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A First Course in Linear Algebra, 2017a

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158 R n ⃗u 2⃗v<br />

⃗u + 2⃗v<br />

⃗u − 1 2 ⃗v<br />

⃗u<br />

− 1 2 ⃗v<br />

♠<br />

4.6 Parametric L<strong>in</strong>es<br />

Outcomes<br />

A. F<strong>in</strong>d the vector and parametric equations of a l<strong>in</strong>e.<br />

We can use the concept of vectors and po<strong>in</strong>ts to f<strong>in</strong>d equations for arbitrary l<strong>in</strong>es <strong>in</strong> R n , although <strong>in</strong><br />

this section the focus will be on l<strong>in</strong>es <strong>in</strong> R 3 .<br />

To beg<strong>in</strong>, consider the case n = 1sowehaveR 1 = R. There is only one l<strong>in</strong>e here which is the familiar<br />

number l<strong>in</strong>e, that is R itself. Therefore it is not necessary to explore the case of n = 1further.<br />

Now consider the case where n = 2, <strong>in</strong> other words R 2 . Let P and P 0 be two different po<strong>in</strong>ts <strong>in</strong> R 2<br />

which are conta<strong>in</strong>ed <strong>in</strong> a l<strong>in</strong>e L. Let⃗p and ⃗p 0 be the position vectors for the po<strong>in</strong>ts P and P 0 respectively.<br />

Suppose that Q is an arbitrary po<strong>in</strong>t on L. Consider the follow<strong>in</strong>g diagram.<br />

Q<br />

P<br />

P 0<br />

Our goal is to be able to def<strong>in</strong>e Q <strong>in</strong> terms of P and P 0 . Consider the vector −→ P 0 P = ⃗p − ⃗p 0 which has its<br />

tail at P 0 and po<strong>in</strong>t at P. Ifweadd⃗p − ⃗p 0 to the position vector ⃗p 0 for P 0 , the sum would be a vector with<br />

its po<strong>in</strong>t at P. Inotherwords,<br />

⃗p = ⃗p 0 +(⃗p − ⃗p 0 )<br />

Now suppose we were to add t(⃗p − ⃗p 0 ) to ⃗p where t is some scalar. You can see that by do<strong>in</strong>g so, we<br />

could f<strong>in</strong>d a vector with its po<strong>in</strong>t at Q. In other words, we can f<strong>in</strong>d t such that<br />

⃗q = ⃗p 0 +t (⃗p − ⃗p 0 )

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