Phenomenon the kinetic energy and the inertia material of the bodies

Transcription

1 Phnomnon th kinti nrgy and th inrtia matrial of th bodis F. F. Mnd Abstrat In th artil is xamind physial natur of th inrtia of matrial tl. Good is known, that for th alration matrial th bodis it is nssary to spnd nrgy, for what to by it is nssary to apply th for. Exutd th work passs into kinti nrgy th motion. ith braking th body rturns this nrgy to th surrounding bodis, for what thy b rquird th fors, rrs that, whih th body alratd. This is th phnomnon th inrtia. Is lar, that th pross th alration aumulats into th body what form of nrgy, whih and rturns thn to xtrnal mdium with its braking. But not on of xisting into prsnt th tim th thoris not gis th answr to a qustion, that this for nrgy and by what by th mans it is aumulatd and it rturns. Chargd th bodis and th hargs ar had ltrial th fild, possssing nrgy. It is possibl it was to xpt, that th dpndn of ths pour on from th spd it ould spill th light to this a qustion. In th spial th thory of th rlatiity (STR) ltrial

2 th fild of th hargs dpnd from th spd, and, it would sm, this of th thory it must was gi th answr to this intrsting a qustion. But into STR th harg is th inariant of th spd. Into th works [-3], is shown, that into th framwork of th Galilan transformations salar th potntial of th harg dpnds from his th rlati spd. ith this ltrial th fild, normal to th dirtion its th motion, inras, into of th of th tim as longitudinal th fild rmain onstant. Similar th approah gis th possibility to xplain and th phnomnon of th kinti nrgy and th phnomnon th inrtia. Th ltron has ltrial th fild, nrgy whih of asy to alulat. Spifi nrgy ltrial pour on it is writtn as w = ε E. Th tnsion ltrial pour on th ltron it is dtrmind by th quality E =. ε r Using th lmnt th olum r dr, w obtain of nrgy pour on that bing rsting th ltron: dr = =, 8ε ε a a 8 r whr - th harg of th ltron, and a - its a radius. If th ltron mos from with th spd, th its ltrial th fild, normal to th dirtion th motion aording to th onpt of salar-tor potntial thy inras:

3 E = Eh E + Lt us writ down ltrial th fild, normal to th dirtion th motion into to th systm th oordinats, that rprsntd in Fig. dq q r dr. rdq r sin q Fig.. Th lmnt th olum r sin q dq dr, utilizd for th alulation nrgy pour on that moing th ltron. E = E + sin q Thn nrgy pour on that moing th ltron it will b writtn down 3 sin q dqdr = + 8ε r Th intgration on to th angl gis 3 sin ( os ) (os ) os 3 3 os q q dq = q d q = q + = 3 3

4 Thrfor dr = 3 + = 8ε a r ε a For th spds is onsidrabl smallr th spd of th light th trm an b disrgardd, thrfor = ε a Th onntion btwn by nrgy pour on and with th mass th rst of th ltron it is gin by th quality []: = m 3 8ε a =. Consquntly additional nrgy th ltron, onntd from that, that its th fild dpnd on th spd, to b dtrmind by th rlationship = m. This and is kinti nrgy that moing th ltron. It is diffrd from that onntional th alu by th offiint, but this indiats only th, that offiially aptd th alu th mass th ltron it is nssary to dras into two tims. By suh by th mans, w stablishd physial th rason for th prsn in moing hargd th bodis th kinti nrgy and onsquntly and thir inrtia th proprtis of. Ths th proprty ar onntd from

5 with th dpndn th salar th potntial hargs on thir rlati th spd. REFERENCE. Менде Ф. Ф. Существуют ли ошибки в современной физике. Харьков, Константа, с.. Менде Ф. Ф. Непротиворечивая электродинамика. Харьков, НТМТ, 8, - 53 с. 3. Mnd F. F. On rfinmnt of rtain laws of lassial ltrodynamis, arxi, physis/8.. Фейнман Р., Лейтон Р., Сэндс М. Фейнмановские лекции по физике. М: Мир,