Let us, in this particular given arbitrary case scenario, consider both the general wave-tug of the energy of the Hamiltonian Operator, And, the general wave-tug of the correlative energy of the Lagrangian, to act as two different covariant, co-determinable, and co-differentiable, individually taken general genre of phenomenology, of what may be considered here, in the panoply of their multiplicity, to act as two different general types of Metaphorical "forces." Let us now, Metaphorically think, of that general genus of wave-tug, that is here to be eminently representative, to the del of the gauged-action, that is of the general tense of the Hamiltonian Operator, to be physically SYMBOLLIC of that "normal force," of which is here to be inversely related, to the Metaphorical "force," that is here to actually be representative, to the respective wave-tug, of the said Hamiltonian Operator. Now; Let us Metaphorically think, of that general genus of wave-tug, that is here to be eminently representative, to the del of the gauged-action, that is of the general tense of the Lagrangian, to be physically SYMBOLLIC of that "normal force," of which is here to be inversely related, to the Metaphorical "force," that is here to actually be representative, to the respective wave-tug, of the said Lagrangian. I hope that this makes things a little bit clearer! (1989). SAMUEL ROACH.
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