Dipoles—continued

A dipole and its scalar potential thus represent a true negative resistor system of the most fundamental kind. The dipole continually receives EM energy in unusable form (reactive power, which cannot perform real work), converts it to usable form (real power, which can perform real work), and outputs it as usable, real EM energy flow (real power) in 3-space. 

We must pay for the initial energy input to the generator to establish the source dipole. Once formed, the dipole continuously extracts and pours out enormous observable EM energy flow from the vacuum—if we do not foolishly... 

A broken 3-space symmetry exists of a magnetic dipole [18] of a permanent magnet, well known in particle physics since 1957 but inexplicably not yet added into classical electrodynamics theory, wherein the broken symmetry of the magnetic dipole rigorously requires that the dipole continually absorb magnetic energy from the active vacuum in unusable form, and that the... 

The emerging overunity electrical power systems—including self-powered systems freely taking all their energy from the local vacuum—will produce a total revolution in transportation, electrical power systems, backup power systems, and so on [68,69]. In the process, the electrical power is obtained freely and cleanly from the vacuum, from permanent-magnet dipoles continuously replenished from the active vacuum via the giant negentropy process. 

Induced dipoles continually arise and disappear as a result of electron movement, but the force between neighbouring dipoles is always attractive. Thus, although the average dipole on each molecule measured over time is zero, the resultant forces between molecules at any instant are not zero. 

The relationship between the piezoelectricity d and the orientation of dipoles 0 (b) are given in Figure 4, for the films polarized at a high temperature with various E, and for the films heat-treated at various temperatures. iSe polarization at 140°C seems to induce the piezoelectricity with less orientation at low E, the piezoelectricity becomes parallel to the orientation of dipoles with medium E, and only the orientation of dipoles continues to increasi as E increases further. When the films polarized at 140 with 670kv/cm were heat-treated at various temperatures, the orientation of dipoles decreases more quickly than the piezoele-... 

In Ih e quail tiiin mechanical description of dipole moment, the charge is a continuous distribution that is a I linction of r. and the dipole moment man average over the wave function of the dipole moment operator, p ... 

TABLE 5.17 Dielectric Constant (Permittivity) and Dipole Moment of Various Organic Substances Continued)... 

TABLE 5.18 Viscosity, Dielectric Constant, Dipole Moment, and Surface Tension of Selected Inorganic Substances Continued)... 

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