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Module 2 · Matrix Algebra

A⁻¹ and Ax = b

Using the inverse matrix to understand and solve systems of linear equations.

$A^{-1}$ and $A\mathbf{x}=\mathbf{b}$

In the previous lesson, we introduced the inverse matrix.

If $A$ is invertible, its inverse satisfies

\[AA^{-1}=A^{-1}A=I.\]

We interpreted $A^{-1}$ as the transformation that undoes the transformation performed by $A$.

Now we can connect that idea directly to one of the central equations of linear algebra:

\[A\mathbf{x}=\mathbf{b}.\]

The key result of this lesson is

$$ A\mathbf{x}=\mathbf{b} \quad\Longrightarrow\quad \mathbf{x}=A^{-1}\mathbf{b}. $$

But rather than treating this as just a formula, we want to understand why it works, what it means, and when it is useful.


1. Start with a familiar equation

Consider the ordinary equation

\[5x=10.\]

How do we solve it?

We multiply both sides by the reciprocal of $5$:

\[\frac{1}{5}(5x) = \frac{1}{5}(10).\]

Therefore,

\[x=2.\]

The important idea is that multiplication by $5$ can be undone by multiplication by

\[\frac{1}{5}.\]

In other words,

\[\frac{1}{5}\cdot5=1.\]

The number $1$ leaves $x$ unchanged:

\[1x=x.\]

2. The matrix version

Now consider

\[A\mathbf{x}=\mathbf{b}.\]

This looks similar to

\[5x=10.\]

The difference is that $A$ is a matrix and $\mathbf{x}$ and $\mathbf{b}$ are vectors.

We need something that plays the role of

\[\frac{1}{5}.\]

That something is the inverse matrix:

\[A^{-1}.\]

Recall that

\[A^{-1}A=I.\]

The identity matrix $I$ plays the role of the number $1$.

So we multiply both sides of

\[A\mathbf{x}=\mathbf{b}\]

by $A^{-1}$:

$$ A^{-1}(A\mathbf{x}) = A^{-1}\mathbf{b}. $$

Using associativity,

\[(A^{-1}A)\mathbf{x} = A^{-1}\mathbf{b}.\]

Since

\[A^{-1}A=I,\]

we obtain

\[I\mathbf{x}=A^{-1}\mathbf{b}.\]

And because

\[I\mathbf{x}=\mathbf{x},\]

we finally get

$$ \mathbf{x}=A^{-1}\mathbf{b}. $$

This is the matrix equivalent of dividing both sides of an ordinary equation by $5$.


3. What does $A^{-1}\mathbf{b}$ mean?

The expression

\[A^{-1}\mathbf{b}\]

may initially look abstract.

But remember what $A^{-1}$ does.

The matrix $A$ takes an input vector and transforms it:

\[\mathbf{x} \longrightarrow A\mathbf{x}.\]

Suppose the result is $\mathbf{b}$:

\[\mathbf{x} \xrightarrow{\;A\;} \mathbf{b}.\]

Then $A^{-1}$ reverses the transformation:

\[\mathbf{b} \xrightarrow{\;A^{-1}\;} \mathbf{x}.\]

So we have

$$ \mathbf{x} \;\xrightarrow{\;A\;}\; \mathbf{b} \;\xrightarrow{\;A^{-1}\;}\; \mathbf{x}. $$

Therefore,

\[A^{-1}\mathbf{b}\]

means:

Take $\mathbf b$ and reverse the transformation $A$.

The result is the vector $\mathbf{x}$ that produced $\mathbf b$.


4. A complete numerical example

Consider the system

$$ \begin{aligned} 2x+y&=5,\\ x+y&=3. \end{aligned} $$

In matrix form,

$$ \begin{bmatrix} 2&1\\ 1&1 \end{bmatrix} \begin{bmatrix} x\\ y \end{bmatrix} = \begin{bmatrix} 5\\ 3 \end{bmatrix}. $$

Write this as

\[A\mathbf{x}=\mathbf{b},\]

where

$$ A= \begin{bmatrix} 2&1\\ 1&1 \end{bmatrix}, \qquad \mathbf{x}= \begin{bmatrix} x\\ y \end{bmatrix}, \qquad \mathbf{b}= \begin{bmatrix} 5\\ 3 \end{bmatrix}. $$

From the previous lesson, we know that

\[A^{-1} = \begin{bmatrix} 1&-1\\ -1&2 \end{bmatrix}.\]

Therefore,

\[\mathbf{x}=A^{-1}\mathbf{b}.\]

Substitute the matrices:

$$ \mathbf{x} = \begin{bmatrix} 1&-1\\ -1&2 \end{bmatrix} \begin{bmatrix} 5\\ 3 \end{bmatrix}. $$

Multiply:

$$ \mathbf{x} = \begin{bmatrix} 1(5)+(-1)(3)\\ (-1)(5)+2(3) \end{bmatrix} = \begin{bmatrix} 2\\ 1 \end{bmatrix}. $$

Therefore,

\[x=2,\qquad y=1.\]

5. Check the answer

We should always be able to check a solution.

The original system was

\[2x+y=5\]

and

\[x+y=3.\]

Substitute

\[x=2,\qquad y=1.\]

Then

\[2(2)+1=5\]

and

\[2+1=3.\]

Both equations are satisfied.

So

$$ \mathbf{x} = \begin{bmatrix} 2\\ 1 \end{bmatrix} $$

is indeed the solution.


6. The inverse gives a formula for the solution

The previous example illustrates a general result.

If $A$ is invertible, then

\[A\mathbf{x}=\mathbf{b}\]

has the unique solution

$$ \mathbf{x}=A^{-1}\mathbf{b}. $$

This means that once $A^{-1}$ is known, we can solve the system for any right-hand side $\mathbf b$.

That observation becomes especially important when $A$ stays fixed but $\mathbf b$ changes.


7. What if $\mathbf b$ changes?

Suppose the matrix $A$ stays fixed:

\[A\mathbf{x}=\mathbf b.\]

Imagine that we need to solve several systems:

$$ A\mathbf{x}_1=\mathbf b_1, $$ $$ A\mathbf{x}_2=\mathbf b_2, $$ $$ A\mathbf{x}_3=\mathbf b_3. $$

If $A$ is invertible, then

$$ \mathbf{x}_1=A^{-1}\mathbf b_1, $$ $$ \mathbf{x}_2=A^{-1}\mathbf b_2, $$ $$ \mathbf{x}_3=A^{-1}\mathbf b_3. $$

The same inverse works for every right-hand side.

This is one reason the inverse is mathematically useful.

The matrix $A$ determines the transformation.

The vector $\mathbf b$ tells us the desired output.

The inverse tells us which input produces that output.


8. Think of $A$ as a machine

Here is another way to see the same idea.

Imagine that $A$ is a machine.

You put in $\mathbf{x}$:

\[\mathbf{x} \longrightarrow A \longrightarrow \mathbf b.\]

The equation

\[A\mathbf{x}=\mathbf b\]

asks:

Which input $\mathbf{x}$ produces the output $\mathbf b$?

If $A$ is invertible, we can run the machine backward:

\[\mathbf b \longrightarrow A^{-1} \longrightarrow \mathbf{x}.\]

Therefore,

\[\mathbf{x}=A^{-1}\mathbf b.\]

This interpretation will become increasingly important as we study linear transformations.


9. The columns of $A$ tell us something important

Suppose

\[A= \begin{bmatrix} |&|\\ \mathbf a_1&\mathbf a_2\\ |&| \end{bmatrix}.\]

Then

\[A \begin{bmatrix} x_1\\ x_2 \end{bmatrix} = x_1\mathbf a_1+x_2\mathbf a_2.\]

Therefore,

\[A\mathbf{x}=\mathbf b\]

can be written as

\[x_1\mathbf a_1+x_2\mathbf a_2=\mathbf b.\]

This says something fundamental:

We are looking for a combination of the columns of $A$ that produces $\mathbf b$.

The coefficients of that combination are the entries of $\mathbf{x}$.

So solving

\[A\mathbf{x}=\mathbf b\]

is also a question about the columns of $A$.


10. A two-dimensional example

Consider

\[A= \begin{bmatrix} 2&1\\ 1&1 \end{bmatrix}.\]

Its columns are

\[\mathbf a_1= \begin{bmatrix} 2\\ 1 \end{bmatrix}, \qquad \mathbf a_2= \begin{bmatrix} 1\\ 1 \end{bmatrix}.\]

Suppose

\[\mathbf{x} = \begin{bmatrix} 2\\ 1 \end{bmatrix}.\]

Then

$$ A\mathbf{x} = 2 \begin{bmatrix} 2\\ 1 \end{bmatrix} + 1 \begin{bmatrix} 1\\ 1 \end{bmatrix} = \begin{bmatrix} 5\\ 3 \end{bmatrix}. $$

So

\[\mathbf b= \begin{bmatrix} 5\\ 3 \end{bmatrix}\]

is produced by taking

\[2\mathbf a_1+\mathbf a_2.\]

The solution

\[\mathbf{x} = \begin{bmatrix} 2\\ 1 \end{bmatrix}\]

contains exactly those coefficients.

This gives us another interpretation:

\[A\mathbf{x}=\mathbf b\]

asks:

Which linear combination of the columns of $A$ gives $\mathbf b$?


11. What does the inverse do to the columns?

Now something interesting happens.

Let

\[I= \begin{bmatrix} 1&0\\ 0&1 \end{bmatrix}.\]

Consider

\[AX=I.\]

Here $X$ is an unknown matrix.

We want to find the matrix $X$ that transforms $A$ into $I$.

Since

\[A^{-1}A=I,\]

we know that

\[X=A^{-1}.\]

Therefore,

\[AA^{-1}=I.\]

But let’s look at this column by column.

Write

\[A^{-1} = \begin{bmatrix} |&|\\ \mathbf x_1&\mathbf x_2\\ |&| \end{bmatrix}.\]

Then

\[AA^{-1} = \begin{bmatrix} |&|\\ A\mathbf x_1&A\mathbf x_2\\ |&| \end{bmatrix}.\]

But

\[AA^{-1}=I.\]

Therefore,

\[A\mathbf x_1=\mathbf e_1\]

and

\[A\mathbf x_2=\mathbf e_2,\]

where

\[\mathbf e_1= \begin{bmatrix} 1\\ 0 \end{bmatrix}, \qquad \mathbf e_2= \begin{bmatrix} 0\\ 1 \end{bmatrix}.\]

This gives us a useful interpretation of the inverse.


12. The columns of $A^{-1}$

The first column of $A^{-1}$ is the solution of

\[A\mathbf x=\mathbf e_1.\]

The second column of $A^{-1}$ is the solution of

\[A\mathbf x=\mathbf e_2.\]

More generally, for an $n\times n$ matrix,

\[A^{-1} = \begin{bmatrix} |&|&&|\\ \mathbf x_1&\mathbf x_2&\cdots&\mathbf x_n\\ |&|&&| \end{bmatrix},\]

where

\[A\mathbf x_1=\mathbf e_1,\] \[A\mathbf x_2=\mathbf e_2,\]

and so on.

Therefore,

$$ A^{-1} = \left[ \begin{array}{cccc} |&|&&|\\ A^{-1}\mathbf e_1& A^{-1}\mathbf e_2& \cdots& A^{-1}\mathbf e_n\\ |&|&&| \end{array} \right]. $$

This is a useful way to understand where the inverse comes from.


13. Finding the inverse means solving many systems

This gives us a new perspective.

To find $A^{-1}$, we need to solve

\[AX=I.\]

Since $I$ has $n$ columns, this is equivalent to solving $n$ systems:

$$ A\mathbf x_1=\mathbf e_1, \qquad A\mathbf x_2=\mathbf e_2, \qquad \ldots, \qquad A\mathbf x_n=\mathbf e_n. $$

The solutions become the columns of $A^{-1}$.

So computing an inverse is really a collection of linear-system problems.

This connects our earlier lessons directly to the inverse.


14. Why $[A\mid I]$ works

This also explains the augmented-matrix method we saw in the previous lesson.

Start with

\[[A\mid I].\]

The goal is to transform the left side into $I$:

$$ [A\mid I] \quad\longrightarrow\quad [I\mid A^{-1}]. $$

Why?

Because the row operations are effectively finding the matrix that transforms $A$ into $I$.

If the sequence of elementary matrices is

\[E_k\cdots E_2E_1,\]

then

$$ E_k\cdots E_2E_1A=I. $$

Therefore,

$$ E_k\cdots E_2E_1=A^{-1}. $$

Applying those same operations to $I$ gives the inverse.

That is why the algorithm works.


15. Inverse and uniqueness

Now we can understand why invertibility is closely connected to unique solutions.

Suppose

\[A\mathbf{x}=\mathbf b\]

and $A^{-1}$ exists.

Then

\[\mathbf{x}=A^{-1}\mathbf b.\]

There is only one possible value for $\mathbf{x}$.

Therefore:

$$ A\text{ invertible} \Longrightarrow A\mathbf{x}=\mathbf b \text{ has exactly one solution for every }\mathbf b. $$

This is a major result.

An invertible matrix does not merely allow us to calculate a solution.

It guarantees that the solution is unique.


16. What happens if $A$ is singular?

Now consider a singular matrix:

\[A= \begin{bmatrix} 1&2\\ 2&4 \end{bmatrix}.\]

Its columns are

\[\mathbf a_1= \begin{bmatrix} 1\\ 2 \end{bmatrix}\]

and

\[\mathbf a_2= \begin{bmatrix} 2\\ 4 \end{bmatrix}.\]

Notice:

\[\mathbf a_2=2\mathbf a_1.\]

So the columns point in the same direction.

They do not provide two independent directions.

Now consider

\[A \begin{bmatrix} x\\ y \end{bmatrix} = \begin{bmatrix} b_1\\ b_2 \end{bmatrix}.\]

The left side is

$$ x \begin{bmatrix} 1\\ 2 \end{bmatrix} + y \begin{bmatrix} 2\\ 4 \end{bmatrix} = (x+2y) \begin{bmatrix} 1\\ 2 \end{bmatrix}. $$

Every output lies on the same line.

Therefore, a vector such as

\[\begin{bmatrix} 1\\ 3 \end{bmatrix}\]

cannot be produced.

So the system

\[A\mathbf{x} = \begin{bmatrix} 1\\ 3 \end{bmatrix}\]

has no solution.


17. But singular can also mean infinitely many solutions

Consider instead

\[\mathbf b= \begin{bmatrix} 1\\ 2 \end{bmatrix}.\]

Then

\[A\mathbf{x}=\mathbf b\]

becomes

$$ \begin{bmatrix} 1&2\\ 2&4 \end{bmatrix} \begin{bmatrix} x\\ y \end{bmatrix} = \begin{bmatrix} 1\\ 2 \end{bmatrix}. $$

The two equations are

\[x+2y=1\]

and

\[2x+4y=2.\]

But the second equation is simply twice the first.

So we really have only one independent equation:

\[x+2y=1.\]

There are infinitely many solutions.

For example,

\[y=0 \quad\Longrightarrow\quad x=1,\]

while

\[y=1 \quad\Longrightarrow\quad x=-1.\]

Both work.

So a singular matrix can lead to:

  • no solution, or
  • infinitely many solutions.

But it cannot give exactly one solution for every $\mathbf b$.


18. The three possibilities

For a square system

\[A\mathbf{x}=\mathbf b,\]

there are three possibilities.

One solution

The matrix $A$ is invertible.

$$ \mathbf{x}=A^{-1}\mathbf b $$

for every $\mathbf b$.

No solution

The vector $\mathbf b$ is not reachable by the columns of $A$.

Infinitely many solutions

The columns of $A$ do not provide enough independent directions, but $\mathbf b$ is still reachable.

This gives us the basic picture:

$$ \begin{array}{c|c} \text{Matrix }A & \text{Solutions of }A\mathbf{x}=\mathbf b\\ \hline \text{Invertible} & \text{Exactly one for every }\mathbf b\\ \text{Singular} & \text{None or infinitely many} \end{array} $$

19. Why can an invertible matrix never have two solutions?

Suppose $A$ is invertible and somehow

\[A\mathbf{x}_1=\mathbf b\]

and

\[A\mathbf{x}_2=\mathbf b.\]

Then

\[A\mathbf{x}_1=A\mathbf{x}_2.\]

Subtract:

\[A(\mathbf{x}_1-\mathbf{x}_2)=\mathbf0.\]

Now multiply by $A^{-1}$:

$$ A^{-1}A(\mathbf{x}_1-\mathbf{x}_2) = A^{-1}\mathbf0. $$

Therefore,

\[\mathbf{x}_1-\mathbf{x}_2=\mathbf0.\]

So

\[\mathbf{x}_1=\mathbf{x}_2.\]

Thus two different solutions are impossible.

This proves uniqueness.


20. The homogeneous system

There is a particularly important special case:

\[A\mathbf{x}=\mathbf0.\]

This is called the homogeneous system.

There is always at least one solution:

\[\mathbf{x}=\mathbf0.\]

Why?

Because

\[A\mathbf0=\mathbf0.\]

But the important question is:

Is the zero vector the only solution?

If $A$ is invertible, multiply by $A^{-1}$:

\[A^{-1}A\mathbf{x} = A^{-1}\mathbf0.\]

Therefore,

\[\mathbf{x}=\mathbf0.\]

So an invertible matrix satisfies

$$ A\mathbf{x}=\mathbf0 \quad\Longrightarrow\quad \mathbf{x}=\mathbf0. $$

This fact will become extremely important when we study linear independence.


21. The inverse and the columns of $A$

Recall that

\[A\mathbf{x} = x_1\mathbf a_1 + x_2\mathbf a_2 + \cdots + x_n\mathbf a_n.\]

If

\[A\mathbf{x}=\mathbf b,\]

then solving the system means finding coefficients

\[x_1,x_2,\ldots,x_n\]

that express $\mathbf b$ as a combination of the columns of $A$.

If $A$ is invertible, those coefficients are unique.

Therefore:

An invertible matrix has columns that can uniquely represent every vector in $\mathbb R^n$.

This is a deeper interpretation of the inverse.

It connects inverse matrices to the ideas we will study later:

  • linear combinations,
  • span,
  • linear independence,
  • column space,
  • basis.

22. One inverse, many right-hand sides

Suppose we have the same matrix $A$ but many different right-hand sides:

$$ A\mathbf{x}_1=\mathbf b_1, \qquad A\mathbf{x}_2=\mathbf b_2, \qquad \ldots, \qquad A\mathbf{x}_k=\mathbf b_k. $$

If $A^{-1}$ exists, then

$$ \mathbf{x}_1=A^{-1}\mathbf b_1, \qquad \mathbf{x}_2=A^{-1}\mathbf b_2, \qquad \ldots, \qquad \mathbf{x}_k=A^{-1}\mathbf b_k. $$

We can put all the right-hand sides into one matrix:

\[B= \begin{bmatrix} |&|&&|\\ \mathbf b_1&\mathbf b_2&\cdots&\mathbf b_k\\ |&|&&| \end{bmatrix}.\]

Similarly, put all the solutions into

\[X= \begin{bmatrix} |&|&&|\\ \mathbf x_1&\mathbf x_2&\cdots&\mathbf x_k\\ |&|&&| \end{bmatrix}.\]

Then all the systems can be written at once:

\[AX=B.\]

Multiply by $A^{-1}$:

$$ A^{-1}AX=A^{-1}B. $$

Therefore,

$$ X=A^{-1}B. $$

This is one of the reasons matrix notation is so powerful.

A whole collection of linear systems can be represented by one matrix equation.


23. A numerical example with multiple right-hand sides

Suppose

\[A= \begin{bmatrix} 2&1\\ 1&1 \end{bmatrix}\]

and

\[A^{-1} = \begin{bmatrix} 1&-1\\ -1&2 \end{bmatrix}.\]

Suppose we want to solve two systems at once:

$$ A \begin{bmatrix} x_1&x_2\\ y_1&y_2 \end{bmatrix} = \begin{bmatrix} 5&7\\ 3&4 \end{bmatrix}. $$

Call the unknown matrix $X$ and the right-hand side matrix $B$:

\[AX=B.\]

Then

\[X=A^{-1}B.\]

Therefore,

$$ X = \begin{bmatrix} 1&-1\\ -1&2 \end{bmatrix} \begin{bmatrix} 5&7\\ 3&4 \end{bmatrix}. $$

Multiply:

$$ X = \begin{bmatrix} 2&3\\ 1&1 \end{bmatrix}. $$

So the two solutions are

\[\mathbf{x}_1= \begin{bmatrix} 2\\ 1 \end{bmatrix}\]

and

\[\mathbf{x}_2= \begin{bmatrix} 3\\ 1 \end{bmatrix}.\]

The same inverse solved both systems.


24. A practical warning

At this point, it may seem that the best way to solve every system is:

\[\mathbf{x}=A^{-1}\mathbf b.\]

Mathematically, this is completely correct.

But computationally, we usually do not explicitly calculate $A^{-1}$ just to solve one system.

Instead, we typically solve

\[A\mathbf{x}=\mathbf b\]

directly using elimination or related methods.

Why?

Because calculating the entire inverse can require substantially more work than solving one system.

For example, if we only need one solution,

\[A\mathbf{x}=\mathbf b,\]

there is usually no reason to calculate every column of $A^{-1}$.

We can simply use elimination.

So there are two different ideas.

Mathematical viewpoint

$$ \mathbf{x}=A^{-1}\mathbf b $$

is extremely useful for understanding the structure of the problem.

Computational viewpoint

We usually solve

$$ A\mathbf{x}=\mathbf b $$

directly.

This distinction becomes important as matrices become large.


25. Why elimination is still important

This explains why we have not abandoned elimination.

Elimination solves

\[A\mathbf{x}=\mathbf b\]

without necessarily forming $A^{-1}$.

In fact, elimination is one of the main computational methods for solving linear systems.

The inverse gives us a conceptual description of the solution:

\[\mathbf{x}=A^{-1}\mathbf b.\]

Elimination gives us an efficient procedure for actually finding $\mathbf{x}$.

The two viewpoints are closely connected.


26. Inverse versus elimination

It is useful to compare them.

Question Inverse Elimination
What is the solution? $A^{-1}\mathbf b$ Back substitution after elimination
What does it emphasize? Structure Computation
Need to form $A^{-1}$? Yes, if used directly No
Useful for many right-hand sides? Yes conceptually Yes, especially after factorization
Connection to transformations? Very strong Strong
Numerical computation? Often not preferred Usually preferred

The important lesson is:

The inverse tells us what the solution is; elimination gives us an efficient way to find it.


27. A deeper connection: $A^{-1}A=I$

Let’s return to the equation

\[A^{-1}A=I.\]

What does this mean geometrically?

Suppose

\[\mathbf{x} \longrightarrow A\mathbf{x}.\]

Then applying $A^{-1}$ gives

\[A\mathbf{x} \longrightarrow A^{-1}A\mathbf{x}.\]

But

\[A^{-1}A=I,\]

so

\[A^{-1}A\mathbf{x} = I\mathbf{x} = \mathbf{x}.\]

Therefore,

$$ \mathbf{x} \xrightarrow{\;A\;} A\mathbf{x} \xrightarrow{\;A^{-1}\;} \mathbf{x}. $$

The transformation is completely reversible.

This is exactly what it means for $A$ to be invertible.


28. The big picture

We can now put together the ideas from the last several lessons.

We began with a system of equations:

\[A\mathbf{x}=\mathbf b.\]

We learned elimination as a method for solving it.

Then we learned matrix multiplication and viewed matrices as transformations.

Now we have introduced the inverse:

\[AA^{-1}=A^{-1}A=I.\]

The inverse reverses the transformation:

\[\mathbf{x} \rightarrow A\mathbf{x} \rightarrow A^{-1}A\mathbf{x} = \mathbf{x}.\]

And therefore:

$$ A\mathbf{x}=\mathbf b \quad\Longrightarrow\quad \mathbf{x}=A^{-1}\mathbf b. $$

But there is an even deeper interpretation.

The equation

\[A\mathbf{x}=\mathbf b\]

asks whether $\mathbf b$ can be constructed from the columns of $A$.

If $A$ is invertible, every $\mathbf b$ has exactly one set of coefficients.

That means the columns of $A$ have a special structure.

We will return to that structure later when we study linear combinations, span, and linear independence.


Key idea

The inverse matrix is the operation that reverses $A$.

For an invertible matrix,

\[AA^{-1}=A^{-1}A=I.\]

Therefore, the system

$$ A\mathbf{x}=\mathbf b $$

has the unique solution

$$ \mathbf{x}=A^{-1}\mathbf b. $$

But the inverse is more than a formula.

It tells us that:

Every output $\mathbf b$ comes from exactly one input $\mathbf x$.

That is the fundamental meaning of an invertible matrix.


Try it yourself

Exercise 1 — Direct use of the inverse

Let

\[A= \begin{bmatrix} 3&1\\ 2&1 \end{bmatrix}.\]

Find $A^{-1}$.

Then use it to solve

$$ A \begin{bmatrix} x\\ y \end{bmatrix} = \begin{bmatrix} 8\\ 5 \end{bmatrix}. $$

Exercise 2 — Verify

For

\[A= \begin{bmatrix} 2&1\\ 1&1 \end{bmatrix},\]

verify that

\[AA^{-1}=I.\]

Also verify that

\[A^{-1}A=I.\]

Exercise 3 — Think in columns

Let

\[A= \begin{bmatrix} 1&2\\ 3&4 \end{bmatrix}.\]

Write the equation

\[A\mathbf{x}=\mathbf b\]

as a linear combination of the columns of $A$.

What do the entries of $\mathbf{x}$ represent?


Exercise 4 — Invertibility

Consider

\[A= \begin{bmatrix} 1&2\\ 2&4 \end{bmatrix}.\]

Does $A^{-1}$ exist?

What does this imply about the possible number of solutions to

\[A\mathbf{x}=\mathbf b?\]

Can you give an example of a $\mathbf b$ for which there is no solution?

Can you give an example for which there are infinitely many solutions?


Exercise 5 — Homogeneous systems

Suppose $A$ is invertible.

Show that

\[A\mathbf{x}=\mathbf0\]

has only the solution

\[\mathbf{x}=\mathbf0.\]

Exercise 6 — Multiple right-hand sides

Suppose

\[AX=B.\]

Show that if $A$ is invertible, then

\[X=A^{-1}B.\]

What does this tell us about solving several systems with the same coefficient matrix?


What is next?

We now know that

\[A^{-1}\]

can solve

\[A\mathbf{x}=\mathbf b.\]

But there is an important computational question:

How can we organize elimination so that solving systems becomes more efficient?

In the earlier lessons, we performed elimination step by step.

Now we will collect those elimination steps into matrices.

This leads to the factorization

$$ A=LU. $$

where:

  • $L$ records the elimination steps,
  • $U$ is the resulting upper-triangular matrix.

This is LU Factorization.

It will give us a powerful connection between elimination, matrix multiplication, and solving $A\mathbf{x}=\mathbf b$.

Finished this lesson?