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M(V)     / [1    (V2 / c 2)]1/2

 

P(V)     =  (   V ) / [1 

  (V2 / c 2)]1/2

 

Ekin(V)  =   c2   {{1 / [1 

  (V2 / c 2)]1/2}  1}

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

P =  Const

 

E  =  Const

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

THE MATHEMATICAL PHYSICS

the relativity theory

 

The special theory of a relativity

 

 

 

Relativistic dynamics 

 
 

 

    

The basic subjects of articles

 

 presented in a subheading

 

 "Relativistic dynamics":

 

 

 

0

Articles recommended for

 viewing

 

I

Definition of dependences of weight, impulse and kinetic energy of a body from speed of its movement (for cases, when transition factor β> 1 and 0 <β <1)

 

II

Comparison of dependences of weight, impulse and kinetic energy of a body from speed of its movement for cases, when transition factor β> 1 and 0 <β <1

 

III

Graphic representations of dependences of weight, impulse and kinetic energy of a body from speed of its movement for cases, when transition factor β> 1 and     0 <β <1

 

IV

Check of dependences of weight, impulse and energy of a body from speed of its movement on performance of laws of preservation of an impulse and kinetic energy by consideration of concrete examples of the closed mechanical systems in which interaction of components has instant character, for cases, when transition factor β> 1 and     0 <β <1

 

V

Definition of values of constants 1 and 2 in transition factor β

 

VI

Considerations of the concrete example showing infringement of laws of preservation of an impulse and energy of closed mechanical system, interaction of which separate elements can have constant character, for cases, when transition factor β> 1 and 0 <β <1

 

VII

Definition of conditions of performance of laws of preservation of an impulse and energy of the closed mechanical system for cases, when transition factor β> 1 and 0 <β <1

 

VIII

Consideration of concrete examples of infringement of laws of preservation of an impulse and energy of the closed mechanical system at application of the special theory of a relativity

 

IX

Possibility of variables on time of values of an impulse and energy of the closed system at application of the special theory of a relativity

 

X

Calculation of sizes of an impulse and kinetic energy of the concrete closed mechanical system, interaction of which separate elements has constant character

 

XI

Schedules of dependence of sizes of an impulse and kinetic energy from time, received by consideration of the concrete closed mechanical system, interaction of which separate elements has constant character

 

XII

Definition of conditions of performance of laws of preservation of an impulse and energy of the closed mechanical system, interaction of which separate elements has constant character

 

XIII

Substantiation of possibility of use of transformations Galilee for any values of speeds of movement of inertial systems of readout

 

XIV

Consideration of the example showing possibility of infringement of the law of preservation of an impulse at linearly located closed mechanical system

 

XV

Communication between coordinates and time in pseudo-inertial systems of readout

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

(V) / [1   

 (V2 / c12)]1/2

 

P(V)>     =  (  

 V ) / [1   

 (V2 / c12)]1/2

 

Ekin(V)> =

c12 {{1 / [1  

(V2/c12)]1/2}  1}

 

(V)<   / [1 

(V2 / c22)]1/2

 

P(V)<     =  (  

 V ) / [1 

(V2 / c22)]1/2

 

Ekin(V)<     =  

 c22 { 1

  {1 / [1  +  (V2 /

c22)]1/2}}

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

P ≠  Const

 

E  ≠  Const

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

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