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IB Maths AA 3.11 Notes

This page contains our IB Maths AA notes for 3.11. By reading each one of these notes, you will fully cover the content for IB Maths AA 'Lines'.

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Equations of a line

A line can be written in vector form as:

r=a+λb\mathbf{r}=\mathbf{a}+\lambda\mathbf{b}

Here:

  • a\mathbf{a} is the position vector of a fixed point on the line
  • b\mathbf{b} is a direction vector
  • λ\lambda is a scalar parameter

As λ\lambda changes, the point r\mathbf{r} moves along the line.

Math Topic 3 subTopic 11 notes image 1

A line passes through the point (1,2,3)(1,2,3) and has direction vector (412)\begin{pmatrix}4\\-1\\2\end{pmatrix}. Write down its vector equation.

So r=(123)+λ(412)\mathbf{r}=\begin{pmatrix}1\\2\\3\end{pmatrix}+\lambda\begin{pmatrix}4\\1\\-2\end{pmatrix}.

We can also write an equation in parametric form. From r=(x0y0z0)+λ(lmn)\mathbf{r}=\begin{pmatrix}x_0\\y_0\\z_0\end{pmatrix}+\lambda\begin{pmatrix}l\\m\\n\end{pmatrix} we get the parametric equations:

x=x0+λlx=x_0+\lambda l

y=y0+λmy=y_0+\lambda m

z=z0+λnz=z_0+\lambda n

Find the parametric equations for the line r=(123)+λ(412)\mathbf{r}=\begin{pmatrix}1\\2\\3\end{pmatrix}+\lambda\begin{pmatrix}4\\1\\-2\end{pmatrix}.

So, x=1+4λx=1+4\lambda, y=2λy=2-\lambda, z=3+2λz=3+2\lambda.

Lastly, we can write a line in Cartesian form. If the direction vector is (l,m,n)(l,m,n), then the Cartesian form is

xx0l=yy0m=zz0n\frac{x-x_0}{l}=\frac{y-y_0}{m}=\frac{z-z_0}{n}

For the same line we used before, the Cartesian form is x14=y21=z32\frac{x-1}{4}=\frac{y-2}{-1}=\frac{z-3}{2}.

To write the equation of a line, you need:

  • one point on the line
  • a direction vector

The direction vector can come from:

  • two points on the line
  • a parallel line
  • physical information such as velocity

Find the equation of the line through A(2,1,1)A(2,1,-1) and B(5,3,4)B(5,3,4).

First find the direction vector: AB=(5,3,4)(2,1,1)=(325)\overrightarrow{AB}=(5,3,4)-(2,1,-1)=\begin{pmatrix}3\\2\\5\end{pmatrix}.

So the vector equation is r=(211)+λ(123)\mathbf{r}=\begin{pmatrix}2\\1\\-1\end{pmatrix}+\lambda\begin{pmatrix}1\\2\\3\end{pmatrix}.

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