Intuition for Material Derivative I am studying fluid mechanics and am trying to gain a finer intuition for the meaning behind the material derivative. So, firstly this is defined as $ (\partial_t + \mathbf{u}\cdot\nabla )f$ where $f$ is some multivariable function and $\mathbf{u}$ is the velocity field. I know the material derivative gives the rate of change of $f$ in a particular fluid element as it flows with the fluid. The first term gives the contribution from the temporal rate of change of f at a specific point, and the second term gives the contribution from the movement of the fluid element itself, and is the directional derivative of f in the direction of the velocity. However, it is stated in my notes that the second term, $\mathbf{u}\cdot\nabla(f)$ is the rate of change of f along some streamline multiplied by the magnitude of $\mathbf{u}$, ie. $\mathbf{u}\cdot\nabla(f)= df/ds \vert{\mathbf{u}}\vert$ where s is the distance along the streamline. I dont understand this. We are following the fluid element along a particle path, why is there some random streamline important? Can someone explain?
 A: This is to answer the question $u \cdot \nabla f = \frac{df}{ds} |u|$, where $u$ is the velocity field. Everything is time-independent (stationary) here. 
Let's hypothesize that $\frac{df}{d\tau}$ means the derivative along the stream line. A streamline is an integral line of (i.e. the solution of the ODE, traced out) $X'(\tau) = u(X(\tau))$, and let's say $X(0) = x_0$ is where we evaluate the formula in question. Here, $\tau$ is a fictitious time that parameterizes the streamline (it coincides with the real time if $u$ is stationary).
Then $\frac{d f}{d \tau}(x_0)$ is the derivative of the function $h(\tau) := f(X(\tau))$ at $\tau = 0$.
By the chain rule and the definitions,
$$
h'(\tau) = \nabla f(X(\tau)) \cdot X'(\tau)
= \nabla f(X(s)) \cdot u(X(s))
$$
so that
$$
\frac{df}{d\tau}(x_0) = h'(0) = \nabla f(x_0) \cdot u(x_0).
$$
Ok, that's not what we wanted; the variable $s$ in the formula is apparently not what I called the fictitious time. Let's take $s = \tau |u|$ which has the unit of length. Now we parameterize the streamline by length rather than time. This looks uncomfortable, because $u$ depends on spatial variable; indeed, the streamline is an integral line of the unit-speed $Y'(s) = u(Y(s)) / |u(Y(s))|$ with $Y(0) = x_0$. Let us set $g(s) := f(Y(s))$, and compute the derivative $g'(0)$. We have
$$
g'(s) = \nabla f(Y(s)) \cdot Y'(s) = \nabla f(Y(s)) \cdot u(Y(s)) / |u(Y(s))|
$$
so that
$$
\frac{df}{ds}(x_0) = g'(0) = \nabla f(x_0) \cdot u(x_0) / |u(x_0)|
.
$$
Multiply by $|u(x_0)|$ to obtain the original formula.
