Page 101 - Dynamic Vision for Perception and Control of Motion
P. 101

3.4 Behavioral Capabilities for Locomotion      85


            magnitude A, but with opposite signs and one with zero output in between. The two
            characteristic time durations are T SR for ± A and IJ for the central zero-output.
              A·T SR yields the maximum steering angle Ȝ f (fixing the turn radius), with which
            a circular arc of duration IJ is driven (see Table 3.2); the total maneuver time T DC
            for a change in heading direction then is 2·T SR + W. The total angular change in
            heading is the integral of curvature over the arc length and depends on the axle dis-
            tance of the car (see Figure 3.10  for the idealized case  of infinitely stiff tires).
            Proper application of Equation 3.12 yields the (idealized) numerical values.
              A special case is the 90° heading change for turning off onto a crossroad. If the
            vehicle chosen drives at 27 km/h (V § 7.5 m/s, column 2 in Table 3.2) then T SR =
            T 2 is § 5.6 seconds, and the limit of 2 m/s² for lateral acceleration is reached with
                                                                             í1
            ǻȜ f = 6.4° and ǻȤ f § 42.6°. The radius of curvature R is 28.1 m (C =  0.0356 m ,
            Equation 3.9); this yields a turn rate C·V (Equation 3.10) of 15.3°/s. Steering back
            to straight-ahead driving on the crossroad with the mirrored maneuver for the steer-
            ing angle leaves almost no  room for a circular arc  with  radius  R f [W = (90  –
            2·42.6)/15.3 § 0.3 s]; the total turn–off–duration then is § 11.2 s and the total dis-
            tance traveled is about 84 m.
              For tight turns on narrow roads, either the allowed lateral acceleration has to be
            increased, or lower speed has to be selected. A minimal turn radius of 6 m driven at
            V = 7 m/s yields an ideal turn rate V/R of about 67°/s and a (nominal) lateral accel-
            eration V²/R of about 0.82 g (~ 8 m/s²); this is realizable only on dry ground with
            good homogeneous friction coefficients at all wheels. Slight variations will lead to
            slipping motion and uncontrollable behavior. For the selected convenient limit of
            maximum lateral acceleration of 2 m/s² with the minimal turn radius possible (6
            m), a speed of V § 3.5 m/s (§ 12.5 km/h or 7.9 mph)should be chosen. These ef-
            fects have to be kept in mind when planning turns.
              The type of control according to Figure 3.13 is often used at higher speeds with
            smaller values for A and T SR (W close to 0) for heading corrections after some per-
            turbation. Switching the sequence of the sign of A results in a heading change in
            the opposite direction.
            Lane change maneuvers: Combining two extended pulses of opposite sign with
            proper control of magnitude and duration results in a “lane change maneuver” dis-
            cussed above and displayed in Figure 3.16.
              The numerical values and the temporal extensions of these segments for a lateral
            translation of one lane width depend on the speed driven and the maximum lateral
            acceleration level acceptable. The behavioral capability of lane changing may thus
            be represented symbolically by a name and the parameters specifying this control
            output (just a few numbers, as given in the legend of the figure). Together with the
            initial and final boundary values of the state variables and maybe some extreme
            values in between, this is sufficient for the (abstract) planning and decision level.
            Only the processor directly controlling the actuator needs to know the details of
            how the maneuver is realized. For very high speeds, maneuver times for the pulses
            become very small [see T2–curve (solid) in Figure 3.11]. In these cases, tire stiff-
            ness effects  play an important role; there  will be additional dynamic  responses
            which interact with vehicle dynamics. This will be discussed in Section 3.4.5.2.
   96   97   98   99   100   101   102   103   104   105   106