JulienB said:
So far I understand it like that: the partial differentials hold for analytical use of a function, while the total differential becomes useful when wanting to approximate the slope at a given point. Would you support that statement?
Not really. Partial derivatives also approximate the slope at a given point. Just in the direction of the coordinates. A total differential approximates a function ##f## as a whole by a linear function ##L## (the total differential), i.e. you may write ##f(\vec{x}+\vec{v}) = f(\vec{x}) + L(\vec{v}) +r(\vec{v})## such that ##\lim_{\vec{v} \rightarrow 0} \frac{r(\vec{v}}{||\vec{v}||} = 0##. This means ##f## can be approximated by ##L## such that the error terms in ##r## run faster towards zero than ##L## does, or as it often occurs (e.g. in Taylor expansions), ##r## has terms in ##\vec{v}## of higher orders than ##1##.
If not, could you maybe give me an example of partial and total differentiation so that I can visualise it? My interpretation is based on the following observation (for the case ##f: \mathbb{R}^n \to \mathbb{R}##):
##f' (\vec{x}) = \frac{\partial (f_1, ... , f_m)}{\partial (x_1, ... , x_n)} (x) = \mbox{vector}##
##f' (\vec{x}) = \sum \frac{\partial f}{\partial x_i} dx_i = \mbox{scalar}##
First of all, is that correct? And if so, would you say that "the total differentiability allows us to choose any direction" when we plug in arbitrary ##dx_i## for a given point ##\vec{x}##?
I have difficulties with naming everything ##x##. You should try to get used to distinguish when you are speaking of a function in the variable ##x##, coordinates ##x_i## or ##x^i## and eventual evaluation points ##x_0=p,## e.g. where the derivative is evaluated at. I'm not sure if I got you right. E.g. you may denote a gradient better by $$grad(f) = \nabla f = \sum_{i=1}^{n}\frac{\partial f}{\partial x_i} \vec{e}_i$$ or more physical $$\nabla f = \sum_{i=1}^{n}\frac{\partial f}{\partial x_i} dx_i$$ and $$\nabla_p f = \sum_{i=1}^{n}\left(\frac{\partial f}{\partial x_i}\right)_{x=p} dx_i$$
In addition, how can ##f'(\vec{x})## simultaneously be a vector and a scalar? Only by evaluation of ##\nabla_p f## at a certain point, which should not be denoted by the variable name.
An example for the difference between partial and total differentiation is the following:
$$f(\vec{x}) = \begin{cases} \frac{2x_1x_2}{x_1^2+x_2^2} & \text{if } (x_1,x_2) \neq (0,0) \\ \\ 0 & \text{if } (x_1,x_2) = (0,0) \end{cases}$$
##f## is partially differentiable at ##(0,0)## but not continuous at ##(0,0)##. And you might want to calculate what happens along the line ##x_1 = x_2##. The latter is an example of a direction that is not along a coordinate.