In the following, essential kinematic and elastokinematic properties of the wheel suspension are described and it is shown by which hardpoint coordinates these can be specifically influenced. One advantage of the system described is that the properties can essentially be defined independently of one another without conflicting targets. The baseline configuration for the following explanations is a suspension system in which all lateral control arms are of equal length, symmetrical to the wheel center and horizontally aligned (variant 0). The inclination angle of all control arms in plan view is 3° in the baseline configuration.
6.1 Roll compensation
To increase the transmissible lateral forces during cornering, a negative camber during jounce motion is desirable. This can be achieved - as with a conventional multi-link axle - by lowering \({P}_{7}\), \({P}_{9}\) or by raising \({P}_{3}\), \({P}_{5}\), respectively. The behavior of the camber angle with respect to wheel travel is shown in Fig. 7. In addition, the roll center height is determined by the inclination angles of the control arms in the lateral plane.
6.2 Kingpin inclination and camber angle
In the case of a general spatial suspension concept, the steering axis cannot be determined geometrically, but is defined as the instantaneous axis of motion of the wheel carrier during a steering movement. For any point on the steering axis, the velocity vector and angular velocity vector of the wheel carrier are parallel to each other. The inclination of the steering axis in the front view defines the kingpin angle. For the symmetrical baseline configuration, the steering axis runs in vertical direction through the centers of the distances \({P}_{8}\)-\({P}_{10}\), resp. \({P}_{4}\)-\({P}_{6}\) (variant 0: kingpin angle \(\sigma =0\)°). By changing the relative length of the distance \({P}_{8}\)-\({P}_{10}\) (upper link plane) to the distance \({P}_{4}\)-\({P}_{6}\) (lower link plane) in the side view, the instantaneous steering axis and thus the kingpin angle can be specifically influenced. If the distance \({P}_{8}\)-\({{P}_{10}}_{ }\) is smaller than the distance \({P}_{4}\)-\({P}_{6}\) the result is an inwardly inclined kingpin axis (variant 1: \(\sigma >0^\circ\)), in the opposite case an outward inclined spread axis (variant 2: \(\sigma <0^\circ\)).
Kingpin angle and the camber angle as functions of the wheel steering angle are shown in Fig. 8 for the configurations mentioned. A positive kingpin angle causes the wheel to turn into positive camber during steering. This behavior is typical for conventional suspensions, such as a double wishbone axle.
6.3 Scrub radius
In conventional drive trains with sideshafts, unlike the brake torque, the drive torque does not act on the suspension but is transmitted to the body via the engine mount system. For wheel hub motors, both drive and braking torque act on the wheel suspension. For this reason, the scrub radius is the determining lever arm for the reaction moments. Since a wheel hub motor occupies significant installation space inside the rim, the outer knuckle connection points to the control arms are positioned relatively far from the center of the wheel. This represents a conceptual disadvantage of this drive concept. A positive kingpin angle reduces the scrub radius. In addition to the option already mentioned in Chap. 6.2 for defining the kingpin angle, the scrub radius can be reduced further without influencing the kingpin offset (disturbance force lever arm at wheel center height) by moving the upper outer attachment points (\({P}_{8}\), \({P}_{10}\)) inboard and the lower attachment points (\({P}_{4}\), \({P}_{6}\)) outboard. With these measures, the scrub radius can be reduced from 120 mm in the base configuration to about 0 mm in the optimized variant.
6.4 Caster angle and trail
With the general suspension concept any desired caster angle/trail can be implemented. Using a common suspension system with identical components for all four corners is desirable to reduce piece cost and tooling. In order to fulfill this requirement the caster angle has been set to 0° in this specific case. Therefore, aligning torques result exclusively from the tire pneumatic trail. Due to the self-locking steering gear, the aligning torques are not transmitted to the rotor of the steering motor but are supported by the body structure via the gear housing.
6.5 Longitudinal poles
The longitudinal poles can be defined by the vertical position of the trailing arm attachment \({P}_{1}\) on the body structure. The position of the longitudinal pole defines on the one hand the brake/drive pitch angles (anti-dive/anti-lift) and on the other hand the kinematic wheel recession during jounce movements (Fig. 9). Since reduced pitch angles and increased wheel recession on the front axle are conflicting requirements, the longitudinal control arm attachment \({P}_{1}\) is positioned lower on the front axle than on the rear axle.
6.6 Elastokinematics
Due to the stiff connection of the control arms with ball joints and the low caster trail only very small elastokinematic track width and toe angle changes occur under lateral forces. The dynamic driving behavior of the vehicle can in addition be actively influenced by individually controlling the four wheel steering angles (Abe 2015). The targeted toe angle change under longitudinal forces can be adjusted by the lateral position of the trailing arm connection point \({P}_{2}\) on the outer knuckle. If this geometry point is located on the instantaneous steering axis the effect is minimal, if point \({P}_{2}\) is moved inward, toe-out under braking force results. Shifting it outward produces toe-in, which is desirable for braking stability under \(\mu\)-split conditions (Fig. 10). In the longitudinal direction of the vehicle, the trailing arm bearing can be designed softly according to the requirements for rolling comfort and road noise.
6.7 Maximum road wheel steering angle
With the selected suspension geometry, a usable road wheel steering angle range of up to +/-70° can be achieved (Fig. 11). The transfer function between the steering actuator angle and the road wheel angle is linear in the range up to about +/-65°. As the links approach the stretch position, which is defined by a toggle angle of 180° between control arm and knuckle, the steering torques increase progressively. The stretch position, which will create a singularity in the underlying mathematical equations, is reached at a wheel steering angle of about +/- 75°. For many practical vehicle driving maneuvers, the wheel steering angle range of +/-70° that can be realized with the concept is sufficient, since turning the vehicle on the spot is possible and maneuverability is significantly improved compared with a conventional vehicle concept. Which compromises relevant to practice are to be accepted in comparison to a system with a +/- 90° road wheel angle will be addressed in the course of further research.