Navier Stokes Equations - Helmholtz-Hodge decomposition and pressure

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SUMMARY

The discussion centers on the relationship between the Helmholtz-Hodge decomposition and the pressure equation in the context of the Navier-Stokes (NS) equations for incompressible fluid flow. The participants clarify that while both methods aim to maintain flow divergence-free conditions, they are distinct approaches. The pressure equation, particularly Euler's pressure equation, applies under specific conditions such as inviscid and irrotational flows, while the continuity equation is essential for general NS problems. The Leray Projection is also highlighted as a method to project onto divergence-free functions, which simplifies the pressure term in weak solutions.

PREREQUISITES
  • Understanding of Navier-Stokes equations for incompressible fluid flow
  • Familiarity with Helmholtz-Hodge decomposition
  • Knowledge of pressure equations in fluid dynamics, specifically Euler's pressure equation
  • Concept of Leray Projection and Sobolev spaces
NEXT STEPS
  • Study the derivation and applications of the Helmholtz-Hodge decomposition in fluid dynamics
  • Explore the implications of the Leray Projection in solving Navier-Stokes equations
  • Investigate the Clebsch decomposition and its limitations compared to Helmholtz decomposition
  • Review literature on pressure update formulas in computational fluid dynamics
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Researchers, graduate students, and professionals in fluid dynamics, particularly those focusing on computational methods for solving Navier-Stokes equations and understanding flow characteristics in incompressible fluids.

Bucky
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Hi, I've been doing some work with the NS equations. I've read a few papers by fellow undergrads that imply a relationship between the helmholtz-hodge decomposition and the pressure equation.

As far as I can see, they're both separate ways of resolving the problem of keeping the flow divergence free. Am I wrong in thinking this?
 
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What "pressure equation" are you talking about?
Euler's pressure equation? That only holds for certain inviscid flows, most notably for irrotational flow, but an analogue can be made when a Clebsch decomposition* can be made (i.e, when the helicity in closed vortex tubes is zero, rather than just constant (the latter being the general case for inviscid flows).

Anyhow, none of this is applicable for general NS problems; for those, the continuity equation (rather than the condition of a solenoidal field) is an indispensable fourth equation along with the three momentum equations.


Possibly, I've misunderstood what you are referring to; it's been awhile since I was slightly acquainted with all of this.


* The Clebsch decomposition is not a general decomposition like the Helmholtz decomposition, and looks like this:
\vec{v}=\nabla\phi+\alpha\nabla\beta
where alpha and beta are concerned with, and in their form represents a limitation on, the vorticity in the fluid field.
 
Last edited:
sorry I guess my post was rather vague. Let's try again

The Navier Stokes equations for incompressible fluid flow are the following:

\frac{\partial u} {\partial t} = -(u. \nabla )u - \frac {1} {\rho} \nabla p + v \nabla ^2 u + f

\nabla .u = 0

The second equation (the incompressibility equation) is the one I'm curious about.

I've read that this can be resolved through the pressure equation, or through the helmholtz-hodge decomposition.

One paper suggested this was done through substituting a pressure update formula into the divergence formula.

the pressure update formula is
u^{n+1} _{i+1/2,j} = u_{i+1/2,j} - \delta t \frac{1}{\rho} \frac{p_{i+1,j} - pi,j}{\delta x}
u^{n+1} _{i,j+1/2} = u_{i,j+1/2} - \delta t \frac{1}{\rho} \frac{p_{i,j+1} - pi,j}{\delta x}

substituting into the divergence formula gives

\frac{\delta t}{\rho} (\frac{4p_{i,j}-p_{i,j+1}-p_{i+1,j}-p_{i-1,j}-p_{i,j-1}}{\Delta x^2}) = -\frac{u_{i+1/2,j}-u_{i-1/2,j}}{\Delta x} + \frac{v_{i,j+1/2} - v_{i,j-1/2}}{\Delta x}

The helmholtz-hodge decomposition is

<br /> <br /> \xi = \nabla u + \nabla .v +h<br />

where u is a scalar potential field (note that \nabla * (\nabla u) = 0
where v is a vector potential field (note that \nabla .(\nabla * v) = 0
where h is the harmonic vector field (note that \nabla .h = 0

One of the papers I've read states that it uses a Poisson equation to derive a height field, which is subtracted from \xi to yield a divergence free flow (it should be noted that this paper altogether ignores the harmonic vector field). The paper can be found here:
http://www.dgp.toronto.edu/people/stam/reality/Research/pdf/GDC03.pdf


in a few papers I've read the authors have implied a relationship between the pressure and helmholtz-hodge solutions. However I don't see how they're related; in fact in that paper I just mentioned the author doesn't even acknowledge the pressure equation in his statement of the NS equations as pertaining to his solver, so I'm finding difficulty in tieing these things together.

I hope this has made my question more clear, and look forward to any answers.
 
hi. I am interested in the HH decomposition too. Unfortunately, I am stuck on that. Please be in touch if you have found something interesting.
P.S. Are you from CG?
 
From my understanding, the way the second equation is manifests itself onto the pressure field is through the Leray Projection. The Leray Projection, using Hodge orthogonal decomposition, projects the Sobolev space onto the space of divergence free functions (satisfying the second equation). If looking for a weak solution to the problem, then we can integrate by parts and the pressure term becomes the L2 inner product between (p,div(v)). Since we projected v onto the space of divergence free functions this term is zero and the weak statement no longer involves the pressure field. Is that what you are asking about?
 

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