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Solution<br />

a. Since the direction vectors are parallel—that is, 211, 2, 52 12, 4, 102—<br />

this means that the two lines are parallel. To show that the equations are<br />

equivalent, we must show that a point on one of the lines is also on the other<br />

line. This is based on the logic that, if the lines are parallel and they share a<br />

common point, then the two equations must represent the same line. To check<br />

whether 14, 10, 212 is also on L 1 substitute into its vector equation.<br />

14, 10, 212 11, 0, 42 s11, 2, 52<br />

Using the x component, we find 4 1 s, or s 5. Substituting s 5<br />

into the above equation, 11, 0, 42 511, 2, 52 14, 10, 212. This<br />

verifies that the point 14, 10, 212 is also on L 1 .<br />

Since the lines have the same direction, and a point on one line is also on the<br />

second line, the two given equations represent the same line.<br />

b. The first check is to compare the direction vectors of the two lines. Since<br />

2Q 1 the lines must be parallel. As in part a,<br />

2 , 1 2 , 1R 11, 1, 22,<br />

13, 10, 122 must be a point on L 3 for the equations to be equivalent. Therefore,<br />

13, 10, 122 11, 6, 12 l11, 1, 22 must give a consistent value of l for<br />

each component. If we solve, this gives an inconsistent result since l 4 for<br />

the x and y components, and 12 1 2l, or l 11 for the z component. This<br />

2<br />

verifies that the two equations are not equations for the same line.<br />

Symmetric Equations of Lines in R 3<br />

We introduce a new form for a line in R 3 , called its symmetric equation. The<br />

symmetric equation of a line is derived from using its parametric equations and<br />

solving for the parameter in each component, as shown below<br />

x x 0 ta 4 t x x 0<br />

, a 0<br />

y y 0 tb 4 t y a<br />

y 0<br />

, b 0<br />

z z 0 tc 4 t z b<br />

z 0<br />

, c 0<br />

c<br />

x x<br />

Combining these statements gives 0<br />

y y 0<br />

z z 0, a, b, c 0.<br />

a b c<br />

These equations are called the symmetric equations of a line in R 3 .<br />

R 3<br />

Symmetric Equations of a Line in<br />

x x 0<br />

y y 0<br />

z z 0<br />

, a 0, b 0, c 0<br />

a b c<br />

where 1x 0 , y 0 , z 0 2 is the vector from the origin to a point on the line, and 1a, b, c2<br />

is a direction vector of the line.<br />

NEL<br />

CHAPTER 8 447

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