Gravitational Sensors and the Structure of the Gravitational Field in Six Dimensions of Space and Time

1. Introduction:

Gravitational waves have been predicted and observed by general relativity.[1] Gravitational wave detectors have a very high accuracy for detecting gravitational waves.[2,3] According to the six-dimensional space-time theory, time has two orthogonal dimensions.[4] Gravitational waves affect both dimensions. Electromagnetic waves cause distortions in space and time. However, no interaction between electromagnetic waves and the gravitational field has been observed. In this article, using the properties of Mobius space, a direct connection between electromagnetism and gravity is established. Gravitational field distortions can be detected and measured by Möbius coils. Although the manufactured test sample has high noise and error, it can measure and record changes in the gravitational field. The difference between gravitational waves and gravitational field distortions is their dimension. Gravitational waves oscillate in five dimensions, but gravitational field distortions are four-dimensional. Based on this, antigravity can be developed. This article explores some specifics of antigravity based on the properties of the gravitational field.[5,6,7]

2. Field Stricture:

The gravitational field is a hypercone in five-dimensional space. Figure 1. The hypercone field rotates like a Möbius strip. The field consists of different layers of space-time density. The distance between layers is like the distance between musical notes. Also, the distance between prime numbers in six groups follows this theorem. Also, the eccentricity of the ellipse (density changes) and the distance between prime numbers have a direct relationship with the golden spiral. (2.1) Table 1

$${Log}_2\left({\displaystyle \frac{f_2}{f_1}}\right)=c$$

$$e^{\pi }+\phi =24.758$$

$${Log}_{24}\left({\displaystyle \frac{72}{3}}\right)=1\mathrm{s}\mathrm{e}\mathrm{c}({sin}^{-1}({Log}_n\left({\displaystyle \frac{s}{k}}\right)={\displaystyle \frac{1}{\sqrt{1-\frac{{\left(\ln \left(\frac{s}{k}\right)\right)}^2}{{\left(\ln \left(n\right)\right)}^2}}}}\equiv {\displaystyle \frac{1}{\sqrt{1-\frac{{\left(v\right)}^2}{{\left(c\right)}^2}}}}$$

$$\Rightarrow sec({sin}^{-1}({Log}_n\left({\displaystyle \frac{s}{k}}\right)y={\displaystyle \frac{1}{\sqrt{1+\frac{{-y^2(ln(\frac{s}{k}))}^2}{{(ln(n))}^2}}}}, {Log}_{{\displaystyle \frac{1}{5}}}\left({\displaystyle \frac{72}{360}}\right)=1 , {\displaystyle \frac{\mathrm{l}\mathrm{n}(1)}{\mathrm{l}\mathrm{n}(2)}}=0 , \mathrm{l}\mathrm{n}(\phi )\cong ({{\displaystyle \frac{1}{2}})}^6{\pi }^3$$

2.1

There are two orthogonal dimensions of time. The gravitational field affects both dimensions. Figure 2

Mass results, from changes in the density of space over time. Fluctuations in density can lead to the emergence or dissolution of mass.(2.2) eccentricity of the ellipse in one axis causes eccentricity of the ellipse in other axes. Mass is caused by the absence of three-dimensional matter in higher dimensions. Accordingly, an eccentricity of the three-dimensional ellipse in the gravitational field forms the hyperbolic equation of free fall.

$$\mathrm{s}\mathrm{e}\mathrm{c}({sin}^{-1}({Log}_n\left({\displaystyle \frac{{\rho }_2}{{\rho }_1}}\right)\left(-\sqrt{{\displaystyle \frac{2GM}{r}}}\right)={\displaystyle \frac{1}{\sqrt{1+\frac{-2GM}{r{c}^2}}}}\Rightarrow \ln \left(n\right)=c$$

$$G=\left({\displaystyle \frac{{\left(\frac{{\mathit{tan}}^{-1}\left(\phi \right)-\left(\frac{180}{\pi }\right)}{2\pi }\right)}^3\left(\frac{1}{6}\right){\pi }^3}{c}}\right)$$

2.2

The different layers of the gravitational field follow groups of prime numbers. Also, these layers have a direct relationship with the wave function. (2.3) Table 1

$${\int }_{-\rho }^{+\rho }{\int }_{-t}^{+t}{\int }_{-\infty }^{+\infty }{\left|\psi (\rho ,t,x)\right|}^{2}d\rho dtdx=1 , \left|\mathsf{\Psi }⟩=b_1\left|{\tilde{\psi }}_1⟩+b_2\left|{\tilde{\psi }}_2⟩+\dots +b_n\left|{\tilde{\psi }}_n⟩\right.\right.\right.\right.$$

$$\left|\tilde{\psi }⟩={\alpha }_1\left|A_1⟩+{\alpha }_2\left|A_2⟩+{\alpha }_3\left|A_3⟩+{\alpha }_4\left|A_4⟩+\right.\right.\right.\right.\right.{\alpha }_5\left|A_5⟩+{\alpha }_6\left|A_6⟩\right.\right.$$

2.3