2_z}
\end{pmatrix}

Is it ok to do this:

\begin{pmatrix}
\bar v'^2_{xx} & 0& 0\\
0 & \bar {v'^2_y} &0 \\
0& 0 & \bar {v'^2_z}
\end{pmatrix}

?
 
  • #14
dRic2 said:
I might have misunderstood your previous answer:
I thought it was referred to this:
What I meant was that all the elements of the turbulent stress tensor can be non-zero, including the shear components.
 
  • #15
dRic2 said:
Sorry, I'm so dumb...

Is it ok to do this:

\begin{pmatrix}
\bar v'^2_{xx} & 0& 0\\
0 & \bar {v'^2_y} &0 \\
0& 0 & \bar {v'^2_z}
\end{pmatrix}

?

So this is generally false, right?
 
  • #16
dRic2 said:
So this is generally false, right?
Yes.
 

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