Vector Equations of Lines and Planes in Three Dimensions - StudyPulse
Boost Your VCE Scores Today with StudyPulse
8000+ Questions AI Tutor Help
Home Subjects Specialist Mathematics Vector equations in 3D

Vector Equations of Lines and Planes in Three Dimensions

Specialist Mathematics
StudyPulse

Vector Equations of Lines and Planes in Three Dimensions

Specialist Mathematics
12 May 2026

Vector Equations of Lines and Planes in Three Dimensions

In Specialist Mathematics Unit 4, vectors are extended from two-dimensional space into three-dimensional space (\(\mathbb{R}^3\)). This involves defining lines and planes using vector notation, which provides a powerful alternative to Cartesian coordinate geometry.


1. Vector Equations of Lines in 3D

A line in three-dimensional space is uniquely determined by a point on the line and a direction vector parallel to the line.

The Vector Equation

The vector equation of a line passing through a point with position vector \(\mathbf{a}\) and parallel to a direction vector \(\mathbf{d}\) is given by:
\$\(\mathbf{r} = \mathbf{a} + \lambda \mathbf{d}, \quad \lambda \in \mathbb{R}\)\$
Where:
* \(\mathbf{r} = x\mathbf{i} + y\mathbf{j} + z\mathbf{k}\) is the position vector of any general point on the line.
* \(\mathbf{a} = x_1\mathbf{i} + y_1\mathbf{j} + z_1\mathbf{k}\) is a known point on the line.
* \(\mathbf{d} = l\mathbf{i} + m\mathbf{j} + n\mathbf{k}\) is the direction vector.
* \(\lambda\) is a scalar parameter.

Parametric Equations

By equating the \(\mathbf{i, j, k}\) components of the vector equation, we obtain the parametric equations:
\$\(x = x_1 + \lambda l\)\$
\$\(y = y_1 + \lambda m\)\$
\$\(z = z_1 + \lambda n\)\$

Cartesian (Symmetric) Equation

By solving each parametric equation for \(\lambda\) and equating them, we derive the Cartesian form:
\$\(\frac{x - x_1}{l} = \frac{y - y_1}{m} = \frac{z - z_1}{n}\)\$
Note: If one of the direction components is zero (e.g., \(l=0\)), the line lies in a plane parallel to a coordinate plane (e.g., \(x = x_1\)).

EXAM TIP: When finding the equation of a line passing through two points \(A\) and \(B\), remember that the direction vector \(\mathbf{d}\) is simply the displacement vector \(\vec{AB} = \mathbf{b} - \mathbf{a}\).


2. Vector Equations of Planes

A plane in 3D can be defined in several ways, most commonly by a point in the plane and a vector perpendicular to the surface.

The Normal Form (Scalar Product Form)

If a plane contains a point with position vector \(\mathbf{a}\) and is perpendicular to a normal vector \(\mathbf{n} = a\mathbf{i} + b\mathbf{j} + c\mathbf{k}\), any point \(\mathbf{r}\) on the plane satisfies:
\$\((\mathbf{r} - \mathbf{a}) \cdot \mathbf{n} = 0\)\$
Rearranging gives the standard vector equation of a plane:
\$\(\mathbf{r} \cdot \mathbf{n} = \mathbf{a} \cdot \mathbf{n}\)\$
Let \(\mathbf{a} \cdot \mathbf{n} = d\) (a scalar constant). The equation becomes:
\$\(\mathbf{r} \cdot \mathbf{n} = d\)\$

Cartesian Equation of a Plane

Expanding the scalar product \(\mathbf{r} \cdot \mathbf{n} = d\) where \(\mathbf{r} = x\mathbf{i} + y\mathbf{j} + z\mathbf{k}\) and \(\mathbf{n} = a\mathbf{i} + b\mathbf{j} + c\mathbf{k}\) results in:
\$\(ax + by + cz = d\)\$
The coefficients \((a, b, c)\) are the components of the normal vector to the plane.

Parametric Form of a Plane

A plane can also be defined by a point \(\mathbf{a}\) and two non-parallel (linearly independent) vectors \(\mathbf{u}\) and \(\mathbf{v}\) that lie within the plane:
\$\(\mathbf{r} = \mathbf{a} + \lambda \mathbf{u} + \mu \mathbf{v}, \quad \lambda, \mu \in \mathbb{R}\)\$

KEY TAKEAWAY: The normal vector \(\mathbf{n}\) is the most critical piece of information for a plane. If you are given two vectors \(\mathbf{u}\) and \(\mathbf{v}\) in the plane, you can find the normal vector using the cross product: \(\mathbf{n} = \mathbf{u} \times \mathbf{v}\).


3. Intersections and Relationships

Intersection of a Line and a Plane

To find where the line \(\mathbf{r} = \mathbf{a} + \lambda \mathbf{d}\) intersects the plane \(\mathbf{r} \cdot \mathbf{n} = d\):
1. Substitute the expression for \(\mathbf{r}\) from the line equation into the plane equation.
2. Solve for the scalar \(\lambda\): \((\mathbf{a} + \lambda \mathbf{d}) \cdot \mathbf{n} = d\).
3. \(\mathbf{a} \cdot \mathbf{n} + \lambda(\mathbf{d} \cdot \mathbf{n}) = d \implies \lambda = \frac{d - \mathbf{a} \cdot \mathbf{n}}{\mathbf{d} \cdot \mathbf{n}}\).
4. Substitute \(\lambda\) back into the line equation to find the position vector of the intersection point.

Parallel and Perpendicular Conditions

Relationship Condition
Line parallel to Plane Direction vector \(\mathbf{d}\) is perpendicular to normal \(\mathbf{n}\): \(\mathbf{d} \cdot \mathbf{n} = 0\)
Line perpendicular to Plane Direction vector \(\mathbf{d}\) is parallel to normal \(\mathbf{n}\): \(\mathbf{d} = k\mathbf{n}\)
Two Planes are Parallel Normal vectors are parallel: \(\mathbf{n_1} = k\mathbf{n_2}\)
Two Planes are Perpendicular Normal vectors are perpendicular: \(\mathbf{n_1} \cdot \mathbf{n_2} = 0\)

COMMON MISTAKE: Students often assume that if a line is parallel to a plane, its direction vector is parallel to the normal. In fact, if a line is parallel to a plane, it is perpendicular to the plane’s normal vector.


4. Angles in 3D Space

All angle calculations in 3D rely on the scalar product formula: \(\cos(\theta) = \frac{\mathbf{u} \cdot \mathbf{v}}{|\mathbf{u}||\mathbf{v}|}\).

Angle between Two Lines

The angle \(\theta\) between two lines is the angle between their direction vectors \(\mathbf{d_1}\) and \(\mathbf{d_2}\):
\$\(\cos(\theta) = \frac{|\mathbf{d_1} \cdot \mathbf{d_2}|}{|\mathbf{d_1}||\mathbf{d_2}|}\)\$

Angle between Two Planes

The angle \(\theta\) between two planes is the angle between their normal vectors \(\mathbf{n_1}\) and \(\mathbf{n_2}\):
\$\(\cos(\theta) = \frac{|\mathbf{n_1} \cdot \mathbf{n_2}|}{|\mathbf{n_1}||\mathbf{n_2}|}\)\$

Angle between a Line and a Plane

The angle \(\alpha\) between a line with direction \(\mathbf{d}\) and a plane with normal \(\mathbf{n}\) is the complement of the angle between \(\mathbf{d}\) and \(\mathbf{n}\). If \(\theta\) is the angle between \(\mathbf{d}\) and \(\mathbf{n}\):
\$\(\sin(\alpha) = \cos(\theta) = \frac{|\mathbf{d} \cdot \mathbf{n}|}{|\mathbf{d}||\mathbf{n}|}\)\$

VCAA FOCUS: VCAA frequently asks for the “acute” angle. Always use the absolute value of the dot product in the numerator to ensure \(\cos(\theta) > 0\), resulting in an acute angle.


5. Distances

Distance from a Point to a Plane

The shortest (perpendicular) distance from a point \(P\) with position vector \(\mathbf{p}\) to the plane \(\mathbf{r} \cdot \mathbf{n} = d\) is:
\$\(\text{Distance} = \frac{|\mathbf{p} \cdot \mathbf{n} - d|}{|\mathbf{n}|}\)\$
If the plane is in Cartesian form \(ax + by + cz = d\) and the point is \((x_0, y_0, z_0)\):
\$\(\text{Distance} = \frac{|ax_0 + by_0 + cz_0 - d|}{\sqrt{a^2 + b^2 + c^2}}\)\$

Distance from the Origin to a Plane

Substituting \(\mathbf{p} = \mathbf{0}\) into the formula:
\$\(\text{Distance} = \frac{|d|}{|\mathbf{n}|}\)\$

REMEMBER: The unit normal vector \(\hat{\mathbf{n}} = \frac{\mathbf{n}}{|\mathbf{n}|}\) is useful here. The equation \(\mathbf{r} \cdot \hat{\mathbf{n}} = p\) represents a plane where \(p\) is the perpendicular distance from the origin to the plane.

Table of Contents