How to register gravitational waves


It is known that in the theory of relativity, “events” appear as a point argument. It follows that the trajectory of motion in this theory resembles a film consisting of a large set of individual frames. In Dmitriev's theory of motion, an “event” appears as a wave, and therefore a quantum argument. Therefore, the trajectory of motion in it is more like an image on a movie screen, consisting of a continuous series of views. Both theories predict the existence of gravitational waves. The only difference is that the theory of relativity predicts the existence of traveling transverse waves, analogous to electromagnetic waves, while Dmitriev's theory predicts the existence of standing gravitational waves.

Attempts to detect Einstein's gravitational waves have so far been unsuccessful. This does not take into account reports such as the one that appeared in 2016, which claimed that gravitational waves coming to us after the merger of two black holes in the universe had been successfully detected. This was a very powerful and grandiose announcement. But for us, it is fundamentally important to learn how to detect gravitational waves near the tree under which Newton experienced their persistent impact. In this article, we will look at a simple and effective way to detect standing gravitational waves, which the esteemed Newton encountered directly under an apple tree.

In order to register standing gravitational waves, we need to construct a relatively simple piece of technical equipment in the form of a special detector. You will probably be surprised, but with the help of this simple equipment, we will be able to photograph standing gravitational waves.

The detector should be a 100-meter aluminum pipe with a diameter of 1 to 1.5 meters. High-sensitivity photographic film should be glued along the entire length of one inner wall of the tube. On the opposite side, a pulse generator capable of emitting a light flux that is as short as possible and sufficiently intense should be placed along the entire length of the tube. Most likely, laser technology will have to be used here, as a microsecond light pulse will be required. Of course, the body of the pipe must be positioned vertically, and we must have control over the pulse light generator. All this is quite sufficient for the reliable detection of standing gravitational waves.

According to Dmitriev's theory of motion, standing gravitational waves arise as a result of the curvature of space into a temporal dimension in terms of the quality of past, present, and future time. This circumstance should be reflected on the exposed photographic film, after a single attack by a pulse generator, in the form of a short flash. The developed photographic film will look like a wave-like zebra, divided into a darker field, which is closer to the quality of the present time, and a lighter field, which is closer to the quality of the past and future. The fact is that the chemical blackening reaction in the zone corresponding to the present should be much more active than in the zone corresponding to the past and future. In this way, we can obtain a real photographic image of standing gravitational waves.

The success of the experiment will largely depend on the light sensitivity of the photographic material used. It may be necessary to create a particularly light-sensitive photographic material capable of responding to the shortest possible exposure to light. Most likely, traditional photographic film will be replaced by high-tech electronic sensors, perhaps photoresistors, which are used in micro lithography. And, of course, much will depend on the capabilities of the generating device, its ability to provide a sufficiently intense flow with a very short light pulse. This is because the emergence of standing gravitational waves, i.e., wave disturbances in space in the time dimension in terms of the quality of past, present, and future time, occurs at the speed of light. If we are unable to fit our experiment into the extreme photo mode, the overall picture on the developed film will be blurred into a single color, and we will not see the gravitational wave zebra. Although preliminary calculations indicate that modern technical means are quite sufficient to achieve positive results.  

At the beginning of this article, we provided a brief comparative analysis between the theory of relativity and Dmitriev's theory of motion, using the example of a film strip with individual frames and a continuous image on the movie screen. So, the detector for registering gravitational waves works in reverse, as it were. It allows us to break down the continuous series of motion trajectories that occur in the surrounding world into separate wave frames. After all, we know that an aluminum detector standing vertically on Earth, according to the principle of equivalence, remains in a state that cannot be distinguished from acceleration.

To verify the validity of Dmitriev's theory of motion, this same detector should be lifted on a balloon and released into free fall. After exposing and developing the photographic material, we should find that the film is evenly colored, without wave-like stripes. This is because, according to Dmitriev's theory, free fall in a gravitational field is equivalent to a state of rest. This is when space is not curved into a wave dimension in terms of the quality of past, present, and future time.

February 9, 2026. Boris Dmitriev.