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Herring, Graneau. Pappas, Phipps and others.This has been started in theanalysis of Ampere s hairpin experiment by Saria and Spencer'*.The Edwards EffectIn the Edwards effect, the source isthe receiver is stationary so u»0, du/dt.a steady current so dv/dt-0 andih«^jfc^?Fig. 3In this special case the Weber equation, Eq. (3). becomes,Fw= ar4nz^r1 n- v^' 3(v.t/2c(30)For the classical equation (10),Fc - tr4n£^r(31)and for the new relative velocity formulation. Eq. (13)
- IllQ4ne^rV X (v X tj.)2c(32)Adding terms from Eqs. (30), (31) and hZ) for both positive and negativecharges in the conductor, the coulomb terms cancel andFw -ar^ 21-^sin4nz^r 2\c 92(?3)Fc =(34)^ ^-1 cos 9 a,Snc^r 2 c (35)The classical theory predicts that the Edwards effect does not exist.Both theWeber and the relative velocity formulation give a force which isproportional to (v/c)2.However, the directions and the angular dependenceare different. Only the expression, Eq. (35), is in agreement with theEdwards experiments as has been previously pointed out20.ConclusionsThus, we can conclude that there appears to be a large body ofexperiments which can be explained by the new relative velocityformulation of electrodynamics.The Weber-Ampere formulation appears toprovide tangential forces when d2Fir is considered. However, when thenecessary integrations are carried out for a closed circuit dFv is alwaysperpendicular to the current element and agrees exactly with classicaltheory. The relative velocity expression contains a true tangentialcomponent which does not disappear when d2FR isintegrated about a closedcircuit. Detailed analysis of each experimental configuration is necessary to
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Stefan MarinovTHE THORNY WAYOF TRUT
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EOM TEBE, n03T, rOFDC ^H -OCTAJibHO
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- 3nEPflHCJlOBHE ,^„ ,,(FARTVIORD
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T/iX6 dAowlng, ca wzit ca alZ dfiam
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Because aware of all of this, Dr. M
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i,^ t^^^l.^.^4A:% oeiM9^^
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AKaACMOK B. H. rO:ibflAIICKIinMiic
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.J|r«.j;i^^SCIENTIFICPAPERS
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^- 15 - MarinovLet us calculate fir
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- 17 - I Man' noVMaking calculation
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_ 19 - MarinovI did such an experim
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- 21 - .,^ MarinovAs the power incr
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- 23 - f MarinovVREFERENCES1. S. Ma
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Z5 -Fig. 3ll
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- 27 - Marinovtheory and Gras'smann
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- 29 - MarinovThis assertion of Gra
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,.Then/ w ."- 31 - Mari'novB = rotA
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- 33 - MarinovFig. 1
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- 35 -#•\- '
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jI 37Uwolule and RelaUve Nwfton-Lor
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- 40 -1845. ANNALEN JVo. 1DER PHYSI
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â.die Einwirkungchics gesclilossen
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- 44 -4) Ich gelic (lalicr, ohiic z
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46fiir ciiieii Winkclshom cbcii so
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48 -Siroinclcraentczwei Glicdcnidic
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Zu- 50 -iiientheile cbcii so den Wi
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- 52 -^^ben Ebenc aiigcIiOrcii. F(i
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eingcschalteten54sonst ebcii A i"h1
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«56die Wirkiing a«f ^ "^^'^ ^^'*
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58Na A ^ BSi^N
Page 64 and 65: - 60 -DE L'ACADEMIE DE PARIS, vol.
Page 66 and 67: .- 62 - ^0 -i ,according to the vie
Page 68 and 69: 64PrefaceThis book has resulted fro
Page 70 and 71: -66 -considers the specific current
Page 72 and 73: 68What results from equation (2) is
Page 74 and 75: - ?oc^Then,dx dy dzarc the componen
Page 76 and 77: - 72 -into(9) ^•^.==2j2j"rv^'dF"^
Page 78 and 79: s = -n -
Page 80 and 81: - 76 -Wc will want to continue to t
Page 82 and 83: - 78 -VV?tr,(6)^ ^ ^' J^r 2 zi' £'
Page 84 and 85: - 80,(1) ,(1)•>y, di ^ 'by dt ^y
Page 86 and 87: Thus, Weber's hypothesis, in the ca
Page 88 and 89: and function g here is dependent on
Page 90 and 91: - 86 -when the summation is extende
Page 92 and 93: The Equivalence of Ampere's Electro
Page 94 and 95: - 90 -Equivalence of Ampere* s Elec
Page 96 and 97: - 92 -to the flow of current was va
Page 98 and 99: • w-AMPERE'S CARDINAL LAW IN EXPL
Page 100 and 101: ,forcesLorentz's Formula (6) implie
Page 102 and 103: - 98 -similar coils, supplied with
Page 104 and 105: 100 -product of q and *, but for th
Page 106 and 107: - 102Fig.1The force per unit lest c
Page 108 and 109: - IMHowever, if we follow the Gauss
Page 110 and 111: - 106Fr.-IQ1Q2I4nc^ru. X (tr)< tf)2
Page 112 and 113: 1C8 -However, if there are Ni and N
Page 116 and 117: determine whether these qualitative
Page 118 and 119: - 114 -MARINOVS COMMENTS ON THE PRE
Page 120 and 121: 116vity w = V -u, wherew is the vel
Page 122 and 123: - use-The following paper was prese
Page 124 and 125: - 120 -debate. I have chosen to pos
Page 126 and 127: -It- 122 -route this energy takes,
Page 128 and 129: This- 124 -Invariance with translat
Page 130 and 131: - 126 -how currents produced by hea
Page 132 and 133: - 128 -classical relativlstlc expre
Page 134 and 135: - 130 -Without wishing to criticize
Page 136 and 137: - 132 -The conclusion to be drawn f
Page 138 and 139: - 134 -2. WHAT WAS WRONG WITH THE I
Page 140 and 141: 136 -My expression for the magnetic
Page 142 and 143: - 138done) any efforts so that the
Page 144 and 145: •Such.be some group beliefs held
Page 146 and 147: tapping, and the Great I Am), it is
Page 148 and 149: 144SEAGREEN (Bologna), Nr. 5/6, Inv
Page 150 and 151: - 146rhadata.Secondo le cosIk) pens
Page 152 and 153: 148R. Vediamo... ancora la velocity
Page 154 and 155: 150Stefan marinovdilatazionecinemat
Page 156 and 157: - 152 -osservatore che sa che il pr
Page 158 and 159: - 154 -stessa iTtezza cm h suto pos
Page 160 and 161: - 156 -Considehamo dunque una giost
Page 162 and 163: j158THE PLASMA GENERATOR OF FREE EN
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160 -the case with all known to hum
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162of us have seen at storms. The b
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- 164 -generator "Nigotron". During
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- 166 -only the rotational pump as
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- 168 -power surely is bigger than
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- 170 -rnivwsiUI J. E. Purky&i Bnw.
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*m«»l'^173132 V. Fabsky und J. Ja
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- 175 -134V. Fabskt and J. Jxti6A10
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IVacuum energy:iabreakthrough177 -P
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179beta-decay by 6.0%. This is only
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1816) Samokhin writes: "It is gener
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183 -defined, however, by a new act
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185 -constructive units of the rest
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187 -It would be fine, but quite st
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'^'- 189REFERENCES1. Kiyoshi Kato,
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191 - TABLE 4-18R|^ (in 10 m) for s
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I193CORRESPONDENCE
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195CZECHOSLOVAK JOURNAL OF PHYSICSR
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197 -(But S in equ.
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199INDIAN JOURNAL OF PHYSICSINDIAN
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201CZECHOSLOVAK JOURNAL OF PHYSICSA
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- 203i:^.^. ? ;.surements also on o
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- 205ĀCTA PHYSICA SLOVACA(see TWT-
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'•Dr.> JJ .'-'•' :'' ''Petr Bec
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209 - ACTA PHYSICS SLOVACAAUTHOR'S
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I211The derivation of the Lorentz f
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STEFAN ^:''ÂB1N0VA-gOlOOR^Z- AUSTR
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215STEFAN MARBVOVMorellenfeldgasse
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217PHYSICS LETTERS AROr ESSOR J.R V
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219INDIAN JOURNAL OF PHYSICSINDIAN
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1- 221 -PHYSICS LETTERS AOFESSOR V.
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.- 223 -A-8010 GKf>.:^ — AUSTRIAT
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2252. The referee knows (I presume)
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J. P. WESLEY, Ph.D. Physicist- 227
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229ANNALS OF PHYSICSEditor-in-Chief
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^WORLD- 231SCIENTIFIC PUBLISHING CO
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233Editor:PHYSICS ESSRVSAN INTERNAT
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235 -Mord'cnfoHc-.r.'ê 16 25 April
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- 237DEM CHRISTLICHEN KOMÛNISMUS E
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- 239 -MEINE VORSCHLAGE ZU DEM 27.P
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241 -'HYSICS LETTERS AHoping to rec
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does not depend on the radius of cu
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.dit orial not e. See Marinov's Sin
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[ needftf'**!Ône must especially E
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^pere: d^d^d^' = (R/R^) C -2J.J' .
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251Zentralkomitee derKommunistische
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- 253 -International scientific, te
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255 -Moreilenfeldgasse 16A-3010 GRA
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- 257 -Sre^NMAEINOV p,of. I. Kovacs
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,- 259 --7 2legs) must be \1q = 4tt
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STEFAN MARINOV- 261 -'acta'^physJca
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.STEFAN MARINOV,- 263 -Prof. Robert
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265PHYSICS EssnvsEditor:E. Panarell
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-267-STEFAN MARINOV Dr. Peter Newma
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.269 -over a sinall volume where J,
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- 271-2 20 2 2f = 4tt/c = 4Tr/9xlO
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: shall: wish- 273 -STEFAN MARINOV
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,275annnor maphhoba k efo yawio amc
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''I uber27 7-; Tran, nurwenige Kilo
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- 279 -VIS 900612"address for proof
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Morellcnfcldgasse 16A-8010 GRAZ - A
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.283GALILEAN ELECTRODYNAMICSBox 251
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P. T. PAPPAS- 285 -Prof, of Mathema
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;- FAN'287itefan Marinov's seasonal
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- 289 - 1 LETTER TO THE EDITOR OF "
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- 291 -STEFAN MARINOV Prof. p. T. P
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STEFAN MARINOVMorellenfeldgasse 16A
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- 295 -PHYSICAL SOCIETY OF JAPANKik
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:- 297 -STEFAT^ MARINOV Dr. Petr Be
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STEFAN MAPJNOVMorcllcnfeldgasse 16A
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- 301 -SIEFAN MARINOVp ^ i p v•Mo
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'STFFAN,- 303 -MAPIlSinV ^^' Taizo
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- 305ANNALS OF PHYSICSEditor-in-Chi
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- 307 -International scientific, te
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- 309&IEFAN MAMNOV ^ ^- ^ ,^^^Dr. S
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MarinovSir— I wish to state that
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STEFAN MAPINOV- 313 -^ iMorellenfel
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315 -BEFORX OH TBB PAPKR ERXIXUSDPH
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I,The- 317 -Bohm-Aharonov effect ar
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1Dr. P. BeckmannSTEFAN MARINOV319 -
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- 321 -CONTENTS:Preface (nepAHcnoBH
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The eighth part of the collection o
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