# Linear Algebra/Projection Onto a Subspace

*This subsection, like the others in this section, is optional. It also requires material from the optional earlier subsection on Combining Subspaces.*

The prior subsections project a vector onto a line by decomposing it into two parts: the part in the line and the rest . To generalize projection to arbitrary subspaces, we follow this idea.

- Definition 3.1

For any direct sum and any , the **projection of onto along ** is

where with .

This definition doesn't involve a sense of "orthogonal" so we can apply it to spaces other than subspaces of an . (Definitions of orthogonality for other spaces are perfectly possible, but we haven't seen any in this book.)

- Example 3.2

The space of matrices is the direct sum of these two.

To project

onto along , we first fix bases for the two subspaces.

The concatenation of these

is a basis for the entire space, because the space is the direct sum, so we can use it to represent .

Now the projection of onto along is found by keeping the part of this sum and dropping the part.

- Example 3.3

Both subscripts on are significant. The first subscript matters because the result of the projection is an , and changing this subspace would change the possible results. For an example showing that the second subscript matters, fix this plane subspace of and its basis

and compare the projections along two different subspaces.

(Verification that and is routine.) We will check that these projections are different by checking that they have different effects on this vector.

For the first one we find a basis for

and represent with respect to the concatenation .

The projection of onto along is found by keeping the part and dropping the part.

For the other subspace , this basis is natural.

Representing with respect to the concatenation

and then keeping only the part gives this.

Therefore projection along different subspaces may yield different results.

These pictures compare the two maps. Both show that the projection is indeed "onto" the plane and "along" the line.

Notice that the projection along is not orthogonal— there are members of the plane that are not orthogonal to the dotted line. But the projection along is orthogonal.

A natural question is: what is the relationship between the projection operation defined above, and the operation of orthogonal projection onto a line? The second picture above suggests the answer— orthogonal projection onto a line is a special case of the projection defined above; it is just projection along a subspace perpendicular to the line.

In addition to pointing out that projection along a subspace is a generalization, this scheme shows how to define orthogonal projection onto any subspace of , of any dimension.

- Definition 3.4

The **orthogonal complement**of a subspace of is

(read " perp"). The **orthogonal projection** of a vector is its projection onto along .

- Example 3.5

In , to find the orthogonal complement of the plane

we start with a basis for .

Any perpendicular to every vector in is perpendicular to every vector in the span of (the proof of this assertion is Problem 10). Therefore, the subspace consists of the vectors that satisfy these two conditions.

We can express those conditions more compactly as a linear system.

We are thus left with finding the nullspace of the map represented by the matrix, that is, with calculating the solution set of a homogeneous linear system.

- Example 3.6

Where is the -plane subspace of , what is ? A common first reaction is that is the -plane, but that's not right. Some vectors from the -plane are not perpendicular to every vector in the -plane.

Instead is the -axis, since proceeding as in the prior example and taking the natural basis for the -plane gives this.

The two examples that we've seen since Definition 3.4 illustrate the first sentence in that definition. The next result justifies the second sentence.

- Lemma 3.7

Let be a subspace of . The orthogonal complement of is also a subspace. The space is the direct sum of the two . And, for any , the vector is perpendicular to every vector in .

- Proof

First, the orthogonal complement is a subspace of because, as noted in the prior two examples, it is a nullspace.

Next, we can start with any basis for and expand it to a basis

for the entire space. Apply the Gram-Schmidt process to get an orthogonal basis for . This is the concatenation of two bases (with the same number of members as ) and . The first is a basis for , so if we show that the second is a basis for then we will have that the entire space is the direct sum of the two subspaces.

Problem 9 from the prior subsection proves this about any orthogonal basis: each vector in the space is the sum of its orthogonal projections onto the lines spanned by the basis vectors.

To check this, represent the vector , apply to both sides , and solve to get , as desired.

Since obviously any member of the span of is orthogonal to any vector in , to show that this is a basis for we need only show the other containment— that any is in the span of this basis. The prior paragraph does this. On projections onto basis vectors from , any gives and therefore () gives that is a linear combination of . Thus this is a basis for and is the direct sum of the two.

The final sentence is proved in much the same way. Write . Then is gotten by keeping only the part and dropping the part . Therefore consists of a linear combination of elements of and so is perpendicular to every vector in .

We can find the orthogonal projection onto a subspace by following the steps of the proof, but the next result gives a convienent formula.

- Theorem 3.8

Let be a vector in and let be a subspace of with basis . If is the matrix whose columns are the 's then where the coefficients are the entries of the vector . That is, .

- Proof

The vector is a member of and so it is a linear combination of basis vectors . Since 's columns are the 's, that can be expressed as: there is a such that (this is expressed compactly with matrix multiplication as in Example 3.5 and 3.6). Because is perpendicular to each member of the basis, we have this (again, expressed compactly).

Solving for (showing that is invertible is an exercise)

gives the formula for the projection matrix as .

- Example 3.9

To orthogonally project this vector onto this subspace

first make a matrix whose columns are a basis for the subspace

and then compute.

With the matrix, calculating the orthogonal projection of any vector onto is easy.

## Exercises edit

*This exercise is recommended for all readers.*

- Problem 1

Project the vectors onto along .

*This exercise is recommended for all readers.*

- Problem 2

Find .

- Problem 3

This subsection shows how to project orthogonally in two ways, the method of Example 3.2 and 3.3, and the method of Theorem 3.8. To compare them, consider the plane specified by in .

- Find a basis for .
- Find and a basis for .
- Represent this vector with respect to the concatenation
of the two bases from the prior item.
- Find the orthogonal projection of onto by keeping only the part from the prior item.
- Check that against the result from applying Theorem 3.8.

*This exercise is recommended for all readers.*

- Problem 4

We have three ways to find the orthogonal projection of a vector onto a line, the Definition 1.1 way from the first subsection of this section, the Example 3.2 and 3.3 way of representing the vector with respect to a basis for the space and then keeping the part, and the way of Theorem 3.8. For these cases, do all three ways.

- Problem 5

Check that the operation of Definition 3.1 is well-defined. That is, in Example 3.2 and 3.3, doesn't the answer depend on the choice of bases?

- Problem 6

What is the orthogonal projection onto the trivial subspace?

- Problem 7

What is the projection of onto along if ?

- Problem 8

Show that if is a subspace with orthonormal basis then the orthogonal projection of onto is this.

*This exercise is recommended for all readers.*

- Problem 9

Prove that the map is the projection onto along if and only if the map is the projection onto along . (Recall the definition of the difference of two maps: .)

*This exercise is recommended for all readers.*

- Problem 10

Show that if a vector is perpendicular to every vector in a set then it is perpendicular to every vector in the span of that set.

- Problem 11

True or false: the intersection of a subspace and its orthogonal complement is trivial.

- Problem 12

Show that the dimensions of orthogonal complements add to the dimension of the entire space.

*This exercise is recommended for all readers.*

- Problem 13

Suppose that are such that for all complements , the projections of and onto along are equal. Must equal ? (If so, what if we relax the condition to: all orthogonal projections of the two are equal?)

*This exercise is recommended for all readers.*

- Problem 14

Let be subspaces of . The perp operator acts on subspaces; we can ask how it interacts with other such operations.

- Show that two perps cancel: .
- Prove that implies that .
- Show that .

*This exercise is recommended for all readers.*

- Problem 15

The material in this subsection allows us to express a geometric relationship that we have not yet seen between the rangespace and the nullspace of a linear map.

- Represent given by
- Generalize that to apply to any .
- Represent
*Hint*. See the third item of Problem 14.) - Generalize that to apply to any .

This, and related results, is called the **Fundamental Theorem of Linear Algebra**
in (Strang 1993).

- Problem 16

Define a **projection** to be a linear transformation
with the property that
repeating the projection does nothing more than does the projection
alone:
for all .

- Show that orthogonal projection onto a line has that property.
- Show that projection along a subspace has that property.
- Show that for any such
there is a basis for such that
- Conclude that every projection is a projection along a subspace.
- Also conclude that every projection has a representation

- Problem 17

A square matrix is **symmetric** if each entry equals the
entry (i.e., if the matrix equals its transpose).
Show that the projection matrix
is symmetric. (Strang 1980)
*Hint*. Find properties of transposes by looking in the index
under "transpose".