Setting Up of the Set of Equations of the Rotary Antigravitation Engine
Posted On Wednesday May 21 2008 @ 9:00 aAbstract
It can be inferred from the theory of relativity that a rotating body in a certain situation can bring about the effect of the inertial frame dragging. Based on this principle a rotary engine can be designed, which can produce usable and controllable effect of the inertial frame dragging, and which can be used in the fields like space flight.
1. The Sine-Curve-Like Geodesic of a Body in Inertial Motion
Suppose a well-balanced body called Body B is in inertial motion along the x-axis. According to the general theory of relativity, since Body B has mass, the space around it is curved.
Because of Lorentz contraction, the curvatures both in front of and at the back of Body B are larger. According to the general theory of relativity, the geodesic of Body B will be bent. First it will leave the x-axis, go round the area where the curvature is larger, and then get near the x-axis. When Body B moves along this geodesic, a new area in which the curvature is larger forms. So the geodesic will dodge this new area and, when arriving at the x-axis, will go round this new area on the other side of the x-axis.
Hence the geodesic of Body B looks like a sine curve. Since the energy of Body B is constant, the geodesic should be a sine curve.
Let the sine-curve-like geodesic be
y = A sin ( ��x + ��o ) (1)
where A is the amplitude, �� is the angular frequency, and ��o is the initial phase.