Diagram 1 you are missing the resultant force at the swingarm pivot bolt. That force would be pulling down and away from the frame at the pivot bolt.
The force acting at the fork wouldn't be vertical at that point. The force is at the wheel which is offset from the support so you would have an additional moment at that point in the frame. This moment could be shown as two counteracting forces one at the top of the stem and one at the bottom. The bottom of the stem is pulling in and the top of the stem is pushing out.
Diagram 2 is interesting but I don't agree that changing the axis of "A" would be beneficial. That brace is additionally resisting the moment developed from the wheels distance from the frame. I would imagine that that the load in the front would increase at higher speed cornering which would could torque the front stem. Having "A" braced at its angle would resist that.
Developing a static model wouldn't be hard but who actually knows the forces developed from riding in a turn? Looking at the frame like this really helps to explain why the monoshock is the modern rear suspension.
Reading the rest of your comments, there is a common theme. You seem to think that the X-Z plane bending moment is significant if not more important that the torsion effects I described.
Given the relative motion of wheel axis (axles) during aggressive riding I don't see how this bending moment, within reason as being a major concern to handling. It is a concern for JED, if he cuts off is back triangle that is the primary supporting structure for the bike and rider weight but that is the exception.
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