On a Uniform Geometrical Theory of Diffraction based Complex Source Beam Diffraction by a Curved Wedge with Applications to Reflector Antenna Analysis

Size: px
Start display at page:

Download "On a Uniform Geometrical Theory of Diffraction based Complex Source Beam Diffraction by a Curved Wedge with Applications to Reflector Antenna Analysis"

Transcription

1 On a Unfom Gomtcal Thoy of Dffacton bad Comlx Souc Bam Dffacton by a Cuvd Wdg wth Alcaton to flcto Antnna Analy Dtaton Pntd n Patal Fulfllmnt of th qumnt fo th Dg Docto of Phloohy n th Gaduat School of Th Oho Stat Unvty By Youngchl Km, B.S., M.S. Gaduat Pogam n lctcal and Comut ngnng Th Oho Stat Unvty 009 Dtaton Commtt: Pabhaka H. Pathak, Adv obto oja-tan obt J. Bukhold

2 Coyght by Youngchl Km 009

3 Abtact A unfom gomtcal thoy of dffacton (UTD) oluton dvlod fo dcbng th hgh fquncy (HF) lctomagntc (M) fld uoundng an abtaly cuvd, fct lctcally conductng (PC) wdg, that llumnatd by a ont ouc, n comlx ac, whch gnat a comlx ouc bam (CSB). Th oluton ungly found to b th am a th UTD oluton obtand vouly fo PC cuvd wdg llumnatd by a al ont ouc aft t analytcally contnud fo dalng wth CSB llumnaton; hnc, t dfnd h a th CSB-UTD fo cuvd wdg. Th oluton fo cuvd wdg dvlod fom canoncal HF oluton fo a taght wdg wth lana fac. Fo a al ont ouc, th canoncal UTD oluton obtand va a ml aymtotc HF bad ft od Paul-Clmmow mthod (PCM) of tt dcnt. Howv, a CSB fld conttut a comlx wav, and th ft od PCM tctly not vald fo olvng th canoncal wdg oblm wth CSB llumnaton. Hnc, fo comlx wav, a dffnt, l comact, ft od aymtotc aoxmaton, known a th Van d Wadn mthod (VWM) of tt dcnt, nd to b mloyd. Th ft od VWM lad to a canoncal wdg oluton whch may b

4 vwd a an xtndd UTD (o UTD) wdg oluton fo th CSB llumnaton, dfnd h a th CSB-UTD oluton, bcau t can b xd a CSB-UTD = CSB-UTD. Howv, found to b nglgbl fo th wdg ca; t fo th aon that a ft od PCM bad CSB-UTD man accuat vn though PCM not tctly vald fo th ca. Aft havng tablhd th fact that th CSB-UTD oluton fo th canoncal wdg th am a f th canoncal UTD wdg oluton fo a al ouc xctaton mly and dctly analytcally contnud to dal wth a comlx ouc locaton (o a CSB), th CSB-UTD fo th abtaly cuvd wdg can thu alo b mlaly dvlod by analytcally contnung th coondng UTD oluton fo th am cuvd wdg xctd by a al ont ouc, to now dal wth th xctaton by a ont ouc n comlx ac (o CSB). Th cuvd wdg CSB-UTD oluton mloyd to analyz th adaton fom an offt aabolc flcto llumnatd by a CSB. Th CSB-UTD ult fo th flcto a comad wth a numcal hycal otc (PO) aoach to llutat th accuacy of th CSB-UTD. Th CSB-UTD xtmly fat comad to th numcal PO mthod; alo, th latt bcom ncangly tm conumng wth nca n fquncy, wha th CSB-UTD man ntally ndndnt of fquncy. Th comlx ont of ufac flcton and dg dffacton on th comlx xtnon of th flcto a comutd h ung a latvly fat and ffcnt ocdu, thu makng t vy actcal to tac comlx ay wth almot th am d and ffcncy a tacng al ay.

5 Ddcaton To H gloy, kngdom and ol v

6 Acknowldgmnt I would lk to x my nc gattud to my advo Pofo P. H. Pathak fo h gudanc, hang h valuabl knowldg and xnc, and dcuon thoughout th cou of th ach. Alo, I wh to thank hm fo h hl n th fnal aaton of th manuct. I would lk to thank th oth mmb of th dtaton adng commtt, Pofo obto oja-tan and Pofo obt J. Bukhold, fo th hlful commnt. Scal thank to go to my fom uvo D. Th-Hong L fo h gudanc dung my ft fw ya of tudy and ach at th lctoscnc Laboatoy. Alo, thank go to Andw O bn fo vwng th matal n at of chat 4 and all th Andc. Futhmo, I would alo lk to thank vyon who ha ayd fo m, cally my ant and my wf, th. Wthout th ay and tual uot, I would not hav comltd all th cou of my ducaton at Th Oho Stat Unvty. I alo thank my on, Ian, fo havng bn tayng hay and halthy, v nc h wa bon. Abov all, my dt gattud go to Hm who bought m to th Untd Stat and wokd though m fo H gat lan. v

7 Vta Al 4, 974. Bon Kwangju, South Koa 00...B.S. n Avonc ngnng, Koa Aoac Unvty Kyoungg, South Koa M.S. n lctcal ngnng, Th Oho Stat Unvty, Columbu, Oho 00nt..Gaduat ach Aocat, lctoscnc Laboatoy, Th Oho Stat Unvty, Columbu,Oho. Publcaton Y. Km and T-H. L, Shad Cculaly Symmtc Dual flcto Antnna by Combnng Local Convntonal Dual flcto Sytm, I Tanacton Antnna and Poagaton, vol 57, No, Jan 009. Fld of Study Majo Fld: lctcal and Comut ngnng v

8 Tabl of Contnt Abtact Ddcaton...v Acknowldgmnt..v Vta..v Lt of Fgu...x Chat:. Intoducton..... Canoncal oblm of D CSB dffacton by a taght wdg wth lana PC fac xctd by a comlx ln ouc.9.. Dffacton coffcnt of a CSB dffactd by a PC wdg fo a comlx ln ouc xctaton.... Numcal ult fo a comlx ln ouc xctaton Canoncal oblm of M CSB dffacton by a taght wdg wth lana PC fac xctd by an abtaly ontd comlx ont ouc Comlx ay-fxd coodnat ytm Dyadc dffacton coffcnt of an M CSB dffactd by a PC wdg Numcal ult fo an M comlx ont ouc xctaton ad analy of offt aabolc flcto antnna va CSB-UTD and CSB-UTD mthod 9 v

9 4.. GO bad CSB (CSB-GO) flctd fld by a PC cuvd ufac Dyadc CSB-UTD and CSB-UTD dffacton coffcnt fo a CSB xctd PC cuvd ufac Analytcal aoach to analyz offt aabolc flcto antnna va CSB-GO and CSB-UTD oluton Gomtcal Paamt aocatd CSB-GO flctd fld Gomtcal Paamt aocatd CSB-UTD dffactd fld Numcal ult fo analy of offt aabolc flcto antnna CSB ncdnt on nfnt aabolc flcto CSB ncdnt on fnt offt aabolc flcto Concluon and futu wok. 5 Andc: A. Two unfom hgh fquncy mthod of th tt dcnt...57 A.. Summay of valuaton of an ntgal va two unfom hgh fquncy mthod...57 A.. Summay of valuaton of I ( κ ) va th PCM mthod...6 A.. Summay of valuaton of I ( κ ) va th VWM mthod...67 A.. Mathmatcal dtal of th oluton bad on two mthod...69 I κ aco SB bad on I PCM...73 A... Chck on th contnuty of ( ) A... Chck on th contnuty of ( κ ) I aco SB bad on I VWM...77 B. Dcontnuty n th tanton functon at th hadow bounda...8 C. Comlx dffacton ont on th taght dg...8 D. Comlx flcton ont on an offt aabolc flcto ufac Comlx dffacton ont on an offt aabolc flcto dg...89 F. Comlx ouc bam...9 G. Shadow bounda...03 v

10 Lt of Fgu Fgu Pag. A ln ouc ncdnt on th wdg...0 ± and th comlx ξ lan toology fo a al ln ouc llumnaton of a canoncal wdg. Th tajctoy of ξ ndcatd. Stt dcnt ath, ( π ) along th al ax Comlx ln ouc bam llumnat on th wdg. b th bam aamt and bˆ th dcton of bam ax. Comlx ay and ouc locaton a dawn ymbolcally Stt dcnt ath, ( π ) tajctoy of ξ ndcatd fo ( ) 0 ± and th comlx ξ lan toology. Th Im ξ < Tajctoy of hadow bounda whn a CSB llumnat a half lan na th dg (a) Symbolcal comlx ay gomty at th nc of a PC wdg. (b) Comaon of total CSB fld and dffactd CSB fld obtand va CSB-UTD and CSB-UTD. Th ncdnt and flctd CSB a hadowd at ISB and SB Th tajcto α Im wth ct to th angl of th obvaton fo ISB (to) and SB (bottom) x

11 .8 Dcontnuou tanton functon aco ISB and SB. H, F and F 4 a tanton functon n th cond and fouth tm n dffacton coffcnt, whch a motant to ncdnt and flctd CSB, ctvly Contnuou cotangnt functon aco ISB and SB. H, C and C 4 a cotangnt functon n th cond and fouth tm n dffacton coffcnt, whch a motant to ncdnt and flctd CSB, ctvly Nglgbl addtonal CSB-UTD tm n th cond (to) and fouth (bottom) of CSB-UTD dffacton coffcnt whch a motant to th ncdnt and flctd CSB...4. Tajctoy of ξ na SB a th coondng ol, ξ, aoach ξ S = π 3.4 (b) P ( ξ ) 0 ξ aoach ξ S = π (a) Tajctoy of ξ na ISB a th coondng ol, ξ, aoach ξ S = π 3.4 (b) P ( ξ ) 0 ξ aoach ξ S = π (a) Symbolcal comlx ay gomty at th nc of a PC wdg. (b) Comaon of total CSB fld and dffactd CSB fld obtand va CSB-UTD and CSB-UTD. Th ncdnt and flctd CSB a hadowd at ISB and SB Th tajcto Im α wth ct to th angl of th obvaton fo ISB (to) and SB (bottom) Nglgbl addtonal CSB-UTD tm n th cond (to) and fouth (bottom) of CSB-UTD dffacton coffcnt whch a motant to th ncdnt and flctd CSB (a) Tajctoy of ξ na SB a th coondng ol, ξ, aoach ξ S = π 3.4 (b) P ( ξ ) 0 ξ aoach ξ S = π (a) Tajctoy of ξ na ISB a th coondng ol, ξ, aoach ξ S = π 3.4 (b) P ( ξ ) 0 ξ aoach ξ S = π (a) Symbolcal comlx ay gomty at th nc of a PC wdg. (b) Comaon of total CSB fld and dffactd CSB fld obtand va CSB-UTD and CSB-UTD. Th ncdnt and flctd CSB a hadowd at ISB and SB x

12 .9 Th tajcto Im α wth ct to th angl of th obvaton fo ISB (to) and SB (bottom) Nglgbl addtonal UTD tm n th cond (to) and fouth (bottom) of CSB-UTD dffacton coffcnt whch a motant to th ncdnt and flctd CSB (a) Tajctoy of ξ na SB a th coondng ol, ξ, aoach ξ S = π 3.4 (b) P ( ξ ) 0 ξ aoach ξ S = π (a) Tajctoy of ξ na ISB a th coondng ol, ξ, aoach ξ S = π 3.4 (b) P ( ξ ) 0 ξ aoach ξ S = π Tajctoy of CSB ISB and SB a th obvaton ont mov away fom th dg wth dffnt locaton of a ln ouc n al ac. Th CSB ISB and SB fom away fom ISB ( φ = 50 ) and SB ( φ =50 ) fo a al ouc xctaton of a wdg, ctvly A CSB ncdnt on th wdg wth t ax httng th ufac. Tajctoy of CSB ISB and SB a th obvaton ont mov away fom th dg wth dffnt locaton of a ln ouc n al ac. Th CSB ISB and SB fom away fom ISB ( φ =40 ) and SB ( φ = 0 ) fo a al ouc xctaton of a wdg, ctvly A CSB ncdnt on th wdg wth t ax httng th dg. Tajctoy of CSB ISB and SB a th obvaton ont mov away fom th dg wth dffnt locaton of a ln ouc n al ac. Th CSB ISB and SB a dntcal to ISB ( φ =40 ) and SB ( φ = 0 ) fo a al ouc xctaton of a wdg, ctvly A CSB ncdnt on th wdg wth t ax mng th ufac. Tajctoy of CSB ISB and SB a th obvaton ont mov away fom th dg wth dffnt locaton of a ln ouc n al ac. Th CSB ISB and SB fom away fom ISB ( φ =40 ) and SB ( φ = 0 ) fo a al ouc xctaton of a wdg, ctvly Th dffnc btwn ult fom CSB-UTD and CSB-UTD oluton fo ach ca hown n Fgu.6,.3 and.8, ctvly Comlx ont ouc bam llumnat on th wdg. b th bam aamt and bˆ th dcton of bam ax. Q a unqu comlx ont on th dg fo a x

13 gvn ouc and obvaton ont. Comlx ay and ouc locaton a dawn ymbolcally A ont ouc bam llumnaton of a PC wdg. H, Q a unqu al ont of dffacton on th dg fo a gvn ouc and obvaton ont (a) z-dctd comlx ont ouc llumnaton of a wdg. Comlx ay and ouc locaton a dawn only ymbolcally. (b) Comaon of total and dffactd CSB fld obtand va CSB-UTD and CSB-UTD Th tajcto of Im α wth ct to th angl of obvaton fo ISB (to) and SB (bottom) Nglgbl addtonal CSB-UTD tm n th cond (to) and fouth (bottom) of CSB-UTD dffacton coffcnt whch a motant to th ncdnt and flctd CSB (a) z-dctd comlx ont ouc llumnaton of a wdg. Comlx ay and ouc locaton a dawn only ymbolcally. (b) Comaon of total and dffactd CSB fld obtand va CSB-UTD and CSB-UTD Th tajcto of Im α wth ct to th angl of obvaton fo ISB (to) and SB (bottom) Nglgbl addtonal CSB-UTD tm n th cond (to) and fouth (bottom) of CSB-UTD dffacton coffcnt whch a motant to th ncdnt and flctd CSB (a) z-dctd comlx ont ouc llumnaton of a wdg. Comlx ay and ouc locaton a dawn only ymbolcally. (b) Comaon of total and dffactd CSB fld obtand va CSB-UTD and CSB-UTD Th tajcto of Im α wth ct to th angl of obvaton fo ISB (to) and SB (bottom) Nglgbl addtonal CSB-UTD tm n th cond (to) and fouth (bottom) of CSB-UTD dffacton coffcnt whch a motant to th ncdnt and flctd CSB A CSB ncdnt on a cuvd ufac wth dg. Th ncdnt, flctd and dffactd comlx ay a hown ymbolcally. Th ont of flcton wth th bam ax ( bˆ ) al...94 x

14 4. flcton of a comlx ay at a cuvd ufac hown ymbolcally Cautc dtanc aocatd wth th dffacton by a cuvd dg Plan tangnt to th cuvd ufac at th ont of dffacton Q An offt aabolc flcto llumnatd by an ncdnt CSB catd by a comlx ont ouc at wth an abtay ontaton, ˆ Incdnc and flcton of comlx ay on th aabolc offt flcto antnna. Th comlx ouc coodnat ytm, ( x S, y S, zs ) a dfnd wth ' at t ogn dg cuvatu aamt of an offt aabolc flcto. (a) 3D vw (lft) and th dg cuvatu n x-y lan (ght). Th ogn, O ', locatd at th cnt of flcto atu n x-y lan. (b) dg cuvatu and aamt n th lan contanng th dg Th comlx angl φ and φ a hown ymbolcally n th lan ndcula to th dg tangnt vcto ê at Q. Th dcton of ncdnc and dffacton, and unt ufac nomal at Q a ojctd onto th lan and alo ndcatd ymbolcally Ontaton of a ont ouc n al ac ndcula to th ncdnt CSB ax Incdnt CSB llumnaton fom th focu on an nfnt aabolc ufac wth a bam ax httng Q on th ufac...5 B 4. Comaon of CSB flcton fom an nfnt aabolc ufac. Th ncdnt CSB launchd at th focu Incdnt CSB llumnaton away fom th focu on an nfnt aabolc ufac wth a bam ax httng Q on th ufac...7 B 4.3 Comaon of CSB flcton fom an nfnt aabolc ufac. Th ncdnt CSB launchd away fom th focu Incdnt CSB llumnaton fom th focu on a fnt aabolc ufac wth a bam ax httng Q on th mathmatcal xtnon of th ufac...3 B x

15 4.5 Comaon of offt flcto antnna adaton, wth CSB llumnaton fom th focu, va th numcal PO, CSB-UTD, CSB-UTD. Th ncdnt CSB ax ht th mathmatcal xtnon of th flcto ufac n th ymmty lan Dtmnaton of hadow and lt gon whn two hadow bounda xt. (a) d t tajctoy of n th Im (b) flctd, ( ) dffactd ( ) and total CSB ( ) α vcnty of two SB Incdnt CSB llumnaton fom th focu on a fnt aabolc ufac wth a bam ax httng Q on th actual ufac fa away fom th dg B 4.8 Comaon of offt flcto antnna adaton, wth CSB llumnaton fom th focu, va th numcal PO, CSB-UTD, CSB-UTD. Th ncdnt CSB ax ht th actual flcto ufac fa away fom th dg n th ymmty lan Incdnt CSB llumnaton away fom th focu on a fnt aabolc ufac wth a bam ax httng Q on th mathmatcal xtnon of th ufac outd th B ymmty lan Comaon of offt flcto antnna adaton, wth CSB llumnaton away fom th focu, va th numcal PO, CSB-UTD, CSB-UTD. Th ncdnt CSB ax ht th mathmatcal xtnon of th ufac outd th ymmty lan Incdnt CSB llumnaton away fom th focu on a fnt aabolc ufac wth a bam ax httng Q on th actual ufac fa away fom th dg outd th B ymmty lan Comaon of offt flcto antnna adaton, wth CSB llumnaton away fom th focu, va th numcal PO, CSB-UTD, CSB-UTD. Th ncdnt CSB ax ht th actual ufac fa away fom th dg outd th ymmty lan Incdnt CSB llumnaton fom th focu on a fnt aabolc ufac wth a bam ax httng Q on th actual ufac na th dg n th ymmty B lan Comaon of offt flcto antnna adaton, wth CSB llumnaton fom th focu, va th numcal PO, CSB-UTD, CSB-UTD. Th ncdnt CSB ax ht th actual ufac na th dg n th ymmty lan...43 xv

16 4.5 Incdnt CSB llumnaton away fom th focu on a fnt aabolc ufac wth a bam ax httng Q on th actual ufac na th dg outd th ymmty B lan Comaon of offt flcto antnna adaton, wth CSB llumnaton away fom th focu, va th numcal PO, CSB-UTD, CSB-UTD. Th ncdnt CSB ax ht th actual ufac na th dg outd th ymmt y lan Incdnt CSB llumnaton away fom th focu on a fnt aabolc ufac wth a bam ax httng Q on th actual ufac na th dg outd th ymmty B lan Comaon of offt flcto antnna adaton, wth CSB llumnaton away fom th focu, va th numcal PO, CSB-UTD, CSB-UTD. Th ncdnt CSB ax ht th actual ufac na th dg outd th ymmty lan Incdnt CSB llumnaton away fom th focu on a fnt aabolc ufac wth a bam ax httng Q on th actual ufac na th dg outd th ymmty B lan Comaon of offt flcto antnna adaton, wth CSB llumnaton away fom th focu, va th numcal PO, CSB-UTD, CSB-UTD. Th ncdnt CSB ax ht th actual ufac na th dg outd th ymmty lan Incdnt CSB llumnaton away fom th focu on a fnt aabolc ufac wth a bam ax httng Q on th actual ufac na th dg n th ymmty B lan Comaon of offt flcto antnna adaton, wth CSB llumnaton away fom th focu, va th numcal PO, CSB-UTD, CSB-UTD. Th ncdnt CSB ax ht th actual ufac na th dg nd th ymmty lan...5 A. Banch cut fo a ud n dfnng F( ± κa )...65 A. Two banch of F. Th o banch th on coondng to hadd gon...66 C. ay gomty to fnd a comlx dffacton ont on a taght wdg...83 F. Th al at of th comlx dlacmnt contant on hod (hafont jk of th CSB functon ), whl th magnay at contant on th xv

17 jk hybolod (quamltud ufac of ). It notd that and a nomalzd wth b n th Fgu...94 F. A hcal wav adaton and a CSB adaton...99 F.3 Coodnat of a comlx ouc...0 G. Th tt dcnt ath () and th tajctoy of ol n th comlx ξ lan G. Th tt dcnt ath () and th tajctoy of ol n th comlx α lan...04 xv

18 Chat :Intoducton A unfom gomtcal thoy of dffacton (UTD) oluton dvlod fo dcbng th hgh fquncy (HF) lctomagntc (M) fld uoundng an abtaly cuvd, fct lctcally conductng (PC) wdg, that llumnatd by a ont ouc, n comlx ac, whch gnat a comlx ouc bam (CSB). Th oluton ungly found to b th am a th UTD oluton obtand vouly fo PC cuvd wdg llumnatd by a al ont ouc aft that analytcally contnud fo a CSB llumnaton; hnc, t dfnd h a th CSB-UTD fo cuvd wdg. Th oluton fo cuvd wdg dvlod fom two and th dmnonal canoncal HF oluton fo a taght wdg wth lana fac llumnatd by ln and ont ouc, ctvly. Fo a al ln o ont ouc, th canoncal UTD oluton obtand va a ml aymtotc HF bad ft od Paul-Clmmow mthod (PCM) of tt dcnt. Howv, a CSB fld conttut a comlx wav, and th ft od PCM tctly not vald fo olvng th canoncal wdg oblm wth CSB llumnaton. Hnc, fo comlx wav, a dffnt, l comact, ft od aymtotc aoxmaton, known a th Van d Wadn mthod (VWM) of tt dcnt, nd to b mloyd fo olvng th canoncal oblm. Th ft od VWM lad to a canoncal wdg

19 oluton whch may b vwd a an xtndd UTD (o UTD) wdg oluton fo th CSB llumnaton, dfnd h a th CSB-UTD oluton, bcau t can b xd a CSB-UTD = CSB-UTD. Howv, found to b nglgbl fo th wdg ca; t fo th aon that a ft od PCM bad CSB-UTD man accuat vn though PCM not tctly unfomly vald fo th ca. H unfomly vald f to th aymtotc oluton to th ft od ovd a contnuou total fld aco th o calld ncdnt and flctd bam hadow bounda a wll b laboatd futh n th chat. Aft havng tablhd th fact that th CSB-UTD oluton fo th canoncal wdg th am a f th canoncal UTD wdg oluton fo a al ouc xctaton mly and dctly analytcally contnud to dal wth a comlx ouc locaton (o a CSB), th CSB-UTD fo th abtaly cuvd wdg can thu alo b mlaly dvlod by analytcally contnung th coondng UTD oluton fo th am cuvd wdg xctd by a al ont ouc, to now dal wth th xctaton by a ont ouc n comlx ac (o CSB). Th cuvd wdg CSB-UTD oluton mloyd to analyz th adaton fom an offt aabolc flcto llumnatd by a CSB. Th CSB- UTD ult fo th flcto a comad wth a numcal hycal otc (PO) aoach to llutat th accuacy of th CSB-UTD. Th CSB-UTD xtmly fat comad to th numcal PO mthod; alo, th latt bcom ncangly tm conumng wth nca n fquncy, wha th CSB-UTD man ntally ndndnt of fquncy. Th comlx ont of ufac flcton and dg dffacton on th comlx xtnon of th flcto a comutd h ung a latvly fat and ffcnt ocdu, thu makng t vy actcal to tac comlx ay wth almot th

20 am d and ffcncy a tacng al ay. Th abov commnt a ntally xandd, n mo dtal, n th manng at of th chat, whch alo nclud a ummay of th latonh of th nt wok to that otd vouly by oth. Th CSB-UTD oluton fo th cuvd wdg dvlod h utlzd fo th ad and accuat analy of lctcally lag offt aabolc flcto antnna llumnatd by a CSB. On not that th total fld comutd va convntonal UTD fo al ay (a wll a by th unfom aymtotc thoy of dffacton (UAT) [4]) fal n gon of ay cautc, whl th total fld comutd va th CSB-UTD man vald th nc th cautc a now uhd nto comlx ac fo th CSB xctaton ca. Fo xaml, a convntonal UTD (o UAT) ay analy of a tycal focu-fd offt aabolc flcto antnna fal n th dcton of th man bam n th fa zon bcau of th ovla of th cautc of al (a ood to comlx) flctd and dffactd ay, ctvly, along th flcton hadow bounday [5]. A a ult, th hycal otc (PO) ufac ntgaton mthod oftn mloyd to comut th fld na th man bam and ft fw dlob to comlmnt th UTD (o UAT). Howv, nc th PO mthod bad on th ntgaton ov cunt nducd on th flcto ufac [6] and th ntgaton n gnal ha to b fomd numcally, t cla that a numcal PO valuaton comutatonally vy nffcnt, cally fo th analy of lctcally lag flcto antnna. In contat, th nt CSB-UTD oluton xtmly fat, nc t xd n clod fom and do not qu any numcal ntgaton. Alo, nc th comlx ay ath of a CSB a ndndnt of th fquncy, th comutaton vy ffcnt comad to th fquncy dndnt numcal PO mthod of analy. 3

21 In addton, th nt mthod dvlod n th dtaton ovd a hycal nght nto th vaou adaton/cattng wav contbuton wthn th famwok of UTD. It alo notd that th PO mthod fo flcto antnna u th aoxmat gomtcal otc (GO) cunt n th xact ntgal ntaton fo th cattd fld; howv, th GO cunt dcontnuou at a hadow bounday and not coct na an dg [7,8], but th PO tll a aonabl aoxmaton whn th adatng/cattng ufac wll llumnatd and lowly vayng wth ct to th lctcal wavlngth. Nvthl, th PO mthod xctd to b naccuat n gon wh th GO cunt do not oduc th domnat cattng [5]. A a conqunc, whn a convntonal M ont ouc n al ac llumnat a aabolc flcto, th numcal PO mthod not a accuat a th convntonal UTD fo al ay cally fo dctng th fld n th dlob gon away fom th man bam. On th oth hand, th PO mthod dct th man bam and ft fw dlob accuatly whl th ay mthod (UTD and UAT) fal n th man bam gon fo th aon mntond al. Th naccuacy of th PO mthod n th gon away fom th man bam can b movd by addng an addtonal dg dffacton cocton tm bad on th hycal thoy of dffacton (PTD) [9]. Howv, whn a CSB, a ood to a al ouc, llumnat an offt aabolc flcto na th dg, th PO mthod may not b uffcntly accuat n th gon of man bam fo th followng aon. Whn th ax of an ncdnt CSB m th flcto and ht ntad th mathmatcal xtnon of th aabolc flcto at t dg, thn th flctd CSB not domnant, bcau th dffacton of th ncdnt CSB can now bcom a motant a th flctd CSB fld 4

22 contbuton. In addton, nc th ncdnt CSB dcayng adly away fom t ax, th aoxmat ufac cunt nducd by th ncdnt CSB a concntatd na th dg wh th nducd cunt bad on th PO aoxmaton a ncoct [7,8]. Thfo, whn an ncdnt CSB ax dctd outd th actual flcto ufac na th dg, th numcal PO can lo t accuacy n th gon of th dlob and obly vn th man bam, fo th ty of CSB. Whn an ncdnt CSB ax ht th actual flcto ufac na th dg, th flctd CSB much mo domnant than th dffactd CSB, and fo th ca th PO mthod lo only nglgbl amount of accuacy (< 0. db) n th man bam gon comad to th ca whn th ncdnt CSB ax m th actual flcto ufac. Th PO mthod of cou cov t accuacy n th gon of man bam whn th ncdnt CSB ax ht th actual ufac fa away fom th dg. Conquntly, th nt CSB-UTD mthod dvlod n th dtaton ovcom th lmtaton of UTD (and UAT) fo al ay, and alo of th numcal PO. Th nt CSB-UTD oluton dvlod n th dtaton can alo b gnalzd to tat an atgmatc Gauan bam (GB) llumnaton of abtay wdg. Alo, th CSB-UTD oluton can b ald to analyz flcto antnna llumnatd by an abtay M fld fom a fd o a ubflcto, aft xandng th M fld llumnatng th flcto nto a t of CSB. Howv both th toc a not tatd n th nt wok. Fo an ncdnt CSB whch tk a flctng ufac uffcntly fa fom any ont on th dg, th bam dffactd by th dg bcom nglgbl n comaon to flcton ffct bcau th ncdnt CSB dcay adly away fom t ax. Howv, 5

23 whn th ncdnt CSB tongly llumnat th dg and whn th ncdnt CSB ax ntct th flcto ufac, thn th bam dffactd by th dg not nglgbl, and th only oton of ncdnt CSB that tk th flctng ufac gt flctd. Th ath of th CSB whch flctd fom th ufac found va gomtcal otc (GO) aft analytcally contnung th locaton of ouc nto comlx ac n th wok; hnc, th flctd contbuton wll hncfoth b fd to a th CSB-GO fld. To obtan th flctd bam fld va CSB-GO, t ncay to fnd th comlx ont of flcton fo a gvn obv that obvouly locatd n al ac. Snc th ncdnt CSB comod of comlx ay that oagat n comlx ac fom th ouc oton n comlx ac to th obv n al ac, on ha to tac th comlx ay n comlx ac to fnd th comlx ont of flcton on th comlx xtnon of hycal flctng ufac. Thu, th tatonay ha condton mloyd and th comlx ont of flcton fo a gvn al obv achd numcally. Only fo a wdg wth lana fac can th comlx ont of flcton b found n clod fom mly va mag thoy ud n conjuncton wth a comlx ont ouc locaton. Th ont of dffacton on th dg of a cattng objct alo bcom comlx fo a CSB llumnaton. Th Kll law of dg dffacton [,3] mloyd to fnd a comlx dffacton ont, fo a gvn al obv, whch alo ha to b numcally achd. It notd that fo a two dmnonal (D) wdg ca wth a CSB llumnaton (du to a comlx ln ouc), th ont of dffacton bcom al and concd wth th dg, a can b hown analytcally aft mly calzng th oblm of fndng a dffacton ont on a 3D taght dg to th D ca. Th comutatonal ffot utlzd n th wok 6

24 fo achng both comlx ont of flcton and dffacton nglgbl and th mthod ud h fo localty uch comlx ont aocatd wth comlx ay mak t almot a fat a tacng convntonal ay n al ac. It notd that all oth M fld aamt aocatd wth comlx ont of flcton and dffacton gnally bcom comlx n comutng th flctd and dffactd fld va CSB-GO and CSB-UTD, ctvly. Th dtal of dvlomnt of flctd and dffactd fld contbuton to th fld ang fom a CSB llumnaton of a cuvd ufac, and th aocatd comlx ay aamt (ncludng ont of flcton and dffacton) a dcbd lat n th dtaton. Whn an ncdnt CSB tk a flctng ufac wth an dg o t mathmatcal xtnon na th dg, only th oton of comlx ay aocatd wth th ncdnt CSB that a catud by th ufac a tanfomd nto th flctd CSB. Thu, th ncdnt and flctd CSB bcom dcontnuou at th ctv hadow bounda whch a taght ln n comlx ac. Unlk th adaton of M fld xctd by a al ont ouc, th CSB oagat though comlx ac untl t av at th obvaton n al ac. Thfo, th locaton of GO lk ncdnt and flcton hadow bounda, aocatd wth th ncdnt and flctd at of th CSB, namly th ISB and SB, ctvly, gnally do not aa to b at th am locaton a fo th ca of th M fld xctd by a al ont ouc. Futhmo, th CSB-GO latd ISB and SB can not b found aly vn fo a latvly ml oblm, uch a fo th ca of a D CSB xctaton of a half lan. Hnc, th xlct xon to locat th ISB and SB a dvlod n th wok fo th CSB xctaton of a gnal 7

25 cuvd wdg, and th condton dfnng th xtnc of th lt and hadow gon fo th ncdnt and flctd CSB a alo tablhd fo th ca o that a comlt CSB- UTD mthodology bcom avalabl fo th u. It motant to not that only fo th canoncal taght wdg wth lana fac and fo a wdg wth cuvd fac n D, th flctd CSB alo a CSB ognatng fom a comlx ont ouc locatd at th mag ont. On th oth hand, an ncdnt CSB that flctd fom a wdg wth cuvd fac n 3D, th flctd bam bcom atgmatc vn n comlx ac. Th nt CSB-UTD oluton ft dvlod va a unfom aymtotc valuaton of an ntgal ntaton fo th M fld uoundng a canoncal PC wdg xctd by a D and 3D CSB. Two dffnt but wll tablhd unfom aymtotc tchnqu, bad on th mthod of tt dcnt, a mloyd, fo aon gvn blow, fo valuatng th canoncal wdg fld ntgal at HF. Th unfom aymtotc tchnqu a tycally fd to a th Paul-Clmmow mthod (PCM) [3, 9-] and th Van d Wadn mthod [-5], ctvly. Th tchnqu hav bn comad mathmatcally n th at [,6-0]. Both tchnqu a utlzd to valuat th ntgal that nt th fld n th canoncal oblm of th dffacton of an ncdnt D and 3D CSB by a taght wdg wth PC lana fac. Thn, th oluton of th D and 3D canoncal oblm whch a xd wthn th UTD fomat a gnalzd ung aoat ocdu to dal wth th ca of CSB llumnaton of an abtaly cuvd PC wdg. Th latt dctly alcabl to th analy of aabolc offt flcto xctd wth a CSB, and alo to gnal (not 8

26 ncaly aabolc) flcto gomt. In th nt wok, th CSB-UTD ald only to aabolc flcto to llutat t accuacy and d. Th PCM and VWM a tycally utlzd fo aymtotcally valuatng a cla of comlx contou ntgal, by th mthod of tt dcnt, whn thy contan ntgand chaactzd by a ft od addl ont and a naby ml ol. A n fom [3,6], uch tt dcnt mthod can alo b utlzd fo tatng hgh od addl ont, hgh od ol, and multl ol, tc.; howv, th tuaton a not condd n th dtaton. It known that th ft od aymtotc oluton bad on th PCM tctly not vald fo tatng any of th canoncal oblm tanng to comlx wav [4,7,8], wha th ft od VWM vald vn fo th ca. Howv, t found h that vn whn t ald to dal wth comlx wav aocatd wth CSB ty wdg llumnaton, th ft od PCM wok ungly accuatly fo analyzng th oblm of CSB dffacton by a wdg; an xlanaton fo th unxctd ult ovdd n th wok. Th latt outcom of th PCM bad oluton fo th CSB wdg dffacton oblm ha an motant mlcaton on th oblty of xtndng th unfom gomtcal thoy of dffacton (UTD) oluton fo a PC wdg xctd by a ouc otond n al ac [,3,], to dctly tat th ca of CSB wdg xctaton (tanng to a ouc otond n comlx ac) mly va analytc contnuaton of th avalabl UTD oluton fo th al ouc. It obvd, n gnal, that th PCM mo convnnt fo numcal comutaton than th VWM, cally fo tatng oblm nvolvng al (a ood to comlx) wav; th u bfly dcud n Andx A, and a lghtly mo convnnt fom 9

27 of th VWM alo ntd h. Th latt xd a th um of th PCM bad ult togth wth a cocton tm; th aangd VWM fd to n th wok a th xtndd PCM (o PCM). Th PCM (whch ovd an xlct cocton to PCM) thu vald fo both al and comlx wav, nc t mly aangmnt of th VWM whch mhaz th dffnc btwn th ft od PCM and VWM. Snc th convntonal UTD fo al ay ognally bad on th aymtotc valuaton of a tnnt wav ntgal va PCM [,3], th oluton found va PCM (=VWM), whch alo vald fo comlx wav, fd to a th xtndd UTD (UTD) oluton n th dtaton. In th PCM and VWM, ctvly, th ognal ath of ntgaton n th comlx lan dfomd to th tt dcnt ath () on whch th ha of th ntgand tay contant o a to allow an ffcnt clod fom valuaton of th wav ntgal at hgh fqunc fo whch th ha of th ntgand othw hghly ocllatoy. A ol of th ntgand can b cod n th contou dfomaton to th ; hnc, t contbuton mut b ncludd va th Cauchy du thom []. Oth banch cut contbuton, f thy xt, mut alo b ncludd whn thy a cod n th contou dfomaton; howv, uch banch cut contbuton a not catud fo th canoncal oblm of ntt whn thy a fomulatd n tm of ctal ntgal n ola (o angula ctal doman) fom fo th total fld. Tycally, n th ctal ntgal fomulaton of th oluton to th canoncal oblm of ntt, th mov latv to th addl ont (o vc va) a th obvaton ont mov n ac; hnc, th a om obvaton dcton (o act angl) fo whch th lvant ol 0

28 catud n th contou dfomaton but not o fo oth angl, thu dfnng a hadow gon wh th ol wav contbuton abnt lavng only th contbuton. In atcula, lt u nt th total cala wav fld nt n th canoncal oblm of CSB dffacton by a PC wdg, whch a addd n th dtaton. Alo lt u PW and u nt th catud ol wav contbuton (o th du of th ntgand) and th wav contbuton, ctvly. Thn, u = u H, (-) PW u wh th Havd t functon, H, ha a valu of unty whn th ol catud, and zo whn th ol not catud, ctvly, n th dfomaton of th ognal ntgaton contou to th. vn though u PW H a dcontnuou functon, u not; hnc, u mut contan a comnatng dcontnuty to k th total fld, u, contnuou vywh n th ac uoundng th adatng o dffactng tuctu. Whn u aoxmatd aymtotcally, thn on obtan an ntally clod fom aymtotc xanon n nv factonal ow of fquncy fo th tm [4,6,8,]. To facltat a ytmatc dvlomnt of th aymtotc, th ntgal n th ognal comlx ctal angula lan, dnotd h a th ξ lan, tanfomd va a tandad mang to th al ax n th nw tanfomd comlx doman, dnotd h by α, wh now th addl ont alway man fxd at th ogn ( α =0) of th comlx α lan [4]. Th ognal ctal ntgal thn ducd to a gnc ntgal along th nfnt al ax n th α doman; uch an ntgal can b

29 ducd ytmatcally va th PCM o th VWM to av at th dd unfom aymtotc xanon [9,-4,6-8]. H, unfom man that th ultng aymtotc uod to ovd a total hgh fquncy oluton that man unfomly vald aco th ol wav hadow bounday (SB); th latt SB dlnat th uoundng ac nto a hadow and lt gon coondng to wh th upw tm xt and wh t do not (accodng to whn H o 0 n ()). In th α doman, th alway man fxd along th al α ax (wth th addl ont at th ogn ( α =0) ndcatd abov; a uch, only th ol can mov aco th n th α lan a th obv chang oton. Th locaton of th SB can thu b dfnd a that obvaton (o act) dcton at whch th ol jut co th. In th gad, t notd that f only th ft od ult n th aymtotc valuaton tand n th PCM, thn th aymtotc ult fo u to th od contnuou only f th ol co th though th addl ont at th ogn ( α =0) ; othw, th PCM bad ult not tctly unfom (.., do not guaant contnuty) aco th SB. On th oth hand, t can b hown that th ft od, VWM alway man vald aco th SB,.. t ovd a contnuou total fld u aco th SB, vn f th ol co th away fom th addl ont. Fo all th canoncal oblm bng condd h nvolvng comlx wav, th ol alway co th away fom th addl ont. Conquntly, only th VWM bad aoach wll man tctly unfom fo comlx wav bng tatd h. Howv, a mntond vouly, t hown n th wok, that th PCM wok ungly accuatly fo th oblm of CSB dffacton by a ) a

30 wdg. Of cou, t ha bn vouly dmontatd that th comlt PCM bad aymtotc xanon can b tanfomd nto th comlt VWM bad aymtotc xanon [,6,8]; thu, t ndd obl that contnuty of th aymtotc tmat fo th total u can b tod n th PCM whn th ol co th away fom th addl ont, by ncluon of hgh od tm n th PCM. On th oth hand, uch addton of hgh od tm to th ft od PCM mak t fa mo comlcatd to u than f on mloy only th ft od tm of th VWM. It n that n ca wh th ft od PCM bad oluton vald, t gnally ml fo alcaton than th ft od VWM bad oluton. Aft th valuaton of th ntgal contbuton, u n (-) va PCM and PCM (=VWM) who oluton a dcbd n dtal n Andx A, th PCM (o UTD) oluton contan th cocton tm fo th PCM (=UTD) oluton and t ymbolcally xd a wh PCM u and PCM u u PCM = u PCM, (-) a oluton of u found va PCM and PCM, ctvly. A xland bfo, a cocton to PCM u wthout whch PCM u alon can not man tctly vald fo comlx wav wh th ol gnally co th away fom th addl ont. If th ol co th though th addl ont a t gnally do fo oblm nvolvng al wav, only thn do = 0 at th SB o that PCM PCM u = u n tho ca. In th comlx wav oblm nvolvng CSB dffacton by a wdg, 3

31 found to b ungly nglgbl a mntond al, and o fo th cal ca PCM PCM UTD UTD u u ( u ) u a dcud n Andx A. Many ach n th at hav xlotd th CSB conct o t Gauan bam (GB) fld aoxmaton wthn th aaxal gon [3][38]. A vaty of oblm hav bn tatd by thm fo bam oagaton n comlx nvonmnt ncludng GB tanmon though adom by Gao and Fln [3], GB tanmon though lan and cuvd dlctc lay by Macl and Fln [4,5], and though nhomognou and anotoc mda by Hyman [6]. Moov, a owful combnaton of th CSB mthod and th aymtotc ay tho ha bn ald fo th analy of bam flcton fom th 3-D aabolc flcto ufac by Halman and Fln [7] wh an nfnt aabolc ufac ud and hnc th dffacton abnt n that wok. Du to th dlacmnt of th ouc locaton nto comlx ac n [7], ach ont of flcton tacd n comlx ac by ung th tatonay ha condton and th comlx flcton ont a found numcally. Gn, Bton and Fln [8] ntoducd th conct of hadow bounda fo D CSB llumnatng a half lan, and ovdd clod fom oluton n two cal ca aft ntoducng ctan aoxmaton; on whn th fld ont locatd n fa zon of th dg and th oth whn th bam wat locatd fa away fom th dg. In th lat ca, th dlacmnt of a ouc n al ac nto comlx ac do not hft th hadow bounda gnfcantly, bcau th bam fld may b n a lan wav at th dg manatd by a ouc n al ac fa away fom th dg. Sudan and Jull n [9, 30, 3] hav utlzd th combnaton of th CSB mthod and an analytc contnuaton of 4

32 UTD fo cala ln and ont ouc. Howv, n [9], th SB a found aoxmatly only fo th ca wh th dtanc fom th dg to th obv much fath than th dtanc fom th dg to th bam wat. In addton, thy dd not tat th ca wh th bam ax clo to th dg,.. whn th bam tongly llumnat th dg. In [30], thy dmontatd th ca whn th dg on th bam ax, n whch th dg ht only by a al ay (axal ay). In atcula, thy dd not comut a combnaton of th flctd and dffactd bam fld to how th comlt total fld and th contnuty of th total fld uoundng a -D aabolc flcto n [3], but howd only th dffactd fld. Thy mloyd atu ntgal (AI) mthod fo calculatng th man bam and ft fw dlob ntad of calculatng CSB flctd and dffactd fld n th fowad gon. Anatau and Pathak [3], and Zogb and Pathak [33], dvlod an aoxmat aoach fo analyzng th flcton and dffacton of an ncdnt GB by a fnt cuvd flcto; t bad on an aymtotc valuaton of th aoxmat PO ntgal fo th ufac cunt nducd by th ncdnt GB on th D and th 3D flcto gomt, ctvly. Th aoach ovd clod fom oluton fo both flctd and dffactd fld, a wll a fo th comlx flcton and dffacton ont. A a ult, th oluton vy fat to analyz lctcally lag flcto antnna a comad to numcal valuaton of PO and atu ntgal (AI) fomulaton. Th ult n [3] vald only fo analy of -D flcto n th fa zon. Th oluton n [33] ovd 3-D dg dffacton fom flcto, but jut a th wok n [3], th oluton of [33] alo contan ctan aoxmaton n th PO ntgand; futhmo th ultng xon fo both th 5

33 flctd and dffactd fld a mo comlcatd than th UTD xon dvlod h. Chou and Pathak [34] dvlod a mo comact and gnal 3-D oluton to ovcom th dfcncy n [33] and ovdd a mo comact oluton. Th oluton n [34] alo alcabl to mo gnal 3-D cuvd ufac than tho whch can b tatd va [33]. Th comlx ont of flcton and dffacton n [34] a found n clod fom oluton bad on a local aabold aoxmaton at th flcton ont thby avodng comlx ay tacng. Howv, th accuacy of th oluton n [34] wthn th am lvl a th numcal PO oluton, bcau th GB analy dvlod fom an aymtotc clod fom valuaton of th PO ntgal tlf. Hyman and Ianconu [35] mloyd th CSB mthod n th tm doman to analyz th dffacton of a uld bam by a wdg. Thy ovdd uful hycal nght nto th bhavo of th cattd wavackt, but th oluton lmtd to a taght dg wth lana fac. Plo and Sll [36] dvlod a numcal aoach though th alcaton of th aabolc quaton to obtan th oluton of GB dffacton fom a PC wdg. A ln ntgal ntaton of PO dvlod by Matn t al [37] to fnd th cattd fld fom a fctly conductng qua lat. Th ncmntal thoy of dffacton (ITD) ha bn ald to comut th dffactd fld by an dgd objct by a CSB n th wok of Polm t al [38]. Th ITD tchnqu avod fndng comlx ont of dffacton, but ntad qu th valuaton of a ln ntgal on th dg; nvthl t ha hown t ffctvn to comut th fld adatd and cattd fom fctly conductng qua lat and dk llumnatd by CSB. Howv, th wok n [36-38] tctd to an dg n tuctu wth lana fac. Thfo, th 6

34 nt CSB-UTD oluton, dvlod h n clod fom to dcb th wav flctd and dffactd by an abtay 3D cuvd PC wdg llumnatd by a CSB ovcom th lmtaton of afomntond contbuton and ovd a mo gnal ult obtand ytmatcally fom an aoat xtnon of aymtotc oluton to aoat canoncal oblm. Th fomat of th dtaton a follow. In Chat, th canoncal oblm of a CSB dffacton by a PC taght wdg wth lana fac llumnatd by a comlx ln ouc tatd. Th cala D dffacton coffcnt nt wthn th CSB-UTD and CSB-UTD oluton that a dvlod n chat a xlctly dntfd. In Chat 3, th dyadc dffacton coffcnt of CSB-UTD and CSB-UTD a obtand fo th canoncal oblm of a 3D M CSB dffacton by a PC taght wdg wth lana fac. In both Chat and 3, numcal ult a ntd to how th valdty of two unfom oluton namly th CSB-UTD bad on th PCM and th CSB- UTD bad on th VWM, ctvly, and ov numcally th cocton tm n th dffacton coffcnt of CSB-UTD nglgbl o that CSB-UTD bacally and ungly duc to CSB-UTD. Th latt jutf obtanng th CSB-UTD oluton fom a dct analytc contnuaton of th coondng UTD wdg oluton whch wa obtand vouly va a PCM bad valuaton of aoat canoncal wdg dffacton oblm [,3]. Wthout th abov jutfcaton obtand analytcally, on could not hav bn u that CSB-UTD would ovd contnuou total fld aco ISB and SB a tctly guaantd by CSB-UTD, but not by CSB-UTD. Th xlct xon to dtmn th ISB and SB a alo dcud n both analytcally and 7

35 numcally. Alo, th cta to dtmn th lt and hadow gon fo th ncdnt and flctd CSB a hown fo th gnal ca of CSB llumnaton of an abtay cuvd wdg. In Chat 4, th oluton fo th oblm of a fully 3D cuvd PC wdg xctd by a CSB dvlod by gnalzng th canoncal oluton obtand n chat 3 ung analytcally contnuaton agumnt. Th gnal CSB-UTD oluton thn ald to analyz a 3D aabolc flcto llumnatd by a CSB, and numcal ult obtand va both th CSB-UTD and CSB-UTD a ntd fo th ca and comad wth th numcal PO mthod to dmontat th accuacy and comutatonal ffcncy of th clod fom CSB-UTD oluton. It notd that th aymtotc aoxmaton ud n chat and 3 fo olvng th canoncal taght wdg oblm, and hnc thn xtnon ud n chat 4 to dal wth an abtaly cuvd wdg, a all vald a long a th obvaton ont not xtmly clo to th dg. Th latt ntal to guaant that κ, th aymtotc lag aamt ud n chat and 3 nv too mall to tan th aymtotc HF CSB-UTD oluton fo all ca tatd n th wok. Som concluon and toc fo futu wok a ntd n Chat 5. An j t ω tm dndnc aumd and ud n th dvlomnt whch follow; h t dnot tm and ω dnot th angula fquncy of th wav. 8

36 Chat : Canoncal oblm of D CSB dffacton by a taght wdg wth lana PC fac xctd by a comlx ln ouc In th chat, t of ntt to dvlo th CSB-UTD and CSB-UTD dffacton coffcnt fo a canoncal D oblm of a CSB dffactd by a taght wdg wth PC lana fac xctd by a ẑ - dctd comlx ln ouc. Th taght dg locatd along th z ax. Alo, th wdg uoundd by f ac (wth wavnumb k). Th ctal ntgal ntaton of th Gn functon fo ẑ - dctd lctc o magntc ln ouc xctaton gvn n [] ud, aft analytcally contnung th locaton of th ouc nto comlx ac to tat th comlx ln ouc xctaton oblm. Th dffacton coffcnt a found by aymtotcally valuatng th ntgal va two mthod of tt dcnt, namly, th PCM whch lad to th wdg oluton CSB-UTD and PCM (= aangd VWM) whch lad to th CSB-UTD wdg oluton; Th PCM and PCM (= VWM) mthod a vwd n Andx A. 9

37 ( ) ρ,φ ρ y φ ' φ ρ ' ( ρ', φ' ) x ( n)π Fgu.. A ln ouc ncdnt on th wdg. 0

38 .. Dffacton coffcnt of a CSB dffactd by a PC wdg fo a comlx ln ouc xctaton Ft, cond a ẑ -dctd unfom ln ouc locatd at ρ ' = ( ρ', φ' ) n al ac whch oduc a cylndcal cala wav that llumnat a PC nfnt wdg, coondng to a D oblm. Th total lctc fld, = z ˆ, and th magntc fld H = zh ˆ z, du to an lctc and a magntc ln ouc, ctvly, at ρ' can b wttn u a, n tm of a two dmnonal cala Gn functon, ( ρ '), h ρ z H z ( ρ, ρ' ) = jωµ I u ( ) ρ ρ' ( ρ, ρ' ) = jωε M u ( ρ ρ' ) z h (.) wh th al obvaton locaton at ρ = ( ρ, φ). H, ω th angula fquncy of th wav. Alo, µ and ε a th mablty and mttvty of th otoc, homognou mdum uoundng th wdg, ctvly. In (.), I and M a th tngth of th lctc and magntc ln ouc, ctvly. Th ubct and h on th wdg Gn functon nt th ca fo whch th ln ouc lctc and magntc, ctvly. Th ctal ntgal ntaton of th Gn u fo z-dctd lctc o magntc ln ouc xctaton gvn n functon ( ρ '), h ρ [] fo th al ouc ca (.. fo a al ouc locaton) a ( ρ ρ' ) = u( ρ, ρ'; β ) u( ρ, ρ'; β ), (.) u, h wh β = φ φ', (.3)

39 u ( ρ, ρ'; β ) 8π jn L L' dξ jk π ( ρ ρ' ρρ' coξ ) ξ β cot n jk ( ρ ρ ' ρρ ' coξ ) (.4) wh k al and lag. Th qua oot quantt n (.4) ult fom an aymtotc lag agumnt aoxmaton of Hankl functon of cond knd, od zo, and agumnt gvn by th qua oot quantty. Th ntgal ath L L' hown n Fgu. th wll known Sommfld contou. Thu, th ntgaton ov L L' atf Sommfld adaton condton and conttut a contou on whch th ntgal convg [3]. Th xonntal n (.4) aoxmatd a by t two tm bnomal xanon a ρρ ' ( ) ( ) ( ) ( co ) ' jk ξ jk ρ ρ ρρ 'coξ jk ρ ρ ' ρ ρ ' (.5) ρρ' wh ( coξ ) ( ) ρ ρ' aumd to b mall; th aoxmaton wll b jutfd lat. Thfo, ncooatng (.5) nto (.4) yld wh u κf ( ξ ) ( ρ, ρ'; β ) g( ξ, β ) L L' dξ, (.6) g ( ξ, β ) = 8π jn jk π ( ρ ρ' ρρ' coξ ) ξ β cot n jk ( ρ ρ ' ), (.7) ρρ' f ξ = j (.8) ( ) ( ) ( co ξ ) ρ ρ',

40 κ = k. (.9) Th addl ont of f ( ξ ) a found va f '( ) = 0 Th ( ξ,β ) ξ. It follow that fom (.8) ξ ξ = ξ = mπ, wh m = 0,,, 3,. (.0) ± g n (.7) alo ha banch ont ngulat at ξ = ξb whch a oot of ρ ρ' ρρ' coξ = 0, namly, ρ ρ' ξb = l π ± j coh, l = 0, ±, ±, ± 3, ± 4, (.) ρρ' and ξ b a not n th vcnty of th addl ont at ξ = ± mπ. In od to facltat th Cauchy thom [] n valuatng th ntgal n (.6), on ha to dtmn to fom a clod ath wth C = L L'. Th a obtand by th condton, Im f ( ξ ) = Im f ( ξ ) and ( ξ ) < 0 f a Im ξ. Thfo, th a dfnd wth ξ = u jv, a fo ( ξ ) < 0 ξ = ±π cou coh v =, (.) f a Im ξ. Thu only that a though th addl ont nd to b mloyd a hown n Fgu.. Th ( ξ, β ) ty ngulat at ± = 0, ±, ±, ± 3, ± 4, ± ξ = ξ = β nn π, g alo ha ml ol N (.3) 3

41 Im( ξ ) ξb ξb ξb ( π ) L ( π ) ( ) β ξ 3π π ξ = π π ξ = π π π 3π (ξ L' ξ b ξ b ξ b Fgu... Stt dcnt ath, ( π ) ouc llumnaton of a canoncal wdg. Th tajctoy of ± and th comlx ξ lan toology fo a al ln ξ ndcatd along th al ax. 4

42 wh ± N dtmn th ol whch clot to on of addl ont. Th uct '± ' on ξ and N n (.3) tan to th addl ont ξ = ± π ntg that mot naly atf th followng quaton. S. ± N dfnd a th N ± ± π β π n ( β ) =, (.4) Th nto wdg angl dfnd a ( n)π n Fgu.. Thfo, th addl ± ont at ξ = ± π, and only th ol at ξ = β nn π that l wthn th clod ath C ( π ) ( π ) ±, ctvly, contbut to th ntgal. It notd that fo uffcntly lag k, th majo contbuton to th ntgal valuatd ov ( ± π ) occu only fom th mmdat vcnty of th addl ont ( ξ = ± π ) ( co ). Thu, ξ bcom vy mall a ξ ξ = ± π, whch th uffcnt condton fo th aoxmaton of (.5). Thfo, th ntgal n (.6) dfomd nto va Cauchy Thom [] a follow wh u u ( ρ, ρ'; β ) u ( )( ξ, β ) u ( ξ, β ) H ( ξ ) π u ± κf ( ξ ) ( ± π )( ξ β ) = g( ξ, β ) ( ± π ) PW ( π )( ξ β ) upw ( ξ, β ) H ( ξ ),, (.5), dξ, (.6) ± ± ( ξ, β ) πj ( ξ, β ) u, (.7) PW = 5

43 ( ) ρ,φ ρ y φ ρ ' φ ' b = bbˆ φ b ( ρ ', φ ') x ( n)π Fgu.3. A comlx ln ouc bam ncdnt on th wdg. b th bam aamt and bˆ th dcton of bam ax. Comlx ay and ouc locaton a dawn only ymbolcally. 6

44 wh ( ξ, β ) ± du of ntgand n (.4) fo coondng ol and th addl ont. Th du contbuton n (.5) automatcally tctd by th ± Havd t functon ( ) H ξ to b aocatd wth only tho ol whch l wthn th clod ath of ntgaton fomd by C = L L' and ( ± π ). Th locaton of th ln ouc n al ac nxt analytcally contnud nto comlx ac va ' = ρ' j b ρ at ( ρ ', φ '). Th bam ax ontd along bˆ = coφ xˆ nφ yˆ wh th lan ndcula to th dg only condd. A b b tld ndcat a comlx quantty. Th comlx ay and comlx aamt, ( ρ ', φ ') tc. a llutatd only ymbolcally n Fgu.3. Th gnaton of a CSB and th comlx quantty of ( ', φ ') ρ a vwd n Andx F. Th total lctc and th magntc fld aocatd wth a CSB du to an lctc and a magntc ln ouc, ctvly, at Gn functon, ( ρ ') ρ ' can b wttn n tm of an aoxmat two dmnonal cala u a,, h ρ H z ( ) = ( ρ, ρ jωµ I u ρ ρ' ) z ( ) ( = ρ, ρ jωε M u ρ ρ' ) wh th al obvaton locaton at ρ = ( ρ, φ) of th Gn functon ( ρ '), h ρ h (.8). Th ctal ntgal ntaton u fo z-dctd comlx lctc o magntc ln ouc xctaton can b found fom th ult n (.5)(.7) by analytcally contnung th locaton of a ln ouc n al ac nto th comlx ac. Thu, 7

45 u, h ( ) ( ', '; ) (, ρ ρ = u ρ ρ β u ρ ρ'; β ), (.9) wh β = φ φ ', (.0) u u ( ρ, ρ'; β ) u ( )( ξ, β ) u ( ξ, β ) H ( ξ ) PW π u ± κf ( ξ ) ( ± π )( ξ β ) = g( ξ, β ) ( ± π ) PW ( π )( ξ β ) upw ( ξ, β ) H ( ξ ),, (.), dξ, (.) ± ± ( ξ, β ) πj ( ξ, β ) u, (.3) = g ( ξ, β ) = 8π jn jk π ( ρ ρ' ρρ ' coξ ) ξ β cot n jk ' ( ρ ρ ), (.4) ρρ ' f ξ = j ξ (.5) ( ) ( ) ( ρ ρ' co ), κ = k. (.6) It notd that fo th comlx ouc locaton, th addl ont man th am a th al ln ouc xctaton ca, ξ = ± π, and th a fo th comlx ouc ca alo unchangd a n (.). Th nd ont of th ath S L L' at nfnty a wthn th hadd gon to ovd convgnc of th ctal ntgal and to atfy th adaton condton; howv, L L' not allowd to co any ol o banch ont n th oc of analytc contnuaton fom a al to comlx ouc locaton. Th ol a now comlx n contat to al ol fo th al ouc ca; thy a tll gvn by th condton, 8

46 Im( ξ ) ξb ξb ξb ( π ) L ( π ) ξ ( β ) ξ ( β ) 3π π ξ = π π O ξ = π π π 3π ( ξ ) L' ξ b ξ b ξ b Fgu..4. Stt dcnt ath, ( π ) ξ ndcatd fo ( ξ ) 0. Im < ± and th comlx ξ lan toology. Th tajctoy of 9

47 wh ± ± ξ = ξ = β nn π, N = 0, ±, ±, ± 3, ± 4, (.7) ± N dtmn th ol whch clot to on of addl ont. Smlaly, th uct '± ' on ξ and N n (.7) tan to th addl ont ξ S = ± π. Fo a comlx ouc xctaton, quaton. ± N dfnd a th ntg that mot naly atf th followng N ± ± π ( ) ( β ) β =, π n (.8) Fgu.4 how th and th tajctoy of ol. ± Snc ( ξ, β ) th du of ntgand n (.4) fo coondng ol and th addl ont. Th du contbuton n (.) automatcally tctd by th ± Havd t functon ( ) H ξ to b aocatd wth only tho ol whch l wthn th clod ath of ntgaton fomd by C = L L' and ( ± π ). Th du contbuton nt th ncdnt and flctd CSB contbuton ang fom th comlx ln ouc llumnaton of th wdg. Th du ± ( ξ β ) found to b j j jk ρ ρ ' ρρ 'co ξ, = ± ( ), (.9) πj 4 πk ρ ρ' ρρ ' coξ Thfo, ncooatng (.9) nto (.) yld u, h { π PW ( ρ ρ' ) u ( )( ξ, β ) u ( ξ, β ) H ( ξ ) u ( π )( ξ, β ) upw ( ξ, β ) H ( ξ ) } 30

48 { u u ( π )( ξ, β ) upw ( ξ, β ) H ( ξ ) ( π )( ξ β ) upw ( ξ, β ) H ( ξ )},. (.30) Th ft and th cond du tm ( u PW n (.30)) contbut to th dct CSB lctc/magntc fld fo th n-fac and o-fac llumnaton, ctvly, wha th thd and th foth du tm contbut to th flctd CSB lctc/magntc fld fo th n-fac and o-fac llumnaton, ctvly. Th total bam fld a comod of a uoton of th ncdnt CSB, th flctd CSB and th bam dffactd fld, ctvly a n (.30), n atcula, th addl ont contbuton n (.30) coond to th bam dffactd fld. Thfo, ach u n (.30) fom ξ S = ± π nd to b valuatd and uod to fnd th bam dffactd by th wdg and ubquntly, th total fld n (.8). Nxt, th UTD coffcnt of bam dffactd by a PC wdg xctd by a z- dctd comlx ln ouc a found va two mthod of tt dcnt, namly, PCM whch lad to a CSB-UTD oluton and PCM (=aangd VWM) whch lad to a CSB-UTD oluton. Fom Andx A, on can valuat th Gn functon aymtotcally n clod fom fo th bam dffactd fld n (.) a u u UTD, h UTD, h UTD ( ρ ρ ' ) d jkρ h, u UTD ( ρ ρ ' ) ρ d, h (.3) wh jkρ ' j j u =, (.3) 4 πk ρ' 3

49 d { d ( β, ξ ( β ) d ( β, ξ ( )} UTD, h UTD UTD = β { d ( β, ξ ( β ) ( β, ξ ( β )} UTD d, (.33) { d ( β, ξ ( β ) d ( β, ξ ( )} UTD, h UTD UTD d = β, π UTD { d ( β, ξ ( β ) ( β, ξ ( β )} UTD d (.34) [ ] j 4 ± ± π ± β [ β, ξ ( β )] cot ± d UTD = ± ( β ) π F ka, (.35) n k n d ± UTD π UTD [ ] j 4 ± π ± β [ β, ξ ( β )] cot ± = F ± ka ( β ) n πk n ± ρ ρ ' δ n ± ( ξ ( β ) co( ξ ( β ) ) π β cot n [ ± ± ka ( )] ( F ), β ± (.36) ( ), ( ) ' ± ± ρρ ξ co β a β = (.37) ρ ρ' ± ± ( ξ ( β ) ρ ρ' ρρ ± 'coξ ( β ) δ =. (.38) ( ) wh ( ± F ± ka β ) th convntonal UTD tanton functon fo dg whch not gnalzd to comlx ac a dcbd n Andx A. It notd that u nt th ncdnt CSB at th dg fo lag ρ ' j = 0 ρ. Th 4 () k wh u H ( k ') UTD d, h and UTD h d, a th CSB wdg dffacton coffcnt found va CSB-UTD and CSB-UTD, ctvly, n th ca of a comlx ln ouc xctaton. A dcud n Andx A, 3

50 ach tm of th dffacton coffcnt va CSB-UTD n (.34) contan an xta tm n addton to th coondng tm of th dffacton coffcnt obtand fom CSB-UTD n (.33). It hown analytcally n Andx A that th addtonal tm ngnfcant bcau th ft backt of cond tm n (.36) bcom nglgbl whn th obvaton at and na th SB and bcau th cond backt bcom nglgbl whn th obvaton away fom th SB, whch alo vfd numcally n th nxt cton. Thfo, th oluton va CSB-UTD and CSB-UTD a naly dntcal; th fact wll alo b vfd wth cfc numcal xaml n th nxt cton... Numcal ult fo a comlx ln ouc xctaton Bad on th oluton found n th vou cton, th CSB dffactd by a PC wdg xctd by a comlx ln ouc locatd at ρ ' = ( ρ', φ ' ) comutd. Th total CSB fld at th nc of a wdg obtand by th uoton of ncdnt, flctd and dffactd fld. Th flctd CSB fld aa to b manat fom th mag of th actual comlx ouc locatd at ' ( ', φ ρ = ρ ' ). Th ncdnt ( ) flctd ( ) z z and th CSB fld a du to th ognal z-dctd comlx lctc ln ouc and t mag, ctvly. Th fld dnotd a CSB-GO fld a gvn by th coondng ol contbuton and can b wttn a, z jk ρ ρ ' = 0 j 4 j πk ρ ρ ', ( ρ ) ± C,, (.39) 33

51 wh th ngatv gn fo z du to th olazaton chang val ang fom flcton off th lana PC wdg fac bng llumnatd. Alo, C0 = jωµ I n (.39) a comlx contant nt n (.8). A dcud n Andx A, th SB fo, z can b dtmnd a th locaton of obvaton coondng to whn th ncdnt/flctd CSB ol co th aoat. In oth wod, th SB a found to b th φ coodnat of th obvaton ont whn Im α = 0 n th comlx α lan of Andx A. Th α to fnd ncdnt (ISB) and flcton (SB) hadow bounda a gvn, ctvly, a α, ( β ) = ρρ ' ξ co ρ ρ' ( β ) j 4 π, (.40) wh th banch cfd a dcud n Andx A. It notd that th comutatonal ffot to calculat ISB and SB nglgbl. Th lt and hadow gon fo th ncdnt and flctd CSB hould b dtmnd o to th comutaton of th total fld. A cta of choong th lt and hadow gon dcud at th nd of th chat. Fgu.5 llutat th tajctoy of ISB and SB fo a comlx ln ouc at a fxd comlx locaton llumnatng a PC half lan, a th adal dtanc of obv chang. A llutatd n Fgu.5, th ISB and SB a not a taght ln a n th ca of a ln ouc n al ac xctaton. Th llutaton n Fgu.5 th only ca wh th dtanc to th ouc and th obvaton fom th dg nth fa no clo. 34

Multi-linear Systems and Invariant Theory. in the Context of Computer Vision and Graphics. Class 4: Mutli-View 3D-from-2D. CS329 Stanford University

Multi-linear Systems and Invariant Theory. in the Context of Computer Vision and Graphics. Class 4: Mutli-View 3D-from-2D. CS329 Stanford University Mult-lna Sytm and Invaant hoy n th Contxt of Comut Von and Gahc Cla 4: Mutl-Vw 3D-fom-D CS39 Stanfod Unvty Amnon Shahua Cla 4 Matal W Wll Cov oday Eola Gomty and Fundamntal Matx h lan+aallax modl and latv

More information

EE 584 MACHINE VISION

EE 584 MACHINE VISION MTU 584 Lctu Not by A.AydnALATAN 584 MACHIN VISION Photomtc Sto Radomty BRDF Rflctanc Ma Rcovng Sufac Ontaton MTU 584 Lctu Not by A.AydnALATAN Photomtc Sto It obl to cov th ontaton of ufac atch fom a numb

More information

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28 Chapt 10 Phys 3 Lctu 8 Dffacton Dffacton: gnal Fsnl vs. Faunhof dffacton Sval cohnt oscllatos Sngl-slt dffacton Dffacton Gmald, 1600s: dffacto, dvaton of lght fom lna popagaton Dffacton s a consqunc of

More information

Period vs. Length of a Pendulum

Period vs. Length of a Pendulum Gaphcal Mtho n Phc Gaph Intptaton an Lnazaton Pat 1: Gaphng Tchnqu In Phc w u a vat of tool nclung wo, quaton, an gaph to mak mol of th moton of objct an th ntacton btwn objct n a tm. Gaph a on of th bt

More information

Massachusetts Institute of Technology Introduction to Plasma Physics

Massachusetts Institute of Technology Introduction to Plasma Physics Massachustts Insttut of Tchnology Intoducton to Plasma Physcs NAME 6.65J,8.63J,.6J R. Pak Dcmb 5 Fnal Eam :3-4:3 PM NOTES: Th a 8 pags to th am, plus on fomula sht. Mak su that you copy s complt. Each

More information

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28

Diffraction. Diffraction: general Fresnel vs. Fraunhofer diffraction Several coherent oscillators Single-slit diffraction. Phys 322 Lecture 28 Chapt 10 Phys 3 Lctu 8 Dffacton Dffacton: gnal Fsnl vs. Faunhof dffacton Sval cohnt oscllatos Sngl-slt dffacton Dffacton Gmald, 1600s: dffacto, dvaton of lght fom lna popagaton Dffacton s a consqunc of

More information

CIVL 7/ D Boundary Value Problems - Axisymmetric Elements 1/8

CIVL 7/ D Boundary Value Problems - Axisymmetric Elements 1/8 CIVL 7/8 -D Bounday Valu Poblms - xsymmtc Elmnts /8 xsymmtc poblms a somtms fd to as adally symmtc poblms. hy a gomtcally th-dmnsonal but mathmatcally only two-dmnsonal n th physcs of th poblm. In oth

More information

5- Scattering Stationary States

5- Scattering Stationary States Lctu 19 Pyscs Dpatmnt Yamou Unvsty 1163 Ibd Jodan Pys. 441: Nucla Pyscs 1 Pobablty Cunts D. Ndal Esadat ttp://ctaps.yu.du.jo/pyscs/couss/pys641/lc5-3 5- Scattng Statonay Stats Rfnc: Paagaps B and C Quantum

More information

( V ) 0 in the above equation, but retained to keep the complete vector identity for V in equation.

( V ) 0 in the above equation, but retained to keep the complete vector identity for V in equation. Cuvlna Coodnats Outln:. Otogonal cuvlna coodnat systms. Dffntal opatos n otogonal cuvlna coodnat systms. Dvatvs of t unt vctos n otogonal cuvlna coodnat systms 4. Incompssbl N-S quatons n otogonal cuvlna

More information

Chapter 10 DIELECTRICS. Dielectrics

Chapter 10 DIELECTRICS. Dielectrics 86 Dlctcs Chat DILCTRICS Dlctcs : Dlctcs a fct nsulatos. In dlctcs lctons a vy tghtly bound to th atoms so that at odnay tmatus thy do not conduct any lctc cunt. xamls: Solds: glass, ocln; gass: H, N ;

More information

Lecture 7 Diffusion. Our fluid equations that we developed before are: v t v mn t

Lecture 7 Diffusion. Our fluid equations that we developed before are: v t v mn t Cla ot fo EE6318/Phy 6383 Spg 001 Th doumt fo tutoal u oly ad may ot b opd o dtbutd outd of EE6318/Phy 6383 tu 7 Dffuo Ou flud quato that w dvlopd bfo a: f ( )+ v v m + v v M m v f P+ q E+ v B 13 1 4 34

More information

Load Equations. So let s look at a single machine connected to an infinite bus, as illustrated in Fig. 1 below.

Load Equations. So let s look at a single machine connected to an infinite bus, as illustrated in Fig. 1 below. oa Euatons Thoughout all of chapt 4, ou focus s on th machn tslf, thfo w wll only pfom a y smpl tatmnt of th ntwok n o to s a complt mol. W o that h, but alz that w wll tun to ths ssu n Chapt 9. So lt

More information

Moving Target Hough Detector in Pulse Jamming*

Moving Target Hough Detector in Pulse Jamming* BULGARIA ACADEMY OF SCIECES CYBEREICS AD IFORMAIO ECHOLOGIES Volum 7 o Sofa 7 Movng agt Hough Dtcto n ul Jammng* Lyuba Douova Inttut of Infomaton chnolog 3 Sofa Abtact: h Hough dtcto wth two typ of a Contant

More information

Chapter 3 Basic Crystallography and Electron Diffraction from Crystals. Lecture 12. CHEM 793, 2008 Fall

Chapter 3 Basic Crystallography and Electron Diffraction from Crystals. Lecture 12. CHEM 793, 2008 Fall Chapt 3 Bac Cytalloaphy and Elcton Dacton om Cytal Lctu 1 CHEM 793, 008 all Announcmnt Mdtm Exam: Oct., Wdnday, :30 4:30 CHEM 793, 008 all Th xctaton o, Ba' Law and th Lau quaton pdct dacton at only pc

More information

COMPSCI 230 Discrete Math Trees March 21, / 22

COMPSCI 230 Discrete Math Trees March 21, / 22 COMPSCI 230 Dict Math Mach 21, 2017 COMPSCI 230 Dict Math Mach 21, 2017 1 / 22 Ovviw 1 A Simpl Splling Chck Nomnclatu 2 aval Od Dpth-it aval Od Badth-it aval Od COMPSCI 230 Dict Math Mach 21, 2017 2 /

More information

A closed form analytical solution to the radiation problem from a short dipole antenna above flat ground using spectral domain approach

A closed form analytical solution to the radiation problem from a short dipole antenna above flat ground using spectral domain approach A closd fom analytcal soluton to th adaton poblm fom a shot dpol antnna abov flat gound usng spctal doman appoach S. Sautbov*, *uasan Natonal Unvsty,5, Munatpasov St., Astana, Kazashtan sautb@mal.u P.

More information

Control Systems. Lecture 8 Root Locus. Root Locus. Plant. Controller. Sensor

Control Systems. Lecture 8 Root Locus. Root Locus. Plant. Controller. Sensor Cotol Syt ctu 8 Root ocu Clacal Cotol Pof. Eugo Schut hgh Uvty Root ocu Cotoll Plat R E C U Y - H C D So Y C C R C H Wtg th loo ga a w a ttd tackg th clod-loo ol a ga va Clacal Cotol Pof. Eugo Schut hgh

More information

Homework: Due

Homework: Due hw-.nb: //::9:5: omwok: Du -- Ths st (#7) s du on Wdnsday, //. Th soluton fom Poblm fom th xam s found n th mdtm solutons. ü Sakua Chap : 7,,,, 5. Mbach.. BJ 6. ü Mbach. Th bass stats of angula momntum

More information

Analysis of a M/G/1/K Queue with Vacations Systems with Exhaustive Service, Multiple or Single Vacations

Analysis of a M/G/1/K Queue with Vacations Systems with Exhaustive Service, Multiple or Single Vacations Analyss of a M/G// uu wth aatons Systms wth Ehaustv Sv, Multpl o Sngl aatons W onsd h th fnt apaty M/G// uu wth th vaaton that th sv gos fo vaatons whn t s dl. Ths sv modl s fd to as on povdng haustv sv,

More information

Melitz-type Computable General Equilibrium Model

Melitz-type Computable General Equilibrium Model Mlt-ty Coutabl Gnal Equlbu Modl Auut 23 26 Nobuo Hoo Natonal Gaduat Inttut o Polcy Stud noo@.ac.. Modl Outln A Mlt-ty coutabl nal qulbu (CGE) odl dvlod on t ba o t tandad CGE odl by Hoo t al. (2) wt t

More information

8-node quadrilateral element. Numerical integration

8-node quadrilateral element. Numerical integration Fnt Elmnt Mthod lctur nots _nod quadrlatral lmnt Pag of 0 -nod quadrlatral lmnt. Numrcal ntgraton h tchnqu usd for th formulaton of th lnar trangl can b formall tndd to construct quadrlatral lmnts as wll

More information

E F. and H v. or A r and F r are dual of each other.

E F. and H v. or A r and F r are dual of each other. A Duality Thom: Consid th following quations as an xampl = A = F μ ε H A E A = jωa j ωμε A + β A = μ J μ A x y, z = J, y, z 4π E F ( A = jω F j ( F j β H F ωμε F + β F = ε M jβ ε F x, y, z = M, y, z 4π

More information

( ) + is the distance from the point of interest to the location of the charge q i

( ) + is the distance from the point of interest to the location of the charge q i Elctcal Engy and apactanc 57. Bcaus lctc ocs a consvatv, th kntc ngy gand s qual to th dcas n lctcal potntal ngy, o + + 4 4 KE PE q( ).. so th coct choc s (a).. Fom consvaton o ngy, KE + PE KE + PE, o

More information

Physics 111. Lecture 38 (Walker: ) Phase Change Latent Heat. May 6, The Three Basic Phases of Matter. Solid Liquid Gas

Physics 111. Lecture 38 (Walker: ) Phase Change Latent Heat. May 6, The Three Basic Phases of Matter. Solid Liquid Gas Physics 111 Lctu 38 (Walk: 17.4-5) Phas Chang May 6, 2009 Lctu 38 1/26 Th Th Basic Phass of Matt Solid Liquid Gas Squnc of incasing molcul motion (and ngy) Lctu 38 2/26 If a liquid is put into a sald contain

More information

The angle between L and the z-axis is found from

The angle between L and the z-axis is found from Poblm 6 This is not a ifficult poblm but it is a al pain to tansf it fom pap into Mathca I won't giv it to you on th quiz, but know how to o it fo th xam Poblm 6 S Figu 6 Th magnitu of L is L an th z-componnt

More information

Applications of Lagrange Equations

Applications of Lagrange Equations Applcaton of agang Euaton Ca Stuy : Elctc Ccut ng th agang uaton of oton, vlop th athatcal ol fo th ccut hown n Fgu.Sulat th ult by SIMI. Th ccuty paat a: 0.0 H, 0.00 H, 0.00 H, C 0.0 F, C 0. F, 0 Ω, Ω

More information

Folding of Regular CW-Complexes

Folding of Regular CW-Complexes Ald Mathmatcal Scncs, Vol. 6,, no. 83, 437-446 Foldng of Rgular CW-Comlxs E. M. El-Kholy and S N. Daoud,3. Dartmnt of Mathmatcs, Faculty of Scnc Tanta Unvrsty,Tanta,Egyt. Dartmnt of Mathmatcs, Faculty

More information

The Random Phase Approximation:

The Random Phase Approximation: Th Random Phas Appoxmaton: Elctolyts, Polym Solutons and Polylctolyts I. Why chagd systms a so mpotant: thy a wat solubl. A. bology B. nvonmntally-fndly polym pocssng II. Elctolyt solutons standad dvaton

More information

Grand Canonical Ensemble

Grand Canonical Ensemble Th nsmbl of systms mmrsd n a partcl-hat rsrvor at constant tmpratur T, prssur P, and chmcal potntal. Consdr an nsmbl of M dntcal systms (M =,, 3,...M).. Thy ar mutually sharng th total numbr of partcls

More information

Electromagnetics: The Smith Chart (9-6)

Electromagnetics: The Smith Chart (9-6) Elctomagntcs: Th Smth Chat (9-6 Yoonchan Jong School of Elctcal Engnng, Soul Natonal Unvsty Tl: 8 (0 880 63, Fax: 8 (0 873 9953 Emal: yoonchan@snu.ac.k A Confomal Mappng ( Mappng btwn complx-valud vaabls:

More information

NEW ATTACKS ON TAKAGI CRYPTOSYSTEM

NEW ATTACKS ON TAKAGI CRYPTOSYSTEM Jounal of Algba umb Thoy: Advancs and Alcatons Volum 8 umb - 7 Pags 5-59 Avalabl at htt://scntfcadvancscon DOI: htt://dxdoog/86/antaa_785 EW ATTACKS O TAKAGI CRYPTOSYSTEM MUHAMMAD REAL KAMEL ARIFFI SADIQ

More information

ORBITAL TO GEOCENTRIC EQUATORIAL COORDINATE SYSTEM TRANSFORMATION. x y z. x y z GEOCENTRIC EQUTORIAL TO ROTATING COORDINATE SYSTEM TRANSFORMATION

ORBITAL TO GEOCENTRIC EQUATORIAL COORDINATE SYSTEM TRANSFORMATION. x y z. x y z GEOCENTRIC EQUTORIAL TO ROTATING COORDINATE SYSTEM TRANSFORMATION ORITL TO GEOCENTRIC EQUTORIL COORDINTE SYSTEM TRNSFORMTION z i i i = (coωcoω in Ωcoiinω) (in Ωcoω + coωcoiinω) iniinω ( coωinω in Ωcoi coω) ( in Ωinω + coωcoicoω) in icoω in Ωini coωini coi z o o o GEOCENTRIC

More information

Exercises for lectures 7 Steady state, tracking and disturbance rejection

Exercises for lectures 7 Steady state, tracking and disturbance rejection Exrc for lctur 7 Stady tat, tracng and dturbanc rjcton Martn Hromčí Automatc control 06-3-7 Frquncy rpon drvaton Automatcé řízní - Kybrnta a robota W lad a nuodal nput gnal to th nput of th ytm, gvn by

More information

Collisionless Hall-MHD Modeling Near a Magnetic Null. D. J. Strozzi J. J. Ramos MIT Plasma Science and Fusion Center

Collisionless Hall-MHD Modeling Near a Magnetic Null. D. J. Strozzi J. J. Ramos MIT Plasma Science and Fusion Center Collisionlss Hall-MHD Modling Na a Magntic Null D. J. Stoi J. J. Ramos MIT Plasma Scinc and Fusion Cnt Collisionlss Magntic Rconnction Magntic connction fs to changs in th stuctu of magntic filds, bought

More information

for the magnetic induction at the point P with coordinate x produced by an increment of current

for the magnetic induction at the point P with coordinate x produced by an increment of current 5. tatng wth th ffnta psson B fo th magntc nucton at th pont P wth coonat pouc by an ncmnt of cunt at, show pcty that fo a oop cayng a cunt th magntc nucton at P s B Ω wh Ω s th so ang subtn by th oop

More information

Equil. Properties of Reacting Gas Mixtures. So far have looked at Statistical Mechanics results for a single (pure) perfect gas

Equil. Properties of Reacting Gas Mixtures. So far have looked at Statistical Mechanics results for a single (pure) perfect gas Shool of roa Engnrng Equl. Prort of Ratng Ga Mxtur So far hav lookd at Stattal Mhan rult for a ngl (ur) rft ga hown how to gt ga rort (,, h, v,,, ) from artton funton () For nonratng rft ga mxtur, gt mxtur

More information

sub-cells. b,c, Mapping of (ρ, B -1 ) with the control of (to, ti) using b, the full solutions in (14) and c,

sub-cells. b,c, Mapping of (ρ, B -1 ) with the control of (to, ti) using b, the full solutions in (14) and c, ulnty Fgu chtc of th t-to nd dcould contol of w t Agnnt of g u nd dlcnt jk fo th bn nd ub-cll bc ng of - wth th contol of t t ung b th full oluton n nd c th oton 5 ght t Hz ulnty Fgu nd tuctu of th t-to

More information

Chapter 3 Binary Image Analysis. Comunicação Visual Interactiva

Chapter 3 Binary Image Analysis. Comunicação Visual Interactiva Chapt 3 Bnay Iag Analyss Counação Vsual Intatva Most oon nghbohoods Pxls and Nghbohoods Nghbohood Vznhança N 4 Nghbohood N 8 Us of ass Exapl: ogn nput output CVI - Bnay Iag Analyss Exapl 0 0 0 0 0 output

More information

Linear Algebra. Definition The inverse of an n by n matrix A is an n by n matrix B where, Properties of Matrix Inverse. Minors and cofactors

Linear Algebra. Definition The inverse of an n by n matrix A is an n by n matrix B where, Properties of Matrix Inverse. Minors and cofactors Dfnton Th nvr of an n by n atrx A an n by n atrx B whr, Not: nar Algbra Matrx Invron atrc on t hav an nvr. If a atrx ha an nvr, thn t call. Proprt of Matrx Invr. If A an nvrtbl atrx thn t nvr unqu.. (A

More information

Solving the Dirac Equation: Using Fourier Transform

Solving the Dirac Equation: Using Fourier Transform McNa Schola Reeach Jounal Volume Atcle Solvng the ac quaton: Ung oue Tanfom Vncent P. Bell mby-rddle Aeonautcal Unvety, Vncent.Bell@my.eau.edu ollow th and addtonal wok at: http://common.eau.edu/na Recommended

More information

New bounds on Poisson approximation to the distribution of a sum of negative binomial random variables

New bounds on Poisson approximation to the distribution of a sum of negative binomial random variables Sogklaaka J. Sc. Tchol. 4 () 4-48 Ma. -. 8 Ogal tcl Nw bouds o Posso aomato to th dstbuto of a sum of gatv bomal adom vaabls * Kat Taabola Datmt of Mathmatcs Faculty of Scc Buaha Uvsty Muag Chobu 3 Thalad

More information

ME 200 Thermodynamics I Spring 2014 Examination 3 Thu 4/10/14 6:30 7:30 PM WTHR 200, CL50 224, PHY 112 LAST NAME FIRST NAME

ME 200 Thermodynamics I Spring 2014 Examination 3 Thu 4/10/14 6:30 7:30 PM WTHR 200, CL50 224, PHY 112 LAST NAME FIRST NAME M 00 hrodynac Sprng 014 xanaton 3 hu 4/10/14 6:30 7:30 PM WHR 00, CL50 4, PHY 11 Crcl your dvon: PHY 11 WHR 00 WHR 00 CL50 4 CL50 4 PHY 11 7:30 Joglkar 9:30 Wagrn 10:30 Gor 1:30 Chn :30 Woodland 4:30 Srcar

More information

Solutions to Supplementary Problems

Solutions to Supplementary Problems Solution to Supplmntay Poblm Chapt Solution. Fomula (.4): g d G + g : E ping th void atio: G d 2.7 9.8 0.56 (56%) 7 mg Fomula (.6): S Fomula (.40): g d E ping at contnt: S m G 0.56 0.5 0. (%) 2.7 + m E

More information

A study on Ricci soliton in S -manifolds.

A study on Ricci soliton in S -manifolds. IO Joual of Mathmatc IO-JM -IN: 78-578 p-in: 9-765 olum Iu I Ja - Fb 07 PP - wwwojoualo K dyavath ad Bawad Dpatmt of Mathmatc Kuvmpu vtyhaaahatta - 577 5 hmoa Kaataa Ida Abtact: I th pap w tudy m ymmtc

More information

TRANSIENT PROCESSES AND DYNAMIC OF VARIABLE SPEED PUMP STORAGE UNIT

TRANSIENT PROCESSES AND DYNAMIC OF VARIABLE SPEED PUMP STORAGE UNIT Ol Shal, 203, Vol. 30, No. 2S, pp. 244 256 ISSN 020889X do: 0.376/ol.203.2S.05 203 Etonan Acadmy ublh TRANSIENT ROCESSES AND DYNAMIC OF VARIABLE SEED UM STORAGE UNIT RIMANTAS RANAS DEKSNYS *, DARIUS ALIŠAUSKAS

More information

MECH321 Dynamics of Engineering System Week 4 (Chapter 6)

MECH321 Dynamics of Engineering System Week 4 (Chapter 6) MH3 Dynamc of ngnrng Sytm Wk 4 (haptr 6). Bac lctrc crcut thor. Mathmatcal Modlng of Pav rcut 3. ompl mpdanc Approach 4. Mchancal lctrcal analogy 5. Modllng of Actv rcut: Opratonal Amplfr rcut Bac lctrc

More information

Neural Networks The ADALINE

Neural Networks The ADALINE Lat Lctu Summay Intouction to ua to Bioogica uon Atificia uon McCuoch an itt LU Ronbatt cton Aan Bnaino, a@i.it.ut.t Machin Laning, 9/ ua to h ADALI M A C H I L A R I G 9 / cton Limitation cton aning u

More information

PERTURBATION THEORY FOR ELECTROMAGNETIC WAVE SCATTERING

PERTURBATION THEORY FOR ELECTROMAGNETIC WAVE SCATTERING TSI DI DOTTORATO UIVRSITÀ DGLI STUDI DI APOLI FDRICO II DIPARTIMTO DI IGGRIA LTTROICA DLL TLCOMUICAZIOI DOTTORATO DI RICRCA I IGGRIA LTTROICA DLL TLCOMUICAZIOI PRTURBATIO THORY FOR LCTROMAGTIC WAV SCATTRIG

More information

Structure and Features

Structure and Features Thust l Roll ans Thust Roll ans Stutu an atus Thust ans onsst of a psly ma a an olls. Thy hav hh ty an hh loa apats an an b us n small spas. Thust l Roll ans nopoat nl olls, whl Thust Roll ans nopoat ylnal

More information

ECE Spring Prof. David R. Jackson ECE Dept. Notes 6

ECE Spring Prof. David R. Jackson ECE Dept. Notes 6 ECE 6345 Spring 2015 Prof. David R. Jackon ECE Dpt. Not 6 1 Ovrviw In thi t of not w look at two diffrnt modl for calculating th radiation pattrn of a microtrip antnna: Elctric currnt modl Magntic currnt

More information

CHAPTER 5 CIRCULAR MOTION

CHAPTER 5 CIRCULAR MOTION CHAPTER 5 CIRCULAR MOTION and GRAVITATION 5.1 CENTRIPETAL FORCE It is known that if a paticl mos with constant spd in a cicula path of adius, it acquis a cntiptal acclation du to th chang in th diction

More information

ESCI 341 Atmospheric Thermodynamics Lesson 16 Pseudoadiabatic Processes Dr. DeCaria

ESCI 341 Atmospheric Thermodynamics Lesson 16 Pseudoadiabatic Processes Dr. DeCaria ESCI 34 Atmohi hmoynami on 6 Puoaiabati Po D DCaia fn: Man, A an FE obitaill, 97: A omaion of th uialnt otntial tmatu an th tati ngy, J Atmo Si, 7, 37-39 Btt, AK, 974: Futh ommnt on A omaion of th uialnt

More information

[ ] 1+ lim G( s) 1+ s + s G s s G s Kacc SYSTEM PERFORMANCE. Since. Lecture 10: Steady-state Errors. Steady-state Errors. Then

[ ] 1+ lim G( s) 1+ s + s G s s G s Kacc SYSTEM PERFORMANCE. Since. Lecture 10: Steady-state Errors. Steady-state Errors. Then SYSTEM PERFORMANCE Lctur 0: Stady-tat Error Stady-tat Error Lctur 0: Stady-tat Error Dr.alyana Vluvolu Stady-tat rror can b found by applying th final valu thorm and i givn by lim ( t) lim E ( ) t 0 providd

More information

Systemic design and modelling of a coiled rotor synchronous motor dedicated to electric traction

Systemic design and modelling of a coiled rotor synchronous motor dedicated to electric traction mcan Jounal of Elctcal Pow an Engy Sytm 5; 4(-): -7 Publh onln Novmb 5, 4 (htt://www.cncublhnggou.com/j/) o:.648/j...54. ISSN: 36-9X (Pnt); ISSN: 36-9 (Onln) Sytmc gn an mollng of a col oto ynchonou moto

More information

PLANAR KNOTTING MECHANISMS FOR TURKISH HAND WOVEN CARPET

PLANAR KNOTTING MECHANISMS FOR TURKISH HAND WOVEN CARPET PLANAR KNOTTIN ECHANISS OR TURKISH HAND WOVEN CARPET E THEORY O ACHINES INSTRUCTOR:POR.DR.TECH.SCI.RASI ALIZADE ASISTANT:RES.ASST.OZUN SELVI :ROUUP EBER NAES: AHET APAK 7 SERKAN CİLARA DENİZ ÖZÜN 6 LEVENT

More information

(1) Then we could wave our hands over this and it would become:

(1) Then we could wave our hands over this and it would become: MAT* K285 Spring 28 Anthony Bnoit 4/17/28 Wk 12: Laplac Tranform Rading: Kohlr & Johnon, Chaptr 5 to p. 35 HW: 5.1: 3, 7, 1*, 19 5.2: 1, 5*, 13*, 19, 45* 5.3: 1, 11*, 19 * Pla writ-up th problm natly and

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

STRIPLINES. A stripline is a planar type transmission line which is well suited for microwave integrated circuitry and photolithographic fabrication.

STRIPLINES. A stripline is a planar type transmission line which is well suited for microwave integrated circuitry and photolithographic fabrication. STIPLINES A tiplin i a plana typ tanmiion lin hih i ll uitd fo mioav intgatd iuity and photolithogaphi faiation. It i uually ontutd y thing th nt onduto of idth, on a utat of thikn and thn oving ith anoth

More information

The Fourier Transform

The Fourier Transform /9/ Th ourr Transform Jan Baptst Josph ourr 768-83 Effcnt Data Rprsntaton Data can b rprsntd n many ways. Advantag usng an approprat rprsntaton. Eampls: osy ponts along a ln Color spac rd/grn/blu v.s.

More information

Variable Structure Control ~ Basics

Variable Structure Control ~ Basics Varable Structure Control ~ Bac Harry G. Kwatny Department of Mechancal Engneerng & Mechanc Drexel Unverty Outlne A prelmnary example VS ytem, ldng mode, reachng Bac of dcontnuou ytem Example: underea

More information

How to Use. The Bears Beat the Sharks!

How to Use. The Bears Beat the Sharks! Hw t U Th uc vd 24 -wd dng ctn bd n wht kd ncunt vy dy, uch mv tng, y, n Intnt ch cn. Ech ctn ccmnd by tw w-u ctc g ng tudnt cmhnn th ctn. Th dng ctn cn b ud wth ndvdu, m gu, th wh c. Th B cnd bmn, Dn

More information

Cluster Optimization for Takagi & Sugeno Fuzzy Models and Its Application to a Combined Cycle Power Plant Boiler

Cluster Optimization for Takagi & Sugeno Fuzzy Models and Its Application to a Combined Cycle Power Plant Boiler Clut Optmzaton o Takag & Sugno Fuzzy Modl It Applcaton to a Combnd Cycl Pow Plant Bol Do Sáz, Mmb IEEE, Robto Zuñga, Studnt Mmb IEEE Abtact- In th pap, a nw mthod o clut numb optmzaton o Takag & Sugno

More information

Homework 1: Solutions

Homework 1: Solutions Howo : Solutos No-a Fals supposto tst but passs scal tst lthouh -f th ta as slowss [S /V] vs t th appaac of laty alty th path alo whch slowss s to b tat to obta tavl ts ps o th ol paat S o V as a cosquc

More information

AI BASED VECTOR CONTROL OF INDUCTION MOTOR

AI BASED VECTOR CONTROL OF INDUCTION MOTOR AI BASED VECTOR CONTROL OF INDUCTION MOTOR K.Padukola Elctcal and lctonc ngnng S Vdya collg of Engnng and Tchnology, Inda padukola@gmal.com Abtact- In modn hgh pfomanc ac dv uually th dct vcto contol chm

More information

GMm. 10a-0. Satellite Motion. GMm U (r) - U (r ) how high does it go? Escape velocity. Kepler s 2nd Law ::= Areas Angular Mom. Conservation!!!!

GMm. 10a-0. Satellite Motion. GMm U (r) - U (r ) how high does it go? Escape velocity. Kepler s 2nd Law ::= Areas Angular Mom. Conservation!!!! F Satllt Moton 10a-0 U () - U ( ) 0 f ow g dos t go? scap locty Kpl s nd Law ::= Aas Angula Mo. Consaton!!!! Nwton s Unsal Law of Gaty 10a-1 M F F 1) F acts along t ln connctng t cnts of objcts Cntal Foc

More information

Chapter 23: Magnetic Field Shielding

Chapter 23: Magnetic Field Shielding ELECTROMAGNETIC COMPATIBILITY ANDBOOK 1 Chapt : Magntc Fld Shldng.1 Usng th Bt-Savat law, vfy th magntc fld xpssn X (pvdd by yu nstuct) gvn n th cunt dstbutns and th magntc flds tabl n ths chapt.. Usng

More information

Heisenberg Model. Sayed Mohammad Mahdi Sadrnezhaad. Supervisor: Prof. Abdollah Langari

Heisenberg Model. Sayed Mohammad Mahdi Sadrnezhaad. Supervisor: Prof. Abdollah Langari snbrg Modl Sad Mohammad Mahd Sadrnhaad Survsor: Prof. bdollah Langar bstract: n ths rsarch w tr to calculat analtcall gnvalus and gnvctors of fnt chan wth ½-sn artcls snbrg modl. W drov gnfuctons for closd

More information

Fourier transforms (Chapter 15) Fourier integrals are generalizations of Fourier series. The series representation

Fourier transforms (Chapter 15) Fourier integrals are generalizations of Fourier series. The series representation Pof. D. I. Nass Phys57 (T-3) Sptmb 8, 03 Foui_Tansf_phys57_T3 Foui tansfoms (Chapt 5) Foui intgals a gnalizations of Foui sis. Th sis psntation a0 nπx nπx f ( x) = + [ an cos + bn sin ] n = of a function

More information

School of Electrical Engineering. Lecture 2: Wire Antennas

School of Electrical Engineering. Lecture 2: Wire Antennas School of lctical ngining Lctu : Wi Antnnas Wi antnna It is an antnna which mak us of mtallic wis to poduc a adiation. KT School of lctical ngining www..kth.s Dipol λ/ Th most common adiato: λ Dipol 3λ/

More information

Improvements on Waring s Problem

Improvements on Waring s Problem Imrovement on Warng Problem L An-Png Bejng 85, PR Chna al@nacom Abtract By a new recurve algorthm for the auxlary equaton, n th aer, we wll gve ome mrovement for Warng roblem Keyword: Warng Problem, Hardy-Lttlewood

More information

ILSim A compact simulation tool for interferometric lithography

ILSim A compact simulation tool for interferometric lithography LSm A compact smulaton tool fo ntfomtc lthogaphy Yongfa an, Anatoly Bouov, Lna Zavyalova, Janmng Zhou, Anw stoff, al Laffty, Buc W. Smth Rochst nsttut of Tchnology, Mcolctonc ngnng Dpatmnt 8 Lomb Mmoal

More information

Jones vector & matrices

Jones vector & matrices Jons vctor & matrcs PY3 Colást na hollscol Corcagh, Ér Unvrst Collg Cork, Irland Dpartmnt of Phscs Matr tratmnt of polarzaton Consdr a lght ra wth an nstantanous -vctor as shown k, t ˆ k, t ˆ k t, o o

More information

The far field calculation: Approximate and exact solutions. Persa Kyritsi November 10th, 2005 B2-109

The far field calculation: Approximate and exact solutions. Persa Kyritsi November 10th, 2005 B2-109 Th fa fl calculao: Appoa a ac oluo Pa K Novb 0h 005 B-09 Oul Novb 0h 005 Pa K Iouco Appoa oluo flco fo h gou ac oluo Cocluo Pla wav fo Ic fl: pla wav k ( ) jk H ( ) λ λ ( ) Polaao fo η 0 0 Hooal polaao

More information

PO with Modified Surface-normal Vectors for RCS calculation of Scatterers with Edges and Wedges

PO with Modified Surface-normal Vectors for RCS calculation of Scatterers with Edges and Wedges wth Modfed Suface-nomal Vectos fo RCS calculaton of Scattees wth Edges and Wedges N. Omak N. Omak, T.Shjo, and M. Ando Dep. of Electcal and Electonc Engneeng, Tokyo Insttute of Technology, Japan 1 Outlne.

More information

The Hyperelastic material is examined in this section.

The Hyperelastic material is examined in this section. 4. Hyprlastcty h Hyprlastc matral s xad n ths scton. 4..1 Consttutv Equatons h rat of chang of ntrnal nrgy W pr unt rfrnc volum s gvn by th strss powr, whch can b xprssd n a numbr of dffrnt ways (s 3.7.6):

More information

STATISTICAL MECHANICS OF DIATOMIC GASES

STATISTICAL MECHANICS OF DIATOMIC GASES Pof. D. I. ass Phys54 7 -Ma-8 Diatomic_Gas (Ashly H. Cat chapt 5) SAISICAL MECHAICS OF DIAOMIC GASES - Fo monatomic gas whos molculs hav th dgs of fdom of tanslatoy motion th intnal u 3 ngy and th spcific

More information

Lecture 2: Frequency domain analysis, Phasors. Announcements

Lecture 2: Frequency domain analysis, Phasors. Announcements EECS 5 SPRING 24, ctu ctu 2: Fquncy domain analyi, Phao EECS 5 Fall 24, ctu 2 Announcmnt Th cou wb it i http://int.c.bkly.du/~5 Today dicuion ction will mt Th Wdnday dicuion ction will mo to Tuday, 5:-6:,

More information

Optimum PSK Signal Mapping for Multi-Phase Binary-CDMA Systems

Optimum PSK Signal Mapping for Multi-Phase Binary-CDMA Systems Omum Sgnal Mappng fo Mult-Pha Bnay-CDMA Sytm Yong-Jn So and Yong-Hwan L Shool of Eltal Engnng and INMC Soul Natonal Unvty Kwanak P O Box 34 Soul 5-744 Koa -mal: yl@nuak Atat - Although th CDMA ytm an ffntly

More information

Chapter-10. Ab initio methods I (Hartree-Fock Methods)

Chapter-10. Ab initio methods I (Hartree-Fock Methods) Chapt- Ab nto mthods I (Hat-Fock Mthods) Ky wods: Ab nto mthods, quantum chmsty, Schodng quaton, atomc obtals, wll bhavd functons, poduct wavfunctons, dtmnantal wavfunctons, Hat mthod, Hat Fock Mthod,

More information

Precomputed Radiance Transfer: Theory and Practice

Precomputed Radiance Transfer: Theory and Practice Pecomute Raance Tanfe: Theoy an Pactce 1 Pecomute Raance Tanfe: Theoy an Pactce Pecomute Raance Tanfe: Theoy an Pactce Pete-Pke Sloan Mcooft Jaakko ehtnen elnk Unv. of Techn. & Remey Entetanment Jan Kautz

More information

GRAVITATION 4) R. max. 2 ..(1) ...(2)

GRAVITATION 4) R. max. 2 ..(1) ...(2) GAVITATION PVIOUS AMCT QUSTIONS NGINING. A body is pojctd vtically upwads fom th sufac of th ath with a vlocity qual to half th scap vlocity. If is th adius of th ath, maximum hight attaind by th body

More information

A Note on Estimability in Linear Models

A Note on Estimability in Linear Models Intrnatonal Journal of Statstcs and Applcatons 2014, 4(4): 212-216 DOI: 10.5923/j.statstcs.20140404.06 A Not on Estmablty n Lnar Modls S. O. Adymo 1,*, F. N. Nwob 2 1 Dpartmnt of Mathmatcs and Statstcs,

More information

Environmental Engineering / Fundamentals of Fluid Mechanics and Heat Transfer 2017/2018

Environmental Engineering / Fundamentals of Fluid Mechanics and Heat Transfer 2017/2018 H H Envonmntal Engnng / Fundamntal o Flud Mcanc and Hat an 07/08. Dtmn t tack pu n a buldng wc m g, t ndoo a tmpatu = +0 C and outdoo a tmpatu = C. Wat t nutal lvl gt, t a two opnng n t buldng nvlop, on

More information

Exam 2 Solutions. Jonathan Turner 4/2/2012. CS 542 Advanced Data Structures and Algorithms

Exam 2 Solutions. Jonathan Turner 4/2/2012. CS 542 Advanced Data Structures and Algorithms CS 542 Avn Dt Stutu n Alotm Exm 2 Soluton Jontn Tun 4/2/202. (5 ont) Con n oton on t tton t tutu n w t n t 2 no. Wt t mllt num o no tt t tton t tutu oul ontn. Exln you nw. Sn n mut n you o u t n t, t n

More information

Why switching? Modulation. Switching amp. Losses. Converter topology. i d. Continuous amplifiers have low efficiency. Antag : u i

Why switching? Modulation. Switching amp. Losses. Converter topology. i d. Continuous amplifiers have low efficiency. Antag : u i Modlaton Indtral Elctrcal Engnrng and Atomaton Lnd nvrty, Swdn Why wtchng? Contno amplfr hav low ffcncy a b Contno wtch pt ( t ) = pn( t) = ( a b) Antag : ( a b) = Pn = Pt η = = = Pn Swtchng amp. Lo Convrtr

More information

If we cannot accept your contribution in your preferred presentation mode, would you still be prepared to present in the alternative mode (tick one):

If we cannot accept your contribution in your preferred presentation mode, would you still be prepared to present in the alternative mode (tick one): Pap Submon Fom Nam of Pntng Autho Ahmt Bd Öz Add )ÕUDW hqlyhuvlwhvl 0 KHQGLVOLN )DN OWHVL %LOJLVD\DU 0 KHQGLVOL L (OD]Õ 7 UNL\H Phon (+904242370000 (5292) cp: 05333303642) Fax (+90424 2383787) Oth autho:

More information

Speed Control of Direct Torque Controlled Induction Motor By using PI, Anti-Windup PI and Fuzzy Logic Controller

Speed Control of Direct Torque Controlled Induction Motor By using PI, Anti-Windup PI and Fuzzy Logic Controller Intnatonal Jounal of Intllgnt Sytm and Applcaton n Engnng Advancd Tchnology and Scnc ISSN:7-7997-799 www.atcnc.og/ijisae Ognal Rach Pap Spd Contol of Dct Toqu Contolld Inducton Moto By ung, Ant-Wndup and

More information

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law Physcs 11b Lectue # Electc Feld Electc Flux Gauss s Law What We Dd Last Tme Electc chage = How object esponds to electc foce Comes n postve and negatve flavos Conseved Electc foce Coulomb s Law F Same

More information

ECE 107: Electromagnetism

ECE 107: Electromagnetism ECE 07: Elcomagnsm S 8: Plan wavs Insuco: Pof. Valy Lomakn Dpamn of Elccal and Compu Engnng Unvsy of Calfona, San Dgo, CA 92093 Wav quaon Souc-f losslss Maxwll s quaons Apply cul = jωμ ε = = jωε μ = 2

More information

References. Basic structure. Power Generator Technologies for Wind Turbine. Synchronous Machines (SM)

References. Basic structure. Power Generator Technologies for Wind Turbine. Synchronous Machines (SM) Gnato chnologi fo Wind ubin Mhdad Ghandhai mhdad@kth. Rfnc 1. Wind Plant, ABB, chnical Alication Pa No.13.. WECC Wind Plant Dynamic Modling Guid, WECC Rnwabl Engy Modling ak Foc. 3. Wind ubin Plant Caabiliti

More information

Rectification and Depth Computation

Rectification and Depth Computation Dpatmnt of Comput Engnng Unvst of Cafona at Santa Cuz Rctfcaton an Dpth Computaton CMPE 64: mag Anass an Comput Vson Spng 0 Ha ao 4/6/0 mag cosponncs Dpatmnt of Comput Engnng Unvst of Cafona at Santa Cuz

More information

( r) E (r) Phasor. Function of space only. Fourier series Synthesis equations. Sinusoidal EM Waves. For complex periodic signals

( r) E (r) Phasor. Function of space only. Fourier series Synthesis equations. Sinusoidal EM Waves. For complex periodic signals Inoducon Snusodal M Was.MB D Yan Pllo Snusodal M.3MB 3. Snusodal M.3MB 3. Inoducon Inoducon o o dsgn h communcaons sd of a sall? Fqunc? Oms oagaon? Oms daa a? Annnas? Dc? Gan? Wa quaons Sgnal analss Wa

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

4.8 Huffman Codes. Wordle. Encoding Text. Encoding Text. Prefix Codes. Encoding Text

4.8 Huffman Codes. Wordle. Encoding Text. Encoding Text. Prefix Codes. Encoding Text 2/26/2 Word A word a word coag. A word contrctd ot of on of th ntrctor ar: 4.8 Hffan Cod word contrctd ng th java at at word.nt word a randozd grdy agorth to ov th ackng rob Encodng Txt Q. Gvn a txt that

More information

Small signal analysis

Small signal analysis Small gnal analy. ntroducton Let u conder the crcut hown n Fg., where the nonlnear retor decrbed by the equaton g v havng graphcal repreentaton hown n Fg.. ( G (t G v(t v Fg. Fg. a D current ource wherea

More information

4D SIMPLICIAL QUANTUM GRAVITY

4D SIMPLICIAL QUANTUM GRAVITY T.YUKAWA and S.HORATA Soknda/KEK D SIMPLICIAL QUATUM GRAITY Plan of th talk Rvw of th D slcal quantu gravty Rvw of nurcal thods urcal rsult and dscusson Whr dos th slcal quantu gravty stand? In short dstanc

More information

E-Companion: Mathematical Proofs

E-Companion: Mathematical Proofs E-omnon: Mthemtcl Poo Poo o emm : Pt DS Sytem y denton o t ey to vey tht t ncee n wth d ncee n We dene } ] : [ { M whee / We let the ttegy et o ech etle n DS e ]} [ ] [ : { M w whee M lge otve nume oth

More information

Outline. Motivation. Motivation. Theoretical method. Main results. Summary. Motivation. Theoretical method. Main results. Summary.

Outline. Motivation. Motivation. Theoretical method. Main results. Summary. Motivation. Theoretical method. Main results. Summary. Outln Thotcal Study on Elcton Impact Exctaton and Dlctonc Rcombnaton of Hghly Chagd Tungstn Ions Thotcal mthod, Zhongwn Wu, and Chnzhong Dong Ky Lab of Atomc and Molcula Physcs & Functonal Matals of Gansu,

More information

Ερωτήσεις και ασκησεις Κεφ. 10 (για μόρια) ΠΑΡΑΔΟΣΗ 29/11/2016. (d)

Ερωτήσεις και ασκησεις Κεφ. 10 (για μόρια) ΠΑΡΑΔΟΣΗ 29/11/2016. (d) Ερωτήσεις και ασκησεις Κεφ 0 (για μόρια ΠΑΡΑΔΟΣΗ 9//06 Th coffcnt A of th van r Waals ntracton s: (a A r r / ( r r ( (c a a a a A r r / ( r r ( a a a a A r r / ( r r a a a a A r r / ( r r 4 a a a a 0 Th

More information

Theoretical Electron Impact Ionization, Recombination, and Photon Emissivity Coefficient for Tungsten Ions

Theoretical Electron Impact Ionization, Recombination, and Photon Emissivity Coefficient for Tungsten Ions TM on Unctanty ssssmnt and Bnchmak Expmnts fo &M Data fo Fuson pplcatons Thotcal Elcton Impact Ionzaton, Rcombnaton, and Photon Emssvty Coffcnt fo Tungstn Ions D.-H. Kwon, Koa tomc Engy Rsach Insttut 2016.

More information