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Linear Algebra

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Section III. Reduced Echelon Form 51<br />

(a) 2x + y − z =1<br />

4x − y =3<br />

(b) x − z =1<br />

y +2z − w =3<br />

x +2y +3z − w =7<br />

(d) a +2b +3c + d − e =1<br />

3a − b + c + d + e =3<br />

1.10 Give two distinct echelon form versions of this matrix.<br />

� �<br />

2 1 1 3<br />

6 4 1 2<br />

1 5 1 5<br />

(c) x − y + z =0<br />

y + w =0<br />

3x − 2y +3z + w =0<br />

−y − w =0<br />

� 1.11 List the reduced echelon forms possible for each size.<br />

(a) 2×2 (b) 2×3 (c) 3×2 (d) 3×3<br />

� 1.12 What results from applying Gauss-Jordan reduction to a nonsingular matrix?<br />

1.13 The proof of Lemma 1.4 contains a reference to the i �= j condition on the<br />

row pivoting operation.<br />

(a) The definition of row operations has an i �= j condition on the swap operation<br />

ρi ↔ ρj. Show that in A ρi↔ρj −→ ρi↔ρj −→ A this condition is not needed.<br />

(b) Write down a 2×2 matrix with nonzero entries, and show that the −1·ρ1 +ρ1<br />

operation is not reversed by 1 · ρ1 + ρ1.<br />

(c) Expand the proof of that lemma to make explicit exactly where the i �= j<br />

condition on pivoting is used.<br />

1.III.2 Row Equivalence<br />

We will close this section and this chapter by proving that every matrix is<br />

row equivalent to one and only one reduced echelon form matrix. The ideas<br />

that appear here will reappear, and be further developed, in the next chapter.<br />

The underlying theme here is that one way to understand a mathematical<br />

situation is by being able to classify the cases that can happen. We have met this<br />

theme several times already. We have classified solution sets of linear systems<br />

into the no-elements, one-element, and infinitely-many elements cases. We have<br />

also classified linear systems with the same number of equations as unknowns<br />

into the nonsingular and singular cases. We adopted these classifications because<br />

they give us a way to understand the situations that we were investigating. Here,<br />

where we are investigating row equivalence, we know that the set of all matrices<br />

breaks into the row equivalence classes. When we finish the proof here, we will<br />

have a way to understand each of those classes — its matrices can be thought<br />

of as derived by row operations from the unique reduced echelon form matrix<br />

in that class.<br />

To understand how row operations act to transform one matrix into another,<br />

we consider the effect that they have on the parts of a matrix. The crucial<br />

observation is that row operations combine the rows linearly.

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