Z-Theory. Introduction

In 20th-century physics, those points were called “points of space with equal potential energy”. In case of Z-Continuum, they possess the exact physical value of Z-Continuum disturbance. In other words,

Therefore, any object follows that law as long as it keeps a constant absolute altitude. Points H1-H3 and J1-J4 are good examples. Points H1-H3 remain at the same absolute altitude L2 and keep the same level of interaction with Z-Continuum. Points J1-J4 use another (constant) level of interaction. Therefore, an object that maintains a continuous absolute altitude also maintains the same level of interaction with the Z-Continuum. Moreover, any relocation of such an object (by any distance) within the same altitude changes nothing in its way of interaction with the Z-Continuum.

As mentioned above, Z-Continuum exists everywhere and at all times. In other words, it supports some physical connection between all its points. For example, Bob covers some trajectory by his car between points H1 and H3 in three days. The vehicle maintains the same level of interaction with the Z-Continuum at both the first and last points of its route.

Suppose now this, Bob covers that route in five days. The situation remains unchanged in this case because the level of interaction between the car and the Z-Continuum at both points remains the same, regardless of the car's later arrival at the destination point. In other words, the relocation of a vehicle along a route with a constant altitude changes nothing in its interaction with the Z-Continuum, regardless of its points of location and duration of travel.

Suppose now that Bob looks at the Z-Continuum from another perspective, one that includes that continuum as the first aspect of the Universe. In that case, Z-Continuum becomes responsible for some level of interaction between an object and the continuum itself. That interaction lasts forever and reaches a specific level at any point on the Z-Continuum.

For example, an object (supposed to be a car) located at the point H1 has some level of interaction with Z-Continuum equal to C1. Another object (believed to be an aircraft) situated at the point J2 has another level of interaction with Z-Continuum equal to C2.

Any object maintains the same level of interaction with the Z-Continuum as long as it remains in a location within the Z-Continuum that has a constant value of such interaction. Those are Equal Strength Points (ESP). Strength appears as force (of some exact magnitude) caused by the interaction of a particle of a given body with the disturbance that Z-Continuum delivers to that same point.

In the case of aircraft and the Earth, the Z-Continuum supports the propagation of all disturbances caused by the planet's electrical charges toward the aircraft. As mentioned above, this disturbance causes forces to be applied to the aircraft. However, the net force remains zero because the elementary forces of each pair compensate each other. For example, there are two elementary forces, Fc1p and Fc1n, that make the level of interaction between the Earth and another object located at the absolute altitude L1 equal to C1. Z-Continuum supports propagation of that disturbance.

Any physicist of the 20th century tells you that the Earth is “an electrically neutral body”. That illusion comes from the way of field detection. A pair of equal electrical charges makes two forces on another electrical charge. Those forces compensate each other at the level of an object. Still, they remain as physical entities at the level of any charged particle. That happens because fields follow the law of superposition and never make any impact on each other. They affect only particles placed in those fields.

Statement C leads to some critical conclusions. Suppose now this. An aircraft moves from point J1 to J4. The level of interaction between the plane and Z-Continuum remains the same at both points. Therefore, such relocation by trajectory J1-J2-J3-J4 changes nothing in the physical interaction between the aircraft and Z-Continuum at the first and the last points of the trajectory.

It is also possible for the aircraft to change altitude. Therefore, it can reach point J4 by the J1-H2-J4 trajectory. Despite the changes in trajectory, the result remains the same, and the aircraft maintains the same level of interaction with the Z-Continuum at both the first and last points of the trajectory.

A similar line of thought leads to the conclusion that the aircraft maintains the same level of interaction with the Z-Continuum at the first and last points of the trajectory, which remains at the same absolute altitude regardless of the trajectory that connects those points.

That statement is well known in 20th-century physics as the principle of conservation of energy in conservative fields. In other words, the full energy of the free-falling object remains constant at each point of its trajectory. Moreover, so-called “potential energy” remains steady at any point of the trajectory that remains at the same altitude. Z-Theory explains a similar aspect by physical interaction between a moving object and the Z-Continuum.

In that case, the presence of a physical trajectory in so-called "space" (RW-Trajectory or W-Trajectory, in categories of Z-Theory) becomes also negligible. In other words, Bob needs a powerful car to reach his destination because of the resisting force that drags his car back as soon as it starts moving. For the Z-Continuum, relocating the vehicle between two points (H1 and H3) requires no energy consumption or exchange of energy.

It looks strange at first glance. However, artificial satellites use a similar condition of motion. They need no “constant power” to cover long distances above the atmosphere because there is no resisting force there.