Paper on the conservation of energy principle
In order to calculate the energy density in joules per cubic metre of the ECE2 vacuum, we can proceed as in UFT399. First define the vacuum fluctuations of position as in Lamb shift theory (Eq. (1) of UFT399). This is shivering or zitterbwegung and gives a very accurate description of the Lamb shift in atomic H, as is well known. This leads to the force equation and the ECE2 vacuum electric field strength (E(vac)) in volts per metre (J / C / m). In ECE2 theory this is E(vac) = omega phi, where omega is the vector spin connection and phi the scalar potential. The vacuum energy density is:
En = epsilon sub 0 E(vac) dot E(vac)
in joules per unit volume V, i.e. in joules per cubic metre. Given a volume of radiation V the energy density can be calculated as in the UFT papers reviewed in UFT400. UFT399 describes how the experimentally observed electromagnetic potential is defined:
phi (r + delta r) = phi(r) + phi (vac)
A Taylor series, isotropic averaging and an Euler Bernoulli method is then used to show that at resonance, the energy from the ECE2 vacuum becomes infinite as in any Euler Bernoulli resonance. Many other UFT papers deal with this topic. The total energy density is the vacuum energy density plus the material energy density. The total energy density is conserved in a conservative system. So if infinite energy is defined as an Euler Bernoulli resonance, it can exist with conservation of total energy density. This was first proposed in the early spin connection resonance papers, which were developed in the Eckardt / Lindstrom papers, UFT292 to UFT299. By now all these papers are classics. having been read tens of thousands to hundreds of thousands of times or more in toto.