If you don’t like the previous definition, you are right, and you should be proud. But we won’t provide a better one in this page. This website does have (or will have) a precise definition of the vector in the appropriate section. Here we will just review how vectors work.

In the picture above, we have \(\overrightarrow{AB}=\overrightarrow{CD}\), while \(\overrightarrow{AB}\neq \overrightarrow{EF}\).

You may have noticed that the vectors \(\overrightarrow{AB}\) and \(\overrightarrow{EF}\) have the same length. That’s right.

We write \(|\overrightarrow{AB}|=|\overrightarrow{EF}|\) to say that the vectors \(\overrightarrow{AB}\) and \(\overrightarrow{EF}\) have the same length.

If one vector starts exactly where the other ends, then the addition is easy. This case is illustrated by the picture above. We have \(\overrightarrow{AB}+\overrightarrow{BC}=\overrightarrow{AC}\).

In the example from the picture above, we want to find \(\overrightarrow{AB}+\overrightarrow{CD}\). These two vectors are drawn in black. We will reduce this case to the previous one in which one vector starts where the other ends. We first construct a point \(E\) such that \(\overrightarrow{CD}=\overrightarrow{BE}\). Then we have

\[\overrightarrow{AB}+\overrightarrow{CD}=\overrightarrow{AB}+\overrightarrow{BE}=\overrightarrow{AE}.\]

The point \(E\) is blue in the picture, as well as the vector \(\overrightarrow{BE}\). The resulting vector \(\overrightarrow{AE}\) is also blue.

The opposite vector to the vector \(\overrightarrow{AB}\) is the vector \(\overrightarrow{BA}\). We also write

\[-\overrightarrow{AB}=\overrightarrow{BA}.\]

Now we can define subtraction of vectors: \(\overrightarrow{AB}-\overrightarrow{CD}=\overrightarrow{AB}+(-\overrightarrow{CD})=\overrightarrow{AB}+\overrightarrow{DC}\).

In the previous picture we can represent \(\overrightarrow{OB}=\overrightarrow{i}+2\overrightarrow{j}\), and \(\overrightarrow{OA}=-\overrightarrow{i}+1.5\overrightarrow{j}\). We also say that each vector is a linear combination of \(\overrightarrow i\) and \(\overrightarrow j\).

Each vector in the plane can be written in terms of \(\overrightarrow{i}\) and \(\overrightarrow{j}\). We can write

\[\overrightarrow{AB}=\overrightarrow{AO}+\overrightarrow{OB}=-\overrightarrow{OA}+\overrightarrow{OB}=\overrightarrow{i}-1.5\overrightarrow{j}+\overrightarrow{i}+2\overrightarrow{j}=2\overrightarrow i+0.5\overrightarrow j.\]

We say that 2 and 0.5 are

\[\overrightarrow u\cdot\overrightarrow v=u_xv_x+u_yv_y+u_zv_z.\]

The dot product of two vectors is always a scalar. For example, \(\langle 3,2,-1\rangle\cdot \langle -4,5,2\rangle=3\cdot (-4)+2\cdot 5+(-1)\cdot 2=-4\).

The following properties of the dot product are very easy to verify. However, they will have powerful consequences:

\[\overrightarrow u\cdot \overrightarrow v=|\overrightarrow u|\cdot|\overrightarrow v|\cos\theta.\]

We will start by formal definition of the cross product.

It is easier to remember the cross product if it is written in the form of a determinant: \[\overrightarrow u\times\overrightarrow v=\mbox{det }\left|\begin{array}{ccc} \overrightarrow i&\overrightarrow j&\overrightarrow k\newline x_u&y_u&z_u\newline x_v&y_v&z_v\end{array}\right|.\]

The following theorem lists the properties of the cross product. It is very easy to prove (using just the definition of the cross product, and following the order in which the statements are listed).

- \(\overrightarrow u\times (\beta\overrightarrow v+\gamma\overrightarrow w)=\beta\overrightarrow u\times\overrightarrow v+\gamma\overrightarrow u\times\overrightarrow w\).
- \(\overrightarrow u\times\overrightarrow v=-\overrightarrow v\times\overrightarrow u\)
- \(\left|\overrightarrow u\times\overrightarrow v\right|^2+\left(\overrightarrow u\cdot\overrightarrow v\right)^2=\left|\overrightarrow u\right|^2\cdot\left|\overrightarrow v\right|^2\)
- \(\left|\overrightarrow u\times\overrightarrow v\right|=\left|\overrightarrow u\right|\cdot \left|\overrightarrow v\right|\cdot \left|\sin \theta\right|\), where \(\theta\) is the angle between vectors \(\overrightarrow u\) and \(\overrightarrow v\). This implies that the length of the cross product is equal to the area of the parallelogram determined by \(\overrightarrow u\) and \(\overrightarrow v\).
- The vector \(\overrightarrow u\times \overrightarrow v\) is perpendicular to both \(\overrightarrow u\) and \(\overrightarrow v\).

Notice that the result of a triple product is a scalar, and the absolute value of that scalar is equal to the volume of the parallelepiped spanned by the vectors \(\overrightarrow u\), \(\overrightarrow v\), and \(\overrightarrow w\).

You are probably familiar with the equations of the form \(y=3x+5\). There are many ordered pairs \((x,y)\) of real numbers. Some of them satisfy the previous equation, others don’t. Those that do satisfy the equation determine the points in the plane - and if you paint those points in green - you get a green line.

This is the basic principle behind equations of geometric objects. A line in geometry is uniquely determined by a point and a vector. Let us consider a line \(\ell\) that is determined by a point \(A(x_0,y_0,z_0)\) and a vector \(v=\langle a,b,c\rangle\). We want to describe all those points \(P(x,y,z)\) that belong to \(l\). Geometric description is easy:

The last sentence has alternative form:

Let us denote the origin by \(O\). Notice that \[\overrightarrow{AP}=\overrightarrow{AO}+\overrightarrow{OP}=\overrightarrow{OP}-\overrightarrow{OA}=\langle x,y,z\rangle-\langle x_0,y_0,z_0\rangle=\langle x-x_0,y-y_0,z-z_0\rangle.\] The last sentence can now be easily translated into algebraic form:

The last form of the equation of the line is called the *vector equation of the line* \(\ell\). Its equivalent version is used most often and is called the *parametric equation of the line*:
\[x=x_0+at\]
\[y=y_0+bt\]
\[z=z_0+bt\]
\[t\in\mathbb R.\]

A plane in three dimensional space is uniquely determined by one of the following three combinations :

- (i) any three of its points
- (ii) a point and any two vectors
- (iii)a point and a normal vector

It turns out that in practice we use (ii) and (iii) to determine the equations of the plane. If we are given three points, we transform the problem from (i) to either (ii) or (iii) and try to deal with consequences.

Let us assume that we are given a point \(A\) and two vectors \(\overrightarrow u=\langle a_u,b_u,c_u\rangle\) and \(\overrightarrow v=\langle a_v,b_v,c_v\rangle\). Let us consider the plane \(\alpha\) that passes through \(A\) and is parallel to both \(\overrightarrow u\) and \(\overrightarrow v\). A points \(P(x,y,z)\) belongs to \(\alpha\) if and only if there are two real numbers \(s\) and \(t\) such that \(\overrightarrow{AP}= s\overrightarrow u+t\overrightarrow v\), i.e. \(\overrightarrow{OP}=\overrightarrow{OA}+s\overrightarrow u+t\overrightarrow v\). This can be written as \[x=x_0+sa_u+ta_v\] \[y=y_0+sb_u+tb_v\] \[z=z_0+sc_u+tc_v\] \[s\in\mathbb R, \;\;\; t\in\mathbb R.\]
The above equations are called *parametric equations of the plane* \(\alpha\).

Notice that the parametric equations of the line have one parameter, while the parametric equations of the plane have two parameters (\(s\) and \(t\)). That is why people say that line has dimension 1, while plane has dimension 2.

Assume we are given a point \(A(x_0,y_0,z_0)\) and a vector \(\overrightarrow n=\langle a,b,c\rangle\). Let us find the equation of the plane \(\alpha\) that passes through \(A\) and is orthogonal to \(\overrightarrow n\). A point \(P(x,y,z)\) belongs to \(\alpha\) if and only if the vector \(\overrightarrow{AP}\) is orthogonal to \(\overrightarrow n\), i.e. if and only if \(\overrightarrow{AP}\cdot \overrightarrow n=0\). Since \(\overrightarrow{AP}=\langle x-x_0, y-y_0, z-z_0\rangle\), the last statment can be written as \[(x,y,z)\in\alpha\;\;\;\Leftrightarrow \;\;\; \langle x-x_0,y-y_0,z-z_0\rangle \cdot \langle a,b,c\rangle=0,\;\;\;\mbox{ or, equivalently}\] \[a(x-x_0)+b(y-y_0)+c(z-z_0)=0.\] Sometimes the last equation is written as \(ax+by+cz=d\), where \(d=ax_0+by_0+cz_0\) is a constant.

**(A)**All six points belong to a plane.**(B)**None four of the given points belong to a plane.**(C)**The points \(A\), \(B\), \(E\), and \(F\) belong to a plane.**(D)**The points \(A\), \(B\), \(D\), and \(E\) belong to a plane.**(E)**The points \(A\), \(B\), \(C\), and \(F\) belong to a plane.