\(\def \u#1{\,\mathrm{#1}}\) \(\def \abs#1{\left|#1\right|}\) \(\def \ast{*}\) \(\def \deg{^{\circ}}\) \(\def \tau{\uptau}\) \(\def \ten#1{\times 10^{#1}}\) \(\def \redcancel#1{{\color{red}\cancel{#1}}}\) \(\def \BLUE#1{{\color{blue} #1}}\) \(\def \RED#1{{\color{red} #1}}\) \(\def \PURPLE#1{{\color{purple} #1}}\) \(\def \th#1,#2{#1,\!#2}\) \(\def \lshift#1#2{\underset{\Leftarrow\atop{#2}}#1}}\) \(\def \rshift#1#2{\underset{\Rightarrow\atop{#2}}#1}}\) \(\def \dotspot{{\color{lightgray}{\circ}}}\) \(\def \ccw{\circlearrowleft}\) \(\def \cw{\circlearrowright}\)
Appendix B: Vectors
4.

Vector Basis and Notation

Adding vectors graphically can be fun, but it would be frustrating to get precise answers out of it. Sometimes we need numbers.

Before we can write a vector this way we must specify a basis: that is, we need to define a positive x-direction, and a positive y-direction perpendicular to it. (If we're working in 3D we will need a "z" as well.) The conventional basis is the one shown here: with \(x\) pointing to the right and \(y\) pointing up, but you should not assume that this is always the case.

(no alternate text)

We can write vectors as a set of two or three numbers, called a tuple, like this force: \(\vec F = (4, − 5)\u{N}\). The individual numbers 4 and –5 are called components of the vector, and are written \(F_x=4\) and \(F_y=-5\). The picture on the right shows the vector (4,–5) given the conventional basis above: the vector goes “over 4 and down 5”.

There is nothing particularly special about the conventional basis; we can use whatever basis we want.. For instance, we could make x point down and y point to the right. In that case, the same vector would be written (5,4).

Footnote

Instead of using tuple notation, physicists will often write vectors using unit-vector notation, which looks like this: $$\vec F=(F_x,F_y,F_z) = F_x\,\hat i + F_y\,\hat j + F_z\,\hat k \quad\text{ or }\quad F_x\,\hat x+F_y\,\hat y+F_z\,\hat z$$ So for example, they would write $(3,-5)$ as $3\hat i-5\hat j$ or $3\hat x-5\hat y$.

The symbols with the hats, like $\hat x$, are called unit vectors. The unit vectors $\hat i$ and $\hat x$ are vectors that point in the positive-$x$ direction, which have a length of 1. (Not 1 meter or 1m/s or anything, just "1".) Thus $3\hat x$ is a vector which also points in the positive $x$ direction, but which has a length of $3$.

We won't use this notation in this book, but you may see it elsewhere.