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212                                    Autonomous Mobile Robots

                                and the σ process



                                                        ξ 1 = x
                                                             1   3
                                                        ξ 2 =  sec θ tan φ
                                                             l
                                                             tan θ
                                                        ξ 3 =
                                                              x
                                                             y
                                                        ξ 4 =
                                                             x 2


                                we obtain a system described by equations of the form



                                                         ˙ ξ 1 = u 1
                                                         ˙ ξ 2 = u 2
                                                             ξ 2 − ξ 3
                                                         ˙ ξ 3 =   u 1
                                                               ξ 1
                                                             ξ 3 − 2ξ 4
                                                         ˙ ξ 4 =    u 1
                                                                ξ 1


                                thatis, byequationsoftheform(5.25)withn = 4. Thus, usingProposition(5.2),
                                we design the state feedback control law



                                                    u 1          −kξ 1
                                                        =
                                                    u 2    p 2 ξ 2 + p 3 ξ 3 + p 4 ξ 4

                                In the original coordinates the feedback law is described by


                                            x
                                    v 1 =−k
                                           cos θ
                                         3   2            x
                                    v 2 = k sin φ tan θ sec θ
                                         l              cos θ

                                                          1                 tan θ        y
                                             2     3          3
                                        + l cos φ cos θ p 2  sec θ tan φ + p 3    + p 4  2
                                                          l                  x         x


                                 © 2006 by Taylor & Francis Group, LLC



                                FRANKL: “dk6033_c005” — 2006/3/31 — 16:42 — page 212 — #26
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