Control Systems
|
|
- Eunice Fox
- 5 years ago
- Views:
Transcription
1 6.5 Cntrl Sytem Tday we are ging t ver part f Chapter 6 and part f Chapter 8 Cntrllability and Obervability State Feedba and State Etimatr Lat Time : Cntrllability Obervability Cannial dempitin Cntrllable/unntrllable Obervable/unbervable Cntrllability: Definitin Cnider the ytem x x Bu x R n ; u R Cntrllability i a relatinhip between tate and input. Definitin: The ytem r the pair (B) i aid t be ntrllable if fr any initial tate x()=x and any final tate x d there exit a finite time T > and an input u(t) t[t] uh that T (T-τ) x(t) e x e Bu( τ)dτ x T p. d ()
2 t τ 'τ (tτ) '(tτ) W (t) e BB'e dτ e BB'e d Equivalent nditin fr ntrllability: ) W (t) i nningular fr any t >. ) The matrix G = [B B B n- B] ha full rw ran i.e. (G ) = n. ) The matrix G n-p+ = [B B B n-p B] ha full rw ran (p=ran(b)) ) M() = [-I B] ha full rw ran at every eigenvalue f. t Obervability: dual nept Cnider an n-dimeninal p-input q-utput ytem: x x Bu; u Sytem y Cx Du ume that we nw the input and an meaure the utput but have n ae t the tate. Definitin: The ytem i aid t be bervable if fr any unnwn initial tate x() there exit a finite t > uh that x() an be exatly evaluated ver [t ] frm the input u and the utput y. Otherwie the ytem i aid t be unbervable. y
3 Equivalent nditin fr bervability: ) W (t) i nningular fr me t >. ) The bervability matrix C C G C C n-p r ( G ) np n C C ha full lumn ran (G n-p+) = n. (p=ran(c)) ) The matrix M ( λ) λi C ha full lumn ran at every eigenvalue f. 5 Cntrllability dempitin Therem: Suppe that (G ) = n < n. Let Q be a nningular matrix whe firt n lumn are LI lumn f G. Let P=Q - and z=px. Then nn np PP B PB R B R C C C B Mrever the pair ( B ) i ntrllab le and C ( I ) B D C(I ) B D z z z y C z C z z B u z z B u y C z i ntrllable and ha the ame tranfer funtin a the riginal ytem. The tate unntrllable z z z i The ntrl ha n effet n it 6
4 Obervability dempitin (fllw frm duality) Therem: Suppe that (G ) = n < n. Let P be a nningular matrix whe firt n rw are LI rw f G. Then PP C nn qn C C R B B PB B R Mrever the pair ( C ) i bervable and C ( I ) B D C(I ) B D B R np Diuin: fter tate tranfrmatin the equivalent ytem i z z B u z may be affeted by z z z z Bu but ha n effet n y r z y C z Du z nt bervable z z Bu y C z Du ha the ame tranfer funtin a the riginal ytem and i bervable. 7 Tday: Cntrllability and bervability ntinued Cntrllability/bervability dempitin Minimal realizatin Cnditin fr Jrdan frm nditin Parallel reult fr direte-time ytem Cntrllability after ampling State feedba deign Ple aignment Uing ntrllable annial frm By lving matrix equatin 8
5 Cntrllability-Obervability dempitin Therem: ll LTI ytem an be tranfrmed via equivalent tranfrmatin int the fllwing frm: z z z z y z B z B u z z C C z Du B where i ntrllab le B ( B ) i ntrllab le and ( C ) i bervable. ( C ) i bervable. Mrever z C ( I ) B D C(I ) B D z B u y C z Du i a ntrllable and bervable realizatin It ha the ame tranfer funtin a the riginal ytem 9 Minimal realizatin f a tranfer matrix Obervatin: Let G() be a prper ratinal tranfer matrix. We learned earlier that there exit (BCD) uh that G()=C(I-) - B+D The realizatin i nt unique. Definitin: realizatin (BCD) f G whih ha the minimal dimenin f tate pae i alled a minimal realizatin f G. Quetin: Whih ne i a minimal realizatin? Hw t btain a minimal realizatin? Therem: (BCD) i a minimal realizatin iff (B) i ntrllable and (C) i bervable. 5
6 Predure t btain a minimal realizatin: n earlier reult: Fr a tritly prper and ratinal matrix G() Let d()= r + a r- + a r- +.+ a r- +a r be the leat mmn denminatr f all entrie Then G() an be expreed a (aume G i qp) G() d() r r qp N N N N N r r i R realizatin f G() i given a: aip a Ip a ri p Ip Ip Ip C N N N r Nr a ri p Ip B Ue equivalene tranfrmatin z = Px uh that PP B B PB B C CP C C ( B) i ntrllable and ( C) i bervable. Then ( C B (I C ) B C(I ) B G() and ) i a minimal realizatin f G(). If G() i nt tritly prper we an firt dempe it a G() = G p () + D where G p () i tritly prper. 6
7 Cnditin fr Jrdan frm equatin Equivalene tranfrmatin d nt hange ntrllability and bervability Thee prpertie are eay t ee frm Jrdan frm. Therem: ume that ha m ditint eigenvalue m and ha a Jrdan frm arranged by the eigenvalue with bl J diag[jj... JJ J mj m...] m Let the rw f B rrepnding t the lat rw f J ij be b ij. Let the lumn f C rrepnding t the firt lumn f J ij be ij Then the ytem i ntrllable iff fr eah i the rw {b i b i } are LI. The ytem i bervable iff fr eah i the lumn { i i } are LI. Example: λ λ λ λ λ λ λ b * b B b * b * C * * *. (B) i ntrllable iff {b b b } i LI and b (C) i bervable iff { } i LI and The lumn f C and the rw f B mared by * have n effet n ntrllability r bervability. 7
8 8 5 Example: λ λ λ λ λ λ λ * * * B * * * C Cae :. Cae : =. b b b b Example: C b b b b B λ λ λ λ Cae :. Therem: Fr a ingle input ytem It i ntrllable iff fr eah ditint eigenvalue there i nly ne Jrdan bl and eah element f B rrepnding t the lat rw f a Jrdan bl i nnzer; It i bervable iff fr eah ditint eigenvalue there i nly ne Jrdan bl and eah element f C rrepnding t the firt lumn f a Jrdan bl i nnzer. (B) i ntrllable iff b and b (C) bervable iff and Cae : = then what?
9 Direte-Time Sytem The ytem deribed by differene equatin: x[+] = x[]+bu[] y[]= Cx[]+Du[] Reult n ntrllability and bervability are quite imilar t the fr ntinuu-time ytem. 7 Definitin Cnider the differene equatin x[ ] x[] Bu[] y[] Cx[] D[] where xr n ur p. Definitin : The ytem r the pair (B) i aid t be ntrllable if fr any initial tate x()=x and any final tate x d there exit an integer > and a equene f input u[] [ ] uh that m --m x[ ] x u[m] x Definitin : The ytem r the pair (C) i aid t be bervable if fr any unnwn initial tate x() there exit a finite > uh that x() an be exatly evaluated ver [ ] frm the input u and the utput y. Otherwie the ytem i aid t be unbervable. d () 8 9
10 Equivalent nditin fr ntrllability: The fllwing are equivalent nditin fr the pair (B) t be ntrllable: ) The matrix G = [B B B n- B] ha full rw ran i.e. (G ) = n. ) The matrix M () = [I B] ha full rw ran at every eigenvalue f. ) The fllwing nn matrix i nningular W d [n ] n m m BB'( Nte: There may exit an integer n < n uh that W d (n -) i nningular. m )' 9 Equivalent nditin fr bervability: ) The bervability matrix C G C n C ha full lumn ran. ) The matrix M ( λ) C λi ha full lumn ran at every eigenvalue f. ) The fllwing nn matrix i nningular W d [n ] n m ( m )' C' C m
11 Cntrllability after ampling ntinuu-time ytem x x Bu; Let the ampling perid be T. During the ampling perid u(t) = u(t) fr all t [T (+)T) = Define u[]:= u[t]; x[]=x[t]. The relatin between u[] and x[] i gverned by the differene equatin: where x[ ] x[] B u[] d e T d B d d [ d - I]B Quetin: I ntrllability retained after diretizatin? Summary f reult frm 6.7 If the pair (B) i unntrllable then ( d B d ) i al unntrllable fr any ampling time T. If all the eigenvalue f i real then (B) ntrllable implie that ( d B d ) i ntrllable. If ha mplex eigenvalue ntrllability maybe lt fr me peial ampling perid T. We ue Re[x] and Im[x] t dente the real part and the imaginary part f a mplex number x. Suppe (B) i ntrllable. uffiient nditin fr ( d B d ) t be ntrllable i that Im[ i j ] m/t fr m= whenever Re[ i - j ]=. The nditin i t enure that the number f Jrdan bl will nt inreae fr a partiular eigenvalue. Nte that if i i an eigenvalue f then e it i an eigenvalue f d. If i and j have ame real part e it and e jt may be the ame.
12 Example: x x Bu β G B B detg β β β B The CT ytem i ntrllable if. Nw uppe. Let the ampling perid be T. x[ ] d x[] B u[] d d e T e T βt in T in T βt B d βt βin βt β β T β in βt What happen when T=? S far we have tudied ntrllability and bervability Main Prblem f the Cure nalyi: Slutin t LTI ytem tability et. Cntrllability and bervability; Feedba deign and ntrutin f berver Optimal ntrl Next we will tart t addre deign prblem
13 Stabilizatin prblem Given a LTI ytem x x Bu. typial ntrl prblem i t bring the tate x frm any initial nditin t the rigin and eep it there. If i table we nly need t et u= and x(t) will nverge t the rigin aympttially. nther prblem i t bring x t a deirable pint x d a fat a pible and eep it there. Bth f thee prblem are abut tabilizatin at an equilibrium pint. The end prblem an be tranfrmed int the firt ne. 5 Fr example given an LTI ytem: z z Bv; y Cz Dv Suppe that i nningular and v = u + u e. (u e a given ntant). We have z z Bu e Bu; Let z e = Bu e and define x = z z e. Then x z z Bue Bu (z - ze) Bu x Bu; x x Bu. Suppe that z e i a deirable pint where we wuld lie t eep z there. If i table then by etting u = x(t) will nverge t frm any initial x and will tay there. z(t) = x(t) + z e nverge t z e and tay there. Quetin: What if i nt table? What if i table but the nvergene rate i t lw? 6
14 Fr the equatin x x Bu. Reall that if (B) i ntrllable then the fllwing ntrl u(t) B'e t) t W (t )[e x x ' (t an bring x frm any initial nditin x t any final detinatin x d. The time duratin [t ] an be arbitrarily mall. nd the ntrl i f minimal energy. Hwever thi ntrl trategy i nt ued in pratie. Rean: Very enitive t parameter hange and implementatin errr; Even if the tate i at the rigin diturbane eep driving it away frm the rigin. Nt eay t mpute. In ummary: nt reliable mpliated and frutrating. d ] (*) 7 pratial and effetive lutin: tate feedba Fr the ytem x x Bu y Cx Du If we let u = r K x. Then x ( BK)x Br. If i untable but (B) i ntrllable we an mae BK table by hing K prperly; If i table but the nvergene rate i t lw we an imprve the nvergene prperty by deigning K prperly. The feedba law u = r Kx i imple fr implementatin but very effetive. We hall find ut hw t deign a tate feedba law. 8
15 n additinal tl: State etimatin What if the tate annt be btained thrugh meaurement? ume that all the infrmatin that an be meaured i y = Cx+Du. If the ytem i bervable we hall ue a tate-etimatr alled an berver t etimate the tate frm the meaurement y and the input u. The berver i al an LTI ytem with input a u and y and it utput i the etimate f the tate x: u xˆ(t) - an etimate f x(t) Oberver y We will learn hw t deign an berver. We Start with State Feedba Deign 9 State feedba deign: ingle input ae ingle input ingle utput ytem x x bu y x (aume D= fr impliity) where R nn br n ha nly ne lumn and R n ha ne rw. p=q=. Let R n be a rw vetr. Then x R. With tate feedba u= r x we have x ( b)x br y x Therem: The pair (-b b) i ntrllable iff (b) i ntrllable. (ee page fr prf.) Cmment: tate-feedba de nt hange ntrllability prperty. Hwever the bervability f (-b) might be different frm that f (). 5
16 What an be gained frm uing tate feedba? The riginal ytem: x x bu y x With tate feedba we have: x ( b)x br y x reult t be hwn later: if (b) i ntrllable then the eigenvalue f -b an be plaed anywhere by hing prperly. Example: b b Eigenvalue f : = = untable. Charateriti plynmial fr -b i ()= +( -)+( - -8)= +a +a The tw effiient a and a an tae any value. Cntrllable Cannial Frm Fr impliity we nider a th-rder ytem. The reult fr the general ae an be eaily extended frm the pattern. Therem: Suppe that (b) i ntrllable and det(i ) - Let Q : P b b b b With the tate tranfrmatin z = Px we have - PP b Pb P β β β β Cntrllable Cannial frm Furthermre β (I) b β β β 6
17 7 Prf: We an brea the tranfrmatin int tw tep: x P x P P x where Q P b b b b Q P - With the firt tranfrmatin we btain B Q B Q Q With the end tranfrmatin we btain B Q B Q Q Here we an verify that B B Q Q Q Exat ple aignment Therem: Suppe that (b) i ntrllable. Then the eigenvalue f -b an be arbitrarily aigned prvided that mplex njugate eigenvalue are aigned in pair. Prf: Let z = Px be the tate tranfrmatin that tranfrm the equatin int ntrllable annial frm: Pb b PP - b - have we With ) ( ) ( ) ( b) det(i
18 det(i b) Thi mean that the eigenvalue f aigned. Hw abut - b? ( ) ( ) ( ) b an be arbitrarily - If we let Q P - then - b QQ QbQ Q( b)q The eigenvalue f - b are the ame a the f b Frm the prf a predure t deign the feedba gain an be derived. 5 Predure fr aigning the eigenvalue f -b. Step. Che the deired eigenvalue et { i i= n} whih ntain njugate mplex pair e.g. i = -+j and i+ = j and btain the effiient f n n n () (λ )(λ ) (λ ) d Step. Cmpute the harateriti plynmial f () det(i) n n n and the tranfrmatin matrix e.g. fr n = Q : P - b b b b n n n 6 8
19 9 7 Pb b PP Then - b - Step : i i i Che b Then - Step : P. Cmpute...n} i {λ the deired eigenvalue ha b)q Q( - b then i 8 Example: le. ntrllab (B) nningular B B B G untable - eigenvalue : B Step : The deired eigenvalue - -+j --j 8 5 j) j)( )( ( ) ( d Step : Charateriti plynmial f ) I det( Q P G Q
20 9 Step : 8 8; ; ; Step : 9 8 P Step 5: Verify: b j - - j b : f Eigenvalue ) ) )(( ( ) )( ( 8 9 ) det(i Tranfer funtin f the feedba ytem: β β β β b The riginal ytem x y bu x x The ytem with tate feedba x y br ( - b)x x Tranfer funtin frm u t y: β β β β b ) (I -b Tranfer funtin frm r t y: ) ( ) ( ) ( β β β β b b) (I
21 Cmpare: (I) b β β β β (I b) β β β β b ( ) ( ) ( ) Cnluin: State feedba de nt hange the zer f the ytem. If (b) i ntrllable the ple an be arbitrarily aigned. The feedba gain that aign the eigenvalue i unique. (Nt unique if the ytem ha multiple input). If a new ple i the ame a ne f the zer the rder f the led-lp ytem an be redued. mut be unbervable. (ine the ntrllability i the ame). Deirable eigenvalue regin t the firt tep f the predure we need t he the deirable eigenvalue. Hw t d thi? There are me general rule depending n the perfrmane pe. Suh a the verht rie time ettling time (nvergene rate). Generally Large real part f eigenvalue fat nvergene hrt ettling time Large imaginary part f eigenvalue big illatin and big verht. If the rati between the imag part and the real part i apprpriate we may have mall verht and fat rie time typial regin fr deired eigenvalue Im Re
22 State feedba deign: multiple input ae Cnider a ytem x x Bu; y Cx Du where R nn BR np CR qn. We an al tranfrm the ytem int a ntrllable annial frm. The idea i extended frm the ingle-input ae; The annial frm al reveal the truture t ee hw the ple are mved; Hwever the predure an be very mpliated. (ee 8.6.) Here we will tudy a quite different apprah. It al applie t ingle input ytem. State feedba deign: By lving matrix equatin In thi apprah we dn t tranfrm a ytem int a ntrllable annial frm Hw de it wr? The main idea i a fllw. The prblem: Find K.t. - BK ha a et f deired eigenvalue ay the eigenvalue f F. Thi i the ae if -BK and F are imilar i.e. there exit a nningular matrix T.t. - BK = TFT - ~ Similar matrie have ame eigenvalue Key: Find bth K and T
23 The new prblem: Given B and F find K and nningular T uh that - BK = TFT - Multiply bth ide frm right with T we btain T -BKT = TF Sine T i nningular there i a ne t ne rrepndene between KT and K. If we let K = KT then K=K T -. Nw T BK = TF T T F = BK The predure: he K R pn. Slve T T F = BK fr T. If T i nningular let K=K T -. Then -BK and F are imilar. Then -BK ha the deired eigenvalue. Main nern: Hw t lve the matrix equatin T-TF=BK? Under what nditin i the lutin T nningular? 5 Main nern: Hw t lve the matrix equatin T T F = BK? Under what nditin i the lutin T nningular? Summary f the main pint: The matrix equatin an be tranfrmed int a regular linear algebrai equatin with nn unnwn. It ha a unique lutin iff and F have n mmn eigenvalue. If (B) i ntrllable then the lutin i generally nningular with K arbitrarily hen. If K i generated by rand(pn) r randn(pn) then the prbability that T i nningular i. When p = the reulting K=K T - i unique. When p > the reulting K=K T - i nt unique. Baed n thee reult ptimizatin algrithm an be develped fr imprving ther perfrmane while the eigenvalue are at the deired latin. 6
24 Tranfrmatin int a regular algebrai equatin: Example: Slve T - TF = BK F S T TF t t BK t t t T t t t t t t t t t t t t t BK De it have a lutin? Regnizing that we have variable and nditin the abve an be nverted t: t t t t 7 but the lutin t T TF = BK Therem : If and F have n mmn eigenvalue then the equatin ha a unique lutin. (.7) Therem : If and F have n mmn eigenvalue the neeary nditin fr T t be nningular are that { B} i ntrllable and {FK } i bervable. Fr the ingle input ae (p=) T i nningular iff { B} i ntrllable and {FK } i bervable. Therem : Suppe that and F have n mmn eigenvalue and (B) i ntrllable. Then fr almt all K T i nningular. 8
25 lgrithm Selet F having deired led-lp eigenvalue whih are different frm the f Che an arbitrary K uh that {FK } i bervable Slve T-TF=BK t btain the unique T. The matlab mmand t lve the equatin i T=lyap(-F-B*K) If T i nn-ingular let K = K T -. Then -BK ha the deired eigenvalue. If T i ingular whih i rarely the ae he a different K and try again Finally dn t frget t he if -BK ha the deired eigenvalue. Yu might have typed the wrng number. eig(-b*k)=? 9 but the eletin f F: Firt elet the deired eigenvalue with me rule If the deired eigenvalue are all real imply let F=diag{ n } If the deired eigenvalue ha mplex njugate pair ay +j -j +j -j he λ F β β β β 5 5
26 Example: B F 5 Ue T= lyap(-f-b*k) and K=K*inv(T) K: K Oberve that me K have mall element but me may have 5 big element. In implementatin we lie t ue mall valued K. Obervatin: If there are mre than ne K that aign the eigenvalue f -BK t the ame latin then there are infinitely many f them. n intereting and meaningful prblem: Pi ne frm the K whih aign the eigenvalue uh that the petral nrm f K i.e. K i minimized. We may al develp algrithm t he K t ptimize r imprve ther perfrmane ee e.g. T. Hu Z. Lin and J. Lam `` unified gradient apprah t perfrmane ptimizatin under ple aignment ntraint" Jurnal f Optimizatin Thery and ppliatin July T. Hu and J. Lam ``Imprvement f parametri tability margin under ple aignment'' IEEE Tranatin n utmati Cntrl Vl.~ N.~ pp.~
27 Hw t realize tate-feedba in Simulin? u x x Bu y Cx Same ytem an be equivalently realized with u x xbu y x Under tate feedba u=v-kx v u y x x Bu x y x K x nt available in thi bl C x y C y y=cy =Cx The purpe f ding thi i t get x 5 Tday: Cntrllability and bervability ntinued Cntrllability/bervability dempitin Minimal realizatin Cnditin fr Jrdan frm nditin Parallel reult fr direte-time ytem Cntrllability after ampling State feedba deign Uing ntrllable annial frm By lving matrix equatin Next Time: Regulatin and traing Rbut traing and diturbane rejetin Stabilizatin State etimatin 5 7
28 8 55 Prblem et #. I the fllwing tate equatin ntrllable? Obervable? x y u x x 56. Fr the fllwing tate equatin x y u x x ) Find a tate feedba u = r - x t plae the ple at ---. Ue bth methd (via ntrllable annial frm via lving matrix equatin hw all tep) and mpare the reult. ) Find a tate feedba u = r - f x t plae the ple at -+j --j -8 Ue bth methd and mpare the reult. ) Ue imulin t imulate the led-lp ytem reulting frm ) and ) repetively under initial nditin x()=[ - ] and r(t) =unit tep. Plt y(t) fr the tw ae in the ame figure.
29 . Fr the fllwing tate equatin x x u y x ) Find tw different tate feedba u = r K x and u = r- K x t plae the ple at -+j --j -6. Try t find K and K uh that ne ha relatively larger element and the ther ne ha relatively mall element. ) Ue imulin t imulate the led-lp ytem reulting frm Cae : u = r - K x x()=[ ] and r(t) =. Cae : u = r - K x x()=[ ] and r(t) =. Plt y(t) fr the tw ae in the ame figure. Plt u (t) fr the tw ae in the ame figure. Plt u (t) fr the tw ae in the ame figure. u Nte that u u 57 9
Chapter 8. Root Locus Techniques
Chapter 8 Rt Lcu Technique Intrductin Sytem perfrmance and tability dt determined dby cled-lp l ple Typical cled-lp feedback cntrl ytem G Open-lp TF KG H Zer -, - Ple 0, -, -4 K 4 Lcatin f ple eaily fund
More informationECE-320: Linear Control Systems Homework 1. 1) For the following transfer functions, determine both the impulse response and the unit step response.
Due: Mnday Marh 4, 6 at the beginning f la ECE-: Linear Cntrl Sytem Hmewrk ) Fr the fllwing tranfer funtin, determine bth the imule rene and the unit te rene. Srambled Anwer: H ( ) H ( ) ( )( ) ( )( )
More informationName Student ID. A student uses a voltmeter to measure the electric potential difference across the three boxes.
Name Student ID II. [25 pt] Thi quetin cnit f tw unrelated part. Part 1. In the circuit belw, bulb 1-5 are identical, and the batterie are identical and ideal. Bxe,, and cntain unknwn arrangement f linear
More informationChapter 9 Compressible Flow 667
Chapter 9 Cmpreible Flw 667 9.57 Air flw frm a tank thrugh a nzzle int the tandard atmphere, a in Fig. P9.57. A nrmal hck tand in the exit f the nzzle, a hwn. Etimate (a) the tank preure; and (b) the ma
More information1. Introduction: A Mixing Problem
CHAPTER 7 Laplace Tranfrm. Intrductin: A Mixing Prblem Example. Initially, kg f alt are dilved in L f water in a tank. The tank ha tw input valve, A and B, and ne exit valve C. At time t =, valve A i pened,
More informationControl Systems. Controllability and Observability (Chapter 6)
6.53 trl Systems trllaility ad Oservaility (hapter 6) Geeral Framewrk i State-Spae pprah Give a LTI system: x x u; y x (*) The system might e ustale r des t meet the required perfrmae spe. Hw a we imprve
More informationDigital Filter Specifications. Digital Filter Specifications. Digital Filter Design. Digital Filter Specifications. Digital Filter Specifications
Digital Filter Deign Objetive - Determinatin f a realiable tranfer funtin G() arximating a given frequeny rene eifiatin i an imrtant te in the develment f a digital filter If an IIR filter i deired, G()
More informationChapter 9. Design via Root Locus
Chapter 9 Deign via Rt Lcu Intrductin Sytem perfrmance pecificatin requirement imped n the cntrl ytem Stability Tranient repne requirement: maximum verht, ettling time Steady-tate requirement :.. errr
More informationNONISOTHERMAL OPERATION OF IDEAL REACTORS Plug Flow Reactor. F j. T mo Assumptions:
NONISOTHERMAL OPERATION OF IDEAL REACTORS Plug Flw Reactr T T T T F j, Q F j T m,q m T m T m T m Aumptin: 1. Hmgeneu Sytem 2. Single Reactin 3. Steady State Tw type f prblem: 1. Given deired prductin rate,
More informationCHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS
CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.1 INTRODUCTION 8.2 REDUCED ORDER MODEL DESIGN FOR LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.3
More informationRichard s Transformations
4/27/25 Rihard Tranfrmatin.d /7 Rihard Tranfrmatin Reall the put impedane f hrt-iruited and peniruited tranmiin le tub. j tan β, β t β, β Nte that the put impedane are purely reatie jut like lumped element!
More informationPattern Recognition 2014 Support Vector Machines
Pattern Recgnitin 2014 Supprt Vectr Machines Ad Feelders Universiteit Utrecht Ad Feelders ( Universiteit Utrecht ) Pattern Recgnitin 1 / 55 Overview 1 Separable Case 2 Kernel Functins 3 Allwing Errrs (Sft
More informationThis section is primarily focused on tools to aid us in finding roots/zeros/ -intercepts of polynomials. Essentially, our focus turns to solving.
Sectin 3.2: Many f yu WILL need t watch the crrespnding vides fr this sectin n MyOpenMath! This sectin is primarily fcused n tls t aid us in finding rts/zers/ -intercepts f plynmials. Essentially, ur fcus
More informationGreedy Algorithms. Kye Halsted. Edited by Chuck Cusack. These notes are based on chapter 17 of [1] and lectures from CSCE423/823, Spring 2001.
#! Greedy Algrithms Kye Halsted Edited by Chuk Cusak These ntes are based n hapter 17 f [1] and letures frm CCE423/823, pring 2001. Greedy algrithms slve prblems by making the hie that seems best at the
More informationLyapunov Stability Stability of Equilibrium Points
Lyapunv Stability Stability f Equilibrium Pints 1. Stability f Equilibrium Pints - Definitins In this sectin we cnsider n-th rder nnlinear time varying cntinuus time (C) systems f the frm x = f ( t, x),
More informationComputational modeling techniques
Cmputatinal mdeling techniques Lecture 4: Mdel checing fr ODE mdels In Petre Department f IT, Åb Aademi http://www.users.ab.fi/ipetre/cmpmd/ Cntent Stichimetric matrix Calculating the mass cnservatin relatins
More informationChapter #4 EEE8013. Linear Controller Design and State Space Analysis. Design of control system in state space using Matlab
EEE83 hapter #4 EEE83 Linear ontroller Deign and State Space nalyi Deign of control ytem in tate pace uing Matlab. ontrollabilty and Obervability.... State Feedback ontrol... 5 3. Linear Quadratic Regulator
More informationMATHEMATICS SYLLABUS SECONDARY 5th YEAR
Eurpean Schls Office f the Secretary-General Pedaggical Develpment Unit Ref. : 011-01-D-8-en- Orig. : EN MATHEMATICS SYLLABUS SECONDARY 5th YEAR 6 perid/week curse APPROVED BY THE JOINT TEACHING COMMITTEE
More informationDead-beat controller design
J. Hetthéssy, A. Barta, R. Bars: Dead beat cntrller design Nvember, 4 Dead-beat cntrller design In sampled data cntrl systems the cntrller is realised by an intelligent device, typically by a PLC (Prgrammable
More information, which yields. where z1. and z2
The Gaussian r Nrmal PDF, Page 1 The Gaussian r Nrmal Prbability Density Functin Authr: Jhn M Cimbala, Penn State University Latest revisin: 11 September 13 The Gaussian r Nrmal Prbability Density Functin
More informationLead/Lag Compensator Frequency Domain Properties and Design Methods
Lectures 6 and 7 Lead/Lag Cmpensatr Frequency Dmain Prperties and Design Methds Definitin Cnsider the cmpensatr (ie cntrller Fr, it is called a lag cmpensatr s K Fr s, it is called a lead cmpensatr Ntatin
More informationCOMP 551 Applied Machine Learning Lecture 11: Support Vector Machines
COMP 551 Applied Machine Learning Lecture 11: Supprt Vectr Machines Instructr: (jpineau@cs.mcgill.ca) Class web page: www.cs.mcgill.ca/~jpineau/cmp551 Unless therwise nted, all material psted fr this curse
More informationLongitudinal Dispersion
Updated: 3 Otber 017 Print verin Leture #10 (River & Stream, nt) Chapra, L14 (nt.) David A. Rekhw CEE 577 #10 1 Lngitudinal Diperin Frm Fiher et al., 1979 m/ m -1 E U B 0 011 HU. * Width (m) Where the
More informationPart a: Writing the nodal equations and solving for v o gives the magnitude and phase response: tan ( 0.25 )
+ - Hmewrk 0 Slutin ) In the circuit belw: a. Find the magnitude and phase respnse. b. What kind f filter is it? c. At what frequency is the respnse 0.707 if the generatr has a ltage f? d. What is the
More informationMeshless implementations of Local Integral Equations for bending of thin plates
Bundary Element and Other Meh Redutin Methd XXXIV 15 Mehle implementatin f Lal Integral Euatin fr bending f thin plate V. Sladek, J. Sladek & L. Satr Intitute f Cntrutin and Arhiteture, Slvak Aademy f
More informationSupport-Vector Machines
Supprt-Vectr Machines Intrductin Supprt vectr machine is a linear machine with sme very nice prperties. Haykin chapter 6. See Alpaydin chapter 13 fr similar cntent. Nte: Part f this lecture drew material
More informationA solution of certain Diophantine problems
A slutin f certain Diphantine prblems Authr L. Euler* E7 Nvi Cmmentarii academiae scientiarum Petrplitanae 0, 1776, pp. 8-58 Opera Omnia: Series 1, Vlume 3, pp. 05-17 Reprinted in Cmmentat. arithm. 1,
More informationCHAPTER 4 DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL
98 CHAPTER DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL INTRODUCTION The deign of ytem uing tate pace model for the deign i called a modern control deign and it i
More informationLinear System Fundamentals
Linear Sytem Fundamental MEM 355 Performance Enhancement of Dynamical Sytem Harry G. Kwatny Department of Mechanical Engineering & Mechanic Drexel Univerity Content Sytem Repreentation Stability Concept
More informationCambridge Assessment International Education Cambridge Ordinary Level. Published
Cambridge Assessment Internatinal Educatin Cambridge Ordinary Level ADDITIONAL MATHEMATICS 4037/1 Paper 1 Octber/Nvember 017 MARK SCHEME Maximum Mark: 80 Published This mark scheme is published as an aid
More informationCh. 3: Inverse Kinematics Ch. 4: Velocity Kinematics. The Interventional Centre
Ch. : Invee Kinemati Ch. : Velity Kinemati The Inteventinal Cente eap: kinemati eupling Apppiate f ytem that have an am a wit Suh that the wit jint ae ae aligne at a pint F uh ytem, we an plit the invee
More informationECE 2100 Circuit Analysis
ECE 2100 Circuit Analysis Lessn 25 Chapter 9 & App B: Passive circuit elements in the phasr representatin Daniel M. Litynski, Ph.D. http://hmepages.wmich.edu/~dlitynsk/ ECE 2100 Circuit Analysis Lessn
More informationRoot Locus Diagram. Root loci: The portion of root locus when k assume positive values: that is 0
Objective Root Locu Diagram Upon completion of thi chapter you will be able to: Plot the Root Locu for a given Tranfer Function by varying gain of the ytem, Analye the tability of the ytem from the root
More information[COLLEGE ALGEBRA EXAM I REVIEW TOPICS] ( u s e t h i s t o m a k e s u r e y o u a r e r e a d y )
(Abut the final) [COLLEGE ALGEBRA EXAM I REVIEW TOPICS] ( u s e t h i s t m a k e s u r e y u a r e r e a d y ) The department writes the final exam s I dn't really knw what's n it and I can't very well
More informationLHS Mathematics Department Honors Pre-Calculus Final Exam 2002 Answers
LHS Mathematics Department Hnrs Pre-alculus Final Eam nswers Part Shrt Prblems The table at the right gives the ppulatin f Massachusetts ver the past several decades Using an epnential mdel, predict the
More informationHypothesis Tests for One Population Mean
Hypthesis Tests fr One Ppulatin Mean Chapter 9 Ala Abdelbaki Objective Objective: T estimate the value f ne ppulatin mean Inferential statistics using statistics in rder t estimate parameters We will be
More informationFinite Automata. Human-aware Robo.cs. 2017/08/22 Chapter 1.1 in Sipser
Finite Autmata 2017/08/22 Chapter 1.1 in Sipser 1 Last time Thery f cmputatin Autmata Thery Cmputability Thery Cmplexity Thery Finite autmata Pushdwn autmata Turing machines 2 Outline fr tday Finite autmata
More informationChem 116 POGIL Worksheet - Week 8 Equilibrium Continued - Solutions
Chem 116 POGIL Wrksheet - Week 8 Equilibrium Cntinued - Slutins Key Questins 1. Cnsider the fllwing reatin At 425 C, an equilibrium mixture has the fllwing nentratins What is the value f K? -2 [HI] = 1.01
More informationThis document is downloaded from DR-NTU, Nanyang Technological University Library, Singapore.
Thi dument i dwnladed frm DR-NTU Nanyang Tehnlgial Univerity Library Singapre. Title An advaned-time-haring withing trategy fr multipleinput buk nverter Authr() Xian Liang; Wang Yuyi Citatin Xian L. &
More informationPhysical Layer: Outline
18-: Intrductin t Telecmmunicatin Netwrks Lectures : Physical Layer Peter Steenkiste Spring 01 www.cs.cmu.edu/~prs/nets-ece Physical Layer: Outline Digital Representatin f Infrmatin Characterizatin f Cmmunicatin
More informationLesson Plan. Recode: They will do a graphic organizer to sequence the steps of scientific method.
Lessn Plan Reach: Ask the students if they ever ppped a bag f micrwave ppcrn and nticed hw many kernels were unppped at the bttm f the bag which made yu wnder if ther brands pp better than the ne yu are
More informationTuring Machines. Human-aware Robotics. 2017/10/17 & 19 Chapter 3.2 & 3.3 in Sipser Ø Announcement:
Turing Machines Human-aware Rbtics 2017/10/17 & 19 Chapter 3.2 & 3.3 in Sipser Ø Annuncement: q q q q Slides fr this lecture are here: http://www.public.asu.edu/~yzhan442/teaching/cse355/lectures/tm-ii.pdf
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 informationGrumman F-14 Tomcat Control Design BY: Chike Uduku
Grumman F-4 Tmcat Cntrl Deign BY: Chike duku I. Atract SECTIONS II. III. IV. Deign jective eaured Cntant Deign V. Reult VI. VII. Cncluin Cmplete atla Cde I. Atract Deigning cntrller fr fighter jet i a
More informationCompressibility Effects
Definitin f Cmpressibility All real substances are cmpressible t sme greater r lesser extent; that is, when yu squeeze r press n them, their density will change The amunt by which a substance can be cmpressed
More information1 The limitations of Hartree Fock approximation
Chapter: Pst-Hartree Fck Methds - I The limitatins f Hartree Fck apprximatin The n electrn single determinant Hartree Fck wave functin is the variatinal best amng all pssible n electrn single determinants
More informationNUMBERS, MATHEMATICS AND EQUATIONS
AUSTRALIAN CURRICULUM PHYSICS GETTING STARTED WITH PHYSICS NUMBERS, MATHEMATICS AND EQUATIONS An integral part t the understanding f ur physical wrld is the use f mathematical mdels which can be used t
More informationTrigonometric Ratios Unit 5 Tentative TEST date
1 U n i t 5 11U Date: Name: Trignmetric Ratis Unit 5 Tentative TEST date Big idea/learning Gals In this unit yu will extend yur knwledge f SOH CAH TOA t wrk with btuse and reflex angles. This extensin
More informationNOTE ON APPELL POLYNOMIALS
NOTE ON APPELL POLYNOMIALS I. M. SHEFFER An interesting characterizatin f Appell plynmials by means f a Stieltjes integral has recently been given by Thrne. 1 We prpse t give a secnd such representatin,
More informationChapter 5. Root Locus Techniques
Chapter 5 Rt Lcu Techique Itrducti Sytem perfrmace ad tability dt determied dby cled-lp l ple Typical cled-lp feedback ctrl ytem G Ope-lp TF KG H Zer -, - Ple 0, -, - K Lcati f ple eaily fud Variati f
More informationLecture 6: Phase Space and Damped Oscillations
Lecture 6: Phase Space and Damped Oscillatins Oscillatins in Multiple Dimensins The preius discussin was fine fr scillatin in a single dimensin In general, thugh, we want t deal with the situatin where:
More informationIAML: Support Vector Machines
1 / 22 IAML: Supprt Vectr Machines Charles Suttn and Victr Lavrenk Schl f Infrmatics Semester 1 2 / 22 Outline Separating hyperplane with maimum margin Nn-separable training data Epanding the input int
More informationChapter 3 Kinematics in Two Dimensions; Vectors
Chapter 3 Kinematics in Tw Dimensins; Vectrs Vectrs and Scalars Additin f Vectrs Graphical Methds (One and Tw- Dimensin) Multiplicatin f a Vectr b a Scalar Subtractin f Vectrs Graphical Methds Adding Vectrs
More informationLaPlace Transforms in Design and Analysis of Circuits Part 2: Basic Series Circuit Analysis
LaPlace Tranfrm in Deign and Analyi f Circuit Part : Baic Serie Circuit Analyi Cure N: E- Credit: PDH Thma G. Bertenhaw, Ed.D., P.E. Cntinuing Educatin and Develpment, Inc. 9 Greyridge Farm Curt Stny Pint,
More informationBuilding to Transformations on Coordinate Axis Grade 5: Geometry Graph points on the coordinate plane to solve real-world and mathematical problems.
Building t Transfrmatins n Crdinate Axis Grade 5: Gemetry Graph pints n the crdinate plane t slve real-wrld and mathematical prblems. 5.G.1. Use a pair f perpendicular number lines, called axes, t define
More informationLecture 13 - Boost DC-DC Converters. Step-Up or Boost converters deliver DC power from a lower voltage DC level (V d ) to a higher load voltage V o.
ecture 13 - Bt C-C Cnverter Pwer Electrnic Step-Up r Bt cnverter eliver C pwer frm a lwer vltage C level ( ) t a higher la vltage. i i i + v i c T C (a) + R (a) v 0 0 i 0 R1 t n t ff + t T i n T t ff =
More informationENGI 4430 Parametric Vector Functions Page 2-01
ENGI 4430 Parametric Vectr Functins Page -01. Parametric Vectr Functins (cntinued) Any nn-zer vectr r can be decmpsed int its magnitude r and its directin: r rrˆ, where r r 0 Tangent Vectr: dx dy dz dr
More informationNote: Please use the actual date you accessed this material in your citation.
MIT OpenCureWare http://w.mit.edu 6.03/ESD.03J Eletrmagneti and ppliatin, Fall 005 Pleae ue the fllwing itatin frmat: Marku Zahn, Erih Ippen, and David Staelin, 6.03/ESD.03J Eletrmagneti and ppliatin,
More informationMODULE 1. e x + c. [You can t separate a demominator, but you can divide a single denominator into each numerator term] a + b a(a + b)+1 = a + b
. REVIEW OF SOME BASIC ALGEBRA MODULE () Slving Equatins Yu shuld be able t slve fr x: a + b = c a d + e x + c and get x = e(ba +) b(c a) d(ba +) c Cmmn mistakes and strategies:. a b + c a b + a c, but
More informationExam Review Trigonometry
Exam Review Trignmetry (Tyler, Chris, Hafsa, Nasim, Paniz,Tng) Similar Triangles Prving Similarity (AA, SSS, SAS) ~ Tyler Garfinkle 3 Types f Similarities: 1. Side Side Side Similarity (SSS) If three pairs
More informationDistributions, spatial statistics and a Bayesian perspective
Distributins, spatial statistics and a Bayesian perspective Dug Nychka Natinal Center fr Atmspheric Research Distributins and densities Cnditinal distributins and Bayes Thm Bivariate nrmal Spatial statistics
More informationANSWER KEY FOR MATH 10 SAMPLE EXAMINATION. Instructions: If asked to label the axes please use real world (contextual) labels
ANSWER KEY FOR MATH 10 SAMPLE EXAMINATION Instructins: If asked t label the axes please use real wrld (cntextual) labels Multiple Chice Answers: 0 questins x 1.5 = 30 Pints ttal Questin Answer Number 1
More informationCHAPTER 24: INFERENCE IN REGRESSION. Chapter 24: Make inferences about the population from which the sample data came.
MATH 1342 Ch. 24 April 25 and 27, 2013 Page 1 f 5 CHAPTER 24: INFERENCE IN REGRESSION Chapters 4 and 5: Relatinships between tw quantitative variables. Be able t Make a graph (scatterplt) Summarize the
More informationGain and Phase Margins Based Delay Dependent Stability Analysis of Two- Area LFC System with Communication Delays
Gain and Phae Margin Baed Delay Dependent Stability Analyi of Two- Area LFC Sytem with Communication Delay Şahin Sönmez and Saffet Ayaun Department of Electrical Engineering, Niğde Ömer Halidemir Univerity,
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 informationDigital Control System
Digital Control Sytem - A D D A Micro ADC DAC Proceor Correction Element Proce Clock Meaurement A: Analog D: Digital Continuou Controller and Digital Control Rt - c Plant yt Continuou Controller Digital
More informationPart 3 Introduction to statistical classification techniques
Part 3 Intrductin t statistical classificatin techniques Machine Learning, Part 3, March 07 Fabi Rli Preamble ØIn Part we have seen that if we knw: Psterir prbabilities P(ω i / ) Or the equivalent terms
More informationCOMP 551 Applied Machine Learning Lecture 9: Support Vector Machines (cont d)
COMP 551 Applied Machine Learning Lecture 9: Supprt Vectr Machines (cnt d) Instructr: Herke van Hf (herke.vanhf@mail.mcgill.ca) Slides mstly by: Class web page: www.cs.mcgill.ca/~hvanh2/cmp551 Unless therwise
More informationFunction notation & composite functions Factoring Dividing polynomials Remainder theorem & factor property
Functin ntatin & cmpsite functins Factring Dividing plynmials Remainder therem & factr prperty Can d s by gruping r by: Always lk fr a cmmn factr first 2 numbers that ADD t give yu middle term and MULTIPLY
More informationAdmissibility Conditions and Asymptotic Behavior of Strongly Regular Graphs
Admissibility Cnditins and Asympttic Behavir f Strngly Regular Graphs VASCO MOÇO MANO Department f Mathematics University f Prt Oprt PORTUGAL vascmcman@gmailcm LUÍS ANTÓNIO DE ALMEIDA VIEIRA Department
More informationConservation of Momentum
Cnervatin f Mmentum PES 1150 Prelab Quetin Name: Lab Statin: 003 ** Diclaimer: Thi re-lab i nt t be cied, in whle r in art, unle a rer reference i made a t the urce. (It i trngly recmmended that yu ue
More informationLecture 13: Markov Chain Monte Carlo. Gibbs sampling
Lecture 13: Markv hain Mnte arl Gibbs sampling Gibbs sampling Markv chains 1 Recall: Apprximate inference using samples Main idea: we generate samples frm ur Bayes net, then cmpute prbabilities using (weighted)
More informationLecture 7: Damped and Driven Oscillations
Lecture 7: Damped and Driven Oscillatins Last time, we fund fr underdamped scillatrs: βt x t = e A1 + A csω1t + i A1 A sinω1t A 1 and A are cmplex numbers, but ur answer must be real Implies that A 1 and
More informationThermodynamics Partial Outline of Topics
Thermdynamics Partial Outline f Tpics I. The secnd law f thermdynamics addresses the issue f spntaneity and invlves a functin called entrpy (S): If a prcess is spntaneus, then Suniverse > 0 (2 nd Law!)
More informationChapter 3. Electric Flux Density, Gauss s Law and Divergence
Chapter 3. Electric Flu Denity, Gau aw and Diergence Hayt; 9/7/009; 3-1 3.1 Electric Flu Denity Faraday Eperiment Cncentric phere filled with dielectric material. + i gien t the inner phere. - i induced
More informationCS 477/677 Analysis of Algorithms Fall 2007 Dr. George Bebis Course Project Due Date: 11/29/2007
CS 477/677 Analysis f Algrithms Fall 2007 Dr. Gerge Bebis Curse Prject Due Date: 11/29/2007 Part1: Cmparisn f Srting Algrithms (70% f the prject grade) The bjective f the first part f the assignment is
More information( ) kt. Solution. From kinetic theory (visualized in Figure 1Q9-1), 1 2 rms = 2. = 1368 m/s
.9 Kinetic Mlecular Thery Calculate the effective (rms) speeds f the He and Ne atms in the He-Ne gas laser tube at rm temperature (300 K). Slutin T find the rt mean square velcity (v rms ) f He atms at
More informationELEC 372 LECTURE NOTES, WEEK 11 Dr. Amir G. Aghdam Concordia University
ELEC 37 LECTURE NOTES, WEE Dr Amir Aghdam Cncrdia Univrity Part f th nt ar adaptd frm th matrial in th fllwing rfrnc: Mdrn Cntrl Sytm by Richard C Drf and Rbrt H Bihp, Prntic Hall Fdback Cntrl f Dynamic
More informationComputational modeling techniques
Cmputatinal mdeling techniques Lecture 2: Mdeling change. In Petre Department f IT, Åb Akademi http://users.ab.fi/ipetre/cmpmd/ Cntent f the lecture Basic paradigm f mdeling change Examples Linear dynamical
More informationDataflow Analysis and Abstract Interpretation
Dataflw Analysis and Abstract Interpretatin Cmputer Science and Artificial Intelligence Labratry MIT Nvember 9, 2015 Recap Last time we develped frm first principles an algrithm t derive invariants. Key
More informationRoot locus ( )( ) The given TFs are: 1. Using Matlab: >> rlocus(g) >> Gp1=tf(1,poly([0-1 -2])) Transfer function: s^3 + 3 s^2 + 2 s
The given TFs are: 1 1() s = s s + 1 s + G p, () s ( )( ) >> Gp1=tf(1,ply([0-1 -])) Transfer functin: 1 ----------------- s^ + s^ + s Rt lcus G 1 = p ( s + 0.8 + j)( s + 0.8 j) >> Gp=tf(1,ply([-0.8-*i
More informationMODULE 5 Lecture No: 5 Extraterrestrial Radiation
1 P age Principle and Perfrmance f Slar Energy Thermal Sytem: A Web Cure by V.V.Satyamurty MODULE 5 Lecture N: 5 Extraterretrial Radiatin In Mdule 5, Lecture N. 5 deal with 5.1 INTRODUCTION 5. EXTRA TERRESTRIAL
More informationEE Control Systems LECTURE 14
Updated: Tueday, March 3, 999 EE 434 - Control Sytem LECTURE 4 Copyright FL Lewi 999 All right reerved ROOT LOCUS DESIGN TECHNIQUE Suppoe the cloed-loop tranfer function depend on a deign parameter k We
More informationB. Definition of an exponential
Expnents and Lgarithms Chapter IV - Expnents and Lgarithms A. Intrductin Starting with additin and defining the ntatins fr subtractin, multiplicatin and divisin, we discvered negative numbers and fractins.
More informationRELIABILITY OF REPAIRABLE k out of n: F SYSTEM HAVING DISCRETE REPAIR AND FAILURE TIMES DISTRIBUTIONS
www.arpapre.com/volume/vol29iue1/ijrras_29_1_01.pdf RELIABILITY OF REPAIRABLE k out of n: F SYSTEM HAVING DISCRETE REPAIR AND FAILURE TIMES DISTRIBUTIONS Sevcan Demir Atalay 1,* & Özge Elmataş Gültekin
More informationDetermining the Accuracy of Modal Parameter Estimation Methods
Determining the Accuracy f Mdal Parameter Estimatin Methds by Michael Lee Ph.D., P.E. & Mar Richardsn Ph.D. Structural Measurement Systems Milpitas, CA Abstract The mst cmmn type f mdal testing system
More informationCorrection for Simple System Example and Notes on Laplace Transforms / Deviation Variables ECHE 550 Fall 2002
Correction for Simple Sytem Example and Note on Laplace Tranform / Deviation Variable ECHE 55 Fall 22 Conider a tank draining from an initial height of h o at time t =. With no flow into the tank (F in
More informationOn the Origin of the Special Relativity Anomalies
On the Origin f the Speial Relatiity Anmalies Radwan M. Kassir February 2015 radwan.elkassir@dargrup.m ABSTRACT In this paper, the nlusie rigin f the Speial Relatiity (SR) mathematial nflits identified
More informationBootstrap Method > # Purpose: understand how bootstrap method works > obs=c(11.96, 5.03, 67.40, 16.07, 31.50, 7.73, 11.10, 22.38) > n=length(obs) >
Btstrap Methd > # Purpse: understand hw btstrap methd wrks > bs=c(11.96, 5.03, 67.40, 16.07, 31.50, 7.73, 11.10, 22.38) > n=length(bs) > mean(bs) [1] 21.64625 > # estimate f lambda > lambda = 1/mean(bs);
More informationSolutions to Problems in Hydromechanics 3. Open Channel Flow General + Energy Principle I m /s
Sltin t Prblem in Hdrmehani Open Channel Flw General + Energ Priniple I. (F.7) Cr-etinal area: A = 0.6 0 = 8 m A = 5. 6 = 0.6 m A = 0.6 60 = 6 m Determine the ttal flw in the mpite hannel: Q= A + A + A
More informationL a) Calculate the maximum allowable midspan deflection (w o ) critical under which the beam will slide off its support.
ecture 6 Mderately arge Deflectin Thery f Beams Prblem 6-1: Part A: The department f Highways and Public Wrks f the state f Califrnia is in the prcess f imprving the design f bridge verpasses t meet earthquake
More informationLecture 4. Chapter 11 Nise. Controller Design via Frequency Response. G. Hovland 2004
METR4200 Advanced Control Lecture 4 Chapter Nie Controller Deign via Frequency Repone G. Hovland 2004 Deign Goal Tranient repone via imple gain adjutment Cacade compenator to improve teady-tate error Cacade
More informationMore Tutorial at
Answer each questin in the space prvided; use back f page if extra space is needed. Answer questins s the grader can READILY understand yur wrk; nly wrk n the exam sheet will be cnsidered. Write answers,
More informationCHM112 Lab Graphing with Excel Grading Rubric
Name CHM112 Lab Graphing with Excel Grading Rubric Criteria Pints pssible Pints earned Graphs crrectly pltted and adhere t all guidelines (including descriptive title, prperly frmatted axes, trendline
More informationStability. ME 344/144L Prof. R.G. Longoria Dynamic Systems and Controls/Lab. Department of Mechanical Engineering The University of Texas at Austin
Stability The tability of a ytem refer to it ability or tendency to eek a condition of tatic equilibrium after it ha been diturbed. If given a mall perturbation from the equilibrium, it i table if it return.
More information4th Indian Institute of Astrophysics - PennState Astrostatistics School July, 2013 Vainu Bappu Observatory, Kavalur. Correlation and Regression
4th Indian Institute f Astrphysics - PennState Astrstatistics Schl July, 2013 Vainu Bappu Observatry, Kavalur Crrelatin and Regressin Rahul Ry Indian Statistical Institute, Delhi. Crrelatin Cnsider a tw
More informationExperiment #3. Graphing with Excel
Experiment #3. Graphing with Excel Study the "Graphing with Excel" instructins that have been prvided. Additinal help with learning t use Excel can be fund n several web sites, including http://www.ncsu.edu/labwrite/res/gt/gt-
More informationFall 2013 Physics 172 Recitation 3 Momentum and Springs
Fall 03 Physics 7 Recitatin 3 Mmentum and Springs Purpse: The purpse f this recitatin is t give yu experience wrking with mmentum and the mmentum update frmula. Readings: Chapter.3-.5 Learning Objectives:.3.
More informationMath 105: Review for Exam I - Solutions
1. Let f(x) = 3 + x + 5. Math 105: Review fr Exam I - Slutins (a) What is the natural dmain f f? [ 5, ), which means all reals greater than r equal t 5 (b) What is the range f f? [3, ), which means all
More information