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Linear Algebra

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34 Chapter 1. <strong>Linear</strong> Systems<br />

position, as a column. For instance, the ‘one over and two up’ vectors above are<br />

denoted in this way.<br />

� �<br />

1<br />

2<br />

More generally, the plane vector starting at (a1,a2) and stretching to (b1,b2) is<br />

denoted<br />

� �<br />

b1 − a1<br />

b2 − a2<br />

since the prior paragraph shows that when the vector starts at the origin, it<br />

ends at this location.<br />

We often just say “the point<br />

� �<br />

1<br />

”<br />

2<br />

rather than “the endpoint of the canonical position of” that vector. That is, we<br />

shall find it convienent to blur the distinction between a point in space and the<br />

vector that, if it starts at the origin, ends at that point. Thus, we will refer to<br />

both of these as Rn .<br />

{(x1,x2) � � �<br />

x1 ��<br />

� x1,x2 ∈ R} { x1,x2 ∈ R}<br />

In the prior section we defined vectors and vector operations with an algebraic<br />

motivation;<br />

� � � � � � � � � �<br />

v1 rv1 v1 w1 v1 + w1<br />

r · =<br />

+ =<br />

v2 rv2 v2 w2 v2 + w2<br />

we can now interpret those operations geometrically. For instance, if �v represents<br />

a displacement then 3�v represents a displacement in the same direction<br />

but three times as far, and −1�v represents a displacement of the same distance<br />

as �v but in the opposite direction.<br />

−�v<br />

�v<br />

And, where �v and �w represent displacements, �v + �w represents those displacements<br />

combined.<br />

�v + �w<br />

�v<br />

3�v<br />

�w<br />

x2

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