I am thinking about the directional derivative. I think that the easiest way how to express it is
\begin{equation} \frac{\partial f(\mathbf{x})}{\partial \mathbf{v}} = \lim_{||v|| \rightarrow 0} \frac{f(\mathbf{x} + \mathbf{v})-f(\mathbf{x})}{||\mathbf{v}||}, \end{equation}
but the directional derivative is usually defined as
\begin{equation} \frac{\partial f(\mathbf{x})}{\partial \mathbf{v}} = \lim_{h \rightarrow 0} \frac{f(\mathbf{x} + h \mathbf{v})-f(\mathbf{x})}{h}. \end{equation}
Can you rigorously explain the transition from first and second definition?
Thanks!
Edit:
Just to make it clear.
The first definition is primarily wrong because the orientation of the directional vector is not fixed. So if I correct it like this (switching to conventional notation)
\begin{equation} \nabla_{\mathbf{v}} f(\mathbf{x}) = \lim_{||\mathbf{v}|| \to 0} \frac{f(\mathbf{x} + ||\mathbf{v}||\mathbf{\hat{v}})-f(\mathbf{x})}{||\mathbf{v}||}, \end{equation}
it makes a little bit more sense ($ \mathbf{\hat{v}}$ denotes unit vector). BUT the norm allows to get close to zero just from right side ($ ||\mathbf{v}|| \to 0+ $) and the limit makes sense even for vector reversal (~ negative norm). So we can actually use any scalar $h$ scaling the vector and write the derivative as
\begin{equation} \nabla_{\mathbf{v}} f(\mathbf{x}) = \lim_{h \to 0} \frac{f(\mathbf{x} + h\mathbf{\hat{v}})-f(\mathbf{x})}{h} \end{equation}
or you can find it equivalently written as
\begin{equation} \nabla_{\mathbf{v}} f(\mathbf{x}) = \lim_{h \to 0} \frac{f(\mathbf{x} + h\mathbf{v})-f(\mathbf{x})}{h||\mathbf{v}||}. \end{equation}
