You're right; I should have caught that when you last qualified your statement. This is indeed the case under your definition, though of course not others (e.g., parallel [lines]: non-intersecting in the same plane). That was pure inattention on my part.drachefly wrote:He meant any point which is on CF and not in H must be in J. That's perfectly justifiable. The problem is that CF isn't parallel as I defined it.
Not quite. Geodesics are beasts of metric geometry, with sometimes quite contradictory properties (e.g., it is not the case that every two distinct points determine one and only one geodesic). I suppose we could work with metric geometry only, and simply specify some constrains (e.g., constant curvature) to regain this property, but there is no requirement of actually doing so. More traditional geometrical axioms work well enough, and have the advantage of not requiring a very substantial amount of background theory to be accessible.drachefly wrote:We do have more appropriate terms, such as 'geodesic'
Of course. Alternatively, we can also do nothing.drachefly wrote:we can take G or ¬G as an axiom and see what comes out. Those would be new axioms.
[/quote]drachefly wrote:no, and that's my point.Kuroneko wrote:If G is the Gödel sentence for a given system, is there any reason to prefer G over ¬G?
If that's the case, then I'm afraid I fail to see the relevance of your comment. If we choose among {G,¬G} to make a new axiom and append it to our system, it will simply be another system. This is fully compatible with my interpretation of axiomatic systems.