The discussion revolves around the acceleration of weights connected by springs when the top spring is cut. The initial assumption is that the top weight will have an acceleration equal to gravity (a = g), while the bottom weight will have an acceleration of zero (a = 0). However, it is clarified that the top weight actually experiences an acceleration greater than g due to the force of the stretched spring, while the bottom weight remains stationary. The importance of considering the forces acting on each mass and the instantaneous effects of cutting the spring is emphasized. Overall, the consensus is that the top weight's acceleration exceeds g, contradicting the teacher's initial belief.