Einstein s Velocity Composition Proven Wrong. The Complete Proof. Copyright 2003 Joseph A. Rybczyk Revised October 10, 2003

Transcription

1 Einstein s Veloity Composition Proen Wrong he Complete Proof Copyright 003 Joseph A. Rybzyk jrybzyk@erizon.net Reised Otober 0, 003 Abstrt Presented in this work is methodil, systemti, nlysis ontining the omplete proof tht Einstein s eloity omposition formul is inlid for its intended purpose inoling uniform motion. In the nlysis, it is shown in indisputble terms, tht Einstein s formul tully inoles elertion nd is in ft n elertion omposition formul. Nonetheless, it is further shown tht een in tht pplition, the formul is less urte thn the millennium reltiity elertion omposition formul erlier deried for tht sme purpose. In onlusion, it is lso shown tht the erlier deried millennium reltiity formul for eloity omposition is the only lid formul for the purpose originlly limed for Einstein s formul.. he Findings of the Millennium heory In the millennium reltiity pper on eloity omposition, it ws shown tht Einstein s formul for eloity omposition, u + u u u u + () Speil Reltiity Veloity Composition nnot be orret. In this formul, u nd u re uniform motion speeds reltie to the sttionry frme (SF) nd u is uniform motion speed reltie to the uniform motion frme (UF) moing t speed u. he orret formul for eloity omposition ws then deried nd introdued s, u u + u u () Millennium Reltiity Veloity Composition where ll of the ribles he the sme definitions just gien. hese findings hllenge some of the most bsi ssumptions underlying the priniples of reltiity, nd should not be tken lightly by the sientifi estblishment. Subsequent findings, ulminting 8 months of exhustie reserh, not only reinfore the initil findings, but lso go on to show tht Einstein s formul tully inoles elertion nd not uniform motion s speified in his theory. Our objetie here is to present these findings in suh expliit terms s to defy repudition by een the stunhest defenders of Einstein s theory.. Aelertion Composition for Instntneous Speeds Of first importne in estblishing the proofs to be presented here is to disredit ny rguments tht might onsider the findings inlid simply beuse they were disoered during the deelopment of n lterntie theory to speil reltiity. As should be obious in the presented nlysis, suh rguments re entirely without merit nd ompletely irrelent sine the findings n lterntely be onfirmed within the ontext of speil reltiity. Proeeding then, it ws shown in seerl reent works tht the following formul,

2 k m + (3) Reltiisti Formul for Kineti Energy is orret formul for reltiisti kineti energy. his lim hs sine been orroborted by theoretil physiist t SLAC 3. Sine the boe formul gies the sme results s Einstein s formul, it n be further limed tht there is no onflit here regrding the stndrd model. Along tht sme line of resoning, it n lso be limed tht tht there is no new physis here, nd tht ws preisely the onlusion of the physiist t SLAC. Although the uthor disgrees, wht is tully importnt here is how this formul is deried. Speifilly, it is deried through diret modifition of Newton s kineti energy formul using gmm s follows: k m (4) Newton s Formul for Kineti Energy k m( γ ) + γ (5) Newton s Formul Corretly Modified for Reltiisti Kineti Energy In the boe modifition, gmm is gien s, γ (6) Alterntie Form for Gmm whih is simply nother form of the more fmilir, γ (7) Speil Reltiity Gmm speil reltiity gmm; so gin there is no onflit with the stndrd model. Of next importne is the ft tht in onsistent mnner, Newton s distne formul for onstnt elertion n lso be modified to its reltiisti form using gmm. ht is, where is the SF distne treled under onstnt rte of elertion during the SF time interl tht instntneous speed reltie to the SF is rehed, the resulting Newtonin formul for the distne treled during onstnt elertion, D (8) Newtonin Formul for Constnt Aelertion Distne n be modified to its reltiisti form using gmm s follows: Beginning with the millennium theory time trnsformtion formul, first introdued in the min Millennium heory of Reltiity 4 pper, we he, t. (9) ime rnsformtion for Inertil Frme In this formul, t is the UF frme time interl tht trnspires during SF time interl. Sine, it ws lredy shown in eqution (6) tht the mthemtil expression, Millennium heory Expression for Gmm n be represented by the Greek symbol, γ (gmm) the time trnsformtion formul n be expressed s,

3 t t. γ γ or, (0) ime rnsformtion using Gmm Lstly, it ws gien in the millennium pper, he Lws of Aelertion 5, tht the orret formul for onstnt elertion is, t () Millennium heory Formul for Constnt Aelertion where is the onstnt rte of elertion required to reh speed (i.e., trnsition from the SF to UF frme moing t speed ) during the UF frme time interl t tht trnspires during the SF time interl. his formul is ompletely onsistent with the epted priniples of reltiity in tht it ssoites the onstnt rte of elertion with the elertion frme where it belongs, while the gien time interl is orretly ssoited with the inertil frme tht mthes the speed of the elerting objet t ny instnt in time. In the ltter regrd, interl t is the time interl tht trnspires in eh of these instntneously trnsitioned through inertil frmes during the period of elertion, nd ordingly tkes on the lue of the finl frme trnsitioned to when the elertion is disontinued. (o find the time interl tht trnspires in the elertion frme, refer to the millennium reltiity pper on motion perspetie 6.) We re now redy to derie the elertion distne formul using the onstnt rte of elertion,. By substituting the right side of the finl form of eqution (0) for the rible, t in eqution () we derie, γ () Alternte Formul for Constnt Aelertion n lternte form of the formul for. We n then substitute the right side of this just deried formul for the rible in the Newtonin formul (8) to rrie t, γ whereupon finl modifition to the onstnt ½ gies us, + γ γ whih is orret reltiisti formul for the SF distne treled during the elertion. his formul is then simplified to gie, + γ γ γ + γ

4 + γ γ nd, γ + γ (3) Aelertion Distne using Gmm s the finl ersion still ontining the gmm rible. Substituting the right side of eqution (6) for gmm in the boe formul then gies, + whih n be simplified further to obtin, + nd finlly, + (4) Reltiisti Formul for SF Distne from Constnt Aelertion whih is the millennium reltiity formul for distnes treled during onstnt elertion first introdued in the reltiisti motion perspetie pper 7. With regrd to lidity, een more onining thn the onsistent mnner in whih this formul is deried is the ft tht the formul itself forms n integrl prt of the kineti energy formul. hus, it n lterntely be deried from, or onersely be used to derie, the kineti energy formul. Speifilly, where p is reltiisti momentum, it ws shown in the millennium pper on motion perspetie tht the below formul, k pd (5) Alternte Form of the Reltiisti Kineti Energy Formul is lso orret formul for reltiisti kineti energy. Also, s ws preiously shown in the millennium ppers on energy 8, the following formul, p m (6) Formul for Reltiisti Momentum is orret formul for reltiisti momentum, nd gies identil results to the speil reltiity formul for momentum. It ws then lter shown in the preiously mentioned millennium pper on motion perspetie, tht the right side of this formul long with the right side of distne formul (4) n be substituted into the just gien formul for kineti energy to rrie t,

5 m k + tht when simplified gies, k m ( + ) nd finlly, k m + (3) Reltiisti Formul for Kineti Energy whih is, of ourse, the formul initilly gien for reltiisti kineti energy. In iew of the ft tht the kineti energy formul hs lredy been orroborted, in ddition to the fts tht the distne formul is deried in onsistent mnner, nd is in turn n integrl prt of the kineti energy formul, there n be little doubt tht the distne formul is lid formul for the distnes treled by n objet under onstnt elertion. Gien the foregoing nlyses nd ll of the demonstrted reltionships of the distne formul to the kineti energy formul, it is resonble to onlude tht gin there is no onflit with the stndrd model. hus, it is limed tht the distne formul is lid een within the frmework of speil reltiity. Yet, s will be shown next, when the distne formul is used in the subsequent derition of n elertion omposition formul, it n be seen tht Einstein s eloity omposition formul tully inoles elertion, nd not uniform motion s speified in his theory. (hese findings re oered in detil in the most reent pper of the millennium theory, titled, Millennium Reltiity Aelertion Composition 9.) Assume now tht there re two different objets elerting wy from sttionry frme of referene in extly the sme diretion nd during the sme SF time interl. Further, ssume tht the rtes of elertion re onstnt, nd one of the rtes is greter thn the other. In suh se the SF distne treled by the fster elerting objet n be represented diretly by eqution (4), + (4) SF Distne reled by Fster Aelerting Objet where is the SF distne, nd is the hieed speed during SF time interl. he SF distne treled by the slower elerting objet n then be represented by the modified eqution, + (7) SF Distne reled by Slower Aelerting Objet where is shorter distne thn, nd hieed speed is slower speed thn speed. If we now wish to determine the speed of the fster moing objet reltie to the slower moing objet for ny instnt in time, we must first determine the distne between the two objets t tht sme instnt. o omplish this, we n gin modify eqution (4), but this time using terms tht re lid for the inertil frme in whih the reltie speed between the two objets is lid, nmely, the frme trnsitioned to by the slower objet t tht instnt. hus, we obtin, D + t (8) Equilent SF Distne reled by hird Interepting Objet where is the distne between the two objets expressed in terms of third objet tht trels the sme

6 distne during time interl. It is importnt to understnd tht speed is the intereption speed of this third objet, (its speed when it interepts the seond objet) nd not the speed of the seond objet reltie to the first. (his, of ourse mens it is higher speed thn tht of the seond objet reltie to the first.) o find the speed of the seond objet reltie to the first objet we must use the eloity omposition formul s will be explined lter in the nlysis. hus, in the boe formul, is the speed of the third objet reltie to the first t the instnt the seond objet is interepted, nd time interl t is the time tht trnspires in inertil frme during SF time interl s gien by the formul, t. (9) ime rnsformtion for Inertil Frme Wheres distne is lid distne in inertil frme, it is importnt to understnd tht it is lso lid distne in the sttionry frme. Although the tul distne remins unhnged in both frmes, beuse of the differene in time, this sme distne represents omprtiely smller distne in the SF thn it does in the frme. Sine distne is lid distne in the SF, we n express the reltionship between ll of the distnes by the formul, D D + D (0) Reltionship of to nd where distne, treled by the fster elerting objet reltie to the SF during time interl, is the sum of the two smller distnes, nd. We re now redy to derie the millennium theory formul for elertion omposition inoling the instntneous speeds,,, nd tht re hieed during SF time interl. By tking distne formul (4), + (4) SF Distne reled by Fster Aelerting Objet nd soling for, we obtin, D + D () Formul for Instntneous Speed where is the speed hieed during SF time interl by the fster of the two elerting objets. If we now substitute the right side of distne eqution (0) for in the boe eqution for speed, we obtin, + ( D + D ) ( D + D ) () Formul for Speed using nd where speed is dependent on distnes, nd. We n then substitute the right sides of distne equtions, (7) nd (8) for nd respetiely, in the just deried eqution to rrie t,

7 + + + t + + t + + (3) Aelertion Composition (Speed) whih is the millennium reltiity formul for elertion omposition 0 bsed on instntneous speeds,,, nd. Before going on to show tht Einstein s formul gies essentilly the sme results s the just deried millennium formul, it will be useful to first reiew the derition of the orret formul for eloity omposition. 3. Veloity Composition for Uniform Motion Speeds In similr mnner to the wy distnes were used to derie the orret formul for elertion omposition, they my lso be used to derie the orret formul for eloity omposition of uniform motion speeds. here re, howeer, two notieble differenes between the two different deritions. With regrd to the first differene, in the se of elertion, the effets of trnsitioning between referene frmes must be tken into onsidertion. herefore, een the Newtonin formuls for distnes diretly relted to the SF, (i.e. nd ) hd to be modified to ount for suh effets. his is not true for the se inoling uniform motion distnes. In ft, sine the trnsitioning effets he lredy been ounted for in the elertion formuls, to ount for them gin in the uniform motion formuls would tully mount to ounting for the sme effets twie. In plin words, when working with uniform motion speeds, it is understood tht the speeds resulted from pst elertions during whih the reltiisti effets of time trnsformtion he lredy been ounted for. hese effets re the ery reson tht more energy is require to hiee the speeds rehed thn n be ounted for by Newtonin priniples lone nd re diretly relted to the slower time in moing frme of referene. hus, our only onern fter suh elertion hs ourred is to be sure to use time interls tht re pproprite for the inertil frme being referened. In tht regrd the SF, time interls re gin represented by the rible,, while for the UF s u nd u, the orresponding time interls, bsed on time trnsformtion, re represented by the ribles t u nd t u respetiely. Aordingly, in the se of the sttionry frme, the distne treled by the fster of two uniform motion objets n be expressed by the formul, D u u (4) SF Distne reled by Fster Uniform Motion Objet where D u is the SF distne, u is the speed reltie to the SF, nd is the SF time interl. he distne treled by the slower of the two objets n then be expressed by modified form of formul (4) to gie, D u u (5) SF Distne reled by Slower Uniform Motion Objet where D u is the SF distne, u is the speed reltie to the SF, nd gin is the SF time interl. he seond differene in methods of derition, mentioned erlier, inoles the speed of the seond objet reltie to the first. Unlike the se inoling elertion, in the se of uniform motion we n diretly determine the speed of the fster objet reltie to the slower objet t the end of ny time interl by simply expressing the distne treled by the fster objet reltie to the slower objet in terms tht re lid for the inertil frme in whih the speed is referened. In this se, it is UF u whih is where the slower objet lwys resides. hus, formul (4) n be modified gin to gie, D u t u u (6) SF Distne reled by Fster Objet Reltie to Slower Objet where D u is the UF u distne treled t speed u during UF u time interl, t u. Similr to the se with elertion, time interl t u is the time tht trnspires in inertil frme u during SF time interl s gien by the formul,

8 t u u. (7) ime rnsformtion for Inertil Frme u And, gin similr to the se inoling elertion, wheres distne D u is lid distne in inertil frme u, it is importnt to understnd tht it is lso lid distne in the sttionry frme. As stted preiously, lthough the tul distne remins unhnged in both frmes, beuse of the differene in time, this sme distne represents omprtiely smller distne in the SF thn it does in the u frme. Sine distne D u is lid distne in the SF, we n express the reltionship between ll of the distnes by the formul, D D + D u u u (8) Reltionship of D u to D u nd D u where distne D u, treled by the fster uniform motion objet reltie to the SF during time interl, is the sum of the two smller distnes, D u nd D u. We re now redy to derie the millennium theory formul for eloity omposition inoling the uniform motion speeds, u, u, nd u tht re hieed during SF time interl. By substituting the right sides of equtions, (4, 5, nd 6) for the ribles, D u, D u, nd D u respetiely in formul (8), we derie, u u + u t u (9) Reltionship of Uniform Motion Distnes in erms of Speeds nd imes giing the reltionships of the uniform motion distnes in terms of speeds oer time interls. We n then substitute the right side of eqution (7) for the rible t u in the just rried t eqution to derie, u u + u u whih redues to, u u + u u () Millennium Reltiity Veloity Composition whih is, of ourse, the millennium formul for eloity omposition originlly gien t the beginning of this pper. 4. Diret Comprisons of the Composition Formuls o permit diret omprisons of both, this formul, nd Einstein s formul for eloity omposition, not only to eh other, but to the millennium formul for elertion omposition, we need only to exhnge the ribles, u, u, nd u in both formuls for the ribles,,, nd respetiely tht re used in the elertion formul. his gie us, + + (30) Speil Reltiity Veloity Composition nd, + (3) Millennium Reltiity Veloity Composition

9 for whih the results n be ompred diretly to eh other, nd lso to the results obtined using the millennium elertion formul (3). o deelop omprison grph onsistent with the methods used to generte the Dt bles for the elertion omposition pper where it ws first disoered tht Einstein s formul inoles elertion, nd not uniform motion, we need two dditionl formuls. hese re the formuls needed to determine speeds nd from the ssigned elertion rtes nd time interls. By tking eqution () nd modifying it to gie elertion rtes, nd, we obtin, t (3) nd t (33) respetiely. hen, by tking the right side of eqution (9) nd substituting it for the rible t in eqution (3) we obtin, whih when soled for, gies, + ( ) (34) Formul for Instntneous Speed whih is the formul for instntneous speeds first introdued s eqution (6) in the ime nd Energy pper. If we gin tke eqution (9) nd modify it to gie time interl t, we obtin, t t (35) ime rnsformtion for UF whih is the time trnsformtion formul for UF first introdued in the eloity omposition pper (p 3). By tking the right side of this eqution, nd substituting it for the rible t in eqution (33), we obtin, t whih when soled for, gies, + t t ( ) (36) Formul for Instntneous Speed whih is the formul for instntneous speed, first introdued in the elertion omposition pper (p 44, Addendum A). We now he ll of the formuls used to generte the dt for the grph shown in Figure. Using the lues, m/s, g m/s,,000,000 s/interl, g, nd.5g, first the lue for ws obtined using eqution (34). hen, eqution (9) ws used to determine the orresponding time interl t for eh SF time interl. Instntneous speed ws then determined using eqution (36), nd finlly, using the lues obtined for speeds nd, equtions (3, 3, nd 30) were used to generte the lues for

10 V u Rybzyk, V Rybzyk, nd V u Einstein respetiely..4 Comprison of Formuls Speed in frtions of u R u E R Vu Rybzyk V Rybzyk Vu Einstein V V 0 ime Interls (eh diision equls,000,000 seonds) FIGURE Formul Comprison Grph In the interest of ury, the dt used to generte the grph in Figure were lso inputted into the Mthd model used to generte the bles gien in the elertion omposition work. he results of the Mthd model were identil to those shown in the grph of Figure. Referring now to Figure, it n be redily seen tht Einstein s eloity omposition formul produes results tht ery losely pproximte those of the millennium reltiity elertion omposition formul. On lose inspetion, it will be notied tht initilly when the lue of rises boe the lue of, Einstein s u drops ery slightly below Rybzyk s. hen, when the lue of rises to equl, Einstein s u is indistinguishble from Rybzyk s, nd finlly, when the lue of rises boe the lue of, Einstein s u rises ery slightly boe the lue of Rybzyk s. his behior ws first identified in the millennium pper on elertion omposition. Of importne here, is the ft tht Einstein s formul losely trks the millennium formul for elertion omposition, nd not the millennium formul for eloity omposition. Also of importne here, is the ft tht the results shown for the millennium reltiity eloity omposition formul (V u Rybzyk) re inlid, not beuse the formul is wrong, but beuse the inputs re inlid for this purpose. ht is, this formul, long with Einstein s formul for eloity omposition re inorretly used to tret instntneous speeds s though they re uniform motion speeds. Stted more preisely, the inputs re inorret for the millennium formul, nd unintended for Einstein s formul. If the orret inputs re proided to both of these formuls, the millennium formul will produe results tht re orret for eloity omposition nd in omplete greement with those shown for elertion omposition, while Einstein s formul will proide results tht re inlid for this intended pplition. he problem, s will be demonstrted next, enters on the lue of speed,. In plin words, speed nnot be lid, instntneous speed nd uniform motion speed t the sme time. Quite obiously, n objet tht trels t uniform rte of speed during gien time interl, will trel greter distne thn nother objet tht elertes from speed of 0 to tht sme speed during the sme time interl. Conersely, uniform motion speed used to trel the sme distne, during the sme time interl, s

11 n elerting objet will be lower speed thn the finl speed rehed by the elerting objet during tht time interl. o orretly ompre Einstein s formul to the millennium formul for eloity omposition in their intended pplition we need only to go bk to our originl exmple nd onsider wht would hppen if the elertions were disontinued t ny instnt. Sine the instntneous speeds,, nd rehed during tht time interl re in referene to the SF, the objets would ontinue t these speeds t uniform rte of motion reltie to the SF. hus, it is lid to used these sme speeds s either instntneous speeds, or uniform motion speeds reltie to the SF of referene. For the resons preiously gien, howeer, this is not true of instntneous speed, reltie to UF,. ht is, the uniform rte of speed of the fster objet to the slower objet must be lower speed thn speed. o determine wht the true uniform rte of speed would be, we need only to sole the millennium reltiity eloity omposition formul for speed. hen the resulting lternte form of the formul n be used to sole for the uniform motion speed between the two objets. (Einstein s formul nnot be used for this purpose sine it hs lredy been proen tht it is irtully orret for instntneous speeds, nd not uniform motion speeds.) hus, tking formul (3) nd soling for we obtin, u ( ) (37) Millennium Veloity Composition Formul for V u where the rible hs been relbeled, u to distinguish it from its originl use. (his formul ws originlly introdued s formul (57) in the elertion omposition pper.) Obiously, if this rible is subsequently substituted for the rible, in the millennium formul for eloity omposition (Formul (3)) the millennium formul will produe the sme result for tht ws preiously produed by the millennium formul for elertion omposition. Eqully obious is the ft tht if this rible is substituted into Einstein s formul in similr mnner, Einstein s formul will no longer produe the sme result for tht it preiously produed. his is bsolute proof tht Einstein s formul nnot be orret for its intended pplition inoling uniform motion, sine we lredy know wht the lue of must be. Referring now to Figure, grph is presented tht shows the results of the millennium formul for eloity omposition ompred with the results for Einstein s formul for eloity omposition using the results for u in ple of the results for for the entire rnge of input lues used in the originl exmple.

12 As n be seen, the ure gien for the millennium eloity omposition formul, designted u Rybzyk, is identil to the ure originlly obtined for the elertion formul, designted Rybzyk, in the grph of Figure. Also, s n be seen, the results for Einstein s formul, designted u Einstein, re fr lower now thn preiously gien, nd no longer return the orret lue for the speed of the fster moing objet. Of seondry interest is the ft tht the ure for is lso unhnged from wht it ws in the grph of figure. In short, the speeds of the two objets reltie to the SF re unhnged, s they should be, nd only the reltie speed between the objets hs been ffeted, nd in the mnner expeted. ht is, uniform speed u is lower speed thn instntneous speed. Of gret importne here is the ft tht speed u, s determined by formul (37), orretly represents the speed of the fster elerting objet reltie to the slower elerting objet for ny instnt in time. o understnd why this is so, we need only to onsider the following: During ny instnt in time, (e.g. t the end of ny time interl ) the elertions of the two objets n be disontinued. At tht instnt, their instntneous speeds beome uniform motion speeds. hus, for ny instnt in time, speeds nd n be treted s either instntneous speeds, or uniform motion speeds. With tht being the se, formul (37) is lid formul for determining the speed of the fster objet reltie to the slower objet t tht sme instnt. his onlusion, is onsistent not only with ll of the millennium priniples deeloped to dte, but lso with the eidene tht supports suh priniples. Perhps the only other importnt point of interest is tht inoling the results for Einstein s formul for speeds tht re smll frtion of light-speed. As n be seen in the grph of Figure, s the speeds drop below., the ure from Einstein s formul merges with the orret ure gien by the millennium formul. his would pper to indite tht it ould be somewht diffiult to determine tht Einstein s formul is inorret

13 through experiments onduted in these lower rnges of speeds. On the other hnd, the ft tht Einstein s formul losely pproximtes the orret lues for instntneous speeds ould present itself s soure of onfusion inoling een those experiments in the higher speed rnges. With ll of this in mind nd tking into onsidertion the gret diffiulty the uthor experiened in the mthemtil nlysis inoling eloity omposition, it is no wonder tht it took so long to unoer this disrepny in Einstein s theory. 5. Conlusion he eidene presented in this pper proides oerwhelming proof tht Einstein s eloity omposition formul is inlid for it intended purpose inoling uniform motion. Quite lerly, Einstein s formul inoles elertion omposition, nd s demonstrted in this pper, is not entirely urte in tht pplition either. Moreoer, in iew of wht ws shown, nd if reltiisti priniples re indeed lid, then only the millennium reltiity formuls for elertion omposition, nd eloity omposition pper to be orret for eh of these respetie pplitions. he only still remining unresoled issue in regrd to this mtter is tht inoling eptne of this eidene by the sientifi ommunity. As the uthor hs stted in the pst, this eidene will not go wy. Let it lso be understood tht the uthor is not requesting suh orrobortion in order to see if the presented eidene is orret. he uthor knows it is orret. Perhps the sientifi ommunity needs to be reminded of its responsibility to soiety. If Einstein s theory is wrong, the tx pying publi who ultimtely funds most of the reserh tht is onduted in the U.S. hs right to know bout it. And wht bout our hildren nd grndhildren in the uniersities? Are we going to, for politil resons, or out of just plin stubbornness, ontinue tehing them something tht we know is wrong? How does this benefit the dnement of siene in the U.S., nd wht does this portend for Ameri s future position in the highly ompetitie world of siene? REFERENCES Joseph A. Rybzyk, Millennium Reltiity Veloity Composition, Unpublished Work, 00 Joseph A. Rybzyk, ime nd Energy, Unpublished Work, 00; ime nd Energy, Inertil nd Grity, Unpublished Work, 00; Reltiisti Motion Perspetie, Out of ourtesy, sine permission hs not been grnted, the physiist s identity will not be mde publi. he physiist s identity ws gien by the uthor to offiils of the Ntionl Siene Foundtion, howeer, in reltionship to reent proposl by the uthor. 4 Joseph A. Rybzyk, Millennium heory of Reltiity, Unpublished Work, 00 5 Joseph A. Rybzyk, he Lws of Aelertion, Unpublished Work, 00 6 Joseph A. Rybzyk, Reltiisti Motion Perspetie, Unpublished Work, Originlly introdued s formul (6) in the boe referened work, Reltiisti Motion Perspetie. 8 Joseph A. Rybzyk, ime nd Energy, Unpublished Work, 00; ime nd Energy, Inertil nd Grity, Unpublished Work, 00 9 Joseph A. Rybzyk, Millennium Reltiity Aelertion Composition, Unpublished Work, Originlly introdued s formul (35) in the boe referened work, Millennium Reltiity Aelertion Composition. Note: he boe referened works re ll ilble t the Millennium Reltiity Web Site t: Notie: his work is proteted under U.S. nd Interntionl Copyright Lws

14 Einstein s Veloity Composition Proen Wrong he Complete Proof Copyright 003 Joseph A. Rybzyk All rights resered inluding the right of reprodution in whole or in prt in ny form without permission