The Vector Differential, $d\rr$

Figure 7: The infinitesimal displacement vector $d\rr$ along a curve, shown in an “infinite magnifying glass”. In this and subsequent figures, artistic license has been taken in the overall scale and the location of the origin in order to make a pedagogical point.

The position vector \begin{equation} \rr=x\,\ii+y\,\jj+z\,\kk \end{equation} describes the location of the point $(x,y,z)$ in rectangular coordinates. It is instructive to draw a picture of the small change $\Delta\rr=\Delta x\,\ii + \Delta y\,\jj + \Delta z\,\kk$ in the position vector between nearby points. Try it! This picture is so useful that we will go one step further, and consider an infinitesimal change in position. Instead of $\Delta\rr$, we will write $d\rr$ for the vector between two points which are infinitesimally close together. This is illustrated in Figure 7, which shows a view of the curve through an “infinite magnifying glass”.

Figure 8a: The rectangular components of the vector differential $d\rr$ in two dimensions.

Like any vector, $d\rr$ can be expanded with respect to $\ii$, $\jj$, $\kk$; the components of $d\rr$ are just the infinitesimal changes $dx$, $dy$, $dz$, in the $x$, $y$, and $z$ directions, respectively, that is \begin{equation} d\rr = dx\,\ii + dy\,\jj + dz\,\kk \label{drdef} \end{equation} as shown in Figure 8a. We will use this geometric notion of $d\rr$ as an infinitesimal vector displacement as a unifying them to help us in visualizing the geometry of all of vector calculus.

What is the infinitesimal distance $ds$ between nearby points? Just the length of $d\rr$. We have \begin{equation} ds = |d\rr| = \sqrt{d\rr\cdot d\rr} = \sqrt{dx^2 + dy^2 + dz^2} \label{dsdef} \end{equation}

Figure 8b: The infinitesimal version of the Pythagorean Theorem.

and squaring both sides leads to \begin{equation} ds^2 = |d\rr|^2 = d\rr\cdot d\rr = dx^2 + dy^2 + dz^2 \label{ds1} \end{equation} which is just the infinitesimal Pythagorean Theorem, the two-dimensional version of which is shown in Figure 8b. 1)

1) When dealing with infinitesimals, we prefer to avoid second-order errors by anchoring all vectors to the same point.

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