Questions about Navier-Stokes equations, Einstein notation, tensor rank I'm looking at Navier-Stokes equation in index notation and how to get them in vector notation:
$$
{\partial u_i \over \partial t}+  u_j {\partial u_i \over \partial x_j}= -\frac{1}{\rho}{\partial p \over \partial x_i}+ \nu {\partial^2 u_i \over \partial x_j \partial x_j}+g_i
$$
1st equation: The local acceleration, pressure, and body forcing terms seem simple. Is it correct to say as they have 1 free index (i) that they are tensors of rank 1, thus vectors where i = 1,2, and 3 for 3D?
2nd Question: For the convection acceleration term (I assume the diffusive term would be similar):
$$
u_j {\partial u_i \over \partial x_j},
$$
is it correct to say the $u_j {\partial \over \partial x_j}$ component, as it has no free indices and 1 dummy index (j), is a rank 0 tensor and thus a scalar (after summation)?
3rd Question: If Question 2 is correct can $u_i$ in the same term, a vector, simply then be multiplied by $u_j {\partial \over \partial x_j}$, a scalar, to then get a vector?
This is probably a softball question for anyone that does a lot of tensor calculus. I'm trying to teach some things about the Navier-Stokes equations and I'm trying to make sure all of my definitions regarding tensor rank and index notation are correct.
 A: 
Is it correct to say as they have 1 free index (i) that they are tensors of rank 1, thus vectors where i = 1,2, and 3 for 3D?

Yes but... not always. In general, an expression with a free index $i$ might be interpreted as the $i$-th component of a $1 \times n$ array of numbers. If it has 2 free indices $i,j$ as the (i,j)-th component of a matrix, and so on. Yet, arrays and tensors are not the same thing. Tensors must obey certain transformation rules under rotations for example, and we 'represent' these tensors with arrays of numbers. For your problem, these quantities are vectors but you can always avoid getting into the details of the transformation properties and just think about them as arrays. Actually, whenever a dummy index arises from non-relativistic physics, it is almost always certain that the quantity is also the component of a vector.

is it correct to say the $_\frac{∂}{∂_}$ component, as it has no free indices and 1 dummy index (j), is a rank 0 tensor and thus a scalar (after summation)?

Yes, it is a scalar operator (no free indices) but take into account that this might change depending on the object on which it acts, e.g: if it acts on a function (scalar) it will be scalar, if it acts on a vector (1 free index) it will be a vector, and so on. Also, take into account that you cannot add up quantities with different ranks (i.e: a number + a vector is not a valid operation, therefore, if you identify that an equation is made up of a sum of vectors like Navier Stokes,  then... the other terms must also be vectors).

If Question 2 is correct can $_$ in the same term, a vector, simply then be multiplied by $_\frac{∂}{∂_}$, a scalar, to then get a vector

Yes, read the previous comments.
Also, you might find useful to interpret things like $\frac{∂}{∂_}$ as the components of $\vec{\nabla}$ (a gradient), contractions as dot products, $_\frac{∂}{∂_}$ as a directional derivative $\vec{u}\cdot\vec{\nabla}$, $\frac{∂}{∂_∂_}$ as a Laplacian $\Delta^2$, etc. Further, take into account that $_\frac{∂}{∂_}\neq \frac{∂_}{∂_}$ (the first one is a directional derivative, and the latter a divergence).
