autogyro46
Electrical
- Sep 23, 2009
- 35
First, I'm a newbie here. But, as a teenage lad, I constantly took out Costin and Phipps (first edition! when it was new!)from the library and never quite got over it. As an EE, I tend to look at suspensions in terms of common-mode and differential movements, and my questions may sound at times naive.
My question is the following; it strikes me that one can look at the behavior (OK, I'm a Yank) of anti-dive and squat geometry as geometrically governed motions of the CG about a pitch centre (the UK spelling tends to get better answers) much the same way that unequal length non-parallel control arms govern CG movements about a (notional) roll centre. If that is so, it should be possible to arrange the intersecting planes of the control arms so that they intersect well past the CG at a height at or perhaps above it.
One could then further arrange the two intersections so that the lines from the contact patches to each of them from the tires intersect at a predetermined point in relation to the CG thus forming a pitch centre that could be made stabile over some range of deflection, much like a roll centre
By moving the plane intersections way out, the effects of binding could be reduced, and one one could have a more stable geometry. In addition, one could place this centre very near the CG
Oh, I forgot the question: am I out to lunch?
My question is the following; it strikes me that one can look at the behavior (OK, I'm a Yank) of anti-dive and squat geometry as geometrically governed motions of the CG about a pitch centre (the UK spelling tends to get better answers) much the same way that unequal length non-parallel control arms govern CG movements about a (notional) roll centre. If that is so, it should be possible to arrange the intersecting planes of the control arms so that they intersect well past the CG at a height at or perhaps above it.
One could then further arrange the two intersections so that the lines from the contact patches to each of them from the tires intersect at a predetermined point in relation to the CG thus forming a pitch centre that could be made stabile over some range of deflection, much like a roll centre
By moving the plane intersections way out, the effects of binding could be reduced, and one one could have a more stable geometry. In addition, one could place this centre very near the CG
Oh, I forgot the question: am I out to lunch?