Consider a straight line passing through the point \(A(\vec{a})\) and parallel to the vector \(\vec{b}.\)

Any point \(\vec{r}\) on this line can be written in terms of real parameter  \(\lambda \).


\[\begin{align}& \vec{r}=\overrightarrow{OA}+\overrightarrow{AR} \\\\  &\;\ =\vec{a}+\lambda \vec{b}\,\,\qquad\qquad\qquad\;where\,\,\lambda \in \mathbb{R} \\ \end{align}\]

The equation

\[\boxed{\vec r = \vec a + \lambda \vec b}\]

can be viewed as the (vector) equation of this line. As we vary \(\lambda \), we get varying position vectors \(\vec{r}\) and hence varying points on this line.

This form of the equation of a line is called the parametricform since it involves the use of a parameter \(\lambda \). We could also have specified the equation in non-parametric form. Observe that since \(\overrightarrow {AR} \) is parallel to  \(\vec b,\) we have

\[\begin{align}&\qquad\;\left( {\vec r - \vec a} \right) \times \vec b = \vec 0 \hfill \\&\Rightarrow \quad  \boxed{\vec r \times \vec b = \vec a \times \vec b} \hfill \\ \end{align} \]

This is the required equation of the line. You must convince yourself that this equation is valid; in particular, understand that only points lying on the line and none other will satisfy this equation.

We can use the equations obtained above to obtained the equation of a line passing through the points \(A(\vec a)\,and\,B(\vec b).\)

\[\boxed{\vec r = \vec a + \lambda (\vec b - \vec a)}\qquad \qquad Parametric{\text{ }}form\]


\[\begin{align}& \qquad\;(\vec r - \vec a) \times (\vec b - \vec a) = \vec 0 \hfill \\\\&\Rightarrow \quad  \boxed{\vec r \times (\vec b - \vec a) = \vec a \times \vec b}\qquad \qquad Non{\text{ }} - {\text{ }}parametric{\text{ }}form \hfill \\ \end{align} \]

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