Math 1600 Lecture 19, Section 2, 20 Oct 2014

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Announcements:

Continue reading Section 3.5. Work through recommended homework questions.

Tutorials: Midterm review this week. No quiz.

Office hour: today, 3:00-3:30, MC103B.

Help Centers: Monday-Friday 2:30-6:30 in MC106.

Extra Midterm Review: Friday, October 24, details TBA. Bring questions.

Midterm: Saturday, October 25, 7-10pm. Rooms: A-E: UCC37. F-Ma: UCC56 (this room). Mc-Z: UCC146. It will cover the material up to and including today's lecture. Practice midterms are on website.

Partial review of Lecture 18:

Subspaces

Definition: A subspace of $\R^n$ is any collection $S$ of vectors in $\R^n$ such that:
1. The zero vector $\vec 0$ is in $S$.
2. $S$ is closed under addition: If $\vu$ and $\vv$ are in $S$, then $\vu + \vv$ is in $S$.
3. $S$ is closed under scalar multiplication: If $\vu$ is in $S$ and $c$ is any scalar, then $c \vu$ is in $S$.

Conditions (2) and (3) together are the same as saying that $S$ is closed under linear combinations.

Example: $\R^n$ is a subspace of $\R^n$. Also, $S = \{ \vec 0 \}$ is a subspace of $\R^n$.

A line or plane through the origin in $\R^3$ is a subspace. Applet.

On the other hand, a plane not through the origin is not a subspace. It of course fails (1), but the other conditions fail as well, as shown in the applet.

Theorem 3.19: Let $\vv_1, \vv_2, \ldots, \vv_k$ be vectors in $\R^n$. Then $\span(\vv_1, \ldots, \vv_k)$ is a subspace of $\R^n$.

Subspaces associated with matrices

Theorem 3.21: Let $A$ be an $m \times n$ matrix and let $N$ be the set of solutions of the homogeneous system $A \vx = \vec 0$. Then $N$ is a subspace of $\R^n$.

Spans and null spaces are the two main sources of subspaces.

Definition: Let $A$ be an $m \times n$ matrix.

1. The row space of $A$ is the subspace $\row(A)$ of $\R^n$ spanned by the rows of $A$.
2. The column space of $A$ is the subspace $\col(A)$ of $\R^m$ spanned by the columns of $A$.
3. The null space of $A$ is the subspace $\null(A)$ of $\R^n$ consisting of the solutions to the system $A \vx = \vec 0$.

Example: The column space of $A = \bmat{rr} 1 & 2 \\ 3 & 4 \emat$ is $\span(\coll 1 3, \coll 2 4)$, which we saw is all of $\R^2$. We also saw that the row space of $A$ is $\R^2$ and the null space is $\{ \vec 0 \}$.

Example: The column space of $A = \bmat{rr} 1 & 2 \\ 3 & 4 \\ 5 & 6 \emat$ is the span of the two columns, which is a subspace of $\R^3$. Since the columns are linearly independent, this is a plane through the origin in $\R^3$.

Basis

We know that to describe a plane $\cP$ through the origin, we can give two direction vectors $\vu$ and $\vv$ which are linearly independent. Then $\cP = \span(\vu, \vv)$. We know that two vectors is always enough, and one vector will not work.

Definition: A basis for a subspace $S$ of $\R^n$ is a set of vectors $\vv_1, \ldots, \vv_k$ such that:
1. $S = \span(\vv_1, \ldots, \vv_k)$, and
2. $\vv_1, \ldots, \vv_k$ are linearly independent.

Condition (2) ensures that none of the vectors is redundant, so we aren't being wasteful. Giving a basis for a subspace is a good way to "describe" it.

Example 3.42: The standard unit vectors $\ve_1, \ldots, \ve_n$ in $\R^n$ are linearly independent and span $\R^n$, so they form a basis of $\R^n$ called the standard basis.

Example: We saw above that $\coll 1 3$ and $\coll 2 4$ span $\R^2$. They are also linearly independent, so they are a basis for $\R^2$.

Note that $\coll 1 0$ and $\coll 0 1$ are another basis for $\R^2$. A subspace will in general have many bases, but we'll see soon that they all have the same number of vectors! (Grammar: one basis, two bases.)

New material

Example: Let $\cP$ be the plane through the origin with direction vectors $\colll 1 3 5$ and $\colll 2 4 6$. Then $\cP$ is a subspace of $\R^3$ and these two vectors are a basis for $\cP$.

Example: Find a basis for $S = \span(\colll 3 0 2, \colll {-2} 1 1, \colll 1 1 3)$.

Solution:

In more complicated situations, there are two ways to find a basis of the span of a set of vectors. The first way uses the following result:

Theorem 3.20: Let $A$ and $B$ be row equivalent matrices. Then $\row(A) = \row(B)$.

Proof: Suppose $B$ is obtained from $A$ by performing elementary row operations. Each of these operations expresses the new row as a linear combination of the previous rows. So every row of $B$ is a linear combination of the rows of $A$. So $\row(B)\ \red{\subseteq}\ \row(A)$.

On the other hand, each row operation is reversible, so reversing the above argument gives that $\row(A) \subseteq \row(B)$. Therefore, $\row(A) = \row(B). \quad \Box$

This will be useful, because it is easy to understand the row space of a matrix in row echelon form.

Example: Let's redo the above example. Consider the matrix $$ A = \bmat{rrr} 3 & 0 & 2 \\ -2 & 1 & 1 \\ 1 & 1 & 3 \emat $$ whose rows are the given vectors. So $S = \row(A)$.

Row reduction produces the following matrix $$ B = \bmat{ccc} 1 & 0 & 2/3 \\ 0 & 1 & 7/3 \\ 0 & 0 & 0 \emat $$ which is in reduced row echelon form. By Theorem 3.20, $S = \row(B)$. But the first two rows clearly give a basis for $\row(B)$, so another solution to the question is $\ccolll 1 0 {2/3}$ and $\ccolll 0 1 {7/3}$.

Theorem: If $R$ is a matrix in row echelon form, then the nonzero rows of $R$ form a basis for $\row(R)$.

Example: Let $$ R = \bmat{rrrr} 1 & 2 & 3 & 4 \\ 0 & 5 & 6 & 7 \\ 0 & 0 & 0 & 8 \\ 0&0&0&0 \emat = \collll {\va_1} {\va_2} {\va_3} {\va_4} $$ $\row(R)$ is the span of the nonzero rows, since zero rows don't contribute. So we just need to see that the nonzero rows are linearly independent. If we had $c_1 \va_1 + c_2 \va_2 + c_3 \va_3 = \vec 0$, then $c_1 = 0$, by looking at the first component. So $5 c_2 = 0$, by looking at the second component. And so $8 c_3 = 0$, by looking at the fourth component. So $c_1 = c_2 = c_3 = 0$.

The same argument works in general, by looking at the pivot (leading) columns, and this proves the Theorem.

This gives rise to the row method for finding a basis for a subspace $S$ spanned by some vectors $\vv_1, \ldots, \vv_k$:

1. Form the matrix $A$ whose rows are $\vv_1, \ldots, \vv_k$, so $S = \row(A)$.
2. Reduce $A$ to row echelon form $R$.
3. The nonzero rows of $R$ will be a basis of $S = \row(A) = \row(R)$.

Notice that the vectors you get are usually different from the vectors you started with. Given $S = \span(\vv_1, \ldots, \vv_k)$, one can always find a basis for $S$ which just omits some of the given vectors. We'll explain this next.

Suppose we form a matrix $A$ whose columns are $\vv_1, \ldots, \vv_k$. A nonzero solution to the system $A \vx = \vec 0$ is exactly a dependency relationship between the given vectors. Also, recall that if $R$ is row equivalent to $A$, then $R \vx = \vec 0$ has the same solutions as $A \vx = \vec 0$. This means that the columns of $R$ have the same dependency relationships as the columns of $A$.

Example 3.47: Find a basis for the column space of $$ A = \bmat{rrrrr} 1 & 1 & 3 & 1 & 6 \\ 2 & -1 & 0 & 1 & -1 \\ -3 & 2 & 1 & -2 & 1 \\ 4 & 1 & 6 & 1 & 3 \emat $$ Solution: The reduced row echelon form is $$ R = \bmat{rrrrr} 1 & 0 & 1 & 0 & -1 \\ 0 & 1 & 2 & 0 & 3 \\ 0 & 0 & 0 & 1 & 4 \\ 0 & 0 & 0 & 0 & 0 \emat $$ Write $\vr_i$ for the columns of $R$ and $\va_i$ for the columns of $A$. You can see immediately that $\vr_3 = \vr_1 + 2 \vr_2$ and $\vr_5 = -\vr_1 + 3\vr_2 + 4\vr_4$. So $\col(R) = \span(\vr_1, \vr_2, \vr_4)$, and these three are linearly independent since they are standard unit vectors.

It follows that the columns of $A$ have the same dependency relationships: $\va_3 = \va_1 + 2 \va_2$ and $\va_5 = -\va_1 + 3\va_2 + 4\va_4$. Also, $\va_1$, $\va_2$ and $\va_4$ must be linearly independent. So a basis for $\col(A)$ is given by $\va_1$, $\va_2$ and $\va_4$.

Note that these are the columns corresponding to the leading 1's in $R$!

Warning: Elementary row operations change the column space! So $\col(A) \neq \col(R)$. So while $\vr_1$, $\vr_2$ and $\vr_4$ are a basis for $\col(R)$, they are not a solution to the question asked.

The other kind of subspace that arises a lot is the null space of a matrix $A$, the subspace of solutions to the homogeneous system $A \vx = \vec 0$. We learned in Chapter 2 how to find a basis for this subspace, even though we didn't use this terminology.

Example 3.48: Find a basis for the null space of the $4 \times 5$ matrix $A$ above.

Solution: The reduced row echelon form of $[A \mid \vec 0\,]$ is $$ [R \mid \vec 0\,] = \bmat{rrrrr|r} 1 & 0 & 1 & 0 & -1 & 0 \\ 0 & 1 & 2 & 0 & 3 & 0 \\ 0 & 0 & 0 & 1 & 4 & 0 \\ 0 & 0 & 0 & 0 & 0 & 0 \emat $$ We see that $x_3$ and $x_5$ are free variables, so we let $x_3 = s$ and $x_5 = t$ and use back substitution to find that $$ \vx = \colllll {x_1} {x_2} {x_3} {x_4} {x_5} = s \colllll {-1} {-2} 1 0 0 + t \colllll 1 {-3} 0 {-4} 1 \qqtext{(See text.)} $$ Therefore, the two column vectors shown form a basis for the null space.

The vectors that arise in this way will always be linearly independent, since if all $x_i$'s are $0$, then the free variables must be zero, so the parameters must be zero.

Summary

Finding bases for $\row(A)$, $\col(A)$ and $\null(A)$:

1. Find the reduced row echelon form $R$ of $A$.
2. The nonzero rows of $R$ form a basis for $\row(A) = \row(R)$.
3. The columns of $A$ that correspond to the columns of $R$ with leading 1's form a basis for $\col(A)$.
4. Use back substitution to solve $R \vx = \vec 0$; the vectors that arise are a basis for $\null(A) = \null(R)$.

You just need to do row reduction once to answer all three questions!

We have seen two ways to compute a basis of a span of a set of vectors. One is to make them the columns of a matrix, and the other is to make them the rows. The column method produces a basis using vectors from the original set. Both ways require about the same amount of work.

Similarly, if asked to find a basis for $\row(A)$, one could use the column method on $A^T$.

Dimension

We have seen that a subspace has many bases. Have you noticed anything about the number of vectors in each basis?

Idea of proof:

A very similar argument works for the general case.

Definition: The number of vectors in a basis for a subspace $S$ is called the dimension of $S$, denoted $\dim S$.

Example: $\dim \R^n = \query{n}$

Example: If $S$ is a line through the origin in $\R^2$ or $\R^3$, then $\dim S = \query{1}$

Example: If $S$ is a plane through the origin in $\R^3$, then $\dim S = \query{2}$

Example: If $S = \span(\colll 3 0 2, \colll {-2} 1 1, \colll 1 1 3)$, then $\dim S = \query{2}$