In Chapter 2.4, we described lines and planes through the origin using spans and parametric equations. Here, we’ll describe them using linear equations:
Recall, a homogenous linear equation is one whose right-hand side above is 0. We will focus on homogenous equations here, and explore nonzero values of in Chapter 2.6.
Why does one linear equation describe a plane?¶
In , a linear equation of the form , with not both zero, describes a line.
In , a single linear equation with at least one nonzero coefficient describes a plane. For now, we’ll focus on homogeneous equations:
Why a plane instead of a line? For example, consider
or equivalently,
We can plug in any and any to get an output . For instance, when and , we get . Allowing every possible pair of and gives us a plane.
The plane , or . Every pair of and determines a point on the plane.
But a line only works for very specific pairs of and . Recall the line spanned by from Chapter 2.4. There’s no point on this line that has and . Rather, when , is forced to be 4, and is forced to be 5.
So we cannot describe this line by a formula for in terms of and that lets us plug in any and any : most pairs of and -values do not lie on the line.
For example, gives us the -plane.
The equation describes another plane through the origin.
Linear equations for planes¶
Let’s return to the plane from Chapter 2.4:
Note that we don’t yet have a linear equation describing this plane: we’ve expressed the plane as the span of two vectors. How might we find a linear equation that describes this plane?
The plane spanned by and .
For now, we’ll just tell it to you: an equation for this plane is
You should verify yourself that both and satisfy the equation above.
How could we have found this equation without guessing? The key is to find a vector perpendicular to the plane. Note that the equation above can be written as
All vectors that satisfy are perpendicular to !
Normal vectors¶
Remember that in Chapter 2.1, we saw that in the equation of a line in ,
the vector – found by reading the coefficients of and above – is orthogonal to the line above.
Let’s try the same thing here. The coefficients on , , and in
imply the normal vector
The vector is perpendicular to the plane .
To show that is perpendicular to , we need to show that it’s orthogonal to every vector in . There are infinitely many such vectors, but we only need two dot products to get started:
Remember that every vector in is a linear combination of and . Since both dot products above are 0, the dot product of with any of their linear combinations is also 0:
That’s why checking the two spanning vectors is enough. It tells us that is perpendicular to the entire plane.
For our plane through the origin (where ), we can write
The above form is sometimes called the dot-product form equation of a plane.
We’ll write for the set of vectors orthogonal to every vector in . Here it is the line
This extends the perpendicular notation from Chapter 2.1 through Chapter 2.3.
In , the vectors perpendicular to a line through the origin form another line.
In , the vectors perpendicular to a plane through the origin form a line, while the vectors perpendicular to a line through the origin form a plane.
A normal vector is not unique. Using gives , which is the original equation multiplied by 3. The plane does not change.
Finding a normal vector for a plane¶
So far, we’ve checked a normal vector after being given an equation. What if we only know the spanning vectors? Let’s find a normal to the same plane
Write the unknown normal as . It must be orthogonal to both spanning vectors, so
The second equation gives . Substituting into the first gives
Thus and . Choosing gives
These are exactly the coefficients in the plane’s equation:
Any nonzero choice of gives a scalar multiple of this normal and an equivalent equation for the same plane.
Here’s a video reviewing how to find the equation of the plane spanned by two vectors in .
Lines as intersections of planes¶
We now have an understanding of how planes in can be expressed:
As the span of two linearly independent vectors in .
As a linear equation,
(so far, we’ve only seen the case where .)
How do we describe lines using linear equations, when a single linear equation in terms of , , and describes a plane? That is what we will now explore. First, some terminology:
A linear system is a collection of linear equations in the same unknowns.
A solution gives values of the unknowns that satisfy every equation simultaneously. We typically express the solutions as vectors.
The solution set is the set of all solutions – we often think of this as a set of vectors.
A system is homogeneous if every right-hand side is zero. Otherwise, it is nonhomogeneous.
For a concrete example in , consider
Adding the equations gives , so and . Thus, the solution set is
Geometrically, the two lines intersect at the point . The system is nonhomogeneous because its right-hand sides are not all zero.
Now let’s return to . To describe a line, we need two linear equations and take their common solutions. Consider
How do we find two equations? Pick two independent vectors and in , the plane of vectors perpendicular to .
The two independent vectors and lie in (blue), perpendicular to the line (orange).
In our example, a vector is in if
We can choose any values of and and solve for . For instance, choosing gives , while choosing gives . Thus we can use
Both are perpendicular to , and they are not multiples of each other. The line is exactly the set of vectors orthogonal to both normals, so it is the solution set of
What’s happening geometrically? Each equation describes a plane:
The line consists of the points on both planes. In other words,
The symbol means intersection.
The blue plane and orange plane intersect along the pink line .
Our choices of normals were somewhat arbitrary. For example, we could instead use
These are also perpendicular to and are not multiples of each other. They give another pair of planes,
whose intersection is the same line: . The two descriptions are shown side by side below.
Different pairs of planes can have the same intersection: . Drag either panel to rotate its view.
We’ve now described lines and planes through the origin using linear equations (here in Chapter 2.5) as well as in parametric form (in Chapter 2.4). In Chapter 2.6, we’ll translate these objects to study affine lines and planes, which do not need to pass through the origin.