MULTIVARIABLE CONTROLLER TUNING

Size: px
Start display at page:

Download "MULTIVARIABLE CONTROLLER TUNING"

Transcription

1 MULTIVARIABLE CONTROLLER TUNING Karl H. Johansson, Bn Jams, Gryham F. Bryant, and Karl J. Åström Abstract Th problm of tuning individual loops in a multivariabl controllr is invstigatd. It is shown how th prformanc of a spcific loop rlats to a row in th controllr matrix. Svral intrprtations of this rlation ar givn. An algorithm is also prsntd that stimats th modl rquird for th tuning via a rlay fdback xprimnt. Th algorithm dos not nd any prior information about th systm or th controllr. Th rsults ar illustratd by an xampl.. Introduction Poorly tund control loops rprsnt a larg conomic cost for industry [5, 4]. Control paramtrs ar oftn st to dfault valus or ar manually tund in an ad hoc way. Th rason for this is that thr is a grat lack of tools for tuning industrial controllrs systmatically. Nowadays thr xist mthods for automatic tuning of SISO control loops, which hav bn widly accptd and implmntd in svral commrcial controllrs []. Many control loops ar, howvr, coupld and th intraction has to b considrd in th control dsign to gain improvd prformanc [8]. Most modrn multivariabl control dsign mthods rquir a full modl of th procss []. In many cass such a modl is not availabl and physical modling or systm idntification may rquir a prohibitiv nginring ffort. Furthrmor, it is hard, or impossibl, to impos a crtain control structur on standard multivariabl dsign mthods. Thrfor, thr is a nd for simpl mthods of tuning multivariabl controllrs; particularly mthods that compromis optimality for nginring fficincy. This papr focus on th problm of rtuning an xisting multivariabl control systm. A framwork is dvlopd whr it is possibl to driv th influnc of rtuning on loop on th ovrall closd-loop prformanc. A badly tund loop can in this way b improvd by changing crtain lmnts of th controllr matrix. Tuning a loop corrsponds to changing a row in th Dpartmnt of Automatic Control, Lund Institut of Tchnology, Box 8, S- Lund, Swdn, fkall,kjag@control.lth.s. Exposur Managmnt, Bank of Amrica, Elmfild Road, Bromly, London, Unitd Kingdom, @compusrv.com. Industrial Systms Group, Cntr for Procss Systms Enginring, Imprial Collg of Scinc, Tchnology and Mdicin, Exhibition Road, London, SW7 BT, Unitd Kingdom, g.bryant@ic.ac.uk. controllr matrix; hnc, to solv a SIMO control dsign problm. Svral quantitis usful for stimating th influnc of a controllr row on th closd-loop systm ar drivd. Th information rquird for this typ of dsign is also discussd togthr with how this information can b obtaind. It is shown that no prior knowldg of th procss dynamics or of th controllr dynamics is ndd, if a modling xprimnt basd on rlay fdback is usd. In xisting work on xtnding th auto-tuning mthod for SISO control systms dvlopd in [] to MIMO systms, ithr on rlay is usd for ach xprimnt by closing on loop at a tim [7, 6, 9, 7] or all loops ar st undr rlay fdback simultanously [3, 9,, ]. A major drawback with th lattr approach is that instad of giving stationary limit cycls th rlays can induc vry complicatd oscillations [9, 9]. Thr xist no rsults in trms of plant data for whn this may or may not happn. Basd on a succssful rlay xprimnt a controllr is dsignd. Most authors limit th control structur to a dcntralizd configuration of SISO PID controllrs [, 9, 3, 7, ]. Dcoupling dsign is drivd in [6, ]. Tuning cascad controllrs (MISO controllrs) is considrd in [7, ]. For a survy on rlay fdback mthods s [3, 9]. Th outlin of th papr is as follows. Sction prsnts som rsults that ar usful for loop tuning. Rtuning a row in th controllr matrix is formalizd. In Sction 3 it is shown that th rquird information about th systm can b obtaind from an xprimnt with SISO rlay fdback. Sction 4 dscribs an application to a modl of a nw laboratory procss. Som concluding rmarks ar givn in Sction 5. An xtndd vrsion of this papr is givn in [9].. Loop Tuning Suppos that a multivariabl control systm with unsatisfactory closd-loop prformanc is givn. Th basic ida is to adjust crtain lmnts of th controllr matrix in ordr to improv th closd-loop bhavior. In gnral, such an adjustmnt will affct all loops in th systm. Th challng is to obtain this ffct on th dsird loop without dgrading th prformanc of th othr loops. This sction givs rsults which nabls th dsignr to comput th ffct of an adjustmnt of a singl loop on th ovrall closd-loop bhavior.

2 r _ ē ȳ H r m m K G y m K _ G r Figur Opning of control loop m. Notation Assum that thr xists a stabl closd-loop systm comprising a procss G and a nominal controllr K, both with m inputs and m outputs. Dnot th manipulatd variabl or procss input u (u,..., ) T,th controlld variabl or procss output y (y,...,y m ) T, and th rfrnc or st-point r (r,...,r m ) T.Th controllr matrix K acts on th rror signal (,..., m ) T r y.hnc,y Gu and u K.Th aim of th tuning procdur is to improv th prformanc of on loop by adjusting appropriat lmnts of th controllr matrix. Without loss of gnrality, considr loop m and dfin th following partitions: G m m G G, K m m K k. () Partition th vctors u ( T, ) T, y (ȳ T, y m ) T, r ( r T,r m ) T,and (ē T, m ) T corrspondingly, so that (u,..., ) T tc. Thn ε T m K k k + +k m m, whr ε T m (,...,,) and k i, i,...,m,arth lmnts of k. Row m of th controllr matrix K thus contains th coupling from th rror to th control signal. Figur shows th closd-loop systm with th signal path brokn. Any snsibl choic of th controllr row k that improvs th prformanc of loop m, rquirs at last knowldg of th SIMO transfr matrix from to in this partially opn systm. W dnot this transfr matrix H (I+G K ) G and assum that it is stabl. Th block diagram of Figur shows xplicitly th contribution of controllr row m to th fdback control of th systm. Th transfr matrics of th full multivariabl closd-loop systm can asily b dscribd in trms of thos for th systm with H acting as a procss and k as a controllr. In othr words, th multivariabl control dsign problm for G is rducd to a SIMO control problm for H with MISO controllr k. Paramtrization and stability It is simpl to calculat th ffct of nw or rdsignd controllr row lmnts of th singl-loop opning ap- k Figur Contribution of controllr row k. proach. Th input snsitivity function is givn by S i : (I + KG) and th output snsitivity function by S o : (I+ GK). Th diagonal lmnt m of th snsitivity matrix S i capturs much of th prformanc in loop m. By th dfinition of H and k, w hav ε T ms i ε m /( kh). Knowldg of H alon is thus sufficint to comput th transfr function for loop m that rsults from a particular choic of k. Th closd-loop transfr matrics ar affin functions in th Youla paramtr Q : (I+KG) K if G is stabl []. For xampl, th snsitivity and complmntary snsitivity matrics with rfrnc to procss inputs ar S i I QG and T i QG, rspctivly, and th corrsponding matrics with rfrnc to procss outputs ar S o I GQ and T o GQ. Th closdloop transfr matrics ar also affin functions in q : k/( kh). This mvctor of transfr functions is th Youla paramtr for th partially opn systm. Som calculations giv th rlation btwn q and Q as Q K (I + G K ) + K H q(i + G K ). Paramtrization of stabilizing controllr rows and columns ar studid in [8]. Naturally, any adjustmnts of controllr row m must b mad in such a way that th closd-loop systm rmains stabl. Th following rsult follows from th Nyquist thorm. Assum th closd-loop systm is stabl with controllr row k. Ltkb rplacd by k, whr k is such that no unstabl mods ar canclld and that th numbr of opn-loop RHP pols dos not chang. Thn th adjustd closd-loop systm rmains stabl if and only if N ( kh,) N( kh,), whrn (f(s),z)is th numbr of clockwis ncirclmnts of th point z by th imag of th usual Nyquist contour D N undr th map f as it is travrsd in a clockwis dirction.

3 .5 H.5 K G r Figur Thr important points on th Nyquist curv. W ε T m 3. Extndd Rlay Exprimnt A rlay fdback xprimnt is a simpl and robust way of doing closd-loop idntification. Th stup for th original SISO xprimnt is simply to rplac th SISO controllr by a rlay []. Th main advantags of an idntification xprimnt basd on rlay fdback ar () that th frquncy of th xcitation signal is nar th cross-ovr frquncy of th opn-loop systm, () that th xprimnt is don in closd loop, and (3) that no prior knowldg about th procss dynamics is ndd. Th frquncy of th rlay output is clos to optimum in th sns that it is in th band whr th stimatd modl has to b accurat to support a satisfying control dsign. Evn if no controllr is prsnt in th loop during th xprimnt, th rlay itslf givs a high-gain fdback. This mans, for instanc, that th procss is automatically kpt clos to its oprating point during th xprimnt. A drawback with th original rlay fdback xprimnt is in som cass its lack of xcitation. Thrfor, w introduc a modification of th standard rlay xprimnt, by simply stimating two points on th Nyquist curv instad of on. It is wll-known that with a filtr in sris with th rlay, any point on th Nyquist curv can b stimatd []. This ida has bn xplord for SISO systms in [5, 6]. Prsson [3] invstigatd th amount of procss information ndd for control dsign in numbr of points and thir location on th Nyquist curv. Thr crucial points ar markd with crosss in Figur 3. Point is dtrmind by a standard rlay xprimnt, whras Point is dtrmind from an xprimnt with a rlay and an intgrator in sris. Th mthod can b intrprtd as putting a filtr W in sris with th rlay. Th filtr is initially st to W and thn to W /s. Togthr with stady-stat data, th gaind information is sufficint to driv a modl of th form b s+b G(s). () s 3 +a s +a s+a 3 Th controllr tuning dscribd in Sction is basd on knowldg of th column vctor H. Th st-up for Figur 4 Rlay xprimnt for idntifying H. an xtndd rlay xprimnt to idntify H is shown in Figur 4, compar with Figur. Th block with ε T m picks out rror signal m. Th rlay is thus connctd btwn W m and. This givs an oscillation with frquncis dtrmind by H m, which is typically th most important transfr function for controllr tuning in loop m. From masuring ē and m, w can stimat all lmnts of H. Wsummarizthmthodinth following algorithm. ALGORITHM SIMO RELAY EXPERIMENT. St W and wait for a stationary oscillation. Masur th frquncy ω and driv th rspons for ach lmnt H i.. St W /s and wait for a stationary oscillation. Masur th frquncy ω and driv th rspons for ach lmnt H i. 3. Frz th rlay output and wait for stadystat and driv th stady-stat gains for ach lmnt H i. 4. Estimat H i as in () basd on th rsponss and th corrsponding frquncis ω and ω. Th amounts of tim rquird for a stationary oscillation in Stp and Stp ar small. Exprimnts show that stationarity is oftn rachd aftr thr four rlay switchs. Not that Algorithm automatically givs highst priority to th last lmnt of H in th sns that th xcitation frquncis ar adjustd to suit H m.this mans also that if H,...,H m giv small rsponss around th cross-ovr frquncy of H m, thn th stimats of H,...,H m ar probably poor. Howvr, bcaus th lmnts ar small, th lack of accuracy has only a small influnc on th control prformanc.

4 u u 5 5 tim Figur 5 Extndd rlay xprimnt for minimum phas systm. Th rror signal (dashd) is ngligibl compard to (solid) tim Figur 7 Extndd rlay xprimnt for nonminimum phas systm. Th rror signals (dashd) and (solid) ar of th sam magnitud. Im R Figur 6 Nyquist curvs of H for minimum phas systm. Th crosss ar stimatd frquncy points from rlay fdback xprimnts. Th small crosss corrspond to H and th larg to H. A third-ordr stimat of H is also shown (solid lin). Th frquncy rspons of H is ngligibl compard to th rspons of H. 4. Exampl In this sction th rtuning procdur is applid to a multivariabl lvl control problm. Th considrd systm is a normalizd modl of th quadrupl-tank laboratory procss dscribd in [9, ]. Th systm including modls for actuators and snsors is givn by G 5 (s + ) γ γ s + (s + ) γ γ (s + ) s +. Th paramtrs γ,γ [,]ar dtrmind by how two valvs ar st prior to an xprimnt. Th systm G has a RHP zro if and only if γ + γ (,].Nxt w study th systm for on minimum-phas stting and on nonminimum-phas stting. Minimum phas systm Lt γ γ 4/5. Thn G has zros in 5/4and 3/4, so th systm is minimum Th rtuning procdur in this papr has bn applid to th ral laboratory procss in [4]. Im R Figur 8 Nyquist curvs of H for nonminimum phas systm, compar Figur 6. Th frquncy rsponss of H and H ar of th sam magnitud. phas. Lt K diag{, } b th initial controllr. Th rspons of th xtndd rlay xprimnt dscribd in Algorithm is shown in Figur 5. Th rspons of is small compard to. This is furthr illustratd in Figur 6, whr th small crosss ar th stimatd frquncy points for H and th larg crosss th points for H. Th dashd curvs ar th Nyquist curvs for th tru systms, whras th solid curv is a third-ordr stimat of H. Th rsult from th rlay xprimnt indicats that w can nglct th influnc of H and simply rtun th last lmnt of k. Th PI controllr k (, (s + 3)/s ) givs th pols 4.9 and.±4.6ifor th scond diagonal lmnt of S i. Not that th tuning hr corrsponds to applying SISO mthods. For this xampl th MIMO charactristics of th systm ar insignificant. Nonminimum phas systm Lt us now chang th valvs so that γ γ /5. Thn G has zros in 5/ and/, so th systm is nonminimum phas. Lt K diag{.,.} b th initial controllr. Figur 7 shows th rsult of th rlay xprimnt. Th stimatd Nyquist curvs (solid) ar shown in Figur 8, togthr with th tru ons (dashd). W

5 s that th intraction is svr, so it is probably not sufficint to only rtun th scond loop. If a rlay xprimnt is also don in th first loop, it is straightforward to driv a multivariabl controllr, for xampl basd on dcoupling. 5. Conclusions It was shown how a poorly tund multivariabl controllr can b rtund through a simpl closd-loop xprimnt basd on rlay fdback and controllr row dsign. In particular, th cas with on bad loop was discussd. Th standard SISO rlay fdback xprimnt in [] was xtndd to giv bttr xcitation and a mor accurat modl, which sms to b ncssary for many MIMO control dsigns. Svral rsults on how a row in th controllr matrix affcts th closd-loop prformanc wr drivd. No fully automatic procdur was dscribd in th sns of automatic tuning for SISO systms. It is blivd that this can only b don if th considrd class of systms is mor limitd than in this papr. It was pointd out through an xampl that for simpl multivariabl control systms th proposd mthod agrs with automatic SISO tuning. For difficult MIMO control problms th mthod still provids a solid ground for controllr dsign. 6. Rfrncs [] K. J. ÅSTRÖM and T. HÄGGLUND. Automatic tuning of simpl rgulators with spcifications on phas and amplitud margins. Automatica,, pp , 984. [] K. J. ÅSTRÖM and T. HÄGGLUND. PID Controllrs: Thory, Dsign, and Tuning. Instrumnt Socity of Amrica, Rsarch Triangl Park, NC, scond dition, 995. [3] K. J. ÅSTRÖM, T.H.LEE, K.K.TAN, and K. H. JOHANS- SON. Rcnt advancs in rlay fdback mthods a survy. In IEEE SMC Confrnc, pp. 66 6, Vancouvr, WA, 995. Invitd papr. [4] W. L. BIALKOWSKI. Drams vs rality: A viw from both sids of th gap. In Control Systms 9, Whistlr, B.C., Canada, 99. [5] D. B. ENDER. Procss control prformanc: Not as good as you think. Control Enginring, 4:, pp. 8 9, 993. [6] M. FRIMAN and K. V. WALLER. Autotuning of multiloop control systms. Ind. Eng. Chm. Rs., 33, pp , 994. [7] C. C. HANG, A.P.LOH, and V. U. VASNANI. Rlay fdback auto-tuning of cascad controllrs. IEEE Trans. on Control Systms Tchnology, :, pp. 4 45, 994. In 34th IEEE Confrnc on Dcision and Control, Nw Orlans, LA, 995. [9] K. H. JOHANSSON. Rlay fdback and multivariabl control. PhD thsis ISRN LUTFD/TFRT--48--SE, Dpartmnt of Automatic Control, Lund Institut of Tchnology, Lund, Swdn, Novmbr 997. [] K. H. JOHANSSON and J. L. R. NUNES. A multivariabl laboratory procss with an adjustabl zro. In 7th Amrican Control Confrnc, Philadlphia, PA, 998. [] J. M. MACIEJOWSKI. Multivariabl Fdback Dsign. Addison-Wsly, Rading, MA, 989. [] Z. J. PALMOR, Y. HALEVI, and N. KRASNEY. Automatic tuning of dcntralizd PID controllrs for TITO procsss. Automatica, 3:7, pp., 995. [3] P. PERSSON. Towards Autonomous PID Control. PhD thsis ISRN LUTFD/TFRT--37--SE, Dpartmnt of Automatic Control, Lund Institut of Tchnology, Lund, Swdn, April 99. [4] V. RECICA. Automatic tuning of multivariabl controllrs. Mastr thsis ISRN LUTFD/TFRT SE, Dpartmnt of Automatic Control, Lund Institut of Tchnology, Lund, Swdn, 998. [5] T. S. SCHEI. A mthod for closd loop automatic tuning of PID controllrs. Automatica, 8:3, pp , 99. [6] T. S. SCHEI. Automatic tuning of PID controllrs basd on transfr function stimation. Automatica, 3:, pp , 994. [7] S.-H. SHEN and C.-C. YU. Us of rlay-fdback tst for automatic tuning of multivariabl systms. AIChE Journal, 4:4, pp , 994. [8] F. G. SHINSKEY. Controlling Multivariabl Procsss. Instrumnt Socity of Amrica, Rsarch Triangl Park, NC, 98. [9] V. U. VASNANI. Towards Rlay Fdback Auto-Tuning of Multi-Loop Systms. PhD thsis, National Univrsity of Singapor, 994. [] Q. G. WANG, B. ZOU, T. H. LEE, and Q. BI. Auto-tuning of multivariabl PID controllrs from dcntralizd rlay fdback. Automatica, 33:3, pp , 997. [] P. ZGORZELSKI, H. UNBEHAUEN, and A. NIEDERLINSKI. A nw simpl dcntralizd adaptiv multivariabl rgulator and its application to multivariabl plants. In IFAC th Trinnial World Congrss, pp , Tallinn, Estonia, 99. [] M. ZHUANG and D. P. ATHERTON. Optimum cascad PID controllr dsign for SISO systms. In IEE Control 94, pp. 66 6, Warwick, 994. [3] M. ZHUANG and D. P. ATHERTON. PID controllr dsign for a TITO systm. IEE Proc. Control Thory Appl., 4:, pp., 994. [8] B. JAMES and G. F. BRYANT. A paramtrization for automatic loop-by-loop multivariabl controllr dsign.

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by D. Klain Vrsion 207.0.05 Corrctions and commnts ar wlcom. Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix A A k I + A + k!

More information

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by Dan Klain Vrsion 28928 Corrctions and commnts ar wlcom Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix () A A k I + A + k!

More information

Construction of asymmetric orthogonal arrays of strength three via a replacement method

Construction of asymmetric orthogonal arrays of strength three via a replacement method isid/ms/26/2 Fbruary, 26 http://www.isid.ac.in/ statmath/indx.php?modul=prprint Construction of asymmtric orthogonal arrays of strngth thr via a rplacmnt mthod Tian-fang Zhang, Qiaoling Dng and Alok Dy

More information

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation.

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation. Lur 7 Fourir Transforms and th Wav Euation Ovrviw and Motivation: W first discuss a fw faturs of th Fourir transform (FT), and thn w solv th initial-valu problm for th wav uation using th Fourir transform

More information

Transitional Probability Model for a Serial Phases in Production

Transitional Probability Model for a Serial Phases in Production Jurnal Karya Asli Lorkan Ahli Matmatik Vol. 3 No. 2 (2010) pag 49-54. Jurnal Karya Asli Lorkan Ahli Matmatik Transitional Probability Modl for a Srial Phass in Production Adam Baharum School of Mathmatical

More information

Estimation of apparent fraction defective: A mathematical approach

Estimation of apparent fraction defective: A mathematical approach Availabl onlin at www.plagiarsarchlibrary.com Plagia Rsarch Library Advancs in Applid Scinc Rsarch, 011, (): 84-89 ISSN: 0976-8610 CODEN (USA): AASRFC Estimation of apparnt fraction dfctiv: A mathmatical

More information

(Upside-Down o Direct Rotation) β - Numbers

(Upside-Down o Direct Rotation) β - Numbers Amrican Journal of Mathmatics and Statistics 014, 4(): 58-64 DOI: 10593/jajms0140400 (Upsid-Down o Dirct Rotation) β - Numbrs Ammar Sddiq Mahmood 1, Shukriyah Sabir Ali,* 1 Dpartmnt of Mathmatics, Collg

More information

Full Order Observer Controller Design for Two Interacting Tank System Based on State Space Approach

Full Order Observer Controller Design for Two Interacting Tank System Based on State Space Approach Intrnational Journal of Application or Innovation in Enginring & Managmnt (IJAIEM) Wb Sit: www.ijaim.org Email: ditor@ijaim.org Volum 6, Issu 7, July 07 ISSN 39-4847 Full Ordr Obsrvr Controllr Dsign for

More information

Recursive Estimation of Dynamic Time-Varying Demand Models

Recursive Estimation of Dynamic Time-Varying Demand Models Intrnational Confrnc on Computr Systms and chnologis - CompSysch 06 Rcursiv Estimation of Dynamic im-varying Dmand Modls Alxandr Efrmov Abstract: h papr prsnts an implmntation of a st of rcursiv algorithms

More information

Application of Vague Soft Sets in students evaluation

Application of Vague Soft Sets in students evaluation Availabl onlin at www.plagiarsarchlibrary.com Advancs in Applid Scinc Rsarch, 0, (6):48-43 ISSN: 0976-860 CODEN (USA): AASRFC Application of Vagu Soft Sts in studnts valuation B. Chtia*and P. K. Das Dpartmnt

More information

COMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, April 04, 2005, 8:35 AM) PART I: CHAPTER TWO COMB MATH.

COMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, April 04, 2005, 8:35 AM) PART I: CHAPTER TWO COMB MATH. C:\Dallas\0_Courss\03A_OpSci_67\0 Cgh_Book\0_athmaticalPrliminaris\0_0 Combath.doc of 8 COPUTER GENERATED HOLOGRAS Optical Scincs 67 W.J. Dallas (onday, April 04, 005, 8:35 A) PART I: CHAPTER TWO COB ATH

More information

Rotor Stationary Control Analysis Based on Coupling KdV Equation Finite Steady Analysis Liu Dalong1,a, Xu Lijuan2,a

Rotor Stationary Control Analysis Based on Coupling KdV Equation Finite Steady Analysis Liu Dalong1,a, Xu Lijuan2,a 204 Intrnational Confrnc on Computr Scinc and Elctronic Tchnology (ICCSET 204) Rotor Stationary Control Analysis Basd on Coupling KdV Equation Finit Stady Analysis Liu Dalong,a, Xu Lijuan2,a Dpartmnt of

More information

EXST Regression Techniques Page 1

EXST Regression Techniques Page 1 EXST704 - Rgrssion Tchniqus Pag 1 Masurmnt rrors in X W hav assumd that all variation is in Y. Masurmnt rror in this variabl will not ffct th rsults, as long as thy ar uncorrlatd and unbiasd, sinc thy

More information

What are those βs anyway? Understanding Design Matrix & Odds ratios

What are those βs anyway? Understanding Design Matrix & Odds ratios Ral paramtr stimat WILD 750 - Wildlif Population Analysis of 6 What ar thos βs anyway? Undrsting Dsign Matrix & Odds ratios Rfrncs Hosmr D.W.. Lmshow. 000. Applid logistic rgrssion. John Wily & ons Inc.

More information

A Propagating Wave Packet Group Velocity Dispersion

A Propagating Wave Packet Group Velocity Dispersion Lctur 8 Phys 375 A Propagating Wav Packt Group Vlocity Disprsion Ovrviw and Motivation: In th last lctur w lookd at a localizd solution t) to th 1D fr-particl Schrödingr quation (SE) that corrsponds to

More information

Difference -Analytical Method of The One-Dimensional Convection-Diffusion Equation

Difference -Analytical Method of The One-Dimensional Convection-Diffusion Equation Diffrnc -Analytical Mthod of Th On-Dimnsional Convction-Diffusion Equation Dalabav Umurdin Dpartmnt mathmatic modlling, Univrsity of orld Economy and Diplomacy, Uzbistan Abstract. An analytical diffrncing

More information

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero.

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero. SETION 6. 57 6. Evaluation of Dfinit Intgrals Exampl 6.6 W hav usd dfinit intgrals to valuat contour intgrals. It may com as a surpris to larn that contour intgrals and rsidus can b usd to valuat crtain

More information

Homotopy perturbation technique

Homotopy perturbation technique Comput. Mthods Appl. Mch. Engrg. 178 (1999) 257±262 www.lsvir.com/locat/cma Homotopy prturbation tchniqu Ji-Huan H 1 Shanghai Univrsity, Shanghai Institut of Applid Mathmatics and Mchanics, Shanghai 272,

More information

CS 361 Meeting 12 10/3/18

CS 361 Meeting 12 10/3/18 CS 36 Mting 2 /3/8 Announcmnts. Homwork 4 is du Friday. If Friday is Mountain Day, homwork should b turnd in at my offic or th dpartmnt offic bfor 4. 2. Homwork 5 will b availabl ovr th wknd. 3. Our midtrm

More information

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark

Answer Homework 5 PHA5127 Fall 1999 Jeff Stark Answr omwork 5 PA527 Fall 999 Jff Stark A patint is bing tratd with Drug X in a clinical stting. Upon admiion, an IV bolus dos of 000mg was givn which yildd an initial concntration of 5.56 µg/ml. A fw

More information

cycle that does not cross any edges (including its own), then it has at least

cycle that does not cross any edges (including its own), then it has at least W prov th following thorm: Thorm If a K n is drawn in th plan in such a way that it has a hamiltonian cycl that dos not cross any dgs (including its own, thn it has at last n ( 4 48 π + O(n crossings Th

More information

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 0 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat th

More information

Elements of Statistical Thermodynamics

Elements of Statistical Thermodynamics 24 Elmnts of Statistical Thrmodynamics Statistical thrmodynamics is a branch of knowldg that has its own postulats and tchniqus. W do not attmpt to giv hr vn an introduction to th fild. In this chaptr,

More information

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes Procdings of th 9th WSEAS Intrnational Confrnc on APPLICATIONS of COMPUTER ENGINEERING A Sub-Optimal Log-Domain Dcoding Algorithm for Non-Binary LDPC Cods CHIRAG DADLANI and RANJAN BOSE Dpartmnt of Elctrical

More information

Gradient-based step response identification of low-order model for time delay systems Rui Yan, Fengwei Chen, Shijian Dong, Tao Liu*

Gradient-based step response identification of low-order model for time delay systems Rui Yan, Fengwei Chen, Shijian Dong, Tao Liu* Gradint-basd stp rspons idntification of low-ordr modl for tim dlay systms Rui Yan, Fngwi Chn, Shijian Dong, ao Liu* Institut of Advancd Control chnology, Dalian Univrsity of chnology, Dalian, 64, P R

More information

Numerical considerations regarding the simulation of an aircraft in the approaching phase for landing

Numerical considerations regarding the simulation of an aircraft in the approaching phase for landing INCAS BULLETIN, Volum, Numbr 1/ 1 Numrical considrations rgarding th simulation of an aircraft in th approaching phas for landing Ionl Cristinl IORGA ionliorga@yahoo.com Univrsity of Craiova, Alxandru

More information

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches. Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M

More information

5.80 Small-Molecule Spectroscopy and Dynamics

5.80 Small-Molecule Spectroscopy and Dynamics MIT OpnCoursWar http://ocw.mit.du 5.80 Small-Molcul Spctroscopy and Dynamics Fall 008 For information about citing ths matrials or our Trms of Us, visit: http://ocw.mit.du/trms. Lctur # 3 Supplmnt Contnts

More information

Data Assimilation 1. Alan O Neill National Centre for Earth Observation UK

Data Assimilation 1. Alan O Neill National Centre for Earth Observation UK Data Assimilation 1 Alan O Nill National Cntr for Earth Obsrvation UK Plan Motivation & basic idas Univariat (scalar) data assimilation Multivariat (vctor) data assimilation 3d-Variational Mthod (& optimal

More information

Sliding Mode Flow Rate Observer Design

Sliding Mode Flow Rate Observer Design Sliding Mod Flow Rat Obsrvr Dsign Song Liu and Bin Yao School of Mchanical Enginring, Purdu Univrsity, Wst Lafaytt, IN797, USA liu(byao)@purdudu Abstract Dynamic flow rat information is ndd in a lot of

More information

Higher order derivatives

Higher order derivatives Robrto s Nots on Diffrntial Calculus Chaptr 4: Basic diffrntiation ruls Sction 7 Highr ordr drivativs What you nd to know alrady: Basic diffrntiation ruls. What you can larn hr: How to rpat th procss of

More information

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA

NEW APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA NE APPLICATIONS OF THE ABEL-LIOUVILLE FORMULA Mirca I CÎRNU Ph Dp o Mathmatics III Faculty o Applid Scincs Univrsity Polithnica o Bucharst Cirnumirca @yahoocom Abstract In a rcnt papr [] 5 th indinit intgrals

More information

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory Ch. 4 Molcular Raction Dynamics 1. Collision Thory Lctur 16. Diffusion-Controlld Raction 3. Th Matrial Balanc Equation 4. Transition Stat Thory: Th Eyring Equation 5. Transition Stat Thory: Thrmodynamic

More information

ph People Grade Level: basic Duration: minutes Setting: classroom or field site

ph People Grade Level: basic Duration: minutes Setting: classroom or field site ph Popl Adaptd from: Whr Ar th Frogs? in Projct WET: Curriculum & Activity Guid. Bozman: Th Watrcours and th Council for Environmntal Education, 1995. ph Grad Lvl: basic Duration: 10 15 minuts Stting:

More information

The Equitable Dominating Graph

The Equitable Dominating Graph Intrnational Journal of Enginring Rsarch and Tchnology. ISSN 0974-3154 Volum 8, Numbr 1 (015), pp. 35-4 Intrnational Rsarch Publication Hous http://www.irphous.com Th Equitabl Dominating Graph P.N. Vinay

More information

STABILITY ANALYSIS OF FUZZY CONTROLLERS USING THE MODIFIED POPOV CRITERION

STABILITY ANALYSIS OF FUZZY CONTROLLERS USING THE MODIFIED POPOV CRITERION SABILIY ANALYSIS OF FUZZY CONROLLERS USING HE MODIFIED POPOV CRIERION Mauricio Gonçalvs Santana Junior Instituto cnológico d Aronáutica Pça Mal Eduardo Goms, 50 Vila das Acácias - CEP 2228-900 São José

More information

A Prey-Predator Model with an Alternative Food for the Predator, Harvesting of Both the Species and with A Gestation Period for Interaction

A Prey-Predator Model with an Alternative Food for the Predator, Harvesting of Both the Species and with A Gestation Period for Interaction Int. J. Opn Problms Compt. Math., Vol., o., Jun 008 A Pry-Prdator Modl with an Altrnativ Food for th Prdator, Harvsting of Both th Spcis and with A Gstation Priod for Intraction K. L. arayan and. CH. P.

More information

Einstein Equations for Tetrad Fields

Einstein Equations for Tetrad Fields Apiron, Vol 13, No, Octobr 006 6 Einstin Equations for Ttrad Filds Ali Rıza ŞAHİN, R T L Istanbul (Turky) Evry mtric tnsor can b xprssd by th innr product of ttrad filds W prov that Einstin quations for

More information

MEASURING HEAT FLUX FROM A COMPONENT ON A PCB

MEASURING HEAT FLUX FROM A COMPONENT ON A PCB MEASURING HEAT FLUX FROM A COMPONENT ON A PCB INTRODUCTION Elctronic circuit boards consist of componnts which gnrats substantial amounts of hat during thir opration. A clar knowldg of th lvl of hat dissipation

More information

Quasi-Classical States of the Simple Harmonic Oscillator

Quasi-Classical States of the Simple Harmonic Oscillator Quasi-Classical Stats of th Simpl Harmonic Oscillator (Draft Vrsion) Introduction: Why Look for Eignstats of th Annihilation Oprator? Excpt for th ground stat, th corrspondnc btwn th quantum nrgy ignstats

More information

ECE602 Exam 1 April 5, You must show ALL of your work for full credit.

ECE602 Exam 1 April 5, You must show ALL of your work for full credit. ECE62 Exam April 5, 27 Nam: Solution Scor: / This xam is closd-book. You must show ALL of your work for full crdit. Plas rad th qustions carfully. Plas chck your answrs carfully. Calculators may NOT b

More information

LINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM

LINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM Elctronic Journal of Diffrntial Equations, Vol. 2003(2003), No. 92, pp. 1 6. ISSN: 1072-6691. URL: http://jd.math.swt.du or http://jd.math.unt.du ftp jd.math.swt.du (login: ftp) LINEAR DELAY DIFFERENTIAL

More information

INFLUENCE OF GROUND SUBSIDENCE IN THE DAMAGE TO MEXICO CITY S PRIMARY WATER SYSTEM DUE TO THE 1985 EARTHQUAKE

INFLUENCE OF GROUND SUBSIDENCE IN THE DAMAGE TO MEXICO CITY S PRIMARY WATER SYSTEM DUE TO THE 1985 EARTHQUAKE 13 th World Confrnc on Earthquak Enginring Vancouvr, B.C., Canada August 1-6, 2004 Papr No. 2165 INFLUENCE OF GROUND SUBSIDENCE IN THE DAMAGE TO MEXICO CITY S PRIMARY WATER SYSTEM DUE TO THE 1985 EARTHQUAKE

More information

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 07 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat

More information

Linear-Phase FIR Transfer Functions. Functions. Functions. Functions. Functions. Functions. Let

Linear-Phase FIR Transfer Functions. Functions. Functions. Functions. Functions. Functions. Let It is impossibl to dsign an IIR transfr function with an xact linar-phas It is always possibl to dsign an FIR transfr function with an xact linar-phas rspons W now dvlop th forms of th linarphas FIR transfr

More information

Linear Non-Gaussian Structural Equation Models

Linear Non-Gaussian Structural Equation Models IMPS 8, Durham, NH Linar Non-Gaussian Structural Equation Modls Shohi Shimizu, Patrik Hoyr and Aapo Hyvarinn Osaka Univrsity, Japan Univrsity of Hlsinki, Finland Abstract Linar Structural Equation Modling

More information

Estimation of odds ratios in Logistic Regression models under different parameterizations and Design matrices

Estimation of odds ratios in Logistic Regression models under different parameterizations and Design matrices Advancs in Computational Intllignc, Man-Machin Systms and Cybrntics Estimation of odds ratios in Logistic Rgrssion modls undr diffrnt paramtrizations and Dsign matrics SURENDRA PRASAD SINHA*, LUIS NAVA

More information

Iterative learning control with initial rectifying action for nonlinear continuous systems X.-D. Li 1 T.W.S. Chow 2 J.K.L. Ho 3 J.

Iterative learning control with initial rectifying action for nonlinear continuous systems X.-D. Li 1 T.W.S. Chow 2 J.K.L. Ho 3 J. Publishd in IET Control Thory and Applications Rcivd on 24th Dcmbr 27 Rvisd on 21st May 28 doi: 1.149/it-cta:27486 ISSN 1751-8644 Itrativ larning control with initial rctifying action for nonlinar continuous

More information

Dealing with quantitative data and problem solving life is a story problem! Attacking Quantitative Problems

Dealing with quantitative data and problem solving life is a story problem! Attacking Quantitative Problems Daling with quantitati data and problm soling lif is a story problm! A larg portion of scinc inols quantitati data that has both alu and units. Units can sa your butt! Nd handl on mtric prfixs Dimnsional

More information

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012 Th van dr Waals intraction D. E. Sopr 2 Univrsity of Orgon 20 pril 202 Th van dr Waals intraction is discussd in Chaptr 5 of J. J. Sakurai, Modrn Quantum Mchanics. Hr I tak a look at it in a littl mor

More information

Forces. Quantum ElectroDynamics. α = = We have now:

Forces. Quantum ElectroDynamics. α = = We have now: W hav now: Forcs Considrd th gnral proprtis of forcs mdiatd by xchang (Yukawa potntial); Examind consrvation laws which ar obyd by (som) forcs. W will nxt look at thr forcs in mor dtail: Elctromagntic

More information

Scattering States of l-wave Schrödinger Equation with Modified Rosen Morse Potential

Scattering States of l-wave Schrödinger Equation with Modified Rosen Morse Potential Commun. Thor. Phys. 66 06 96 00 Vol. 66, No., August, 06 Scattring Stats of l-wav Schrödingr Equation with Modifid Rosn Mors Potntial Wn-Li Chn í,, Yan-Wi Shi á, and Gao-Fng Wi Ôô, Gnral Education Cntr,

More information

ARIMA Methods of Detecting Outliers in Time Series Periodic Processes

ARIMA Methods of Detecting Outliers in Time Series Periodic Processes Articl Intrnational Journal of Modrn Mathmatical Scincs 014 11(1): 40-48 Intrnational Journal of Modrn Mathmatical Scincs Journal hompag:www.modrnscintificprss.com/journals/ijmms.aspx ISSN:166-86X Florida

More information

1 Minimum Cut Problem

1 Minimum Cut Problem CS 6 Lctur 6 Min Cut and argr s Algorithm Scribs: Png Hui How (05), Virginia Dat: May 4, 06 Minimum Cut Problm Today, w introduc th minimum cut problm. This problm has many motivations, on of which coms

More information

That is, we start with a general matrix: And end with a simpler matrix:

That is, we start with a general matrix: And end with a simpler matrix: DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss

More information

Full Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient

Full Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient Full Wavform Invrsion Using an Enrgy-Basd Objctiv Function with Efficint Calculation of th Gradint Itm yp Confrnc Papr Authors Choi, Yun Sok; Alkhalifah, ariq Ali Citation Choi Y, Alkhalifah (217) Full

More information

Impact of the Sampling Period on the Design of Digital PID Controllers

Impact of the Sampling Period on the Design of Digital PID Controllers Impact of th Sampling Priod on th Dsign of Digital PID Controllrs Dimitris Tsamatsoulis Halyps Building Matrials S.A. 17 th klm Nat. Road Athns Korinth, Aspropyrgos, Grc d.tsamatsoulis@halyps.gr Abstract

More information

2.3 Matrix Formulation

2.3 Matrix Formulation 23 Matrix Formulation 43 A mor complicatd xampl ariss for a nonlinar systm of diffrntial quations Considr th following xampl Exampl 23 x y + x( x 2 y 2 y x + y( x 2 y 2 (233 Transforming to polar coordinats,

More information

First derivative analysis

First derivative analysis Robrto s Nots on Dirntial Calculus Chaptr 8: Graphical analysis Sction First drivativ analysis What you nd to know alrady: How to us drivativs to idntiy th critical valus o a unction and its trm points

More information

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values Dnamic Macroconomic Thor Prof. Thomas Lux Bifurcation Thor Bifurcation: qualitativ chang in th natur of th solution occurs if a paramtr passs through a critical point bifurcation or branch valu. Local

More information

Basic Polyhedral theory

Basic Polyhedral theory Basic Polyhdral thory Th st P = { A b} is calld a polyhdron. Lmma 1. Eithr th systm A = b, b 0, 0 has a solution or thr is a vctorπ such that π A 0, πb < 0 Thr cass, if solution in top row dos not ist

More information

Volterra Kernel Estimation for Nonlinear Communication Channels Using Deterministic Sequences

Volterra Kernel Estimation for Nonlinear Communication Channels Using Deterministic Sequences 1 Voltrra Krnl Estimation for Nonlinar Communication Channls Using Dtrministic Squncs Endr M. Ekşioğlu and Ahmt H. Kayran Dpartmnt of Elctrical and Elctronics Enginring, Istanbul Tchnical Univrsity, Istanbul,

More information

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002 3.4 Forc Analysis of Linkas An undrstandin of forc analysis of linkas is rquird to: Dtrmin th raction forcs on pins, tc. as a consqunc of a spcifid motion (don t undrstimat th sinificanc of dynamic or

More information

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013 18.782 Introduction to Arithmtic Gomtry Fall 2013 Lctur #20 11/14/2013 20.1 Dgr thorm for morphisms of curvs Lt us rstat th thorm givn at th nd of th last lctur, which w will now prov. Thorm 20.1. Lt φ:

More information

4. Money cannot be neutral in the short-run the neutrality of money is exclusively a medium run phenomenon.

4. Money cannot be neutral in the short-run the neutrality of money is exclusively a medium run phenomenon. PART I TRUE/FALSE/UNCERTAIN (5 points ach) 1. Lik xpansionary montary policy, xpansionary fiscal policy rturns output in th mdium run to its natural lvl, and incrass prics. Thrfor, fiscal policy is also

More information

u x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula

u x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula 7. Intgration by Parts Each drivativ formula givs ris to a corrsponding intgral formula, as w v sn many tims. Th drivativ product rul yilds a vry usful intgration tchniqu calld intgration by parts. Starting

More information

Section 6.1. Question: 2. Let H be a subgroup of a group G. Then H operates on G by left multiplication. Describe the orbits for this operation.

Section 6.1. Question: 2. Let H be a subgroup of a group G. Then H operates on G by left multiplication. Describe the orbits for this operation. MAT 444 H Barclo Spring 004 Homwork 6 Solutions Sction 6 Lt H b a subgroup of a group G Thn H oprats on G by lft multiplication Dscrib th orbits for this opration Th orbits of G ar th right costs of H

More information

Types of Transfer Functions. Types of Transfer Functions. Types of Transfer Functions. Ideal Filters. Ideal Filters

Types of Transfer Functions. Types of Transfer Functions. Types of Transfer Functions. Ideal Filters. Ideal Filters Typs of Transfr Typs of Transfr x[n] X( LTI h[n] H( y[n] Y( y [ n] h[ k] x[ n k] k Y ( H ( X ( Th tim-domain classification of an LTI digital transfr function is basd on th lngth of its impuls rspons h[n]:

More information

CO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS

CO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS CO-ORDINATION OF FAST NUMERICAL RELAYS AND CURRENT TRANSFORMERS OVERDIMENSIONING FACTORS AND INFLUENCING PARAMETERS Stig Holst ABB Automation Products Swdn Bapuji S Palki ABB Utilitis India This papr rports

More information

Function Spaces. a x 3. (Letting x = 1 =)) a(0) + b + c (1) = 0. Row reducing the matrix. b 1. e 4 3. e 9. >: (x = 1 =)) a(0) + b + c (1) = 0

Function Spaces. a x 3. (Letting x = 1 =)) a(0) + b + c (1) = 0. Row reducing the matrix. b 1. e 4 3. e 9. >: (x = 1 =)) a(0) + b + c (1) = 0 unction Spacs Prrquisit: Sction 4.7, Coordinatization n this sction, w apply th tchniqus of Chaptr 4 to vctor spacs whos lmnts ar functions. Th vctor spacs P n and P ar familiar xampls of such spacs. Othr

More information

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields Lctur 37 (Schrödingr Equation) Physics 6-01 Spring 018 Douglas Filds Rducd Mass OK, so th Bohr modl of th atom givs nrgy lvls: E n 1 k m n 4 But, this has on problm it was dvlopd assuming th acclration

More information

Two Products Manufacturer s Production Decisions with Carbon Constraint

Two Products Manufacturer s Production Decisions with Carbon Constraint Managmnt Scinc and Enginring Vol 7 No 3 pp 3-34 DOI:3968/jms9335X374 ISSN 93-34 [Print] ISSN 93-35X [Onlin] wwwcscanadant wwwcscanadaorg Two Products Manufacturr s Production Dcisions with Carbon Constraint

More information

Inference Methods for Stochastic Volatility Models

Inference Methods for Stochastic Volatility Models Intrnational Mathmatical Forum, Vol 8, 03, no 8, 369-375 Infrnc Mthods for Stochastic Volatility Modls Maddalna Cavicchioli Cá Foscari Univrsity of Vnic Advancd School of Economics Cannargio 3, Vnic, Italy

More information

Design Guidelines for Quartz Crystal Oscillators. R 1 Motional Resistance L 1 Motional Inductance C 1 Motional Capacitance C 0 Shunt Capacitance

Design Guidelines for Quartz Crystal Oscillators. R 1 Motional Resistance L 1 Motional Inductance C 1 Motional Capacitance C 0 Shunt Capacitance TECHNICAL NTE 30 Dsign Guidlins for Quartz Crystal scillators Introduction A CMS Pirc oscillator circuit is wll known and is widly usd for its xcllnt frquncy stability and th wid rang of frquncis ovr which

More information

Derangements and Applications

Derangements and Applications 2 3 47 6 23 Journal of Intgr Squncs, Vol. 6 (2003), Articl 03..2 Drangmnts and Applications Mhdi Hassani Dpartmnt of Mathmatics Institut for Advancd Studis in Basic Scincs Zanjan, Iran mhassani@iasbs.ac.ir

More information

4.2 Design of Sections for Flexure

4.2 Design of Sections for Flexure 4. Dsign of Sctions for Flxur This sction covrs th following topics Prliminary Dsign Final Dsign for Typ 1 Mmbrs Spcial Cas Calculation of Momnt Dmand For simply supportd prstrssd bams, th maximum momnt

More information

Observer Bias and Reliability By Xunchi Pu

Observer Bias and Reliability By Xunchi Pu Obsrvr Bias and Rliability By Xunchi Pu Introduction Clarly all masurmnts or obsrvations nd to b mad as accuratly as possibl and invstigators nd to pay carful attntion to chcking th rliability of thir

More information

PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS

PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS Intrnational Journal Of Advanc Rsarch In Scinc And Enginring http://www.ijars.com IJARSE, Vol. No., Issu No., Fbruary, 013 ISSN-319-8354(E) PROOF OF FIRST STANDARD FORM OF NONELEMENTARY FUNCTIONS 1 Dharmndra

More information

Search sequence databases 3 10/25/2016

Search sequence databases 3 10/25/2016 Sarch squnc databass 3 10/25/2016 Etrm valu distribution Ø Suppos X is a random variabl with probability dnsity function p(, w sampl a larg numbr S of indpndnt valus of X from this distribution for an

More information

Chapter 6. The Discrete Fourier Transform and The Fast Fourier Transform

Chapter 6. The Discrete Fourier Transform and The Fast Fourier Transform Pusan ational Univrsity Chaptr 6. Th Discrt Fourir Transform and Th Fast Fourir Transform 6. Introduction Frquncy rsponss of discrt linar tim invariant systms ar rprsntd by Fourir transform or z-transforms.

More information

Problem Set 6 Solutions

Problem Set 6 Solutions 6.04/18.06J Mathmatics for Computr Scinc March 15, 005 Srini Dvadas and Eric Lhman Problm St 6 Solutions Du: Monday, March 8 at 9 PM in Room 3-044 Problm 1. Sammy th Shark is a financial srvic providr

More information

Partial Derivatives: Suppose that z = f(x, y) is a function of two variables.

Partial Derivatives: Suppose that z = f(x, y) is a function of two variables. Chaptr Functions o Two Variabls Applid Calculus 61 Sction : Calculus o Functions o Two Variabls Now that ou hav som amiliarit with unctions o two variabls it s tim to start appling calculus to hlp us solv

More information

Evaluating Reliability Systems by Using Weibull & New Weibull Extension Distributions Mushtak A.K. Shiker

Evaluating Reliability Systems by Using Weibull & New Weibull Extension Distributions Mushtak A.K. Shiker Evaluating Rliability Systms by Using Wibull & Nw Wibull Extnsion Distributions Mushtak A.K. Shikr مشتاق عبذ الغني شخير Univrsity of Babylon, Collg of Education (Ibn Hayan), Dpt. of Mathmatics Abstract

More information

Title: Vibrational structure of electronic transition

Title: Vibrational structure of electronic transition Titl: Vibrational structur of lctronic transition Pag- Th band spctrum sn in th Ultra-Violt (UV) and visibl (VIS) rgions of th lctromagntic spctrum can not intrprtd as vibrational and rotational spctrum

More information

Model-based Scheduling for Networked Control Systems

Model-based Scheduling for Networked Control Systems Modl-basd Schduling for Ntworkd Control Systms Han Yu, Eloy Garcia and Panos J. Antsaklis Abstract In this papr, w introduc a modl-basd schduling stratgy to achiv ultimat bounddnss stability in th snsor-actuator

More information

EEO 401 Digital Signal Processing Prof. Mark Fowler

EEO 401 Digital Signal Processing Prof. Mark Fowler EEO 401 Digital Signal Procssing Prof. Mark Fowlr ot St #18 Introduction to DFT (via th DTFT) Rading Assignmnt: Sct. 7.1 of Proakis & Manolakis 1/24 Discrt Fourir Transform (DFT) W v sn that th DTFT is

More information

Coupled Pendulums. Two normal modes.

Coupled Pendulums. Two normal modes. Tim Dpndnt Two Stat Problm Coupld Pndulums Wak spring Two normal mods. No friction. No air rsistanc. Prfct Spring Start Swinging Som tim latr - swings with full amplitud. stationary M +n L M +m Elctron

More information

COUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM

COUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM COUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM Jim Brown Dpartmnt of Mathmatical Scincs, Clmson Univrsity, Clmson, SC 9634, USA jimlb@g.clmson.du Robrt Cass Dpartmnt of Mathmatics,

More information

Thus, because if either [G : H] or [H : K] is infinite, then [G : K] is infinite, then [G : K] = [G : H][H : K] for all infinite cases.

Thus, because if either [G : H] or [H : K] is infinite, then [G : K] is infinite, then [G : K] = [G : H][H : K] for all infinite cases. Homwork 5 M 373K Solutions Mark Lindbrg and Travis Schdlr 1. Prov that th ring Z/mZ (for m 0) is a fild if and only if m is prim. ( ) Proof by Contrapositiv: Hr, thr ar thr cass for m not prim. m 0: Whn

More information

Rational Approximation for the one-dimensional Bratu Equation

Rational Approximation for the one-dimensional Bratu Equation Intrnational Journal of Enginring & Tchnology IJET-IJES Vol:3 o:05 5 Rational Approximation for th on-dimnsional Bratu Equation Moustafa Aly Soliman Chmical Enginring Dpartmnt, Th British Univrsity in

More information

EECE 301 Signals & Systems Prof. Mark Fowler

EECE 301 Signals & Systems Prof. Mark Fowler EECE 301 Signals & Systms Prof. Mark Fowlr ot St #21 D-T Signals: Rlation btwn DFT, DTFT, & CTFT 1/16 W can us th DFT to implmnt numrical FT procssing This nabls us to numrically analyz a signal to find

More information

Equidistribution and Weyl s criterion

Equidistribution and Weyl s criterion Euidistribution and Wyl s critrion by Brad Hannigan-Daly W introduc th ida of a sunc of numbrs bing uidistributd (mod ), and w stat and prov a thorm of Hrmann Wyl which charactrizs such suncs. W also discuss

More information

The failure of the classical mechanics

The failure of the classical mechanics h failur of th classical mchanics W rviw som xprimntal vidncs showing that svral concpts of classical mchanics cannot b applid. - h blac-body radiation. - Atomic and molcular spctra. - h particl-li charactr

More information

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding...

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding... Chmical Physics II Mor Stat. Thrmo Kintics Protin Folding... http://www.nmc.ctc.com/imags/projct/proj15thumb.jpg http://nuclarwaponarchiv.org/usa/tsts/ukgrabl2.jpg http://www.photolib.noaa.gov/corps/imags/big/corp1417.jpg

More information

The pn junction: 2 Current vs Voltage (IV) characteristics

The pn junction: 2 Current vs Voltage (IV) characteristics Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n

More information

Procdings of IC-IDC0 ( and (, ( ( and (, and (f ( and (, rspctivly. If two input signals ar compltly qual, phas spctra of two signals ar qual. That is

Procdings of IC-IDC0 ( and (, ( ( and (, and (f ( and (, rspctivly. If two input signals ar compltly qual, phas spctra of two signals ar qual. That is Procdings of IC-IDC0 EFFECTS OF STOCHASTIC PHASE SPECTRUM DIFFERECES O PHASE-OLY CORRELATIO FUCTIOS PART I: STATISTICALLY COSTAT PHASE SPECTRUM DIFFERECES FOR FREQUECY IDICES Shunsu Yamai, Jun Odagiri,

More information

Deift/Zhou Steepest descent, Part I

Deift/Zhou Steepest descent, Part I Lctur 9 Dift/Zhou Stpst dscnt, Part I W now focus on th cas of orthogonal polynomials for th wight w(x) = NV (x), V (x) = t x2 2 + x4 4. Sinc th wight dpnds on th paramtr N N w will writ π n,n, a n,n,

More information

Recall that by Theorems 10.3 and 10.4 together provide us the estimate o(n2 ), S(q) q 9, q=1

Recall that by Theorems 10.3 and 10.4 together provide us the estimate o(n2 ), S(q) q 9, q=1 Chaptr 11 Th singular sris Rcall that by Thorms 10 and 104 togthr provid us th stimat 9 4 n 2 111 Rn = SnΓ 2 + on2, whr th singular sris Sn was dfind in Chaptr 10 as Sn = q=1 Sq q 9, with Sq = 1 a q gcda,q=1

More information

Problem Set #2 Due: Friday April 20, 2018 at 5 PM.

Problem Set #2 Due: Friday April 20, 2018 at 5 PM. 1 EE102B Spring 2018 Signal Procssing and Linar Systms II Goldsmith Problm St #2 Du: Friday April 20, 2018 at 5 PM. 1. Non-idal sampling and rcovry of idal sampls by discrt-tim filtring 30 pts) Considr

More information

MCB137: Physical Biology of the Cell Spring 2017 Homework 6: Ligand binding and the MWC model of allostery (Due 3/23/17)

MCB137: Physical Biology of the Cell Spring 2017 Homework 6: Ligand binding and the MWC model of allostery (Due 3/23/17) MCB37: Physical Biology of th Cll Spring 207 Homwork 6: Ligand binding and th MWC modl of allostry (Du 3/23/7) Hrnan G. Garcia March 2, 207 Simpl rprssion In class, w drivd a mathmatical modl of how simpl

More information