The thorny way of truth - Free Energy Community

-65^2EIGHTH DIVISIONThe Fundamental LawOf Electric InteractionSection 94The Potential Of The InteractionOf Two CurrentsThe theorem in section 93 can be transferred immediately to twononlinear closed currents. One only has to assume that the specificcurrent intensities will undergo only infinitely small changes in timeclement dt at every place in the first as well as in the second conductor andto advance the hypothesis that the total work that originates in the interactionof both galvanic currents in time element dt is the completedifferential of a function which possesses the characteristic properties of apotential (in the broader sense).In order to comprehend this, one only needs to consider that one canconceive of one as well as the other nonlinear current as each being asystem of linear currents.The train of thought in section 93 will be repeated here. In equations(5), (6), and (7) in section 89, we found these expressions for function PP = -^ I dS {u\ I, -f- «; t, -\- h; {,)(1)*dS.dS'(^ +sr i; h h + h h)'We will now also want to consider this function P for the case where thespecific current intensity can be independent of time. What matters thenare the changes that function P undergoes in time element dtunder thevarious permissible assumptions. 5,P will denote the change that occurswhen the specific current intensities iri both conductors are regarded asindependent of t, 5„P will denote the change that originates when one271