I'm trying to write the heat transfer equation in an arbitrary fluid (compressible and viscous). Consider an adiabatic system where the only heat generated is due to the internal friction/viscosity. In a fluid, the dissipation function is:
Φv=ˇτ:ˇ∇Tˇν
\boldsymbol{\tau} is defined as
\check{\tau}=\check{\sigma}-P\check{I} \tag{2}
Where \boldsymbol{\sigma} is the Cauchy stress tensor and P is the hydrostatic pressure.
Assuming that conduction and radiation are negligible, and convection is the only form of heat transfer, I think I can write the conservation of heat as:
\frac{\partial}{\partial t}\left( q \right) +\check{\nabla}\left( q \, \check{\nu}^T \right)= \check{\tau}: \check{\nabla}^T \check{\nu} \tag{3}
Now what I do not understand is which one represent heat: enthalpy h or internal energy e? For example I'm trying to write the equation for an ideal gas. Can I use enthalpy and write the conservation of heat as:
\frac{\partial}{\partial t}\left( \rho T \right) +\check{\nabla}\left( \rho T \, \check{\nu}^T \right)= \frac{1}{c_P} \check{\tau}:\check{\nabla}^T\check{\nu} \tag{4}
Or should I use the internal energy:
\frac{\partial}{\partial t}\left( \rho T \right) +\check{\nabla}\left( \rho T \, \check{\nu}^T \right)= \frac{1}{c_{\nu}} \check{\tau}:\check{\nabla}^T\check{\nu} \tag{5}
Which one of the equations 4 or 5 is the correct form? Or maybe they are both wrong?
Notation:
- \check{A} is the matrix representation of tensor \boldsymbol{A}
- : is the the double dot product of two square matrices (i.e. \check{A}:\check{B}=a_{ij}b_{ji} in Einstein notation form)
- \check{a}^T\check{b} (Where \check{a} and \check{b} are row matrices) is the dyadic product of first rank tensors \boldsymbol{a} and \boldsymbol{b}, usually noted as \boldsymbol{a}\boldsymbol{b}. Also known as outer product \vec{a} \otimes \vec{b} in vector form.
- \check{A}\check{B} is the matrix multiplication and for row matrices \check{a}\check{b}^T \equiv\vec{a}.\vec{b} dot product in vector form
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