## Linear Algebra and Its Applications, Exercise 2.2.9

Exercise 2.2.9. Consider the following $A$ and $b$:

$A = \begin{bmatrix} 1&2&0&3 \\ 2&4&0&7 \end{bmatrix} \qquad b = \begin{bmatrix} b_1 \\ b_2 \end{bmatrix}$

For what values of $b_1$ and $b_2$ does the system $Ax = b$ have a solution? Also, determine the nullspace of $A$ and provide two examples of vectors within it, and find the general solution to $Ax = b$.

Answer: We perform elimination by subtracting 2 times the first row from the third row:

$\begin{bmatrix} 1&2&0&3 \\ 2&4&0&7 \end{bmatrix} \begin{bmatrix} u \\ v \\ w \\ y \end{bmatrix} = \begin{bmatrix} b_1 \\ b_2 \end{bmatrix} \Rightarrow \begin{bmatrix} 1&2&0&3 \\ 0&0&0&1 \end{bmatrix} \begin{bmatrix} u \\ v \\ w \\ y \end{bmatrix} = \begin{bmatrix} b_1 \\ b_2 - 2b_1 \end{bmatrix}$

This completes elimination and produces the system $Ux = c$:

$\begin{bmatrix} 1&2&0&3 \\ 0&0&0&1 \end{bmatrix} \begin{bmatrix} u \\ v \\ w \\ y \end{bmatrix} = \begin{bmatrix} b_1 \\ b_2 - 2b_1 \end{bmatrix}$

Since the pivots of $U$ are in columns 1 and 4, the basic variables are $u$ and $y$ and the free variables are $v$ and $w$. There are no constraints on the values of $b_1$ and $b_2$.

To find the general solution to $Ax = b$ we start with the system $Ax = 0$, which is equivalent to $Ux = 0$:

$\begin{bmatrix} 1&2&0&3 \\ 0&0&0&1 \end{bmatrix} \begin{bmatrix} u \\ v \\ w \\ y \end{bmatrix} = \begin{bmatrix} 0 \\ 0 \end{bmatrix}$

From the second equation we must have $y = 0$. Substituting the value of $y$ into the first equation we have $u + 2v = 0$ or $u = -2v$. The general solution to $Ax = 0$ can then be expressed in terms of the free variables $v$ and $w$ as follows:

$x_{homogeneous} = v \begin{bmatrix} -2 \\ 1 \\ 0 \\ 0 \end{bmatrix} + w \begin{bmatrix} 0 \\ 0 \\ 1 \\ 0 \end{bmatrix}$

By setting $v = 1$ and $w = 0$ we obtain one vector $(-2, 1, 0, 0)$ in the nullspace of $A$ and by setting $v = 0$ and $w = 1$ we obtain another vector $(0, 0, 1, 0)$ also in the nullspace.

We can obtain a particular solution to $Ax = b$ by going back to the system $Ux = c$ derived above:

$\begin{bmatrix} 1&2&0&3 \\ 0&0&0&1 \end{bmatrix} \begin{bmatrix} u \\ v \\ w \\ y \end{bmatrix} = \begin{bmatrix} b_1 \\ b_2 - 2b_1 \end{bmatrix}$

From the second equation we have $y = b_2 - 2b_1$. Substituting for $y$ into the first equation we have $u + 2v + 3(b_2 - 2b_1) = u + 2v +3b_2 - 6b_1 = b_1$ or $u = -2v + 7b_1 - 3b_2$. Setting the free variables $v$ and $w$ to zero gives the particular solution

$x_{particular} = \begin{bmatrix} 7b_1 - 3b_2 \\ 0 \\ 0 \\ -2b_1 + b_2 \end{bmatrix}$

The general solution to $Ax = b$ is then

$x = x_{particular} + x_{homogeneous} = \begin{bmatrix} 7b_1 - 3b_2 \\ 0 \\ 0 \\ -2b_1 + b_2 \end{bmatrix} + v \begin{bmatrix} -2 \\ 1 \\ 0 \\ 0 \end{bmatrix} + w \begin{bmatrix} 0 \\ 0 \\ 1 \\ 0 \end{bmatrix}$

NOTE: This continues a series of posts containing worked out exercises from the (out of print) book Linear Algebra and Its Applications, Third Edition by Gilbert Strang.

If you find these posts useful I encourage you to also check out the more current Linear Algebra and Its Applications, Fourth Edition, Dr Strang’s introductory textbook Introduction to Linear Algebra, Fourth Edition and the accompanying free online course, and Dr Strang’s other books.

This entry was posted in linear algebra. Bookmark the permalink.