New perspectives on the classical theory of motion, interaction and geometry of space-time

Size: px
Start display at page:

Download "New perspectives on the classical theory of motion, interaction and geometry of space-time"

Transcription

1 Nw prspvs on h lassal hory of moon, nraon an gomry of spa-m. R. Hajsfanar Dparmn of Mhanal an rospa Engnrng Sa Unvrsy of Nw York a Buffalo Buffalo, NY 46 US ah@buffalo.u bsra By xamnng h hory of rlavy, as orgnally propos by Lornz, Ponar an Ensn, a funamnal hory of gnral moon s vlop. From hs, h rlaonshp bwn spa-m an mar s sovr. s a rsul, h gomral hory of nraon s nrou. h orrsponng gomral hory of lroynams rsolvs h orgn of lromagn nraon, as a vorx-lk fl, an larfs som of h xsng ambgus.. Inrouon Ponar s hory of rlavy xplans h physal manng of h Lornz ransformaon among nral sysms by unfaon of spa-m. lhough shows a rlaonshp bwn pur Lornz ransformaon an hyprbol roaon, os no spfy wha s roang. hs s h orgn of mos roubls n h hory of rlavy an lroynams. For xampl, alhough h Maxwllan hory of lroynams s h mos unrsoo among h hors of funamnal fors, h lromagn nraon, all h Lornz for, s no a r onsqun of Maxwll s quaons. I has o b posula n an npnn mannr, whh s h manfs of nomplnss

2 of h hory. lhough has bn no ha h lromagn fl srngh nsor an Lornz for ar boh a naural onsqun of h gomr sruur of Mnkowskan spa-m, s funamnal manng has no bn sovr. nohr roubl s h magn monopol whos xsn s apparnly ompabl wh fully symmrz Maxwll s quaons. I sms only mofaon of Maxwll s quaons suff o allow magn hargs n lroynams. Howvr, no magn monopol has bn foun o hs a. o rsolv hs an ohr ffuls, w vlop a funamnal gomral hory of moon an nraon, whh shows ha h Lornz for an Maxwll s quaons ar smpl gomral rlaons bas on four-mnsonal roaon. I s sn ha hs gomry s non-eulan wh nrsng onsquns. hs hory larfs h rlavy of spa-m an s rlaonshp wh mar. I also rvvs h a of h lromagn fl as vorx moon n a unvrsal ny. In h followng son, w frs prsn h hory of rlav nral sysms an knmas of parls n h framwork of Ponar s rlavy. Subsqunly, n Son 3, w vlop h onssn hory of movng parls by xplorng h rlaon bwn mass an spa-m. hs rsolvs h roubls n Ponar s rlavy by larfyng h orgn of h govrnng non-eulan gomry. frwars, n Son 4, w vlop h gomral hory of funamnal nraon, whh shows ha a Lornz-lk for as a roaonal ff s an ssnal harar of vry funamnal nraon. hrfor, vry funamnal nraon s spf by a four-mnsonal vorx-lk fl. Inrsngly, hs mans a unfaon of all fors bas on h gomral hory of moon an nraon. In son 5, w monsra all h als of hs vorx hory for lromagn nraon. hrfor, lroynams s ompl wh lr hargs an magn monopols o no xs. h gomral vw also larfs h spn ynams of harg lmnary parls. h n, s sn ha h orrsponng onssn hory of gravy s a gnralz

3 Nwonan gravy. hs analogous Maxwllan hory of gravy s also vlop n al n Son 6. summary an gnral onluson s prsn n Son 7.. Ponar s hory of rlav nral sysms s an nral rfrn fram n h Mnkowskan spa-m, a four-mnsonal oorna sysm x x x3x4 s onsr suh ha x xx3 s h usual spa an x 4 h axs masurng m wh magnary valus, suh ha four-vor bass (,,, ) (,,, ) x 4. By onsrng h un (.) 3 4 (,,,) (,,, ) h spa-m poson four-vor an b rprsn by Howvr, for smply w somms wr or vn an also ofn us x n pla of x. x x (.) (, ) ( x, y, z, ) x ( x, x 4) x (.3) x ( x, x4) (.4) Wh hs onvnn lmnary noaon, w o no n o us ovaran an onravaran forms of four-nsors n mr noaons. Imporanly, s sn ha h non-eulan gomry govrnng moon an nraon s muh larr n hs omplx numbr noaon. Howvr, all vlop hory an b asly prsn n any ohr noaon. h squar lngh of poson four-vor s x x x x x x x x + y + z (.5) 3

4 whr w no ha h sam symbol x also rprsns h marx form of x. homognous Lornz ransformaon x Λ x (.6) s any ransformaon whh lavs h lngh of h four-vors nvaran x x x x (.7) hs rqurs x x Λ Λ x x (.8) α β α β whh las o h followng orhogonaly onon on Λ Λ Λ δ (.9) α β αβ s wll b sn, w us only frs an son orr hr an four-mnsonal nsors. hrfor, for onvnn w us h marx rprsnaon for hs nsors wh h sam symbol. Bas on hs onvnon, (.9) an b wrn n mor ompa form Λ Λ (.) hs shows ha h Lornz ransformaon s an orhogonal ransformaon n h spf four mnsonal spa-m. Convrsly, any ransformaon, whh sasfs hs orhogonal onon, s a Lornz ransformaon. ll of hs ransformaons form a group n h mahmaal sns. Wha w hav s h rlaon bwn oornas of a pon or vn n wo ffrn four-mnsonal oorna sysms x x x3x4 an x x x 3x 4. On xps ha unrsanng h manng of hs rlaon s rual n vlopng a hory of spa-m an moon. 4

5 .. Spa roaon famlar xampl of a Lornz ransformaon s h rlav spa ornaon of wo oorna sysms wh ommon orgn, whh s spaal roaon. In gnral, for hs ransformaon, w hav Q Λ (.) whr Q s a onsan propr ral orhogonal marx spfyng h spa roaon of h nw rfrn sysm rlav o h orgnal oorna sysm. In hs as, h ransformaon omposs o x Qx (.) s an xampl, for roaon abou h z-axs wh angl φ, w hav osφ snφ Q snφ osφ (.3) In gnral, for roaon abou an arbrary axs no by un vor n wh angl φ, whr φ φn (.4) w hav ) Q δ ε n φ + ( osφ)( n n δ ) j j mj m sn (.5) j j I s onvnn o assoa an an-symmr marx o som axal vor w ( w, w w ) R w fn by w3 w R w w3 w (.6) w w, 3. If G s an arbrary vor, hn w G R G (.7) whh s a rlaon frqunly us n hs arl. hrfor, (.5) an b wrn as w 5

6 ( )( nn ) Q sn φr n + osφ (.8) In rms of lmns Q os nn nn3 φ + ( osφ) n ( ) ( ) nn osφ + n3 snφ nn3 osφ n snφ ( ) ( ) ( ) ( ) ( ) ( ) osφ n3 snφ osφ + osφ n nn3 osφ + n snφ osφ + n snφ n n osφ n snφ osφ + osφ n 3 3 (.9) By usng Cayly-Hamlon horm, an b shown ha Q xp ( ) R φ xp φ3 φ φ φ 3 φ φ xp n3φ nφ n φ 3 n φ nφ n φ (.) Bas on h Eulr horm for h hr-mnsonal moon of a rg boy, vry propr orhogonal marx Q s quvaln o a roaon abou an axs []. hs mans ha h form gvn hr for Q s a gnral form. In pra, h Eulr angls ar wly us o rprsn h roaon marx Q []. I shoul b no ha h rlaons for bas un spa hr-vors ar Q (.) j j j Q (.) wh Q Q QQ (.3) I s obvous ha for h four-mnsonal bas vors w hav j Λ (.4) Λ (.5) I shoul b no ha (,,,) (.6) 4 4 6

7 whh mans h nw m oorna s h sam as h ol on. L h ral orhogonal marx ransformng from x o x b sgna by Q Q x (.7) x an h son orhogonal marx from x o x b Q x Q x (.8) Hn h marx of ompl ransformaon Q from x o x s x Qx (.9) Q Q Q (.3) In gnral h roaons ar no ommuav. In ohr wors, h roaon vors φ φn an φ φn o no follow h Eulan vor summaons. I an b shown ha φ φ φ φ φ os os os sn sn n n (.3) φ φ φ φ φ φ φ sn n sn os n + sn os n + sn sn n n (.3) hs rlaons ar mor onvnnly rv, f a quarnon rprsnaon of roaons or unmoular rprsnaon wh Cayly-Kln paramrs s us []. I s sn ha h summaon of half vor of roaons φ an φ oby h ruls of sphral gomry. h rangl rprsnng hs vors an b onsr as a sphral rangl on a un sphr, wh h angl oppos o llp vor φ gvn by h angl bwn h wo axs of roaon. hrfor, h voral rprsnaon of spaal roaon s govrn by an llp yp of non-eulan gomry. Howvr, for nfnsmal roaons, hs gomry rus o Eulan gomry, whr h nfnsmal roaon vors ommu. 7

8 8.. Boos h ohr mporan form of Lornz ransformaon s a pur Lornz ransformaon or boos spf wh rlav vloy v. h boos paramr or rapy s fn by v anh (.33) h nvrson of hs rlaon gvs ln anh v v v v v v v (.34) h vor rapy also an b onsr as (.35) whr s h un vor n h ron of v. Hr, w mphasz h us of rapy as an ssnal paramr. smpl xampl of a boos s h boos along h x-axs, for whh osh snh snh osh Λ (.36) whh s usually wrn as γ βγ βγ γ Λ (.37) wh v / β an / ) ( β γ, whr γ osh (.38) βγ snh (.39)

9 h sruur of hs ransformaon nsor s rmnsn of a roaon nsor, bu wh hyprbol funons nsa of rular. Inrsngly, w an fn ψ (.4) whr snψ snh (.4) hrfor, h ransformaon marx an b wrn as os ψ osh (.4) osψ snψ Λ (.43) snψ osψ On an ralz hs s a roaon wh magnary angl ψ rprsnng h vaon of plan x x rlav o plan x x 4 4. nalogous o h spaal roaon, h bas fourvors of h nw sysm ar ( osh,,, snh ) (,,, ) (,,, ) 3 (.44) (,,, osh ) 4 snh hrfor, w hav (, ) osh osψ os (, ) snh snψ os 4 (, ) snh snψ os 4 (.45) (, ) osh osψ os 4 4 Rlaons (.45) show ha hs magnary an omplx angls ar ( ) ψ, 9

10 π π, 4 + ψ + ( ) π π 4, + ψ + (.46) ( ) ( ), 4 4 For a gnral boos, whh s no paralll o any of oorna axs, w hav + (osh ) snh Λ (.47) snh osh By usng h Cayly-Hamlon horm, w an show Λ xp + snh xp + ( osh ) (.48) In rms of h lmns w hav + ( osh ) ( osh ) ( osh ) ( osh ) + ( osh ) ( osh ) ( osh ) ( osh ) + ( osh ) 3 snh 3 snh Λ (.49) snh snh snh 3 snh osh hrfor, w xp h bas four-vors of h nw sysm n rms of ol ons o b ( + (osh ), (osh ), (osh ) 3, ) ((osh ), + (osh ), (osh ) 3, ) ((osh ), + (osh ), + (osh ), ) snh snh (.5) snh 4 ( snh, snh, snh 3,osh ) ( snh, osh ) 3

11 I s sn ha h angls among nw an ol axs an b oban asly. For xampl, from w oban (, ) osh os 4 4 (.5) ( ) ψ (.5) 4, 4 hs shows h angl bwn h m axs s spf by rapy, whh s xp..3. Gnral Lornz ransformaons Evry homognous Lornz ransformaon n gnral an b ompos no a pur Lornz ransformaon Λ B (boos) an a spaal roaon Λ R (n hr orr) []. For h as whr a Lornz ransformaon s rprsn as h prou of a boos + (osh ) snh Λ B (.53) snh osh from h ol sysm x x x3x4 o h nrma sysm y y y3 y4, whr y Λ x (.54) follow by a spaal roaon Q Λ R (.55) from y y y3 y4 o h nw sysm x x x 3x 4 B R w hav h oal homognous Lornz ransformaon whh s x Λ y (.56) Λ Λ Λ (.57) R B Q + (osh ) Λ snh Q + (osh ) Q snh snh osh snhq osh (.58)

12 I s obvous h ransformaons Λ R an Λ B ar no gnrally ommuav. hs s baus h vors an φ ar non-eulan an hrfor hr aon os no follow h ruls of Eulan gomry. Now w monsra h mporan propry of a pur Lornz ransformaon or boos whh follows h hyprbol yp of non-eulan gomry. L h pur Lornz ransformaon from x o x b sgna by Λ x (.59) x Λ an a son Lornz ransformaon from x o x b Λ x Λ x (.6) Hn h marx of ompl ransformaon Λ from x o x x Λ x (.6) s Λ Λ Λ (.6) whr Λ + (osh ) snh snh osh + (osh ) snh snh osh (.63) I s sn ha h ompl ransformaon s no n gnral a pur Lornz ransformaon. hs ransformaon s n gnral form (.58), whr osh osh + (.64) osh snh snh hs rsul s h naon of hyprbol gomry govrnng h vloy aon law. hs has bn no an vlop xnsvly by arly nvsgaors of rlavy suh as Varǎk [-4]. I s sn ha hs non-eulan gomry s h orgn of h famous homas-wgnr roaon, whh has bn xplan by Borl [5]. n aoun of hs

13 nvsgaons an b foun n h arl by Walr [6]. On an ralz ha for nfnsmal rapy vors, h hyprbol gomry rus o Eulan gomry, whr h rapy or vloy vors ommu. If h ransformaons Λ an Λ ar gnral Lornz ransformaons, s sn ha Λ Q whr + (osh ) Q snh snhq osh Q osh snh snh + (osh ) Q snh snh Q osh (.65) osh osh + Q (.66) I wll b shown ha hs rlaon an b furhr gnralz o alrang sysms. W an s ha h nral sysms ar orn from ah ohr by a four-mnsonal roaon. h homognous Lornz ransformaon jus spfs hs roaon rlav o a fx nral sysm as rfrn fram. hs ransformaon n gnral an b ompos no a pur Lornz ransformaon (boos) an a spaal roaon. In a gomral vw, h Lornz ransformaon an b spf by a hyprbol vor rprsnng h hyprbol angl assoa wh h boos an an llp vor φ rprsnng h spa angl roaon. h gomry govrnng hs vors s non- Eulan as was monsra. In gnral, h bas un four-vors of wo nral sysms ar rla by Λ (.67) or Λ (.68) hrfor, h angls among hs rons ar suh ha (, ) Λ os (.69) 3

14 (, ) Λ os (.7) I woul b nrsng o prsn a smpl gnral Lornz ransformaon. L hs ransformaon b h prou of a boos n h x-ron follow by a spaal roaon aroun a z-axs osφ snφ osh snh snφ osφ Λ (.7) snh osh whh an b wrn as osφ osh snφ osφ snh snφ osh osφ snφ snh Λ (.7) snh osh h bas un four-vors of h nw sysm ar ( osφ osh, snφ,, osφ snh ) ( snφ osh, osφ,, - snφ snh ) (.73) 3 (,,, ) (,,, osh ) 4 snh I s no ha (, ) osφ osh os (, ) snφ os (.74) (, ) os 3 (, ) osφ snh os 4 I s sn ha hs rlaons ar h rsul of h aon of non-ommuav non- Eulan vors an φ. 4

15 Wha w hav monsra s h vry mporan harar of h s of four-mnsonal sysms wh hr ral oornas an on magnary oorna. I s sn ha hs sysms ar orn from ah ohr, n a mannr whh an b rprsn by a ombnaon of rular an hyprbol angls. I an b ralz ha hs s s h s of all nral sysms n Ponar s rlavy. In hs hory, spa an m ar no longr spara as n Gallan rlavy an moon s nohng bu roaon. Howvr, Ponar s rlavy os no spfy wha s roang. Our am n h followng sons s o rsolv hs funamnal quson. lhough w hav bn usng h onp of four-vor an four-nsor rpaly, w hav no gvn hr rgorous fnon. hrfor, for fuur rfrn, h fnon of a four-nsor s prov hr. four-nsor G of orr n s fn as a mahmaal obj wh n ns whh has 4 n omponns ransforms va G L n L Λ G n Λ LΛ n n n a gvn nral sysm an G (.75) o a nw nral sysm. h mos mporan four-nsors ar hos nvolv n h hory of lroynams, whh wll b suss lar. For smply, w hav bn usng h sam symbols suh as x,, Q, x, an Λ o rprsn h marx form of hr orrsponng hr an four nsors. L n 3. Funamnal hory of moon In hs son, w vlop h hory of alrang parls, whh shows h funamnal rlaon bwn spa-m an mar. I larfs h rlavy of spam an shows how an nral sysm ransforms o ohr nral sysms. hs s nohng bu h gomral hory of nraon. I s sn ha h rlav moon s h rsul of h four-mnsonal roaon of hs sysms rlav o ah ohr. W sar wh lassal parl knmas an vlop h funamnal hory of moon. h hory of nraon wll b suss n h nx son. 5

16 3.. Knmas of a parl L us spfy h nral sysm x x x3x4 as an nral rfrn fram. Consr a parl wh mass m movng rlav o hs nral fram. any poson, h moon may b onsr as akng pla n h plan ha onans h pah a hs poson. hs plan s ofn all h osulang plan. h vloy vor v s angn o h pah urv n hs plan. h alraon of h parl v a (3.) ls also n hs plan. W an onsr a loal oorna sysm by fnng h un vor angn o h urv a hs poson, h un vor n n h ron of prnpal normal o h urv n h osulang plan, an h b-normal un vor b, whh s normal o h osulang plan a h pon. h rlaon (3.) b among hs vors hols. In hs loal (angnal, normal, b-normal) oorna sysm w hav v v (3.3) wh ss v (3.4) whr s s s h lngh of h nfnsmal splamn of h parl on h spa urv n m nrval. For alraon, w hav v a + v (3.5) For h son rm, w apply h onp of urvaur n h form s s n n (3.6) s R whr R s s h raus of urvaur a h parl poson pon. hrfor, h alraon n rms of angnal an normal omponns a an a n s a a + a n (3.7) 6

17 whr v a a (3.8) a n v ann n (3.9) R s I sms h ffrnal gomry govrnng h knmas of h parl s mor ompl f w nrou h onp of orson of h urv fn by b n (3.) s R whr R or s h raus of orson of h urv. I an b asly shown ha s s s or n n + b (3.) s R R or hrfor, h quaons for urvaur of urv mgh b wrn as ss n s S Rs b ss R s R or R or n b (3.) hs rlaon s all h Frn-Srr formula n ffrnal gomry. h ansymmr nsor on h rgh han s posssss h whol nformaon abou h urvaur an ws of h urv a h pon unr onsraon. Howvr, an nrsng nrpraon of hs rlaon an b gvn as follows. h prnpal rons spfy a loal orhogonal rfrn sysm aah o h parl. hs rfrn sysm roas as h parl movs on h urv pah. I s obvous hs rlaon shows h graual roaon of hs loal sysm wh rsp o any nral sysm. If w wr h rlaon as n b 7

18 8 b n or or s s b n R v R v R v R v (3.3) h an-symmr nsor s h angular vloy nsor of h roang loal sysm b n. By onsrng h angular vloy vor s or R v R v ω (3.4) w oban h rlaon b n b n ω (3.5) I s nrsng o no ha hr s no angular vloy omponn n h n ron. h Frn Srr formulas an b gnralz o hghr mnsonal Eulan spas by fnng gnralz urvaurs. I an b shown ha n h prnpal loal oorna sysm, whh s all h Frn Srr fram, h an-symmr urvaur nsor s r-agonal [7]. n mporan analogy wll b sn n vlopng h rlavs hory of moon.

19 3.. Rlavs knmas of a parl In a rlavs suy, h vloy an alraon of h parl mus b fn as four-vors. Howvr, s sn ha h vors v an a ar sll usful n hs vlopmn. h poson of a parl n h nral rfrn fram srbs a pah known as h worl ln. By onsrng wo nghborng vns on h worl ln of h parl wh oornas x an x + x, w hav ( x, ) ( v ) h squar lngh of hs nfnsmal four-vor x, (3.6) v s x x x x x (3.7) s h salar nvaran unr all Lornz ransformaon. I s sn ha h magnary lngh on h worl ln s v s (3.8) h propr m bwn h vns τ s fn by hrfor, v τ γ (3.9) s τ (3.) By usng h onp of rapy w no v anh (.33) γτ τ osh (3.) 9

20 h un four-vor angn o h worl ln s fn as whr x x (3.) s s (3.3) h four-vor vloy u u s fn as h ra of hang of h poson vor of parl x wh rsp o s propr m x u (3.4) τ h spa an m omponns of u ( ) u u,u 4 (3.5) ar an u γv v v snh (3.6) u γ 4 v osh (3.7) hrfor whh an b wrn as wh ( snh, osh ) u (3.8) u (3.9) ( snh, osh ) (3.3) h lngh of h four-vor vloy s a onsan sn an s hus m-lk. I s sn u u uu u + u4 (3.3)

21 (3.3) s whh mans s s normal o h worl ln. By onsrng h un four-vor n n hs normal ron all h frs normal an usng h onp of urvaur, w hav n (3.33) s R whr R s h worl ln raus of urvaur a h pon unr onsraon. h mnus sgn s for onvnn an wll b jusf shorly. I s sn ha (3.34) s s R h four-alraon b b s fn as u x b (3.35) τ τ whh s always prpnular o h four-vor vloy whr, u u (3.36) τ I an b asly shown ha 4 v a 4 v a b γ a + γ v, γ (3.37) h lngh of four-vor alraon an b foun o b 4 6 v a b bb γ a + γ (3.38) Sn b b s posv, h four-alraon s spa-lk. Howvr, s mor appalng o onsr h four-alraon rlav o h worl ln. By usng (3.33), w oban b τ R n (3.39)

22 whh shows h four alraon s n ron of frs-normal of worl ln an s valu s b (3.4) R Now w suy h rlav moon of a parl n ffrn nral sysms. L us onsr h nral sysms x xx3x4 an x x x 3x 4, whh ar rla by h Lornz ransformaon x Λ x (.6) whr Q + (osh ) Λ snh Q + (osh ) Q snh snh osh snhq osh (.58) ssum parl movs n h frs nral sysm wh ( ) vloy s whr u x an s four-vor x ( u, u 4 ) ( snh, osh ) (3.4) v anh (3.4) hs parl also movs n h son nral sysm wh x x ( ) (, u ) ( 4 snh, ), suh ha u u osh (3.43) whr v anh (3.44) hs four-vor vlos ar also rla by h nsor ransformaon hrfor, u Λ u (3.45)

23 Q + (osh ) Q snhq snh u (3.46) snh osh osh whh gvs h rlaons snh Q[ + (osh ) ]snh snh osh Q (3.47) osh osh osh snh snh (3.48) h rlaon (3.48) shows ha h vloy aon law s val vn whn on of h vlos s no onsan. W nvsga shorly h valy of hs law whn all parls ar alrang Moon of parl as a four-mnsonal roaon fr rvwng knmas of a parl, w vlop h mporan harar of s moon as a four-mnsonal roaon. o show hs w onsr h moon of h parl as h ransformaon of s four-vloy vor u n h nral rfrn fram sysm. L u b h nal four-vor vloy a poson x, suh ha u ( x ) u. W an onsr h ransformaon u ( x) L ( x, x) u ( x) (3.49) whr h ransformaon nsor L ( x, x ) pns on h urrn poson of h parl. hs rlaon an b wrn as ( ) L( x, x u u x ) (3.5) Sn h lngh of h four-vor vloy s onsan, w hav u ( x) u ( x) u ( x ) u ( x) (3.5) hrfor, Lα ( x, x ) Lβ ( x, x) δ αβ ] uα ( x) uβ ( x ) (3.5) [ hs rqurs h orhogonaly onon L ) δ (3.53) α ( x, x) Lβ ( x, x αβ 3

24 I s sn ha alhough L( x, x ) looks smlar o a Lornz ransformaon among nral sysms, vars wh moon of h parl. Manwhl, h nvrs rlaon s whh n rms of omponns s ( x ) L x, x u( x) u ( ) (3.54) u ( ) L x, x u ( x) x (3.55) ( ) hs gvs h orhogonaly onon n h form L x, x ) L ( x, ) ( x (3.56) or L ) δ (3.57) α ( x, x) Lα ( x, x By akng h rvav of (3.57) wh rsp o h propr m of h parl, w oban L α ( x, x) Lα ( x, x) Lα ( x, x) + Lα ( x, x) τ τ (3.58) Now by fnng h four-nsor Ω Lα ( x, x) x) Lα ( x, x ) (3.59) τ ( w an s ha h rlaon (3.58) boms Ω ( x) + Ω ( x) (3.6) or Ω ( x) + Ω ( x) whh shows Ω ( x) s an an-symmr four-nsor. In ompa form, w hav (3.6) L( x, x) Ω ( x) L ( x, x) (3.6) τ 4

25 By mulplng h rlaon (3.59) wh L β x, x ) an usng h orhogonaly onon, ( w oban L ( x, x τ ) Ω (3.63) α ( x) L ( x, x ) α hs may raly b wrn as L( x, x τ ) Ω ( x) L( x, ) x (3.64) Now h alraon from h orgnal ransformaon rlaon s u ( x) L ( x, x u ( x ) u ) (3.49) ( x) τ By subsung from (3.63), w hav u τ whh rus o h rlaon ( x) u L (, ) x x u ( x ) (3.65) τ ( x) L ( x, x u ( x ) Ωα α ) (3.66) τ ( x) ( x) u ( x) Ω (3.67) α α hs s h rlaon bwn four alraon u τ ( x) an four-vloy a ah pon on h worl ln. I shoul b no ha h rlaon (3.67) s aually (3.35) an (3.37) wrn as a ransformaon. I s also no ha h rlaon (3.67) s smlar o h non-rlavs rlaon for ra of hang of a onsan lngh vor G aah o a roang sysm G ω G (3.68) 5

26 whr ( ω, ω ω ) ω s h angular vloy of ha roang sysm. I s rmmbr, 3 ha h omponns ω, ω an ω 3 ar h angular vlos of h boy sysm n h yz, zx an xy plans of an nral fram. Baus of h mporan of (3.68), s avanagous o monsra h mahmaal als of s rvaon. L h prm sysm o b h boy sysm. hn h omponns of hs vor G ar onsan n hs sysm. hrfor, w hav G Q( ) G( ) (3.69) whr Q () s h orhogonal roaon marx. hs rlaon an b wrn as ( ) Q ( )G G (3.7) h ra of hang of h vor G ( ) rlav o h fx rfrn fram s G Q fr lmnangg by usng (3.69), w oban ( ) G (3.7) Now by fnng h nsor G Q QG (3.7) w hav G WG whh n h nx noaon an b wrn as Q W Q (3.73) (3.74) G WjG (3.75) j Now by ffrnang h orhogonaly onon wh rsp o h m, w oban Q Q (3.76) 6

27 Q Q + Q Q (3.77) whh may raly b wrn as W + W (3.78) hs rlaon shows ha h nsor W s an-symmr. hs nsor s h known angular vloy nsor of h roang sysm rlav o h nral sysm. In rms of lmns, hs nsor s ω3 ω W R ω ω3 ω (3.79) ω ω hrfor, h rlaon (3.74) s h ohr form of (3.68) G ω G (3.68) I shoul b no ha h Frn-Srr formula (3.5) s h applaon of hs quaon for funamnal bas un vors. Now, w hav a rmarkabl analogy for u τ wh ( x) ( x) u ( x) Ω (3.67) α α G WjG (3.75) j u I s sn ha h four-vor alraon s h rsul of onnuous roaon of h τ four-vor vloy u n a four-mnsonal sns. hrfor, sms u s aah o a four-mnsonal sysm x x x 3x 4 n h x 4 ron, whr (,, ) u, (3.8) 7

28 an hs sysm s roang wh four-mnsonal angular vloy Ω rlav o h nral sysm, suh ha L ( x, x τ ) Ω (3.63) α ( x) L ( x, x ) α hrfor, w hav sovr ha hr s a funamnal rlaon bwn spa-m an mar. massv parl spfs a loal four-mnsonal orhogonal sysm wh hr ral axs an on magnary axs. Whn hs loal x x x 3x 4 spa-m sysm, h parl has aah four-vloy wh magnu n h m ron. h roaon of hs spa-m or four-mnsonal sysm gnras moon of h parl rlav o h nral sysm. hs roaon s rprsn by h four-nsor angular vloy Ω Ω n h nral rfrn fram. h naur of hs four-mnsonal angular vloy s xplor vry shorly. s was mnon abov, a any pon on h worl ln, w hav h ransformaon ( x) u ( x) u Λ (3.8) whr h varyng nsor ransformaon Λ ( x) looks lk a Lornz ransformaon. hrfor, hr mus b a rlaon bwn nsors Λ ( x) an ( x). For a parl a L an nal pon x, w hav ( x ) u ( ) u Λ (3.8) x hrfor Λ ( x) u ( x) Λ ( x ) u ( ) x (3.83) By subsung for u ( x) from (3.49), w oban Λ ( x) L ( x, x u ( x ) Λ ( x ) u ( x ) α ) α α α (3.84) hs shows h rlaon 8

29 whh an b wrn as ( x) L ( x, x Λ ( x ) Λ α ) α (3.85) ( x) ( x, x Λ( x ) Λ L ) (3.86) hrfor ( x) Λ( ) L ( x, x) Λ x (3.87) I shoul b no ha alhough Λ ( x) s no onsan any mor, follows h gnral form of Lornz ransformaon (.58) QP + (osh ) PP snhpp Λ snhpp oshp (3.88) Q + P (oshp ) QPPP snhpqpp snhpp oshp whr h physal manng of h paramrs n P an Q P has no bn spf. Howvr, w an xplor hr rlaon wh h moon of h parl n h ours of our vlopmn. By usng h rlaon (3.8), w oban u ( snh, osh ) (3.89) P P P hs shows h vor P s aually h rapy vor of h parl. hrfor, Q P + (osh ) Λ snh Q P + (osh ) Q P snh snh osh snhq P osh (3.9) I s sn ha h poson vor x( ) x of h parl os no spfy s rlav poson n h rfrn nral fram omplly. I s also nssary o spfy s boy fram ornaon Λ() Λ rlav o hs fram. Howvr, h rapy vor () s oban from h vloy vor () an orhogonal marx ( ) x v. hrfor, h poson vor x x( ) Q omplly spfy h parl poson. P Q P 9

30 Now, w nvsga h harar of h an-symmr nsor Ω Ω. h nal four-vor vloy s ( snh, ) osh u (3.9) For smply w ak h spa oornas of h nal boy fram o b paralll o h saonary nral fram, whr Q ( ) P. hrfor, + (osh ) snh Λ (3.9) snh osh By akng h rvav wh rsp o h propr m τ n h quaon w oban ( x) Λ( ) L ( x, x) Λ x (3.87) L( x, x) Λ τ τ ( x) Λ ( x ) (3.93) hrfor, h rlaon boms an fnally w hav ( x) L( x, x) Ω ( x) L ( x, x) (3.94) τ ( x) Λ Λ( x ) Λ ( x ) Λ( x) (3.95) τ Ω Ω ( x) ( x) Λ Λ( x) (3.96) τ For ( x) Λ from (3.9) 3

31 3 + osh snh snh ) (osh P Q Λ (3.97) By akng h rvav wh rsp o h propr m, w oban osh snh snh ) (osh snh snh osh snh osh ) (osh snh τ τ τ τ τ τ τ τ P p Q Q Λ (3.98) hrfor, for ( ) x Ω n (3.96), w hav τ τ τ τ τ τ τ osh snh snh ) (osh osh snh snh ) (osh osh snh snh ) (osh snh snh osh snh osh ) (osh snh P P Q Q Ω (3.99) Now by usng h rlaon P P P Q Q R ω τ (3.) whr P ω s an angular vloy vor n a mahmaal sns, w oban

32 snh snh snh snh ) (osh P P P ω ω ω R R R Ω τ τ (3.) hs rlaon an b wrn n h form η η R Ω ω (3.) whr + P R R ω ω ) (osh (3.3) + P R η ω τ τ snh (3.4) On an s hs rlaons an also b wrn as ( ) P ω ω + τ osh (3.5) + P ω η τ τ snh (3.6) hs rlaons an b smplf furhr by usng h rlaons n s R v τ osh (3.7) an n b (3.) h four-nsor ( ) x Ω n rms of lmns n h nral rfrn fram s η η η η ω ω η ω ω η ω ω Ω (3.8)

33 hs s h gnral form of an an-symmr four-nsor angular vloy Ω. I shoul b no ha h lmns Ω4 Ω4 η ar magnary. I s obsrv ha h angular vlos ω, ω an ω 3 n xy, yz an zx plans gnra spa roaon of h boy fram; h magnary angular vlos η, η an η3 n x, y an z plans gnra boos of h boy fram. hrfor, h spa-m boy fram sysm roas rlav o h nral sysm wh angular vloy nsor Ω, whh s a ombnaon of llp an hyprbol angular vlos ω an η. Rurnng o h quaon for four-alraon ( x) u Ωα ( x) uα ( x) (3.67) τ w hav h spa an m omponns of four-vor alraon as u ω u τ η u 4 η u τ u 4 (3.9) (3.) hs rlaons an also b wrn n h form v v / u η + ω v (3.) u 4 η u v / (3.) o monsra h physal manng of h four-nsor angular vloy Ω, w onsr h as whr h parl sars movng from rs a. hs rqurs n (3.6) an (3.7). hrfor, a hs momn, ω ω P (3.3) 33

34 η τ a (3.4) hs man ω an η a ar h rular an hyprbol angular vloy of h boy fram rlav o h nral fram. W no ha a hs nsan τ an η a a (3.5) an hrfor φ ωτ (3.6) v aτ aτ (3.7) h nfnsmal an-symmr four-mnsonal roaon nsor Φ s fn whh an b wrn as R φ Φ v Φ Ωτ (3.8) v (3.9) hs nsor n rms of lmns s φ3 φ v φ3 φ v Φ (3.) φ φ v3 v v v3 hs xplanaon an b us for h spal as whr h nral sysm s onn wh h boy fram nsanly, whh s ofn all a ommovng nral fram sysm. For hs as, w hav Q P an h rlaon boms L τ L ( x) τ Ω ( x) α Ω ( x) L ( x) α ( x) (3.) (3.) 34

35 whr Rω Ω η η Rω a a (3.3) I s sn ha an a hs nsan ω (3.4) ω P η a a (3.5) τ an w hav φ ω τ (3.6) v a τ a τ (3.7) I s sn ha ω an η a ar h rular an hyprbol angular vloy of h boy fram rlav o h ommovng nral fram sysm. h nfnsmal fourmnsonal roaon Φ of h boy fram rlav o h ommovng nral fram sysm s R φ v Φ (3.8) v I s obvous h four-nsor angular vloy nsor h ommovng fram an w hav Ω s h rprsnaon of Ω on Ω Ω (3.9) From hs, s xp ha Ω Λ α Λ (3.3) βω αβ hs nsor ransformaon an also b wrn as Ω L L Ω α β αβ (3.3) 35

36 lhough w sll us h noaons ω an η an all hm angular vlos, hs vors anno b akn as a propr angular vloy vors lk vors ω an η. hs s h rsul of h non-eulan gomry govrnng h four-mnsonal roaons. ombnaon of h rular an hyprbol angular vlos ω an η n h rlaon (3.3) gvs h vors ω an η. h famous homas prsson for alrang parls s manfs of h govrnng hyprbol gomry. Now s lar why w no subsrp P n h orhogonal nsor orhogonal nsor Q spfs ω hrough h rlaon Q P, whh spfs ω P. h R ω Q Q (3.3) lhough Q an ω ar ssnal mahmaal ns, hy anno b monsra gomrally as rly as Q P or ω P. Howvr, w mus b arful whn w onsr ω as a rular angular vloy. W mgh rop h subsrp P auously. hrfor, w hav larn ha h moon of a parl n h lassal sns s h rsul of h hyprbol par of roaon of s boy fram. h spa roaon s also par of h moon, whh s h orgn of spn prsson of an lron n a magn fl. hs wll b suss n mor al shorly. I s ralz ha h non-eulan gomry s h rsul of ransformng four-nsors an four-vors among ffrn spa-m boy frams. hrough hs mporan physal raly, on appras h work of hos who onsr h possbly of non- Eulan gomry. h non-eulan asp of h vloy aon law for unform moon has bn su by Robb, Varǎk, Lws, Wlson an Borl [6]. Howvr, hs sovrs hav no bn appra nough by lar nvsgaors. Forunaly, hr hav bn som avoas of rvvng hs mporan ssu rnly [8]. Now w appra ha hs pah rsolvs nonssns an paraoxs n rlavy. I also 36

37 xplans h gomral mhansm bhn moon an nraon, whh wll b vlop n h nx son. W hav also no an mporan ssu rgarng h four-vor vloy of a parl. I has bn shown ha h four-vor vloy s aah o s boy fram suh ha ( x) u ( x) u Λ (3.8) hs has bn shown symbolally n Fg. by onsrng a wo mnsonal spa an on m ron. I shoul b no ha h nral rfrn fram an boy fram of h parl boh hav aah four vor-vlos u R an P u n hr spa-m frams, rspvly. Howvr, h Lornz ransformaon (3.8) rlas h omponns of four-vor vloy u of parl P n s fram an s omponns of four-vor vloy u ( x) n h nral rfrn fram of parl R. I shoul b no ha h four-vor vloy omponns u (,,,) an u ( x) ( snh, osh ) ar rprsnaons of P u n boy fram of parl an nral rfrn fram, rspvly. Inral rfrn fram Boy fram of parl x x x x R u u ( x) ( snh, osh ) x 4 P u (,, ) u, x 4 Fg.. Inral rfrn fram an boy fram. hrfor, w an onsr a nw yp of four-vor G all an aah four-vor an fn as a four-vor aah o h boy fram of a parl, suh ha G Λ G (3.33) no mar whhr h boy fram s nral or alrang. For hs four-vor 37

38 G τ Ω G (3.34) hs an b wrn as or n ompa form G s Ω G (3.35) G ΩG (3.36) s Usng hs rlaon for un bas angnal four-vor, w hav Ω (3.37) s By omparng hs rlaon wh h rlaon (3.33) for h worl ln raus of urvaur, w oban n Ω R I s sn ha h worl ln raus of urvaur sasfs whr h symmr nsor Ω Ω s R (3.38) Ω (3.39) ωω ω + ηη ω η ( ) ω η η (3.4) I s also sn ha h funamnal quaon (3.63) an b wrn as L s or n h ompa form ( x) ( x) L s Ωα ( x) Lα ( x) (3.4) Ω( x) L( x) (3.4) 38

39 39 For h bas four-vors of boy fram, w hav ( ) x s Ω (3.43) whh an b wrn as s s s s η η η η ω ω η ω ω η ω ω (3.44) On ralzs ha hs quaon s aually a Frn-Srr-lk formula for ornaon of h loal boy fram rlav o h nral sysm. Howvr, shoul b no ha hs ornaon s n rms of gnralz urvaurs of h worl ln bu no gnrally n prnpal rons. h angn o h worl ln spf by 4 s a prnpal ron, bu h prpnular rons o h angn ar no usually prnpal rons. I shoul b also mnon ha Syng has alray su h Mnkowskan Frn-Srr movng fram [9]. Wha w hav shown s ha hs fram s a rprsnaon of h funamnal boy fram of a parl. In hs son, has bn monsra ha hr s a rlaonshp bwn Mnkowskan spa-m an massv parls. h parl spfs s spa-m boy fram rlav o h nral rfrn fram. Now h naural quson onrns h vry xsn of hs spa-m sysms. I s sn ha w ar ompll o am h xsn of a unvrsal ny, whh has nohng o o wh any spal spa-m. I s n hs unvrsal ny n whh parls an hr orrsponng spa-m boy fram xs. Lar w wll nvsga mor abou hs unvrsal ny.

40 3.4. Gnral rlav moon an vloy aon law Now w vlop h hory of rlav moon for gnral alrang parls. I s sn ha h govrnng rlaons an vloy aon law n Ponar s rlavy ar sll val for hs gnral as. Consr wo parls an B movng wh vlos () v an v ( ) v B v B rlav o an nral sysm. h four-vor vlos u an u B ar aah fourvors, whr w hav ( u ) Λ u (3.45) ( u ) an ( B ) B whr ( ub ) Λ BuB B (3.46) u ar rprsnng hs four-vors on hr orrsponng boy fram ( ) ( u ) (,, ) u (3.47) B, B h ransformaons () Λ an ( ) Λ Λ rprsn h ornaon of hs boy B Λ B frams rlav o h nral fram. For hs ransformaons, w xplly hav an Q + (osh ) Q snh Q Λ () (3.48) snh osh Q B + (oshb ) Q BB snhbq BB Λ () B B (3.49) snhbb oshb By usng (3.47) an ombnng (3.45) an (3.46), w oban u Λ Λ u (3.5) B B Rlav ornaon of h boy fram B rlav o a m s no by Λ an s B fn suh ha Λ Λ Λ (3.5) B B 4

41 hs rlaon shows Λ Λ Λ (3.5) B B hrfor, (3.5) boms u Λ u (3.53) B B whh an also b wrn as u B Λ u (3.54) B I shoul b no ha Λ s h rlav Lornz ransformaon from boy fram B o boy fram B masur by our nral rfrn fram a m. hrfor all h rlaons ar rlav o hs obsrvr a m. Howvr, w shoul rv smlar rlaons rlav o h obsrvr aah o h boy fram. For hs w no ha h vloy of B rlav o masur by an obsrvr n h boy fram of s ( ub ) ( ub ) Λ ub (3.55) By subsung for u B from (3.46), w oban ( ub ) ( ub ) Λ Λ B ( u B ) B (3.56) W also hav h obvous rlaon whh an b wrn as ( u ) ( Λ B ) ( ub ) (3.57) ( ub ) ( Λ B ) ( u ) (3.58) By omparng (3.56) an (3.57) an usng (3.55) w oban h rlaon whh an b wrn as ( ) Λ Λ Λ (3.59) B ( ) Λ Λ B B B Λ (3.6) 4

42 Inrsngly, s sn ha ( ) Λ Λ Λ Λ (3.6) B B whh looks lk h ransformaon for nsor Λ from nral rfrn fram o h B boy fram. Wha w hav s h vlopmn of h gnral hory of rlav moon. Explly from (3.55), w hav snh u B (3.6) snh osh oshb Q + (osh ) Q snh Q B B ( ) From hs, w oban h rlaons ( snh B / B ) snh osh BQ + Q [ + (osh ) ] snh BB ( B ) osh oshb snh snhb B (3.63) osh (3.64) hs rlaons ar h manfs of hyprbol gomry govrnng h vloy aon law vn for alrang parls. hs propry hols for all aah four-vors an four nsors. Inral obsrvrs rla omponns of aah four-vors an fournsors by Lornz ransformaons. hs s h orgn of non-eulan gomry govrnng h hr vor an hr nsors. s w saw h aon of hr vor vlos follow hyprbol gomry. I shoul b no ha hs rlaons hol sp h fa ha h ransformaon x Λ x (3.65) s no val among alrang sysms. Wha w hav hr s h omplon of h Ponar s rlavy for alrang sysms. 4

43 4. Funamnal nraon fr vlopng h hory of alrang moon, w ar ray o vlop h hory of funamnal nraon. h quaon of moon for a parl n an nral rfrn fram sysm s gvn by u m F (4.) τ whr F s h four-vor Mnkowsk for. hs for s h rsul of nraon of h parl wh a fl, suh as an lromagn fl. W ar lookng o xplor h gomral harar of hs fl. By subsung for four-alraon from (3.67) n h rlaon (4.), w oban for h Mnkowsk for. Sn F mω u (4.) Ω s an-symmr, w hav F u mω u u (4.3) whh mans h four-vor Mnkowsk for F s prpnular o h four-vor vloy u. h rlaon (4.) shows ha hs for pns on four-vor vloy u an four-nsor angular vloy Ω a h poson of h parl ~ x. s a rsul, h fl srngh mus pn on h four-nsor angular vloy Ω. I s sn ha h smpls amssbl fl s hararz by a fl srngh four-nsor ( x) Θ suh ha a h poson of h parl ( x ) mω ~ (4.4) αθ Salar α s a propry of h parl an pns on h yp of nraon. hs quany an b rognz as lr harg n lromagn nraon. hrfor, w an onsr a funamnal nraon o b an nraon hararz by an an- Θ x, suh ha a h poson of h parl ~ x symmr srngh nsor fl ( ) α Ω ( ~ Θ x ) (4.5) m 43

44 lhough ( x~ ) Θ s npnn of h parl, h Mnkowsk for pns on h parl hrough α an four vor vloy u, suh ha F αθu (4.) hrfor, h quaon of moon boms u ( x ) u (4.6) τ m αθ ~ On an s ha h an-symmr srngh nsor ( x) Θ looks lk a four-mnsonal vory fl analogous o h hr-mnsonal vory n roaonal flu flow. hrfor, w an onsr a four-vor vloy-lk fl V V nu o h spa-m of h nral rfrn fram, suh ha s four mnsonal url s h vory-lk srngh nsor ( x) V V Θ (4.7) From our famlary wh lroynams, s obvous ha lromagn nraon s omplly ompabl wh hs gomral hory of nraon. hrfor, n h nx son, w prsn h ovaran hory of lromagns an xplor s gomral asps bas on h four-mnsonal vory hory. I s sn ha hs gomral hory rsolvs som ambgus n h raonal hory of lromagns. Mor mporanly, on ralzs ha hs hory s a mol for any ohr funamnal nraon. hrfor, h orrsponng gravaonal hory s also vlop n al n Son 6. W shoul rmmbr ha h hory of rlavy has s orgn n h hory of lroynams. Now w an s ha h hory of nraon also has s orgn n hs hory. 44

45 5. Gomral hory of lromagn nraon In h hory of lroynams [], n an nral rfrn fram, h for on a harg parl an b xprss n rms of wo vor fls, an lr fl E(x, ) an a magn fl B(x, ). In rms of hs fls, h for on a parl wh harg q movng wh vloy v s gvn by F q( E + v B) (5.) q( E B v) hs s known as h Lornz for n SI uns. I s no ha h vor B s aually an axal or psuo-vor. hrfor, hr s a orrsponng an-symmr nsor B3 B R B B3 B (5.) B B suh ha h Lornz for n marx form s F q ( E R v) (5.3) B In h ovaran hory of lroynams, h orrsponng four-vor Mnkowsk for s F qf ~ x u (5.4) whr h lromagn srngh fl F s ( ) B3 B E B3 B E R B E F (5.5) B B E3 E E E E3 hrfor, h quaon of moon of hs parl s gvn by u ( x ) u (5.6) τ m qf ~ 45

46 I s obvous ha h quaon (5.6) has h form of h quaon (4.6), whh was oban bas on h knmaal onsraons. I s sn ha α q (5.7) Θ F (5.8) hrfor, h spa-m boy fram of h parl roas wh four-nsor angular vloy q Ω F ( ~ x ) (5.9) m rlav o h nral fram. I s sn ha h hyprbol an rular angular vlos of h boy fram ar an η q E( ~ x ) (5.) m ω q B( ~ x ) (5.) m rspvly. Now w ralz ha h lromagn srngh fl nsor an Lornz for vor ar boh a naural onsqun of h gomr sruur of rlav spa m. Bas on our xprn wh onnuum mhans, as w mnon bfor, h srngh nsor F fl sms lk a four-mnsonal vory fl. hs lromagn vory four-nsor fl s a ombnaon of hyprbol lromagn vory E an rular lromagn vory B. I s sn ha h salar m q maps h vory fl F a h poson of h parl o h four-nsor angular vloy Ω of s boy fram. hrfor, h ff of lromagn nraon on a harg parl s nohng bu h nsananous four-mnsonal roaon of s boy fram. h quaons (3.) an (3.) for h parl an b wrn as u ω u + τ v / η (5.) 46

47 η u τ v / (5.3) hs quaons ar quvaln o h spa an m omponns of quaon (5.6) for lromagn nraon as u m mv q v / ( E + v B) (5.4) m v / qe v (5.5) s w know, h frs quaon s h quaon of moon, whr s rgh han s s h famlar Lornz for. h son quaon s h ra a whh h lromagn fl os work on h parl an hangs s nrgy. In ovaran lromagn hory, h four-vor lr urrn nsy J ( J, J 4 ) ( J, ρ ) ρ ( v, ) (5.6) E E E E E sasfyng h onnuy quaon ρe J E, J E + (5.7) gnras h lromagn four-vor ponal, whr E (, 4 ) (5.8) n spa-m orrsponng o h nral rfrn fram. h spa omponn s h magn vor ponal an h m omponn 4 s rla o h lr salar ponal φ as 4 φ (5.9) h four-mnsonal url of gvs h lromagn fl srngh nsor F F (5.) 47

48 hrfor, h fls E an B ar xprss n rms of hs ponals as E φ (5.) B (5.) I shoul b no ha h four-vor V orrspons o h ngav of V (5.3) an an b onsr as an lromagn vloy fl nu n four-mnsonal spa-m rlav o h nral fram. s was mnon prvously, s fourmnsonal url s h lromagn vory four-nsor F Θ F (5.4) h ovaran form of h govrnng quaon for srngh or vory nsor F u o h lr urrn nsy s 4πK F J E (5.5) whh s h ompa form of Maxwll s nhomognous quaons E 4πKρ E (5.6) E 4πK B + J E (5.7) Equaon (5.6) s Gauss s law an quaon (5.7) s mpr s law wh Maxwll s orron. In hs quaons, h onsan K s h lrosa or Coulomb onsan ha usually s wrn as also h rlaon K, whr ε s h prmvy of fr spa. hr s 4πε, whr onsan s all h prmably of fr spa ε 4π K an h rlaon hols. hrfor, h quaon (5.5) an b wrn as F J (5.8) E 48

49 an also h Gauss an mpr s laws (4.6) an (4.7) bom ε E ρ E (5.9) E B + J E (5.3) h ompably quaon for F s σ F + F + F (5.3) σ σ hs s h nssary onon o oban h lromagn vloy from vory fl F. I smply hks f a gvn lromagn vory fl s apabl or no. hs quaon s h ovaran form of Maxwll s homognous quaons B (5.3) B E + (5.33) s w know, h quaon (5.3) s Gauss s law for magnsm an h quaon (5.33) s Faraay s law of nuon. h s of quaons (5.9)-(5.3) an (5.3)-(5.33) ar Maxwll s quaons n SI uns. hy smply show h rlaons govrnng h lromagn vory nu o spa-m. I s sn ha h gomral hory of lromagn nraon s vry lar n SI uns. Inrsngly, s ralz ha h lromagn hory woul hav bn muh mor ompabl wh h gomral hory f h salar an vor ponals φ an, an magn fl B ha bn fn as h ngav of hr prsn form. h four-vor ponal fl s no unquly rmn from ompabl srngh four-nsor F u o h gaug from. In, h nw fl + λ (5.34) 49

50 os no hang h fl srngh nsor F. Suh ransformaon s all a gaug ransformaon n whh h funon λ s a funon of oorna x. hs gaug from allows us o hav h Lornz gaug onsran φ + (5.35) hrfor, λ s no ha arbrary. I mus sasfy h wav quaon λ λ λ (5.36) hs wav quaon an b onsr as rprsnng h nral lromagn wavs. Usng h Lornz gaug n (5.8) prous h manfsly ovaran wav quaon J (5.37) α α E Wha w hav shown s ha Maxwll s quaons ar quaons govrnng h hyprbol an rular angular lromagn vors σ E an B. h quaon F + F + F (5.3) s nohng bu a knma ompably for hs lromagn vors. h nonhomognous quaon σ E σ F J (5.8) s h rlaon among hs vors an lr four-vor nsy urrn. n analogy wh onnuum mhans suggss hs rlaon s h quaon of moon for lromagn vors. Maxwll s quaons ar ovaran, whh mans hy ar nvaran unr Lornz ransformaons among nral sysms. hrfor, h four-vor, an four-nsor F ar funamnal fls npnn of any spf spa-m nu n h unvrsal ny mnon bfor. I s h nral obsrvr who spfs a spa-m n hs unvrsal ny an masurs omponns for hs four-vor an four-nsor, for 5

51 xampl F for F. h omponns of hs four-nsor ransform unr Lornz ransformaon among nral sysms as F Λ Λ F (5.38) α β αβ h non-eulan harar of lromagn fl nsors s obvous from hs ransformaons. Inrsngly, h salars F F ( B E ) (5.39) F ( E B) (5.4) ar h nvarans of h four-nsor F unr h Lornz ransformaons. hy show ha h salar B + E s nvaran. I s obvous ha h non-nral obsrvrs ar no qualf o us (5.38), baus h ransformaon x Λ x (.6) os no hol among hm. W monsra hs fa by a smpl xampl. Consr h lromagn vory fl gnra by a fr harg parl. Is boy fram s an nral fram an has a unform moon rlav o ohr nral obsrvrs. h parl gnras h lr fl n s nral boy fram, suh ha hrfor, s sn ha whr q E 4πε r rˆ (5.4) (,,, φ ) (5.4) q φ (5.43) 4πε r 5

52 s paralll o h four-vor vloy u (,,, ). Rlav o h rfrn nral fram, w hav an x Λ x (5.44) Λ (5.45) I sms as f h four-vor fl wr aah o h boy fram rgly n h m ron, suh ha looks roa rlav o h fx nral sysm. Howvr, hs rg lk harar an ovaran rlaons ar no val whn h parl s alrang. I sms h spa-m boy fram of an alrang parl os no look rg n hs sns o any obsrvr. hrfor, h poson four-vor x, four-vor ponal an four-nsor F fl o no ransform unr a unform hyprbol roaon. hs non-rg harar an b onsr as h gomral orgn of lromagn raaon. h raaon of an alrang parl an b analyz by usng h gnral quaon J (5.37) α α E n h onx of Lénar-Whr ponal []. Wha s h onsqun of h non-rgy of h spa-m boy fram of an alrang parl? s w saw, h four-alraon of a harg parl u q F ~ ( x ) u (5.46) τ m boy fram n h nghborhoo of h parl. hrfor, w fn ( ) s h rsul of rg-lk nsananous roaon of s boy fram. Howvr, w now ralz ha h global rg-lk harar of h boy fram s no a rqurmn for hs gomral rvaon. I s only nssary o onsr h nsananous roaon of h Ω x~ as h fourmnsonal angular vloy of h boy fram a h poson of h parl q Ω ( ~ x ) F ( ~ x ) (5.47) m 5

53 Inrsngly, wh hs vlopmn w an xamn h harar of parls n quanum hory o xplan h wav-parl ualy of mar. I s n lassal mhans whr w spfy poson of a parl, for xampl, a h orgn of s spa boy fram. In quanum mhans, a fr lmnary parl wh spf momnum os no hav a spf poson n s spa-m an an b anywhr n s boy or nral rfrn fram. On an suggs ha h wav funon of h parl rprsns h ra of s spa-m boy fram on h nral rfrn fram. hrfor, s nssary o unrsan h Dra spnor wav funon n h framwork of h prsn spa-m hory. hs nw vw looks vry promsng f w rmmbr ha h wav funon of an nrang parl s loalz an s ffrn from h wav funon of a fr parl. I s sn ha hs s nohng bu h manfsaon of a formaon-lk harar of h spa-m boy fram of an nrang parl. Inrsngly, w ralz ha h raon an annhlaon of parls an b xplan as h rsul of onsrans n h m ron. I s lar ha w may xp o rsolv ambgus n h quanum worl an ohr branhs of morn physs wh our nw vw of spa-m. Hr, w shoul mnon ha h affny of h Lornz ransformaon wh lromagn srngh fl nsor an Lornz for has bn ralz bfor. For xampl, Burago has sa ha h lromagn srngh fl nsor an Lornz for ar boh a naural onsqun of h gomr sruur of Mnkowskan spa m, whh nas a funamnal manng n physs []. Obvously, wha w hav hr s vlopmn of hs funamnal manng. Now s m o xplor mor abou h unvrsal funamnal ny n whh parls ra hr spa-m an nra hrough vory fls. I urns ou ha h rvw of lromagn nrgy-momnum nsor an Maxwll srss nsor s usful. 5.. Elromagn nrgy-momnum nsor Rlav o h spa-m nral rfrn fram, h Lornz for pr un volum on a mum wh a harg nsy ρ E an urrn nsy J E s gvn by f ρ E + J B (5.48) E E 53

54 h gnralzaon of hs for n ovaran lroynams s whr ( ) f F J (5.49) E f f, f 4 s h for-nsy four vor wh f 4 J E E (5.5) W no ha w J E E (5.5) s h work on pr un m pr un volum by h lr fl on movng hargs. hrfor w f4 (5.5) By subsung J E from h quaons of moon of h lromagn fl F J (5.3) E an som nsor algbra, w oban f (5.53) whr s h lromagn nrgy-momnum nsor fn by Fσ Fσ + δ Fαβ Fαβ 4 (5.54) h xpl form of h omponns of hs four-nsor n rms of E an B ar all h Maxwll srss nsor, an j ε ( EE j Ek Ekδ j ) + ( B B j Bk Bkδ j ) (5.55) 54

55 h lromagn nrgy nsy, an whr h Poynng vor S s fn by 4 44 u ε + E B (5.56) 4 B S E B ( E ) S (5.57) (5.58) hrfor, h symmr four-nsor an b wrn n shma marx form as j S (5.59) S u h raon or for xr by hs fl on a un ara of a surfa n spa wh un normal vor n s j j ( n) n (5.6) hrough hs smlary wh onnuum mhans, w an ak as a four-srss nsor. h m-spa omponns of h quaon (5.53) ar f j x j S (5.6) S j u f4 (5.6) x Ingrang hs rlaons ovr a volum V boun by surfa, an usng h vrgn horm, w oban fv + SV V V j n j j (5.63) V f4 V + + uv Sn V (5.64) 55

56 hs quaons show ha h lromagn fl has nrgy an arrs momnum. h Poynng vor S rprsns h nrgy pr un m, pr un ara, ranspor by h fls n spa. I s also sn ha h lromagn fl arrs momnum, suh ha G S ε E B (5.65) s h lromagn momnum nsy vor. By nong an W F f V oal for ang on volum V (5.66) V f4 V work on pr un m by h lr (5.67) V fl on movng hargs n V w oban h quaons (5.63) an (5.64) as ( n F G V ) + (5.68) V W + V uv + S n (5.69) I s sn ha by onsrng P mh F (5.7) whr an an P mh mhanal momnum of hargs n volum V (5.7) P fl GV lromagn momnum n volum V (5.7) V U fl uv lromagn nrgy n volum V (5.73) V w oban h momnum an nrgy onsrvaon laws 56

57 ( n ( P + P ) ) fl mh (5.74) ( W + U ) + S n fl (5.75) hs rlaons n voral form ar ( n ( P + P ) ) mh fl (5.76) ( W + U ) + n fl S (5.77) In aon, no ha h rlaon Fσ Fσ + δ Fαβ Fαβ 4 (5.54) looks lk a onsuv rlaon for four-srss nsor n rm of h four-nsor lromagn vory F n h unvrsal ny. In lnar onnuum mhans, h onsuv quaons rla h srss nsor lnarly o sran or sran ra, bu h nrgy nsy s a quara funon of sran or sran ra nsor. Howvr, wha w hav hr s four-mnsonal analogous as n whh h srss four-nsor s a quara funon of vory four-nsor n h unvrsal ny. hrfor, s sn ha h unvrsal ny bhavs lk a onnuum n whh harg parls ra srsss an lromagn vors. Inrsngly, h pon harg parls ar sngulars of hs vors an four srss nsors. hrfor, h Mnkowsk fors xr on hs pon parls ar h Lornz fors, whh an b onsr also as four-mnsonal lf fors. lhough hs onluson looks vry nrsng, hsoral aouns show s no omplly nw. hs vlopmn s smlar o h ffors of nvsgaors of hr hory. Ehr was h rm us o srb a mum for h propagaon of lromagn wavs. For xampl, s vry nrsng o no ha MCullaugh [] onsr hr o b a nw kn of mum n whh h nrgy nsy pns only on h roaon of h volum lmn of hr. h work of MCullough has bn a bas for work of ohr proponns of hr hory suh as Lor Klvn, Maxwll, Krhhoff, 57

58 Lornz an Larmor. Whakr [3] gvs a al aoun of hs nvsgaons n whh w larn ha Maxwll agr o a roaonal harar for magn fl an a ranslaonal harar for lr fl. W also larn ha Larmor [4] onsr ha h hr was spara from mar an ha parls, suh as lrons, srv as sour of vors n hr. Wha s surprsng s ha w hav us smlar as abou srss an vory, bu n a four-mnsonal onx. In our vlopmn, h magn fl has h sam harar as rular roaon, bu h lr fl has h harar of hyprbol roaon. I s sn ha s wll jusf o all our funamnal unvrsal ny h hsoral hr ou of rsp, whh now s rprsn by four-mnsonal spa-m sysms. hrfor, n h nw vw, parls spfy hr spa-m boy frams n h hr an nra wh ah ohr hrough four-vory an four-srss ha hy ra n h hr. s w mnon, h Lornz for F qf ~ x u (5.4) ( ) s analogous o h lf for n flu ynams. h lf on an arfol s prpnular o h vloy of flow pas h surfa. hs s h mhanal xplanaon of four-vor lromagn Lornz for. I s obvous ha unrsanng mor abou hr an spa-m s an mporan sp owar unrsanng mor abou morn physs. Howvr, h gomral hory of lromagn nraon rsolvs som ffuls vn n hs lassal sa. W arss wo mporan ass. 5.. Magn monopol os no xs Wh h nw vw, h magn fl B s h spa lromagn vory nu o h hr rlav o h rfrn nral fram. hs s analogous o h vory fl n a roaonal flu flow. From non-rlavs flu mhans, w know ha h vory s h url of h vloy fl of h flu an s w h angular vloy of 58

59 h flu lmn. hrfor, w s h sam for h lromagn vory. h magn fl B s h url of h lromagn vloy vor fl B (5.) hs fnon rqurs B (5.3) whh s h knmaal ompably quaon. hs s h nssary onon for h xsn of vor ponal for a gvn magn fl B. Exsn of a magn monopol volas hs rval knmaal ompably quaon. W monsra hs furhr by onraon as follows. L us assum, a h orgn, hr s a pon magn monopol of srngh q m. hrfor, n SI uns ( 3) B q δ ( ) (5.78) m x an h sa magn fl s hn gvn by q B m rˆ (5.79) 4π r Howvr, h rlaon (5.78) onras h knmaal ompably (5.3). Inrsngly, bas on h Hlmholz omposon horm, hs fl an only b rprsn by a salar ponal [5] q φ m m ( x ) (5.8) 4π r whr h magn fl B s gvn by B φ m (5.8) Bu hs s absur baus h lromagn vory vor fl B has o b always rprsn by url of h lromagn vloy vor. hrfor, magn monopols anno xs. I s onlu ha h magn fl B s only gnra by movng lr hargs. 59

60 I has bn long spula ha magn monopols mgh no xs baus hr s no ompl symmry bwn B an E. hs s u o h fa ha B s a psuo-vor, bu E s a polar vor. Wha w hav hr s h onfrmaon of hs orr spulaon ha hr s no ualy bwn E an B n lroynams. W hav shown ha h magn fl B has h harar of a rular vory fl an s vrgn fr. Howvr, h lr fl E has h harar of a hyprbol vory wh lr hargs as s sours, whr ε E ρ E (5.9) I s sn ha hs xplanaon s aually larfaon of Larmor s hr hory. s mnon prvously, h lr harg q of a parl has h propry of a knmaal ouplng, whh maps h four-mnsonal lromagn vory a h poson of h parl o h angular vloy of s boy fram. W hav shown ha lr harg s h only ouplng prsn. Furhrmor, hr s no n for any ohr ouplng. I s naïv o assum ha a smpls mofaon of Maxwll s quaons suff o allow h xsn of magn hargs n lroynams Spn ynams an magn momn I s known ha vry lmnary parl, suh as an lron, has an nrns angular momnum all spn. h spn an b onsr as a onsan lngh four-vor ( ) s s, s 4 suh ha rlav o h parl boy fram, h spn four-vor has only spa omponns. hs mans ha s normal o h parl s four-vor vloy rlav o s fram an also h nral rfrn fram u s u s (5.8) If h lromagn fls ar unform, h quaon for spn s gvn by h BM quaon ) 6

61 s q g g F s + us Fλuλ τ (5.83) m whr g s all h gyro-magn rao. By usng an analogy wh orbal angular momnum of sysms of harg parls an h onp of magn pol momn, w an show g. Howvr, xprmns show s a numbr vry nar. h Dra rlavs wav quaon for an lron shows g []. hrfor, h BM quaon boms s q F s (5.84) τ m hs s fanas! I s sn ha h valu g s ompabl wh h vlop gomral-knmaal hory of lroynams. h spn four-vor s an aah four-vor, whh s roang wh q Ω F ( ~ x ) (5.9) m hrfor, h onsan lngh spn roas wh h boy fram, suh ha s q Ω s F s (5.85) τ m I shoul b no ha h spn four-vor has only spa omponns n s boy fram, whh s onssn wh (5.8). Inrsngly, now w ralz ha h analogy o orbal angular momnum an usng h onp of magn pol momn, whh las o g, s mslang. 6. Maxwllan hory of gravy h Maxwllan hory of gravy gnralzs h Nwonan hory of gravy o movng masss. I s lar ha hs s h ompabl hory wh our gomral hory of nraon. h pulary of hs hory, alhough lassal hory offrs no ompllng 6

62 rason bhn, s ha h gravaonal harg m G s proporonal o h nral mass m, as far as w know. hs s all h quvaln prnpl, whh mans n a propr sysm of uns, suh as h SI sysm, hs wo masss ar qual m G m (6.) Howvr, shoul b no ha n h vlop gomral nraon hory, h quvaln prnpl s no a funamnal nssy a all. If, n fuur, hs prnpl s nvala n som rang of masss, hs hory wll sll rman val. In hs hory, h gravaonal mass (harg) nus h four-momnum pr un gravaonal mass or gravaonal four-vloy U, whr U U ( U, U 4) (6.) o h hr rlav o h spa-m nral obsrvr. Baus of h quvaln prnpl, h gravaonal four-vloy fl U looks lk h four-vloy u of h parl. hs xplans why w us h symbol U o rprsn hs vloy-lk fl. By analogy o h lromagn hory, U 4 shoul b rla o h salar Nwonan ponal Φ. I wll b shorly shown ha Φ U 4 (6.3) h an-symmr four-nsor gravaonal nnsy fl s hararz by h url Ω G ( U U ) (6.4) whh s h gravaonal four-vory nu n h hr masur by an nral obsrvr analogous o F n lroynams. W hav hosn h symbol Ω o mphasz h analogy of h spa gravaonal vory o vory n lassal flu mhans. In rms of omponns G 6

Consider a system of 2 simultaneous first order linear equations

Consider a system of 2 simultaneous first order linear equations Soluon of sysms of frs ordr lnar quaons onsdr a sysm of smulanous frs ordr lnar quaons a b c d I has h alrna mar-vcor rprsnaon a b c d Or, n shorhand A, f A s alrady known from con W know ha h abov sysm

More information

Advanced Queueing Theory. M/G/1 Queueing Systems

Advanced Queueing Theory. M/G/1 Queueing Systems Advand Quung Thory Ths slds ar rad by Dr. Yh Huang of Gorg Mason Unvrsy. Sudns rgsrd n Dr. Huang's ourss a GMU an ma a sngl mahn-radabl opy and prn a sngl opy of ah sld for hr own rfrn, so long as ah sld

More information

Fluctuation-Electromagnetic Interaction of Rotating Neutral Particle with the Surface: Relativistic Theory

Fluctuation-Electromagnetic Interaction of Rotating Neutral Particle with the Surface: Relativistic Theory Fluuaon-lroagn Inraon of Roang Nural Parl w Surfa: Rlavs or A.A. Kasov an G.V. Dov as on fluuaon-lroagn or w av alula rar for of araon fronal on an ang ra of a nural parl roang nar a polarabl surfa. parl

More information

EE243 Advanced Electromagnetic Theory Lec # 10: Poynting s Theorem, Time- Harmonic EM Fields

EE243 Advanced Electromagnetic Theory Lec # 10: Poynting s Theorem, Time- Harmonic EM Fields Appl M Fall 6 Nuruhr Lcur # r 9/6/6 4 Avanc lcromagnc Thory Lc # : Poynng s Thorm Tm- armonc M Fls Poynng s Thorm Consrvaon o nrgy an momnum Poynng s Thorm or Lnar sprsv Ma Poynng s Thorm or Tm-armonc

More information

Summary: Solving a Homogeneous System of Two Linear First Order Equations in Two Unknowns

Summary: Solving a Homogeneous System of Two Linear First Order Equations in Two Unknowns Summary: Solvng a Homognous Sysm of Two Lnar Frs Ordr Equaons n Two Unknowns Gvn: A Frs fnd h wo gnvalus, r, and hr rspcv corrspondng gnvcors, k, of h coffcn mar A Dpndng on h gnvalus and gnvcors, h gnral

More information

The Variance-Covariance Matrix

The Variance-Covariance Matrix Th Varanc-Covaranc Marx Our bggs a so-ar has bn ng a lnar uncon o a s o daa by mnmzng h las squars drncs rom h o h daa wh mnsarch. Whn analyzng non-lnar daa you hav o us a program l Malab as many yps o

More information

CONTINUOUS TIME DYNAMIC PROGRAMMING

CONTINUOUS TIME DYNAMIC PROGRAMMING Eon. 511b Sprng 1993 C. Sms I. Th Opmaon Problm CONTINUOUS TIME DYNAMIC PROGRAMMING W onsdr h problm of maxmng subj o and EU(C, ) d (1) j ^ d = (C, ) d + σ (C, ) dw () h(c, ), (3) whr () and (3) hold for

More information

V A. V-A ansatz for fundamental fermions

V A. V-A ansatz for fundamental fermions Avan Parl Phy: I. ak nraon. A Thory Carfl analy of xprnal aa (pary volaon, nrno hly pn hang n nlar β-ay, on ay propr oghr w/ nvraly fnally l o h -A hory of (nlar wak ay: M A A ( ( ( ( v p A n nlon lpon

More information

The Electrodynamic Origin of the Force of Inertia (F = m i a) Part 2

The Electrodynamic Origin of the Force of Inertia (F = m i a) Part 2 h loyna On of h o of Ina ( a Pa Chals W. Luas J. 5 Lvnson Dv Mhansvll MD 65-7 bll@oonsnssn.o bsa. vw of Nwon s Pnpa [] shows hs pnn on hs xsn ho fo absolu spa an n o o xplan h fo of na an h nfual fo n

More information

t=0 t>0: + vr - i dvc Continuation

t=0 t>0: + vr - i dvc Continuation hapr Ga Dlay and rcus onnuaon s rcu Equaon >: S S Ths dffrnal quaon, oghr wh h nal condon, fully spcfs bhaor of crcu afr swch closs Our n challng: larn how o sol such quaons TUE/EE 57 nwrk analys 4/5 NdM

More information

Conventional Hot-Wire Anemometer

Conventional Hot-Wire Anemometer Convnonal Ho-Wr Anmomr cro Ho Wr Avanag much mallr prob z mm o µm br paal roluon array o h nor hghr rquncy rpon lowr co prormanc/co abrcaon roc I µm lghly op p layr 8µm havly boron op ch op layr abrcaon

More information

(heat loss divided by total enthalpy flux) is of the order of 8-16 times

(heat loss divided by total enthalpy flux) is of the order of 8-16 times 16.51, Rok Prolson Prof. Manl Marnz-Sanhz r 8: Convv Ha ransfr: Ohr Effs Ovrall Ha oss and Prforman Effs of Ha oss (1) Ovrall Ha oss h loal ha loss r n ara s q = ρ ( ) ngrad ha loss s a S, and sng m =

More information

Version 1.0 VLADIMIR V. KOROSTELEV. A Primer in Quantum Mechanics for NMR Students

Version 1.0 VLADIMIR V. KOROSTELEV. A Primer in Quantum Mechanics for NMR Students Vrson. VADMR V. KOROSTEEV A Prmr n Quanum Mhans for NMR Sudns Vladmr Koroslv, 8 vladmr.v.koroslv@ramblr.ru Tabl of Conns Conns. nroduon. Quanum Sas of Spn / 3. Opraors for Spn / 6 4. Hamlonan of spn n

More information

Supplementary Figure 1. Experiment and simulation with finite qudit. anharmonicity. (a), Experimental data taken after a 60 ns three-tone pulse.

Supplementary Figure 1. Experiment and simulation with finite qudit. anharmonicity. (a), Experimental data taken after a 60 ns three-tone pulse. Supplmnar Fgur. Eprmn and smulaon wh fn qud anharmonc. a, Eprmnal daa akn afr a 6 ns hr-on puls. b, Smulaon usng h amlonan. Supplmnar Fgur. Phagoran dnamcs n h m doman. a, Eprmnal daa. Th hr-on puls s

More information

Engineering Circuit Analysis 8th Edition Chapter Nine Exercise Solutions

Engineering Circuit Analysis 8th Edition Chapter Nine Exercise Solutions Engnrng rcu naly 8h Eon hapr Nn Exrc Soluon. = KΩ, = µf, an uch ha h crcu rpon oramp. a For Sourc-fr paralll crcu: For oramp or b H 9V, V / hoo = H.7.8 ra / 5..7..9 9V 9..9..9 5.75,.5 5.75.5..9 . = nh,

More information

Vertical Sound Waves

Vertical Sound Waves Vral Sond Wavs On an drv h formla for hs avs by onsdrn drly h vral omonn of momnm qaon hrmodynam qaon and h onny qaon from 5 and hn follon h rrbaon mhod and assmn h snsodal solons. Effvly h frs ro and

More information

NAME: ANSWER KEY DATE: PERIOD. DIRECTIONS: MULTIPLE CHOICE. Choose the letter of the correct answer.

NAME: ANSWER KEY DATE: PERIOD. DIRECTIONS: MULTIPLE CHOICE. Choose the letter of the correct answer. R A T T L E R S S L U G S NAME: ANSWER KEY DATE: PERIOD PREAP PHYSICS REIEW TWO KINEMATICS / GRAPHING FORM A DIRECTIONS: MULTIPLE CHOICE. Chs h r f h rr answr. Us h fgur bw answr qusns 1 and 2. 0 10 20

More information

Exponential Stability Analysis of a System Comprised of a Robot and its Associated Safety Mechanism

Exponential Stability Analysis of a System Comprised of a Robot and its Associated Safety Mechanism rongs of nnul onfrn of hn nsu of ommunons Eponnl Sbl nlss of Ssm omprs of obo n s sso Sf Mhnsm Whu GUO ng YNG prmn of Mhms n nforms sn Zhngzhou Unvrs of lgh nusr Zhngzhou hn; E-ml: whguosr@hooomn; ngp66@hoon

More information

MA1506 Tutorial 2 Solutions. Question 1. (1a) 1 ) y x. e x. 1 exp (in general, Integrating factor is. ye dx. So ) (1b) e e. e c.

MA1506 Tutorial 2 Solutions. Question 1. (1a) 1 ) y x. e x. 1 exp (in general, Integrating factor is. ye dx. So ) (1b) e e. e c. MA56 utorial Solutions Qustion a Intgrating fator is ln p p in gnral, multipl b p So b ln p p sin his kin is all a Brnoulli quation -- st Sin w fin Y, Y Y, Y Y p Qustion Dfin v / hn our quation is v μ

More information

Chapter 7 Stead St y- ate Errors

Chapter 7 Stead St y- ate Errors Char 7 Say-Sa rror Inroucon Conrol ym analy an gn cfcaon a. rann ron b. Sably c. Say-a rror fnon of ay-a rror : u c a whr u : nu, c: ouu Val only for abl ym chck ym ably fr! nu for ay-a a nu analy U o

More information

Frequency Response. Response of an LTI System to Eigenfunction

Frequency Response. Response of an LTI System to Eigenfunction Frquncy Rsons Las m w Rvsd formal dfnons of lnary and m-nvaranc Found an gnfuncon for lnar m-nvaran sysms Found h frquncy rsons of a lnar sysm o gnfuncon nu Found h frquncy rsons for cascad, fdbac, dffrnc

More information

Appendix. In the absence of default risk, the benefit of the tax shield due to debt financing by the firm is 1 C E C

Appendix. In the absence of default risk, the benefit of the tax shield due to debt financing by the firm is 1 C E C nx. Dvon o h n wh In h sn o ul sk h n o h x shl u o nnng y h m s s h ol ouon s h num o ssus s h oo nom x s h sonl nom x n s h v x on quy whh s wgh vg o vn n l gns x s. In hs s h o sonl nom xs on h x shl

More information

EE105 Fall 2015 Microelectronic Devices and Circuits. LTI: Linear Time-Invariant System

EE105 Fall 2015 Microelectronic Devices and Circuits. LTI: Linear Time-Invariant System EE5 Fall 5 Mrolron Dvs and Crus Prof. Mng C. Wu wu@s.rkl.du 5 Suarda Da all SD - LTI: Lnar Tm-Invaran Ssm Ssm s lnar sudd horoughl n 6AB: Ssm s m nvaran: Thr s no lok or m rfrn Th ransfr funon s no a funon

More information

The Mathematics of Harmonic Oscillators

The Mathematics of Harmonic Oscillators Th Mhcs of Hronc Oscllors Spl Hronc Moon In h cs of on-nsonl spl hronc oon (SHM nvolvng sprng wh sprng consn n wh no frcon, you rv h quon of oon usng Nwon's scon lw: con wh gvs: 0 Ths s sos wrn usng h

More information

1. Quark mixing and CKM matrix

1. Quark mixing and CKM matrix Avan arl hy: IX. Flavor Ollaon an C olaon IX. Flavor ollaon an C volaon. Quark xng an h CM arx. Flavor ollaon: Mxng o nural on 3. C volaon. Nurno ollaon. Quark xng an CM arx. Quark xng: Ma gna ar no ual

More information

Workshop Neckarzimmern. Symmetries Standard Model Langrangian Higgs Coupling to Quarks and Mass Generation CKM Matrix Unitarity Triangles Mixing

Workshop Neckarzimmern. Symmetries Standard Model Langrangian Higgs Coupling to Quarks and Mass Generation CKM Matrix Unitarity Triangles Mixing Workhop Nkarzrn Syr Sanar Mol angrangan gg Couplng o Quark an Ma Gnraon CKM Marx Unary Trangl Mxng Syr T.D.: Th roo o all yry prnpl l n h aupon ha pobl o obrv ran ba quan; h non-obrvabl Thr ar four an

More information

9.4 Absorption and Dispersion

9.4 Absorption and Dispersion 9.4 Absoon and Dsson 9.4. loagn Wavs n Conduos un dnsy n a onduo ollowng Oh s law: J Th Maxwll s uaons n a onduo lna da should b: ρ B B B J To sly h suaon w agu ha h hag dsaas uly n a aoso od. Fo h onnuy

More information

Electromagnetic waves in vacuum.

Electromagnetic waves in vacuum. leromagne waves n vauum. The dsovery of dsplaemen urrens enals a peular lass of soluons of Maxwell equaons: ravellng waves of eler and magne felds n vauum. In he absene of urrens and harges, he equaons

More information

Uncalibrated Visual Servoing of Nonholonomic Mobile Robots

Uncalibrated Visual Servoing of Nonholonomic Mobile Robots 23 IEEE/J Inrnaonal Conrn on Inllgn obos an ysms (IO) Nombr 3-7, 23 okyo, Japan Unalbra Vsal rong o Nonholonom Mobl obos Baoqan L, Yonghn ang, nor Mmbr, IEEE, an Xbo Zhang, Mmbr, IEEE Absra In hs papr,

More information

Chapter 2: Semi-Classical Light- Matter Interaction

Chapter 2: Semi-Classical Light- Matter Interaction Quanum Ops for Phoons and Opolrons (Farhan ana, Cornll Unvrs) Chapr : Sm-Classal Lgh- Mar Inraon. A Two-lvl Ssm Inrang wh Classal Elromagn Fld n h Absn of Dohrn.. Hamlonan for Inraon bwn Lgh and a Two-lvl

More information

Chapter 8 Theories of Systems

Chapter 8 Theories of Systems ~~ 7 Char Thor of Sm - Lala Tranform Solon of Lnar Sm Lnar Sm F : Conr n a n- n- a n- n- a a f L n n- ' ' ' n n n a a a a f Eg - an b ranform no ' ' b an b Lala ranform Sol Lf ]F-f 7 C 7 C C C ] a L a

More information

Article Nonlinear Theory of Elementary Particles: VI. Electrodynamic Sense of the Quantum Forms of Dirac Electron Theory. Alexander G.

Article Nonlinear Theory of Elementary Particles: VI. Electrodynamic Sense of the Quantum Forms of Dirac Electron Theory. Alexander G. 58 Arl Nonlnar Thor o lnar Parls: VI. lrodna Sns o h Quanu Fors o Dra Alandr G. Krakos * Absra In h prsn papr s shown ha a ull orrspondn bwn h quanu and h lroagn ors o h Dra lron hor ss so ha ah ln o h

More information

Homework: Introduction to Motion

Homework: Introduction to Motion Homwork: Inroducon o Moon Dsanc vs. Tm Graphs Nam Prod Drcons: Answr h foowng qusons n h spacs provdd. 1. Wha do you do o cra a horzona n on a dsancm graph? 2. How do you wak o cra a sragh n ha sops up?

More information

Chapter 7. Now, for 2) 1. 1, if z = 1, Thus, Eq. (7.20) holds

Chapter 7. Now, for 2) 1. 1, if z = 1, Thus, Eq. (7.20) holds Chapr 7, n, 7 Ipuls rspons of h ovng avrag flr s: h[, ohrws sn / / Is frquny rspons s: sn / Now, for a BR ransfr funon,, For h ovng-avrag flr, sn / W shall show by nduon ha sn / sn / sn /,, Now, for sn

More information

Mechanics Physics 151

Mechanics Physics 151 Mechancs Physcs 5 Lecure 0 Canoncal Transformaons (Chaper 9) Wha We Dd Las Tme Hamlon s Prncple n he Hamlonan formalsm Dervaon was smple δi δ Addonal end-pon consrans pq H( q, p, ) d 0 δ q ( ) δq ( ) δ

More information

t the propensity to consume the resource good. Maximizing U t in (9) subject to the budget constraint (8) yields

t the propensity to consume the resource good. Maximizing U t in (9) subject to the budget constraint (8) yields ISB 978-9-84468-8-5 Innaonal Confn on Issus n Busnss onoms Mang an Mamas (IBMM-6) Sngapo 5-6 6 Busnss Cls Capal nvonmn an Rnabl Rsous W-Bn Zang Rsuman Asa Paf Unvs Bppu-s Japan Absa: Ts pap nfs busnss

More information

Double Slits in Space and Time

Double Slits in Space and Time Doubl Slis in Sac an Tim Gorg Jons As has bn ror rcnly in h mia, a am l by Grhar Paulus has monsra an inrsing chniqu for ionizing argon aoms by using ulra-shor lasr ulss. Each lasr uls is ffcivly on an

More information

Generalized Den Hartog tuned mass damper system for control of vibrations in structures

Generalized Den Hartog tuned mass damper system for control of vibrations in structures Earhqua Rssan Engnrng Sruurs VII 85 Gnralzd Dn Harog und ass dapr sys for onrol of vbraons n sruurs I. M. Abubaar B. J. M. ard Dparn of Cvl Engnrng, auly of Engnrng, Alahad Unvrsy, Sr, Lbya Absra Th Dn

More information

Control Systems (Lecture note #6)

Control Systems (Lecture note #6) 6.5 Corol Sysms (Lcur o #6 Las Tm: Lar algbra rw Lar algbrac quaos soluos Paramrzao of all soluos Smlary rasformao: compao form Egalus ad gcors dagoal form bg pcur: o brach of h cours Vcor spacs marcs

More information

Integrated Optical Waveguides

Integrated Optical Waveguides Su Opls Faha Raa Cll Uvs Chap 8 Ia Opal Wavus 7 Dl Slab Wavus 7 Iu: A va f ff a pal wavus a us f a u lh a hp Th s bas pal wavu s a slab wavus shw blw Th suu s uf h - Lh s u s h b al al fl a h -la fas Cla

More information

Lecture 4: Laplace Transforms

Lecture 4: Laplace Transforms Lur 4: Lapla Transforms Lapla and rlad ransformaions an b usd o solv diffrnial quaion and o rdu priodi nois in signals and imags. Basially, hy onvr h drivaiv opraions ino mulipliaion, diffrnial quaions

More information

State Observer Design

State Observer Design Sa Obsrvr Dsgn A. Khak Sdgh Conrol Sysms Group Faculy of Elcrcal and Compur Engnrng K. N. Toos Unvrsy of Tchnology Fbruary 2009 1 Problm Formulaon A ky assumpon n gnvalu assgnmn and sablzng sysms usng

More information

4.1 The Uniform Distribution Def n: A c.r.v. X has a continuous uniform distribution on [a, b] when its pdf is = 1 a x b

4.1 The Uniform Distribution Def n: A c.r.v. X has a continuous uniform distribution on [a, b] when its pdf is = 1 a x b 4. Th Uniform Disribuion Df n: A c.r.v. has a coninuous uniform disribuion on [a, b] whn is pdf is f x a x b b a Also, b + a b a µ E and V Ex4. Suppos, h lvl of unblivabiliy a any poin in a Transformrs

More information

Three dimensional viscoelastic medium under thermal shock

Three dimensional viscoelastic medium under thermal shock Engnrng Sol Mhans 4 6 87- Conns lss aalabl a GrongSn Engnrng Sol Mhans hompag:.grongsn.om/sm hr mnsonal solas mm nr hrmal shok Abhk Sr * an M. Kanora Dparmn of Appl Mahmas Unrs of Cala 9 A.P.C. Roa Kolkaa-79

More information

) and furthermore all X. The definition of the term stationary requires that the distribution fulfills the condition:

) and furthermore all X. The definition of the term stationary requires that the distribution fulfills the condition: Assigm Thomas Aam, Spha Brumm, Haik Lor May 6 h, 3 8 h smsr, 357, 7544, 757 oblm For R b X a raom variabl havig ormal isribuio wih ma µ a variac σ (his is wri as ~ (,) X. by: R a. Is X ) a urhrmor all

More information

Bethe-Salpeter Equation Green s Function and the Bethe-Salpeter Equation for Effective Interaction in the Ladder Approximation

Bethe-Salpeter Equation Green s Function and the Bethe-Salpeter Equation for Effective Interaction in the Ladder Approximation Bh-Salp Equaon n s Funcon and h Bh-Salp Equaon fo Effcv Inacon n h Ladd Appoxmaon Csa A. Z. Vasconcllos Insuo d Físca-UFRS - upo: Físca d Hadons Sngl-Pacl Popagao. Dagam xpanson of popagao. W consd as

More information

Gauge Theories. Elementary Particle Physics Strong Interaction Fenomenology. Diego Bettoni Academic year

Gauge Theories. Elementary Particle Physics Strong Interaction Fenomenology. Diego Bettoni Academic year Gau Thors Elmary Parcl Physcs Sro Iraco Fomoloy o Bo cadmc yar - Gau Ivarac Gau Ivarac Whr do Laraas or Hamloas com from? How do w kow ha a cra raco should dscrb a acual hyscal sysm? Why s h lcromac raco

More information

Chaos and Correlation January 8, 2012

Chaos and Correlation January 8, 2012 Chaos and Corrlaon January 8, Chaos and Corrlaon Inrnaonal Journal, January 8, Квантовая электродинамика Лоренца Lornz quanu lrodynas landr P. Trunv (Torono, Canada) landr P. Trunv Обсуждается вопрос о

More information

9. Simple Rules for Monetary Policy

9. Simple Rules for Monetary Policy 9. Smpl Ruls for Monar Polc John B. Talor, Ma 0, 03 Woodford, AR 00 ovrvw papr Purpos s o consdr o wha xn hs prscrpon rsmbls h sor of polc ha conomc hor would rcommnd Bu frs, l s rvw how hs sor of polc

More information

10.5 Linear Viscoelasticity and the Laplace Transform

10.5 Linear Viscoelasticity and the Laplace Transform Scn.5.5 Lnar Vclacy and h Lalac ranfrm h Lalac ranfrm vry uful n cnrucng and analyng lnar vclac mdl..5. h Lalac ranfrm h frmula fr h Lalac ranfrm f h drvav f a funcn : L f f L f f f f f c..5. whr h ranfrm

More information

OUTLINE FOR Chapter 2-2. Basic Laws

OUTLINE FOR Chapter 2-2. Basic Laws 0//8 OUTLINE FOR Chapr - AERODYNAMIC W-- Basc Laws Analss of an problm n fld mchancs ncssarl nclds samn of h basc laws gornng h fld moon. Th basc laws, whch applcabl o an fld, ar: Consraon of mass Conn

More information

Partition Functions for independent and distinguishable particles

Partition Functions for independent and distinguishable particles 0.0J /.77J / 5.60J hrodynacs of oolcular Syss Insrucors: Lnda G. Grffh, Kbrly Haad-Schffrl, Moung G. awnd, Robr W. Fld Lcur 5 5.60/0.0/.77 vs. q for dsngushabl vs ndsngushabl syss Drvaon of hrodynac Proprs

More information

Final Exam : Solutions

Final Exam : Solutions Comp : Algorihm and Daa Srucur Final Exam : Soluion. Rcuriv Algorihm. (a) To bgin ind h mdian o {x, x,... x n }. Sinc vry numbr xcp on in h inrval [0, n] appar xacly onc in h li, w hav ha h mdian mu b

More information

CSE 245: Computer Aided Circuit Simulation and Verification

CSE 245: Computer Aided Circuit Simulation and Verification CSE 45: Compur Aidd Circui Simulaion and Vrificaion Fall 4, Sp 8 Lcur : Dynamic Linar Sysm Oulin Tim Domain Analysis Sa Equaions RLC Nwork Analysis by Taylor Expansion Impuls Rspons in im domain Frquncy

More information

INF5820 MT 26 OCT 2012

INF5820 MT 26 OCT 2012 INF582 MT 26 OCT 22 H22 Jn Tor Lønnng l@.uo.no Tody Ssl hn rnslon: Th nosy hnnl odl Word-bsd IBM odl Trnng SMT xpl En o lgd n r d bygg..9 h.6 d.3.9 rgh.9 wh.4 buldng.45 oo.3 rd.25 srgh.7 by.3 onsruon.33

More information

Chapter 13 Laplace Transform Analysis

Chapter 13 Laplace Transform Analysis Chapr aplac Tranorm naly Chapr : Ouln aplac ranorm aplac Tranorm -doman phaor analy: x X σ m co ω φ x X X m φ x aplac ranorm: [ o ] d o d < aplac Tranorm Thr condon Unlaral on-dd aplac ranorm: aplac ranorm

More information

innovations shocks white noise

innovations shocks white noise Innovaons Tm-srs modls ar consrucd as lnar funcons of fundamnal forcasng rrors, also calld nnovaons or shocks Ths basc buldng blocks sasf var σ Srall uncorrlad Ths rrors ar calld wh nos In gnral, f ou

More information

Practice papers A and B, produced by Edexcel in 2009, with mark schemes. Practice Paper A. 5 cosh x 2 sinh x = 11,

Practice papers A and B, produced by Edexcel in 2009, with mark schemes. Practice Paper A. 5 cosh x 2 sinh x = 11, Prai paprs A ad B, produd by Edl i 9, wih mark shms Prai Papr A. Fid h valus of for whih 5 osh sih =, givig your aswrs as aural logarihms. (Toal 6 marks) k. A = k, whr k is a ral osa. 9 (a) Fid valus of

More information

Lecture 4 : Backpropagation Algorithm. Prof. Seul Jung ( Intelligent Systems and Emotional Engineering Laboratory) Chungnam National University

Lecture 4 : Backpropagation Algorithm. Prof. Seul Jung ( Intelligent Systems and Emotional Engineering Laboratory) Chungnam National University Lcur 4 : Bacpropagaon Algorhm Pro. Sul Jung Inllgn Sm and moonal ngnrng Laboraor Chungnam Naonal Unvr Inroducon o Bacpropagaon algorhm 969 Mn and Papr aac. 980 Parr and Wrbo dcovrd bac propagaon algorhm.

More information

Lecture 1: Numerical Integration The Trapezoidal and Simpson s Rule

Lecture 1: Numerical Integration The Trapezoidal and Simpson s Rule Lcur : Numrical ngraion Th Trapzoidal and Simpson s Rul A problm Th probabiliy of a normally disribud (man µ and sandard dviaion σ ) vn occurring bwn h valus a and b is B A P( a x b) d () π whr a µ b -

More information

Institute of Actuaries of India

Institute of Actuaries of India Insiu of Acuaris of India ubjc CT3 Probabiliy and Mahmaical aisics Novmbr Examinaions INDICATIVE OLUTION Pag of IAI CT3 Novmbr ol. a sampl man = 35 sampl sandard dviaion = 36.6 b for = uppr bound = 35+*36.6

More information

New Mexico Tech Hyd 510

New Mexico Tech Hyd 510 New Meo eh Hy 5 Hyrology Program Quanave Mehos n Hyrology Noe ha for he sep hange problem,.5, for >. he sep smears over me an, unlke he ffuson problem, he onenraon a he orgn hanges. I s no a bounary onon.

More information

On the Existence and uniqueness for solution of system Fractional Differential Equations

On the Existence and uniqueness for solution of system Fractional Differential Equations OSR Jourl o Mhms OSR-JM SSN: 78-578. Volum 4 ssu 3 Nov. - D. PP -5 www.osrjourls.org O h Es d uquss or soluo o ssm rol Drl Equos Mh Ad Al-Wh Dprm o Appld S Uvrs o holog Bghdd- rq Asr: hs ppr w d horm o

More information

A L A BA M A L A W R E V IE W

A L A BA M A L A W R E V IE W A L A BA M A L A W R E V IE W Volume 52 Fall 2000 Number 1 B E F O R E D I S A B I L I T Y C I V I L R I G HT S : C I V I L W A R P E N S I O N S A N D TH E P O L I T I C S O F D I S A B I L I T Y I N

More information

Decline Curves. Exponential decline (constant fractional decline) Harmonic decline, and Hyperbolic decline.

Decline Curves. Exponential decline (constant fractional decline) Harmonic decline, and Hyperbolic decline. Dlin Curvs Dlin Curvs ha lo flow ra vs. im ar h mos ommon ools for forasing roduion and monioring wll rforman in h fild. Ths urvs uikly show by grahi mans whih wlls or filds ar roduing as xd or undr roduing.

More information

Midterm exam 2, April 7, 2009 (solutions)

Midterm exam 2, April 7, 2009 (solutions) Univrsiy of Pnnsylvania Dparmn of Mahmaics Mah 26 Honors Calculus II Spring Smsr 29 Prof Grassi, TA Ashr Aul Midrm xam 2, April 7, 29 (soluions) 1 Wri a basis for h spac of pairs (u, v) of smooh funcions

More information

P a g e 5 1 of R e p o r t P B 4 / 0 9

P a g e 5 1 of R e p o r t P B 4 / 0 9 P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e

More information

The Procedure Abstraction Part II: Symbol Tables and Activation Records

The Procedure Abstraction Part II: Symbol Tables and Activation Records Th Produr Absrion Pr II: Symbol Tbls nd Aivion Rords Th Produr s Nm Sp Why inrodu lxil soping? Provids ompil-im mhnism for binding vribls Ls h progrmmr inrodu lol nms How n h ompilr kp rk of ll hos nms?

More information

ELEN E4830 Digital Image Processing

ELEN E4830 Digital Image Processing ELEN E48 Dgal Imag Procssng Mrm Eamnaon Sprng Soluon Problm Quanzaon and Human Encodng r k u P u P u r r 6 6 6 6 5 6 4 8 8 4 P r 6 6 P r 4 8 8 6 8 4 r 8 4 8 4 7 8 r 6 6 6 6 P r 8 4 8 P r 6 6 8 5 P r /

More information

CHAPTER-2. S.No Name of the Sub-Title No. 2.5 Use of Modified Heffron Phillip's model in Multi- Machine Systems 32

CHAPTER-2. S.No Name of the Sub-Title No. 2.5 Use of Modified Heffron Phillip's model in Multi- Machine Systems 32 9 HAPT- hapr : MODIFID HFFON PHILLIP MODL.No Nam of h ub-tl Pag No.. Inroucon..3 Mollng of Powr ym Hffron Phllp Mol.4 Mof Hffron Phllp Mol 7.5 U of Mof Hffron Phllp mol n Mul- Machn ym 3 HAPT-.. Inroucon

More information

EE 247B/ME 218: Introduction to MEMS Design Lecture 27m2: Gyros, Noise & MDS CTN 5/1/14. Copyright 2014 Regents of the University of California

EE 247B/ME 218: Introduction to MEMS Design Lecture 27m2: Gyros, Noise & MDS CTN 5/1/14. Copyright 2014 Regents of the University of California MEMSBase Fork Gyrosoe Ω r z Volage Deermnng Resoluon EE C45: Inrouon o MEMS Desgn LeM 15 C. Nguyen 11/18/08 17 () Curren (+) Curren Eleroe EE C45: Inrouon o MEMS Desgn LeM 15 C. Nguyen 11/18/08 18 [Zaman,

More information

SIMEON BALL AND AART BLOKHUIS

SIMEON BALL AND AART BLOKHUIS A BOUND FOR THE MAXIMUM WEIGHT OF A LINEAR CODE SIMEON BALL AND AART BLOKHUIS Absrac. I s shown ha h paramrs of a lnar cod ovr F q of lngh n, dmnson k, mnmum wgh d and maxmum wgh m sasfy a cran congrunc

More information

Canonical Quantizing of Spinor Fields: Anti-Commutation Relations

Canonical Quantizing of Spinor Fields: Anti-Commutation Relations JOURNA ON POTONICS AND SPINTRONICS VO.5 NO. MAY 6 ISSN - 857 Prn ISSN - 858 Onln h://www.rrh.org/jornl/j/j.hml Cnonl Qnzng of Snor Fl: An-Common Rlon D. Grn PhD Unvr of Brln* Ar Nw mg of hr nor ro on h

More information

Pupil / Class Record We can assume a word has been learned when it has been either tested or used correctly at least three times.

Pupil / Class Record We can assume a word has been learned when it has been either tested or used correctly at least three times. 2 Pupi / Css Rr W ssum wr hs b r wh i hs b ihr s r us rry s hr ims. Nm: D Bu: fr i bus brhr u firs hf hp hm s uh i iv iv my my mr muh m w ih w Tik r pp push pu sh shu sisr s sm h h hir hr hs im k w vry

More information

Boyce/DiPrima 9 th ed, Ch 7.8: Repeated Eigenvalues

Boyce/DiPrima 9 th ed, Ch 7.8: Repeated Eigenvalues Boy/DiPrima 9 h d Ch 7.8: Rpad Eignvalus Elmnary Diffrnial Equaions and Boundary Valu Problms 9 h diion by William E. Boy and Rihard C. DiPrima 9 by John Wily & Sons In. W onsidr again a homognous sysm

More information

Charging of capacitor through inductor and resistor

Charging of capacitor through inductor and resistor cur 4&: R circui harging of capacior hrough inducor and rsisor us considr a capacior of capacianc is conncd o a D sourc of.m.f. E hrough a rsisr of rsisanc R, an inducor of inducanc and a y K in sris.

More information

8. Queueing systems. Contents. Simple teletraffic model. Pure queueing system

8. Queueing systems. Contents. Simple teletraffic model. Pure queueing system 8. Quug sysms Cos 8. Quug sysms Rfrshr: Sml lraffc modl Quug dscl M/M/ srvr wag lacs Alcao o ack lvl modllg of daa raffc M/M/ srvrs wag lacs lc8. S-38.45 Iroduco o Tlraffc Thory Srg 5 8. Quug sysms 8.

More information

Lecture 12: Introduction to nonlinear optics II.

Lecture 12: Introduction to nonlinear optics II. Lcur : Iroduco o olar opcs II r Kužl ropagao of srog opc sgals propr olar ffcs Scod ordr ffcs! Thr-wav mxg has machg codo! Scod harmoc grao! Sum frqucy grao! aramrc grao Thrd ordr ffcs! Four-wav mxg! Opcal

More information

EE"232"Lightwave"Devices Lecture"16:"p7i7n"Photodiodes"and" Photoconductors"

EE232LightwaveDevices Lecture16:p7i7nPhotodiodesand Photoconductors EE"232"Lgwav"Dvcs Lcur"16:"p77n"Pooos"an" Pooconucors" Rang:"Cuang,"Cap."15"(2 n E) Insrucor:"Mng"C."Wu Unvrsy"of"Calforna,"Brkly Elcrcal"Engnrng"an"Compur"Scncs"Dp. EE232$Lcur$16-1 Rvrs"bas%p""n%juncon

More information

Chapter 9 Transient Response

Chapter 9 Transient Response har 9 Transn sons har 9: Ouln N F n F Frs-Ordr Transns Frs-Ordr rcus Frs ordr crcus: rcus conan onl on nducor or on caacor gornd b frs-ordr dffrnal quaons. Zro-nu rsons: h crcu has no ald sourc afr a cran

More information

PHYS ,Fall 05, Term Exam #1, Oct., 12, 2005

PHYS ,Fall 05, Term Exam #1, Oct., 12, 2005 PHYS1444-,Fall 5, Trm Exam #1, Oct., 1, 5 Nam: Kys 1. circular ring of charg of raius an a total charg Q lis in th x-y plan with its cntr at th origin. small positiv tst charg q is plac at th origin. What

More information

10. If p and q are the lengths of the perpendiculars from the origin on the tangent and the normal to the curve

10. If p and q are the lengths of the perpendiculars from the origin on the tangent and the normal to the curve 0. If p and q ar h lnghs of h prpndiculars from h origin on h angn and h normal o h curv + Mahmaics y = a, hn 4p + q = a a (C) a (D) 5a 6. Wha is h diffrnial quaion of h family of circls having hir cnrs

More information

Special Curves of 4D Galilean Space

Special Curves of 4D Galilean Space Irol Jourl of Mhml Egrg d S ISSN : 77-698 Volum Issu Mrh hp://www.jms.om/ hps://ss.googl.om/s/jmsjourl/ Spl Curvs of D ll Sp Mhm Bkş Mhmu Ergü Alpr Osm Öğrmş Fır Uvrsy Fuly of S Dprm of Mhms 9 Elzığ Türky

More information

TRASH ENCLOSURE WITH SOLID GATE 4 STORY BUSINESS / RESIDENTIAL BUILDING CONTAINING 2 BUSINESS SPACES AND 6 DWELLING UNITS 6' - 0"

TRASH ENCLOSURE WITH SOLID GATE 4 STORY BUSINESS / RESIDENTIAL BUILDING CONTAINING 2 BUSINESS SPACES AND 6 DWELLING UNITS 6' - 0 NSN N. PUN WY R. P 0. SG S 4 SRY USNSS / RSN UNG NNNG USNSS SPS N 6 WNG UNS RS NSUR W S G.. RSRV PRKNG $50 N SGN RV S (7) UR PRKNG SPS ' - PRPRY N M N, YP PU Y SG RNGS S GNR NS 6" G UR rchitecture nteriors

More information

UNIT #5 EXPONENTIAL AND LOGARITHMIC FUNCTIONS

UNIT #5 EXPONENTIAL AND LOGARITHMIC FUNCTIONS Answr Ky Nam: Da: UNIT # EXPONENTIAL AND LOGARITHMIC FUNCTIONS Par I Qusions. Th prssion is quivaln o () () 6 6 6. Th ponnial funcion y 6 could rwrin as y () y y 6 () y y (). Th prssion a is quivaln o

More information

September 27, Introduction to Ordinary Differential Equations. ME 501A Seminar in Engineering Analysis Page 1. Outline

September 27, Introduction to Ordinary Differential Equations. ME 501A Seminar in Engineering Analysis Page 1. Outline Introucton to Ornar Dffrntal Equatons Sptmbr 7, 7 Introucton to Ornar Dffrntal Equatons Larr artto Mchancal Engnrng AB Smnar n Engnrng Analss Sptmbr 7, 7 Outln Rvw numrcal solutons Bascs of ffrntal quatons

More information

Mechanics Physics 151

Mechanics Physics 151 Mechancs Physcs 5 Lecure 9 Hamlonan Equaons of Moon (Chaper 8) Wha We Dd Las Tme Consruced Hamlonan formalsm H ( q, p, ) = q p L( q, q, ) H p = q H q = p H = L Equvalen o Lagrangan formalsm Smpler, bu

More information

Overview. Splay trees. Balanced binary search trees. Inge Li Gørtz. Self-adjusting BST (Sleator-Tarjan 1983).

Overview. Splay trees. Balanced binary search trees. Inge Li Gørtz. Self-adjusting BST (Sleator-Tarjan 1983). Ovrvw Bn nr rh r: R-k r n -- r 00 Ing L Gør Amor n Dnm rogrmmng Nwork fow Srng mhng Srng nng Comuon gomr Inrouon o NP-omn Rnom gorhm Bn nr rh r -- r. Aow,, or k r no Prf n. Evr h from roo o f h m ngh.

More information

Mechanics Physics 151

Mechanics Physics 151 Mechancs Physcs 5 Lecure 9 Hamlonan Equaons of Moon (Chaper 8) Wha We Dd Las Tme Consruced Hamlonan formalsm Hqp (,,) = qp Lqq (,,) H p = q H q = p H L = Equvalen o Lagrangan formalsm Smpler, bu wce as

More information

A universal saturation controller design for mobile robots

A universal saturation controller design for mobile robots A unvrsal sauraon conrollr sgn for mobl robos K.D. Do,,Z.P.Jang an J. Pan Dparmn of Elcrcal an Compur Engnrng, Polychnc Unvrsy, NY, USA. Emal: uc@mch.uwa.u.au, zjang@conrol.poly.u Dparmn of Mchancal Engnrng,

More information

Wave Superposition Principle

Wave Superposition Principle Physcs 36: Was Lcur 5 /7/8 Wa Suroson Prncl I s qu a common suaon for wo or mor was o arr a h sam on n sac or o xs oghr along h sam drcon. W wll consdr oday sral moran cass of h combnd ffcs of wo or mor

More information

On the Speed of Heat Wave. Mihály Makai

On the Speed of Heat Wave. Mihály Makai On h Spd of Ha Wa Mihály Maai maai@ra.bm.hu Conns Formulaion of h problm: infini spd? Local hrmal qulibrium (LTE hypohsis Balanc quaion Phnomnological balanc Spd of ha wa Applicaion in plasma ranspor 1.

More information

Motivation. Loop-suppressed B meson decays can serve as sensitive probes for New Physics:

Motivation. Loop-suppressed B meson decays can serve as sensitive probes for New Physics: Prong Nw Phy wh mon ay Ulrh Uwr Conn: Movaon Quark flavor phy n h Sanar Mol Exprmnal Sau Flavor phy yon h Sanar Mol HC Exprmn mon ky maurmn a h HC Movaon oop-uppr mon ay an rv a nv pro for Nw Phy: W Nw

More information

Response of MDOF systems

Response of MDOF systems Response of MDOF syses Degree of freedo DOF: he nu nuber of ndependen coordnaes requred o deerne copleely he posons of all pars of a syse a any nsan of e. wo DOF syses hree DOF syses he noral ode analyss

More information

CH.3. COMPATIBILITY EQUATIONS. Continuum Mechanics Course (MMC) - ETSECCPB - UPC

CH.3. COMPATIBILITY EQUATIONS. Continuum Mechanics Course (MMC) - ETSECCPB - UPC CH.3. COMPATIBILITY EQUATIONS Connuum Mechancs Course (MMC) - ETSECCPB - UPC Overvew Compably Condons Compably Equaons of a Poenal Vecor Feld Compably Condons for Infnesmal Srans Inegraon of he Infnesmal

More information

Reliability Analysis of a Bridge and Parallel Series Networks with Critical and Non- Critical Human Errors: A Block Diagram Approach.

Reliability Analysis of a Bridge and Parallel Series Networks with Critical and Non- Critical Human Errors: A Block Diagram Approach. Inrnaional Journal of Compuaional Sin and Mahmais. ISSN 97-3189 Volum 3, Numr 3 11, pp. 351-3 Inrnaional Rsarh Puliaion Hous hp://www.irphous.om Rliailiy Analysis of a Bridg and Paralll Sris Nworks wih

More information

An N-Component Series Repairable System with Repairman Doing Other Work and Priority in Repair

An N-Component Series Repairable System with Repairman Doing Other Work and Priority in Repair Mor ppl Novmbr 8 N-Compo r Rparabl m h Rparma Dog Ohr ork a ror Rpar Jag Yag E-mal: jag_ag7@6om Xau Mg a uo hg ollag arb Normal Uvr Yaq ua Taoao ag uppor b h Fouao or h aural o b prov o Cha 5 uppor b h

More information

Chain DOUBLE PITCH TYPE RS TYPE RS POLY-STEEL TYPE

Chain DOUBLE PITCH TYPE RS TYPE RS POLY-STEEL TYPE d Fr Flw OULE IC YE YE OLY-EEL YE Oubard wh d s (d ) s usd fr fr flw vya. Usually w srads ar usd h qupm. d s basd sadard rllr ha wh sd rllrs salld xdd ps. hr ar hr yps f bas ha: (1) ubl ph rllr ha wh sadard

More information

Nikon i-line Glass Series

Nikon i-line Glass Series Nkon ln la S ln la VNTS Nkon a an vlopmn of qualy maal a alway bn la o n fo ompany opal pou. Pon ky fao. van n la noloy pn upon pon, an a Nkon xl. Nkon ln la wa vlop fo u w ln ( nm) loapy un. I lv anman

More information