Unclear assumption in deriving fluid energy conservation laws I am currently working through Alexandre Chorin's Mathematical Introduction to Fluid Mechanics. In the first chapter, he treats the change in Kinetic energy of a fluid region $W\subset D$ subject to the fluid flow map $\varphi_t:\mathbf{x}\mapsto\varphi(\mathbf{x},t)$ in the following manner ($\frac{D}{Dt}$ denoting the material derivative):
\begin{aligned} \frac { d } { d t } E _ { \text { kinetic } } & = \frac { d } { d t } \left[ \frac { 1 } { 2 } \int _ { W _ { t } } \rho \| \mathbf { u } \| ^ { 2 } d V \right] \\ & = \frac { 1 } { 2 } \int _ { W _ { t } } \rho \frac { D \| \mathbf { u } \| ^ { 2 } } { D t } d V \\ & = \int _ { W _ { t } } \rho \left( \mathbf { u } \cdot \left( \frac { \partial \mathbf { u } } { \partial t } + ( \mathbf { u } \cdot \nabla ) \mathbf { u } \right) \right) d V \end{aligned}
As best as I can determine, an implicit assumption seems to be made that the fluid has a density constant with time in this derivation. Specifically, it appears that the assumption $\frac{\partial}{\partial t}(\rho\| \mathbf { u } \| ^ { 2 }) = \rho\frac{D}{Dt}(\| \mathbf { u } \| ^ { 2 })$ is being made rather than obeying the typical product rule. I am not quite sure why. I would greatly appreciate it if someone could help shed some light on what is going on here!
If more context is needed, I can provide it upon request, or you may reference the presentation which is given on page 12 of Chorin's book. 
 A: Indeed, there is no assumption.
You can use the Reynolds transport theorem https://en.wikipedia.org/wiki/Reynolds_transport_theorem
With the Green theorem , it gives : 
$\frac{d}{dt}\int\limits_{\Omega (t)}{f\rho d\tau }=\int\limits_{\Omega (t)}{\left( \frac{\partial f\rho }{\partial t}+\nabla \cdot (f\rho \overrightarrow{v}) \right)d\tau }$
Then :
$\overrightarrow{\nabla }\cdot (f\rho \overrightarrow{v})=\rho \overrightarrow{v}\cdot \overrightarrow{\nabla }\cdot (f)+f\overrightarrow{\nabla }\cdot (\rho \overrightarrow{v})$ 
$\frac{\partial f\rho }{\partial t}+\nabla \cdot (f\rho \overrightarrow{v})=\rho \left( \frac{\partial f}{\partial t}+\overrightarrow{v}\cdot \overrightarrow{\nabla }\cdot (f) \right)+f\underbrace{\left( \frac{\partial \rho }{\partial t}+\overrightarrow{\nabla }\cdot (\rho \overrightarrow{v}) \right)}_{0}$ 
$\frac{d}{dt}\int\limits_{\Omega (t)}{f\rho d\tau }=\int\limits_{\Omega (t)}{\left( \frac{\partial f}{\partial t}+\vec{v}\cdot \vec{\nabla }\cdot (f) \right)\rho d\tau }=\int\limits_{\Omega (t)}{\left( \frac{\partial f}{\partial t}+(\vec{v}\cdot \vec{\nabla })\cdot (f) \right)dm}=\int\limits_{\Omega (t)}{\left( \frac{Df}{Dt} \right)dm}$
It is rather intuitive. You apply Newton law to a small fluid particle and you add all.
Sorry for my english ! 
