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Appendix C C-83<br />

PROJECT<br />

Parameterizations for Lines and Circles<br />

In the previous project on lines, circles, and ray tracing we derived a vector<br />

equation for a line in the x-y plane. You and your group might want to review<br />

that derivation. In particular, let P 0 be a point in the x-y plane, P 0 be the position<br />

vector with endpoint P 0 , and A be a nonzero vector. We showed that a vector<br />

equation for the line in the x-y plane passing through the point P 0 with<br />

direction vector A is<br />

P P 0 tA for q t q (1)<br />

where P is the position vector of a point P on the line (see Figure A).<br />

y<br />

P<br />

P<br />

0<br />

P<br />

tA<br />

P<br />

P= +tA<br />

0 P 0<br />

A<br />

x<br />

Figure A<br />

Using equation (1) and vector components we can derive two useful scalar<br />

equations for the same line. Let P 0 (x 0 , y 0 ) be the given point on the line,<br />

A 8a, b9 Z 80, 09 be the nonzero direction vector of the line, and P (x, y)<br />

be an arbitrary point on the line. The corresponding position vectors for the<br />

points P 0 and P are P 0 8x 0 , y 0 9 and P 8x, y9, respectively. Substituting into<br />

equation (1) we get<br />

P P 0 tA for q t q<br />

8x, y9 8x 0 , y 0 9 t8a, b9<br />

8x, y9 8x 0 , y 0 9 8ta, tb9<br />

8x, y9 8x 0 ta, y 0 tb9<br />

So<br />

x x<br />

b 0 ta<br />

for q t q<br />

(2)<br />

y y 0 tb<br />

Equations (2) are called parametric equations for this line. If both a and b are<br />

nonzero then we can solve each equation in (2) for t to get<br />

or more simply,<br />

x x 0<br />

a<br />

x x 0<br />

a<br />

t y y 0<br />

b<br />

y y 0<br />

b<br />

(3)

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