| 21. | The Navier Stokes equations form a vector continuity equation describing the conservation of linear momentum.
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| 22. | The Navier Stokes equations describing the motion of the flow have to be solved separately.
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| 23. | The compressible Navier-Stokes equation describes both the flow field, and the aerodynamically generated acoustic field.
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| 24. | In these cases, with the inviscid assumption, Navier-Stokes equations can be derived as Euler equations.
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| 25. | The pressure and force terms on the right-hand side of the Navier Stokes equation become
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| 26. | Neglecting pressure gradients, the Navier Stokes equations simplify to
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| 27. | The first law is used to derive the non-conservation form of the Navier Stokes equations.
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| 28. | For different types of fluid flow this results in specific forms of the Navier Stokes equations.
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| 29. | Many other interesting theories are non linear, like for example Navier Stokes equations of fluid dynamics.
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| 30. | One splits the Euler equations or the Navier-Stokes equations into an average and a fluctuating part.
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