Multivariable Control Systems
|
|
- Frank Miller
- 5 years ago
- Views:
Transcription
1 Multivaiable Contol Sytem Ali Kaimpou Aociate ofeo Fedowi Univeity of Mahhad Refeence ae appeaed in the lat lide.
2 Stability of Multivaiable Feedback Contol Sytem Topic to be coveed include: Well - oedne of Feedback Loop ntenal Stability The Nyquit Stability Citeion The Genealized Nyquit Stability Citeion Nyquit aay and Gehgoin band Copime Factoization ove Stable Tanfe Function Stabilizing Contolle Stong and Simultaneou Stabilization 2
3 Well - oedne of Feedback Loop Aume that the plant and the contolle K ae fixed eal ational pope tanfe matice. The fit quetion one would ak i whethe the feedback inteconnection make ene o i phyically ealizable. Let, 2 K u 2 n d) 3 3 Hence, the feedback ytem i not phyically ealizable! d i 3
4 Well - oedne of Feedback Loop Definition 7- A feedback ytem i aid to be well-poed if all cloed-loop tanfe matice ae well-defined and pope. Now uppoe that all tanfe matice fom the ignal, n, d and d i u ae epectively well-defined and pope. Thu y and all othe ignal ae alo well-defined and the elated tanfe matice ae pope. to So the ytem i well-poed if and only if the tanfe matix fom d i and d to u exit and i pope. 4
5 Well - oedne of Feedback Loop So the ytem i well-poed if and only if the tanfe matix fom d i and d to u exit and i pope. Theoem 7- The feedback ytem in Figue i well-poed if and only if K ) ) i invetible d oof u K K K d i Thu well - poedne i equivalent to the condition that and i pope. K And thi i equivalent to the condition that the contant tem of the tanfe matix K ) ) i invetible. exit 5
6 6 Well - oedne of Feedback Loop Tanfe matix i invetible. ) ) K i equivalent to eithe one of the following two condition: invetible i ) ) K invetible i ) ) K The well- poedne condition i imple to tate in tem of tate-pace ealization. ntoduce ealization of and K: D C B A D C B A K ˆ ˆ SO well- poedne i equivalent to the condition that invetible i D D
7 Stability of Multivaiable Feedback Contol Sytem Well - oedne of Feedback Loop ntenal Stability The Nyquit Stability Citeion The Genealized Nyquit Stability Citeion Nyquit aay and Gehgoin band Copime Factoization ove Stable Tanfe Function Stabilizing Contolle Stong and Simultaneou Stabilization 7
8 ntenal Stability Aume that the ealization fo ) and K) ae tabilizable and detectable. Let x and xˆ denote the tate vecto fo and K, epectively. x Ax Bu xˆ Ax ˆ ˆ By ˆ y Cx Du u Cx ˆ ˆ Dy ˆ Definition 7-2 The ytem of Figue i aymptotically table, d, d i and i aid to be intenally table if the oigin x, xˆ),) i.e. the n tate x, xˆ) go to zeo fomall initial tate when 8
9 9 ntenal Stability x x C C D D y u ˆ ˆ ˆ x x A x x C C D D B B A A x x ˆ ~ ˆ ˆ ˆ ˆ ˆ ˆ Theoem 7-2 The ytem of above Figue with given tabilizable and detectable ealization fo and K i intenally table if and only if i a Huwitz matix All eigenvalue ae in open left half plane). A ~ A ~ e
10 ntenal Stability x x C C D D y u ˆ ˆ ˆ x x A x x C C D D B B A A x x ˆ ~ ˆ ˆ ˆ ˆ ˆ ˆ A ~ e What about tability in the ene of Lyapunov? The ytem of above Figue with given tabilizable and detectable ealization fo and K i table in the ene of Lyapunov if and only if all eigenvalue of be in A ~
11 ntenal Stability d e u K i p Theoem 7-3 The ytem in Figue i intenally table if and only if the tanfe matix ) ) ) ) K K K K K K K fom d i, -) to u p, - e) be a pope and table tanfe matix. e
12 2 ntenal Stability ) ) ) ) K K K K K K K Note that to check intenal tability, it i neceay and ufficient) to tet whethe each of the fou tanfe matice i table., Let K d e u i p 2 2 2) ) 2 Stability cannot be concluded even if thee of the fou tanfe matice ae table.
13 ntenal Stability Theoem 7-4 Suppoe K itable.then the ytem in Stable the figue i intenally table if K ) i table. and only if Remembe K K ) K ) K K ) K ) oof: The neceity i obviou. To pove the ufficiency let Q K) K K) KQ Stable K K) K QK) Stable K) Q Stable K) K) K) K QK Stable 3
14 ntenal Stability Theoem 7-5 Stable Suppoe itable.then the the figue i intenally table if K K ) i table. ytem in and only if Remembe K K ) K ) K K ) K ) oof: The neceity i obviou. To pove the ufficiency let Q K K) K K) Q Stable K K) Q Stable K) Q) Stable K) K) K K) Q Stable 4
15 ntenal Stability Theoem 7-6 Suppoe and K ae both table.then the ytem in the figue i intenally table if and only if K ) i table. Stable Stable K K ) Remembe K ) K ) K K ) oof: The neceity i obviou. To pove the ufficiency let Q K) K K) KQ Stable K K) KQ K) Q K) Q Stable Stable Stable 5
16 ntenal Stability No pole zeo cancellation Theoem 7-7 The ytemin the figue i intenally table if and only if it iwell - poed and i) the numbe of open RH pole of ) K ) n ii) K ) i table. K K ) Remembe K ) K n K K ) K ) n K i the numbe of RH poleof K n i the numbe of RH poleof oof: See: Eential of Robut contol witten by Kemin Zhou 6
17 Stability of Multivaiable Feedback Contol Sytem Well - oedne of Feedback Loop ntenal Stability The Nyquit Stability Citeion The Genealized Nyquit Stability Citeion Nyquit aay and Gehgoin band Copime Factoization ove Stable Tanfe Function Stabilizing Contolle Stong and Simultaneou Stabilization 7
18 The Nyquit Stability Citeion Now we ae going to check the tability of the above ytemfo vaiou eal value of k. Let det[ kg )]have Then o pole and c zeoin the RH plane. jut a SSO ytem,the Nyquit plot of ) det enciclethe oigin, c o time. kg )) Howeve, we would have to daw the Nyquit locu of fo each value of k in which we wee inteeted, wheea in the claical Nyquit citeion we daw a locu only once, and then infe tability popetie fo all value of k. 8
19 The Nyquit Stability Citeion det[ kg )] [ k )] Whee i i ) i an eigenvalue of G ) det[ kg )] k ) i i i - 9
20 The Nyquit Stability Citeion Theoem 7-8 Genealized Nyquit theoem) f G) with no hidden untable mode, ha o untable Smith-McMillan) pole, then the cloed-loop ytem with etun atio kg) i table if and only if the chaacteitic loci of kg), taken togethe, encicle the point -, o time anticlockwie. Z N kg ) kg ) kg ) G ) 2 Z N
21 The Nyquit Stability Citeion Example 7-: Let G ) 2.5 ) 3 ) 3 ) ).5 ) ) Suppoe that G) ha no hidden mode, check the tability of ytem fo diffeent value of k. G ).5 ) ) 2 3 2
22 The Nyquit Stability Citeion.5 ) 2 ) 3.25 Since G) ha one untable pole, we will have cloed loop tability if thee loci give one net enciclement of -/k ccw) when a negative feedback k i applied. - -/ k / k.5.5 / k -/k no two one no enciclement o thee i one RH cloedlooppole. enciclement o thee i thee RH cloedlooppole. enciclement o thee i two RH cloedlooppole. enciclement o thee i one RH cloedlooppole. 22
23 The Nyquit Stability Citeion Example 7-2: Let G ).25 ) 2) 6 2 Suppoe that G) ha no hidden mode, check the tability of ytem fo diffeent value of k. G ) ) 2) ) 2) 23
24 The Nyquit Stability Citeion ) 2) ) 2) Since G) ha no untable pole, we will have cloed loop tability if thee loci give zeo net enciclement of -/k when a negative feedback k i applied. / k.8,.4 / k and.53 / k no enciclement..8 / k.4 one enciclement o one RH pole in cloed loop ytem. / k.53 two enciclement o two RH pole in cloed loop ytem. 24
25 The nvee Nyquit Stability Citeion Theoem 7-8 Genealized Nyquit theoem) f G) with no hidden untable mode, ha o untable Smith-McMillan) pole, then the cloed-loop ytem with etun atio kg) i table if and only if the chaacteitic loci of kg), taken togethe, encicle the point -, o time anticlockwie. Z Z invg )/ k invg )/ k N kg ) kg ) N Z N kg ) G ) Theoem 7-9 Genealized nvee Nyquit theoem) f G) with no hidden untable mode, ha Z o untable Smith-McMillan) zeo, then the cloed-loop ytem with etun atio kg) i table if and only if the chaacteitic loci of invg)/k, taken togethe, encicle the point -, Z o time anticlockwie. Z Z N kg ) G ) 25
26 The Nyquit Stability Citeion Example 7-3: Let G ) 5) ) Suppoe that G) ha no hidden mode, check the tability of ytem fo diffeent value of k. G ) 5) ) 5) ) k 75 k 75) Two untable pole. 75 k k 75) Stable. -75 k k ) One RH pole. 26
27 Nyquit aay and Gehgoin band The Nyquit aay of G) i an aay of gaph not neceaily cloed cuve), the ij th gaph being the Nyquit locu of g ij ). Theoem 7- Gehgoin theoem) Let Z be a complex matix of dimenion m m.the eigenvalue of Z ae contained in two union of cicleaound the diagonal elementa follow: i m i zii zij, i, 2,..., m j ji m i zii z ji, i, 2,..., m j ji The band obtained in thi way ae called Gehgoin band, each i compoed of Gehgoin cicle. 27
28 Nyquit aay and Gehgoin band Nyquit aay, with Gehgoin band fo a ample ytem f all the Gehgoin band exclude the point -, then we can ae cloed-loop tability by counting the enciclement of - by the Gehgoin band, ince thi tell u the numbe of enciclement made by the chaacteitic loci. f the Gehgoin band of G) exclude the oigin, then we ay that G) i diagonally dominant ow dominant o column dominant). The geate the degee of dominant of G) o +G) ) that i, the naowe the Gehgoin band- the moe cloely doe G) eemble m non-inteacting SSO tanfe function. 28
29 Nyquit aay and Gehgoin band And in geneal: 29
30 Nyquit aay and Gehgoin band Diagonal dominance of a mm matix G): Row Diagonal dominance: f fo all on the Nyquit contou, m gii ) gij ) i,2,..., j ji m Column Diagonal dominance: f fo all on the Nyquit contou, m gii ) g ji ) i,2,..., j ji m 3
31 Stability of Multivaiable Feedback Contol Sytem Well - oedne of Feedback Loop ntenal Stability The Nyquit Stability Citeion The Genealized Nyquit Stability Citeion Nyquit aay and Gehgoin band Copime Factoization ove Stable Tanfe Function Stabilizing Contolle Stong and Simultaneou Stabilization 3
32 Copime Factoization ove Stable Tanfe Function Two polynomial m) and n), with eal coefficient, ae aid to be copime if thei geatet common divio i a contant numbe o they have no common zeo o thee exit polynomial x) and y) uch that x ) m ) y ) n ) Execie7- : Let n)= and m)= find x) and y) if n and m ae copime. Execie 7-2 : Let n)= and m)=+2 how that one cannot find x) and y) in x)m)+y)n)= Similaly, two tanfe function m) and n) in the et of table tanfe function ae aid to be copime ove table tanfe function if thee exit x) and y) in the et of table tanfe function uch that x ) m ) y ) n ) Bezout identitie 32
33 Copime Factoization ove Stable Tanfe Function Definition 7-3 Two matice M and N in the et of table tanfe matice ae ight copime ove the et of table tanfe matice if they have the ame numbe of column and if thee exit matice X and Y in the et of table tanfe matice.t. M N X Y X M Y N Similaly, two matice and in the et of table tanfe matice M ~ ~ N ~ ae left copime ove the et of table tanfe matice if they have the ame numbe of ow and if thee exit two matice X l and Y l in the et of table tanfe matice uch that ~ X ~ ~ l Y l l M N MX NY l 33
34 Copime Factoization ove Stable Tanfe Function Now let be a pope eal-ational matix. A ight-copime factoization cf) of i a factoization of the fom NM whee N and M ae ight-copime in the et of table tanfe matice. Similaly, a left-copime factoization lcf) of ha the fom ~ M ~ N n cf and lcf ~ M ~, N, M and N ae copime in the et of table tanfe function matice 34
35 Copime Factoization ove Stable Tanfe Function Remembe: Matix Faction Deciption MFD) Right matix faction deciption RMFD) Left matix faction deciption LMFD) Let G) i a mm matix and it the Smith McMillan i ~ G ) Let define: diag ),..., ),,..., D ) diag ),..., ),,..., N ) ~ ~ G ) N ) D ) o G ) D ) N ) n Matix Faction Deciption D) and N) ae polynomial matice 35
36 36 Copime Factoization ove Stable Tanfe Function Theoem 7- Suppoe ) i a pope eal-ational matix and D C B A ) i a tabilizable and detectable ealization. Let F and L be uch that A+BF and A+LC ae both table, and define Then cf and lcf of ae: N M ~ ~ NM Execie 7-3 : Let )=+)/+2) find two diffeent cf fo. D DF C F L B BF A X N Y M l l D C F L LD B LC A M N Y X ) ~ ~
37 Copime Factoization ove Stable Tanfe Function The ight copime factoization of a tanfe matix can be given a feedback contol intepetation. x Ax Bu y Cx Du x u y A BF ) x Bv Fx v C DF ) x Dv the tanfe matix fom v to u i M ) A BF F B u v Fx and that fom v to y i N ) A BF C DF B D y ) N ) v ) N ) M ) u ) ) u ) ) N ) M ) Execie7-4 : Deive a imila intepetation fo left copime factoization. 37
38 Stability of Multivaiable Feedback Contol Sytem Well - oedne of Feedback Loop ntenal Stability The Nyquit Stability Citeion The Genealized Nyquit Stability Citeion Nyquit aay and Gehgoin band Copime Factoization ove Stable Tanfe Function Stabilizing Contolle Stong and Simultaneou Stabilization 38
39 Stabilizing Contolle Theoem 7-2 Suppoe i table. Then the et of all tabilizing contolle in Figue can be decibed a K Q Q) fo any Q in the et of table tanfe matice and ) Q ) non ingula. oof: K Q Q) K Q) Q Q K K) Sytem i table. Now uppoe the ytem i table, o K K) i table,then define Q K K) K) K Q KQ K ) Q ) i noningula o K Q Q) 39
40 Stabilizing Contolle Example 7-4 Fo the plant ) ) 2) Suppoe that it i deied to find an intenally tabilizing contolle o that y aymptotically tack a amp input. Solution: Since the plant i table the et of all tabilizing contolle i deived fom K Q S T Q) K fo any K ) table Q Q uch that ) Q ) a b Q 3 a b ) 2) 3) 6 Q 3 i noningula, 4 o let ) 2) 3) a b) ) 2) 3)
41 Stabilizing Contolle Theoem 7-3 Let K matix and Then thee Y X l Whee be l a pope X NM Y eal- ational ~ ~ M N. exit a tabilizing contolle X ~ N Y M ~ M N Y X l l oof. See Multivaiable Feedback Deign By Maciejowki 4
42 42 Theoem 7-emembe) Suppoe ) i a pope eal-ational matix and D C B A ) i a tabilizable and detectable ealization. Let F and L be uch that A+BF and A+LC ae both table, and define D DF C F L B BF A X N Y M l l D C F L LD B LC A M N Y X ) ~ ~ Stabilizing Contolle
43 Stabilizing Contolle Theoem 7-4 oof. See Multivaiable Feedback Deign By Maciejowki 43
44 44 Example 7-5 Fo the plant 2) ) ) The poblem i to find a contolle that. The feedback ytem i intenally table. 2. The final value of y equal when i a unit tep and d=. 3. The final value of y equal zeo when d i a inuoid of ad/ and =. To deive copime factoization let F = [ -5] and L = [-7-23] T clealy A+BF and A+LC ae table. D DF C F L B BF A X N Y M l l D C F L LD B LC A M N Y X ) ~ ~ ] [ 3 2 Clealy D C B A Stabilizing Contolle
45 45 Solution: The et of all tabilizing contolle i: ) ) l l l l NQ X MQ Y K D DF C F L B BF A X N Y M l l D C F L LD B LC A M N Y X ) ~ ~ ) 38 9, ) 72 8, ) ) 2), ) X Y M N l l ) 38 9, 2) 72 8, 2) ) 2) ~, 2) ~ X Y M N Stabilizing Contolle
46 Stabilizing Contolle Solution: The et of all tabilizing contolle i: K Y l MQ l ) X l NQ l ) Clealy fo any table Q the condition atified To met condition 2 the tanfe function fom to y mut atify ~ y ) N Y ~ Q M ) ) N ) Y ) Q ) M )) Q ) 36.5 To met condition 3 the tanfe function fom d i to y mut atify ~ y ) N X ~ Q N) di ) N j) X j) Q j) N j)) Q j) 629 j Now define Q ) x x2 x3 2 ) Execie 7-5: Deive tanfe function fom to y. Execie 7-6: Deive tanfe function fom d i to y. Execie 7-7: Deive Q 46
47 Stability of Multivaiable Feedback Contol Sytem Well - oedne of Feedback Loop ntenal Stability The Nyquit Stability Citeion The Genealized Nyquit Stability Citeion Nyquit aay and Gehgoin band Copime Factoization ove Stable Tanfe Function Stabilizing Contolle Stong and Simultaneou Stabilization 47
48 Stong and Simultaneou actical contol enginee ae eluctant to ue untable contolle, epecially when the plant itelf i table. f the plant itelf i untable, the agument againt uing an untable contolle i le compelling. Howeve, knowledge of when a plant i o i not tabilizable with a table contolle i ueful fo anothe poblem namely, imultaneou tabilization, meaning tabilization of eveal plant by the ame contolle. Simultaneou tabilization of two plant can alo be viewed a an example of a poblem involving highly tuctued uncetainty. A plant i tongly tabilizable if intenal tabilization can be achieved with a contolle itelf i a table tanfe matix. 48
49 Stong and Simultaneou Theoem 7-5: i tongly tabilizable if and only if it ha an even numbe of eal pole between evey pai of eal RH zeo including zeo at infinity). oof. See Linea feedback contol By Doyle. Example 7-6: Which of the following plant i tongly tabilizable? ) 2) ) ) ) 2 3 2) ) Solution: i not tongly tabilizable ince it ha one pole between z= and z= But 2 i tongly tabilizable ince it ha two pole between z= and z= 49
50 Execie 7-8 Find two diffeent lcf fo the following tanfe function matix. 7-9 Find a lcf and a cf fo the following tanfe matix. G ) Find a lcf and a cf fo the following tanfe matix. G ) G ) 2) 3) ) 4 2 ) 7- By ue of MMO ule in peviou chapte how that the following figue intoduce the contolle in the fom: 5
51 Refeence Refeence Web Refeence Multivaiable Feedback Deign, J M Maciejowki, Weley,989. Multivaiable Feedback Contol, S.Skogetad,. otlethwaite, Wiley,25. Contol Configuation Selection in Multivaiable lant, A. Khaki-Sedigh, B. Moaveni, Spinge Velag, 29. تحليل و طراحی سيستم های چند متغيره دکتر علی خاکی صديق 5
Well-Posedness of Feedback Loop:
ntena Stabiity We-oedne of Feedback Loop: onide the foowing feedback ytem - u u p d i d y Let be both pope tanfe function. Howeve u n d di 3 3 ote that the tanfe function fom the extena igna n d d to u
More informationSIMPLE LOW-ORDER AND INTEGRAL-ACTION CONTROLLER SYNTHESIS FOR MIMO SYSTEMS WITH TIME DELAYS
Appl. Comput. Math., V.10, N.2, 2011, pp.242-249 SIMPLE LOW-ORDER AND INTEGRAL-ACTION CONTROLLER SYNTHESIS FOR MIMO SYSTEMS WITH TIME DELAYS A.N. GÜNDEŞ1, A.N. METE 2 Abtact. A imple finite-dimenional
More informationHow to Obtain Desirable Transfer Functions in MIMO Systems Under Internal Stability Using Open and Closed Loop Control
How to Obtain Desiable ansfe Functions in MIMO Sstems Unde Intenal Stabilit Using Open and losed Loop ontol echnical Repot of the ISIS Goup at the Univesit of Note Dame ISIS-03-006 June, 03 Panos J. Antsaklis
More informationThen the number of elements of S of weight n is exactly the number of compositions of n into k parts.
Geneating Function In a geneal combinatoial poblem, we have a univee S of object, and we want to count the numbe of object with a cetain popety. Fo example, if S i the et of all gaph, we might want to
More informationMultivariable Control Systems
Lecture Multivariable Control Sytem Ali Karimpour Aociate Profeor Ferdowi Univerity of Mahhad Lecture Reference are appeared in the lat lide. Dr. Ali Karimpour May 6 Uncertainty in Multivariable Sytem
More informationChapter 19 Webassign Help Problems
Chapte 9 Webaign Help Poblem 4 5 6 7 8 9 0 Poblem 4: The pictue fo thi poblem i a bit mileading. They eally jut give you the pictue fo Pat b. So let fix that. Hee i the pictue fo Pat (a): Pat (a) imply
More informationOn the quadratic support of strongly convex functions
Int. J. Nonlinea Anal. Appl. 7 2016 No. 1, 15-20 ISSN: 2008-6822 electonic http://dx.doi.og/10.22075/ijnaa.2015.273 On the quadatic uppot of tongly convex function S. Abbazadeh a,b,, M. Ehaghi Godji a
More informationGravity. David Barwacz 7778 Thornapple Bayou SE, Grand Rapids, MI David Barwacz 12/03/2003
avity David Bawacz 7778 Thonapple Bayou, and Rapid, MI 495 David Bawacz /3/3 http://membe.titon.net/daveb Uing the concept dicued in the peceding pape ( http://membe.titon.net/daveb ), I will now deive
More informationSolution to HW 3, Ma 1a Fall 2016
Solution to HW 3, Ma a Fall 206 Section 2. Execise 2: Let C be a subset of the eal numbes consisting of those eal numbes x having the popety that evey digit in the decimal expansion of x is, 3, 5, o 7.
More information18.06 Problem Set 4 Solution
8.6 Poblem Set 4 Solution Total: points Section 3.5. Poblem 2: (Recommended) Find the lagest possible numbe of independent vectos among ) ) ) v = v 4 = v 5 = v 6 = v 2 = v 3 =. Solution (4 points): Since
More informationInference for A One Way Factorial Experiment. By Ed Stanek and Elaine Puleo
Infeence fo A One Way Factoial Expeiment By Ed Stanek and Elaine Puleo. Intoduction We develop etimating equation fo Facto Level mean in a completely andomized one way factoial expeiment. Thi development
More informationA Crash Course in (2 2) Matrices
A Cash Couse in ( ) Matices Seveal weeks woth of matix algeba in an hou (Relax, we will only stuy the simplest case, that of matices) Review topics: What is a matix (pl matices)? A matix is a ectangula
More informationEM Boundary Value Problems
EM Bounday Value Poblems 10/ 9 11/ By Ilekta chistidi & Lee, Seung-Hyun A. Geneal Desciption : Maxwell Equations & Loentz Foce We want to find the equations of motion of chaged paticles. The way to do
More informationFI 2201 Electromagnetism
FI Electomagnetim Aleande A. Ikanda, Ph.D. Phyic of Magnetim and Photonic Reeach Goup ecto Analyi CURILINEAR COORDINAES, DIRAC DELA FUNCION AND HEORY OF ECOR FIELDS Cuvilinea Coodinate Sytem Cateian coodinate:
More informationBasic propositional and. The fundamentals of deduction
Baic ooitional and edicate logic The fundamental of deduction 1 Logic and it alication Logic i the tudy of the atten of deduction Logic lay two main ole in comutation: Modeling : logical entence ae the
More informationOn the Quasi-inverse of a Non-square Matrix: An Infinite Solution
Applied Mathematical Sciences, Vol 11, 2017, no 27, 1337-1351 HIKARI Ltd, wwwm-hikaicom https://doiog/1012988/ams20177273 On the Quasi-invese of a Non-squae Matix: An Infinite Solution Ruben D Codeo J
More informationTRAVELING WAVES. Chapter Simple Wave Motion. Waves in which the disturbance is parallel to the direction of propagation are called the
Chapte 15 RAVELING WAVES 15.1 Simple Wave Motion Wave in which the ditubance i pependicula to the diection of popagation ae called the tanvee wave. Wave in which the ditubance i paallel to the diection
More informationASTR 3740 Relativity & Cosmology Spring Answers to Problem Set 4.
ASTR 3740 Relativity & Comology Sping 019. Anwe to Poblem Set 4. 1. Tajectoie of paticle in the Schwazchild geomety The equation of motion fo a maive paticle feely falling in the Schwazchild geomety ae
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 informationSection 25 Describing Rotational Motion
Section 25 Decibing Rotational Motion What do object do and wh do the do it? We have a ve thoough eplanation in tem of kinematic, foce, eneg and momentum. Thi include Newton thee law of motion and two
More informationOn Locally Convex Topological Vector Space Valued Null Function Space c 0 (S,T, Φ, ξ, u) Defined by Semi Norm and Orlicz Function
Jounal of Intitute of Science and Technology, 204, 9(): 62-68, Intitute of Science and Technology, T.U. On Locally Convex Topological Vecto Space Valued Null Function Space c 0 (S,T, Φ, ξ, u) Defined by
More informationStanford University CS259Q: Quantum Computing Handout 8 Luca Trevisan October 18, 2012
Stanfod Univesity CS59Q: Quantum Computing Handout 8 Luca Tevisan Octobe 8, 0 Lectue 8 In which we use the quantum Fouie tansfom to solve the peiod-finding poblem. The Peiod Finding Poblem Let f : {0,...,
More informationDevelopment of Model Reduction using Stability Equation and Cauer Continued Fraction Method
Intenational Jounal of Electical and Compute Engineeing. ISSN 0974-90 Volume 5, Numbe (03), pp. -7 Intenational Reeach Publication Houe http://www.iphoue.com Development of Model Reduction uing Stability
More informationSecond Order Fuzzy S-Hausdorff Spaces
Inten J Fuzzy Mathematical Achive Vol 1, 013, 41-48 ISSN: 30-34 (P), 30-350 (online) Publihed on 9 Febuay 013 wwweeachmathciog Intenational Jounal o Second Ode Fuzzy S-Haudo Space AKalaichelvi Depatment
More informationChapter 5 Linear Equations: Basic Theory and Practice
Chapte 5 inea Equations: Basic Theoy and actice In this chapte and the next, we ae inteested in the linea algebaic equation AX = b, (5-1) whee A is an m n matix, X is an n 1 vecto to be solved fo, and
More informationSection 8.2 Polar Coordinates
Section 8. Pola Coodinates 467 Section 8. Pola Coodinates The coodinate system we ae most familia with is called the Catesian coodinate system, a ectangula plane divided into fou quadants by the hoizontal
More informationMODULE 5a and 5b (Stewart, Sections 12.2, 12.3) INTRO: In MATH 1114 vectors were written either as rows (a1, a2,..., an) or as columns a 1 a. ...
MODULE 5a and 5b (Stewat, Sections 2.2, 2.3) INTRO: In MATH 4 vectos wee witten eithe as ows (a, a2,..., an) o as columns a a 2... a n and the set of all such vectos of fixed length n was called the vecto
More informationChapter 13. Root Locus Introduction
Chapter 13 Root Locu 13.1 Introduction In the previou chapter we had a glimpe of controller deign iue through ome imple example. Obviouly when we have higher order ytem, uch imple deign technique will
More informationThe Archimedean Circles of Schoch and Woo
Foum Geometicoum Volume 4 (2004) 27 34. FRUM GEM ISSN 1534-1178 The Achimedean Cicles of Schoch and Woo Hioshi kumua and Masayuki Watanabe Abstact. We genealize the Achimedean cicles in an abelos (shoemake
More informationPHYS 705: Classical Mechanics. Small Oscillations
PHYS 705: Classical Mechanics Small Oscillations Fomulation of the Poblem Assumptions: V q - A consevative system with depending on position only - The tansfomation equation defining does not dep on time
More informationSeveral new identities involving Euler and Bernoulli polynomials
Bull. Math. Soc. Sci. Math. Roumanie Tome 9107 No. 1, 016, 101 108 Seveal new identitie involving Eule and Benoulli polynomial by Wang Xiaoying and Zhang Wenpeng Abtact The main pupoe of thi pape i uing
More informationRotational Motion. Lecture 6. Chapter 4. Physics I. Course website:
Lectue 6 Chapte 4 Physics I Rotational Motion Couse website: http://faculty.uml.edu/andiy_danylov/teaching/physicsi Today we ae going to discuss: Chapte 4: Unifom Cicula Motion: Section 4.4 Nonunifom Cicula
More informationTheorem 2: Proof: Note 1: Proof: Note 2:
A New 3-Dimenional Polynomial Intepolation Method: An Algoithmic Appoach Amitava Chattejee* and Rupak Bhattachayya** A new 3-dimenional intepolation method i intoduced in thi pape. Coeponding to the method
More informationMotithang Higher Secondary School Thimphu Thromde Mid Term Examination 2016 Subject: Mathematics Full Marks: 100
Motithang Highe Seconday School Thimphu Thomde Mid Tem Examination 016 Subject: Mathematics Full Maks: 100 Class: IX Witing Time: 3 Hous Read the following instuctions caefully In this pape, thee ae thee
More information22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 18
.65, MHD Theoy of Fuion Sytem Pof. Feidbeg Lectue 8. Deive δw fo geneal cew pinch. Deive Suydam citeion Scew Pinch Equilibia μ p + + ( ) = μ J = μ J= Stability ( ) m k ξ=ξ e ι +ι ξ=ξ e +ξ e +ξ e =ξ +ξ
More informationState Space: Observer Design Lecture 11
State Space: Oberver Deign Lecture Advanced Control Sytem Dr Eyad Radwan Dr Eyad Radwan/ACS/ State Space-L Controller deign relie upon acce to the tate variable for feedback through adjutable gain. Thi
More informationDetermining the Best Linear Unbiased Predictor of PSU Means with the Data. included with the Random Variables. Ed Stanek
Detemining te Bet Linea Unbiaed Pedicto of PSU ean wit te Data included wit te andom Vaiable Ed Stanek Intoduction We develop te equation fo te bet linea unbiaed pedicto of PSU mean in a two tage andom
More informationSolutions Practice Test PHYS 211 Exam 2
Solution Pactice Tet PHYS 11 Exam 1A We can plit thi poblem up into two pat, each one dealing with a epaate axi. Fo both the x- and y- axe, we have two foce (one given, one unknown) and we get the following
More informationPDF Created with deskpdf PDF Writer - Trial ::
A APPENDIX D TRIGONOMETRY Licensed to: jsamuels@bmcc.cun.edu PDF Ceated with deskpdf PDF Wite - Tial :: http://www.docudesk.com D T i g o n o m e t FIGURE a A n g l e s Angles can be measued in degees
More informationVector d is a linear vector function of vector d when the following relationships hold:
Appendix 4 Dyadic Analysis DEFINITION ecto d is a linea vecto function of vecto d when the following elationships hold: d x = a xxd x + a xy d y + a xz d z d y = a yxd x + a yy d y + a yz d z d z = a zxd
More informationExercises for lectures 19 Polynomial methods
Exercie for lecture 19 Polynomial method Michael Šebek Automatic control 016 15-4-17 Diviion of polynomial with and without remainder Polynomial form a circle, but not a body. (Circle alo form integer,
More informationDo Managers Do Good With Other People s Money? Online Appendix
Do Manages Do Good With Othe People s Money? Online Appendix Ing-Haw Cheng Haison Hong Kelly Shue Abstact This is the Online Appendix fo Cheng, Hong and Shue 2013) containing details of the model. Datmouth
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 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 informationTo Feel a Force Chapter 7 Static equilibrium - torque and friction
To eel a oce Chapte 7 Chapte 7: Static fiction, toque and static equilibium A. Review of foce vectos Between the eath and a small mass, gavitational foces of equal magnitude and opposite diection act on
More informationSolutions. Digital Control Systems ( ) 120 minutes examination time + 15 minutes reading time at the beginning of the exam
BSc - Sample Examination Digital Control Sytem (5-588-) Prof. L. Guzzella Solution Exam Duration: Number of Quetion: Rating: Permitted aid: minute examination time + 5 minute reading time at the beginning
More informationProblem Set #10 Math 471 Real Analysis Assignment: Chapter 8 #2, 3, 6, 8
Poblem Set #0 Math 47 Real Analysis Assignment: Chate 8 #2, 3, 6, 8 Clayton J. Lungstum Decembe, 202 xecise 8.2 Pove the convese of Hölde s inequality fo = and =. Show also that fo eal-valued f / L ),
More informationarxiv: v1 [math.co] 4 May 2017
On The Numbe Of Unlabeled Bipatite Gaphs Abdullah Atmaca and A Yavuz Ouç axiv:7050800v [mathco] 4 May 207 Abstact This pape solves a poblem that was stated by M A Haison in 973 [] This poblem, that has
More informationChapter 6. NEWTON S 2nd LAW AND UNIFORM CIRCULAR MOTION. string
Chapte 6 NEWTON S nd LAW AND UNIFORM CIRCULAR MOTION 103 PHYS 1 1 L:\103 Phy LECTURES SLIDES\103Phy_Slide_T1Y3839\CH6Flah 3 4 ting Quetion: A ball attached to the end of a ting i whiled in a hoizontal
More informationGeometry of the homogeneous and isotropic spaces
Geomety of the homogeneous and isotopic spaces H. Sonoda Septembe 2000; last evised Octobe 2009 Abstact We summaize the aspects of the geomety of the homogeneous and isotopic spaces which ae most elevant
More informationCALCULUS II Vectors. Paul Dawkins
CALCULUS II Vectos Paul Dawkins Table of Contents Peface... ii Vectos... 3 Intoduction... 3 Vectos The Basics... 4 Vecto Aithmetic... 8 Dot Poduct... 13 Coss Poduct... 21 2007 Paul Dawkins i http://tutoial.math.lama.edu/tems.aspx
More informationChapter 6. NEWTON S 2nd LAW AND UNIFORM CIRCULAR MOTION
Chapte 6 NEWTON S nd LAW AND UNIFORM CIRCULAR MOTION Phyic 1 1 3 4 ting Quetion: A ball attached to the end of a ting i whiled in a hoizontal plane. At the point indicated, the ting beak. Looking down
More informationVoltage ( = Electric Potential )
V-1 of 10 Voltage ( = lectic Potential ) An electic chage altes the space aound it. Thoughout the space aound evey chage is a vecto thing called the electic field. Also filling the space aound evey chage
More informationPHYS 1114, Lecture 21, March 6 Contents:
PHYS 1114, Lectue 21, Mach 6 Contents: 1 This class is o cially cancelled, being eplaced by the common exam Tuesday, Mach 7, 5:30 PM. A eview and Q&A session is scheduled instead duing class time. 2 Exam
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 informationENGI 4430 Non-Cartesian Coordinates Page xi Fy j Fzk from Cartesian coordinates z to another orthonormal coordinate system u, v, ˆ i ˆ ˆi
ENGI 44 Non-Catesian Coodinates Page 7-7. Conesions between Coodinate Systems In geneal, the conesion of a ecto F F xi Fy j Fzk fom Catesian coodinates x, y, z to anothe othonomal coodinate system u,,
More informationMany Electron Atoms. Electrons can be put into approximate orbitals and the properties of the many electron systems can be catalogued
Many Electon Atoms The many body poblem cannot be solved analytically. We content ouselves with developing appoximate methods that can yield quite accuate esults (but usually equie a compute). The electons
More informationEncapsulation theory: radial encapsulation. Edmund Kirwan *
Encapsulation theoy: adial encapsulation. Edmund Kiwan * www.edmundkiwan.com Abstact This pape intoduces the concept of adial encapsulation, wheeby dependencies ae constained to act fom subsets towads
More informationNoether Theorem, Noether Charge and All That
Noethe Theoem, Noethe Chage and All That Ceated fo PF by Samalkhaiat 10 Tanfomation Let G be a Lie goup whoe action on Minkowki pace-time fomally ealized by coodinate tanfomation ( ) ( 1,3,η) M i Infiniteimally,
More informationLocalization of Eigenvalues in Small Specified Regions of Complex Plane by State Feedback Matrix
Jounal of Sciences, Islamic Republic of Ian (): - () Univesity of Tehan, ISSN - http://sciencesutaci Localization of Eigenvalues in Small Specified Regions of Complex Plane by State Feedback Matix H Ahsani
More informationMEM 355 Performance Enhancement of Dynamical Systems Root Locus Analysis
MEM 355 Performance Enhancement of Dynamical Sytem Root Locu Analyi Harry G. Kwatny Department of Mechanical Engineering & Mechanic Drexel Univerity Outline The root locu method wa introduced by Evan in
More informationEstimation and Confidence Intervals: Additional Topics
Chapte 8 Etimation and Confidence Inteval: Additional Topic Thi chapte imply follow the method in Chapte 7 fo foming confidence inteval The text i a bit dioganized hee o hopefully we can implify Etimation:
More informationElectrostatic Potential
Chapte 23 Electostatic Potential PowePoint Lectues fo Univesity Physics, Twelfth Edition Hugh D. Young and Roge A. Feedman Lectues by James Pazun Copyight 2008 Peason Education Inc., publishing as Peason
More informationChapter Eight Notes N P U1C8S4-6
Chapte Eight Notes N P UC8S-6 Name Peiod Section 8.: Tigonometic Identities An identit is, b definition, an equation that is alwas tue thoughout its domain. B tue thoughout its domain, that is to sa that
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 informationDynamic Visualization of Complex Integrals with Cabri II Plus
Dynamic Visualiation of omplex Integals with abi II Plus Sae MIKI Kawai-juu, IES Japan Email: sand_pictue@hotmailcom Abstact: Dynamic visualiation helps us undestand the concepts of mathematics This pape
More informationBoise State University Department of Electrical and Computer Engineering ECE470 Electric Machines
Boie State Univeity Depatment of Electical and Compute Engineeing ECE470 Electic Machine Deivation of the Pe-Phae Steady-State Equivalent Cicuit of a hee-phae Induction Machine Nomenclatue θ: oto haft
More informationLectures on Multivariable Feedback Control
Lectues on Mutivaiabe Feedback onto i Kaimpou epatment of Eectica Engineeing, Facuty of Engineeing, Fedowsi Univesity of Mashhad (Septembe 9 hapte 4: Stabiity of Mutivaiabe Feedback onto Systems 4- We-Posedness
More informationRigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018
Rigid Body Dynamics 2 CSE169: Compute Animation nstucto: Steve Rotenbeg UCSD, Winte 2018 Coss Poduct & Hat Opeato Deivative of a Rotating Vecto Let s say that vecto is otating aound the oigin, maintaining
More informationPhysics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism
Physics 2020, Sping 2005 Lab 5 page 1 of 8 Lab 5. Magnetism PART I: INTRODUCTION TO MAGNETS This week we will begin wok with magnets and the foces that they poduce. By now you ae an expet on setting up
More informationPhysics 235 Chapter 5. Chapter 5 Gravitation
Chapte 5 Gavitation In this Chapte we will eview the popeties of the gavitational foce. The gavitational foce has been discussed in geat detail in you intoductoy physics couses, and we will pimaily focus
More informationON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION. 1. Introduction. 1 r r. r k for every set E A, E \ {0},
ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION E. J. IONASCU and A. A. STANCU Abstact. We ae inteested in constucting concete independent events in puely atomic pobability
More information7.2. Coulomb s Law. The Electric Force
Coulomb s aw Recall that chaged objects attact some objects and epel othes at a distance, without making any contact with those objects Electic foce,, o the foce acting between two chaged objects, is somewhat
More information4/18/2005. Statistical Learning Theory
Statistical Leaning Theoy Statistical Leaning Theoy A model of supevised leaning consists of: a Envionment - Supplying a vecto x with a fixed but unknown pdf F x (x b Teache. It povides a desied esponse
More informationChapter 7. Root Locus Analysis
Chapter 7 Root Locu Analyi jw + KGH ( ) GH ( ) - K 0 z O 4 p 2 p 3 p Root Locu Analyi The root of the cloed-loop characteritic equation define the ytem characteritic repone. Their location in the complex
More informationof the contestants play as Falco, and 1 6
JHMT 05 Algeba Test Solutions 4 Febuay 05. In a Supe Smash Bothes tounament, of the contestants play as Fox, 3 of the contestants play as Falco, and 6 of the contestants play as Peach. Given that thee
More informationAPPLICATION OF MAC IN THE FREQUENCY DOMAIN
PPLICION OF MC IN HE FREQUENCY DOMIN D. Fotsch and D. J. Ewins Dynamics Section, Mechanical Engineeing Depatment Impeial College of Science, echnology and Medicine London SW7 2B, United Kingdom BSRC he
More informationSolutions to Problems : Chapter 19 Problems appeared on the end of chapter 19 of the Textbook
Solutions to Poblems Chapte 9 Poblems appeae on the en of chapte 9 of the Textbook 8. Pictue the Poblem Two point chages exet an electostatic foce on each othe. Stategy Solve Coulomb s law (equation 9-5)
More informationCONTROL SYSTEMS. Chapter 5 : Root Locus Diagram. GATE Objective & Numerical Type Solutions. The transfer function of a closed loop system is
CONTROL SYSTEMS Chapter 5 : Root Locu Diagram GATE Objective & Numerical Type Solution Quetion 1 [Work Book] [GATE EC 199 IISc-Bangalore : Mark] The tranfer function of a cloed loop ytem i T () where i
More informationMath 124B February 02, 2012
Math 24B Febuay 02, 202 Vikto Gigoyan 8 Laplace s equation: popeties We have aleady encounteed Laplace s equation in the context of stationay heat conduction and wave phenomena. Recall that in two spatial
More informationTutorial 5 Drive dynamics & control
UNIVERSITY OF NEW SOUTH WALES Electic Dive Sytem School o Electical Engineeing & Telecommunication ELEC463 Electic Dive Sytem Tutoial 5 Dive dynamic & contol. The ollowing paamete ae known o two high peomance
More informationTHE JEU DE TAQUIN ON THE SHIFTED RIM HOOK TABLEAUX. Jaejin Lee
Koean J. Math. 23 (2015), No. 3, pp. 427 438 http://dx.doi.og/10.11568/kjm.2015.23.3.427 THE JEU DE TAQUIN ON THE SHIFTED RIM HOOK TABLEAUX Jaejin Lee Abstact. The Schensted algoithm fist descibed by Robinson
More informationControl Systems Analysis and Design by the Root-Locus Method
6 Control Sytem Analyi and Deign by the Root-Locu Method 6 1 INTRODUCTION The baic characteritic of the tranient repone of a cloed-loop ytem i cloely related to the location of the cloed-loop pole. If
More informationA Power Method for Computing Square Roots of Complex Matrices
JOURNAL OF MATHEMATICAL ANALYSIS AND APPLICATIONS 13, 39345 1997 ARTICLE NO. AY975517 A Powe Method fo Computing Squae Roots of Complex Matices Mohammed A. Hasan Depatment of Electical Engineeing, Coloado
More informationThe Root Locus Method
The Root Locu Method MEM 355 Performance Enhancement of Dynamical Sytem Harry G. Kwatny Department of Mechanical Engineering & Mechanic Drexel Univerity Outline The root locu method wa introduced by Evan
More informationCOORDINATE TRANSFORMATIONS - THE JACOBIAN DETERMINANT
COORDINATE TRANSFORMATIONS - THE JACOBIAN DETERMINANT Link to: phsicspages home page. To leave a comment o epot an eo, please use the auilia blog. Refeence: d Inveno, Ra, Intoducing Einstein s Relativit
More information10/04/18. P [P(x)] 1 negl(n).
Mastemath, Sping 208 Into to Lattice lgs & Cypto Lectue 0 0/04/8 Lectues: D. Dadush, L. Ducas Scibe: K. de Boe Intoduction In this lectue, we will teat two main pats. Duing the fist pat we continue the
More informationRelated Rates - the Basics
Related Rates - the Basics In this section we exploe the way we can use deivatives to find the velocity at which things ae changing ove time. Up to now we have been finding the deivative to compae the
More informationControl Systems Engineering ( Chapter 7. Steady-State Errors ) Prof. Kwang-Chun Ho Tel: Fax:
Control Sytem Engineering ( Chapter 7. Steady-State Error Prof. Kwang-Chun Ho kwangho@hanung.ac.kr Tel: 0-760-453 Fax:0-760-4435 Introduction In thi leon, you will learn the following : How to find the
More informationMarch 18, 2014 Academic Year 2013/14
POLITONG - SHANGHAI BASIC AUTOMATIC CONTROL Exam grade March 8, 4 Academic Year 3/4 NAME (Pinyin/Italian)... STUDENT ID Ue only thee page (including the back) for anwer. Do not ue additional heet. Ue of
More informationAE 423 Space Technology I Chapter 2 Satellite Dynamics
AE 43 Space Technology I Chapte Satellite Dynamic.1 Intoduction In thi chapte we eview ome dynamic elevant to atellite dynamic and we etablih ome of the baic popetie of atellite dynamic.. Dynamic of a
More informationOn a proper definition of spin current
On a pope definition of pin cuent Qian Niu Univeity of Texa at Autin P. Zhang, Shi, Xiao, and Niu (cond-mat 0503505) P. Zhang and Niu (cond-mat/0406436) Culce, Sinova, Sintyn, Jungwith, MacDonald, and
More informationEcon 201: Problem Set 2 Answers
Econ 0: Poblem Set Anses Instucto: Alexande Sollaci T.A.: Ryan Hughes Winte 08 Question (a) The fixed cost is F C = 4 and the total vaiable costs ae T CV (y) = 4y. (b) To anse this question, let x = (x,...,
More informationChapter 3: Theory of Modular Arithmetic 38
Chapte 3: Theoy of Modula Aithmetic 38 Section D Chinese Remainde Theoem By the end of this section you will be able to pove the Chinese Remainde Theoem apply this theoem to solve simultaneous linea conguences
More informationNew problems in universal algebraic geometry illustrated by boolean equations
New poblems in univesal algebaic geomety illustated by boolean equations axiv:1611.00152v2 [math.ra] 25 Nov 2016 Atem N. Shevlyakov Novembe 28, 2016 Abstact We discuss new poblems in univesal algebaic
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 informationTHE CONE THEOREM JOEL A. TROPP. Abstract. We prove a fixed point theorem for functions which are positive with respect to a cone in a Banach space.
THE ONE THEOEM JOEL A. TOPP Abstact. We pove a fixed point theoem fo functions which ae positive with espect to a cone in a Banach space. 1. Definitions Definition 1. Let X be a eal Banach space. A subset
More informationGeometry Contest 2013
eomety ontet 013 1. One pizza ha a diamete twice the diamete of a malle pizza. What i the atio of the aea of the lage pizza to the aea of the malle pizza? ) to 1 ) to 1 ) to 1 ) 1 to ) to 1. In ectangle
More informationSOME GENERAL NUMERICAL RADIUS INEQUALITIES FOR THE OFF-DIAGONAL PARTS OF 2 2 OPERATOR MATRICES
italian jounal of pue and applied mathematics n. 35 015 (433 44) 433 SOME GENERAL NUMERICAL RADIUS INEQUALITIES FOR THE OFF-DIAGONAL PARTS OF OPERATOR MATRICES Watheq Bani-Domi Depatment of Mathematics
More informationBogoliubov Transformation in Classical Mechanics
Bogoliubov Tranformation in Claical Mechanic Canonical Tranformation Suppoe we have a et of complex canonical variable, {a j }, and would like to conider another et of variable, {b }, b b ({a j }). How
More information