An Enhanced Performance PID Filter Controller for First Order Time Delay Processes
|
|
- Luke Barber
- 6 years ago
- Views:
Transcription
1 Jounal of Chial Engining of Jaan, Vol. 4, No. 6,., 7 ah Pa An Enhand Pfoan PID Filt Contoll fo Fit Od Ti Dlay Po Mohaad SHAMSUZZOHA and Moonyong LEE Shool of Chial Engining and Thnology, Yungna Univity, Da-dong 4-, Kyongan 7-749, Koa Kywod: PID Contoll Tuning, Fit Od Plu Dad Ti Po, Dituban jtion, Fit Od Lad/Lag Filt, Two-Dg-of-Fdo Contoll An analytial tuning thod fo a PID ontoll aadd with a lad/lag filt i ood fo FOPDT o bad on th IMC dign inil. Th ontoll i dignd fo th jtion of dituban and a two-dg-of-fdo ontol tutu i ud to lakn th ovhoot in th t-oint on. Th iulation tudy how that th ood dign thod ovid btt dituban jtion than th onvntional PID dign thod whn th ontoll a tund to hav th a dg of obutn. A guidlin of a ingl tuning aat of lod-loo ti ontant (λ) i ovidd fo val diffnt obutn lvl. Intodution Pootional intgal divativ (PID) ontoll hav bn th ot oula and widly ud ontoll in th o induti bau of thi iliity, obutn and wid ang of aliability with na-otial foan. Howv, it ha bn notid that any PID ontoll a oftn ooly tund and a tain aount of ffot ha bn ad to ytatially olv thi obl. Th fftivn of th intnal odl ontol (IMC) dign inil ha ad it attativ in th o induti, wh any attt hav bn ad to xloit th IMC inil to dign PID ontoll fo both tabl and untabl o (Moai and Zafiiou, 989). Th IMC-PID tuning ul hav th advantag of uing only a ingl tuning aat to ahiv a la tad-off btwn th lod-loo foan and obutn. Th PID tuning thod ood by iva t al. (986), Moai and Zafiiou (989), Hon t al. (996), and L t al. (998) a tyial xal of th IMC-PID tuning thod. Th dit ynthi (DS) thod ood by Sith t al. (975) and th dit ynthi fo th dituban (DSd) thod ood by Chn and Sbog () an alo b atgoizd into th a la a th IMC- PID thod, in that thy obtain th PID ontoll aat by outing th idal fdbak ontoll whih giv a dfind did lod-loo on. Although th idal ontoll i oftn o oliatd than th PID ontoll fo ti dlayd ivd on Novb 7, 6; atd on Fbuay 5, 7. Coondn onning thi atil hould b addd to M. L (E-ail add: ynl@yu.a.k). o, th ontoll fo an b dud to that of ith a PID ontoll o a PID ontoll aadd with a low od filt by foing aoiat aoxiation of th dad ti in th o odl. Th ontol foan an b ignifiantly nhand by aading th PID ontoll with a lad/ lag filt, a givn by Eq. (). a K D + τ τ + b I () wh K, τ I and τ D a th ootional gain, intgal ti ontant, and divativ ti ontant of th PID ontoll, tivly, and a and b a th filt aat. Th tutu of th PID ontoll aadd with a filt wa alo uggtd by iva t al. (986), Moai and Zafiiou (989), Hon t al. (996), L t al. (998) and Dwy (3). Th PID filt ontoll in Eq. () an aily b ilntd in odn ontol hadwa. It i ntial to haiz that th PID ontoll dignd aoding to th IMC inil ovid xllnt t-oint taking, but ha a luggih dituban on, ially fo o with a all ti-dlay/ti-ontant atio (Moai and Zafiiou, 989; Chin and Fuhauf, 99; Hon t al., 996; L t al., 998; Chn and Sbog, ; Skogtad, 3). Sin dituban jtion i uh o iotant than t-oint taking fo any o ontol aliation, a ontoll dign that haiz th fo ath than th latt i an iotant dign goal that ha ntly bn th fou of nwd ah. Coyight 7 Th Soity of Chial Engin, Jaan
2 (a) wh i th otion of th odl invtd by th ontoll, A i th otion of th odl not invtd by th ontoll and A (). Th noninvtibl at uually inlud th dad ti and/o ight half lan zo and i hon to b all-a. To obtain a good on fo o with ol na zo, th IMC ontoll q hould b dignd to atify th following ondition.. If th o P ha ol na zo at z, z,..., z, thn q hould hav zo at z, z,..., z.. If th o D ha ol na zo, z d, z d,..., z d, thn ( P q) hould hav zo at z d, z d,..., z d. Sin th IMC ontoll q i dignd a q f, th fit ondition i atifid autoatially. Th ond ondition an b fulfilld by digning th IMC filt f a Fig. (b) Blok diaga of IMC and laial fdbak ontol yt: (a) Th IMC tutu; (b) Fdbak ontol tutu i β i + i f ( λ + ) ( 4) wh λ i an adjutabl aat whih ontol th tadoff btwn th foan and obutn; i ltd to b lag nough to ak th IMC ontoll (i-)o; β i a dtind by Eq. (5) to anl th ol na zo in D. In th nt tudy, a il and ffiint thod i ood fo th dign of a PID filt ontoll with nhand foan. A lod-loo ti ontant (λ) guidlin i ondd fo a wid ang of ti-dlay/ti-ontant atio. A iulation tudy wa fod to illutat th uioity of th ood thod fo both noinal and tubd o.. IMC Contoll Dign Podu Figu (a) and (b) how th blok diaga of th IMC ontol and quivalnt laial fdbak ontol tutu, tivly, wh P i th o, P th o odl, q th IMC ontoll, f th toint filt, and th quivalnt fdbak ontoll. Fo th noinal a (i.., P P ), th t-oint and dituban on in th IMC ontol tutu an b ilifid a: y q+ q d P P D Aoding to th IMC aatization (Moai and Zafiiou, 989), th o odl P i fatod into two at: () 3 P A q P zd, L, zd i A βi + i ( λ + ) Thn, th IMC ontoll o to b q i i β + ( λ + ) i Thu, th lod-loo on i y A i βi + i + ( λ + ) A zd, L, zd ( 5) ( 6) i βi + i d D 7 ( λ + ) Fo th abov dign odu, on an ahiv a tabl lod-loo on by uing th IMC ontoll.. PID filt Contoll Dign fo FOPDT Po Th idal fdbak ontoll that i quivalnt to th IMC ontoll an b xd in t of th intnal odl P and th IMC ontoll q: JOUNAL OF CHEMICAL ENINEEIN OF JAPAN
3 q () 8 q P Subtituting Eq. (3) and (6) into Eq. (8) giv th idal fdbak ontoll: i βi + i ( λ + ) i A βi + i ( λ + ) ( 9) Lt u onid th fit od lu dad ti (FOPDT) o, whih i ot widly utilizd in th hial o induti, a a ntativ odl. P θ K D τ + wh K i th gain, τ th ti ontant, and θ th ti dlay. Th IMC filt tutu i f β + λ + It i notid that th IMC filt fo in Eq. () wa alo utilizd by L t al. (998) and Hon t al. (996). Th ulting IMC ontoll bo q ( τ+ ) ( β+ ) K( λ+ ) Thfo, th idal fdbak ontoll i obtaind a ( + ) ( + ) τ+ β θ K λ+ β [ ] ( 3) Sin th idal fdbak ontoll in Eq. (3) do not hav th PID filt ontoll fo, th aining iu i how to dign th PID filt ontoll that aoxiat th idal fdbak ontoll ot loly. Aoxiating th dad ti θ with a / Pad xanion θ θ θ + θ θ ( 4) ult in C a ( + ) + θ + θ τ ( β + ) θ θ θ θ K ( λ+ ) ( β + ) + ( 5) It i iotant to not that th / Pad aoxiation i i nough to onvt th idal fdbak ontoll into a finit dinional fdbak ontoll with baly any lo of auay. Exanding and aanging Eq. (5) giv θ θ ( τ+ ) β+ βθ + λθ + λ K( λ β + θ) + λ β + θ βθ λθ λ θ λθ λ β + θ λ β + θ 3 (6) A n in Eq. (6), th ulting ontoll ha th fo of th PID ontoll aadd with a high od filt. Th analytial PID foula an b obtaind a K θ θ θ, τ, τ ( 7) K λ β + θ 6 I D Th valu of th xta dg of fdo β i ltd o that it anl out th on-loo ol at /τ that au a luggih on to load dituban. Fo Eq. (5), thi qui [ (β + ) θ /(λ + ) ] /τ. Thu, th valu of β i obtaind a λ θτ β τ τ ( 8) Futho, it i obviou fo Eq. (5) that th aining at of th dnoinato in Eq. (6) ontain th fato (τ + ). Thfo, th filt aat b in Eq. () an b obtaind by taking th fit divativ of Eq. (9) blow + b + βθ βθ λθ λ θ λθ + λθ + λ λ β + θ λ β + θ λ β + θ τ + (9) VOL. 4 NO
4 and ubtituting a βθ + λθ + λ b τ λ β + θ Th filt aat in Eq. () an b aily obtaind fo Eq. (6) a a β Sin th high od t ha littl iat on th ovall ontol foan in th ontol lvant fquny ang, th aining at of th fation in Eq. (6) an b ufully aoxiatd to a il fit od lad/lag filt a ( + a)/( + b). Ou iulation ult (although not hown in thi a) alo onfi th validity of thi odl dution. Th lad t (β + ) in th lod-loo tanf funtion of Eq. (7) au xiv ovhoot in th t-oint on, whih an b adiatd by adding th t-oint filt f a: f γβ + β + wh γ. Th xt a with γ ha no lad t in th t-oint filt whih would au a low vo on. On th oth hand, γ an that th i no t-oint filt. γ an b adjutd onlin to obtain th did d of th t-oint on. Th ood tudy i alo aliabl to th o with ngligibl dad ti whil it i ainly foud on th fit od ti dlay o. 3. obut Stability Sin η q f fo th IMC ontoll, th ulting Eq. (4) bo: fl ( ω) < ω ( 5) Thu, th abov tho an b inttd a l < / η / f, whih guaant obut tability whn th ultiliativ odl o i boundd by () l. η () () < ( 6) wh () dfin th o ultiliativ untainty bound. i.., () ( )/. Thi untainty bound an b utilizd to nt th odl dution o, o inut atuato untainty, and o outut no untainty, t., whih a vy fqunt in th atual o lant. Fo th FOPDT o, th olntay nitivity funtion η () an b obtaind a η () ( β+ ) ( λ + ) θ ( 7) Subtituting Eq. (7) and β into Eq. (6) yild th obut tability ontaint quid fo tuning th adjutabl aat λ λ θτ τ τ + λ + < () Subtituting iω into Eq. (8) ult in ( 8) Th wll-known obut tability tho an b utilizd to analyz th obut tability of th ood ontoll. obut Stability Tho (Moai and Zafiou, 989): Lt u au that all lant P in th faily λ θτ τ ω τ + λω + < ιω ( 9) i i ω ω < : l ω 3 ( iω) hav th a nub of HP ol and that a atiula ontoll tabiliz th noinal lant. Thn, th yt i obutly tabl with th ontoll if and only if th olntay nitivity funtion η fo th noinal lant atifi th following bound: ηl u ηl ( ω ) < ( 4) ω It i oibl fo untainty to ou in any of th th o aat i.., θ, τ, and K. Conquntly, w hav to onid th untainty in th diffnt aat aatly. Lt u onid th FOPDT o having th untainty in all th aat a ( θ+ θ) K K ( + ) τ+ τ ( + ) ( 3) It i ot oon ati that th FOPDT odl aoxiatd fo th high od o in th al 4 JOUNAL OF CHEMICAL ENINEEIN OF JAPAN
5 o lant. Du to thi fo th ti ontant untainty it i aud that th all ti ontant τ i ngltd/iing in dvloing th noinal odl a onidd in Eq. (3) (Sbog t al., 4). Thn th o ultiliativ untainty bound bo K + K () τ + θ ( 3) Subtituting th abov ult into Eq. (9), w obtain th obut tability ontaint a follow: λ θτ τ ω θω τ + K + < K i, λω + τω i + ω > ( 3) Th abov obut tability ontaint i vy uful to adjut λ wh th i untainty in th o aat. Th obut tability ontaint in Eq. (3) an alo b ud to dtin th axiu allowabl valu of untainty in ± K, ± θ and ± τ o vaiou obination of th fo whih obut tability an b guaantd. Fo xal, a lot of η (ω) l (ω) v. ω an b ontutd fo a all valu of any aati untainty and/o obination of diffnt untainti. 4. Siulation Study Thi tion dal with th iulation tudy ondutd fo th ntativ FOPDT o: th lag ti doinant o, th qual dad ti and lag ti o, and th dad ti doinant o. To valuat th obutn of a ontol yt, th axiu nitivity, M, whih i dfind by M ax /[ + (iω)], i ud. Sin th M i th inv of th hott ditan fo th Nyquit uv of th loo tanf funtion to th itial oint (, ), a all M valu indiat that th tability agin of th ontol yt i lag. Th M i a wllknown obutn au and i ud by any ah (Skogtad and Potlthwait, 996; Åtö t al., 998; Chn and Sbog, ; Skogtad, 3). Tyial valu of M a in th ang of.. (Åtö t al., 998; Sbog t al., 4). To nu a fai oaion, it i widly atd fo th odlbad ontoll (, DS, and IMC) to tun by adjuting λ o that th M valu bo th a valu. Thfo, thoughout all ou iulation xal, all of th ontoll oad w dignd to hav th a obutn lvl in t of th axiu nitivity, M. To valuat th lod-loo foan, two foan indi w onidd in th a of both a t t-oint hang and a t load dituban, viz., th intgal of th ti-wightd abolut o (ITAE) dfind by ITAE t (t) dt, and th ovhoot whih at a a au of how uh th on xd th ultiat valu following a t hang in th toint and/o dituban. In thi a, th iulation tudy ha bn ondutd uing th PID ontoll in th fo of Eq. (). Howv, fo al ilntation, th aalll fo of th PID ontoll, () K { + /(τ I ) + τ D / [(.τ D ) + ]}( + a)/( + b), whih i widly ud in th al o, an b alid to aoxiatly th a foan. To valuat th uag of aniulatd inut valu, w out TV of th inut u(t), whih i th u of all of it ovnt of u and down. If w ditiz th inut ignal a a qun [u, u, u 3,..., u i,...], thn TV i u i+ u i hould b a all a oibl. TV i a good au of th oothn of a ignal (Skogtad and Potlthwait, 996; Chn and Sbog, ; Skogtad, 3). 4. Exal : Lag ti doinant o (θ/τ.) Conid th following FOPDT o (Chn and Sbog, ; Sbog t al., 4): D + ( 33) Th ood PID filt ontoll i oad with oth ontoll bad on xiting thod, uh a th thod, and tho ood by iva t al. (986), Hon t al. (996), L t al. (998) and L t al. (998) with a onvntional filt. Th ontoll aat, inluding th foan and obutn atix, a litd in Tabl. In od to nu a fai oaion, all of th ontoll oad a tund to hav M.94 by adjuting λ. Figu oa th t-oint and load on obtaind uing th ood thod, th thod, and th thod ood by L t al. (998) and Hon t al. (996). Th DOF ontoll uing th t-oint filt wa ud in th thod and th thod ood by L t al. (998) and Hon t al. (996) to obtain an nhand t-oint on. It i iotant to not that th t-oint filt ud fo th t-oint on ha a la bnfit whn th o i lag ti doinant. In thi a, it i obvd that.4 γ giv ooth and obut ontol foan. In th ood ontoll, γ in th t-oint filt i ltd a γ.45. Th lod-loo on fo both th t-oint taking and dituban jtion ignifi that th ood thod ovid a uio on fo th a obutn. VOL. 4 NO
6 Tabl PID ontoll aat and foan atix fo xal (θ/τ.) Tuning thod λ K τ I τ D St-oint Dituban ITAE Ovhoot TV ITAE Ovhoot TV Pood thod a L t al. (998) b Hon t al. (996) d iva t al. (986) L t al. (998) f a a K D + τ, wh a 3., b.39; f τ + b I b f f a d K D + τ, wh a 4.3, b.,.34; f τ + b + I K D τ, wh b.45 τ + b I f Th L t al. (998) thod bad on th onvntional IMC filt fo of f /(λ + ) *DOF ontoll i ud only fo th thod of iva t al. (986) and L t al. (998) f (a) Po vaiabl Po vaiabl Pood thod L t al. (998). Hon t al. (996) Ti [in] 9 5 (b) Pood thod L t al. (998) Hon t al. (996) Ti [in] Fig. Siulation ult fo xal Th obut foan i valuatd by inting a tubation untainty of % in all th aat in th wot dition iultanouly and finding th atual o a D. /(8 + ). Th iulation ult fo th odl iath fo vaiou thod a givn in Tabl. Th foan and obutn indi obviouly dontat that th ood thod ha o obut foan than th oth. 4. Exal : Equal lag ti and dad ti o (θ/τ ) Conid th o odl dibd by Chn and Sbog () a follow D + ( 34) 6 JOUNAL OF CHEMICAL ENINEEIN OF JAPAN
7 Tabl 3 PID ontoll aat and foan atix fo xal (θ/τ ) Tuning thod λ K τ I τ D St-oint Dituban ITAE Ovhoot TV ITAE Ovhoot TV Pood thod a L t al. (998) b Hon t al. (996) d iva t al. (986) L t al. (998) f a a.97, b.; f b f f d a.975, b.79,.79; f b.67 *DOF ontoll i ud only fo th thod of iva t al. (986) and L t al. (998) f Tabl obutn analyi fo xal Tuning thod St-oint Dituban ITAE Ovhoot ITAE Ovhoot Pood thod a L t al. (998) b Hon t al. (996) d iva t al. (986) L t al. (998) f Th ood PID filt ontoll i oad with th ontoll and th ontoll dignd by L t al. (998), Hon t al. (996), iva t al. (986) and L t al. (998) with a onvntional filt. Th ontoll aat valu a litd in Tabl 3 along with th foan atix, wh M.84 i ltd fo all ontoll dign. Unit t hang a intodud both in th t-oint and in th dituban fo th iulation. Th iulation ult in Figu 3 indiat that both th dituban and th toint on a fat in th ood ontoll. Th DOF ontoll tutu i ud fo ah dign thod xt iva t al. (986), and L t al. (998) with a onvntional filt. γ i ltd fo th ood ontoll. It i la fo Figu 3 and Tabl 3 that th ood ontoll xhibit btt foan fo both th t-oint and dituban on. 4.3 Exal 3: Dad ti doinant o (θ/τ 5) Conid th o with a long dad ti tudid by Luybn () and Chn and Sbog () 5 D + ( 35) Th ood and afontiond dign thod a oad. Th ontoll tting with th foan ati a givn in Tabl 4. All of th ontoll a dignd to hav M.74. Sin in th a of a dad ti doinant o, th DOF ontoll i uffiint to ahiv atifatoy ontol foan, no t-oint filt i ud fo any dign thod. Th t-oint and load on a hown in Figu 4. Fo thi figu, it i aant that th ood ontoll and th on dignd by L t al. (998) with th onvntional filt ovid iila on, whil th and Hon t al. (996) thod xhibit luggih on and tak a long ti to ttl th on. Th ood ontoll ha xllnt foan whn th lag ti doinat, but it foan bo iila to that of th thod bad on th onvntional filt whn th dad ti doinat. Whn θ/τ >>, th filt ti ontant hould b hon a λ θ >> τ fo th ak of lod-loo tability. Thfo, th o ol at /τ i not a doinant ol in th lod-loo yt. Intad, th ol at /λ dtin th ovall dynai. Thu, intoduing th lad t (β + ) into th IMC filt to onat th o ol at /τ ha littl iat on th dituban on. Futho, th lad t uually ina th olxity of th IMC ontoll, whih in tun dgad th foan of th ulting PID ontoll VOL. 4 NO
8 Tabl 4 PID ontoll aat and foan atix fo xal 3 (θ/τ 5) Tuning thod λ K τ I τ D St-oint Dituban ITAE Ovhoot TV ITAE Ovhoot TV Pood thod a L t al. (998) b Hon t al. (996) d iva t al. (986) L t al. (998) f a a.998, b.689 d a.64, b 3.55,.56 b.96 *DOF ontoll i ud fo all of th thod Po vaiabl Po vaiabl Pood thod L t al. (998). Hon t al. (996) Ti [in] (a) (b) Pood thod L t al. (998) Hon t al. (996) Ti [in] Fig. 3 Siulation ult fo xal by auing a lag diany btwn th idal fdbak ontoll and thu th PID ontoll. It i alo iotant to not that a th od of th filt ina, th ow of th dnoinato t (λ + ) alo ina, whih an au an unnaily low outut on. A a ult, in th a of a dad ti doinant o, th PID ontoll bad on th IMC filt that inlud no lad t off btt foan. 4.4 Exal 4: Polyization o An iotant vioity loo in a olyization o wa idntifid by Chin t al. () a follow: 3 D + ( 36) Th abov-ntiond o ha a lag onloo ti ontant of in and a dad ti of in, whih i alo quit notwothy. Chin t al. () dignd th PI ontoll with th odifid Sith Pdito (SP) by aoxiating th abov o in th fo of an intgating odl with a long dad ti. Figu 5 oa th noinal on by th ood PID filt ontoll and that by th odifid SP. In th ood ontoll, λ 8. i ltd and th ulting tuning aat a obtaind a K.6446, τ I 5., τ D.6667, a and b.978. Th iulation wa ondutd by inting th t t-oint hang at t followd by a load t hang of. at t 9. Th ood ontoll u a il fdbak ontol tutu without any dad ti onato. Nvthl, th ood PID filt ontoll ovid a uio foan, a hown in Figu 5. 8 JOUNAL OF CHEMICAL ENINEEIN OF JAPAN
9 Po vaiabl (a) Pood thod Hon t al. (996) L t al. (998) Po vaiabl 5 5 Ti [in] 5 3 (b).8 Pood thod.6 Hon t al. (996) L t al. (998) Ti [in] Fig. 4 Siulation ult fo xal Pood thod Chin t al. () Po vaiabl Po vaiabl.5. Pood thod. Chin t al. () Ti [in] Fig. 5 Siulation ult of th olyization o Ti [in] Fig. 6 Siulation ult of th olyization o with odl iath Th dituban jtion affodd by th ood ontoll ha a all ttling ti, wha th odifid SP ontoll dibd by Chin t al. () how a luggih and quid long ttling ti. A gad th t-oint on, th odifid SP ontoll ha an initially fat on, bau of th liination of th dad ti, but aftwad it bo low. On th oth hand, th d of th on fo th ood ontoll i unifo and th ttling ti i iila to that by th odifid SP. It i iotant to not that th SP ontol onfiguation ha a la advantag of liinating th ti dlay fo th haatiti quation, whih i vy fftiv to t-oint taking foan. Howv, thi advantag i lot if th o odl i inauat. In od to valuat th obutn againt odl untainty, a iulation tudy wa ondutd fo th wot a of odl iath by auing that th o ha a % iath in th th o aat in th wot dition, a follow 36. D 8 + ( 37) Th lod-loo on a ntd in Figu 6. Noti that th ood thod and th odifid SP thod dibd by Chin t al. () hav iila dituban jtion on fo th odl iath a. Howv, th t-oint on affodd by th odifid SP ontoll how v oillation, whil th ood ontoll giv a o obut on. VOL. 4 NO
10 . M.4 M.5 M.6 M.8 M.9 oad with th o ohitiatd ontoll, uh a th odifid Sith Pdito, in th a of th vioity loo in a olyization o. Th ult how that th ood ontoll giv atifatoy foan without th xtnal dad ti onato. A guidlin of lod-loo ti ontant λ wa alo ood fo a wid ang of θ/τ atio. Fig. 7 In th ood tuning ul, th lod-loo ti ontant λ ontol th tadoff btwn th obutn and foan of th ontol yt. A λ da, th lod-loo on bo fat and an bo untabl. On th oth hand, a λ ina, th lod-loo on bo tabl but luggih. A good tadoff i obtaind by hooing λ to giv an M valu in th ang of.. (Åtö t al., 998; Sbog t al., 4). Th λ guidlin fo val obutn lvl i lottd in Figu 7. Conluion... λ guidlin fo th ood tuning thod A il analytial dign thod fo a PID ontoll aadd with a lad/lag filt wa ood bad on th IMC inil in od to iov it dituban jtion foan. Th ood thod alo inlud a t-oint filt to nhan th t-oint on lik th DOF ontoll uggtd by L t al. (998), Hon t al. (996) and Chn and Sbog (). FOPDT o with th ntativ diffnt θ/τ atio w ud fo th iulation tudy. Th ood PID filt ontoll onitntly ovid uio foan ov th whol ang of th θ/τ atio, whil th oth ontoll bad on th IMC-PID dign thod tak thi advantag only in a liitd ang of th θ/τ atio. In atiula, th ood ontoll how xllnt foan whn th lag ti doinat. Th ood ontoll wa alo Aknowldgnt Thi ah wa uotd by th 6 Engy ou and Thnology Dvlont Poga of Koa. Litatu Citd Åtö, K. J., H. Panagooulo and T. Hägglund; Dign of PI Contoll Bad on Non-Convx Otiization, Autoatia, 34, (998) Chn, D. and D. E. Sbog; PI/PID Contoll Dign Bad on Dit Synthi and Dituban jtion, Ind. Eng. Ch.., 4, () Chin, I. L. and P. S. Fuhauf; Conid IMC Tuning to Iov Contoll Pfoan, Ch. Eng. Pog., 86, 33 4 (99) Chin, I.-L., S. C. Png and J. H. Liu; Sil Contol Mthod fo Intgating Po with Long Dadti, J. Po Contol,, () Dwy, A. O.; Handbook of PI and PID Contoll Tuning ul, Iial Collg P, London, U.K. (3) Hon, I.., J.. Aulandu, J.. Chitoh, J.. VanAntw and. D. Baatz; Iovd Filt Dign in Intnal Modl Contol, Ind. Eng. Ch.., 35, (996) L, Y., S. Pak, M. L and C. Boilow; PID Contoll Tuning fo Did Clod-Loo on fo SI/SO Syt, AIChE J., 44, 6 5 (998) Luybn, W. L.; Efft of Divativ Algoith and Tuning Sltion on th PID Contol of Dad Ti Po, Ind. Eng. Ch.., 4, () Moai, M. and E. Zafiiou; obut Po Contol, Pnti-Hall, Englwood Cliff, U.S.A. (989) iva, D. E., M. Moai and S. Skogtad; Intnal Modl Contol. 4. PID Contoll Dign, Ind. Eng. Ch. Po D. Dv., 5, 5 65 (986) Sbog, D. E., T. F. Edga and D. A. Mlliha; Po Dynai and Contol, nd d., John Wily & Son, Nw Yok, U.S.A. (4) Skogtad, S.; Sil Analyti ul fo Modl dution and PID Contoll Tuning, J. Po Contol, 3, 9 39 (3) Skogtad, S. and I. Potlthwait; Multivaiabl Fdbak Contol; Analyi and Dign, John Wily & Son, Nw Yok, U.S.A. (996) Sith, C. L., A. B. Coiio and J. Matin; Contoll Tuning fo Sil Po Modl, Intu. Thnol.,, (975) JOUNAL OF CHEMICAL ENINEEIN OF JAPAN
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 informationNoise 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 informationMidterm Exam. CS/ECE 181B Intro to Computer Vision. February 13, :30-4:45pm
Nam: Midtm am CS/C 8B Into to Comput Vision Fbua, 7 :-4:45pm las spa ouslvs to th dg possibl so that studnts a vnl distibutd thoughout th oom. his is a losd-boo tst. h a also a fw pags of quations, t.
More informationESCI 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 2 ( ) ( ) ( ) ( ) Two Stage Cluster Sampling and Random Effects Ed Stanek
Two ag ampling and andom ffct 8- Two Stag Clu Sampling and Random Effct Ed Stank FTE POPULATO Fam Labl Expctd Rpon Rpon otation and tminology Expctd Rpon: y = and fo ach ; t = Rpon: k = y + Wk k = indx
More information(( )( )) = = S p S p = S p p m ( )
36 Chapt 3. Rnoalization Toolit Poof of th oiginal Wad idntity o w nd O p Σ i β = idβ γ is p γ d p p π π π p p S p = id i d = id i S p S p d π β γ γ γ i β i β β γ γ β γ γ γ p = id is p is p d = Λ p, p.
More informationThe 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 informationShor s Algorithm. Motivation. Why build a classical computer? Why build a quantum computer? Quantum Algorithms. Overview. Shor s factoring algorithm
Motivation Sho s Algoith It appas that th univs in which w liv is govnd by quantu chanics Quantu infoation thoy givs us a nw avnu to study & tst quantu chanics Why do w want to build a quantu coput? Pt
More informationE 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 informationControl 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 informationAppendix XVI Cracked Section Properties of the Pier Cap Beams of the Steel Girder Bridge using the Moment Curvature Method and ACI Equation
ppndix XV rakd Stion Proprti o th Pir ap Bam o th Stl Girdr Bridg ug th omnt urvatur thod and Equation Wt Bound Pir ap Bam Figur XV- Th atual pir ap bam ro tion [Brown, 99] Th ¾ - al i no longr orrt 5
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
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 informationCharacteristic Equations and Boundary Conditions
Charatriti Equation and Boundary Condition Øytin Li-Svndn, Viggo H. Hantn, & Andrw MMurry Novmbr 4, Introdution On of th mot diffiult problm on i onfrontd with In numrial modlling oftn li in tting th boundary
More informationAnalysis of Feedback Control Systems
Colorado Shool of Mine CHEN403 Feedbak Control Sytem Analyi of Feedbak Control Sytem ntrodution to Feedbak Control Sytem 1 Cloed oo Reone 3 Breaking Aart the Problem to Calulate the Overall Tranfer Funtion
More informationSolutions 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 informationReferences. 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 informationRobustness Analysis of Stator Voltage Vector Direct Torque Control for Induction Motor
IX Symoium Indutial Elctonic INEL, Banja Luka, Novm 3, Routn Analyi of Stato Voltag Vcto ict oqu Contol fo Induction Moto Alkanda Ž. Rakić, Sloodan N. Vukoavić Univity of Blgad, School of Elctical Engining
More informationAli Karimpour Associate Professor Ferdowsi University of Mashhad
LINEAR CONTROL SYSTEMS Ali Karimour Aoiate Profeor Ferdowi Univerity of Mahhad Leture 0 Leture 0 Frequeny domain hart Toi to be overed inlude: Relative tability meaure for minimum hae ytem. ain margin.
More informationPERFORMANCE IMPROVEMENT OF THE INDUCTION MOTOR DRIVE BY USING ROBUST CONTROLLER
PEFOMANCE MPOEMEN OF HE NDUCON MOO DE BY USNG OBUS CONOE S. SEAA, PG Schola,. GEEHA, ctu, N. DEAAAN, Aitant Pofo Abtact -: h tanint pon of th induction oto i obtaind by uing it d-q fnc odl. h tanint pon
More informationLoss factor for a clamped edge circular plate subjected to an eccentric loading
ndian ounal of Engining & Matials Scincs Vol., Apil 4, pp. 79-84 Loss facto fo a clapd dg cicula plat subjctd to an ccntic loading M K Gupta a & S P Niga b a Mchanical Engining Dpatnt, National nstitut
More informationThe 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 informationDirect Power Control of a Doudly Fed Induction Generator with a Fixed Switching Frequency
Dict Pow Contol of a Doudly Fd Induction Gnato with a Fixd Switching Fquncy Won-Sang i, Sung-Tak Jou, yo-bu L School of Elctical and Coput Engining Ajou Univity, Suwon, oa kyl@ajou.ac.k Stv Watkin Fladh
More informationCOMPSCI 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 informationInternal Model Control
Internal Model Control Part o a et o leture note on Introdution to Robut Control by Ming T. Tham 2002 The Internal Model Prinile The Internal Model Control hiloohy relie on the Internal Model Prinile,
More informationP a g e 5 1 of R e p o r t P B 4 / 0 9
P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e
More informationFormula overview. Halit Eroglu, 04/2014 With the base formula the following fundamental constants and significant physical parameters were derived.
Foula ovviw Halit Eolu, 0/0 With th bas foula th followin fundantal onstants and sinifiant physial paats w divd. aiabl usd: Spd of liht G Gavitational onstant h lank onstant α Fin stutu onstant h dud lank
More informationINTRODUCTION TO AUTOMATIC CONTROLS INDEX LAPLACE TRANSFORMS
adjoint...6 block diagram...4 clod loop ytm... 5, 0 E()...6 (t)...6 rror tady tat tracking...6 tracking...6...6 gloary... 0 impul function...3 input...5 invr Laplac tranform, INTRODUCTION TO AUTOMATIC
More informationThree Phase Asymmetrical Load Flow for Four-Wire Distribution Networks
T Aytl Lo Flow o Fou-W Dtuto Ntwo M. Mo *, A. M. Dy. M. A Dtt o Eltl E, A Uvty o Toloy Hz Av., T 59, I * El: o8@yoo.o Att-- Mjoty o tuto two ul u to ul lo, yty to l two l ut. T tt o tuto yt ult y o ovt
More information(, ) which is a positively sloping curve showing (Y,r) for which the money market is in equilibrium. The P = (1.4)
ots lctu Th IS/LM modl fo an opn conomy is basd on a fixd pic lvl (vy sticky pics) and consists of a goods makt and a mony makt. Th goods makt is Y C+ I + G+ X εq (.) E SEK wh ε = is th al xchang at, E
More informationAakash. For Class XII Studying / Passed Students. Physics, Chemistry & Mathematics
Aakash A UNIQUE PPRTUNITY T HELP YU FULFIL YUR DREAMS Fo Class XII Studying / Passd Studnts Physics, Chmisty & Mathmatics Rgistd ffic: Aakash Tow, 8, Pusa Road, Nw Dlhi-0005. Ph.: (0) 4763456 Fax: (0)
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 informationLecture 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 informationPhysics 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 informationADDITIVE INTEGRAL FUNCTIONS IN VALUED FIELDS. Ghiocel Groza*, S. M. Ali Khan** 1. Introduction
ADDITIVE INTEGRAL FUNCTIONS IN VALUED FIELDS Ghiocl Goza*, S. M. Ali Khan** Abstact Th additiv intgal functions with th cofficints in a comlt non-achimdan algbaically closd fild of chaactistic 0 a studid.
More informationCompensation Techniques
D Compenation ehnique Performane peifiation for the loed-loop ytem Stability ranient repone Æ, M (ettling time, overhoot) or phae and gain margin Steady-tate repone Æ e (teady tate error) rial and error
More informationCascade Control. 1. Introduction 2. Process examples 3. Closed-loop analysis 4. Controller design 5. Simulink example
Caae Control. Introution. Proe exale 3. Cloe-loo analyi 4. Controller eign. Siulink exale Introution Feebak ontrol» Corretie ation taken regarle of iturbane oure» Corretie ation not taken until after the
More informationExtinction Ratio and Power Penalty
Application Not: HFAN-.. Rv.; 4/8 Extinction Ratio and ow nalty AVALABLE Backgound Extinction atio is an impotant paamt includd in th spcifications of most fib-optic tanscivs. h pupos of this application
More informationCOHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim.
MTH rviw part b Lucian Mitroiu Th LOG and EXP functions Th ponntial function p : R, dfind as Proprtis: lim > lim p Eponntial function Y 8 6 - -8-6 - - X Th natural logarithm function ln in US- log: function
More informationRecitation PHYS 131. must be one-half of T 2
Reitation PHYS 131 Ch. 5: FOC 1, 3, 7, 10, 15. Pobles 4, 17, 3, 5, 36, 47 & 59. Ch 5: FOC Questions 1, 3, 7, 10 & 15. 1. () The eloity of a has a onstant agnitude (speed) and dietion. Sine its eloity is
More informationII.3. DETERMINATION OF THE ELECTRON SPECIFIC CHARGE BY MEANS OF THE MAGNETRON METHOD
II.3. DETEMINTION OF THE ELETON SPEIFI HGE Y MENS OF THE MGNETON METHOD. Wok pupos Th wok pupos is to dtin th atio btwn th absolut alu of th lcton chag and its ass, /, using a dic calld agnton. In this
More informationCHAPTER IV RESULTS. Grade One Test Results. The first graders took two different sets of pretests and posttests, one at the first
33 CHAPTER IV RESULTS Gad On Tst Rsults Th fist gads tk tw diffnt sts f ptsts and psttsts, n at th fist gad lvl and n at th snd gad lvl. As displayd n Figu 4.1, n th fist gad lvl ptst th tatmnt gup had
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 informationRadiation Equilibrium, Inertia Moments, and the Nucleus Radius in the Electron-Proton Atom
14 AAPT SUER EETING innaolis N, July 3, 14 H. Vic Dannon Radiation Equilibiu, Intia onts, and th Nuclus Radius in th Elcton-Poton Ato H. Vic Dannon vic@gaug-institut.og Novb, 13 Rvisd July, 14 Abstact
More informationJunction Tree Algorithm 1. David Barber
Juntion Tr Algorithm 1 David Barbr Univrsity Collg London 1 Ths slids aompany th book Baysian Rasoning and Mahin Larning. Th book and dmos an b downloadd from www.s.ul.a.uk/staff/d.barbr/brml. Fdbak and
More informationAPVC2007. Rank Ordering and Parameter Contributions of Parallel Vibration Transfer Path Systems *
, Saoo, Jaan Ran Odng and Paa Conbuon of Paalll Vbaon anf Pah Sy * Yn HANG ** Rajnda SINGH *** and Banghun WEN ** **Collg of Mhanal Engnng and Auoaon, Nohan Unvy, POBo 19, No. -11 Wnhua Road, Shnyang,
More informationOn Jackson's Theorem
It. J. Cotm. Math. Scics, Vol. 7, 0, o. 4, 49 54 O Jackso's Thom Ema Sami Bhaya Datmt o Mathmatics, Collg o Educatio Babylo Uivsity, Babil, Iaq mabhaya@yahoo.com Abstact W ov that o a uctio W [, ], 0
More informationTHE SOLAR SYSTEM. We begin with an inertial system and locate the planet and the sun with respect to it. Then. F m. Then
THE SOLAR SYSTEM We now want to apply what we have learned to the olar ytem. Hitorially thi wa the great teting ground for mehani and provided ome of it greatet triumph, uh a the diovery of the outer planet.
More informationChapter 4. Simulations. 4.1 Introduction
Chapter 4 Simulation 4.1 Introdution In the previou hapter, a methodology ha been developed that will be ued to perform the ontrol needed for atuator haraterization. A tudy uing thi methodology allowed
More informationHandout 30. Optical Processes in Solids and the Dielectric Constant
Haut Otal Sl a th Dlt Ctat I th ltu yu wll la: La ut Ka-Kg lat Dlt tat l Itba a Itaba tbut t th lt tat l C 47 Sg 9 Faha Raa Cll Uty Chag Dl, Dl Mt, a lazat Dty A hag l t a gat a a t hag aat by ta: Q Q
More informationTo determine the biasing conditions needed to obtain a specific gain each stage must be considered.
PHYSIS 56 Experiment 9: ommon Emitter Amplifier A. Introdution A ommon-emitter oltage amplifier will be tudied in thi experiment. You will inetigate the fator that ontrol the midfrequeny gain and the low-and
More informationHandout on. Crystal Symmetries and Energy Bands
dou o Csl s d g Bds I hs lu ou wll l: Th loshp bw ss d g bds h bs of sp-ob ouplg Th loshp bw ss d g bds h ps of sp-ob ouplg C 7 pg 9 Fh Coll Uvs d g Bds gll hs oh Th sl pol ss ddo o h l slo s: Fo pl h
More informationCalculus Revision A2 Level
alculus Rvision A Lvl Tabl of drivativs a n sin cos tan d an sc n cos sin Fro AS * NB sc cos sc cos hain rul othrwis known as th function of a function or coposit rul. d d Eapl (i) (ii) Obtain th drivativ
More informationLecture 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 informationThe Z transform techniques
h Z trnfor tchniqu h Z trnfor h th rol in dicrt yt tht th Lplc trnfor h in nlyi of continuou yt. h Z trnfor i th principl nlyticl tool for ingl-loop dicrt-ti yt. h Z trnfor h Z trnfor i to dicrt-ti yt
More informationInventory Model with Time Dependent Demand Rate under Inflation When Supplier Credit Linked to Order Quantity
Int. J Bui. Inf. h. Vol- No. Db 0 Invntoy Mol with i Dpnnt Dan Rat un Inflation Whn Suppli Cit Link to O Quantity R. P. ipathi Dpatnt of Mathati, Gaphi Ea Univity, Dhaun (UK), Inia E-ailtipathi_p0@iffail.o
More informationSTATISTICAL 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 informationSystems Analysis. Prof. Cesar de Prada ISA-UVA
Sytem Analyi Prof. Cear de Prada ISAUVA rada@autom.uva.e Aim Learn how to infer the dynamic behaviour of a cloed loo ytem from it model. Learn how to infer the change in the dynamic of a cloed loo ytem
More informationAssessment of Performance for Single Loop Control Systems
Aement of Performance for Single Loop Control Sytem Hiao-Ping Huang and Jyh-Cheng Jeng Department of Chemical Engineering National Taiwan Univerity Taipei 1617, Taiwan Abtract Aement of performance in
More informationA Tuning of the Nonlinear PI Controller and Its Experimental Application
Korean J. Chem. Eng., 18(4), 451-455 (2001) A Tuning of the Nonlinear PI Controller and Its Experimental Application Doe Gyoon Koo*, Jietae Lee*, Dong Kwon Lee**, Chonghun Han**, Lyu Sung Gyu, Jae Hak
More informationLogarithms. Secondary Mathematics 3 Page 164 Jordan School District
Logarithms Sondary Mathmatis Pag 6 Jordan Shool Distrit Unit Clustr 6 (F.LE. and F.BF.): Logarithms Clustr 6: Logarithms.6 For ponntial modls, prss as a arithm th solution to a and d ar numrs and th as
More informationFourier 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 informationON A GENERALIZED PROBABILITY DISTRIBUTION IN ASSOCIATION WITH ALEPH ( ) - FUNCTION
Intnational Jounal of Engining, Scinc and athmatic Vol. 8, Iu, Januay 8, ISSN: 3-94 Impact Facto: 6.765 Jounal Hompag: http://www.ijm.co.in, Email: ijmj@gmail.com Doubl-Blind P Riwd Rfd Opn Acc Intnational
More informationAP Calculus BC Problem Drill 16: Indeterminate Forms, L Hopital s Rule, & Improper Intergals
AP Calulus BC Problm Drill 6: Indtrminat Forms, L Hopital s Rul, & Impropr Intrgals Qustion No. of Instrutions: () Rad th problm and answr hois arfully () Work th problms on papr as ndd () Pik th answr
More informationCurrent Status of Orbit Determination methods in PMO
unt ttus of Obit Dtintion thods in PMO Dong Wi, hngyin ZHO, Xin Wng Pu Mountin Obsvtoy, HINEE DEMY OF IENE bstct tit obit dtintion OD thods hv vovd ot ov th st 5 ys in Pu Mountin Obsvtoy. This tic ovids
More informationINFLUENCE OF ANTICLIMBING DEVICE ON THE VARIATION OF LOADS ON WHEELS IN DIESEL ELECTRIC 4000 HP
U..B. Si. Bull., Si D, Vol.,., SS 454-5 UEE O AMBG DEVE O HE VARAO O OADS O WHEES DESE EER 4 H onl ătălin OESU Dipozitiul nt intodu ini uplimnt p oţil oiilo loomotilo. n lu pzint iti to ini, unţi d dtl
More informationELECTROMAGNETISM, NUCLEAR STRUCTURES & GRAVITATION
. l & a s s Vo Flds o as l axwll a l sla () l Fld () l olasao () a Flx s () a Fld () a do () ad è s ( ). F wo Sala Flds s b dd l a s ( ) ad oool a s ( ) a oal o 4 qaos 3 aabls - w o Lal osas - oz abo Lal-Sd
More informationPARAMETRIC SENSITIVITY ANALYSIS OF A HEAVY DUTY PASSENGER VEHICLE SUSPENSION SYSTEM
VOL. 4, NO. 8, OCTOBER 009 ISSN 89-6608 ARPN Jounal of Engineeing and Alied Siene 006-009 Aian Reeah Publihing Netwok ARPN. All ight eeved. www.anjounal.om PARAMETRIC SENSITIVITY ANALYSIS OF A HEAVY DUTY
More informationUGC POINT LEADING INSTITUE FOR CSIR-JRF/NET, GATE & JAM. are the polar coordinates of P, then. 2 sec sec tan. m 2a m m r. f r.
UGC POINT LEADING INSTITUE FOR CSIR-JRF/NET, GATE & JAM Solution (TEST SERIES ST PAPER) Dat: No 5. Lt a b th adius of cicl, dscibd by th aticl P in fig. if, a th ola coodinats of P, thn acos Diffntial
More informationExample 1. Centripetal Acceleration. Example 1 - Step 2 (Sum of Vector Components) Example 1 Step 1 (Free Body Diagram) Example
014-11-18 Centipetal Aeleation 13 Exaple with full olution Exaple 1 A 1500 kg a i oing on a flat oad and negotiate a ue whoe adiu i 35. If the oeffiient of tati fition between the tie and the oad i 0.5,
More information1 Input-Output Stability
Inut-Outut Stability Inut-outut stability analysis allows us to analyz th stability of a givn syst without knowing th intrnal stat x of th syst. Bfor going forward, w hav to introduc so inut-outut athatical
More informationJoint Pricing and Inventory Replenishment Decisions in a Multi-level Supply Chain
Engining Ltt 8:4 EL_8_4_09 Joint Piing and Inntoy Rnint iion in a Muti- Suy Cain YUN HUAN EORE Q HUAN Abtat i a oodinat iing and inntoy nint diion in a uti- uy ain ood of uti ui on anufatu and uti tai
More informationUser s Guide. Electronic Crossover Network. XM66 Variable Frequency. XM9 24 db/octave. XM16 48 db/octave. XM44 24/48 db/octave. XM26 24 db/octave Tube
U Guid Elctnic Cv Ntwk XM66 Vaiabl Fquncy XM9 24 db/ctav XM16 48 db/ctav XM44 24/48 db/ctav XM26 24 db/ctav Tub XM46 24 db/ctav Paiv Lin Lvl XM126 24 db/ctav Tub Machand Elctnic Inc. Rcht, NY (585) 423
More informationExercises in functional iteration: the function f(x) = ln(2-exp(-x))
Eiss in funtional itation: th funtion f ln2-p- A slfstudy usin fomal powsis and opato-matis Gottfid Hlms 0.2.200 updat 2.02.20. Dfinition Th funtion onsidd is an ampl tan fom a pivat onvsation with D.Gisl
More informationINTEGRATION BY PARTS
Mathmatics Rvision Guids Intgration by Parts Pag of 7 MK HOME TUITION Mathmatics Rvision Guids Lvl: AS / A Lvl AQA : C Edcl: C OCR: C OCR MEI: C INTEGRATION BY PARTS Vrsion : Dat: --5 Eampls - 6 ar copyrightd
More informationORBITAL 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 informationUtilizing exact and Monte Carlo methods to investigate properties of the Blume Capel Model applied to a nine site lattice.
Utilizing xat and Mont Carlo mthods to invstigat proprtis of th Blum Capl Modl applid to a nin sit latti Nik Franios Writing various xat and Mont Carlo omputr algorithms in C languag, I usd th Blum Capl
More informationprimer B Activity Book Errata Sheet
Loation Inot Cot Chapt Pzzl and anw ky (pag ) Chapt Pzzl and anw ky (pag ) pi B Ativity Book Eata Sht Vion. To find applial hang, find yo vion of th ook litd low (.g., Vion.). All hang litd nd that vion
More information(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 informationLecture 14 (Oct. 30, 2017)
Ltur 14 8.31 Quantum Thory I, Fall 017 69 Ltur 14 (Ot. 30, 017) 14.1 Magnti Monopols Last tim, w onsidrd a magnti fild with a magnti monopol onfiguration, and bgan to approah dsribing th quantum mhanis
More informationFigure 1 Siemens PSSE Web Site
Stability Analyi of Dynamic Sytem. In the lat few lecture we have een how mall ignal Lalace domain model may be contructed of the dynamic erformance of ower ytem. The tability of uch ytem i a matter of
More informationExam 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 informationMon. Tues. Wed. Lab Fri Electric and Rest Energy
Mon. Tus. Wd. Lab Fi. 6.4-.7 lctic and Rst ngy 7.-.4 Macoscoic ngy Quiz 6 L6 Wok and ngy 7.5-.9 ngy Tansf R 6. P6, HW6: P s 58, 59, 9, 99(a-c), 05(a-c) R 7.a bing lato, sathon, ad, lato R 7.b v. i xal
More informationWhile flying from hot to cold, or high to low, watch out below!
STANDARD ATMOSHERE Wil flying fom ot to cold, o ig to low, watc out blow! indicatd altitud actual altitud STANDARD ATMOSHERE indicatd altitud actual altitud STANDARD ATMOSHERE Wil flying fom ot to cold,
More informationEstimation of a Random Variable
Estimation of a andom Vaiabl Obsv and stimat. ˆ is an stimat of. ζ : outcom Estimation ul ˆ Sampl Spac Eampl: : Pson s Hight, : Wight. : Ailin Company s Stock Pic, : Cud Oil Pic. Cost of Estimation Eo
More information( ) Zp THE VIBRATION ABSORBER. Preamble - A NEED arises: lbf in. sec. X p () t = Z p. cos Ω t. Z p () r. ω np. F o. cos Ω t. X p. δ s.
THE VIBRATION ABSORBER Preable - A NEED arie: Lui San Andre (c) 8 MEEN 363-617 Conider the periodic forced repone of a yte (Kp-Mp) defined by : 1 1 5 lbf in : 1 3 lb (t) It natural frequency i: : ec F(t)
More informationImage Enhancement: Histogram-based methods
Image Enhancement: Hitogam-baed method The hitogam of a digital image with gayvalue, i the dicete function,, L n n # ixel with value Total # ixel image The function eeent the faction of the total numbe
More informationLast Lecture Summary ADALINE
Lat Lctu Summa ADALIN Analtical Solution Gadint Bad Laning Batch Laning Incmntal Laning Laning Rat Adatation Statitical Inttation Aland Bnadino al@i.it.utl.t Machin Laning 9/ ADALIN N l l l T Aland Bnadino
More informationGiven the following circuit with unknown initial capacitor voltage v(0): X(s) Immediately, we know that the transfer function H(s) is
EE 4G Note: Chapter 6 Intructor: Cheung More about ZSR and ZIR. Finding unknown initial condition: Given the following circuit with unknown initial capacitor voltage v0: F v0/ / Input xt 0Ω Output yt -
More informationCDS 110b: Lecture 8-1 Robust Stability
DS 0b: Lct 8- Robst Stabilit Richad M. Ma 3 Fba 006 Goals: Dscib mthods fo psnting nmodld dnamics Div conditions fo obst stabilit Rading: DFT, Sctions 4.-4.3 3 Fb 06 R. M. Ma, altch Gam lan: Robst fomanc
More informationTest 2 phy a) How is the velocity of a particle defined? b) What is an inertial reference frame? c) Describe friction.
Tet phy 40 1. a) How i the velocity of a paticle defined? b) What i an inetial efeence fae? c) Decibe fiction. phyic dealt otly with falling bodie. d) Copae the acceleation of a paticle in efeence fae
More informationFr Carrir : Carrir onntrations as a funtion of tmpratur in intrinsi S/C s. o n = f(t) o p = f(t) W will find that: n = NN i v g W want to dtrmin how m
MS 0-C 40 Intrinsi Smiondutors Bill Knowlton Fr Carrir find n and p for intrinsi (undopd) S/Cs Plots: o g() o f() o n( g ) & p() Arrhnius Bhavior Fr Carrir : Carrir onntrations as a funtion of tmpratur
More informationController Design Based on Transient Response Criteria. Chapter 12 1
Controller Design Based on Transient Response Criteria Chapter 12 1 Desirable Controller Features 0. Stable 1. Quik responding 2. Adequate disturbane rejetion 3. Insensitive to model, measurement errors
More informationChapter 11 Solutions ( ) 1. The wavelength of the peak is. 2. The temperature is found with. 3. The power is. 4. a) The power is
Chapt Solutios. Th wavlgth of th pak is pic 3.898 K T 3.898 K 373K 885 This cospods to ifad adiatio.. Th tpatu is foud with 3.898 K pic T 3 9.898 K 50 T T 5773K 3. Th pow is 4 4 ( 0 ) P σ A T T ( ) ( )
More informationES 330 Electronics II Homework # 5 (Fall 2016 Due Wednesday, October 4, 2017)
Pag1 Na olutions E 33 Elctonics II Howok # 5 (Fall 216 Du Wdnsday, Octob 4, 217) Pobl 1 (25 pots) A coon-itt aplifi uss a BJT with cunt ga = 1 whn biasd at I =.5 A. It has a collcto sistanc of = 1 k. (a)
More informationEinstein's Energy Formula Must Be Revised
Eintein' Energy Formula Mut Be Reied Le Van Cuong uong_le_an@yahoo.om Information from a iene journal how that the dilation of time in Eintein peial relatie theory wa proen by the experiment of ientit
More informationGalaxy Photometry. Recalling the relationship between flux and luminosity, Flux = brightness becomes
Galaxy Photomty Fo galaxis, w masu a sufac flux, that is, th couts i ach pixl. Though calibatio, this is covtd to flux dsity i Jaskys ( Jy -6 W/m/Hz). Fo a galaxy at som distac, d, a pixl of sid D subtds
More informationKeywords: Auxiliary variable, Bias, Exponential estimator, Mean Squared Error, Precision.
IN: 39-5967 IO 9:8 Ctifid Intnational Jounal of Engining cinc and Innovativ Tchnolog (IJEIT) Volum 4, Issu 3, Ma 5 Imovd Exonntial Ratio Poduct T Estimato fo finit Poulation Man Ran Vija Kuma ingh and
More informationComparisons of the Variance of Predictors with PPS sampling (update of c04ed26.doc) Ed Stanek
Coparo o th Varac o Prdctor wth PPS aplg (updat o c04d6doc Ed Sta troducto W copar prdctor o a PSU a or total bad o PPS aplg Th tratgy to ollow that o Sta ad Sgr (JASA, 004 whr w xpr th prdctor a a lar
More information( ) rad ( 2.0 s) = 168 rad
.) α 0.450 ω o 0 and ω 8.00 ω αt + ω o o t ω ω o α HO 9 Solution 8.00 0 0.450 7.8 b.) ω ω o + αδθ o Δθ ω 8.00 0 ω o α 0.450 7. o Δθ 7. ev.3 ev π.) ω o.50, α 0.300, Δθ 3.50 ev π 7π ev ω ω o + αδθ o ω ω
More informationSection 11.6: Directional Derivatives and the Gradient Vector
Sction.6: Dirctional Drivativs and th Gradint Vctor Practic HW rom Stwart Ttbook not to hand in p. 778 # -4 p. 799 # 4-5 7 9 9 35 37 odd Th Dirctional Drivativ Rcall that a b Slop o th tangnt lin to th
More information