Caveat
Note, I have reviewed the question below with a similar name, and this is not a duplicate. I am asking about the Mass matrix on a PDE while the reference below is asking about the Mass matrix on a PDE discretization.
What the mass matrix represents?
Question I was trying to augment my understand of what a mass matrix does in a PDE. Now I might be using the wrong term here, but allow me to explain with a simple example using the 2D general heat equation
$$ \rho c_p \frac{\partial T}{\partial t} + \rho c_p \textbf{u}\cdot \nabla T - \nabla \cdot(K\nabla T) = f $$
I am talking specifically about the $\rho c_p$ on the first term of the equation. It always kinda bothered me when I saw this formulation, because I was not sure how this $\rho c_p$ coefficient or matrix in 2D came to be on the time derivative term. Like is it a physics thing? Or is it about expressing the equation in a unitful formulation instead of unitless formulation?
I get that having the $\rho c_p$ term on the time derivative term perhaps makes the math look nice, and we can divide both sides of the equation by $\rho c_p$ to remove the $\rho c_p$ in front of the time derivative. However, I was just wondering whether there might be some other meaning that I am missing when the $\rho c_p$ is applied to the time derivative.
There are two inter-related questions here:
For example, it is common in introductory dynamics to refer to $M$ in the following ODE system:
$$M\vec{x}'' + C\vec{x}' + K\vec{x} = \vec{0}$$
as the mass matrix, and $K$ as the stiffness matrix, because they play those roles when interpreting this equation as modeling a system of dampened interconnected springs. This is likely to be the context in which your $c_p\rho$ term is being interpreted, since it shares a "mass-like" physical interpretation due to representing thermal inertia in that PDE.