Side note:
Delta2 said:
Normally it should be $$\rho_{xx}=\frac{\partial^2\rho}{\partial x^2}$$
Usually density is a scalar, at least that's how I know it when studying most of physics.
When I taught Griffith's level E&M the first time,
I realized another example of notational differences between mathematicians and physicists.
To physicists and advanced physics students, [itex]E_x[/itex] is the x-component of the electric field vector: [itex]\quad[/itex] [itex]\hat x \cdot \vec E[/itex].
To mathematicians and advanced mathematics students, [itex]E_x[/itex] is the partial-derivative of [itex]E[/itex] with respect to [itex]x[/itex]: [itex]\quad[/itex] [itex]\displaystyle\frac{\partial E}{\partial x}[/itex].
(I'd be curious to how [itex]\vec\nabla\cdot \vec E[/itex] would be expanded out... presumably, one would define [itex]\vec E= F(x,y,z) \hat x+ G(x,y,z) \hat y + H(x,y,z) \hat z[/itex])
(Long ago, I was a double major in physics and math, but I guess I probably compartmentalized notations.)
Possibly interesting reading:
http://sites.science.oregonstate.edu/math/bridge/papers/bridge.pdf
"Bridging the Gap between Mathematics and the Physical Sciences"
Tevian Dray and Corinne A. Manogue
http://sites.science.oregonstate.edu/physics/bridge/papers/CMJspherical.pdf
"Spherical Coordinates"
Tevian Dray and Corinne A. Manogue