TIME-OPTIMAL PATHS FOR LATERAL NAVIGATION OF AN AUTONOMOUS UNDERACTUATED AIRSHIP
|
|
- Rosemary Hood
- 5 years ago
- Views:
Transcription
1 IME-OPIMAL PAHS FOR LAERAL NAVIGAION OF AN AUONOMOUS UNDERACUAED AIRSHIP Slim Him nd Ysmin Bsoui Looi Sysèms Comls, CNRS-FRE 9, Unisié d Ey Vl d Essonn 8, Ru du Plou, 9 Ey, Fnc {him, soui}@iu.uni-y.f ABSRAC his dls wih chciion of h shos hs fo ll nigion of n uonomous undcud ishi king ino ccoun is dynmics nd cuo limiions. h iniil nd minl osiions gin. W would lik o scify h conol focs h s h unmnnd il hicl o h gin minl osiion quiing h miniml im fo ll nigion. h licion of Ponygin s Miml Pincil, llows us o find fmily of imoiml hs. Bsd on h symmy of ishi dynmics, i.. wih sc o oion nd nslion, i is ossil o consuc glol jcois conncing wo configuions y succssion of fini num of hs im-oiml hs using gomic soning. INRODUCION Unmnnd il hicls nw focus of sch, cus of hi imon licion onil. hy cn diidd ino h diffn ys : ducd scl fid wing hicls (ilns), oy wing icf (hlico) o ligh hn i hicls (ishis). Ligh hn i hicls sui wid ng of licions, nging fom dising, il hooghy nd suy wok sks. hy sf, cosffci, dul, nionmnlly nign nd siml o o. Aishis off h dng of qui ho wih nois lls much low hn hlicos. Unmnnd moly-od ishis h ldy od hmsls s cm nd V lfoms, suillnc nd fo scilid scinific sks such s h monioing nd nionmnl conol. An cul nd is owd uonomous ishis. Wh mks hicl ligh hn i is h fc h i uss lifing gs (i.. hlium o ho i) in od o ligh hn h suounding i. h incil of Achimds lis in h i s wll s und w. Aishis owd nd h som mns of conolling hi dicion. Non igid ishis h mos common fom nowdys. hy siclly lg gs lloons. h mos common fom of diigil is n llisoid. I is highly odynmiclly ofil wih good sisnc o osics ssus. Is sh is minind y is innl ossu. h only solid s h gondol, h s of oll ( i of oll mound h gondol) nd h il fins. h nlo holds h hlium h mks h lim ligh hn i. In ddiion o h lif oidd y hlium, ishis di odynmic lif fom h sh of h nlo s i mos hough h i. h ojci of his is o gn dsid fligh jcoy o followd y h ishi. h jcoy gnion modul gns nominl s jcoy nd nominl conol inu. A mission ss wih k-off fom h lfom wh h ms h holds h mooing dic of h ishi is mound. yiclly, fligh oion mods cn dfind s: k-off, cuis, lnding nd ho. Af h us hs dfind h gol sks, h h gno hn dmins h fo h hicl h is jcoy in sc. In Aonuics, ln fligh conol ofn inols ll nd longiudinl s dcouling. h olm of jcoy gnion fo ll conol is fomuld s n oimiion olm. his moion gnion ks ino ccoun h consins on lociy nd h ound on h udd ngl. h minimum im olm is sold using h mimum incil of Ponygin. Onc his fnc jcoy dmind, h ishi cn follow i wih n oi fdck. h ligh hn i lfom of h 'Looi ds Sysèms Comls' is h AS y Aisd Aishis. I is moly ilod ishi dsignd fo mo snsing. I is non igid 6m long,.m dim nd 8.6m olum ishi quid wih wo col ngins on h sids of h gondol nd conol sufcs h sn. h fou silis nlly cd on h full nd udd momn is oidd y dic linkg o h sos. Enlo ssu is minind y i fd fom h olls ino h wo llons locd insid h cnl oion of h hull. hs llons slf guling nd cn fd fom ih ngin. h ngins sndd modl icf y unis.
2 Figu LSC ishi lfom AS dscid li o h inil fnc fm whil h lin nd ngul lociis of h hicl should ssd in h ody-fid coodin sysm. his fomulion hs n fis usd fo undw hicls. In his, h oigin C of coincids wih h R m cn of olum of h hicl. Is s h incil s of symmy whn ill. hy mus fom igh hndd ohogonl nomd fm. h is of h onuic fm follows h dicion of h ishi li lociy V wih sc o h wind. α is h ngl of ck wihin h m m ln, nd β h skid ngl wihin h m y m ln. o dsci h osiion nd h oinion of h ishi AIRSHIP DYNAMIC MODELING Kinmic modling A gnl sil dislcmn of igid ody consiss of fini oion ou sil is nd fini nslion long som co. h oionl nd nslionl s in gnl nd no ld o ch oh. I is ofn sis o dsci sil dislcmn s cominion of oion nd nslion moions, wh h wo s no ld. How, h comind ffc of h wo il nsfomions (i.. oion, nslion ou hi sci s) cn ssd s n quiln uniqu scw dislcmn, wh h oionl nd nslionl s in fc coincid. h conc of scw hus sns n idl mhmicl ool o nly sil nsfomion. h fini oion of igid ody dos no oy o h lws of co ddiion (in icul commuiiy) nd s sul h ngul lociy of h ody cnno ingd o gi h iud of h ody. h mny wys o dsci fini oions. Dicion cosins, Rodigu - Hmilon's (qunions) ils, Eul ms, Eul ngls, cn s s mls. Som of hs gous of ils y clos o ch oh in hi nu. h usul miniml snion of oinion is gin y s of h Eul ngls, ssmld wih h h osiion coodins llow h dsciion of h siuion of igid ody. A dicion cosin mi (of Eul oions) is usd o dsci h oinion of h ody (chid y succssi oions) wih sc o som fid fm fnc. h fnc fms considd, figu, in h diion of h kinmics nd dynmics quions of moion. hs h Eh fid fm considd s Gliln, nd wo locl fms chd o ishi, h ody fid fm R nd onuic fm R. h m osiion nd oinion of h hicl should R f Figu Gnl configuion of fms wih sc o h inil fnc fm, h Eulin miion is usd. h h oinion ngls : h Roll φ, h Pich θ nd h Yw ψ. h cun configuion is hn dducd fom h lmny oions. h osiion η nd h oinion η of h hicl in cn scily dscid y: R f ( y ) nd η ( φ θ ψ η ) hn h oinion mi fm R nd fnc R is gin y m f H R f () wn h ody fid, :
3 CψCθ SψCφ + CψSθSφ H SψCθ CψCφ + SψSθSφ Sθ SφCθ () SψSφ + CψSθCφ CψSφ + SψSθCφ CφCθ nd h nsfom mi wn h ody fid H fm Rm nd h onuic fm R cn win s: CαCβ CαSβ Sα H Sβ Cβ SαCβ SαSβ Cα () () () wh C cos nd S sin H nd H SO() dnos h oion mi h scifis h oinion of h ishi fm li o h inil fnc fm in inil fnc fm coodins. SO() is h scil ohogonl gou of od which is snd y h s of ll ohogonl oion mics h chcisics : RR I nd d( R) I sns h idniy mi. π π his dsciion is lid in h gion θ. A singuliy of his nsfomion iss fo: π θ ± k π, k Ζ L's now inoduc V ( u w) s h lin lociy of h oigin C ssd in R nd ( ) Ω q s h ngul lociy ssd in h fm. h kinmics of h ishi cn ssd in h following wy: wh η R η η ( η ) V ( η ) Ω m () Sφ nθ Cφ Cφ Sφ () Sφ Cφ Cθ Cθ Dynmic modling In his scion, nlyic ssions fo h focs nd momns cing on h ishi did. I is dngous o fomul h quions of moion in ody fid fm o k dng of h hicl's gomicl ois. Alying Nwon's lws of moion ling h lid focs nd momns o h suling nslionl nd oionl cclions ssmls h quions of moion fo h 6 dgs of fdom. h focs nd momns fd o sysm of ody-fid s, cnd h ishi cn of olum. W will mk in h squl som simlifying ssumions: h h fid fnc fm is inil, h giionl fild is consn, h ishi is suosd o wll infld, h olsic ffcs ignod, h dnsiy of i is suosd o unifom, nd h influnc of gus is considd s coninuous disunc, ignoing is sochsic chc. h dfomions considd o ngligil. Glol dynmics quion cn win s : M η τ + τ (η) d wh M d nd τ m (η ) scily h ini mi nd h dynmicl (Coiolis nd cnifugl) nsos which du o h mss of ishi, nd τ is h sum of h diffn nl nso, which inol: Glol odynmic nso du o h ddd mss hnomnon lus focs nd momns gnd y h ishi ody (hull, fins nd gondol). Aosic nso dsciing h focs nd momns du o h giy nd uoyncy Poulsion nso du o h cod hus. m (6) Ll dynmics of h ishi h ishi modl consiss of ss, comlicing h conol dsign. In onuics, y nul simlificion consiss of dcomosing h fligh mods ino: k off, cuis nd lnding. hs sks cn diidd ino wo min mods: longiudinl mod nd ll on. In his w focus on ll mod in consn liud. h cod huss nd los ssocid o h longiudinl nigion conoll o hold h liud nd li lociy nigion consn. h udds llow h ishi o nig in h hoionl ln. h mhmicl modl of h immd ll dynmics in h locl fm is gin y 6 : my m + Y + Y + Y + m Y m W m U + Y + Y + + Y ( F G F B ) φ cos( θ ) (7)
4 + N m U + N + m G + N + F φ cos G + m U + L + F φ cos m ( θ ) L N mw + + N ( θ ) L + L + + N mw L (8) (9) hs quions cosond o h Ll, Yw nd oll dynmics. U nd h il nd ll lociy comonns in locl fm. wh Y cofficins. m i, Y, N U, N V V, L cos sin ( β ) ( β ) nd L () h odynmic is h n mss in h i h dicion. i ini mi lmns. m is h ishi mss. θ is h quiliium ich ngl. In gnl, h ishi mos wih low sd. h quiliium wn h cnifugl momn ound is cusd y h udd dflcion nd giionl momn is h cus of n insignificnly smll Roll ngl nd which cn omid. king hs considions ino ccoun, h modl cn simlifid s: m y + m + m N Y mu + Y + Y + N + Y mu + + N + N nd h kinmic quions gin y: ψ V cos y V sin ( ψ + β ) ( ψ + β ) m () () () Rciuling, h modl of h ll dynmics of h ishi cn win s: Figu Ll configuion of ishi (o iw) i fm h coodins of h cn of mss in h locl Rm 6. β is h skid ngl wn h li lociy V nd m is ino m ym ln. In h snc of wind, his ngl s whn h ishi follows h wih non o cuu. Fo fid udd dflcion, i.. cosonding o h cicl h, his ngl ks consn lu whn n quiliium wn odynmic momn, cusd y h ishi ody (hull, h icl fins nd conol sufcs) moion wih sc o h suounding i nd h cnifugl on is slishd. his ngl ks on smll lus. wh: m y β β + + ψ y V V β + + cos sin ( ψ + β ) ( ψ + β ) Y + m + Y N m Y m N Y mu + m + Y N mu my m Y m N () () (6) (7) (8)
5 m N Y + my N my m Y m N m N Y mu + myn mu my m Y m N Y Y m N m y m Y m N m N Y + my N my m Y m N h ll dynmics of h ishi h n ffin sucu. In h comc fom h dynmics cn gin y: X f ( X ) + g (9) wh : β + β + f ( X ) nd g V cos( β + ψ ) V sin( β + ψ ) Som difficulis is wih his modl: h fis on is h undcuion of his sysm, i.. ss sd y singl inu conol. h scond on is h nonholonomic chc: non ingl lionshi wn lociis: sin( β + ψ ) + y cos( β + ψ ) () his kind of consins clld Pfffin Consins 8. im Oiml Emls In his gh, l s inoduc fnc imoiml hs fo h sysm und sudy, king ino ccoun h sysm dynmics nd cuo ciliis. Hnc, his olm cn fomuld s follows: min f d f () X f ( X ) + g( X ) u X ( u min ) X nd X ( f ) u u m X f () h olm is o find h dmissil conol u h minimi h im fo which h sysm chs h finl s fom h iniil on X. Wihou loss of X f gnliy, nd y siml nomliion nd shifing (if h wo ounds of h conol domin no symmic), w cn consin h conol o long o uni inl, i.. u. o sol his olm, w ly h Ponygin s Mimum Pincil (PMP) o oin ncssy condiions fo fnc jcoy of sysm o im-oiml. h PMP ss h: if X () is imoiml jcoy dfind on [, ], nd u() is h cosonding im-oiml fnc conol, hn h iss n soluly coninuous co funcion clld h djoin co, :[, ] R, such h h following condiions sisfid,7,9 :. ( ) fo ll [, ]. H ( X ( ), ( ), u( )) min H ( X ( ), ( ), ( )), wih > fo y fid X ( ), ( ) nd, such h H ( X ( ), ( ), u( )) + ( ), X ( ), wh, is h co sc inn oduc.. h djoin co () sisfis h following H quion: X A il ( X,, u) ifying h ncssy condiions is clld n ml. Fis, consid h Hmilonin H, funcionl fo h oiml conol olm wh mulilis h djoin h consins. h Hmilonin funcion of h sysm is gin y: H( X( ), ( ), ( )) + f ( X) + g( X) + + V + ( β + + ) ( β + + ) + sin( ψ + β) + V nd h co-s dynmics gin y: cos( ψ + β) () Sujc o
6 V V cos( ψ + β) + V sin( ψ + β) V sin( ψ + β) cos( ψ + β) () hfo, s nd consn on [, ] h iss µ nd γ [,π ] such h, [, ] hn : V µ sin( ψ + β γ ) µ cos( γ ) µ sin( γ ) + V µ sin( ψ + β γ ) nd h Hmilonin coms: H( X + + µ V,, ) + ( β + ) ( β + ) + cos( ψ + β γ ) + ( + ) () (6) h minimiion of h Hmilonin wih sc o h conol is oind y minimiing g( X ). h conol longs o uni conol domin, hn his minimiion cn chid y king fo h oosi sign of g(x ), hn: if g < if g > (7) h funcion φ ( ) g( X ), dfind long n ml ( X,, ) is clld h swiching funcion ssocid o h sysm. Clly, h os of his funcion imon fo h sudy of oiml synhsis. If h iss nonmy inl such h φ () is idniclly o, h ml is singul on h inl. Assum now h ml o ng, i.. ks is lus in {, } fo lmos im s such h is no lmos ywh consn on ny inl of h fom ε, + ε, ε >. is clld swiching im fo ] [ s s s nd cosonding s is clld swiching s. h jcois cosonding o h conols ±, figu cicls. h fss wy o un is uning wih h smlls dius, mns h mking h udds dflcion in on of is limis. i.. o un lf o igh. figu nd 6 shows, β nd cus whn h ishi ss fom sigh lin o cicl. hy k consn lus whn h cicl mnn h is ind. β() () Y X Figu Cicl h fo 6 Figu skid ngl β sons fo Figu6 Yw sons fo Singul mls As mniond o, h singul conols chcid y h fc h φ () is idniclly o in nonmy inl. How, h PMP loss is disciminion nu, i.. y conols in U sisfy h ncssy condiions. In his cs, w nd som ddiionl condiions. h nulliy of φ () in nonmy 6
7 inl imlis h ll is im diis null in h inl, i.. φ( ) φ( ) L φ m ( ) h ocss of diion is sod whn h conol in h ssion of hs diion. Fo n ffin sysm, k φ ( ) ( X, ) + ( X, ) (8) k is clld h od of singul conol. Hnc, h singul conol cn ssd s: ( X, ) (9) ( X, ) Poosiion: h singul conols of ou sysm of h fis od nd n noml. Poof: L s di h swiching funcion φ () : + oosiion: h sysm of diffnil quions soluion. Poof: Fom h condiion w find, imlying ( + β γ ) (), (6) (6), hs s sin ψ (7) ψ + β γ kπ (8) wih k Ζ his sul sns h ncssy condiion fo h isnc of h singul conol. Fom h quion (8), w cn s h, h conol cofficin φ( ) g + φ( ) g ( f f g q + + g ) g () () q g is n nishing. So h Hmilonin coms: fom his, ( V cos( ψ + β γ ) H X,, ) + µ V cos( ψ + β γ ) (9) () µ ± () V cos( ψ + β γ ) V nd φ( ) q + g q + ( f f ) q () wh dnos h jcoin mi of h co V. No h V g. Nullifying hs quions, w find: () () lcing in h fis nd h scond quions of h sysm of quions (), w find: + () w cn conclud fom quion ( ) h: µ is n qul o o, cus h o lu of µ imlis null djoin co, his condics PMP smns. o o h minimliy of h singul conols, w mus s h gnlid coniy condiion ofn clld, snghnd Lgnd -Clsh condiion gin y, : d u d k φ k ( ) k k is h od of singul conol. Fo ou sysm: d φ d ( ) µ V cos( ψ + β γ ) fom h quion (): µ V cos( ψ + β γ ) which is u, i.. is osii y dfiniion. () () () 7
8 Hnc, h singul conol, nd fom quion () cn gin y: ( q f f q) ( + ) ( β + ( + ) ) q + g n( ψ + β γ ) () fom h isnc condiion of h singul conol, i.. ψ + β γ kπ, h conol cn ducd o: such h < ( β + ( + ) ) (6) Figu7 singul conol Discussion of h singul conol Onc h singul conol is dmind, w illus h gomic sh of h fnc jcoy of h ishi und his singul conol. Fom h singul conol ncssy condiion, ψ + β γ is consn, nd γ is consn oo, hn ψ + β is consn. his imlis h h ngl wn h li lociy V nd h fnc is is consn. hus h singul jcoy is sigh lin. W cn find h sm sul y lying h conol dfind low in h dynmics of β : β + β + ψ (7) imlying non iion of β + ψ ngl, h fnc jcoy is hus lin. nsiion fom cud h o h lin quis h licion of h singul conol which gows monoonously, figu7. his losion of conol is du o h non ccnc of h disconinuiis in h cuu y h ishi dynmics. Fo his son w wn o smooh his cuu y oimiing h nsiion im wn non o cuu jcoy nd sigh lin. Whn w y o connc wo lignd configuion h oiml h is oiously sigh lin, i.. β, which cosond o (6)..,his conol is mddd in β() () Figu 8 skid ngl sons o 8 - Figu 9 Yw sons o 8
9 wh is mi fomd y h igncos cosonding o h sysm ignlus. h suln digonlid dynmics gin y: Figu ishi configuion on cicl lin nsiion. Oiml nsiion of non null cuu h o sigh lin W now consid h issus ining o h swiching wn h non o cuu h nd sigh lin. W h ldy chcid h foms of h oiml s nd conol jcois in ch mod sly. hfo, w nd o fuh scify h im inl cosonding o h mod swiching nd h ms h dmin whn nd fo how long h singul conol lss. W ocd o ddss oh issus using coninuiy gumn.w look fo h fss wy fo h ishi o mo fom non null cuu hs o sigh lin in oiml im. h lin is chcid y o lus of β nd, nd h non null cuu hs chcid y non o lus of β nd. L s us h dynmics of β nd fo chiing his ojci. In oiml conol liu, h following hom is dmonsd. hom: Fo ny lin noml sysm h oiml conol is of ng-ng y. h nomliy condiion mns h h sysm is conolll wih sc o ch of is conol inus. h dminn of h conolliliy mi is: + ) ( (8) h sysm und considion is noml. L s find h swiching sufc llowing h sysm o insc h oigin, sing fom ny iniil condiion wihin his sufc, nd und scific conol, i.. ±. h dynmics of h Yw nd h skid ngl symoiclly sl. o simlify h clculus, sion of dynmics is fomd y s mi digonliion, y mns of lin s sc il nsfomion. L + + () h cosonding soluions of his sysm gin y: ( ) ( ) + + ( + ) ( + ) () wh nd h iniil condiions. o find h swiching sufc w look fo h iniil condiions fom which h sysm dynmic jcoy coss h oigin und h conol ±. h g oin is ( c ) ( ) c c. How, h coss im wih h oigin is sily clculd fom h sysm (): nd ln + c () ln + c () quliing ims nd soling h suling quion fo w find: + + his quion dfins h swiching sufc in nd () coodins cosonding o ±, figu nd, in figu, w show h whol swiching sufc. β (9) 9
10 Figu swiching sufc fo h condiion in quion () nd swiching whn h < ε is hold. In his cs h conol swich o h oh ng. h sm lgoihm is lid o dc h inscion wih h oigin, whn is h cs, h conol is hold o o. Figu show h suling im-oiml nsiion conol fom cicl o sigh lin. Figu 6 illus comison of β sons und licion of nd. W s h h β sons o chs h o y fs. In figu 7 w show h configuion of h ishi on h suln jcoy y licion of Figu Swiching sufc fo Figu S sc oiml nsiion fom cicl o sigh lin Figu ol swiching sufc figu shows h nsiion jcois whn lying ng-ng conol. h suln jcois h h hyssis cycl fom. h lgoihm of h oiml nsiion is sd on h dcion of h coss oins of h ng-ng jcois wih h swiching sufc, h id is o com h hoionl disnc of h sysm s oin (, ) fom h swiching sufc y lcing Figu im-oiml cicl o lin nsiion conol
11 Figu6 skid ngl β sons o nd Y Byson, A.E., HO, Y.C., Alid Oiml Conol, Oimiion, Esimion nd Conol, OHN WILEY & SONS, 97. Fossn,., Guidnc nd Conol of Ocn Vhicls,. WILEY PRESS, 996. Hygounnc, E., Souès, P., Lcoi, S., Modélision d un Diigl Eud d l Cinémiqu d l Dynmiqu, LAAS-CNRS, 6, Oco. 6 Khouy, G.A., Gill,.D. Edios, Aishi chnology, CAMBRIDGE AEROSPACE, SERIE, Lumond,.P, Roo Moion Plnning nd Conol, Lcu Nos in Conol nd Infomion Scincs 9, SPRINGER, Muy, R.M., Li, Z., Ssy, S., S., Mhmicl Inoducion o Rooic Mniulion, CRC Pss, Ponigin, L., Bolinski, V., Gmkélidé, R., Michchnko, E., h Mhmicl hoy of Oiml Pocsss, Inscinc Pulishs, 96. Roins, H. M., A Gnlid Lgnd-Clsch Condiion fo h Singul Css of Oiml Conol, IBM ounl of Rsch nd Dlomn, Vol.,. 6-7, uly 967. Zfn, M., Kum, V., Cok, C., Mics nd Conncions fo Rigid-Body Kinmics, Innionl ounl of Rooics Rsch, Vol. 8, #,. -8. f X Figu7 Gomic configuion of ishi sons o Conclusion nd fuu wok In his, chciion of h im-oiml fnc hs fo ll nigion of h ishi is slishd, h Mimum Pincil of Ponygin gis locl infomion of h oimliy of h hs. In h fuu wok, his sudy should comld y gomic soning fo oiding wy o slc insid of his fmily, h oiml h o link ny wo configuions in ll ln. Acknowldgmn h uhos wish o hnks P. Souès nd E. Hygounnc, fom LAAS-CNRS (oulous, Fnc). Rfncs Ahns, M., Fl, P. L., Oiml Conol, An inoducion o h hoy nd is Alicions, McGRAW-HILL BOOK COMPANY, 966. Bsoui, Y., Him, S., Som Insighs in Ph Plnning of Smll Auonomous Aishis, ounl of Achis of Conol Scincs, Polish Acdmy of Scincs, ol.,, ; 9-66.
Chapter 4 Circular and Curvilinear Motions
Chp 4 Cicul n Cuilin Moions H w consi picls moing no long sigh lin h cuilin moion. W fis su h cicul moion, spcil cs of cuilin moion. Anoh mpl w h l sui li is h pojcil..1 Cicul Moion Unifom Cicul Moion
More informationA Simple Method for Determining the Manoeuvring Indices K and T from Zigzag Trial Data
Rind 8-- Wbsi: wwwshimoionsnl Ro 67, Jun 97, Dlf Univsiy of chnoloy, Shi Hydomchnics Lbooy, Mklw, 68 CD Dlf, h Nhlnds A Siml Mhod fo Dminin h Mnouvin Indics K nd fom Ziz il D JMJ Jouné Dlf Univsiy of chnoloy
More informationDerivation of the differential equation of motion
Divion of h iffnil quion of oion Fis h noions fin h will us fo h ivion of h iffnil quion of oion. Rollo is hough o -insionl isk. xnl ius of h ll isnc cn of ll (O) - IDU s cn of gviy (M) θ ngl of inclinion
More informationAdrian Sfarti University of California, 387 Soda Hall, UC Berkeley, California, USA
Innionl Jonl of Phoonis n Oil Thnolo Vol. 3 Iss. : 36-4 Jn 7 Rliisi Dnis n lonis in Unifol l n in Unifol Roin s-th Gnl ssions fo h loni 4-Vo Ponil in Sfi Unisi of Clifoni 387 So Hll UC Bkl Clifoni US s@ll.n
More informationCHARACTERIZATION OF NON TRIM TRAJECTORIES OF AN AUTONOMOUS UNDERACTUATED AIRSHIP IN A LOW VELOCITY FLIGHT
HARAERAON OF NON R RAEORE OF AN AUONOOU UNERAUAE ARH N A LOW VELOY FLGH Ysmin Bsoi, Looi s sèms omls L, 9 Unisié E, Fn soi@ini-f As : h oji of his is o gn si fligh h o follo n onomos ishi h s is sos iho
More informationME 141. Engineering Mechanics
ME 141 Engineeing Mechnics Lecue 13: Kinemics of igid bodies hmd Shhedi Shkil Lecue, ep. of Mechnicl Engg, UET E-mil: sshkil@me.bue.c.bd, shkil6791@gmil.com Websie: eche.bue.c.bd/sshkil Couesy: Veco Mechnics
More informationLecture 2: Bayesian inference - Discrete probability models
cu : Baysian infnc - Disc obabiliy modls Many hings abou Baysian infnc fo disc obabiliy modls a simila o fqunis infnc Disc obabiliy modls: Binomial samling Samling a fix numb of ials fom a Bnoulli ocss
More informationSupporting Online Materials for
Suppoing Onlin Mils o Flxibl Schbl nspn Mgn- Cbon Nnoub hin Film Loudspks Lin Xio*, Zhuo Chn*, Chn Fng, Ling Liu, Zi-Qio Bi, Yng Wng, Li Qin, Yuying Zhng, Qunqing Li, Kili Jing**, nd Shoushn Fn** Dpmn
More informationPhysics 201, Lecture 5
Phsics 1 Lecue 5 Tod s Topics n Moion in D (Chp 4.1-4.3): n D Kinemicl Quniies (sec. 4.1) n D Kinemics wih Consn Acceleion (sec. 4.) n D Pojecile (Sec 4.3) n Epeced fom Peiew: n Displcemen eloci cceleion
More information3.4 Repeated Roots; Reduction of Order
3.4 Rpd Roos; Rducion of Ordr Rcll our nd ordr linr homognous ODE b c 0 whr, b nd c r consns. Assuming n xponnil soluion lds o chrcrisic quion: r r br c 0 Qudric formul or fcoring ilds wo soluions, r &
More informationAir Filter 90-AF30 to 90-AF60
Ai il -A o -A6 Ho o Od A /Smi-sndd: Sl on h fo o. /Smi-sndd symol: Whn mo hn on spifiion is uid, indi in lphnumi od. Exmpl) -A-- Sis ompil ih sondy is Mil siion Smi-sndd Thd yp Po siz Mouning lo diion
More informationThe dynamics of the wagon rolling down the hump profile under the impact of fair wind Research Paper
Dic Rsch Jounl of Engining nd Infomion Tchnology (DRJEIT Vol. ( pp. 7-4 y 4 ISSN 354-455 Ailbl onlin dicschpublish.og/dj 4 Dic Rsch Jounls Publish Th dynmics of h gon olling don h hump pofil und h impc
More informationAppendix. In the absence of default risk, the benefit of the tax shield due to debt financing by the firm is 1 C E C
nx. Dvon o h n wh In h sn o ul sk h n o h x shl u o nnng y h m s s h ol ouon s h num o ssus s h oo nom x s h sonl nom x n s h v x on quy whh s wgh vg o vn n l gns x s. In hs s h o sonl nom xs on h x shl
More information() t. () t r () t or v. ( t) () () ( ) = ( ) or ( ) () () () t or dv () () Section 10.4 Motion in Space: Velocity and Acceleration
Secion 1.4 Moion in Spce: Velociy nd Acceleion We e going o dive lile deepe ino somehing we ve ledy inoduced, nmely () nd (). Discuss wih you neighbo he elionships beween posiion, velociy nd cceleion you
More informationT 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 informationTheory of Spatial Problems
Chpt 7 ho of Sptil Polms 7. Diffntil tions of iliim (-D) Z Y X Inol si nknon stss componnts:. 7- 7. Stt of Stss t Point t n sfc ith otd noml N th sfc componnts ltd to (dtmind ) th 6 stss componnts X N
More informationEquations and Boundary Value Problems
Elmn Diffnil Equions nd Bound Vlu Poblms Bo. & DiPim, 9 h Ediion Chp : Sond Od Diffnil Equions 6 คณ ตศาสตร ว ศวกรรม สาขาว ชาว ศวกรรมคอมพ วเตอร ป การศ กษา /555 ผศ.ดร.อร ญญา ผศ.ดร.สมศ กด วล ยร ชต Topis Homognous
More informationMotion on a Curve and Curvature
Moion on Cue nd Cuue his uni is bsed on Secions 9. & 9.3, Chpe 9. All ssigned edings nd execises e fom he exbook Objecies: Mke cein h you cn define, nd use in conex, he ems, conceps nd fomuls lised below:
More information5/17/2016. Study of patterns in the distribution of organisms across space and time
Old Fossils 5/17/2016 Ch.16-4 Evidnc of Evoluion Biogogphy Ag of Eh / Fossil cod Anomy / Embyology Biochmicls Obsving / Tsing NS fis-hnd Sudy of pns in h disibuion of ognisms coss spc nd im Includs obsvion
More informationApplications of these ideas. CS514: Intermediate Course in Operating Systems. Problem: Pictorial version. 2PC is a good match! Issues?
CS514: Inmi Co in Oing Sm Poo Kn imn K Ooki: T liion o h i O h h k h o Goi oool Dii monioing, h, n noiiion gmn oool, h 2PC n 3PC Unling hm: om hing n ong om o onin, om n mng ih k oi To, l look n liion
More informationChapter 2: Random Variables
Chp : ndom ibls.. Concp of ndom ibl.. Disibuion Funcions.. Dnsiy Funcions Funcions of ndom ibls.. n lus nd omns Hypgomic Disibuion.5. h Gussin ndom ibl Hisogms.. Dnsiy Funcions ld o Gussin.7. Oh obbiliy
More informationGet 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 informationAns: In the rectangular loop with the assigned direction for i2: di L dt , (1) where (2) a) At t = 0, i1(t) = I1U(t) is applied and (1) becomes
omewok # P7-3 ecngul loop of widh w nd heigh h is siued ne ve long wie cing cuen i s in Fig 7- ssume i o e ecngul pulse s shown in Fig 7- Find he induced cuen i in he ecngul loop whose self-inducnce is
More informationMotion. ( (3 dim) ( (1 dim) dt. Equations of Motion (Constant Acceleration) Newton s Law and Weight. Magnitude of the Frictional Force
Insucos: ield/mche PHYSICS DEPARTMENT PHY 48 Em Sepeme 6, 4 Nme pin, ls fis: Signue: On m hono, I he neihe gien no eceied unuhoied id on his eminion. YOUR TEST NUMBER IS THE 5-DIGIT NUMBER AT THE TOP O
More informationPath (space curve) Osculating plane
Fo th cuilin motion of pticl in spc th fomuls did fo pln cuilin motion still lid. But th my b n infinit numb of nomls fo tngnt dwn to spc cu. Whn th t nd t ' unit ctos mod to sm oigin by kping thi ointtions
More informationD zone schemes
Ch. 5. Enegy Bnds in Cysls 5.. -D zone schemes Fee elecons E k m h Fee elecons in cysl sinα P + cosα cosk α cos α cos k cos( k + π n α k + πn mv ob P 0 h cos α cos k n α k + π m h k E Enegy is peiodic
More informationChapter 8: Propagating Quantum States of Radiation
Quum Opcs f hcs Oplccs h R Cll Us Chp 8: p Quum Ss f R 8. lcmc Ms Wu I hs chp w wll cs pp quum ss f wus fs f spc. Cs h u shw lw f lcc wu. W ssum h h wu hs l lh qul h -c wll ssum l. Th lcc cs s fuc f l
More informationLECTURE 5. is defined by the position vectors r, 1. and. The displacement vector (from P 1 to P 2 ) is defined through r and 1.
LECTURE 5 ] DESCRIPTION OF PARTICLE MOTION IN SPACE -The displcemen, veloci nd cceleion in -D moion evel hei veco nue (diecion) houh he cuion h one mus p o hei sin. Thei full veco menin ppes when he picle
More informationErlkönig. t t.! t t. t t t tj "tt. tj t tj ttt!t t. e t Jt e t t t e t Jt
Gsng Po 1 Agio " " lkö (Compl by Rhol Bckr, s Moifi by Mrk S. Zimmr)!! J "! J # " c c " Luwig vn Bhovn WoO 131 (177) I Wr Who!! " J J! 5 ri ris hro' h spä h, I urch J J Nch rk un W Es n wil A J J is f
More informationSingle Correct Type. cos z + k, then the value of k equals. dx = 2 dz. (a) 1 (b) 0 (c)1 (d) 2 (code-v2t3paq10) l (c) ( l ) x.
IIT JEE/AIEEE MATHS y SUHAAG SIR Bhopl, Ph. (755)3 www.kolsss.om Qusion. & Soluion. In. Cl. Pg: of 6 TOPIC = INTEGRAL CALCULUS Singl Corr Typ 3 3 3 Qu.. L f () = sin + sin + + sin + hn h primiiv of f()
More information333 Ravenswood Avenue
O AL i D wy Bl o S kw y y ph Rwoo S ho P ol D b y D Pk n i l Co Sn lo Aipo u i R D Wil low R h R M R O g n Ex py i A G z S S Mi lf O H n n iv Po D R A P g M ill y xpw CA Licn No 01856608 Ex p wy R 203
More informationAxe 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 informationCh.4 Motion in 2D. Ch.4 Motion in 2D
Moion in plne, such s in he sceen, is clled 2-dimensionl (2D) moion. 1. Posiion, displcemen nd eloci ecos If he picle s posiion is ( 1, 1 ) 1, nd ( 2, 2 ) 2, he posiions ecos e 1 = 1 1 2 = 2 2 Aege eloci
More informationf(x) dx with An integral having either an infinite limit of integration or an unbounded integrand is called improper. Here are two examples dx x x 2
Impope Inegls To his poin we hve only consideed inegls f() wih he is of inegion nd b finie nd he inegnd f() bounded (nd in fc coninuous ecep possibly fo finiely mny jump disconinuiies) An inegl hving eihe
More informationELECTRIC VELOCITY SERVO REGULATION
ELECIC VELOCIY SEVO EGULAION Gorg W. Younkin, P.E. Lif FELLOW IEEE Indusril Conrols Consuling, Di. Bulls Ey Mrking, Inc. Fond du Lc, Wisconsin h prformnc of n lcricl lociy sro is msur of how wll h sro
More informationA 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 informationADORO TE DEVOTE (Godhead Here in Hiding) te, stus bat mas, la te. in so non mor Je nunc. la in. tis. ne, su a. tum. tas: tur: tas: or: ni, ne, o:
R TE EVTE (dhd H Hdg) L / Mld Kbrd gú s v l m sl c m qu gs v nns V n P P rs l mul m d lud 7 súb Fí cón ví f f dó, cru gs,, j l f c r s m l qum t pr qud ct, us: ns,,,, cs, cut r l sns m / m fí hó sn sí
More informationEuropean and American options with a single payment of dividends. (About formula Roll, Geske & Whaley) Mark Ioffe. Abstract
866 Uni Naions Plaza i 566 Nw Yo NY 7 Phon: + 3 355 Fa: + 4 668 info@gach.com www.gach.com Eoan an Amican oions wih a singl amn of ivins Abo fomla Roll Gs & Whal Ma Ioff Absac Th aicl ovis a ivaion of
More informationRevisiting what you have learned in Advanced Mathematical Analysis
Fourir sris Rvisiing wh you hv lrnd in Advncd Mhmicl Anlysis L f x b priodic funcion of priod nd is ingrbl ovr priod. f x cn b rprsnd by rigonomric sris, f x n cos nx bn sin nx n cos x b sin x cosx b whr
More informationExecutive Committee and Officers ( )
Gifted and Talented International V o l u m e 2 4, N u m b e r 2, D e c e m b e r, 2 0 0 9. G i f t e d a n d T a l e n t e d I n t e r n a t i o n a2 l 4 ( 2), D e c e m b e r, 2 0 0 9. 1 T h e W o r
More information(4) WALL MOUNTED DUPLEX NEMA 5-20R OUTLET AT 18" A.F.F. WIRED TO CIRCUIT NUMBER 4 WITHIN THE PANEL THAT SERVES THE RESIDENTIAL UNIT (4)
LIL ING LIS NI LN II K LIL SOLS IX. IL ONNION O H SVI SIH ILI ON SVI O ON NSO SIION 0.00 ovr St: ltril.00 rr loor ln uilin : ltril.0 irst loor ln uilin : ltril.0 Son loor ln uilin : ltril.0 ir & ourt loor
More informationENGR 1990 Engineering Mathematics The Integral of a Function as a Function
ENGR 1990 Engineering Mhemics The Inegrl of Funcion s Funcion Previously, we lerned how o esime he inegrl of funcion f( ) over some inervl y dding he res of finie se of rpezoids h represen he re under
More informationPHYSICS 1210 Exam 1 University of Wyoming 14 February points
PHYSICS 1210 Em 1 Uniersiy of Wyoming 14 Februry 2013 150 poins This es is open-noe nd closed-book. Clculors re permied bu compuers re no. No collborion, consulion, or communicion wih oher people (oher
More informatione t dt e t dt = lim e t dt T (1 e T ) = 1
Improper Inegrls There re wo ypes of improper inegrls - hose wih infinie limis of inegrion, nd hose wih inegrnds h pproch some poin wihin he limis of inegrion. Firs we will consider inegrls wih infinie
More informationPartial Fraction Expansion
Paial Facion Expanion Whn ying o find h inv Laplac anfom o inv z anfom i i hlpfl o b abl o bak a complicad aio of wo polynomial ino fom ha a on h Laplac Tanfom o z anfom abl. W will illa h ing Laplac anfom.
More informationReinforcement learning
CS 75 Mchine Lening Lecue b einfocemen lening Milos Huskech milos@cs.pi.edu 539 Senno Sque einfocemen lening We wn o len conol policy: : X A We see emples of bu oupus e no given Insed of we ge feedbck
More information2D Motion WS. A horizontally launched projectile s initial vertical velocity is zero. Solve the following problems with this information.
Nme D Moion WS The equions of moion h rele o projeciles were discussed in he Projecile Moion Anlsis Acii. ou found h projecile moes wih consn eloci in he horizonl direcion nd consn ccelerion in he ericl
More informationChapter 1 Basic Concepts
Ch Bsc Cocs oduco od: X X ε ε ε ε ε O h h foog ssuos o css ε ε ε ε ε N Co No h X Chcscs of od: cos c ddc (ucod) d s of h soss dd of h ssocd c S qusos sd: Wh f h cs of h soss o cos d dd o h ssocd s? Wh
More informationC-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 informationPhysic 231 Lecture 4. Mi it ftd l t. Main points of today s lecture: Example: addition of velocities Trajectories of objects in 2 = =
Mi i fd l Phsic 3 Lecure 4 Min poins of od s lecure: Emple: ddiion of elociies Trjecories of objecs in dimensions: dimensions: g 9.8m/s downwrds ( ) g o g g Emple: A foobll pler runs he pern gien in he
More informationStudy of Tyre Damping Ratio and In-Plane Time Domain Simulation with Modal Parameter Tyre Model (MPTM)
Sudy o Ty Damping aio and In-Plan Tim Domain Simulaion wih Modal Paam Ty Modl (MPTM D. Jin Shang, D. Baojang Li, and Po. Dihua Guan Sa Ky Laboaoy o Auomoiv Say and Engy, Tsinghua Univsiy, Bijing, China
More informationRIM= City-County Building, Suite 104 NE INV= Floor= CP #CP004 TOP SE BOLT LP BASE N= E= ELEV=858.
f g c ch c y f M D b c Dm f ubc Wk x c M f g 23 IM=3. y-uy ug, u 0 N INV=0.0 F=0.99 20 M uh Kg, J. v. M, WI 303 h ch b b y v #00 O O O O N=93.200 =2920.00 ckby vyb FG2 f g Ghc c c c 03000 W FI ND O 9 0
More information(b) 10 yr. (b) 13 m. 1.6 m s, m s m s (c) 13.1 s. 32. (a) 20.0 s (b) No, the minimum distance to stop = 1.00 km. 1.
Answers o Een Numbered Problems Chper. () 7 m s, 6 m s (b) 8 5 yr 4.. m ih 6. () 5. m s (b).5 m s (c).5 m s (d) 3.33 m s (e) 8. ().3 min (b) 64 mi..3 h. ().3 s (b) 3 m 4..8 mi wes of he flgpole 6. (b)
More information6. Gas dynamics. Ideal gases Speed of infinitesimal disturbances in still gas
6. Gs dynmics Dr. Gergely Krisóf De. of Fluid echnics, BE Februry, 009. Seed of infiniesiml disurbnces in sill gs dv d, dv d, Coninuiy: ( dv)( ) dv omenum r r heorem: ( ( dv) ) d 3443 4 q m dv d dv llievi
More informationDSP-First, 2/e. This Lecture: LECTURE #3 Complex Exponentials & Complex Numbers. Introduce more tools for manipulating complex numbers
DSP-Fis, / LECTURE #3 Compl Eponnials & Compl umbs READIG ASSIGMETS This Lcu: Chap, Scs. -3 o -5 Appndi A: Compl umbs Appndi B: MATLAB Lcu: Compl Eponnials Aug 016 003-016, JH McClllan & RW Schaf 3 LECTURE
More informationTHIS PAGE DECLASSIFIED IAW EO 12958
L " ^ \ : / 4 a " G E G + : C 4 w i V T / J ` { } ( : f c : < J ; G L ( Y e < + a : v! { : [ y v : ; a G : : : S 4 ; l J / \ l " ` : 5 L " 7 F } ` " x l } l i > G < Y / : 7 7 \ a? / c = l L i L l / c f
More informationIntroduction to Inertial Dynamics
nouon o nl Dn Rz S Jon Hokn Unv Lu no on uon of oon of ul-jon oo o onl W n? A on of o fo ng on ul n oon of. ou n El: A ll of l off goun. fo ng on ll fo of gv: f-g g9.8 /. f o ll, n : f g / f g 9.8.9 El:
More informationFourier. Continuous time. Review. with period T, x t. Inverse Fourier F Transform. x t. Transform. j t
Coninuous im ourir rnsform Rviw. or coninuous-im priodic signl x h ourir sris rprsnion is x x j, j 2 d wih priod, ourir rnsform Wh bou priodic signls? W willl considr n priodic signl s priodic signl wih
More informationThe model proposed by Vasicek in 1977 is a yield-based one-factor equilibrium model given by the dynamic
h Vsick modl h modl roosd by Vsick in 977 is yild-bsd on-fcor quilibrium modl givn by h dynmic dr = b r d + dw his modl ssums h h shor r is norml nd hs so-clld "mn rvring rocss" (undr Q. If w u r = b/,
More informationGUIDE FOR SUPERVISORS 1. This event runs most efficiently with two to four extra volunteers to help proctor students and grade the student
GUIDE FOR SUPERVISORS 1. This vn uns mos fficinly wih wo o fou xa voluns o hlp poco sudns and gad h sudn scoshs. 2. EVENT PARAMETERS: Th vn supviso will povid scoshs. You will nd o bing a im, pns and pncils
More informationFaraday s Law. To be able to find. motional emf transformer and motional emf. Motional emf
Objecie F s w Tnsfome Moionl To be ble o fin nsfome. moionl nsfome n moionl. 331 1 331 Mwell s quion: ic Fiel D: Guss lw :KV : Guss lw H: Ampee s w Poin Fom Inegl Fom D D Q sufce loop H sufce H I enclose
More informationToday - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations
Today - Lecue 13 Today s lecue coninue wih oaions, oque, Noe ha chapes 11, 1, 13 all inole oaions slide 1 eiew Roaions Chapes 11 & 1 Viewed fom aboe (+z) Roaional, o angula elociy, gies angenial elociy
More informationScience Advertisement Intergovernmental Panel on Climate Change: The Physical Science Basis 2/3/2007 Physics 253
Science Adeisemen Inegoenmenl Pnel on Clime Chnge: The Phsicl Science Bsis hp://www.ipcc.ch/spmfeb7.pdf /3/7 Phsics 53 hp://www.fonews.com/pojecs/pdf/spmfeb7.pdf /3/7 Phsics 53 3 Sus: Uni, Chpe 3 Vecos
More informationa dt a dt a dt dt If 1, then the poles in the transfer function are complex conjugates. Let s look at f t H t f s / s. So, for a 2 nd order system:
Undrdamd Sysms Undrdamd Sysms nd Ordr Sysms Ouu modld wih a nd ordr ODE: d y dy a a1 a0 y b f If a 0 0, hn: whr: a d y a1 dy b d y dy y f y f a a a 0 0 0 is h naural riod of oscillaion. is h daming facor.
More informationFourier Series and Parseval s Relation Çağatay Candan Dec. 22, 2013
Fourir Sris nd Prsvl s Rlion Çğy Cndn Dc., 3 W sudy h m problm EE 3 M, Fll3- in som dil o illusr som conncions bwn Fourir sris, Prsvl s rlion nd RMS vlus. Q. ps h signl sin is h inpu o hlf-wv rcifir circui
More informationGRADE 2 SUPPLEMENT. Set D6 Measurement: Temperature. Includes. Skills & Concepts
GRADE 2 SUPPLEMENT S D6 Msn: Tp Inlds Aiviy 1: Wh s h Tp? D6.1 Aiviy 2: Hw Ds h Tp Chng Ding h Dy? D6.5 Aiviy 3: Fs & Al Tps n Th D6.9 Skills & Cnps H d h gh d P201304 Bidgs in Mhis Gd 2 Sppln S D6 Msn:
More informationMath 266, Practice Midterm Exam 2
Mh 66, Prcic Midrm Exm Nm: Ground Rul. Clculor i NOT llowd.. Show your work for vry problm unl ohrwi d (pril crdi r vilbl). 3. You my u on 4-by-6 indx crd, boh id. 4. Th bl of Lplc rnform i vilbl h l pg.
More information176 5 t h Fl oo r. 337 P o ly me r Ma te ri al s
A g la di ou s F. L. 462 E l ec tr on ic D ev el op me nt A i ng er A.W.S. 371 C. A. M. A l ex an de r 236 A d mi ni st ra ti on R. H. (M rs ) A n dr ew s P. V. 326 O p ti ca l Tr an sm is si on A p ps
More informationAverage & instantaneous velocity and acceleration Motion with constant acceleration
Physics 7: Lecure Reminders Discussion nd Lb secions sr meeing ne week Fill ou Pink dd/drop form if you need o swich o differen secion h is FULL. Do i TODAY. Homework Ch. : 5, 7,, 3,, nd 6 Ch.: 6,, 3 Submission
More information1 Lecture: pp
EE334 - Wavs and Phasos Lcu: pp -35 - -6 This cous aks vyhing ha you hav bn augh in physics, mah and cicuis and uss i. Easy, only nd o know 4 quaions: 4 wks on fou quaions D ρ Gauss's Law B No Monopols
More informationOH 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 informationMathcad Lecture #4 In-class Worksheet Vectors and Matrices 1 (Basics)
Mh Lr # In-l Workh Vor n Mri (Bi) h n o hi lr, o hol l o: r mri n or in Mh i mri prorm i mri mh oprion ol m o linr qion ing mri mh. Cring Mri Thr r rl o r mri. Th "Inr Mri" Wino (M) B K Poin Rr o
More informationEngine Thrust. From momentum conservation
Airbrhing Propulsion -1 Airbrhing School o Arospc Enginring Propulsion Ovrviw w will b xmining numbr o irbrhing propulsion sysms rmjs, urbojs, urbons, urboprops Prormnc prmrs o compr hm, usul o din som
More informationDerivative Securities: Lecture 4 Introduction to option pricing
Divaiv cuiis: Lcu 4 Inoducion o oion icing oucs: J. Hull 7 h diion Avllanda and Launc () Yahoo!Financ & assod wbsis Oion Picing In vious lcus w covd owad icing and h imoanc o cos-o cay W also covd Pu-all
More informationOn the Speed of Heat Wave. Mihály Makai
On h Spd of Ha Wa Mihály Maai maai@ra.bm.hu Conns Formulaion of h problm: infini spd? Local hrmal qulibrium (LTE hypohsis Balanc quaion Phnomnological balanc Spd of ha wa Applicaion in plasma ranspor 1.
More information5.1-The Initial-Value Problems For Ordinary Differential Equations
5.-The Iniil-Vlue Problems For Ordinry Differenil Equions Consider solving iniil-vlue problems for ordinry differenil equions: (*) y f, y, b, y. If we know he generl soluion y of he ordinry differenil
More information16.512, Rocket Propulsion Prof. Manuel Martinez-Sanchez Lecture 3: Ideal Nozzle Fluid Mechanics
6.5, Rok ropulsion rof. nul rinz-snhz Lur 3: Idl Nozzl luid hnis Idl Nozzl low wih No Sprion (-D) - Qusi -D (slndr) pproximion - Idl gs ssumd ( ) mu + Opimum xpnsion: - or lss, >, ould driv mor forwrd
More informationMEM 355 Performance Enhancement of Dynamical Systems A First Control Problem - Cruise Control
MEM 355 Prformanc Enhancmn of Dynamical Sysms A Firs Conrol Problm - Cruis Conrol Harry G. Kwany Darmn of Mchanical Enginring & Mchanics Drxl Univrsiy Cruis Conrol ( ) mv = F mg sinθ cv v +.2v= u 9.8θ
More informationElementary Differential Equations and Boundary Value Problems
Elmnar Diffrnial Equaions and Boundar Valu Problms Boc. & DiPrima 9 h Ediion Chapr : Firs Ordr Diffrnial Equaions 00600 คณ ตศาสตร ว ศวกรรม สาขาว ชาว ศวกรรมคอมพ วเตอร ป การศ กษา /55 ผศ.ดร.อร ญญา ผศ.ดร.สมศ
More informationEquations 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 informationSAMPLE LITANY OF THE SAINTS E/G. Dadd9/F. Aadd9. cy. Christ, have. Lord, have mer cy. Christ, have A/E. Dadd9. Aadd9/C Bm E. 1. Ma ry and. mer cy.
LTNY OF TH SNTS Cntrs Gnt flwng ( = c. 100) /G Ddd9/F ll Kybrd / hv Ddd9 hv hv Txt 1973, CL. ll rghts rsrvd. Usd wth prmssn. Musc: D. Bckr, b. 1953, 1987, D. Bckr. Publshd by OCP. ll rghts rsrvd. SMPL
More informationChapter 11: Matter-Photon Interactions and Cavity Quantum Electrodynamics
Quu Ocs f Phcs Olccs h Cll Usy Ch : M-Ph Ics Cy Quu lcycs. A S-Clsscl Ach Pcl-l Ics I hs Ch w wll s uu hy f h cs bw ch cls lcc fl. P hl f h u c lcs wll b cssy l ssbl hy. Yu h s Ch 5 h h ss wy uz s fs chs
More informationChapter 10. Simple Harmonic Motion and Elasticity. Goals for Chapter 10
Chper 0 Siple Hronic Moion nd Elsiciy Gols or Chper 0 o ollow periodic oion o sudy o siple hronic oion. o sole equions o siple hronic oion. o use he pendulu s prooypicl syse undergoing siple hronic oion.
More informationAddition & Subtraction of Polynomials
Addiion & Sucion of Polynomil Addiion of Polynomil: Adding wo o moe olynomil i imly me of dding like em. The following ocedue hould e ued o dd olynomil 1. Remove enhee if hee e enhee. Add imil em. Wie
More informationCircuits 24/08/2010. Question. Question. Practice Questions QV CV. Review Formula s RC R R R V IR ... Charging P IV I R ... E Pt.
4/08/00 eview Fomul s icuis cice s BL B A B I I I I E...... s n n hging Q Q 0 e... n... Q Q n 0 e Q I I0e Dischging Q U Q A wie mde of bss nd nohe wie mde of silve hve he sme lengh, bu he dimee of he bss
More informationNEWBERRY FOREST MGT UNIT Stand Level Information Compartment: 10 Entry Year: 2001
iz oy- kg vg. To. 1 M 6 M 10 11 100 60 oh hwoo uvg N o hul 0 Mix bg. woo, moly low quliy. Coif ompo houghou - WP/hmlok/pu/blm/. vy o whi pi o h ouh fig of. iffiul o. Th o hi i o PVT l wh h g o wll big
More informationMinimum Squared Error
Minimum Squred Error LDF: Minimum Squred-Error Procedures Ide: conver o esier nd eer undersood prolem Percepron y i > 0 for ll smples y i solve sysem of liner inequliies MSE procedure y i i for ll smples
More informationThermal Stresses of Semi-Infinite Annular Beam: Direct Problem
iol ol o L choloy i Eii M & Alid Scic LEMAS Vol V Fy 8 SSN 78-54 hl S o Si-ii Al B: Dic Pol Viv Fl M. S. Wh d N. W. hod 3 D o Mhic Godw Uiviy Gdchioli M.S di D o Mhic Svody Mhvidyly Sidwhi M.S di 3 D o
More informationBoyce/DiPrima 9 th ed, Ch 2.1: Linear Equations; Method of Integrating Factors
Boc/DiPrima 9 h d, Ch.: Linar Equaions; Mhod of Ingraing Facors Elmnar Diffrnial Equaions and Boundar Valu Problms, 9 h diion, b William E. Boc and Richard C. DiPrima, 009 b John Wil & Sons, Inc. A linar
More informationChapter 5 The Laplace Transform. x(t) input y(t) output Dynamic System
EE 422G No: Chapr 5 Inrucor: Chung Chapr 5 Th Laplac Tranform 5- Inroducion () Sym analyi inpu oupu Dynamic Sym Linar Dynamic ym: A procor which proc h inpu ignal o produc h oupu dy ( n) ( n dy ( n) +
More informationrig T h e y plod vault with < abort Ve i waiting for nj tld arrivi distant friend To whom wondering gram?" "To James Boynton." worded?
G F F C OL 7 ^ 6 O D C C G O U G U 5 393 CLLD C O LF O 93 =3 O x x [ L < «x -?" C ; F qz " " : G! F C? G C LUC D?"! L G C O O ' x x D D O - " C D F O LU F L O DOGO OGL C D CUD C L C X ^ F O : F -?! L U
More informationA study Of Salt-Finger Convection In a Nonlinear Magneto-Fluid Overlying a Porous Layer Affected By Rotation
Innion on o Mchnic & Mchonic Engining IMME-IEN Vo: No: A O -ing Concion In Nonin Mgno-i Oing oo Ac Roion M..A-hi Ac hi o in -ing concion in o o nonin gno-i oing oo c oion. o in h i i gon Ni-o qion n in
More informationA New Model for the Pricing of Defaultable Bonds
A Nw Mol fo h Picing of Dflbl Bon Pof. D. Ri Zg Mnich Univiy of chnology Mi 6. Dzmb 004 HVB-Ini fo Mhmicl Finnc A Nw Mol fo h Picing of Dflbl Bon Ovviw Mk Infomion - Yil Cv Bhvio US y Sip - Ci Sp Bhvio
More informationEmigration The movement of individuals out of an area The population decreases
Nm Clss D C 5 Puls S 5 1 Hw Puls Gw (s 119 123) Ts s fs ss us sb ul. I ls sbs fs ff ul sz xls w xl w ls w. Css f Puls ( 119) 1. W fu m ss f ul?. G sbu. Gw b. Ds. A suu 2. W s ul s sbu? I s b b ul. 3. A
More informationSYMMETRICAL COMPONENTS
SYMMETRCA COMPONENTS Syl oponn llow ph un of volg n un o pl y h p ln yl oponn Con h ph ln oponn wh Engy Convon o 4 o o wh o, 4 o, 6 o Engy Convon SYMMETRCA COMPONENTS Dfn h opo wh o Th o of pho : pov ph
More informationCHAPTER 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 informationSliding mode control of nonlinear SISO systems with both matched and unmatched disturbances
Innionl Jounl of cincs nd Tchniqus of Auomic conol compu ngining IJ-TA, Volum, N, July 008, pp. 5067. liding mod conol of nonlin IO sysms wih boh mchd nd unmchd disubncs. Mhiddin Mhmoud, L. Chifi-Aloui,
More informationC o r p o r a t e l i f e i n A n c i e n t I n d i a e x p r e s s e d i t s e l f
C H A P T E R I G E N E S I S A N D GROWTH OF G U IL D S C o r p o r a t e l i f e i n A n c i e n t I n d i a e x p r e s s e d i t s e l f i n a v a r i e t y o f f o r m s - s o c i a l, r e l i g i
More informationRUTH. land_of_israel: the *country *which God gave to his people in the *Old_Testament. [*map # 2]
RUTH 1 Elimlk g ln M 1-2 I in im n ln Irl i n *king. Tr r lr rul ln. Ty r ug. Tr n r l in Ju u r g min. Elimlk mn y in n Blm in Ju. H i nm Nmi. S n Elimlk 2 *n. Tir nm r Mln n Kilin. Ty r ll rm Er mily.
More information7 Wave Equation in Higher Dimensions
7 Wave Equaion in Highe Dimensions We now conside he iniial-value poblem fo he wave equaion in n dimensions, u c u x R n u(x, φ(x u (x, ψ(x whee u n i u x i x i. (7. 7. Mehod of Spheical Means Ref: Evans,
More information