Different forms of fluid energy conservation equations

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The discussion revolves around deriving fluid energy conservation equations, specifically focusing on the expressions involving the material derivative of pressure and energy. The initial equation provided is related to the conservation of internal energy, leading to the challenge of deriving two specific equations: one for pressure and another for the ratio of pressure to density raised to the power of gamma. Participants express confusion about the steps needed to simplify the equations and the role of kinetic energy in the derivation process. The conversation highlights the importance of understanding the continuity equation and the adiabatic assumptions in fluid dynamics. Ultimately, the goal is to clarify how to arrive at the desired equations from the foundational principles of fluid mechanics.
  • #31
Chestermiller said:
This equation is the expression for adiabatic reversible expansion or compression of an ideal gas.

This can be derived from the previous equation using the continuity equation.
I though I had to start with##
\frac{Dp}{Dt} + \gamma p \nabla\cdot \vec{u} = 0

##
The starting point has to be the energy equation and the mass balance equation, also known as continuity equation.
Basically, I have to do what @pasmith says in post #2?
 
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  • #32
happyparticle said:
I though I had to start with##
\frac{Dp}{Dt} + \gamma p \nabla\cdot \vec{u} = 0

##
I don’t think so. This equation can be derived.
 
  • #33
Chestermiller said:
I don’t think so. This equation can be derived.
I guess I misread post #3

I guess I finally found both expression. I think I was completely wrong since the beginning. More than I thought.
 
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