The Gyrogravimeter in m Theory

The Gyrogravimeter from m theory

Dear Bernhard,
This is very interesting. The relevant equation is Eq. (14) of the attached, the Sagnac effect in m theory, where m can be any function of the distance R0 to the centre of the earth (UFT145 to UFT147). It is the basic equation of an instrument that I referred to as the gyrogravimeter. It simply needs a conventional, high accuracy, Sagnac interferometer, made up of as many loops as possible of a fibre optic wire, so the area is maximized and the instrumental accuracy maximized. For example ten thousand loops increases the area by a factor of ten thousand and increases the time difference by a factor of ten thousand for a given angular velocity of platform rotation. Then this portable and compact gyrogravimeter can be used at sea level and on top of high mountain such as the restaurant at the top of the Jungfrau in Switzerland. Your clocks will be more accurate than a cuckoo clock. In general m can be any function of R0. The Einsteinian general relativity uses the function (15). So this experiment can test the Einstein theory, which is known to be completely obsolete. The portable gyrogravimeter can be used to measure the gravity at any point on earth or space, and is useful for geology, prospecting, and so on. The Einstein theory fails completely in a whirlpool galaxy as is well known. This is shown quite simply in UFT420(1). It has just been shown to fail completely in the S2 star, by a factor of a hundred. So this would be an important experiment. I am not sure if Swiss restaurants are equipped with cuckoo clocks, so your timing devices would be orders of magnitude more accurate.

Myron

Dear Myron

Some weeks ago, Horst asked me about the construction of an experiment you suggested. As I understood, the time taken for a light ray to orbit around a ring (or a polygon constructed of mirrors) is to be measured, depending on the distance to the center of the earth, that is, on the strength of the surrounding gravitational field. More general, it seems to be about different physical processes whose timing could be dependent on the gravity.

Of course, I am happy to help with the project, to create the design and to set up and execute the experiment. I have some cesium atomic clocks; maybe their accuracy is sufficient.

However, I have a question about this:

According to Einstein, the run of the clock (the time itself) is dependent on the strength of the gravitational field too, and also depends on the speed of movement, which increases in mid-latitudes with the height above the ground. Therefore, the orbital period of the light in the experiment can not be measured at all using a clock located near by the experiment – unless your theory predicts a different behaviour. The only thing that comes to my mind is to just move the experiment to different locations, but always leave the clock in the same place. For the measurement then a radio connection would be necessary. What is your suggestion?

best wishes,
Bernhard

PS: Do you need some more animations for astronomical or other purposes? (See our previous correspondence below.)

a420thpapernotes4.pdf


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