Equation of Straight Line in Space
Theorem
Symmetric Form
Let $\LL$ be a straight line embedded in a cartesian $3$-space passing through the point $\tuple {x_1, y_1, z_1}$.
$\LL$ is expressed in symmetric form by the equation:
- $\dfrac {x - x_1} l = \dfrac {y - y_1} m = \dfrac {z - z_1} n$
where $l, m, n \in \R$ are the direction ratios of $\LL$.
Two-Point Form
Let $\LL$ be a straight line embedded in a cartesian $3$-space passing through the points $\tuple {x_1, y_1, z_1}$ and $\tuple {x_2, y_2, z_2}$.
$\LL$ is expressed in two-point form by the equation:
- $\dfrac {x - x_1} {x_2 - x_1} = \dfrac {y - y_1} {y_2 - y_1} = \dfrac {z - z_1} {z_2 - z_1}$
Parametric Form
Let $\LL$ be a straight line embedded in a cartesian $3$-space passing through the point $\tuple {x_1, y_1, z_1}$ and with direction cosines $l$, $m$ and $n$.
$\LL$ is expressed in parametric form by the set of equations:
- $\begin {cases} x & = & x_1 + l d \\ y & = & y_1 + m d \\ z & = & z_1 + n d \end {cases}$
where $d \in \R$ is the distance of the variable point $\tuple {x, y, z}$ from $\tuple {x_1, y_1, z_1}$
Vector Form
Let $\mathbf a$ and $\mathbf b$ denote the position vectors of two points in space
Let $L$ be a straight line in space passing through $\mathbf a$ which is parallel to $\mathbf b$.
Let $\mathbf r$ be the position vector of an arbitrary point on $L$.
Then:
- $\mathbf r = \mathbf a + t \mathbf b$
for some real number $t$, which may be positive or negative, or even $0$ if $\mathbf r = \mathbf a$.