The Circular Current Loop as a Model of Fundamental Particles

Size: px
Start display at page:

Download "The Circular Current Loop as a Model of Fundamental Particles"

Transcription

1 Th iul ut Loop s Modl of Fudtl Ptils D.-Ig. Güth Ldvogt Stuwg 9 Hug Gy -il: g.ldvogt@li-dsl.t Astt. Th pstd iul ut loop odl vls tht hgd fudtl ptils suh s th lto osist sstilly of lti d gti gy. Th gti poptis hv th s od of gitud s th lti os. Th ltogti fild gy is th oigi of th itil ss. Th Higgs oso, xistig o ot, is ot dd to xpli ptil ss. Th w d stog ul fos othig ls th gti fos. Th W d Z osos s wll s th gluos ot t ll od i gluig y ptils togth. Th gti ot of fudtl ptils is ot olous! Th oly idits th xist of sll dditiol out of iti gy. Thus fudtl ptils ot puly fild-li suh s photos d ot (sstilly) ss-li suh s tos, thy pst spil id of tt i tw. Thi iti gy is oviously ot du to y ltivisti fft, ut is ltd to idpdt physil lw tht povids, togth with th gti gy, th gul otu xtly to ћ/. Fudtl ptils (t lst) two-disiol. I th siplst s thi o osists of two oti, ly idtil ut loops. Thi ltiv dsig dtils, th oly fto, d th ottiol vloity of th uifoly distiutd lty hg follow fo th stility oditio, i.. lti d gti fo l, d do ot dpd o th ptil s st ss! Fudtl ptils ojts of lssil physis.. Physil Poptis of Fudtl Ptils. Sutoi ptils tht ot sudividd gdd to fudtl. This iluds tht thy stl. Typil fudtl ptils i this ss th lto d th posito. This ivstigtio is povisiolly stitd to th. Thy htid y th followig fou si titis: hg ± oly of gti ot st-ss o gul otu ћ/ As log s o dditiol titis of fudtl ptils ow, ths fou si os suffiit to dsi fudtl ptil. A ptl odl of fudtl ptil hs to pst its fou titis utly d osisttly. This sus tht th odl lso psts divd titis,.g. Boh gto B (.) Mgti ot B (.) Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg

2 opto wvlgth Rst-ss gy (.) (.) Stg ut tu: As lto d posito do ot show y itl stutu, utu his gds th to poit-ptils, i.. to hv o disios t ll. Suh ojt would totlly ulisti d o-physil. It ould ot hv y physil poptis: hg dsity d ss dsity would ifiit; gul otu ( spi ) d gti ot ould ot xist. Fotutly th is pioig xptio. Th ppoh of this igious ivstigtio is uit difft fo this o, ut th sults d olusios ly th s.. Th iul Loop s Modl of Fudtl Ptils. A o-disiol iul ut loop hvig fiit dius d yig th hg is th siplst odl tht fulfill th fou physil uits tiod ov. Th hg ust distiutd hoogously ov its iuf π, d it ust ott t ostt vloity v φ. Ths th oditios fo ostt ut d ostt gti fild. v I (.) This is th oly h tht th odl pst stl, o-ditig ptil. Th ut I ts gti ot I (.) wh v (.). Th Ntu of th Rst-Mss of Fudtl Ptils. As pstd h th ut loop odl is ltogti; silly it dos ot ow stss d st-ss gy. Th odl povids ltostti fild du to its hg ± d ostt gti fild du to th ottio of th hoogously distiutd hg t ostt vloity. osutly th gy ivtoy is xptd to puly ltogti s it is with ltogti wv. y Figu : O-disiol iul ut loop. x Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg

3 Th hg ± dos ot xist s ottd ottig poit-hg, ut s ostt hg dsity wh (.) (.) is th opto dius of ptil hvig st-ss. y Id Idos ρ I x P(ρ,) Figu. Goti Dtils Th out of th lty hg is tity tht is foud to xtly th s with ll lodd ptils. Additiolly thy hv gti ot iludig stg oly. This s tht th hg (dsity) of ll ths ptils is ottig t ostt gul vloity. Th iul ut loop pstig ltogti ptil odl s tspt tht th st-ss is silly illusio sultig fo th ltostti (oulo) fild d fo th gti (Lot) fild of th ptil. Thotilly th ltogti fild is spd out ifiitly wid. Wh ptil is ltd i lti d/o gti fild, th du to th fiit vloity of light th ltogti fild of th ptil is distotd. Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg

4 Th distotd fild tis to pull its spig tl pt. This stoig fo is itptd s ig du to th iti of ss. Th st-ss gy of th ptil is uivlt to th su of its lti gy l d gti gy g : l g (.) Th ptil dos ot possss lti gy l d gti gy g d dditiol stss gy. Th tu of th ptil gy is ltogti, d th st-ss is fititious tity i spit of th ft tht it sud.. Th ltogti Poptis of th iul ut Loop. Th xt thtil ttt of th iul ut loop is ot tivil. But th sults of th xt lultio vy usful wh th iul ut loop is gdd s odl of fudtl ptils o t lst si lt fo uildig up suh odl. O do i pop wy th sults y sv fov s uivsl pltfo fo ll posptiv lultios. At fist th goti ltioship tw il with dius, td t th oigi of othogol oodit syst, d poit P(ρ,) hs to lyd. I Figu th il is pld i th ρ-pl of ylid oodit f. I Figu, th dist of poit o th il hvig th oodits d to poit with th oodits ρ d = is giv y si os (.) As si os (.) (.) os: os (.) Th dist D of th poit o th il to poit P(ρ,) i th ρ--pl is th giv y o D os (.) D os (.5) It will tu out to usful to itodu th vitio (.5) Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg

5 Thus th dist D os D os (.6) Th ltostti situtio is htid y th otiuous d hoogous distiutio of th hg ov th iul otou: d d d (.7) A ptiul hg lt gts t th poit P(ρ,) th itl otiutio dv to th ltostti pottil V d dv d (.8) D os Th ltostti pottil V t th poit P(ρ,) is th su of ll ths otiutios oud th oplt il: d V (.9) os Th gti situtio is dsid y th vto pottil A tht is td y th ottio of th uifoly distiutd hg t ostt vloity v, thus odig to (.) d (.) pstig ostt ut v I (.) Aodig to th vto hvio of th ut, h lt Ids = Id is oly fftiv with its opot vtil to th x xis: I dsff I os d (.) Thus th vto pottil it da is Ids ff I os d da da (.) D os Th vto pottil A of th ut I log th il t th poit P(ρ,) is Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg 5

6 Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg 6 os os d I A A (.) Both th itgls i (.9) d (.) ot solvd i losd fo. It is wll-ow tht thy tsfod to oitios of th two stddid lliptil itgls. But this would oplit th situtio. Th supio thod is to dvlop th idtil doito of th two futios to itgtd ito pow sis: x x x x x x (.) wh os x (.5) Th offiits lultd odig to th usio foul (.6) Thus th two itgls witt s os os d d (.7) os os os d d (.8) Th followig suvy shows wht hpps: d (.9) si os d xd (.) os os x (.) si d x (.)

7 Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg 7 os os os x (.) si si d x (.) Oly th ts with v xpots otiut to th solutios. Thus th itgl fo th ltostti pottil V slts fo th oth futio (.) th v ts d th itgl fo th vto pottil, s h t is ultiplid y os, slts th odd ts. This idits th los ltioship tw V d A, d it vls tht oth othogol to h oth. I gl, os d (.5) d ) ( ) )( ( os d (.6) Fo (.6) follows ) ( ) )( )( ( os d (.7) osutly th usio foul fo th itgtio sults is d d ) ( ) )( )( ( ) ( ) ( ) )( ( os os (.8) Aodigly th fist itgtio sults os d (.9) 8 6 os d (.)

8 Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg os 6 6 d (.) I od to sui th v ts of (.) it is usful to st. This tsfos (.6) d (.7) to (.) d os d (.) osutly th ltostti pottil odig to (.9) witt s V (.) wh (.5) o (.6) Th fist offiits (.7) Siilly th fil fo of (.) is hivd y sttig = +. This sults i d os os (.8) d I A A (.9)

9 Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg 9 wh (.) o (.) Th fist offiits (.) 5. gis Btw Two iul ut Loops. As tt of syty ll poits o sod oti il hvig th dius ρ = d xil dist = fo th oigi hv th s vlus V d A gtd y piy iul ut loop positiod t th oigi. Th ltostti pottil of il is, V (5.) Its vto pottil is, I A A (5.) wh, (5.) Wh il with dius d xil dist is lodd with th uifoly distiutd hg th ltostti gy l tw th two hgd loops is ), ( V l (5.)

10 Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg o,, l (5.5) Wh th hg otts t vloity v th gti gy g is ), ( A v g (5.6) o,, I v g (5.7) wh v v I v (5.8) I od to th lti gy d th gti gy opl, d i od to o to ovit fo, th followig idtitis usd V (5.9) (5.) Thy tsfo (5.5) d (5.7) to,, l (5.) d,, g (5.)

11 Th stddid gis Figus d. l l g, d g is stddid odigly., pstd i Stddid gis, l Figu. g, d l g of two oti ut loops with R d t ltiv dist / R. Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg

12 Figu : Stddid gis l, g, d l g of two oti ut loops with dii d t dist = = d. 6. Fos Btw Two iul ut Loops. Th lti fos F l i th ditio d F l ρ i th ρ ditio d V (, ) Fl (, ) (6.) V (, ) Fl (, ) (6.) wh V (, ) is giv y (5.) d (5.). With pplyig (5.9) th sults Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg

13 Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg ), ( F l (6.) d ), ( F l (6.) Th gti fos F g i ditio d F g ρ i ρ ditio A v F g ), ( (6.5) d g A v F (6.6) wh A is giv y (5.) d (5.). By pplyig (5.8) d 5.9) th sults, F g (6.7) d, v v F g (6.8) Aodig to (5.) th fto / i (6.), (6.), (6.7), d (6.8) y pld fo (6.9) It will tu out tht sotis it is hlpful o ssy to dfi th vg dius

14 R (6.) Figu 5. Stddid xil fos tw two oti ut loops with R s futio of th ltiv dist /R t. Figu 6. Stddid dil fos tw two oti ut loops t dist = = s futio of th tio / t Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg

15 Figus 5 d 6 giv suvy of th ig of th fou fo utios (6.), 6.), (6.7), d (6.8). Th two gy utios (5.) d 5.) d th fou fo utios pst th oplt st to lult ll itstig poptis of th twi-loop syst. Th lti d gti fild opots (fild stgths) ot xpliitly tiod us thy popotiol to th sptiv fo opots. Moov thy ot dd h. 7. Rs, olusios, d Spil Rsults. A sigl iul ut loop hs ltostti pottil V odig to (5.) d vto pottil A odig to (5.), ut o itisi lti d gti gis. gis odig to (5.) d (5.) oly xist tw (t lst) two lti d/o gti pottils. osutly th siplst ltogti odl of hgd ptil is twodisiol d osists of two iul ut loops. Thi totl lod o + is shd tw th. Thus th dil ltostti fos of fudtl ptil lwys pulsiv. I od to stlish th oppotuity of fo l th dil gti fos ust tttiv. This uis tht oth of th uts hv th s ditio. As th two ut loops of ptil otilly positiod i th s pl, oth of th xil fos lti d gti o. Th shig of th idivisil lty lod to two ut loops is o o i physil thoy us o loop is oly thti it d o physil ojt. Th siplst odl of stl fudtl ptil is twi-loop wh th twis ot physilly sptd. Nutl ptils (.g. th uto) osist of two fudtl ptils of opposit lti polity siil to th hydog to. I otst to hgd fudtl ptils th g of utl ptils ltogti fild d osutly thi si liitd. Th six gy d fo utios ovg s <. Wh is los to uity th ovg is vy poo. Fo xt lultios i th ost itstig g.999 o th 8 ts of th sis y dd. Wh = = d siultously = = R, i.. wh th two loops touh h oth t thi iuf, th xiu vlu = is hd. I this sigul s is v v, d th divd sis fo gis d dil fos do ot ovg. Thus th sptiv vlus ot lultd. But th diff d Fl Fg ovg d lultd t ly uliitd uy. Two fsitig 9 sults of th lultios with up to ts l,, g 9 9 l g (7.) wh = (7.) Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg 5

16 d wh F l F,, g (7.) (7.) I stio 9 will show tht th l odl slightly diffs fo this xt s. As to positiv o gtiv sigs of gis d fos it hs to phsid tht th gy d fo utios o thi outs, i.. gtiv sigs oittd. Wh sus o diffs lultd th ot sigs t. I th s of (7.) F is gtiv d F is positiv s. Wh, it is vi vs. Th ost ipott ssg of g / / (7.) is tht g is ot sstilly sll th l wh is los to uity. Figu shows tht i th ditio t dists >> R th lti gy l dss popotiol to /R whs th out of th gti gy g dss popotiol to /R. Th gti gy is highly ottd to th viiity of th iul ut loops, whs th lti gy is o distiutd ov th totl sp. I ts of ltogti fild gy th lto is ot ifiitly sll, ut ifiitly ig. Th disstous poit-ptil thoy suppsss th gti gy us it ot xist d ot lultd i suh odl. Figus 5 d 6 dostt th s sv ist with th fos. I lity th glly gltd gti fo is vy ipott wh th dist of th two ut loops is < R. Figu 5 ipssivly shows tht t /R =.9757 th su Fl Fg hs xiu vlu d dops dow to o t =. Th sptiv hvio of two poit hgs is puly ltostti. Th gti fo is opltly issig. Thus th lti fo d osutly th totl fo would ifiit t =. Figu 5 vls tht th w d stog ul fos othig ls th th tifiilly suppssd gti fos. Th W d Z osos s wll s th gluos ot t ll od i gluig y ptils togth. Fo th g o gluo, o sud vlus vill. This xpl shows how ossil thoy hllgs th ivtio of spiitulisti ffts d ptils. Two oti, idtil ( = = R), o-disiol ut loops pst th idlid odl of ojt tht odig to (7.) d (7.) is htid y l Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg 6

17 l R, d R, l R R, R, g v v (7.5) g ot lultd fo th sptiv pow sis us thy do ot ovg. But th is sipl wy out tht ws ldy sthd i stio : Wh th l R, d twi loop is ltd th lti fild d th gti fild ospodig to R, g t stoig fo h. It is tditiolly lld itil fo d dfis th itil ss. Ths ptiul sss d l R, l (7.6) gr, g (7.7) Th oplt fild gy is l R, R, (7.8) g Wh th twi loop is to pst fudtl ptil its totl hg ust o, i th s of th posito l g (7.9) (7.) As th two loops (idlid) idtil, th (7.) d (7.) As ldy tiod th ptiul loops ot physil ojts. O loop lo ould ot ywy possss gy. lti d gti gis is fo th utul iflu of thi ltogti pottils. Oly fo thtil ttt thy y y th o-physil hg /. Wh th two loops ought togth fo ifiit dist to idtil positio, gy hs to spt i od to t lti gy gist thi utul pulsiv fo. O th oth hd, th gti fo ttts th loops d thus suppots th poss of ptil tio y otiutig gtiv gti gy. Fo (7.5) d (7.) follows Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg 7

18 l g (7.) R Aodig to (7.8) is l (7.) g l g oitio of (7.) d (7.) sults i l (7.5) R d g (7.6) R Th ltil gy is puly stti d thus ot otiut to so dyi ffts suh s gti ot d gul otu. Thus ths ffts xlusivly ttiutd to th gti gy g sptivly to th gti ss g g (7.7) Dvid Bg foultd this ipott sttt ldy o th ys go. Si th it should l why th gul otu is / g R R (7.8) Fo (7.6), (7.7), d (7.8) follows o wh R R R (7.9) (7.) (7.) Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg 8

19 Th pts of th ut loop odl will igoously osidd i stio 9. With th dius odig to (7.) th gis odig to (7.5) d (7.6) o l (7.) g (7.) osutly is l g (7.) Th ut i th twi loop is odig to (7.) I (7.5) R Fo (7.5) follows th gti ot R I R (7.6) R o R (7.7) d filly B (7.8) wh B (7.9) is th Boh gto d -.6 (7.) Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg 9

20 is th ystious gti ot oly. All of ths sults d sttts d so o ldy giv i, ut othig hppd i th ouity of ist physiists. 8. Bl of Fos. Figu 6 illustts tht t i th whol g / th tttiv gti fo is gt th th pulsiv lti fo. This is th uiu h tht stl fudtl ptils y xist. I th totl g / fo h vlu of / two vlus of foud wh F g Fl (8.) This s tht fo l xists wh Fl (8.) F g At th low vlu odig to (8.) th fo l is stl. Th high vlu ig xtly los to / psts istl l. Th ost itstig gio is th g wh is los to d v (8.) is los to uity. Thfo it is ovit to osid th diffs d Fl (8.) F g (8.5) Figu 7 shows s futio of i th s of stl fo l. Th sll d, th o stps ssy to iv t ot vlus. This is iditd y th ft tht th sptiv uvs stt to d upwds s soo s th u of stps is o log suffiit fo full uy. Th oss t d Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg psts th fo l oditio of th lto. Its lultio would hv uid t lst 8 stps. I od to su, th xiu u of stps ws st t 9. Bsd o th sults of stio 9 th sultig fo Fl Fg odig to (6.) d (6.6) i th viiity of th lto fo l poit is show i Figu 8. I otst to Figu 6 th ipssiv uil vlus i MN/ lultd d ltd to th iuf of th iul ut loops. Th lultio is sd o (6.) d (6.9) d

21 Ws.7 77 N (8.6) 5 R (8.7) Th solut fos F g F l d ltd to th iuf N (8.8) F g R Fl R N/ (8.9) Figu 7. Vloity oditio fo dil fo l s futio of. Difft us of stps gig fo -7 to - idit how ovg dpds o. Th oss idits th lto positio. Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg

22 Figu 8. Rdil fo tw th two ut loops of th lto s futio of / 9. A Modl of th lto. Th gol of th followig osidtios is to fid th siplst physil, osistt, ltogti odl of th lto. Th gy d fo utios will spilid to th s =, i.. wh th two loops positiod otilly i th s pl i od to pst stl fudtl ptil. Th dil vloitis v φ d v φ ssud to slightly sll th : v v v v (9.) (9.) (9.) Th itstig g of is wh th lti fo is gtiv (pulsiv) d th gti fo is positiv (tttiv). Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg

23 Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg Aodig to (7.) th diff tw th lti gy l d th gti gy is giv y g l (9.) As ldy tiod i (.) th totl ltogti fild gy is g l (9.5) oitio of (9.) d (9.5) sults i ß ß ß l (9.6) d ß ß ß ß g (9.7) Rlvt fo futh vlutio is th diff ß ß ß ß g l (9.8) Now it s ti to liit so o isitpttios d os fo ptd physis: Th gti ot iss fo th iul ut I : R R v I (9.9) wh R d v odig to (6.) sptivly (8.) vg vlus. Th gti ot is R v R R I (9.)

24 o R (9.) Th xpitl fidig is (9.) Of ous, this is ot, ut th itpttio of s oly is oous. As th gti ot is du to th ut I i φ ditio th sult hs to ltd to th ss φ i ditio th th to th st ss. Wht lly is sud is (9.) Th ottiol gy opot of ottig ojt ot sud y s of ltio o gvittiol xpits. Th sult of suh suts is lwys. Th diff tw d hs to itptd s dditiol ottiol iti gy osutly is i V (9.) (9.5) d (9.6) Thus, th l situtio is s it hs to i ts of lssil physis: B (9.7) wh B is th Boh gto. Fo (9.) d (9.7) iss th lw of osvtio of gul otu: R (9.8) Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg

25 Th xist of th iti gy i odig to (9.) is ipott fo th gul otu J v / (9.9) Wh (9.9) is pplid to th lto it hs to osvd tht oly th ottig pt g i dy (9.) of th ss otiuts to th gul otu. Th oitio of g d i y pp stg, ut it is pov tht thy uivlt. Th xpitl vlu of J is /. Thus fo (9.7), (9.), (9.9), d (9.) follows ß ß ß ß R (9.) wh v i (9.9) is sustitutd fo (9.8) is usd i (9.) th sult is v d is sustitutd odig to (6.). Wh d filly ß ß ß ß ß ß ß ß (9.) (9.) If th iti gy i would ot hv t ito out th ight sid of (9.) would hv o. This would ui ß. So, it would hv ipossil to pst listi odl of th lto. Thus th sults giv i stio 7 d i f idtifid to ppoxitios. opiso of (9.) d (9.8) lds to th ipott sult l g (9.) As th ltogti fild gy is l g (9.5) Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg 5

26 th followig fudtl sttts foultd: l (9.6) g (9.7) dy g i (9.8) totl l dy (9.9) Now th si utios (9.8) d (9.8) xpli vy siply: J dy v R R (9.) o J (9.) Futh lysis d vlutio of (9.) ui so sol ssuptios. Assuptio. Th hg dsity o th two iul loops is ssud to th s: (9.) I (7.9) it ws ldy sttd tht th hg oditio of th lto is (9.) Fo (9.) d (9.) follows d (9.) (9.5) Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg 6

27 Th fto will tu out to vy los to uity. (9.6) Assuptio. Th gul vloitis d of th ottig hgs d ul: This s d (9.7) (9.8) (9.9) Wh this is pplid to (8.) th vg vlu os (9.) Togth with (9.8) d (6.) this lds to (9.) Th ssuptios sultig i (9.6), (9., d (9.) llow to tsfo (9.) to ß ß ß ß (9.) It tus out tht is xlusivly giv y th tio / us is lso dtid y / vi th fo l oditio odig to (8.). It llows lultio fo h vlu of / th sptiv vlu of. Th lultd odig to (9.). Figu 8 shows th sult i th itstig g of /( ) d Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg 7

28 (9.) s futio of /. (9.) oly, Figu 9. Th itstig g of /( ) d s futio of /. Th oss s th positio of th lto. It is igful tht s.7 d tht s.7. By ittio th ossov poit foud t xtly high uy. At sptivly is (9.5) (9.6) / (9.7) Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg 8

29 Th is o igoous poof tht this sigifit poit dsis lso th physil lity, ut y oth hoi would o o lss ity. Th is o dditiol oditio tht i (9.) ould justify oth sttt th. Nvthlss th followig ppoxitio is giv s th oly sol lttiv: Wh i (9.) odig to (9.) is sustitutd fo, th it os As d it is ovious tht (9.8) osutly is d This ospods to d (9.9) (9.5) - (9.5) (9.5) / (9.5) Th xpitl vlu of th lto s gti ot oly is (9.5) Dspit th ft tht th vlus of (9.5) d (9.5) vy los togth, th solutio odig to (9.6) d (9.7) is pfd us it loos o tul d o systti, d it voids th itodutio of dditiol pt. Thus th hg d th gul Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg 9

30 otu / suffiit to div th w uivsl ostts / d. Thy dfi th si stutu of fudtl ptils d su thi stility (fo l). Th fist o is shp fto whil th sod o is ssy fo th gy ivtoy. Thy disiolss us siil to th fi-stutu ostt d fudtl physil ostts us thy hold fo ll sptiv ptils d ivit gist th vg dius R /( v ) sptivly th st ss. Moov it s tht fudtl ptil y widly is (ot ds!) its dius d ds (ot is!) its ottiol vloity v φ,.g. wh it jois oth hgd ptils, s f s odig to (9.8) th gul otu osvtio oditio R (9.55) v is fulfilld. A wll-ow xpl is th o-lto to with th ulus hg Z wh Z d R / Z / Z 5. Moov it ofis tht fudtl ptils show ss-li d ltivisti hvio, whil thi itl stutu is o-ltivisti d sstilly fild-li. O ipott ssg is tht ll f fudtl ptils hvig th hg d th gul otu / ust possss th s vlus of / d, gdlss of thi st ss. Th is stog vid tht this lso holds fo th f poto d th f tipoto 6. It is ipott disovy tht th gti ot oly idits th xist of th iti gy i. It is ssy to th pstd odl pft, d it vls tht fudtl ptils itlly ot puly fild-li suh s photos d ot (sstilly) ss-li suh s tos. Thy pst spil id of tt i tw. Nvthlss th fudtl ptil is opltly ojt of lssil physis iludig th o-olous gti ot /( ) v R /. Th iul ut loop odl is two-disiol. It is th siplst o tht is osistt d psts ll dtils of fudtl ptils t xtly high uy. Aodig to (9.5) th ottiol vloity v of th lto is giv y v (9.56) Th sptiv vlu of th pstd odl is v (9.57) Th xiu d iiu vlus of th twi loop odl (9.58) Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg

31 (9.59) Fo ptil us it is ot ssy to phsi th twi loop ht of fudtl ptil. It will suffiit to lult with th vg dius odig to (9.8) R (9.6) It is dil d ougig tht th pio of th ig odl is still sussfully woig t this sujt 7. Dditio. pulitio. This pp is dditd to Dv Bg who gously suppotd its Rfs. Bg, D. L., d Wsly, J. P., Spiig hgd Rig Modl of lto Yildig Aolous Mgti Mot, Glil ltodyis, vol., o. 5, pp (Spt./Ot.,99). Nul Ptil Goup, Joul of Applid Physis, Vol., p. 59 (July 6). v d Togt,., Th uivl of Mgti d Kiti gy, Glil ltodyis, Vol. 7, No. 6, pp.- (Nov. /D. 6). Physil Msut Lotoy of NIST, ODATA Ittiolly Rodd Vlus of th Fudtl Physil ostts. (6). 5 Mills, R. L., Th Gd Uifid Thoy of lssil Physis, p. - (). 6 Bg, D. L., Spiig hgd Rig Modl of lty Ptils. Glil ltodyis, vol., o., pp. - (Mh/Apil 99). 7 Bg, D. L., All, D.P., J., lto i th Goud gy Stt Pt, Foudtios of Si, Vol. 5, No., pp. - (F. ). Foudtios of Si Fuy, oo Ss Si Rpit/Itt Atil Pg

Chapter 6 Perturbation theory

Chapter 6 Perturbation theory Ct 6 Ptutio to 6. Ti-iddt odgt tutio to i o tutio sst is giv to fid solutios of λ ' ; : iltoi of si stt : igvlus of : otool igfutios of ; δ ii Rlig-Södig tutio to ' λ..6. ; : gl iltoi ': tutio λ : sll

More information

Chapter 3 Higher Order Linear ODEs

Chapter 3 Higher Order Linear ODEs ht High Od i ODEs. Hoogous i ODEs A li qutio: is lld ohoogous. is lld hoogous. Tho. Sus d ostt ultils of solutios of o so o itvl I gi solutios of o I. Dfiitio. futios lld lil iddt o so itvl I if th qutio

More information

Easy Steps to build a part number... Tri-Start Series III CF P

Easy Steps to build a part number... Tri-Start Series III CF P ulti-l i Oti iul ( oto) ow to O ol os sy ts to uil t u... i-tt is 1. 2 3 4. 5. 6. oto y til iis ll tyl ll iz- st t ott y & y/ ywy ositio 50 9 0 17-08 ol ulti-l i oti otos o us wit ulti-o sil o tii o y

More information

Classical Theory of Fourier Series : Demystified and Generalised VIVEK V. RANE. The Institute of Science, 15, Madam Cama Road, Mumbai

Classical Theory of Fourier Series : Demystified and Generalised VIVEK V. RANE. The Institute of Science, 15, Madam Cama Road, Mumbai Clssil Thoy o Foi Sis : Dmystii Glis VIVEK V RANE Th Istitt o Si 5 Mm Cm Ro Mmbi-4 3 -mil ss : v_v_@yhoooi Abstt : Fo Rim itgbl tio o itvl o poit thi w i Foi Sis t th poit o th itvl big ot how wh th tio

More information

Order Reduction of Linear High-Order Discrete Time Systems Using Polynomial Differentiation Technique in w-domain and PID Controller Design

Order Reduction of Linear High-Order Discrete Time Systems Using Polynomial Differentiation Technique in w-domain and PID Controller Design Ittiol Joul of Eltoi Eltil Egiig ISSN 97-7 Volum 5, Num, pp 7-5 Ittiol Rsh Pulitio Hous http://iphousom O Rutio of Li High-O Dist Tim Systms Usig Polyomil Difftitio Thiqu i -Domi PID Cotoll Dsig B Stish

More information

Handout on. Crystal Symmetries and Energy Bands

Handout on. Crystal Symmetries and Energy Bands dou o Csl s d g Bds I hs lu ou wll l: Th loshp bw ss d g bds h bs of sp-ob ouplg Th loshp bw ss d g bds h ps of sp-ob ouplg C 7 pg 9 Fh Coll Uvs d g Bds gll hs oh Th sl pol ss ddo o h l slo s: Fo pl h

More information

CBSE SAMPLE PAPER SOLUTIONS CLASS-XII MATHS SET-2 CBSE , ˆj. cos. SECTION A 1. Given that a 2iˆ ˆj. We need to find

CBSE SAMPLE PAPER SOLUTIONS CLASS-XII MATHS SET-2 CBSE , ˆj. cos. SECTION A 1. Given that a 2iˆ ˆj. We need to find BSE SMLE ER SOLUTONS LSS-X MTHS SET- BSE SETON Gv tht d W d to fd 7 7 Hc, 7 7 7 Lt, W ow tht Thus, osd th vcto quto of th pl z - + z = - + z = Thus th ts quto of th pl s - + z = Lt d th dstc tw th pot,,

More information

Today s topic 2 = Setting up the Hydrogen Atom problem. Schematic of Hydrogen Atom

Today s topic 2 = Setting up the Hydrogen Atom problem. Schematic of Hydrogen Atom Today s topic Sttig up th Hydog Ato pobl Hydog ato pobl & Agula Motu Objctiv: to solv Schödig quatio. st Stp: to dfi th pottial fuctio Schatic of Hydog Ato Coulob s aw - Z 4ε 4ε fo H ato Nuclus Z What

More information

Chapter 2 Reciprocal Lattice. An important concept for analyzing periodic structures

Chapter 2 Reciprocal Lattice. An important concept for analyzing periodic structures Chpt Rcpocl Lttc A mpott cocpt o lyzg podc stuctus Rsos o toducg cpocl lttc Thoy o cystl dcto o x-ys, utos, d lctos. Wh th dcto mxmum? Wht s th tsty? Abstct study o uctos wth th podcty o Bvs lttc Fou tsomto.

More information

The Real Hydrogen Atom

The Real Hydrogen Atom T Ra Hydog Ato ov ad i fist od gt iddt of :.6V a us tubatio toy to dti: agti ffts si-obit ad yfi -A ativisti otios Aso av ab sift du to to sfitatio. Nd QD Dia q. ad dds o H wavfutio at sou of ti fid. Vy

More information

CBSE , ˆj. cos CBSE_2015_SET-1. SECTION A 1. Given that a 2iˆ ˆj. We need to find. 3. Consider the vector equation of the plane.

CBSE , ˆj. cos CBSE_2015_SET-1. SECTION A 1. Given that a 2iˆ ˆj. We need to find. 3. Consider the vector equation of the plane. CBSE CBSE SET- SECTION. Gv tht d W d to fd 7 7 Hc, 7 7 7. Lt,. W ow tht.. Thus,. Cosd th vcto quto of th pl.. z. - + z = - + z = Thus th Cts quto of th pl s - + z = Lt d th dstc tw th pot,, - to th pl.

More information

Rectangular Waveguides

Rectangular Waveguides Rtgulr Wvguids Wvguids tt://www.tllguid.o/wvguidlirit.tl Uss To rdu ttutio loss ig rquis ig owr C ort ol ov rti rquis Ats s ig-ss iltr Norll irulr or rtgulr W will ssu losslss rtgulr tt://www..surr..u/prsol/d.jris/wguid.tl

More information

Kummer Beta -Weibull Geometric Distribution. A New Generalization of Beta -Weibull Geometric Distribution

Kummer Beta -Weibull Geometric Distribution. A New Generalization of Beta -Weibull Geometric Distribution ttol Jol of Ss: Bs Al Rsh JSBAR SSN 37-453 Pt & Ol htt://gss.og/.h?joljolofbsaal ---------------------------------------------------------------------------------------------------------------------------

More information

ENGO 431 Analytical Photogrammetry

ENGO 431 Analytical Photogrammetry EGO Altil Phtgmmt Fll 00 LAB : SIGLE PHOTO RESECTIO u t: vm 00 Ojtiv: tmi th Eti Oitti Pmts EOP f sigl ht usig lst squs justmt u. Giv:. Iti Oitti Pmts IOP f th m fm th Cm Cliti Ctifit CCC; Clit fl lgth

More information

Three Phase Asymmetrical Load Flow for Four-Wire Distribution Networks

Three Phase Asymmetrical Load Flow for Four-Wire Distribution Networks T Aytl Lo Flow o Fou-W Dtuto Ntwo M. Mo *, A. M. Dy. M. A Dtt o Eltl E, A Uvty o Toloy Hz Av., T 59, I * El: o8@yoo.o Att-- Mjoty o tuto two ul u to ul lo, yty to l two l ut. T tt o tuto yt ult y o ovt

More information

KEB INVERTER L1 L2 L3 FLC - RELAY 1 COMMON I1 - APPROACH CLOSE 0V - DIGITAL COMMON FLA - RELAY 1 N.O. AN1+ - ANALOG 1 (+) CRF - +10V OUTPUT

KEB INVERTER L1 L2 L3 FLC - RELAY 1 COMMON I1 - APPROACH CLOSE 0V - DIGITAL COMMON FLA - RELAY 1 N.O. AN1+ - ANALOG 1 (+) CRF - +10V OUTPUT XT SSMLY MOL 00 (O FS) 00 (I- PT) 00 (SIGL SLI) WG O 0 0-0 0-0-0 0.0. 0 0-0 0-0-0 0 0-0 0-0-0 VOLTG F.L...0..0..0.0..0 IIG POW FOM US SUPPLI ISOT (S TL) US OP OUTOS T T 0 O HIGH H IUIT POTTIO OT: H IUIT

More information

Quantum Mechanics & Spectroscopy Prof. Jason Goodpaster. Problem Set #2 ANSWER KEY (5 questions, 10 points)

Quantum Mechanics & Spectroscopy Prof. Jason Goodpaster. Problem Set #2 ANSWER KEY (5 questions, 10 points) Chm 5 Problm St # ANSWER KEY 5 qustios, poits Qutum Mchics & Spctroscopy Prof. Jso Goodpstr Du ridy, b. 6 S th lst pgs for possibly usful costts, qutios d itgrls. Ths will lso b icludd o our futur ms..

More information

New Advanced Higher Mathematics: Formulae

New Advanced Higher Mathematics: Formulae Advcd High Mthmtics Nw Advcd High Mthmtics: Fomul G (G): Fomul you must mmois i od to pss Advcd High mths s thy ot o th fomul sht. Am (A): Ths fomul giv o th fomul sht. ut it will still usful fo you to

More information

Multi-Electron Atoms-Helium

Multi-Electron Atoms-Helium Multi-lecto Atos-Heliu He - se s H but with Z He - electos. No exct solutio of.. but c use H wve fuctios d eegy levels s sttig poit ucleus sceeed d so Zeffective is < sceeig is ~se s e-e epulsio fo He,

More information

LWC 434 East First Street 4440 Garwood Place

LWC 434 East First Street 4440 Garwood Place //0 :: UI IXTUS TO US IIT TOS O T IST UTU I TOY IST OW - ITIO UTUS IST I TSIS. I ST (O, ZU). cui (, ZU). TOTO (OI, O). SO (ZU, Y). TUO (SO, ZU). TOTO (O US). IS (OSOIT, U). UST (ST WIIS, ZU). Y (T&S SS,

More information

C-Curves. An alternative to the use of hyperbolic decline curves S E R A F I M. Prepared by: Serafim Ltd. P. +44 (0)

C-Curves. An alternative to the use of hyperbolic decline curves S E R A F I M. Prepared by: Serafim Ltd. P. +44 (0) An ltntiv to th us of hypolic dclin cuvs Ppd y: Sfim Ltd S E R A F I M info@sfimltd.com P. +44 (02890 4206 www.sfimltd.com Contnts Contnts... i Intoduction... Initil ssumptions... Solving fo cumultiv...

More information

A TYP A-602 A-304 A-602 A-302 GRADE BEAM SEE 95% COMPACTED STRUCTURAL FILL A '-0"

A TYP A-602 A-304 A-602 A-302 GRADE BEAM SEE 95% COMPACTED STRUCTURAL FILL A '-0 W W/TITI -0 X U I I X TITI TY S W TYS TIS X W S SU XISTI -0-0 -0-0 -0-0 ' - " ' - " ' - " ' - " ' - " ' - /" ' - /" ' - " -STUTU I -0 ' - ' - " " ' - " " 0' - " ' - U I S STUT W'S TY UTI W S STUT W'S TY

More information

Bayesian Estimation of the parameters of the Weibull-Weibull Length-Biased mixture distributions using time censored data

Bayesian Estimation of the parameters of the Weibull-Weibull Length-Biased mixture distributions using time censored data Bys Eso of h s of h Wull-Wull gh-bs xu suos usg so S. A. Sh N Bouss I.S.S. Co Uvsy I.N.P.S. Algs Uvsy shsh@yhoo.o ou005@yhoo.o As I hs h s of h Wull-Wull lgh s xu suos s usg h Gs slg hqu u y I sog sh.

More information

Ch. 6 Free Electron Fermi Gas

Ch. 6 Free Electron Fermi Gas Ch. 6 lcto i Gas Coductio lctos i a tal ov fl without scattig b io cos so it ca b cosidd as if walitactig o f paticls followig idiac statistics. hfo th coductio lctos a fqutl calld as f lcto i gas. Coductio

More information

Gavilan JCCD Trustee Areas Plan Adopted November 10, 2015

Gavilan JCCD Trustee Areas Plan Adopted November 10, 2015 Gvil JCCD Tust A Pl Aopt Novmb, S Jos US p Ls Pl Aopt // Cit/Csus Dsigt Plc ighw Cit Aom ollist igm S Jos Ts Pios c Ps 4 ut S Bito ut ils Aom ollist igm Ts Pios S Bito ut Lpoff & Goblt Dmogphic sch, Ic.

More information

«A first lesson on Mathematical Induction»

«A first lesson on Mathematical Induction» Bcgou ifotio: «A fist lesso o Mtheticl Iuctio» Mtheticl iuctio is topic i H level Mthetics It is useful i Mtheticl copetitios t ll levels It hs bee coo sight tht stuets c out the poof b theticl iuctio,

More information

Handout 7. Properties of Bloch States and Electron Statistics in Energy Bands

Handout 7. Properties of Bloch States and Electron Statistics in Energy Bands Hdout 7 Popts of Bloch Stts d Elcto Sttstcs Eg Bds I ths lctu ou wll l: Popts of Bloch fuctos Podc boud codtos fo Bloch fuctos Dst of stts -spc Elcto occupto sttstcs g bds ECE 407 Spg 009 Fh R Coll Uvst

More information

Series III, TV Breakaway Fail-Safe Connectors Quick-Disconnect with an Axial Pull of Lanyard

Series III, TV Breakaway Fail-Safe Connectors Quick-Disconnect with an Axial Pull of Lanyard is, wy il- otos Qui-isot wit xil ull o y ulo ss quo mol i-tt wy il- otos ovi uqul om i viomts quii istt ismt. wy il- oto mily os wi o ltil mil tus: stt ouli m stio omltly itmtl wit st tls (/20 /2) vtoy

More information

a f(x)dx is divergent.

a f(x)dx is divergent. Mth 250 Exm 2 review. Thursdy Mrh 5. Brig TI 30 lultor but NO NOTES. Emphsis o setios 5.5, 6., 6.2, 6.3, 3.7, 6.6, 8., 8.2, 8.3, prt of 8.4; HW- 2; Q-. Kow for trig futios tht 0.707 2/2 d 0.866 3/2. From

More information

The Reign of Grace and Life. Romans 5:12-21 (5:12-14, 17 focus)

The Reign of Grace and Life. Romans 5:12-21 (5:12-14, 17 focus) Th Rig of Gc d Lif Rom 5:12-21 (5:12-14, 17 focu) Th Ifluc of O h d ud Adolph H J o ph Smith B i t l m t Fid Idi Gdhi Ci Lu Gu ich N itz y l M d i M ch Nlo h Vig T L M uhmmd B m i o t T Ju Chit w I N h

More information

Linear Algebra Existence of the determinant. Expansion according to a row.

Linear Algebra Existence of the determinant. Expansion according to a row. Lir Algbr 2270 1 Existc of th dtrmit. Expsio ccordig to row. W dfi th dtrmit for 1 1 mtrics s dt([]) = (1) It is sy chck tht it stisfis D1)-D3). For y othr w dfi th dtrmit s follows. Assumig th dtrmit

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

Face Detection and Recognition. Linear Algebra and Face Recognition. Face Recognition. Face Recognition. Dimension reduction

Face Detection and Recognition. Linear Algebra and Face Recognition. Face Recognition. Face Recognition. Dimension reduction F Dtto Roto Lr Alr F Roto C Y I Ursty O solto: tto o l trs s s ys os ot. Dlt to t to ltpl ws. F Roto Aotr ppro: ort y rry s tor o so E.. 56 56 > pot 6556- stol sp A st o s t ps to ollto o pots ts sp. F

More information

M5. LTI Systems Described by Linear Constant Coefficient Difference Equations

M5. LTI Systems Described by Linear Constant Coefficient Difference Equations 5. LTI Systes Descied y Lie Costt Coefficiet Diffeece Equtios Redig teil: p.34-4, 245-253 3/22/2 I. Discete-Tie Sigls d Systes Up til ow we itoduced the Fouie d -tsfos d thei popeties with oly ief peview

More information

Call for Applications

Call for Applications i Ty Ty v l O 7:H 7 O6 fl x 4 7T q l it y ix k lf t l l H v l lg i li O 7:H7 EDL9 ty i tyi yt Blvi i i g it g vi B l B ll li B i ll iz i ti S B 6 dy li j d ti d l i vi i ik tti w z k ik tti i l w l Hli

More information

ENGG 1203 Tutorial. Difference Equations. Find the Pole(s) Finding Equations and Poles

ENGG 1203 Tutorial. Difference Equations. Find the Pole(s) Finding Equations and Poles ENGG 03 Tutoial Systms ad Cotol 9 Apil Laig Obctivs Z tasfom Complx pols Fdbac cotol systms Ac: MIT OCW 60, 6003 Diffc Equatios Cosid th systm pstd by th followig diffc quatio y[ ] x[ ] (5y[ ] 3y[ ]) wh

More information

Helping every little saver

Helping every little saver Spt th diffc d cut hw u c fid I c spt thigs! Hlpig v littl sv Hw d u p i? I ch Just pp it f u chs. T fid u lcl ch just visit s.c.uk/ch If u pig i chqu, it c tk ud 4 wkig ds t cl Ov th ph Just cll Tlph

More information

Chapter 5: Quantization of Radiation in Cavities and Free Space

Chapter 5: Quantization of Radiation in Cavities and Free Space Quu O f Ph Ol Fh R Cll vy Ch 5: Quz f R Cv F S 5 Cll ly 5 Cll Cvy ly Mxwll u f lg J 4 h lv l C fl vy W f h g f h vy Th vy u luly ll W l u h J Cvy F Mxwll u v h wv u Th v u lv h f h fu h vy I w wh h v l

More information

ASSERTION AND REASON

ASSERTION AND REASON ASSERTION AND REASON Som qustios (Assrtio Rso typ) r giv low. Ech qustio cotis Sttmt (Assrtio) d Sttmt (Rso). Ech qustio hs choics (A), (B), (C) d (D) out of which ONLY ONE is corrct. So slct th corrct

More information

GUC (Dr. Hany Hammad)

GUC (Dr. Hany Hammad) Lct # Pl s. Li bdsid s with ifm mplitd distibtis. Gl Csidtis Uifm Bimil Optimm (Dlph-Tchbshff) Cicl s. Pl s ssmig ifm mplitd citti m F m d cs z F d d M COMM Lct # Pl s ssmig ifm mplitd citti F m m m T

More information

4. Project Options. PUC Docket No Attachment 4b Page 10 of 15. Option 1:

4. Project Options. PUC Docket No Attachment 4b Page 10 of 15. Option 1: P Dt 8 ttht Pg 1 f 15 It i-ps Sit - Bill - K Its Pjt Pli Pjt tis sti th ifft lttis t itif th st lil slti t s th l hs lttis list s flls: ti 1: Istll 69, 12 M hs shiftig tsf (PS) t Si th Si 69 tsissi li

More information

IIT JEE MATHS MATRICES AND DETERMINANTS

IIT JEE MATHS MATRICES AND DETERMINANTS IIT JEE MTHS MTRICES ND DETERMINNTS THIRUMURUGN.K PGT Mths IIT Trir 978757 Pg. Lt = 5, th () =, = () = -, = () =, = - (d) = -, = -. Lt sw smmtri mtri of odd th quls () () () - (d) o of ths. Th vlu of th

More information

Problem Session (3) for Chapter 4 Signal Modeling

Problem Session (3) for Chapter 4 Signal Modeling Pobm Sssio fo Cht Sig Modig Soutios to Pobms....5. d... Fid th Pdé oimtio of scod-od to sig tht is giv by [... ] T i.. d so o. I oth wods usig oimtio of th fom b b b H fid th cofficits b b b d. Soutio

More information

minimize c'x subject to subject to subject to

minimize c'x subject to subject to subject to z ' sut to ' M ' M N uostrd N z ' sut to ' z ' sut to ' sl vrls vtor of : vrls surplus vtor of : uostrd s s s s s s z sut to whr : ut ost of :out of : out of ( ' gr of h food ( utrt : rqurt for h utrt

More information

OH BOY! Story. N a r r a t iv e a n d o bj e c t s th ea t e r Fo r a l l a g e s, fr o m th e a ge of 9

OH BOY! Story. N a r r a t iv e a n d o bj e c t s th ea t e r Fo r a l l a g e s, fr o m th e a ge of 9 OH BOY! O h Boy!, was or igin a lly cr eat ed in F r en ch an d was a m a jor s u cc ess on t h e Fr en ch st a ge f or young au di enc es. It h a s b een s een by ap pr ox i ma t ely 175,000 sp ect at

More information

T h e C S E T I P r o j e c t

T h e C S E T I P r o j e c t T h e P r o j e c t T H E P R O J E C T T A B L E O F C O N T E N T S A r t i c l e P a g e C o m p r e h e n s i v e A s s es s m e n t o f t h e U F O / E T I P h e n o m e n o n M a y 1 9 9 1 1 E T

More information

National Survey of Student Engagement, Spring 2011 The University at Albany, SUNY

National Survey of Student Engagement, Spring 2011 The University at Albany, SUNY Ntil uvy f tudt Eggt, pig 11 T Uivity t Alby, UNY EXECUTIVE UMMARY Jl D. Bl, P.D. Dit f Adi At & uvy R I Fbuy d M 11, T Uivity t Alby ptiiptd i t Ntil uvy f tudt Eggt (NE) f t d ti, fllwig up u pviu ptiipti

More information

Riemann Integral Oct 31, such that

Riemann Integral Oct 31, such that Riem Itegrl Ot 31, 2007 Itegrtio of Step Futios A prtitio P of [, ] is olletio {x k } k=0 suh tht = x 0 < x 1 < < x 1 < x =. More suitly, prtitio is fiite suset of [, ] otiig d. It is helpful to thik of

More information

Chapter 11 Solutions ( ) 1. The wavelength of the peak is. 2. The temperature is found with. 3. The power is. 4. a) The power is

Chapter 11 Solutions ( ) 1. The wavelength of the peak is. 2. The temperature is found with. 3. The power is. 4. a) The power is Chapt Solutios. Th wavlgth of th pak is pic 3.898 K T 3.898 K 373K 885 This cospods to ifad adiatio.. Th tpatu is foud with 3.898 K pic T 3 9.898 K 50 T T 5773K 3. Th pow is 4 4 ( 0 ) P σ A T T ( ) ( )

More information

TRANSFORMS AND PARTIAL DIFFERENTIAL EQUATIONS

TRANSFORMS AND PARTIAL DIFFERENTIAL EQUATIONS TRANSFORMS AND PARTIAL DIFFERENTIAL EQUATIONS UNIT-I PARTIAL DIFFERENTIAL EQUATIONS PART-A. Elimit th ritrry ott & from = ( + )(y + ) Awr: = ( + )(y + ) Diff prtilly w.r.to & y hr p & q y p = (y + ) ;

More information

Instrumentation for Characterization of Nanomaterials (v11) 11. Crystal Potential

Instrumentation for Characterization of Nanomaterials (v11) 11. Crystal Potential Istumtatio o Chaactizatio o Naomatials (v). Cystal Pottial Dlta uctio W d som mathmatical tools to dvlop a physical thoy o lcto diactio om cystal. Idal cystals a iiit this, so th will b som iiitis lii

More information

2.Decision Theory of Dependence

2.Decision Theory of Dependence .Deciio Theoy of Depedece Theoy :I et of vecto if thee i uet which i liely depedet the whole et i liely depedet too. Coolly :If the et i liely idepedet y oepty uet of it i liely idepedet. Theoy : Give

More information

Relation of Finite Mellin Integral Transform. with Laplace and Fourier Transforms

Relation of Finite Mellin Integral Transform. with Laplace and Fourier Transforms Cotmpo Egiig Si Vol. 4 o. 6 69-88 Rltio o Fiit Mlli Itgl Tom with Lpl d Foui Tom S. M. Khi R. M. Pi* d J. N. Sluk** Dptmt o Mthmti Mhht Adm o Egiig Aldi-45Pu Idi mkhi7@gmil.om *Dptmt o Mthmti (A.S.&H.

More information

UNIT V: Z-TRANSFORMS AND DIFFERENCE EQUATIONS. Dr. V. Valliammal Department of Applied Mathematics Sri Venkateswara College of Engineering

UNIT V: Z-TRANSFORMS AND DIFFERENCE EQUATIONS. Dr. V. Valliammal Department of Applied Mathematics Sri Venkateswara College of Engineering UNIT V: -TRANSFORMS AND DIFFERENCE EQUATIONS D. V. Vllimml Deptmet of Applied Mthemtics Si Vektesw College of Egieeig TOPICS:. -Tsfoms Elemet popeties.. Ivese -Tsfom usig ptil fctios d esidues. Covolutio

More information

The tight-binding method

The tight-binding method Th tight-idig thod Wa ottial aoach: tat lcto a a ga of aly f coductio lcto. ow aout iulato? ow aout d-lcto? d Tight-idig thod: gad a olid a a collctio of wa itactig utal ato. Ovla of atoic wav fuctio i

More information

CREATED USING THE RSC COMMUNICATION TEMPLATE (VER. 2.1) - SEE FOR DETAILS

CREATED USING THE RSC COMMUNICATION TEMPLATE (VER. 2.1) - SEE   FOR DETAILS uortig Iormtio: Pti moiitio oirmtio vi 1 MR: j 5 FEFEFKFK 8.6.. 8.6 1 13 1 11 1 9 8 7 6 5 3 1 FEFEFKFK moii 1 13 1 11 1 9 8 7 6 5 3 1 m - - 3 3 g i o i o g m l g m l - - h k 3 h k 3 Figur 1: 1 -MR or th

More information

P a g e 3 6 of R e p o r t P B 4 / 0 9

P a g e 3 6 of R e p o r t P B 4 / 0 9 P a g e 3 6 of R e p o r t P B 4 / 0 9 p r o t e c t h um a n h e a l t h a n d p r o p e r t y fr om t h e d a n g e rs i n h e r e n t i n m i n i n g o p e r a t i o n s s u c h a s a q u a r r y. J

More information

Ch. 22: Classical Theory of Harmonic Crystal

Ch. 22: Classical Theory of Harmonic Crystal C. : Clssl Toy o mo Cysl gl o ml moo o o os l s ld o ls o pl ollowg:. Eqlbm Pops p o ls d Islos Eqlbm sy d Cos Egs Tml Epso d lg. Tspo Pops T pd o lo Tm Fl o Wdm-Fz Lw pody Tml Cody o Islos Tsmsso o od.

More information

How much air is required by the people in this lecture theatre during this lecture?

How much air is required by the people in this lecture theatre during this lecture? 3 NTEGRATON tgrtio is us to swr qustios rltig to Ar Volum Totl qutity such s: Wht is th wig r of Boig 747? How much will this yr projct cost? How much wtr os this rsrvoir hol? How much ir is rquir y th

More information

TRANSFORMS AND PARTIAL DIFFERENTIAL EQUATIONS

TRANSFORMS AND PARTIAL DIFFERENTIAL EQUATIONS TRANSFORMS AND PARTIAL DIFFERENTIAL EQUATIONS UNIT-I PARTIAL DIFFERENTIAL EQUATIONS PART-A. Elimit th ritrry ott & from = ( + )(y + ) = ( + )(y + ) Diff prtilly w.r.to & y hr p & q p = (y + ) ; q = ( +

More information

D. Bertsekas and R. Gallager, "Data networks." Q: What are the labels for the x-axis and y-axis of Fig. 4.2?

D. Bertsekas and R. Gallager, Data networks. Q: What are the labels for the x-axis and y-axis of Fig. 4.2? pd by J. Succ ECE 543 Octob 22 2002 Outl Slottd Aloh Dft Stblzd Slottd Aloh Uslottd Aloh Splttg Algoths Rfc D. Btsks d R. llg "Dt twoks." Rvw (Slottd Aloh): : Wht th lbls fo th x-xs d y-xs of Fg. 4.2?

More information

BINOMIAL THEOREM SOLUTION. 1. (D) n. = (C 0 + C 1 x +C 2 x C n x n ) (1+ x+ x 2 +.)

BINOMIAL THEOREM SOLUTION. 1. (D) n. = (C 0 + C 1 x +C 2 x C n x n ) (1+ x+ x 2 +.) BINOMIAL THEOREM SOLUTION. (D) ( + + +... + ) (+ + +.) The coefficiet of + + + +... + fo. Moeove coefficiet of is + + + +... + if >. So. (B)... e!!!! The equied coefficiet coefficiet of i e -.!...!. (A),

More information

Winnie flies again. Winnie s Song. hat. A big tall hat Ten long toes A black magic wand A long red nose. nose. She s Winnie Winnie the Witch.

Winnie flies again. Winnie s Song. hat. A big tall hat Ten long toes A black magic wand A long red nose. nose. She s Winnie Winnie the Witch. Wnn f gn ht Wnn Song A g t ht Tn ong to A k g wnd A ong d no. no Sh Wnn Wnn th Wth. y t d to A ong k t Bg gn y H go wth Wnn Whn h f. wnd ootk H Wu Wu th t. Ptu Dtony oo hopt oon okt hng gd ho y ktod nh

More information

ME 501A Seminar in Engineering Analysis Page 1

ME 501A Seminar in Engineering Analysis Page 1 Powe Seies Solutios Foeius Metho Septee 6, 7 Powe Seies Solutios Foeius etho L Cetto Mehil Egieeig 5AB Sei i Egieeig Alsis Otoe 6, 7 Outlie Review lst wee Powe seies solutios Geel ppoh Applitio Foeius

More information

Self-Adjusting Top Trees

Self-Adjusting Top Trees Th Polm Sl-jsting Top Ts ynmi ts: ol: mintin n n-tx ost tht hngs o tim. link(,w): ts n g twn tis n w. t(,w): lts g (,w). pplition-spii t ssoit with gs n/o tis. ont xmpls: in minimm-wight g in th pth twn

More information

PESIT Bangalore South Campus Hosur road, 1km before Electronic City, Bengaluru -100 Department of Basic Science and Humanities

PESIT Bangalore South Campus Hosur road, 1km before Electronic City, Bengaluru -100 Department of Basic Science and Humanities P E PESIT Bglo South Cpus Hosu od, k bfo Elctoic Cit, Bgluu -00 Dptt of Bsic Scic d Huitis INTERNAL ASSESSMENT TEST Dt : 0/0/07 Mks: 0 Subjct & Cod : Egiig Mthtics I 5MAT Sc : ALL N of fcult : GVR,GKJ,RR,SV,NHM,DN,KR,

More information

Project 3: Using Identities to Rewrite Expressions

Project 3: Using Identities to Rewrite Expressions MAT 5 Projet 3: Usig Idetities to Rewrite Expressios Wldis I lger, equtios tht desrie properties or ptters re ofte lled idetities. Idetities desrie expressio e repled with equl or equivlet expressio tht

More information

MATH 104: INTRODUCTORY ANALYSIS SPRING 2008/09 PROBLEM SET 10 SOLUTIONS. f m. and. f m = 0. and x i = a + i. a + i. a + n 2. n(n + 1) = a(b a) +

MATH 104: INTRODUCTORY ANALYSIS SPRING 2008/09 PROBLEM SET 10 SOLUTIONS. f m. and. f m = 0. and x i = a + i. a + i. a + n 2. n(n + 1) = a(b a) + MATH 04: INTRODUCTORY ANALYSIS SPRING 008/09 PROBLEM SET 0 SOLUTIONS Throughout this problem set, B[, b] will deote the set of ll rel-vlued futios bouded o [, b], C[, b] the set of ll rel-vlued futios

More information

Coordinate Transformations

Coordinate Transformations Coll of E Copt Scc Mchcl E Dptt Nots o E lss Rvs pl 6, Istcto: L Ctto Coot Tsfotos Itocto W wt to c ot o lss lttv coot ssts. Most stts hv lt wth pol sphcl coot ssts. I ths ots, w wt to t ths oto of fft

More information

POWER UP. Hello, Teachers! With Dr. E tm GRADE TEACHER S GUIDE

POWER UP. Hello, Teachers! With Dr. E tm GRADE TEACHER S GUIDE GDE 6 Hll, h! Ggi P i xly xid h hi ih y hl by vidig gy di iiiiv d h d lig xi i y l W lk d kig ih y d y d ECHE S GUIDE D E M By jiig i h Lig P g, ig D E d h W Sqd, ill dliv gy iiy g hgh i-l ild i, ig hd-

More information

Luiz Leal Oak Ridge National Laboratory. of Massachusetts Institute. of Technology (MIT)

Luiz Leal Oak Ridge National Laboratory. of Massachusetts Institute. of Technology (MIT) LzLl OkRdgNlLby LsPsdhNl Egg Dp f h MsshssIs f Thlgy(MIT) Csy f Lz Ll, Ok Rdg Nl Lby. Usd wh pss. NI T Idpd Tsp Eq f Φ(E,,Ωˆ ) Ωˆ. Φ + Σ Φ = dωˆ ' de'σ s (E' E, Ωˆ ' Ω)Φ(E', ',Ωˆ ) + S 4 π 0 Σ Msplsss

More information

Introduction to Finite Element Method

Introduction to Finite Element Method pt. o C d Eot E. Itodto to t Et Mtod st 5 H L pt. o C d Eot E o to st tt Ass L. o. H L ttp://st.s.. pt. o C d Eot E. Cotts. Itodto. Appoto o tos & to Cs. t Eqtos O so. Mtdso os-estt 5. stzto 6. wo so Estt

More information

Zeroth moment of the Boltzmann Equation The Equation of Continuity (Particle conservation)

Zeroth moment of the Boltzmann Equation The Equation of Continuity (Particle conservation) Plasas as Fluids At this poit w d to us a ub of basi quatios that dsib plasas as fluids. Whil it is possibl to alulat ths quatios fo fist piipls, usig Maxwll s ltoagti fild quatios ad Maxwll s vloity distibutio

More information

LED lighting + 2.3% + 2.2% Controlling energy costs, a major competitiveness driver. Our main projects

LED lighting + 2.3% + 2.2% Controlling energy costs, a major competitiveness driver. Our main projects Clli y ss, j piivss div Sdily isi y qis Dspi pss i y ffiiy, h wldwid liiy spi is wi by ii f 2.3% p y ss ll ss. d is ps hlp y lii h ip f y ss y bsiss Hih d isi pis Th pi f liiy is sdily isi i OECD (Oisi

More information

Model of the multi-level laser

Model of the multi-level laser Modl of th multilvl lsr Trih Dih Chi Fulty of Physis, Collg of turl Sis, oi tiol Uivrsity Tr Mh ug, Dih u Kho Fulty of Physis, Vih Uivrsity Astrt. Th lsr hrtristis dpd o th rgylvl digrm. A rsol rgylvl

More information

G-001 CHATHAM HARBOR AUNT LYDIA'S COVE CHATHAM ATLANTIC OCEAN INDEX OF NAVIGATION AIDS GENERAL NOTES: GENERAL PLAN A6 SCALE: 1" = 500' CANADA

G-001 CHATHAM HARBOR AUNT LYDIA'S COVE CHATHAM ATLANTIC OCEAN INDEX OF NAVIGATION AIDS GENERAL NOTES: GENERAL PLAN A6 SCALE: 1 = 500' CANADA TR ISL ROR UST 8 O. R-2,4-3 R-4 IX O VITIO IS STT PL ORPI OORITS POSITIO 27698 4-39'-" 88 69-6'-4."W 278248 4-4'-" 8968 69-6'-4"W 27973 4-4'-2" 88 69-6'-"W W MPSIR OOR UUST PORTL MI OR 27 8-OOT OR L -

More information

k m The reason that his is very useful can be seen by examining the Taylor series expansion of some potential V(x) about a minimum point:

k m The reason that his is very useful can be seen by examining the Taylor series expansion of some potential V(x) about a minimum point: roic Oscilltor Pottil W r ow goig to stuy solutios to t TIS for vry usful ottil tt of t roic oscilltor. I clssicl cics tis is quivlt to t block srig robl or tt of t ulu (for sll oscilltios bot of wic r

More information

MATH 104: INTRODUCTORY ANALYSIS SPRING 2009/10 PROBLEM SET 8 SOLUTIONS. and x i = a + i. i + n(n + 1)(2n + 1) + 2a. (b a)3 6n 2

MATH 104: INTRODUCTORY ANALYSIS SPRING 2009/10 PROBLEM SET 8 SOLUTIONS. and x i = a + i. i + n(n + 1)(2n + 1) + 2a. (b a)3 6n 2 MATH 104: INTRODUCTORY ANALYSIS SPRING 2009/10 PROBLEM SET 8 SOLUTIONS 6.9: Let f(x) { x 2 if x Q [, b], 0 if x (R \ Q) [, b], where > 0. Prove tht b. Solutio. Let P { x 0 < x 1 < < x b} be regulr prtitio

More information

SOLVED EXAMPLES. Ex.1 If f(x) = , then. is equal to- Ex.5. f(x) equals - (A) 2 (B) 1/2 (C) 0 (D) 1 (A) 1 (B) 2. (D) Does not exist = [2(1 h)+1]= 3

SOLVED EXAMPLES. Ex.1 If f(x) = , then. is equal to- Ex.5. f(x) equals - (A) 2 (B) 1/2 (C) 0 (D) 1 (A) 1 (B) 2. (D) Does not exist = [2(1 h)+1]= 3 SOLVED EXAMPLES E. If f() E.,,, th f() f() h h LHL RHL, so / / Lim f() quls - (D) Dos ot ist [( h)+] [(+h) + ] f(). LHL E. RHL h h h / h / h / h / h / h / h As.[C] (D) Dos ot ist LHL RHL, so giv it dos

More information

Equations from Relativistic Transverse Doppler Effect. The Complete Correlation of the Lorentz Effect to the Doppler Effect in Relativistic Physics

Equations from Relativistic Transverse Doppler Effect. The Complete Correlation of the Lorentz Effect to the Doppler Effect in Relativistic Physics Equtins m Rltiisti Tnss ppl Et Th Cmplt Cltin th Lntz Et t th ppl Et in Rltiisti Physis Cpyight 005 Jsph A. Rybzyk Cpyight Risd 006 Jsph A. Rybzyk Fllwing is mplt list ll th qutins usd in did in th Rltiisti

More information

Get Funky this Christmas Season with the Crew from Chunky Custard

Get Funky this Christmas Season with the Crew from Chunky Custard Hol Gd Chcllo Adld o Hdly Fdy d Sudy Nhs Novb Dcb 2010 7p 11.30p G Fuky hs Chss Sso wh h Cw fo Chuky Cusd Fdy Nhs $99pp Sudy Nhs $115pp Tck pc cluds: Full Chss d buff, 4.5 hou bv pck, o sop. Ts & Codos

More information

TER T U L OFEREE O URRET TREDS TEHOLOGY O OE [6] G OSYTHETS E P T VEME hv xl lly Gy xvly u k uv hk u l u v wll ly ul ly y lf x ly ul f l lly (F

TER T U L OFEREE O URRET TREDS TEHOLOGY O OE [6] G OSYTHETS E P T VEME hv xl lly Gy xvly u k uv hk u l u v wll ly ul ly y lf x ly ul f l lly (F HMEDBD RM UVERSTY STTUTE OF TEHOLOGY 48 8 08-0 E E D 0 BER M - - y u hv Gxl k lwy y u k k v wll wll ul k fu Bu ly vlv l hl l l l f hh u h hwv hul u y vll l f k hul vlu f ll vlu F l xl ff fv x l v ff l

More information

Axe Wo. Blood Circle Just like with using knives, when we are using an axe we have to keep an area around us clear. Axe Safety Check list:

Axe Wo. Blood Circle Just like with using knives, when we are using an axe we have to keep an area around us clear. Axe Safety Check list: k Ax W ls i ms im s i sfly. f w is T x, ls lk g sci Bld Cicl Js lik wi sig kivs, w w sig x w v k d s cl. Wi xs; cl (bld cicl) is s lg f y m ls lg f x ll d s d bv s. T c b bcs, wigs, scs, c. isid y bld

More information

A Review of Dynamic Models Used in Simulation of Gear Transmissions

A Review of Dynamic Models Used in Simulation of Gear Transmissions ANALELE UNIVERSITĂłII ETIMIE MURGU REŞIłA ANUL XXI NR. ISSN 5-797 Zol-Ios Ko Io-ol Mulu A Rvw o ls Us Sulo o G Tsssos Th vsgo o lv s lu gg g olg l us o sov sg u o pps g svl s oug o h ps. Th pupos o h ols

More information

INSTITUTIONAL DEVELOPMENT PLAN & LAWRENCE PUBLIC LIBRARY EXPANSON 707 VERMONT STREET LAWRENCE, KS SITE PLAN FOR LOCATION MAP SP-1

INSTITUTIONAL DEVELOPMENT PLAN & LAWRENCE PUBLIC LIBRARY EXPANSON 707 VERMONT STREET LAWRENCE, KS SITE PLAN FOR LOCATION MAP SP-1 OTIO -1 ITITUTIO VOT & IT O UI IY XO 0 VOT TT, -2 0 VOT TT, UI IY XO O ITITUTIO VOT & IT IT TI IITIO - ITITUTIO VOT & IT O UI IY XO 0 VOT TT, V '0" + 1' '0" '0" O " I YO IT TI, 20, V 2 '0" O, I U, I OTIU

More information

page 11 equation (1.2-10c), break the bar over the right side in the middle

page 11 equation (1.2-10c), break the bar over the right side in the middle I. Corrctios Lst Updtd: Ju 00 Complx Vrils with Applictios, 3 rd ditio, A. Dvid Wusch First Pritig. A ook ought for My 007 will proly first pritig With Thks to Christi Hos of Swd pg qutio (.-0c), rk th

More information

fnm 'et Annual Meeting

fnm 'et Annual Meeting UUVtK Ht.t, A 0 8 4 S.. Rittin Nub t, n L Y t U N i, n ' A N n, t\ V n b n k pny' ull N) 0 R Z A L A V N U X N S N R N R H A V N U R A P A R K A L A N Y Buin Add. N. Stt ity wn / Pvin) Ali l) lil tal?l

More information

Gavilan JCCD Trustee Areas Plan Adopted October 13, 2015

Gavilan JCCD Trustee Areas Plan Adopted October 13, 2015 S Jos Gvil JCCD Trust Ar Pl Aopt Octobr, 0 p Lrs Pl Aopt Oct, 0 Cit/Csus Dsigt Plc ighw US 0 Cit Arom ollistr igmr S Jos Trs Pios cr Ps 4 ut S Bito ut 0 0 ils Arom ollistr igmr Trs Pios 7 S Bito ut Lpoff

More information

and integrated over all, the result is f ( 0) ] //Fourier transform ] //inverse Fourier transform

and integrated over all, the result is f ( 0) ] //Fourier transform ] //inverse Fourier transform NANO 70-Nots Chapt -Diactd bams Dlta uctio W d som mathmatical tools to dvlop a physical thoy o lcto diactio. Idal cystals a iiit this, so th will b som iiitis lii about. Usually, th iiit quatity oly ists

More information

Energy, entropy and work function in a molecule with degeneracy

Energy, entropy and work function in a molecule with degeneracy Avill oli t www.worldsitifiws.om WS 97 (08) 50-57 EISS 39-9 SHOR COMMICAIO Ergy, tropy d work futio i molul with dgry Mul Mlvr Dprtmt of si Sis, Mritim ivrsity of th Cri, Cti l Mr, ul E-mil ddrss: mmf.um@gmil.om

More information

264m. Raggengill Gilkerscleuch. Abington. 250m. Cottage. Iss. Mast. 246m. TER R AC E 240m OO KE TE H U N TE COLEBROOKE. Over Abington STATION.

264m. Raggengill Gilkerscleuch. Abington. 250m. Cottage. Iss. Mast. 246m. TER R AC E 240m OO KE TE H U N TE COLEBROOKE. Over Abington STATION. I 4 4 I I L KY t lttio F 9 ott v bito 4 4 F L ii 3 lui 1 p F L F I I 9 F L I LK i i tip i 9 6 v bito U l K L 6 ott bito i 5 1 5 9 i oo 8 4 6 otl it o ov b i o 116-3 ott 6 i i ollt u o v bito 4 lo i 6 v

More information

Chapter 1 Fundamentals in Elasticity

Chapter 1 Fundamentals in Elasticity Fs s ν . Po Dfo ν Ps s - Do o - M os - o oos : o o w Uows o: - ss - - Ds W ows s o qos o so s os. w ows o fo s o oos s os of o os. W w o s s ss: - ss - - Ds - Ross o ows s s q s-s os s-sss os .. Do o ..

More information

ORDINANCE NO. 13,888

ORDINANCE NO. 13,888 ORDINANCE NO. 13,888 AN ORDINANCE d Mc Cd Cy Ds Ms, Iw, 2000, dd by Odc N. 13,827, ssd J 5, 2000, by g Sc 134-276 d cg w Sc 134-276, d by ddg d cg w Dvs 21A, cssg Scs 134-991 g 134-997, c w "C-3R" C Bsss

More information

ANSWER KEY. Page 1 Page 2 cake key pie boat glue cat sled pig fox sun dog fish zebra. Page 3. Page 7. Page 6

ANSWER KEY. Page 1 Page 2 cake key pie boat glue cat sled pig fox sun dog fish zebra. Page 3. Page 7. Page 6 P 1 P 2 y sd fx s d fsh z ys P 3 P 4 my, ms, m, m, m, m P 6 d d P 7 m y P 5 m m s P 10 y y y P 8 P 9 s sh, s, ss, sd sds, s, sh sv s s P 11 s P 12,, m, m, m,, dd P 13 m f m P 18 h m s P 22 f fx f fsh fm

More information

Summary: Binomial Expansion...! r. where

Summary: Binomial Expansion...! r. where Summy: Biomil Epsio 009 M Teo www.techmejcmth-sg.wes.com ) Re-cp of Additiol Mthemtics Biomil Theoem... whee )!!(! () The fomul is ville i MF so studets do ot eed to memoise it. () The fomul pplies oly

More information

Summary Introduction to Process Control

Summary Introduction to Process Control Suy todutio to Po otol Rf iut Fdbk otol hoy Fowd oto Fdbk oto tuto o ditub Plt Zhyu Yg otol yt obl: Albog Uivity Ebjg A lt: hyil yt dd to b otolld Sifitio: did yt fo DE5 Fll 4 A thodology: to dig otoll

More information

SULIT 3472/2. Rumus-rumus berikut boleh membantu anda menjawab soalan. Simbol-simbol yang diberi adalah yang biasa digunakan.

SULIT 3472/2. Rumus-rumus berikut boleh membantu anda menjawab soalan. Simbol-simbol yang diberi adalah yang biasa digunakan. SULT 347/ Rumus-umus eikut oleh memtu d mejw sol. Simol-simol yg diei dlh yg is diguk. LGER. 4c x 5. log m log m log 9. T d. m m m 6. log = log m log 0. S d m m 3. 7. log m log m. S, m m logc 4. 8. log.

More information

Noise in electronic components.

Noise in electronic components. No lto opot5098, JDS No lto opot Th PN juto Th ut thouh a PN juto ha fou opot t: two ffuo ut (hol fo th paa to th aa a lto th oppot to) a thal at oty ha a (hol fo th aa to th paa a lto th oppot to, laka

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

COHERENCE SCANNING INTERFEROMETRY

COHERENCE SCANNING INTERFEROMETRY COHERENCE SCANNING INTERFEROMETRY Pt 1. Bscs, Cto Austt Sus K. Rsy PD Mc 2013 OUTLINE No cotct suc sut systs Coc sc tot Sts ISO, ASME Pt sts Vto tst Cto, ustt pocus Octv ocus optzto Scc stts w sut stts

More information