First let me say that the axis the car actually roll about is not like a hinge. It is possible to roll the car around a center located within a large area. Therefore, Rc axis position becomes a product of the sum of the car's motion, inertia, mass, geometry, suspension and dampers. Independent (pretty much) from the intersection of the FL. This is what we can say about the actual movement of the sprung mass.
Then the angles of the FL determines how much geometric weight transfer we will get for suspension of each individual wheel. This is quite independent from the previously described movement of roll.
We have now four FL where the force goes straight into the ground without affecting the suspension system. The greater the angle of a single FL are, the more power goes geometrically through the suspension in question.
If we now go back to the place where the FL intersect, but do not call it Rc, so we'll see what significance this has.
If the FL intersecting the middle between the wheels all FL will get the same angle. In a curve the load of the outside wheel FL will produce a lift of the car, while the FL of the inside wheel will press the car down. Since in this case, the intersection of FL is located in the cente of car (the same slope on all fours) so would these forces become equal. But now the outer wheel receives more load and the result is that we get a greater lifting force than lowering. So by altering the FL angle, and thereby altering the spot of FL intersection, during suspension movements we may be able to lessen the lifting (jacking) effect produced by the outside wheel. This is done by creating a geometry that moves the intersection of the FL to the inside wheel during roll.
Of course, there are a number of other things that happen if altering the FL angle, like camber effect during roll and car balance, but this is a to big an issue to bring up here.
Goran