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A First Course in Linear Algebra, 2017a

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4.1. Vectors <strong>in</strong> R n 145<br />

Now, imag<strong>in</strong>e tak<strong>in</strong>g a vector <strong>in</strong> R n and mov<strong>in</strong>g it around, always keep<strong>in</strong>g it po<strong>in</strong>t<strong>in</strong>g <strong>in</strong> the same<br />

direction as shown <strong>in</strong> the follow<strong>in</strong>g picture.<br />

A<br />

B<br />

−→<br />

0P = [ p 1 p 2 p 3<br />

] T<br />

After mov<strong>in</strong>g it around, it is regarded as the same vector. Each vector, −→ 0P and −→ AB has the same length<br />

(or magnitude) and direction. Therefore, they are equal.<br />

Consider now the general def<strong>in</strong>ition for a vector <strong>in</strong> R n .<br />

Def<strong>in</strong>ition 4.2: Vectors <strong>in</strong> R n<br />

Let R n = { (x 1 ,···,x n ) : x j ∈ R for j = 1,···,n } . Then,<br />

⃗x =<br />

⎡<br />

⎢<br />

⎣<br />

⎤<br />

x 1<br />

.. ⎥<br />

. ⎦<br />

x n<br />

is called a vector. Vectors have both size (magnitude) and direction. The numbers x j are called the<br />

components of⃗x.<br />

Us<strong>in</strong>g this notation, we may use ⃗p to denote the position vector of po<strong>in</strong>t P. Notice that <strong>in</strong> this context,<br />

⃗p = −→ 0P. These notations may be used <strong>in</strong>terchangeably.<br />

You can th<strong>in</strong>k of the components of a vector as directions for obta<strong>in</strong><strong>in</strong>g the vector. Consider n = 3.<br />

Draw a vector with its tail at the po<strong>in</strong>t (0,0,0) and its tip at the po<strong>in</strong>t (a,b,c). This vector it is obta<strong>in</strong>ed<br />

by start<strong>in</strong>g at (0,0,0), mov<strong>in</strong>g parallel to the x axis to (a,0,0) and then from here, mov<strong>in</strong>g parallel to the<br />

y axis to (a,b,0) and f<strong>in</strong>ally parallel to the z axis to (a,b,c). Observe that the same vector would result if<br />

you began at the po<strong>in</strong>t (d,e, f ), moved parallel to the x axis to (d + a,e, f ), thenparalleltothey axis to<br />

(d + a,e + b, f ), and f<strong>in</strong>ally parallel to the z axis to (d + a,e + b, f + c). Here, the vector would have its<br />

tail sitt<strong>in</strong>g at the po<strong>in</strong>t determ<strong>in</strong>ed by A =(d,e, f ) and its po<strong>in</strong>t at B =(d + a,e + b, f + c). Itisthesame<br />

vector because it will po<strong>in</strong>t <strong>in</strong> the same direction and have the same length. It is like you took an actual<br />

arrow, and moved it from one location to another keep<strong>in</strong>g it po<strong>in</strong>t<strong>in</strong>g the same direction.<br />

We conclude this section with a brief discussion regard<strong>in</strong>g notation. In previous sections, we have<br />

written vectors as columns, or n × 1 matrices. For convenience <strong>in</strong> this chapter we may write vectors as the<br />

transpose of row vectors, or 1 × n matrices. These are of course equivalent and we may move between<br />

both notations. Therefore, recognize that<br />

[ ]<br />

2<br />

= [ 2 3 ] T<br />

3<br />

Notice that two vectors ⃗u =[u 1 ···u n ] T and ⃗v =[v 1 ···v n ] T are equal if and only if all correspond<strong>in</strong>g

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