The discussion focuses on the integration of gravitational force in the context of work done on a particle moving along a semicircular path. The key point is that the work done is calculated using the integral W = ∫F·dr, where the force is mg cos(θ) and the displacement is represented in terms of the angle θ. Participants clarify that work is not the same as external force and emphasize that the integration accounts for the varying angle as the particle moves. The confusion arises around the limits of integration and the assumption of angles, particularly whether the angle is 90 degrees. Ultimately, the work done is expressed as mgR sin(θ), highlighting the importance of correctly interpreting the semicircular motion.