## The Tables

10. February 2015 · Comments Off on The Tables · Categories: News · Tags: , If we take the coordinate of a linear movement of the body – we mechanical rectilinear system, we take the rotation angle – get a mechanical rotational system, we assume that the change of electrical charge – we get the electrical system, we assume the movement of the fluid – we hydraulic system, etc. For each type of system has received its own table, but all the tables were completely identical in form, only the names and designations quantities, their dimensions and the units were different. It therefore physics and it seems little devoted to her man so divided. But in reality it is everywhere the same. Such tables for specific forms of traffic on this site is presented as many as 25 of all major sections classical physics: from mechanics, electromagnetism, hydroaerodynamics, acoustics, thermodynamics. Not because, of course, that you can not do more than 25 tables, but because the principle of making the already extremely obvious after consideration of those 25-and.

And if someone wants to choose any 26th or 27th state coordinates, then make himself the 22nd or the 27th table he will have no difficulty. It would seem, everything! It's done! But there it was. As its inception, the system of physical quantities ESVP was itself dictate its author all the new demands. First, it turned out that energy forms and types of energy – not the same as it is still considered to be in physics. Had also been revised classification of mechanical motion. Then it turned out that we should share all physical systems to flow through which something is constantly moving, non-flowing, in which can only something to enter, or which can only be something to get out, and integrated with the properties and those and other systems.

## Direction Coordinate

29. January 2012 · Comments Off on Direction Coordinate · Categories: News · Tags: , All points of F in the coordinates x, y, z can be bijectively associated with the points of the actual physical space in which there is no movement, the point mentally can be described equally. To specify the motion must specify the inertia of the system and get them to coordinate transformations. For this we must expand the viewing area of the coordinate q in F (until a single value). Mentally connect the same point O and a point similar to L by a straight line in the real physical space. According to this line mentally Assume the light signal from a point O, in the direction of L.

The distance from O to light signal is denoted R (OS). Once the signal reaches the L and go farther the distance from L to the light signal is denoted R (LS). Now these terms – O, L and the point of moving the light signal S, consider a space F. If the center coordinates to choose a point O, then (using the distance to the light signal) in F can be defined as the coordinate q: q = R (OS) / c. If the center coordinates to select a point L, then so: q '= R (LS) / c. In fact, in the space F Center coordinates defines its coordinate system. In each coordinate system coordinate q (or q ') can be bijectively mapped to the coordinate time of physical space. This is true in some neighborhood, corresponding to the center coordinates.