The discussion centers on understanding the derivation of Lagrange equations in the non-holonomic case, specifically how the final equations relate the linear functionals ##Q_r## and ##\lambda##. A theorem is presented, stating that if the intersection of the kernels of several linear functionals is contained within the kernel of another functional, then a linear combination of these functionals can express the latter. This theorem is further generalized to include linear operators between vector spaces, establishing a relationship between their kernels. The participants seek clarity on applying these concepts to derive the necessary equations in the context of Lagrange mechanics. Understanding these relationships is crucial for solving problems in non-holonomic systems.