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Linear Algebra

  1. Vectors
    1. Scalars
    2. Vectors vs Sets
    3. Addition and Subtraction
    4. Scalar Multiplication
    5. Zero Vectors
    6. Linear Combinations
    7. Real Dot Product
    8. Length of a Vector
    9. Orthogonal Vectors
    10. Parallel Vectors
    11. Angle Between Vectors
    12. Unit Vectors
  2. Matrices
    1. Notation
    2. Indexing
    3. Submatrices
    4. Matrix-by-Vector Product
    5. Addition and Subtraction
    6. Scalar Multiplication
    7. Transpose
    8. Symmetries
    9. Matrix Multiplication
    10. Identity Matrix
    11. Non-Negative Integer Powers
    12. Reverse Order Law of Transposition
  3. Linear Systems
    1. Inverse Matrices
    2. Singular Matrices
    3. Linear Dependence
    4. Solutions
  4. Planes
    1. Vector Cross Product
  5. Gaussian Elimination
Linear Algebra ›Linear Systems ›Inverse Matrices

Inverse Matrix of a Linear System

From the introductory lesson on linear systems, we have learned that a linear system is of the form

Ax⃗=b⃗.A \vec{x} = \vec{b}.Ax=b.

Such a system does not have to have only one solution. In fact, it can have infinitely many solutions, but also no solution at all. It could also have exactly one.

For now we concern ourselves with the case in which a linear system has exactly one solution. One way this can happen, for example, is when the system has a non-singular (or invertible) matrix.

This terminology might seem counter-intuitive, since a non-singular matrix is found in a linear system which has exactly one solution. Keep this in mind to avoid confusing the terminology.

A matrix in a linear system that is non-singular is invertible. To understand what this means, I will use an example from scalar algebra, which is more familiar than matrix algebra.

Parallel Example From Scalar Algebra

Take the equation

ax=b,ax = b,ax=b,

where aaa, xxx, and bbb are all scalars. Say that we want to find the unknown xxx and are given values for aaa and bbb. To solve the equation, we could divide both sides by aaa:

x=ba.x = \dfrac{b}{a}.x=ab​.

What we did was divide by aaa, which is the same as multiplying by 1a\frac{1}{a}a1​, which is the same as multiplying by a−1a^{-1}a−1.

a−1a^{-1}a−1 is said to be the multiplicative inverse of aaa, because

aa−1=1.a a^{-1} = 1.aa−1=1.

What we did was basically

ax=ba−1ax=a−1b1x=1abx=ba\begin{align*} ax &= b \\ a^{-1}ax &= a^{-1} b \\ 1x &= \dfrac{1}{a} b \\[0.5em] x &= \dfrac{b}{a} \end{align*}axa−1ax1xx​=b=a−1b=a1​b=ab​​

In the context of scalars, 111 is the multiplicative identity, which is the equivalent of an identity matrix in linear algebra.

How This Applies to Matrices

The same can be said about matrices. A matrix AAA is said to be invertible when there exists some matrix A−1A^{-1}A−1 such that

AA−1=A−1A=I,A A^{-1} = A^{-1} A = I,AA−1=A−1A=I,

where III is the identity matrix of the appropriate size.

Not all matrices are invertible. For some matrices AAA it is possible to find A−1A^{-1}A−1, for others, this is not the case. Whether a matrix AAA in a linear system is invertible or not tells us a lot about the potential solutions to the system. When the matrix AAA is invertible, we know that there will be exactly one solution which is given by

x⃗=A−1b⃗.\vec{x} = A^{-1} \vec{b}.x=A−1b.

I can already tell you that only square matrices are invertible, whereas rectangular matrices are never invertible in the usual sense.

This is similar to what we saw in the example from scalar algebra that I used above. You just multiply both sides of the equation Ax⃗=b⃗A \vec{x} = \vec{b}Ax=b by A−1A^{-1}A−1. On the left side, you are left with Ix⃗I \vec{x}Ix which is the same as x⃗\vec{x}x. On the right side, you get A−1b⃗A^{-1} \vec{b}A−1b.

Next Steps

We now covered the case for which a linear system has exactly one solution, which is what we would expect and what is most intuitive. But naturally, since I said that in certain cases, A−1A^{-1}A−1 does not exist, what happens in those cases? This is the next question we must ask which I will cover in subsequent lessons.

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Linear Systems - Introduction
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Singular Matrix of a Linear System
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