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β 2     = 1 / [1  –  (V2 / c2)]

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

THE MATHEMATICAL PHYSICS

the relativity theory

 

The special theory of a relativity

 

 

 

Relativistic kinematics 

 

 

    The basic subjects of articles

 

 presented in a subheading "Relativistic

 

 kinematics":

 

 

0

Articles recommended for

 viewing

 

I

The special theory of a relativity in a general view (using only a principle of a relativity and symmetry of space and time, without application of a postulate on a constancy of a velocity of light)
 

 

II

Definition of speed of movement of the point, which size it would be identical in any inertial system of readout
 

 

III

The equation of communication of factors of transition β (in Lorentz's transformations) for various speeds of movement of inertial systems of readout
 

 

IV

Two variants of dependence of factor of transition β from speed of movement of inertial system of readout

 

V

The basic kinematic equations of the special theory of a relativity for cases, when transition factor β> 1 and 0 <β <1
 

 

VI

Graphic representations of the basic kinematic equations of the special theory of a relativity for cases, when transition factor β> 1 and 0 <β <1
 

 

 

VII

Two variantes of a pseudo-Evklidean          space                                                                          J = c12 ∙ t2 − x2 − y2 −z2                                                                  (when transition factor β > 1) and                                                                                  J = c22 ∙ t2 + x2 + y2 +z2                                                                                                (when transition factor  0 < β < 1)

 


 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

β> 2   = 1 / [1 

 (V2 / c12)]

 

β< 2  =  1 / [1 

+ (V2 / c22)]

 

 

 

 

 

 

 

 

 

 

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