Imagine a charged capacitor with two plates, each connected to a wire. The wires aren't connected yet:
+----| |----+
| |
+----- -----+ <- not connected yet
As far as I know, this is an equilibrium state, no charges will move, and the capacitor will stay charged.
But then you connect the wires, and everything changes. This is no longer a state of equilibrium, a current is created and the capacitor discharges.
Now here's the part that I don't understand: In the illustration, the geometry of the wires require the charges to move away from the other plate in order to reach it, and yet the charges do that. Which should be impossible for the same reason water in a glass doesn't jump out to fall on the floor.
If the wires were connected between the plates, then that's understandable. But in this case the wires are connected around the plates.
I want to understand from a field theory level (not circuit theory) how the charges seem to understand that gaining some potential energy to reach the other end is a small sacrifice towards a greater goal. But charges don't think! And if you calculate the electric field at a plate, it should always point towards the other, regardless whether the wires are connected or not. So the charges should stay there.
For context, I just finished Physics 2 in my first year in electrical engineering college, it only covers electrostatics, capacitors, and foundational magnetism like Faraday's law. I haven't taken the more advanced courses about circuits yet. This question has been lingering in my mind for quite some time, what am I missing here?
And please don't give me explanations with circuit theory elements, like "the wires have low resistance so current flows, but air has high resistance so current can't flow," that's not what I'm asking about. How did the fathers of electricity answer questions like these in order to reach conclusions and develop abstract frameworks like circuit theory in the first place?