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Chapter 4: Geometry

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5. Re ec tion in a line with equation Ü · Ý · ¼:<br />

<br />

´Ü ݵ <br />

½ <br />

¾<br />

¾ ¾<br />

´Ü<br />

¾ · ¾ ¾ ¾ ¾ ݵ ´¾ ¾µ<br />

<br />

(4.2.5)<br />

6. Re ec tion in a line going through ´Ü ¼ Ý ¼ µ and making an angle « with the<br />

Ü-axis:<br />

´Ü ݵ ´Ü ¼ Ý ¼ µ·<br />

<br />

Ó× ¾« ×Ò ¾«<br />

´Ü Ü<br />

×Ò ¾« Ó× ¾«<br />

¼ Ý Ý ¼ µ (4.2.6)<br />

7. Glide-re ection in a line Ä with displacement : Apply rst a re ection in Ä,<br />

then a translation by a vector of length in the direction of Ä, that is, by the<br />

vector<br />

½ ´¦<br />

¾ §µ (4.2.7)<br />

· ¾ if Ä has equation Ü · Ý · ¼.<br />

4.2.2 FORMULAE FOR SYMMETRIES: HOMOGENEOUS<br />

COORDINATES<br />

All isometries of the plane can be expressed in homogeneous coordinates in terms<br />

of multiplication by a matrix. This fact is useful in implementing these transformations<br />

on a computer. It also means that the successive application of transformations<br />

reduces to matrix multiplication. The corresponding matrices are as follows:<br />

1. Translation by ´Ü ¼ Ý ¼ µ:<br />

Ì´Ü¼Ý ¼µ<br />

<br />

¾<br />

¿<br />

½ ¼ Ü ¼<br />

¼ ½ Ý ¼<br />

(4.2.8)<br />

¼ ¼ ½<br />

2. Rotation through « around the origin:<br />

Ê « <br />

¾<br />

<br />

¿<br />

Ó× « ×Ò « ¼<br />

×Ò « Ó× « ¼ (4.2.9)<br />

¼ ¼ ½<br />

3. Re ec tion in a line going through the origin and making an angle « with the<br />

Ü-axis:<br />

¾<br />

¿<br />

Ó× ¾« ×Ò ¾« ¼<br />

Å « ×Ò ¾« Ó× ¾« ¼ (4.2.10)<br />

¼ ¼ ½<br />

From this one can deduce all other transformations.<br />

© 2003 by CRC Press LLC

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