Viscosity from DFT (VASP) using the Green-Kubo relation

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Discussion Overview

The discussion revolves around the calculation of viscosity for MgSiO3 using Density Functional Theory (DFT) and the Green-Kubo relation, as applied in VASP. Participants explore different formulations of the Green-Kubo equation, the components of the stress tensor, and the implications of isotropy in liquids on viscosity calculations.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants note two formulations of the Green-Kubo relation for viscosity, one involving a summation over stress tensor components and another focusing on a single off-diagonal component.
  • It is mentioned that due to symmetry, the stress tensor can be reduced from nine components to six, which affects the input for the Green-Kubo equation.
  • One participant references a paper that discusses averaging the autocorrelation functions of five independent components of the stress tensor to find shear viscosity.
  • Another participant argues that viscosity, being a fourth-order tensor in isotropic liquids, can be parameterized with only two parameters, suggesting that different components should yield the same viscosity value.
  • There is a discussion about the correlation of the trace of the stress tensor and its relation to longitudinal viscosity, with a participant suggesting it may yield dilatational viscosity instead.
  • The naming conventions for viscosity types vary across sources, with a reference to "volume viscosity" as defined in Wikipedia.

Areas of Agreement / Disagreement

Participants express differing views on the correct formulation of the Green-Kubo relation and the interpretation of viscosity components. There is no consensus on which equation is definitively correct, and the discussion remains unresolved regarding the implications of the different formulations.

Contextual Notes

Participants highlight the dependence on symmetry and the specific definitions of viscosity components, indicating that assumptions about isotropy and the choice of stress tensor components may influence the results.

Polyamorph
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Hello! In this paper https://pdfs.semanticscholar.org/e8a2/02f25555cd8c4f947bbbdff5a61a0ea0efd2.pdf the authors use VASP to determine MgSiO3 viscosity using the Green-Kubo relation

## \eta = \frac{V}{3k_{\rm{B}}T}\int_{0} \left<\sum_\limits{i<j}\sigma_{ij}(t+t_{0}).\sigma_{ij}(t_{0})\right>dt## where ##\sigma_{ij}## (i and j = x, y, z) is the stress tensor, t is time and t0 is the time origin. But I've seen other papers use:

## \eta = \frac{V}{3k_{\rm{B}}T}\int_{0}^{\infty} dt \left< P_{xy}(t)P_{xy}(0)\right>##, where ##P_{xy}## is the off-diagonal component of the stress tensor ##P_{αβ}## ( α and β are Cartesian components).

OK, so clearly these are essentially exactly the same equation but the second uses only the xy component whereas the first seems to suggest a summation? So which is correct.

Also, VASP outputs the stress tensor components as XX YY ZZ XY YZ ZX. So which of these should I use to input into the Green-Kubo equation? And are there missing components? what about yx, zx, yx?

Thanks in advance.
 
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OK, I've worked out that due to symmetry, XY=YX, YZ=ZY, ZX=XZ, so the tensor reduces from 9-components to 6. So that explains my second question (note typo when I wrote "what about yx, zx, yx?" should have said "what about yx, zy, xz?"

But I still don't understand why the first equation is suggesting a sum of the off-diagonal components whereas the second equation suggests only using one of the off-diagonal components ##P_{xy}##.
 
Polyamorph said:
But I've seen other papers
Can you give an example of these other papers? Were they looking at a 2D case? Without the proper context, it's really difficult to tell what' s going on.
 
Polyamorph said:
Sure, I got the second equation from this paper: http://www.homepages.ucl.ac.uk/~ucfbdxa/pubblicazioni/PRL05161.pdf
I think this is just a schematic equation. Further into that paper (page 2), there's a paragraph starting with "There are five independent components of the traceless stress tensor..." The paper goes on to say that they find the shear viscosity by averaging the autocorrelation functions of these five components and integrating them from 0 to ##t##, taking the limit as ##t \to \infty##. (beginning of the paragraph that starts with "In Fig. 2") I haven't done the nitty gritty math, but it looks like this makes the two definitions in your OP equivalent.
 
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Yes, looks like you're right. Thanks for spotting that.
 
Polyamorph said:
OK, I've worked out that due to symmetry, XY=YX, YZ=ZY, ZX=XZ, so the tensor reduces from 9-components to 6. So that explains my second question (note typo when I wrote "what about yx, zx, yx?" should have said "what about yx, zy, xz?"

But I still don't understand why the first equation is suggesting a sum of the off-diagonal components whereas the second equation suggests only using one of the off-diagonal components ##P_{xy}##.

As liquids are isotropic, viscosity is a 4th order tensor which can be parametrized with only two parameters, ##\eta## and ##\zeta##, ##\eta## is the same whether determined with xy or xz or whathever component of the deviator of the viscosity gradient or of their sums. On the other hand, the correlation of the Trace of the ##\sigma_{ii}## will probably yield the longitudinal viscosity ##\zeta##.
 
DrDu said:
As liquids are isotropic, viscosity is a 4th order tensor which can be parametrized with only two parameters, ##\eta## and ##\zeta##, ##\eta## is the same whether determined with xy or xz or whathever component of the deviator of the viscosity gradient or of their sums. On the other hand, the correlation of the Trace of the ##\sigma_{ii}## will probably yield the longitudinal viscosity ##\zeta##.
I think you mean the dilatational viscosity (proportionality constant between the trace of the stress tensor and the trace of the rate of deformation tensor).
 

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