By A P Levich

The topic of this booklet is time, one of many small variety of elusive essences of the area, unsubdued through human will. the 3 worldwide difficulties of common technological know-how, these of the foundation of the Universe, existence and realization, can't be solved with out checking out the character of time. with no strong development of time it really is very unlikely to explain, to qualify, to forecast and to manage a variety of methods within the animate and inanimate nature. designated awareness is paid to the methods of sufficient inclusion of the homes of time within the derivation of the basic equations of movement for typical structures.

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The topic of this booklet is time, one of many small variety of elusive essences of the area, unsubdued by means of human will. the 3 international difficulties of typical technological know-how, these of the foundation of the Universe, lifestyles and cognizance, can't be solved with out checking out the character of time. with out a strong development of time it's very unlikely to explain, to qualify, to forecast and to regulate a number of tactics within the animate and inanimate nature.

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**Extra resources for On the Way to Understanding the Time Phenomenon: The Constructions of Time in Natural Science, Part 1**

**Sample text**

All points of reference frame could be connected by this signal and all "pictures" will be identical (from the viewpoint of the relative positions of the particles). It is natural to refer all these "pictures" to the same moment of the model time. , at the origin of the coordinates. ) Let us introduce the model time X (a correspondence of this theoretical time to time measured by an ordinary physical clock will be discussed in 6). Let us suppose that the value of the time interval dx is the function of differences of spatial positions (for all particles).

I=l i=l N One cannot conclude the identity about the conservation of the value X u y 1=1 Hence, the total kinetic energy may be constant or not. If M=l then we have the analog of the first Newton's law Assuming that M=2, we obtain from Eq. 11 diii du? Aristov. RELATIVE STATISTICAL MODEL OF CLOCKS 35 Let us denote the expression on the right-hand side of Eq. 12 as the force F12 acted on the first particle from the second one (in such a way a concept of force is defined). Then we obtain the analog of the second Newton's law.

E. "instant") is purely spatial, it has no temporal characteristic. The time is added by small intervals which are determined through differences of "instants" As mentioned above the pairs of "pictures" have been used for this process. Note, however, that in the "pictures" not only the radius vectors r [ are fixed but the small values dr [ too Indeed, "the camera" has a finite time of photographing, therefore all moving particles images are "unclear". Hence, the traces of particle motions are given.