The thorny way of truth - Free Energy Community

- 69 -Iis the necessary and sufficient condition so that T-P=const. S, here, isonly a function of coordinates x, y, z . .. , a function whose expressiondoes not explicitly contain time t, while it is T-D that is a homogeneousfunction of the second degree for x', y', z'Consequently, we canimmediately apply the theorem in section 43, which will now read:When motion is to proceed so that fhe theory of the conservation ofkineticenergy(6) T— 6' — Z> = const.is valid, then the following necessary and sufficient condition is to besatisfied:) Ht-d^-s)dttThis condition yields differential equations of form (6) in section 42.There, one only has to write T-D for T, and S for P to get our case above.Section 96The Potential Of Two ElectricWeber's FormParticles.The point is now to apply the theorem in section 95 to the case wherethe moving material points are electric particles and where the forces thatare in motion due to their influence are the forces of mutual attraction andrepulsion.In this problem, D is the potential of the interaction of the electricparticles, to the extent that it is co-dependent on the velocities. D will consistof three parts, namely, the potential Dj of both currents on eachother, the potential D2 of the first current on itself, and the potential D3of the second current on itself. According to (5) in section 94,(1) D, = -\ I'^^^": = -//(t, t;-f-.-, .•; 4. i, t-;).When an electrical conductor is moving and the electrical particlesinside it are simultaneously in motion, then one can break down themotion of every such particle into two parts, namely, the motion which theconductor imparts to it, and its motion relative to the conductor. Then,dx/dt, dy/dt, dz/dt are the components of the absolute velocity of theelectrical particle e that is concentrated in point (x, y, z) and v/ Vj' V3' arcthe components of the absolute velocity of elements of the Condiictdr;