8/3/2019 1996.03.28 - Stefan Marinov - MARINOV ANNUS HORRIBILIS http://slidepdf.com/reader/full/19960328-stefan-marinov-marinov-annus-horribilis 1/2 .. ,· . .. ·· · · ·· · · :: - r . . t . o : ~ n r . ·• : .. ; • · , .. :· : .: ; •. , 1. · · r · · .. .... . . ..;..._..._--..;..;_..... ,; ____ ....._ ........~ - - - - - - - ........ ..... . ------- --· - . · AOVERT.ISEMENT: ·· . . . . M A R I N O V : A N N U s H O R ~ I B I L I S The year 1998 will be an earthquake year tor conventlonal· phyalca: many formulas In the textbooks will be changed, many century-old dogmas will be renounced ' and many saints will be de-sainted. This radical change had to begin tens ol years ago but the lack of glasnost In physics all over the world has delayed It and Instead to have evolutl onal step-by-step reformati ons and several ' fighter ea rthquakes. now there wil l be a tremendous one . Vou.s l'avez vou/u, Georges Dandinsl By my half -a-century expe rim enta l and theoret ica l wo rl( I sh. owed t h e foll owing (see re ferences In my 18 books, so · re fer eed papers. 8 pa i d advert i sements and numerous papers and edl tqr ' s comments In the journal DEUTSCHE PHYSIK edited by me): t . Tile principle of re/allv/ly Is wrong. Indeed, I measured three times optlco-mechanlcafly and once electromagnetically 'h e Earth's absolute velocity. Its magnitude Is 350 km sec · • with equator ial coordinates of Its a p e x ~ -2 0 • , 11 = 12" (approx.). 2. T h e pr incipl e of equivalence Is wrong. Indeed, my l nter1er o metr J c "c oupl ed m i rr ors " exp er ime n t w hich was ca r r i e d o ut dur i ng a y ea r showed' th at when th e l abor atory' s a cc elerati on was kin ematic (accelerat i on wlt h "?' espect to di sta nt s ta rs), th e l abor atory' s ve l oci ty changed, while when i t was dynami c (g ravl·. ra ti onal attracti on by the Earth) there was no change. 3 . The energy conservation la w Is wrong . My machines MAMIN COLIU and VENETIN COLIU which work with zero, or near to zero, Lenz effect. and SIBERIAN COLIU which tyorks with anii ·Lenz elf ect vi olated this law. Only bec ause of lack of money I could not cl ose th e energetic circle In the i l rst two, but the third one was not expensive and I coul d r un it as a perpetuum mobile. The day when I shalf present t his mac hin e at a press-QOnference w il l the start d ay lor the ea rthq uake. 4. T he L ore ntz equa ti on I s wr on g. II there ar e two ele c tric ch arges q , q' movi ng wit h ve loc i ties v, v' and the vector-dist a nce from q' to q I s r , according to the Lorentz equation the Ioree with which q'v' acts on qv Is given by the following Grassmann formula f 0 = (p 0 qq'/4nr){( v · r)v '- (v·v' )r}. (1) ' . N4mer ous experiments done by othe r authors (Heri ng's ex pe r i · ments ar e /ro m the beg i nni ng of the c e ntury!) and by me showed Ihat t h e f orce a cti ng o n qv can be . not o nly tra n sve rse to it s vel ocity, as requi r e d by (1), but al so lon gi tud in a l. A ny rat ional man wh en seei n g at least one l al s lt y l ng experi ment re fects the res pectiv e fo r mul a (Popper), however lor thousands and thou· sa nds of B e t o n k ~ p f e even hundred experiments were not enough. In lhe photograph there Is one su ch falsifying experiment which (aswell as the other) can be carri ed out by children: A !Jyllndrlcal mag net I s cut along one of Its axial ' planes and the one half Is tur ned up-down (the magneti c for ces themselves do the r qtatlon) . Around thi s magnet. there i s a t ro ugh filled with me r cu r!/ln wh ich th e c opper rin g wh ich can be seen at right swi ms (the c h ll dr eh take sa lt' so l uti on 11 nd s uspe nd t he ri ng on t hreads). After s endi ng c urr ent o f some te ns of amperes !r o m the batt ery at left, whic h Is re gul ated by t he rheostat , the ri ng begi ns to rotate. That's al ii ;> . The Lorentz-Mar/nov eqvation Is the right one . As accordi ng to ( . 1) f' 0 is not equal and oppositely directed to f 0 , I obtained Mar/nov ormu/11 by the most simple and natural symmetrization of (1) (take Into account that r = -r') f u = (f 0 - ( 0 ) / 2 = (p 0 qq' f 8n r ){ ( v ' · r )v + (v ·r )v' - 2(v·v')r} . (2) . • Procee d ing fr om (2) , a nd assu ming 0, 8Af 8t 0,1 obtained by· the mosl si mpl e ca l culations tha t t h e force with which a n el ectr i c system act s on a test charge q movi ng wit h veloci ty v Is f / q =- gra dCI>- D A/ 81 + v x B + v S = E , ., + v x B + vS, '(3 ) wh er e Cl> , A are the electric and magnetic potentials generated by the system at the PC?Int of the charge's location, a,., = r.ot A Is the Lorentz magnetic Intensity, s•• , = - dlv A/ 21s the Whltlaker mag netic Intensity and . . Bm o • = - ()lo/ 811} J ' (v X Y}(r • v) fv'r , S,.. , = ~ ~ J ' (v ·v' )( r ·v )/ v'r' (4) .. . . AMa · mtaT qJtHHM Ha ww a E nron :t . . ar_ e · the Mer/nov vector and scalar magnet ic i n t e n B ='II,.,+ B.,., Ia . called vector magnetic Intensi ty S '"'s..,. + S.... , Is called eca/ar megnetlc Intensity. (3) is ca l:;)rl the Lorentz-Mar/nov equation. If neglecting the last terrn under B we understand il.,,. we obtain the Lorentz equation whicl'l t call the Lorentz- Giassmsnn equation. That' s the wl]ole th eory! 8. The Bngu l armomentum conservation la w Is wr ong. Elul · Cub mac hi ne w il h Interrupted current and rota ti ng Amper e w it h in t errupt ed curr ent rot ated under the action of in t ernal lotcc s only. Ma r l nov' s for mula allows vi ol ati on of th e a n gular mom cmuu . conservallon law as the magnetic torces wil h whi ch two h a r ~ ; · interact ar e equal and oppositely directed but ma y not lie on t ile line connecting them. 7.11 is Impossible to violate the "!Omentum con serva: ic r. t: . i :; electromBgnellsm . Obvious conclusion from Mar i nov's tor mula 8. Dlsplacement . current does no t exist. For c los ed circ vi rs b olll Grassmann and Marlnov formulas do no t a ttow vi ol ali o n ol the momentum and angul ar mome ntum conservation laws as lh e first terms in (1 ) and ( 2) contai n to tal d ilf erenlia ls . A s convc nrion; . t physics be li eves In the di splacem ent cu rr ent of Ma>.w€: 11. it accepts that all currents. always are c l osed. I s howed 1J1 numerous e xperiments that there i s no d i splacem ent cu rr e :> : (neither In va cuum nor In di electrics) and on e c an i n te rr upt 11 •• · circuits by the help ot condensers. At the age ol 15 1 unoe rs r oo· : that dlspfacement current is a phantasmagoria and pres enl ( l() [ t) my teacher In Sof i a the fottowing objec ti on : "11 th e displ acem c>: ! current between the plates of a condense r ac ts with r nag nc i >C forces on oth er cu rr e nts , the n accord ing to Newton' s th i rd'""-' 11 ' ! o!her currents mus t act wit h mag neti c l orc e so n the di sptacc rn""" · l c ur r ent a nd s et I t In moti on. But how. comr ade · t eacher, c i! n vacuum be set In moti on ?" Teach e r's answer was : " Shut v;J. ch fl d l" 9. The gavge transformations are il l egitimat e. Acco rdi ng 10 conventional phy sics not the potentials bu t th e I ntensi ti es de ter· mine the motion ol the test charge (exactly th e opposite is !r u e). and thus any change olthe potentials whi ch l eave s th e intens i ti <Os the same I s attowable, I.e., one can "c a li b rate " the pot entials. 11 is easy to see that t he c al ibration d i vA = 0 I s allowable . Thu"> conventio nal physi cs believes tha t a r eally existing lorC'J, 11· ., Wh it t aker force f, . = - qvd ivA / 2 = qvs • •• . c a n b e p ut equal 1 zero. Monstrosity! To s ee the acti on of f ., , take t wo me tal s phere> the one charged pos it i vely and the o hter n ! ' g ~ t i v e t y Put around one of the sph er es a c ircular wire along wh ich cu rr ent IIOw$ . so that ills perpendicular to the line connec ti ng the spher es. Wh · :: n connecting the spheres by a w ir e and curre nt begins to I! ow . l ilu c i rcular wire be gins to rotate. The only Ior ee whi c h a c ts o n t M c'l rcular wire Is f., . 10. There I s n o propagation of intera ction. As o nly mass c an move tro m one poi nt to a not her, "i nter acti on " can be o nly a ghost. But a rational man do es not beli eve in ghosts. On th e oth er hand. the mat hematical exp r essi ons o f B .,., and Sm., s how that th e " fields " c ann ot p ro pagate In space with a certai n ve locity. M B .,., and s . . dep end on the direction of mo tion of the test c h<trg'! . To these peopl e who may object that on e Is no t s ure whc tt >c: r II > C Lorentz-Marlnov equation Is the right on e, my answer is: Unl i l the day when some falsifying experiment should be present ed ( l tl is day w il l never come!) the world is impelled to accept it as !r ue . 11. Potential , radi ation an d rad i ation r ea ction elec tric i o:ansl · 1/es . These kin ds of Intensities can be obtained if p uHi ng in the expression f o r t h e L or e n tz el ectr i c I nte nsit y (see (3 )) th-:; observation el ect ri c a nt! magnetic pote nti al s Cl> = qf 4ntJor, A= ~ ~ o q v 4 n r (5) with r =I - v' ·r'/c. . ' ' / = v + u r c. where r, v . u are distance, velocity and acceleration at th e observation moment t and I ; v , u' at the adv anced mom ent ( = t -I c (conventional physics wrongly call s r " ret arded moment " ). Conv ention al p h ysics , f o llo w i ng Liena rd and Wiccllen . wr ong ly wr ites A with v' . Fo r th i s r e ason co nve ntional physics obtains o nly the potential and radi ation Inte nsities . E..,.. E,. . and artificially Introd uces the radi ati on re acti on Intensit y E,., . cQm ing