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A First Course in Linear Algebra, 2017a

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4.6. Parametric L<strong>in</strong>es 159<br />

This equation determ<strong>in</strong>es the l<strong>in</strong>e L <strong>in</strong> R 2 . In fact, it determ<strong>in</strong>es a l<strong>in</strong>e L <strong>in</strong> R n . Consider the follow<strong>in</strong>g<br />

def<strong>in</strong>ition.<br />

Def<strong>in</strong>ition 4.19: Vector Equation of a L<strong>in</strong>e<br />

Suppose a l<strong>in</strong>e L <strong>in</strong> R n conta<strong>in</strong>s the two different po<strong>in</strong>ts P and P 0 . Let ⃗p and ⃗p 0 be the position<br />

vectors of these two po<strong>in</strong>ts, respectively. Then, L is the collection of po<strong>in</strong>ts Q which have the<br />

position vector ⃗q given by<br />

⃗q = ⃗p 0 +t (⃗p − ⃗p 0 )<br />

where t ∈ R.<br />

Let ⃗ d = ⃗p − ⃗p 0 .Then ⃗ d is the direction vector for L and the vector equation for L is given by<br />

⃗p = ⃗p 0 +t ⃗ d,t ∈ R<br />

Note that this def<strong>in</strong>ition agrees with the usual notion of a l<strong>in</strong>e <strong>in</strong> two dimensions and so this is consistent<br />

with earlier concepts. Consider now po<strong>in</strong>ts <strong>in</strong> R 3 . If a po<strong>in</strong>t P ∈ R 3 is given by P =(x,y,z), P 0 ∈ R 3 by<br />

P 0 =(x 0 ,y 0 ,z 0 ), then we can write<br />

⎡<br />

where d ⃗ = ⎣<br />

a<br />

b<br />

c<br />

⎤<br />

⎡<br />

⎣<br />

x<br />

y<br />

z<br />

⎤<br />

⎡<br />

⎦ = ⎣<br />

⎤<br />

x 0<br />

y 0<br />

z 0<br />

⎡<br />

⎦ +t ⎣<br />

⎦. This is the vector equation of L written <strong>in</strong> component form .<br />

The follow<strong>in</strong>g theorem claims that such an equation is <strong>in</strong> fact a l<strong>in</strong>e.<br />

Proposition 4.20: <strong>Algebra</strong>ic Description of a Straight L<strong>in</strong>e<br />

Let ⃗a,⃗b ∈ R n with⃗b ≠⃗0. Then⃗x =⃗a +t⃗b, t ∈ R, is a l<strong>in</strong>e.<br />

a<br />

b<br />

c<br />

⎤<br />

⎦<br />

Proof. Let ⃗x 1 ,⃗x 2 ∈ R n . Def<strong>in</strong>e ⃗x 1 = ⃗a and let ⃗x 2 − ⃗x 1 = ⃗ b. S<strong>in</strong>ce ⃗ b ≠⃗0, it follows that ⃗x 2 ≠ ⃗x 1 .Then<br />

⃗a + t⃗b = ⃗x 1 + t (⃗x 2 − ⃗x 1 ). It follows that ⃗x = ⃗a + t⃗b is a l<strong>in</strong>e conta<strong>in</strong><strong>in</strong>g the two different po<strong>in</strong>ts X 1 and X 2<br />

whose position vectors are given by⃗x 1 and⃗x 2 respectively.<br />

♠<br />

We can use the above discussion to f<strong>in</strong>d the equation of a l<strong>in</strong>e when given two dist<strong>in</strong>ct po<strong>in</strong>ts. Consider<br />

the follow<strong>in</strong>g example.<br />

Example 4.21: A L<strong>in</strong>e From Two Po<strong>in</strong>ts<br />

F<strong>in</strong>d a vector equation for the l<strong>in</strong>e through the po<strong>in</strong>ts P 0 =(1,2,0) and P =(2,−4,6).<br />

Solution. We will use the def<strong>in</strong>ition of a l<strong>in</strong>e given above <strong>in</strong> Def<strong>in</strong>ition 4.19 to write this l<strong>in</strong>e <strong>in</strong> the form<br />

⃗q = ⃗p 0 +t (⃗p − ⃗p 0 )

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