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Why only the anisotropic part of the Reynolds-stress tensor affects production.

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Old   October 3, 2016, 00:09
Default Why only the anisotropic part of the Reynolds-stress tensor affects production.
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Why only the anisotropic part of the Reynolds-stress tensor affects production?

PS: I am learning turbulence. I am confused why only the anisotropic part of Reynolds stress tenosr will affect production of TKE (for incompressible flow)

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Old   October 3, 2016, 04:14
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Filippo Maria Denaro
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Quote:
Originally Posted by wertyfg View Post
Why only the anisotropic part of the Reynolds-stress tensor affects production?

are you talking about production of kinetic energy in incompressible flows?
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Old   October 3, 2016, 13:13
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Yes I am talking bout production of TKE in incompressible flow
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Old   October 3, 2016, 14:07
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I give you a more general answer that you can find from the original NS equations :

A stress tensor is decomposed in isotropic and deviatoric parts. The isotropic part acts by means of the action of only normal component (only the entries in the main diagonal are not zero). That resembles the decomposition used in the momentum equation:

T = -pI + Td

Thus, when you consider the averaging of the NS, after the decompostion of the Reynolds stress the isotropic part can be recasted like a modified pressure term p'. Now, considering the kinetic energy equation, the work of the normal stress p' can be effective if you have a volume variation, measured by div v, which is zero for incompressible flow.
You can organize the energy equation in a way to highlight production, dissipation and time variation as illustrated in many fundamental textbooks (Pope, Wilcox, Sagaut).
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Old   October 3, 2016, 16:34
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Quote:
Originally Posted by FMDenaro View Post
I give you a more general answer that you can find from the original NS equations :

A stress tensor is decomposed in isotropic and deviatoric parts. The isotropic part acts by means of the action of only normal component (only the entries in the main diagonal are not zero). That resembles the decomposition used in the momentum equation:

T = -pI + Td

Thus, when you consider the averaging of the NS, after the decompostion of the Reynolds stress the isotropic part can be recasted like a modified pressure term p'. Now, considering the kinetic energy equation, the work of the normal stress p' can be effective if you have a volume variation, measured by div v, which is zero for incompressible flow.
You can organize the energy equation in a way to highlight production, dissipation and time variation as illustrated in many fundamental textbooks (Pope, Wilcox, Sagaut).
FMDenaro Thank you for your reply!
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