Transverse and longitudinal mass moving in the inertial frame of reference

Transcription

1 Fro the SelectedWorks of Vildyan Yanbiko 0 Transerse and longitudinal ass oing in the inertial frae of reference Vildyan Yanbiko Aailable at:

2 Elseier Editorial Syste(t) for Adances in Space Research Manuscript Draft Manuscript Nuber: Title: Transerse and longitudinal ass oing in the inertial frae of reference Article Type: FM Keywords: Calculation of the transersal and longitudinal asses, the ast cosic space, oing inertial reference syste. Corresponding Author: Dr. Vildyan Yanbiko, Corresponding Author's Institution: Independent researcher First Author: Vildyan Yanbiko Order of Authors: Vildyan Yanbiko Abstract: Based on the speed of the spread of ector interaction in a oing inertial frae of reference. A calculation of the transersal and longitudinal ass of eleentary particles. Suggested Reiewers: Vildyan Yanbiko ildyanyanbiko@yandex.ru Yan Vil ildyanyanbiko@yandex.ru Vil Yan ildyanyanbiko@yandex.ru

3 Manuscript Click here to download Manuscript: Macca ENG..doc Click here to iew linked References Transerse and longitudinal ass oing in the inertial frae of reference Yanbiko Vil'dyan Shakyatoich Russian Federation, Volgograd, 000, Bibliotechnaya street, house, apartaent. Phone: e-ail: ildyanyanbiko@yandex.ru Аbstract: Based on the speed of the spread of ector interaction in a oing inertial frae of reference. A calculation of the transersal and longitudinal ass of eleentary particles. Keywords: Calculation of the transersal and longitudinal asses, the ast cosic space, oing inertial reference syste. 0

4 We calculate the cross-section and longitudinal ass oing in the inertial frae of reference Inertial reference syste oing along the axis OZ with soe elocity relatie absolutely fixed reference syste. The axis of X,Y,Z coincide with the axes of the X,Y,Z. Let absolutely identical particles A and B lie in the oing reference syste X,Y,Z. (fig..). The ass of each particle A and B is equal to in the oing syste of reference. In a fixed reference ( = 0 ), the distance between the particles A and B is equal to the r o. In the coordinate syste X,Y,Z, the distance between the sae particles will be equal to r. Let between particles A and B jups carrier the power of interaction. When = 0 period of exchange carrier of interaction will be equal to Т 0 = ; where c is the elocity of light in acuu. In the oing reference syste X,Y,Z, during the exchange carrier of interaction will be equal to T = ; Ask the condition r = r o. Get Т = ; The frequency of exchange carrier of interaction in the syste of reference X,Y,Z equal n = n o ; where n o = and n = ; The strength of the interaction between the particles A and B when = 0 is proportional to the n o. Then it is alid F o = k n o ; Where k is the coefficient of proportionality. Express the force F o through the ass and the acceleration of the reference syste X,Y,Z.Get k n o = o α o ; where o is the ass of particle A or B at = 0 ; α o acceleration of particles A or B at = 0. The strength of the interaction between the particles in coordinate syste X,Y,Z is equal to F = k n = α ; where is the ass of particle A, or B in the reference syste X,Y,Z. α acceleration of particles A or B when 0. The weakening of the forces between the particles in coordinate syste X,Y,Z due to the decreasing frequency of exchange ector of interaction between the particles A and B. F = F o ; Ask condition α = α o. We obtain the ratio = = ; Hence, it turns out = o ; Reduction of forces between the particles A and B. F = F o subject r = r o and α = α o, equals the rise of the ass particles А and В according to the law = ()

5 Now let particle A and B the rest in the reference frae of the X,Y,Z, are as in fig.. Moing with the elocity along the positie direction of the axis OZ. The ass of each particle A and B is equal to in the oing syste of reference. In a fixed reference ( = 0 ) distance between particles A and B is equal to the r o. In the coordinate syste X,Y,Z distance between the sae particles is equal to r. Ask the condition r = r o. Find the dependence of the longitudinal particle ass A and B fro its elocity relatiely absolutely fixed reference syste X,Y,Z. Find the period of exchange carrier of interaction between particles of A and B. Speed ector of interaction of particles A to particle B is equal c z+ = с (- ) ; Speed ector of interaction of particles In a particle B to particle A is equal c z- = ) ; Tie otion ector interaction of particles A to the particle B is t + = ; Tie otion ector interaction of particles B to the particle A is t - = ; The exchange tie t = t + + t - = or t = ; where t = ; During the exchange period T = ; The frequency of exchange carrier of interaction in the syste of reference X,Y,Z equal n = n o / ; where n o = and n = ; The strength of the interaction between the particles A and B, if = 0 proportional n o. Then F o = k n o ; where k is the coefficient of proportionality; Express the force F o through the ass and the acceleration of the reference syste X,Y,Z. Get k n o = o α o ; where o is the ass of particle A, or B at = 0 ; α o acceleration of a particle A or B at = 0. The strength of the interaction between particles in the syste reference X,Y,Z equal F = k n = α ; where the ass of particle A or B in the reference syste X,Y,Z, α particle acceleration A or B when 0. The weakening of the forces between the particles in reference syste X,Y,Z due to the decreasing frequency of exchange ector of interaction between particles A and B. F = F o / ; Ask condition α = α o.

6 Get = = / ; Then = o / ; Reduction of forces between the particles A and B in the for of F = F o Subject r = r o and α = α o, equals the rise of the ass of the particles A and B in the for of = () / ;

7 О Z fig.. А В X О Z fig.. X A B