Think of the Relationship Between Time and Space Again

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1 Repor nd Opinion, 1(3),009 hp://wwwsciencepubne Think of he Relionship Beween Time nd Spce Agin Yng F-cheng Compny of Ruid Cenre in Xinjing 15 Hongxing Sree, Klmyi, Xingjing , CHINA e-mil: ABSTRACT In his pper, he uhor pus forwrd mhemicl model, his model cn give cler relionship beween ime nd spce The uhors pu forwrd from he objecive reliy, he new ides nd mhemicl formul, le people know long he correc rod of lw reflecs reliy [Repor nd Opinion 009;(3): 58-63](ISSN: ) Key words: ligh sphericl, wve-fron, insnneous spce-ime, rnsmission ime 1 INTRODUCTION Time his concep hs been Newonin in Philosophic Nurlis Principle Mhemicl in Time clock is used for mesuring rel ime of kind of insrumen (iming is used o mesure ime clock of n insrumen) Auhors ssume wo reference frme S nd S in reference frme S (excep he source poin) hve rbirry spil poin ligh P, when he movemen of he reference frme S coincides wih sic sysem S compleely momens, poin P o lunch flsh In ech of he origin of he observer nd iming srs, ech frme of reference in differen ime o receive pulse respecively The uhor fer creful considerion, nd ry o esblish new relionship beween ime nd spce RELATIONSHIP BETWEEN TIME AND SPACE In he ps hs pu forwrd he heory of he ligh- speed invrince, he speed nd no sy invribiliy of he phoon wih ny reference poin I refers o he mening iself : From he poin ligh shining pulse, he flsh o spred round he geomery is sphere The sphericl surfce in he vcuum diffusion speed remin unchnged We obined he sphericl equion h ech reference frme 1 Using Algebric Equions is Obined As Fig1 shown, uhors ssume wo reference frme S nd S long he X -xil movemen speed reference frme S for V moves from poin J o A nd presenly coincides wih he reference frme S compleely A his momen, from he ligh-source poin P shining pulse, in heir respecive reference frme origin he observer iming srs, he flsh o spred round he geomery is sphere Poin P is lwys he cener of sphericl rry, bll sphericl surfce(or wve-fron)spred o he source of reference frme S, poin O Timer vlues for reding The spce locion in reference frme S poin P for (x, y, z), insn spce-ime s (x, y, z, ) In ime T 0 o T, pulse propgion disnce is he rdius of he bll[1] According o he Pyhgoren heorem we obin sphericl equion in he reference frme S : x + y + z (c) (1) Move long he X -xis reference frme S, sphericl surfce coninued o spred in, he bll on he pursui of diffusion in fce of reference frme S observer A his momen, in reference frme S o red he clock is he spce locion in reference frme S poin P for (x y z ), insn spce-ime s x y z Figure 1 in nlysis, 58

2 Repor nd Opinion, 1(3),009 hp://wwwsciencepubne obviously, Ligh sphericl diffusion speed relive o he cener from poin of origin for finding C Due o he poin P is fixed in he reference frme S i is relive o he movemen of reference frme S vry wih ime So, insn spce-ime s x y z In ime T 0 o T, pulse propgion disnce is he rdius of he bll According o he Pyhgoren heorem we obin sphericl equion in he reference frme S : x + y + z ( c) () The x -shf nd X xle lod, reference frme S long he X -xis movemen, round he X- xis roion does no Th is, y y, z z y y, z z, x x-v Will formul (1) nd () join soluion formul we hve : y + z ( c) x, ( ) + [( c) x ] ( c) 0 x ( x V ) + [( c) x ] ( c) 0, ( c )( ) + Vx ( c) 0 Decomposiion of he unry qudric equions (1 ) + (Vx ) 0 V V (3) In order o fcilie he process wih V / C Tke equion is roo, we mus : (4) (1 ) + x x 1 Fig1 The reference frme S sphericl equion is Eq(1) The reference frme S sphericl equion is Eq() Derived Using he Geomeric Equions The x -shf nd X xle lod [] nd y -xis prllel xis wih y, z -xis prllel xis wih z Therefore, poin P on reference frme, S nd S, y y, z z In he equion (1), sy flsh signl rnsmission ime vlue, from poin P o O In he equion (), sy flsh signl rnsmission ime vlue, from poin P o O Obviously, in Fig1, Is he 59

3 Repor nd Opinion, 1(3),009 hp://wwwsciencepubne signl propgion dely effec [3] In noher wy, he sme resuls When he movemen of he reference frme S coincides wih sic sysem S momen Compleely A flsh poin P, ligh blls for reference frme S in pursui of he movemen Figure 1 of righ ringle: righ ringle PKO in PKO plne pk + ko po pk + ko po b Type (b) minus () is po po ko ko ko x V ko x, po c nd po c generion of he soring ge ( x V c ) + [( c) x ] ( ) In order o ge on he sme fer he equion ( x V ) + [( c) x ] ( c ) In Fig1, if he negive direcion long he X xis reference frme S movemen, resuls wih he sme formul (3) From he perspecive of geomery discuss he dvnges of: Along he X- xis movemen, reference frme S round he X xis roion my, don ssume y y z z h is y y z z If he vrible is long he X xis reference frme S movemen known s reference frme S speed chnging wih ime, he funcion h cn use he definie inegrl o nswer [4] 3 DISCUSS AND REVIEW Ligh source poin P is hypohesis in he y- xis, by equion (4) h sme ime dilion nd Einsein formul Ligh source poin P is hypohesis in he X xis, ssume he ligh source is on he X xis, wo kinds of circumsnces, is in he posiive direcion of he X xis nd he opposiion upwrd, we hve series of formuls 31 Ligh Source Poin P In y - z Plne Use he formul (3) nd Fig1 nlysis: will be ligh source poin P moves o (y z ) plne, in he formul (3), x 0, we obin : (5) This formul is similr wih Einsein ype Fig Ligh source poin P in y - z plne Y nd z he sme ime is no zero 60

4 Repor nd Opinion, 1(3),009 hp://wwwsciencepubne 3 Ligh Source Poin In he X- xis Will ligh source poin P moves o he X- xis, h is in Fig1 X- xis of negive direcion, x 0, x 0 y 0, z 0, hen we hve: c x, x Subsiue hese vlues ino formul (4) obined : x x 1 ± x V x 1, (6) If he ligh source poin P is moving o he X-xis direcion, x > 0 x V (1 ) c c x 1 (1 )(1 + ) c + V (7) Poin P on he X xis of he opposiion, x < 0 x V (1 + ) c c x (1 )(1 + ) c V (8) 33 The Relionship Beween Moving Phoonic nd Reference Frme Assuming he X xis symmeric poin O on wo poin ligh source of P 1 nd P, s Fig3 shown When he movemen of he reference frme S coincides wih sic sysems S compleely momens, wo poin ligh lso issued flsh ligh, reference frme S o wo poin ligh source of P 1 nd P, clock wih 1 respecively According o he formul (7) nd (8) vilble Reference frme S movemen owrd he ligh source poin : c+ V x/ 1 Th is U 1 c + V x/ 1 (9) Reference frme S movemen wy from ligh poin : c V x/ Th is c x/ U V (10) Anlysis he formul (9) nd (10) Source: P is in reference frme S on he movemen direcion, h sid, ineril sysems S is long he phoon rjecory line movemen Therefore, he phoons movemen speed by Glileo rnsformion (relive reference frme S ) From he formul (9) nd (10), movemen speed of reference frme S for ny vlue 61

5 Repor nd Opinion, 1(3),009 hp://wwwsciencepubne Fig3 Along he X- xis movemen reference frme S, ligh source poin is fixed on he X -xis 4 UNDER THE LIGHT OF THE RELATIONSHIP BETWEEN TIME AND SPACE MOVEMENT In lile ligh in reference frme, relive o heir source of phoon speed isoropic for C As Fig4 shown, source: P is sphericl of cener, bu he relive o heir reference frme ouside he ineril sysem is nisoropic When long he X-xis movemen sysems S nd sillness reference frme S compleely coincidence momens, send flsh poin P In heir respecive reference frme origin he observer iming srs, when he ineri ligh poin P speed is V O V C movemen o poin E, bll sphericl surfce or wve-form spred o he source of reference frme S poin O, imer vlues for reding The spce locion in reference frme S poin P for [ X+V, y, z ], insn spce-ime s [ X+V, y, z, ] From poin A o B disnce is V According o he Pyhgoren heorem we obin sphericl surfce equion in he reference frme S : + y + z ( c ), x (11) Ligh sphericl coninued o spred, in he momen, sphericl surfce diffuse o poin A ble Ineril sysem poin P wih sic reference frme S poin G of superposiion, he ime, in he reference frme S poin P spce-ime is he cener of he bll in According o he Pyhgoren heorem we obin (1) ( x V c + ) + y + z ( ), Suppose y y, z z, y y, z z nd V /c combined he formul (11) wih he formul (1) o form simulneous equions nd o solve his equions We obined, he one-elemen qudric equion of n unknown number : (13) (1 V ) (Vx ) 0 We chose he posiive roo of such qudric equion s follows: 6

6 Repor nd Opinion, 1(3),009 hp://wwwsciencepubne (1 ) + x 1 + x (14) If we like his "discussion nd reviews" nlyicl formul 14 will ge he sme resul wih In Fig4, if he negive direcion long he X xis reference frme S movemen, resuls wih he sme formul (13) If he vrible is long he X xis reference frme S movemen known s reference frme S speed chnging wih ime, he funcion h cn use he definie inegrl o nswer [4,5] + ) + y + z ( x V ( c) x + y + z ( c ) Fig4 The reference frme sphericl equion is Eq(11) The reference frme S sphericl equion is Eq(1) 5 CONCLUSION The speed of ligh sphericl diffusion invrin In he vcuum, ligh sphericl diffusion speed relive o he cener from poin of origin for finding C The chnge of phoonic speed Ineril sysem is long he phoon rjecory line movemen, he speed of phoon nd ineril sysem se closely reled Therefore, he phoons movemen speed by Glileo rnsformion ( relively ll ineril sysem ) REFERENCES [1] Zhng Chong An Mer Regulriy 003, P07, 003 [] Yng F Cheng Mer Regulriy 003, P91, Journl of Xinjing Peroleum Educion College, 001, issue 4, P51 [3] C Kiel e l Berkeley Physies Course, Vol1, Science Press, 1979 [4] Xu Sho Zhi, The Mhemicl Fundion of he Specil Theory of Reliviy is Wrong, Invenion nd Innovion, 001(1) [5] Yng F Cheng, A New Mhemicl Model o Replce he Lorenz Trnsformion, he New probe of spce-ime Theory, A chief Edior, Ho Jin Yu, Beijing, Geology Press,005 4/15/009 63