## Trajectory of Photons

OK thanks, the trajectory of the photon is well known to be changed in a gravitational field, and that has been explained in several previous UFT papers. If gravitaton and electromagnetism interact, your idea could well work, the traejctory of the photon would be changed by a laser. Such experiments with two powerful interactig lasers have already been carried out. See the Omnia Opera and later papers for example. If one laser beam affects another your idea is right.

To: emyrone@aol.com, mail@horst-eckardt.de

Sent: 26/06/2017 06:04:56 GMT Daylight Time

Subj: Re: Discussion of 380(2): Combined Gravitation and Electromagnetism, Biefeld BrownMy point was not about photons being changed in mass but in trajectory.

For example a laser maybe useful in an experiment to measure electrogravitic effects due to light bending.Sean

On June 23, 2017 at 1:37:34 AM, emyrone@aol.com (emyrone) wrote:

The photon is not charged, but in previous UFT papers and in ECE2 (UFT366) the ECE2 theory of light bending by gravitation is given.

Sent: 22/06/2017 20:33:49 GMT Daylight Time

Subj: Re: 380(2): Combined Gravitation and Electromagnetism, Biefeld BrownIf a local gravitational field can be altered by an electric potential can the path of light be warped as means of detection of the gravitational bending?

Sean

On June 21, 2017 at 5:40:42 AM, emyrone@aol.com (emyrone) wrote:

This note gives a scheme of computation on page 7 by which the problem can be solved completely and in general. There are enough equations to find all the unknowns, given of course the skilful use of the computer by co author Horst Eckardt. The Biefeld Brown effect is explained straightforwardly by Eq. (14), which shows that an electric charge density can affect the gravitational scalar potential and therefore can affect g. I did a lit search on the Biefeld Brown effect, it has recently been studied by the U. S. Army Research Laboratory. This report can be found by googling Biefeld Brown effect”, site four. There are various configuration which can all be explained by Eq. (14) – asymmetric electrodes and so on. In the inverse r limit the total potential energy is given by Eq. (19). This gives the planar orbital equations on page 4 of the Note. These can be solved numerically to give some very interesting orbits using the methods of UFT378. The lagrangian in this limit is Eq. (29) and the hamiltonian is Eq. (30). These describe the orbit of a mass m and charge e1 around a mass M and charge e2. If Sommerfeld quantization is applied this method gives the Sommerfeld atom. Otherwise in the classical limit it desribes the orbit of one charge with mass around another. The equations are given in a plane but can easily be extended to three dimensions. Eqs. (31) to (34), solved simultaneously and numerically with Eqs. ((37) and (39), the antisymmetry conditions, are six equations in six unknowns for gravitation and six equations in six unknowns for electromagnetism. These equations give the spin connections and vector potentials in general (three Cartesian components each).

No trackbacks yet.