The discussion centers on the relationship between generalized forces and Hamilton's equations of motion. It asserts that when the generalized force F is not zero, the equation dH/dq = -pdot remains valid, as generalized forces are inherently included in the Lagrangian formulation. The Lagrangian, defined as L = T - V, incorporates the effects of forces through its derivatives, eliminating the need to explicitly include F in Hamilton's equations. The derivation shows that dL/dq leads to the momentum p, confirming that pdot = -dH/dq is consistently true. Overall, the analysis emphasizes that the force is fundamentally embedded within the Lagrangian framework.