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Fundamentals of Matrix Algebra, 2011a

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Chapter 2<br />

<strong>Matrix</strong> Arithmec<br />

In previous secons we were fine stang that the result as<br />

x 1 = 2, x 2 = 0, x 3 = 1,<br />

but we were asked to find ⃗x; therefore, we state the soluon as<br />

⎡ ⎤<br />

.<br />

⃗x =<br />

⎣ 2 0 ⎦ .<br />

1<br />

This probably seems all well and good. While asking one to solve the equaon<br />

A⃗x = ⃗b for ⃗x seems like a new problem, in reality it is just asking that we solve a<br />

system <strong>of</strong> linear equaons. Our variables x 1 , etc., appear not individually but as the<br />

entries <strong>of</strong> our vector ⃗x. We are simply wring an old problem in a new way.<br />

In line with this new way <strong>of</strong> wring the problem, we have a new way <strong>of</strong> wring<br />

the soluon. Instead <strong>of</strong> lisng, individually, the values <strong>of</strong> the unknowns, we simply list<br />

them as the elements <strong>of</strong> our vector ⃗x.<br />

These are important ideas, so we state the basic principle once more: solving the<br />

equaon A⃗x = ⃗b for⃗x is the same thing as solving a linear system <strong>of</strong> equaons. Equivalently,<br />

any system <strong>of</strong> linear equaons can be wrien in the form A⃗x = ⃗b for some<br />

matrix A and vector ⃗b.<br />

Since these ideas are equivalent, we’ll refer to A⃗x = ⃗b both as a matrix–vector<br />

equaon and as a system <strong>of</strong> linear equaons: they are the same thing.<br />

We’ve seen two examples illustrang this idea so far, and in both cases the linear<br />

system had exactly one soluon. We know from Theorem 1 that any linear system has<br />

either one soluon, infinite soluons, or no soluon. So how does our new method <strong>of</strong><br />

wring a soluon work with infinite soluons and no soluons?<br />

Certainly, if A⃗x = ⃗b has no soluon, we simply say that the linear system has no<br />

soluon. There isn’t anything special to write. So the only other opon to consider is<br />

the case where we have infinite soluons. We’ll learn how to handle these situaons<br />

through examples.<br />

. Example 44 .Solve the linear system A⃗x = ⃗0 for ⃗x and write the soluon in<br />

vector form, where [ ]<br />

[ ]<br />

1 2<br />

0<br />

A = and ⃗0 = .<br />

2 4<br />

0<br />

S<br />

(Note: we didn’t really need to specify that<br />

[ ] 0 ⃗0 = ,<br />

0<br />

but we did just to eliminate any uncertainty.)<br />

To solve this system, put the augmented matrix into reduced row echelon form,<br />

which we do below.<br />

[ 1 2<br />

] 0<br />

2 4 0<br />

−→<br />

rref<br />

[ 1 2<br />

] 0<br />

0 0 0<br />

82

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