Strong Stochastic Stability for MANET Mobility Models

Size: px
Start display at page:

Download "Strong Stochastic Stability for MANET Mobility Models"

Transcription

1 trong tochatic tability for MAET Mobility Model R. Timo, K. Blacmore and L. Hanlen Department of Engineering, the Autralian ational Univerity, Canberra {roy.timo, Wirele ignal roceing, ICTA, Canberra Abtract At the core of any MAET imulation i a mobility model. To help enure reliable imulation reult, it i of interet to now if the mobility model i table: Will time-averaged meaurement of mobility model event converge? For example, doe the time-averaged ditance between a pair of node converge a imulation time increae? In thi paper, we tudy the tability of a cla of dicrete Random Waypoint Mobility Model RWMM. Thi cla include the claic Random Waypoint Mobility Model. We how that each mobility model in thi cla atifie a pointwie ergodic theorem a generalized trong law of large number; thu, all bounded time-averaged meaurement of mobility model event converge with probability one. A corollary of thi ergodic theorem how that each mobility model in thi cla alo poee a time-tationary regime. I. ITRODUCTIO rotocol for Mobile Ad-Hoc etwor MAET are contructed uing imulation. Mobility model [] are ued to generate node movement in imulation. It i well documented [2 5] that untable mobility model may lead to imulation reult that are unreliable. We define and tudy a cla of tochatically table mobility model, which include the claic Random Waypoint Mobility Model RWMM. Boudec and Vojnović [5] proved that a general verion of the claic RWMM the Random Trip Mobility Model i table. Thi tability property followed from the exitence and uniquene of a tationary ditribution for node location. We extend thi idea and ay that a mobility model i table if it atifie a pointwie ergodic theorem. If it i not table, then the relative frequency of event may not converge and imulation reult involving time average may change in time. A trong motivation for thi tudy i that a mobility model tability or intability may be paed up though the networ layer. For example, in [6] we how that the Dynamic ource Routing DR protocol preerve the tability of the mobility model; if the pointwie ergodic theorem hold for the mobility model, then it alo hold for the route election random proce. etwor imulation are baed on time average, o the ignificance of thi reult i immediate: If the mobility model i table and the routing protocol preerve thi tability, then the trong law of large number hold for networ layer imulation. A mobility model define a random proce. It i aid to be tationary if the probability law governing node movement doe not change in time. The trong law of large number hold for tationary mobility model, o many wor [4, 5, 7] have developed method which tranform non-tationary model into tationary model. tationary mobility model alo atify the tronger pointwie ergodic theorem. The following example illutrate how thi theorem may be ued. Example : uppoe a node i moved uing a tationary mobility model. Denote it location at time n with the random variable X n. In a imulation we record the node location over time with the equence x x 0, x, x 2,.... ince {X n } i tationary, Birhoff ergodic theorem [8, g. 30] aert that the limit f x lim f x n, x n+, x n+2,... exit almot everywhere a.e. for every bounded meaurement function f. For example, uppoe we are intereted in etimating the mean probability of ome mobility model event A. Chooe f to be the indicator function: fx n, x n+,... A x n, x n+,... {, if xn, x n+,... A The limit A x i the relative frequency of A in x. If we repeat thi imulation a large number of time and average over the reulting relative frequencie A x, the reulting average will converge to the mean probability of event A. Unfortunately, the probability law governing node movement for mot mobility model are not contant in time [4, 5, 7]. Model, uch a the claic RWMM, may be locally non tationary and diplay tarting tranient. The et of tationary mobility model i too mall for the tudy of MAET. In thi paper, we replace the tationary condition with a weaer aymptotically tationary condition. That i, only the long-run behavior of the mobility model need to be tationary. For example, we permit both tarting tranient and local non tationary propertie. A random proce which i aymptotically governed by a tationary proce i called Aymptotically Mean tationary AM. Gray and Kieffer [9, Thm. ] howed that a random proce atifie the pointwie ergodic theorem if and only if it i AM; hence, we hall ay that a mobility model i table if and only if it i AM.

2 In [0, Lem. ] we demontrated that a retricted verion of the claic RWMM i AM. In thi paper we extend AM theory to a general cla of RWMM, which include the claic RWMM a a pecial cae. In the claic RWMM [], each node elect a equence of waypoint w w 0, w,... uing an independent and identically ditributed i.i.d. random proce {W n }. For each pair w i, w i+, i 0,,..., the node elect a peed uniformly at random from the interval [min peed, max peed]. It then travel in a traight line between w i and w i+ at thi peed. The main reult of thi paper Theorem may be ummarized a follow: The claic RWMM i AM table and ergodic, and 2 A ufficient condition for table node movement i: a each node elect waypoint uing an AM random proce, b given a equence of waypoint, each node elect it peed in a tationary fahion. The paper outline i a follow. otation and terminology are introduced in ection II. ection III define table, tationary, ergodic, and AM mobility model. The general RWMM i developed in ection IV, and ection V preent our main reult in Theorem. The paper i concluded in ection VI, and Theorem i proved in the Appendix. II. OTATIO AD TERMIOLOGY Often we hall be intereted in random procee with the ame probability law, but with different notion of time. For clarity, we adopt the dynamical ytem model for a random proce [, 2] give excellent introduction. Let X {X n } be a dicrete time random proce with a dicrete finite alphabet X. We are intereted in the probabilitic behavior of mobility model, o we hall tudy the ditribution of {X n }. The th order joint ditribution of {X n } i the probability meaure on X defined by µ x 0 rob { } X 0 x 0,..., X x where X i0 X i, X i X. The et {µ : 0} i called the ditribution of {X n }. If ome conitency condition are atified 2, the Kolmogorov Repreentation Theorem [, Thm. I..2] aert that we may replace the ditribution with a probability meaure µ on the equence pace X i0 X i, X i X. An important ubet of X i the cylinder et: [x n m] { x X : x i x i, m i n} Let F X denote the σ-field generated [8, g. 2] by cylinder et. The action of time i captured with the hift tranform T n X x x n, x n+, x n+2,..., n Z The pair X, F X i a meaurable pace, the triple X, F X, µ i a probability pace, and the quadruple ode peed wa aumed to be contant. 2 The model tudied in thi paper atify thee condition. X, F X, µ, T X i a dynamical ytem. The original random proce {X n } i related to X, F X, µ, T X by {X n } {Π 0 TX nx} where Π 0x x 0. Why i thi model ueful? uppoe a node i moved according to ome mobility model, which may be decribed by the random proce {X n }. uppoe we record the node poition for the firt n time tep of a imulation: x n 0 x 0, x,..., x n. Thi imulation may be thought of a a probabilitic experiment where the node trajectory x n 0 i an event. The probability pace for thi experiment i X, F X, µ, and the trajectory x n 0 define the event [x n 0 ] F X. Thu, the probability that the trajectory i randomly choen to be x n 0 i µ[x n 0 ]. The ytem X, F X, µ, T X pecifie both the probability pace X, F X, µ and the hift T X. The hift pecifie what time cale i of interet. Thi model i ueful becaue one often need to conider different time cale for the ame mobility model. For example, uppoe we are given a mobility model to which we aociate the probability pace X, F X, µ. Let T X be given by, and let T X be a variable hift defined by T X x T fx X x x fx, x fx+,... where f : X Z. The propertie of the random proce {X n } aociated with T X are almot alway different to the random proce {Xn} aociated with T X. If one i intereted in the behavior of node with repect to T X, then one tudie X, F X, µ, T X. However, if one i intereted in the behavior of node with repect to T X for example, networ router reet their routing table at time at time defined by f then one tudie X, F X, µ, T X. III. TABLE MOBILITY MODEL uppoe the ytem X, F X, µ, T X decribe the mobility model and time cale of interet. A random proce i aid to be tationarity if it probability law doe not change in time. The following definition formalize thi tatement. Definition tationary: The ytem X, F X, µ, T X i aid to be tationary if, for all A F X, we have µa µ T X A, where T X A {x X : T X x A}. The pointwie ergodic theorem hold for tationary ytem: Lemma Birhoff ointwie Ergodic Theorem: [8, Thm. 24.] If X, F X, µ, T X i tationary and f i bounded and meaurable, then the limit f x lim f TX n x exit almot everywhere in µ a.e. [µ]. The value of f x in Lemma i, in general, random. A ytem where f x i contant a.e. [µ] i called ergodic. Definition 2 Ergodic: The ytem X, F X, µ, T X i aid to be ergodic if A T X A implie µa 0 or. Equivalently, a ytem X, F X, µ, T X i ergodic if and only if, for all bounded meaurable function f, the limit f f x lim f TX n x

3 i contant a.e. [µ]. Definition 3 table Mobility Model: A mobility model with dynamical ytem model X, F X, µ, T X i aid to be table if, for every bounded meaurable f, the limit f x lim f TX n x exit a.e. [µ]. From Lemma and Definition 2, it i clear that mobility model which are tationary and / or ergodic are table. However, mobility model do not need to be tationary or ergodic to be table; for example, the claic RWMM i nontationary but table [5]. A we hall ee, the following cla of random procee provide ueful tool for checing the tability of mobility model. Definition 4 Aymptotic Mean tationary AM: The ytem X, F X, µ, T X i aid to be aymptotic mean tationary if, for all A F X, the following limit exit µa lim µ T n X A 2 If X, F X, µ, T X i AM, then 2 define a probability meaure µ on X, F X. The probability meaure µ decribe the long-run average behavior of the ytem, and it i called the tationary mean of µ. Gray and Kieffer [9] howed that AM i both neceary and ufficient for the pointwie ergodic theorem. Lemma 2 AM ointwie Ergodic Theorem: [9, Thm. ] A ytem X, F X, µ, T X i AM if and only if, for every bounded meaurable f, the limit f x lim f TX n x exit a.e. [µ]. For u, Definition 4 and Lemma 2 provide an alternative decription for table mobility model. Lemma 3 table Mobility Model: uppoe we are given a mobility model to which we aociate the probability pace X, F X, µ. The model i table with repect to T X if and only if X, F X, µ, T X i AM. IV. A GEERAL RADOM WAYOIT MOBILITY MODEL In thi ection we preent a general dicrete RWMM. Conider a networ with V mobile node V {v, v 2,..., v V }, where each node i located in a dicrete finite pace. We ue four random procee to decribe the general RWMM. A. Waypoint Random roce er ode Each node v V elect a equence of waypoint w w 0, w,... in a random fahion from the pace. Let W {W i } i0 denote the random proce decribing how the waypoint are elected, and let W, F W, µ w, T W be the correponding dynamical ytem, where W. Example 2 Claic RWMM: In the claic RWMM, the waypoint are choen independently and identically ditributed p 2 5 p 3 6 p Fig.. Random peed election in dicrete pace and time i equivalent to random path election. The tate pace i {, 2,..., 3 }. uppoe the node mut travel from waypoint w to waypoint w 3. The path p, p 2 and p 3 where, for example, p 2, 7, 3, demontrate how the node location i ampled. i.i.d. from W. In thi cae, µ w i a product meaure, and T W i a Bernoulli hift [8, g. 3]. B. ath Random roce er ode Recall the claic RWMM. uppoe node v elect the equence of waypoint w. For each pair w i, w i+, i Z {0,,...}, the node elect a peed uniformly at random from [min peed, max peed]. It then travel in a traight line between w i and w i+ at thi peed. In dicrete pace and time, the node poition i ampled during it trip between w i and w i+ a lower peed will reult in more intermediate ample. The dicrete time equivalent to a random peed i a random path. At each time hift, the node move one tep along the path. Thi idea i depicted in Figure. For each pair w, w W label each path, which connect w and w, with a unique element from the finite et w,w {p, p 2,..., p w,w } Let denote the et of all path w,w W W w,w and i0 i, i, the collection of path equence. We hall now define the random proce { n }, which decribe the election of path. ince conditionally depend on W, the mot convenient way to define i via a channel. Given a equence of waypoint w, node v may randomly elect any equence of path p, which connect the element of w. Fix w W and let u define the collection of allowable path equence w by w {p : p i wi,w i+, i Z } Let F be the σ-field of ubet of generated by cylinder et. Let u define a family of probability meaure ν wp {ν w : w W } on, F uch that ν w w. The triple W, νwp, i called a channel.

4 We hall be intereted in a pecial type of channel: Definition 5 tationary Channel: The channel W, ν wp, i aid to be T W, T tationary if ν TW w A νw T A with w W and A F. Example 3 Claic RWMM: In the claic RWMM, when node v reache waypoint w i, it elect a peed uniformly at random from [min peed, max peed]. In dicrete time and pace, thi i equivalent to electing a path uniformly at random from the et wi,w i+. The dicrete RWMM define a channel W, ν wp,, where ν wp {ν w : w W, } and ν w [p n 0 ] n 2 i0 wi,w i+ if p i wi,w i+, i 0,..., n 2 ote: ν w w, for every w W. 2 ν ha finite input memory of order 2, ee [3, g ]. We now how that thi channel i tationary. Fix w W and conider any p n 0 n it i ufficient to conider cylinder et, then ν TW w [p n 0 ] n 2 i0 3 wi+,w i+2, if p i wi+,w i+2, i 0,..., n 2 4 Let p j+ p j for 0 j n, o that [ p n ] T [pn 0 ]. 0 ] ν w [ p n ] ν w T [pn n 2 i0 wi+,w i+2, if p i wi+,w i+2, i 0,..., n 2 Combine 4 and 5 to ee that the channel i tationary. We hall alo be intereted in the following type of channel. Definition 6 tationary and Ergodic Channel: A tationary channel W, ν wp, i aid to be ergodic if, for all A, B F W, we have lim ν wp T n W A B ν wp A νwp B Example 4 Claic RWMM: We now how that the channel 3 i tationary and ergodic. In thi cae, however, it i eaier to how that the channel atifie a tronger condition called output mixing. A channel i aid to be output mixing if, for all A, B F W and all w W, we have lim ν w T n A B ν w T n A ν w B 0 6 ince F i generated by cylinder et, it i ufficient to how 6 hold for any [p a 0 ], [p b 0 ] F. Let T n [pa 0 ] [ p n+a n ], where p i+n p i, 0 i a. For any n > b the cylinder et [ p n+a n 5 ] and [p b 0 ] depend on value of p i for indice i in dijoint et of integer. ee [, g. 8] for a imilar example. For any > b, we have 7, o 6 hold and the channel i mixing. Recall [4, Lem ] to ee that the channel i alo wea mixing and ergodic. The waypoint random proce W, F W, µ w, T W and the channel W, ν wp, induce a joint probability meaure µν wp on the input-output pace W, F W F µν wp A B µw ν w B w A where A F W and B F. The ditribution of the path random proce i given by µ p B µν wp W B µw ν w B w W where B F. Let, F, µ p, T be the correponding dynamical ytem for { n }. C. Location Random roce er ode uppoe node v elect the equence of path p to connect waypoint w. The total time n i required to travel from waypoint w 0 to waypoint w i i a function of the length of the firt i path p i 0 p 0, p,..., p i. Let lp i denote the length of the i th path p i, o that it tae lp i time tep to move from w i to w i+. We aume the length of each path i non zero and finite: 0 < lp <, p. Let { i n i j0 lp j, if i > 0 8 If we ue 8 to define time, the i th path p i connecting waypoint w i and w i+ tae the form ni, ni+,..., ni+, where j for n i j n i+. The equence of path p mut connect the connect the equence of waypoint w, o we mut have ni w i for all i 0,, 2,.... Given a equence of path p, the node actual movement i given by 0,,.... We let { n } denote the random proce decribing the movement of node v. Let, F, µ, T be the correponding dynamical ytem. D. Location Random roce All ode Let n,v denote the location of node v at time n. Let X n n,, n,2,..., n, V denote the location of every node in at time n. Thi random variable tae value from the dicrete finite pace X V V i i, i. The random proce {X n } repreent the location of all V node in over time n Z. Let X, F X, µ x, T X be the ytem for {X n }. V. MAI REULT Theorem : uppoe the node V {v, v 2,..., v V } are moved randomly uing the general dicrete RWMM defined in ection IV. Let W v and v denote the waypoint and path random procee for node v. Let W v, ν wp, v denote the channel connecting the path and waypoint procee, and let X denote the location proce for every node in the networ. a If, for all v V, W v i AM and W v, ν wp, v i tationary, then X i AM table. b If, for all v V, W v i ergodic, W v, ν wp, v i tationary and ergodic, then X i ergodic.

5 ν w T [pa +a 2 0 ] [p b 0 ] ν w b 2 j wj+,w j+2 [ p +a i0 ] [p b 0 ] wi+,w i+2, if p i wi+,w i+2, i 0,..., b 2, and p j wj+,w j+2, j,..., + a 2, ν w T [pa 0 ] ν µ [p b 0 ] 7 roof: [Theorem ] leae refer to the Appendix. Corollary.: The claic RWMM i AM table and ergodic. roof: [Corollary.] ee Example 2, 3 and 4. VI. COCLUIO In thi paper, a mobility model i aid to be table if it atifie a pointwie ergodic theorem. We how that a mobility model i table if and only if it i probabilitically decribed by an Aymptotically Mean tationary AM random proce. An AM random proce i a generalization of a tationary random proce, which permit tarting tranient and local non-tationary behavior. ince mot mobility model exhibit uch non-tationary propertie, the theory of AM random procee i ideal for the tudy of mobility model. We ue AM theory how that a general cla of dicrete Random Waypoint Mobility Model RWMM i table. Thi cla include, a a pecial cae, the claic RWMM which i ued throughout the MAET literature. The main reult of the paper how that any RWMM i table if node waypoint and peed are elected in a tationary fahion. Thi reult allow networ deigner to tailor table RWMM for individual networ requirement. AEDIX roof: [Theorem ] The proof ue three lemma: Lemma 4: If W v i AM and ergodic and W v, ν wp, v i tationary and ergodic, then v i AM and ergodic. Lemma 5: If v i AM, then v i AM. Lemma 6: If v i ergodic, then v i ergodic. The movement of each node i independent of all other node, o the theorem follow directly from Lemma 4, 5 and 6. We hall drop the ubcript v in the following three proof. roof: [Lemma 4] The channel W, ν wp, connect the waypoint random proce W, F W, µ w, T W to the path random proce, F, µ p, T. The Lemma i a direct conequence of [4, Lem and 9.3.3]. roof: [Lemma 5] Aume, F, µ p, T i AM. Each p i a label for ome path 0,,..., lp, where lp denote path length. Let f : C mar the connection between path label and path, and let L max{lp : p }. For each p, we have fp 0,,..., lp C, where C L i i. Let, F, µ, T be the ytem repreenting node movement. Thi ytem i formed by concatenating path: { n } f 0, f,... 0,..., l0, l0,..., l0+l,... Thi relationhip may be implified by defining a equenceto-equence coder: F :. et F p fp 0, fp, fp 2,.... For all A F, the meaure µ on, F i connected to the meaure µ p on, F by µ A µ p F A, where F A {p : F p A}. Let B denote the et of bounded meaurable function on, F. By the AM pointwie ergodic theorem [9, Thm. ], there exit a ubet of equence of full meaure µ p, uch that the limit g p lim g T n p 9 exit for every p and every g B. Let Ŝ denote the range of F when the domain of F i retricted to : Ŝ { : p, F p }. It Ŝ then follow, µ µ p F Ŝ µ p. Let {A } Ŝ be the partition of where A { p : F p }. ote: the et A are nonempty for every Ŝ. For each Ŝ, chooe a equence p A, o that we may define the peudo-invere F : Ŝ, where F p. For each p and n 0,, 2,..., let u define γ p n n i0 lp i o that we may define the variable-length hift T : : T n Γn T, where { γ Γ n F n, if Ŝ, if / Ŝ Let B denote the et of bounded meaurable function on, F. ic any h B and any Ŝ, then lim up h T n lim up lim up lim up h T Γn 0 h ΓnF p T F p h F Tp n

6 lim up g T n p g p 2 where follow by etting g h F, and 2 follow from 9 and g B. imilarly, we have lim inf h T n g p o that the limit lim h T n exit for every Ŝ, and every h B. ince µ Ŝ, by Lemma 2 the ytem, F, µ, T i AM. By Lemma 7 below we alo have that the ytem, F, µ, T i AM hence, i AM. Lemma 7: Let, F, µ, T be a dynamical ytem and conider the variable length hift T : T n γ T 3 where γ L. If, F, µ, T i AM with tationary mean µ, then, F, µ, T i AM. roof: [Lemma 7] how: if µ i T invariant, then µ i AM with repect to T. We follow [9, E.x. 4]. Define a new meaure µ A E µ [γ] L i0 µ T i A 4 where { : γ }. The et { }L i a partition of, o T A L T A. Alo, µ T A µ A L µ T A L µ A 5 ubtitute T A into 4 and ue 5 to how that µ i T invariant. µ T A L Eµ µ T i A [γ] i0 L µ A + E µ [γ] L µ A µ T A µ A 6 If µ A 0, then lim µ T n A 0. Here µ i aid to aymptotically dominate µ T under T, µ µ. The meaure µ and µ are defined on the ame meaure pace T, F. Ue µ µ with 6 and [9, Thm. 2] to ee that µ i AM with repect to T. 2 how: If µ i AM with repect to T, then µ i AM with repect to T. The ytem, F, µ, T i AM, and the ytem, F, µ, T i tationary. If µ A 0 and T A A, it follow that µ A 0. Furthermore, if A T A, then A T n A for any n, o A i alo T invariant: A T A. If µ A 0 and A T A, it follow that µ A 0. Hence, if µ A 0 and A T A, then µ A 0. Theorem [5, Thm. 2.2] complete the proof. roof: [Lemma 6] Aume, F, µ p, T i ergodic. uppoe A F i T invariant, A T A. By definition, we have that A T n A for all n. Fix A, then for every p where F p, we have F p A T n T n F p A. Thi implie F p A T lp0 F p A, and therefore F p A F T p A 7 ince 7 hold for each A and every p aociated with each, we have that p F A T p F A; hence, F A T F A. ince, F, µ p, T i ergodic, we have that µ p F A 0 or ; therefore, µ A 0 of. By definition,, F, µ, T i ergodic. REFERECE [] T. Camp, J. Boleng, and V. Davie, A urvey of Mobility Model for Ad Hoc etwor Reearch, IEEE Tran. Wirele Commun., vol. 2, no. 4, pp , eptember [2]. Kurowi, T. Camp, and M. Colagroo, MAET imulation tudie: The Incredible, ACM IGMOBILE Mobile Comp. and Commun. Review MC 2 R, vol. 9, no. 4, pp , October [3] T. Andel and A. Yainac, On the Credibility of MAET imulation, Computer, vol. 39, no. 7, pp , July [4] J. Yoon, M. Liu, and B. oble, ound Mobility Model, in roc. IEEE Intl. ymp. Mobile Ad Hoc et. and Comp., MobiHoc, eptember 2003, pp [5] J. Boudec and M. Vojnović, The Random Trip Model: tability, tationary Regime, and erfect imulation, IEEE/ACM Tran. etworing, vol. 4, no. 6, pp , December [6] R. Timo, K. Blacmore, and J. apandriopoulo, trong tochatic tability for Dynamic ource Routing, Tech. Rep. A006280, ICTA, Augut [7] J. Yoon, M. Liu, and B. oble, Random Waypoint Conidered Harmful, in roc. IEEE Annual Joint Conf. IEEE Comp. and Commun. ocietie, IFOCOM, March 2003, vol. 2, pp [8]. Billingley, robability and Meaure, Wiley erie in probability and mathematical tatitic. John Wiley & on, 3 rd edition, 995. [9] R. Gray and J. Kieffer, Aymptotically Mean tationary Meaure, J. Ann. rob., vol. 8, no. 5, pp , October 980. [0] R. Timo, L. Hanlen, and K. Blacmore, A Lower Bound on etwor Layer Control Information, in Joint ACoR/EWCOM Worhop, Vienna, Autria, eptember []. hield, The Ergodic Theory of Dicrete ample ath, vol. 3 of Graduate tudie in Mathematic, American Mathematical ociety, 996. [2] R. Gray, robability Random rocee, and Ergodic ropertie, pringer Verlag, 200 Reviion 987, gray/. [3] A. Feintein, On the Coding Theorem and It Convere for Finite Memory Channel, Inform. and Contr., vol. 2, no., pp , April 959. [4] R. Gray, Entropy and Information Theory, pringer Verlag, 2000 Reviion 990, gray/. [5] Y. Kaihara, Ergodicity and Extremality of AM ource and Channel, International Journal of Mathematic and Mathematical cience, vol. 2003, no. 28, pp , 2003.

Chapter 2 Sampling and Quantization. In order to investigate sampling and quantization, the difference between analog

Chapter 2 Sampling and Quantization. In order to investigate sampling and quantization, the difference between analog Chapter Sampling and Quantization.1 Analog and Digital Signal In order to invetigate ampling and quantization, the difference between analog and digital ignal mut be undertood. Analog ignal conit of continuou

More information

c n b n 0. c k 0 x b n < 1 b k b n = 0. } of integers between 0 and b 1 such that x = b k. b k c k c k

c n b n 0. c k 0 x b n < 1 b k b n = 0. } of integers between 0 and b 1 such that x = b k. b k c k c k 1. Exitence Let x (0, 1). Define c k inductively. Suppoe c 1,..., c k 1 are already defined. We let c k be the leat integer uch that x k An eay proof by induction give that and for all k. Therefore c n

More information

Some Sets of GCF ϵ Expansions Whose Parameter ϵ Fetch the Marginal Value

Some Sets of GCF ϵ Expansions Whose Parameter ϵ Fetch the Marginal Value Journal of Mathematical Reearch with Application May, 205, Vol 35, No 3, pp 256 262 DOI:03770/jin:2095-26520503002 Http://jmredluteducn Some Set of GCF ϵ Expanion Whoe Parameter ϵ Fetch the Marginal Value

More information

Social Studies 201 Notes for March 18, 2005

Social Studies 201 Notes for March 18, 2005 1 Social Studie 201 Note for March 18, 2005 Etimation of a mean, mall ample ize Section 8.4, p. 501. When a reearcher ha only a mall ample ize available, the central limit theorem doe not apply to the

More information

Given the following circuit with unknown initial capacitor voltage v(0): X(s) Immediately, we know that the transfer function H(s) is

Given 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 information

CHAPTER 4 DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL

CHAPTER 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 information

IEOR 3106: Fall 2013, Professor Whitt Topics for Discussion: Tuesday, November 19 Alternating Renewal Processes and The Renewal Equation

IEOR 3106: Fall 2013, Professor Whitt Topics for Discussion: Tuesday, November 19 Alternating Renewal Processes and The Renewal Equation IEOR 316: Fall 213, Profeor Whitt Topic for Dicuion: Tueday, November 19 Alternating Renewal Procee and The Renewal Equation 1 Alternating Renewal Procee An alternating renewal proce alternate between

More information

Lecture 10 Filtering: Applied Concepts

Lecture 10 Filtering: Applied Concepts Lecture Filtering: Applied Concept In the previou two lecture, you have learned about finite-impule-repone (FIR) and infinite-impule-repone (IIR) filter. In thee lecture, we introduced the concept of filtering

More information

List coloring hypergraphs

List coloring hypergraphs Lit coloring hypergraph Penny Haxell Jacque Vertraete Department of Combinatoric and Optimization Univerity of Waterloo Waterloo, Ontario, Canada pehaxell@uwaterloo.ca Department of Mathematic Univerity

More information

CHAPTER 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 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 information

Bogoliubov Transformation in Classical Mechanics

Bogoliubov 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

Social Studies 201 Notes for November 14, 2003

Social Studies 201 Notes for November 14, 2003 1 Social Studie 201 Note for November 14, 2003 Etimation of a mean, mall ample ize Section 8.4, p. 501. When a reearcher ha only a mall ample ize available, the central limit theorem doe not apply to the

More information

Gain and Phase Margins Based Delay Dependent Stability Analysis of Two- Area LFC System with Communication Delays

Gain and Phase Margins Based Delay Dependent Stability Analysis of Two- Area LFC System with Communication Delays Gain and Phae Margin Baed Delay Dependent Stability Analyi of Two- Area LFC Sytem with Communication Delay Şahin Sönmez and Saffet Ayaun Department of Electrical Engineering, Niğde Ömer Halidemir Univerity,

More information

1. The F-test for Equality of Two Variances

1. The F-test for Equality of Two Variances . The F-tet for Equality of Two Variance Previouly we've learned how to tet whether two population mean are equal, uing data from two independent ample. We can alo tet whether two population variance are

More information

Codes Correcting Two Deletions

Codes Correcting Two Deletions 1 Code Correcting Two Deletion Ryan Gabry and Frederic Sala Spawar Sytem Center Univerity of California, Lo Angele ryan.gabry@navy.mil fredala@ucla.edu Abtract In thi work, we invetigate the problem of

More information

Nonlinear Single-Particle Dynamics in High Energy Accelerators

Nonlinear Single-Particle Dynamics in High Energy Accelerators Nonlinear Single-Particle Dynamic in High Energy Accelerator Part 6: Canonical Perturbation Theory Nonlinear Single-Particle Dynamic in High Energy Accelerator Thi coure conit of eight lecture: 1. Introduction

More information

Preemptive scheduling on a small number of hierarchical machines

Preemptive scheduling on a small number of hierarchical machines Available online at www.ciencedirect.com Information and Computation 06 (008) 60 619 www.elevier.com/locate/ic Preemptive cheduling on a mall number of hierarchical machine György Dóa a, Leah Eptein b,

More information

Control Systems Analysis and Design by the Root-Locus Method

Control 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 information

USPAS Course on Recirculated and Energy Recovered Linear Accelerators

USPAS Course on Recirculated and Energy Recovered Linear Accelerators USPAS Coure on Recirculated and Energy Recovered Linear Accelerator G. A. Krafft and L. Merminga Jefferon Lab I. Bazarov Cornell Lecture 6 7 March 005 Lecture Outline. Invariant Ellipe Generated by a Unimodular

More information

Linear System Fundamentals

Linear 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 information

Finding the location of switched capacitor banks in distribution systems based on wavelet transform

Finding the location of switched capacitor banks in distribution systems based on wavelet transform UPEC00 3t Aug - 3rd Sept 00 Finding the location of witched capacitor bank in ditribution ytem baed on wavelet tranform Bahram nohad Shahid Chamran Univerity in Ahvaz bahramnohad@yahoo.com Mehrdad keramatzadeh

More information

arxiv: v2 [math.nt] 30 Apr 2015

arxiv: v2 [math.nt] 30 Apr 2015 A THEOREM FOR DISTINCT ZEROS OF L-FUNCTIONS École Normale Supérieure arxiv:54.6556v [math.nt] 3 Apr 5 943 Cachan November 9, 7 Abtract In thi paper, we etablih a imple criterion for two L-function L and

More information

Chapter 5 Consistency, Zero Stability, and the Dahlquist Equivalence Theorem

Chapter 5 Consistency, Zero Stability, and the Dahlquist Equivalence Theorem Chapter 5 Conitency, Zero Stability, and the Dahlquit Equivalence Theorem In Chapter 2 we dicued convergence of numerical method and gave an experimental method for finding the rate of convergence (aka,

More information

Multicolor Sunflowers

Multicolor Sunflowers Multicolor Sunflower Dhruv Mubayi Lujia Wang October 19, 2017 Abtract A unflower i a collection of ditinct et uch that the interection of any two of them i the ame a the common interection C of all of

More information

ON THE APPROXIMATION ERROR IN HIGH DIMENSIONAL MODEL REPRESENTATION. Xiaoqun Wang

ON THE APPROXIMATION ERROR IN HIGH DIMENSIONAL MODEL REPRESENTATION. Xiaoqun Wang Proceeding of the 2008 Winter Simulation Conference S. J. Maon, R. R. Hill, L. Mönch, O. Roe, T. Jefferon, J. W. Fowler ed. ON THE APPROXIMATION ERROR IN HIGH DIMENSIONAL MODEL REPRESENTATION Xiaoqun Wang

More information

New bounds for Morse clusters

New bounds for Morse clusters New bound for More cluter Tamá Vinkó Advanced Concept Team, European Space Agency, ESTEC Keplerlaan 1, 2201 AZ Noordwijk, The Netherland Tama.Vinko@ea.int and Arnold Neumaier Fakultät für Mathematik, Univerität

More information

A Constraint Propagation Algorithm for Determining the Stability Margin. The paper addresses the stability margin assessment for linear systems

A Constraint Propagation Algorithm for Determining the Stability Margin. The paper addresses the stability margin assessment for linear systems A Contraint Propagation Algorithm for Determining the Stability Margin of Linear Parameter Circuit and Sytem Lubomir Kolev and Simona Filipova-Petrakieva Abtract The paper addree the tability margin aement

More information

One Class of Splitting Iterative Schemes

One Class of Splitting Iterative Schemes One Cla of Splitting Iterative Scheme v Ciegi and V. Pakalnytė Vilniu Gedimina Technical Univerity Saulėtekio al. 11, 2054, Vilniu, Lithuania rc@fm.vtu.lt Abtract. Thi paper deal with the tability analyi

More information

Lecture 8: Period Finding: Simon s Problem over Z N

Lecture 8: Period Finding: Simon s Problem over Z N Quantum Computation (CMU 8-859BB, Fall 205) Lecture 8: Period Finding: Simon Problem over Z October 5, 205 Lecturer: John Wright Scribe: icola Rech Problem A mentioned previouly, period finding i a rephraing

More information

Problem 1. Construct a filtered probability space on which a Brownian motion W and an adapted process X are defined and such that

Problem 1. Construct a filtered probability space on which a Brownian motion W and an adapted process X are defined and such that Stochatic Calculu Example heet 4 - Lent 5 Michael Tehranchi Problem. Contruct a filtered probability pace on which a Brownian motion W and an adapted proce X are defined and uch that dx t = X t t dt +

More information

Unbounded solutions of second order discrete BVPs on infinite intervals

Unbounded solutions of second order discrete BVPs on infinite intervals Available online at www.tjna.com J. Nonlinear Sci. Appl. 9 206), 357 369 Reearch Article Unbounded olution of econd order dicrete BVP on infinite interval Hairong Lian a,, Jingwu Li a, Ravi P Agarwal b

More information

Convex Hulls of Curves Sam Burton

Convex Hulls of Curves Sam Burton Convex Hull of Curve Sam Burton 1 Introduction Thi paper will primarily be concerned with determining the face of convex hull of curve of the form C = {(t, t a, t b ) t [ 1, 1]}, a < b N in R 3. We hall

More information

DYNAMIC MODELS FOR CONTROLLER DESIGN

DYNAMIC MODELS FOR CONTROLLER DESIGN DYNAMIC MODELS FOR CONTROLLER DESIGN M.T. Tham (996,999) Dept. of Chemical and Proce Engineering Newcatle upon Tyne, NE 7RU, UK.. INTRODUCTION The problem of deigning a good control ytem i baically that

More information

Clustering Methods without Given Number of Clusters

Clustering Methods without Given Number of Clusters Clutering Method without Given Number of Cluter Peng Xu, Fei Liu Introduction A we now, mean method i a very effective algorithm of clutering. It mot powerful feature i the calability and implicity. However,

More information

into a discrete time function. Recall that the table of Laplace/z-transforms is constructed by (i) selecting to get

into a discrete time function. Recall that the table of Laplace/z-transforms is constructed by (i) selecting to get Lecture 25 Introduction to Some Matlab c2d Code in Relation to Sampled Sytem here are many way to convert a continuou time function, { h( t) ; t [0, )} into a dicrete time function { h ( k) ; k {0,,, }}

More information

Memoryle Strategie in Concurrent Game with Reachability Objective Λ Krihnendu Chatterjee y Luca de Alfaro x Thoma A. Henzinger y;z y EECS, Univerity o

Memoryle Strategie in Concurrent Game with Reachability Objective Λ Krihnendu Chatterjee y Luca de Alfaro x Thoma A. Henzinger y;z y EECS, Univerity o Memoryle Strategie in Concurrent Game with Reachability Objective Krihnendu Chatterjee, Luca de Alfaro and Thoma A. Henzinger Report No. UCB/CSD-5-1406 Augut 2005 Computer Science Diviion (EECS) Univerity

More information

Stochastic Optimization with Inequality Constraints Using Simultaneous Perturbations and Penalty Functions

Stochastic Optimization with Inequality Constraints Using Simultaneous Perturbations and Penalty Functions Stochatic Optimization with Inequality Contraint Uing Simultaneou Perturbation and Penalty Function I-Jeng Wang* and Jame C. Spall** The John Hopkin Univerity Applied Phyic Laboratory 11100 John Hopkin

More information

Problem Set 8 Solutions

Problem Set 8 Solutions Deign and Analyi of Algorithm April 29, 2015 Maachuett Intitute of Technology 6.046J/18.410J Prof. Erik Demaine, Srini Devada, and Nancy Lynch Problem Set 8 Solution Problem Set 8 Solution Thi problem

More information

Computers and Mathematics with Applications. Sharp algebraic periodicity conditions for linear higher order

Computers and Mathematics with Applications. Sharp algebraic periodicity conditions for linear higher order Computer and Mathematic with Application 64 (2012) 2262 2274 Content lit available at SciVere ScienceDirect Computer and Mathematic with Application journal homepage: wwweleviercom/locate/camwa Sharp algebraic

More information

Simple Observer Based Synchronization of Lorenz System with Parametric Uncertainty

Simple Observer Based Synchronization of Lorenz System with Parametric Uncertainty IOSR Journal of Electrical and Electronic Engineering (IOSR-JEEE) ISSN: 78-676Volume, Iue 6 (Nov. - Dec. 0), PP 4-0 Simple Oberver Baed Synchronization of Lorenz Sytem with Parametric Uncertainty Manih

More information

Lecture 7: Testing Distributions

Lecture 7: Testing Distributions CSE 5: Sublinear (and Streaming) Algorithm Spring 014 Lecture 7: Teting Ditribution April 1, 014 Lecturer: Paul Beame Scribe: Paul Beame 1 Teting Uniformity of Ditribution We return today to property teting

More information

Multi-dimensional Fuzzy Euler Approximation

Multi-dimensional Fuzzy Euler Approximation Mathematica Aeterna, Vol 7, 2017, no 2, 163-176 Multi-dimenional Fuzzy Euler Approximation Yangyang Hao College of Mathematic and Information Science Hebei Univerity, Baoding 071002, China hdhyywa@163com

More information

Advanced Digital Signal Processing. Stationary/nonstationary signals. Time-Frequency Analysis... Some nonstationary signals. Time-Frequency Analysis

Advanced Digital Signal Processing. Stationary/nonstationary signals. Time-Frequency Analysis... Some nonstationary signals. Time-Frequency Analysis Advanced Digital ignal Proceing Prof. Nizamettin AYDIN naydin@yildiz.edu.tr Time-Frequency Analyi http://www.yildiz.edu.tr/~naydin 2 tationary/nontationary ignal Time-Frequency Analyi Fourier Tranform

More information

Unavoidable Cycles in Polynomial-Based Time-Invariant LDPC Convolutional Codes

Unavoidable Cycles in Polynomial-Based Time-Invariant LDPC Convolutional Codes European Wirele, April 7-9,, Vienna, Autria ISBN 978--87-4-9 VE VERLAG GMBH Unavoidable Cycle in Polynomial-Baed Time-Invariant LPC Convolutional Code Hua Zhou and Norbert Goertz Intitute of Telecommunication

More information

A FUNCTIONAL BAYESIAN METHOD FOR THE SOLUTION OF INVERSE PROBLEMS WITH SPATIO-TEMPORAL PARAMETERS AUTHORS: CORRESPONDENCE: ABSTRACT

A FUNCTIONAL BAYESIAN METHOD FOR THE SOLUTION OF INVERSE PROBLEMS WITH SPATIO-TEMPORAL PARAMETERS AUTHORS: CORRESPONDENCE: ABSTRACT A FUNCTIONAL BAYESIAN METHOD FOR THE SOLUTION OF INVERSE PROBLEMS WITH SPATIO-TEMPORAL PARAMETERS AUTHORS: Zenon Medina-Cetina International Centre for Geohazard / Norwegian Geotechnical Intitute Roger

More information

Beta Burr XII OR Five Parameter Beta Lomax Distribution: Remarks and Characterizations

Beta Burr XII OR Five Parameter Beta Lomax Distribution: Remarks and Characterizations Marquette Univerity e-publication@marquette Mathematic, Statitic and Computer Science Faculty Reearch and Publication Mathematic, Statitic and Computer Science, Department of 6-1-2014 Beta Burr XII OR

More information

Green-Kubo formulas with symmetrized correlation functions for quantum systems in steady states: the shear viscosity of a fluid in a steady shear flow

Green-Kubo formulas with symmetrized correlation functions for quantum systems in steady states: the shear viscosity of a fluid in a steady shear flow Green-Kubo formula with ymmetrized correlation function for quantum ytem in teady tate: the hear vicoity of a fluid in a teady hear flow Hirohi Matuoa Department of Phyic, Illinoi State Univerity, Normal,

More information

Connectivity in large mobile ad-hoc networks

Connectivity in large mobile ad-hoc networks Weiertraß-Intitut für Angewandte Analyi und Stochatik Connectivity in large mobile ad-hoc network WOLFGANG KÖNIG (WIAS und U Berlin) joint work with HANNA DÖRING (Onabrück) and GABRIEL FARAUD (Pari) Mohrentraße

More information

Optimal Coordination of Samples in Business Surveys

Optimal Coordination of Samples in Business Surveys Paper preented at the ICES-III, June 8-, 007, Montreal, Quebec, Canada Optimal Coordination of Sample in Buine Survey enka Mach, Ioana Şchiopu-Kratina, Philip T Rei, Jean-Marc Fillion Statitic Canada New

More information

Avoiding Forbidden Submatrices by Row Deletions

Avoiding Forbidden Submatrices by Row Deletions Avoiding Forbidden Submatrice by Row Deletion Sebatian Wernicke, Jochen Alber, Jen Gramm, Jiong Guo, and Rolf Niedermeier Wilhelm-Schickard-Intitut für Informatik, niverität Tübingen, Sand 13, D-72076

More information

Chip-firing game and a partial Tutte polynomial for Eulerian digraphs

Chip-firing game and a partial Tutte polynomial for Eulerian digraphs Chip-firing game and a partial Tutte polynomial for Eulerian digraph Kévin Perrot Aix Mareille Univerité, CNRS, LIF UMR 7279 3288 Mareille cedex 9, France. kevin.perrot@lif.univ-mr.fr Trung Van Pham Intitut

More information

Online Appendix for Managerial Attention and Worker Performance by Marina Halac and Andrea Prat

Online Appendix for Managerial Attention and Worker Performance by Marina Halac and Andrea Prat Online Appendix for Managerial Attention and Worker Performance by Marina Halac and Andrea Prat Thi Online Appendix contain the proof of our reult for the undicounted limit dicued in Section 2 of the paper,

More information

RELIABILITY OF REPAIRABLE k out of n: F SYSTEM HAVING DISCRETE REPAIR AND FAILURE TIMES DISTRIBUTIONS

RELIABILITY OF REPAIRABLE k out of n: F SYSTEM HAVING DISCRETE REPAIR AND FAILURE TIMES DISTRIBUTIONS www.arpapre.com/volume/vol29iue1/ijrras_29_1_01.pdf RELIABILITY OF REPAIRABLE k out of n: F SYSTEM HAVING DISCRETE REPAIR AND FAILURE TIMES DISTRIBUTIONS Sevcan Demir Atalay 1,* & Özge Elmataş Gültekin

More information

NCAAPMT Calculus Challenge Challenge #3 Due: October 26, 2011

NCAAPMT Calculus Challenge Challenge #3 Due: October 26, 2011 NCAAPMT Calculu Challenge 011 01 Challenge #3 Due: October 6, 011 A Model of Traffic Flow Everyone ha at ome time been on a multi-lane highway and encountered road contruction that required the traffic

More information

SMALL-SIGNAL STABILITY ASSESSMENT OF THE EUROPEAN POWER SYSTEM BASED ON ADVANCED NEURAL NETWORK METHOD

SMALL-SIGNAL STABILITY ASSESSMENT OF THE EUROPEAN POWER SYSTEM BASED ON ADVANCED NEURAL NETWORK METHOD SMALL-SIGNAL STABILITY ASSESSMENT OF THE EUROPEAN POWER SYSTEM BASED ON ADVANCED NEURAL NETWORK METHOD S.P. Teeuwen, I. Erlich U. Bachmann Univerity of Duiburg, Germany Department of Electrical Power Sytem

More information

Design By Emulation (Indirect Method)

Design By Emulation (Indirect Method) Deign By Emulation (Indirect Method he baic trategy here i, that Given a continuou tranfer function, it i required to find the bet dicrete equivalent uch that the ignal produced by paing an input ignal

More information

WELL-POSEDNESS OF A ONE-DIMENSIONAL PLASMA MODEL WITH A HYPERBOLIC FIELD

WELL-POSEDNESS OF A ONE-DIMENSIONAL PLASMA MODEL WITH A HYPERBOLIC FIELD WELL-POSEDNESS OF A ONE-DIMENSIONAL PLASMA MODEL WITH A HYPERBOLIC FIELD JENNIFER RAE ANDERSON 1. Introduction A plama i a partially or completely ionized ga. Nearly all (approximately 99.9%) of the matter

More information

Non-stationary phase of the MALA algorithm

Non-stationary phase of the MALA algorithm Stoch PDE: Anal Comp 018) 6:446 499 http://doi.org/10.1007/4007-018-0113-1 on-tationary phae of the MALA algorithm Juan Kuntz 1 Michela Ottobre Andrew M. Stuart 3 Received: 3 Augut 017 / Publihed online:

More information

7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281

7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281 72 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 28 and i 2 Show how Euler formula (page 33) can then be ued to deduce the reult a ( a) 2 b 2 {e at co bt} {e at in bt} b ( a) 2 b 2 5 Under what condition

More information

General System of Nonconvex Variational Inequalities and Parallel Projection Method

General System of Nonconvex Variational Inequalities and Parallel Projection Method Mathematica Moravica Vol. 16-2 (2012), 79 87 General Sytem of Nonconvex Variational Inequalitie and Parallel Projection Method Balwant Singh Thakur and Suja Varghee Abtract. Uing the prox-regularity notion,

More information

Hyperbolic Partial Differential Equations

Hyperbolic Partial Differential Equations Hyperbolic Partial Differential Equation Evolution equation aociated with irreverible phyical procee like diffuion heat conduction lead to parabolic partial differential equation. When the equation i a

More information

On Uniform Exponential Trichotomy of Evolution Operators in Banach Spaces

On Uniform Exponential Trichotomy of Evolution Operators in Banach Spaces On Uniform Exponential Trichotomy of Evolution Operator in Banach Space Mihail Megan, Codruta Stoica To cite thi verion: Mihail Megan, Codruta Stoica. On Uniform Exponential Trichotomy of Evolution Operator

More information

Lecture 4 Topic 3: General linear models (GLMs), the fundamentals of the analysis of variance (ANOVA), and completely randomized designs (CRDs)

Lecture 4 Topic 3: General linear models (GLMs), the fundamentals of the analysis of variance (ANOVA), and completely randomized designs (CRDs) Lecture 4 Topic 3: General linear model (GLM), the fundamental of the analyi of variance (ANOVA), and completely randomized deign (CRD) The general linear model One population: An obervation i explained

More information

5.5 Application of Frequency Response: Signal Filters

5.5 Application of Frequency Response: Signal Filters 44 Dynamic Sytem Second order lowpa filter having tranfer function H()=H ()H () u H () H () y Firt order lowpa filter Figure 5.5: Contruction of a econd order low-pa filter by combining two firt order

More information

Suggested Answers To Exercises. estimates variability in a sampling distribution of random means. About 68% of means fall

Suggested Answers To Exercises. estimates variability in a sampling distribution of random means. About 68% of means fall Beyond Significance Teting ( nd Edition), Rex B. Kline Suggeted Anwer To Exercie Chapter. The tatitic meaure variability among core at the cae level. In a normal ditribution, about 68% of the core fall

More information

Digital Control System

Digital Control System Digital Control Sytem - A D D A Micro ADC DAC Proceor Correction Element Proce Clock Meaurement A: Analog D: Digital Continuou Controller and Digital Control Rt - c Plant yt Continuou Controller Digital

More information

Copyright 1967, by the author(s). All rights reserved.

Copyright 1967, by the author(s). All rights reserved. Copyright 1967, by the author(). All right reerved. Permiion to make digital or hard copie of all or part of thi work for peronal or claroom ue i granted without fee provided that copie are not made or

More information

Advanced D-Partitioning Analysis and its Comparison with the Kharitonov s Theorem Assessment

Advanced D-Partitioning Analysis and its Comparison with the Kharitonov s Theorem Assessment Journal of Multidiciplinary Engineering Science and Technology (JMEST) ISSN: 59- Vol. Iue, January - 5 Advanced D-Partitioning Analyi and it Comparion with the haritonov Theorem Aement amen M. Yanev Profeor,

More information

arxiv: v1 [math.mg] 25 Aug 2011

arxiv: v1 [math.mg] 25 Aug 2011 ABSORBING ANGLES, STEINER MINIMAL TREES, AND ANTIPODALITY HORST MARTINI, KONRAD J. SWANEPOEL, AND P. OLOFF DE WET arxiv:08.5046v [math.mg] 25 Aug 20 Abtract. We give a new proof that a tar {op i : i =,...,

More information

Stable Soliton Propagation in a System with Spectral Filtering and Nonlinear Gain

Stable Soliton Propagation in a System with Spectral Filtering and Nonlinear Gain  Fiber and Integrated Optic, 19:31] 41, 000 Copyright Q 000 Taylor & Franci 0146-8030 r00 $1.00 q.00 Stable Soliton Propagation in a Sytem with Spectral Filtering and Nonlinear Gain  MARIO F. S. FERREIRA

More information

Optimal Strategies for Utility from Terminal Wealth with General Bid and Ask Prices

Optimal Strategies for Utility from Terminal Wealth with General Bid and Ask Prices http://doi.org/10.1007/00245-018-9550-5 Optimal Strategie for Utility from Terminal Wealth with General Bid and Ak Price Tomaz Rogala 1 Lukaz Stettner 2 The Author 2018 Abtract In the paper we tudy utility

More information

ON THE SMOOTHNESS OF SOLUTIONS TO A SPECIAL NEUMANN PROBLEM ON NONSMOOTH DOMAINS

ON THE SMOOTHNESS OF SOLUTIONS TO A SPECIAL NEUMANN PROBLEM ON NONSMOOTH DOMAINS Journal of Pure and Applied Mathematic: Advance and Application Volume, umber, 4, Page -35 O THE SMOOTHESS OF SOLUTIOS TO A SPECIAL EUMA PROBLEM O OSMOOTH DOMAIS ADREAS EUBAUER Indutrial Mathematic Intitute

More information

Sampling and the Discrete Fourier Transform

Sampling and the Discrete Fourier Transform Sampling and the Dicrete Fourier Tranform Sampling Method Sampling i mot commonly done with two device, the ample-and-hold (S/H) and the analog-to-digital-converter (ADC) The S/H acquire a CT ignal at

More information

SOME RESULTS ON INFINITE POWER TOWERS

SOME RESULTS ON INFINITE POWER TOWERS NNTDM 16 2010) 3, 18-24 SOME RESULTS ON INFINITE POWER TOWERS Mladen Vailev - Miana 5, V. Hugo Str., Sofia 1124, Bulgaria E-mail:miana@abv.bg Abtract To my friend Kratyu Gumnerov In the paper the infinite

More information

FOURIER SERIES AND PERIODIC SOLUTIONS OF DIFFERENTIAL EQUATIONS

FOURIER SERIES AND PERIODIC SOLUTIONS OF DIFFERENTIAL EQUATIONS FOURIER SERIES AND PERIODIC SOLUTIONS OF DIFFERENTIAL EQUATIONS Nguyen Thanh Lan Department of Mathematic Wetern Kentucky Univerity Email: lan.nguyen@wku.edu ABSTRACT: We ue Fourier erie to find a neceary

More information

OPTIMAL STOPPING FOR SHEPP S URN WITH RISK AVERSION

OPTIMAL STOPPING FOR SHEPP S URN WITH RISK AVERSION OPTIMAL STOPPING FOR SHEPP S URN WITH RISK AVERSION ROBERT CHEN 1, ILIE GRIGORESCU 1 AND MIN KANG 2 Abtract. An (m, p) urn contain m ball of value 1 and p ball of value +1. A player tart with fortune k

More information

Factor Analysis with Poisson Output

Factor Analysis with Poisson Output Factor Analyi with Poion Output Gopal Santhanam Byron Yu Krihna V. Shenoy, Department of Electrical Engineering, Neurocience Program Stanford Univerity Stanford, CA 94305, USA {gopal,byronyu,henoy}@tanford.edu

More information

Calculation of the temperature of boundary layer beside wall with time-dependent heat transfer coefficient

Calculation of the temperature of boundary layer beside wall with time-dependent heat transfer coefficient Ŕ periodica polytechnica Mechanical Engineering 54/1 21 15 2 doi: 1.3311/pp.me.21-1.3 web: http:// www.pp.bme.hu/ me c Periodica Polytechnica 21 RESERCH RTICLE Calculation of the temperature of boundary

More information

Reliability Analysis of Embedded System with Different Modes of Failure Emphasizing Reboot Delay

Reliability Analysis of Embedded System with Different Modes of Failure Emphasizing Reboot Delay International Journal of Applied Science and Engineering 3., 4: 449-47 Reliability Analyi of Embedded Sytem with Different Mode of Failure Emphaizing Reboot Delay Deepak Kumar* and S. B. Singh Department

More information

NONLINEAR CONTROLLER DESIGN FOR A SHELL AND TUBE HEAT EXCHANGER AN EXPERIMENTATION APPROACH

NONLINEAR CONTROLLER DESIGN FOR A SHELL AND TUBE HEAT EXCHANGER AN EXPERIMENTATION APPROACH International Journal of Electrical, Electronic and Data Communication, ISSN: 232-284 Volume-3, Iue-8, Aug.-25 NONLINEAR CONTROLLER DESIGN FOR A SHELL AND TUBE HEAT EXCHANGER AN EXPERIMENTATION APPROACH

More information

The continuous time random walk (CTRW) was introduced by Montroll and Weiss 1.

The continuous time random walk (CTRW) was introduced by Montroll and Weiss 1. 1 I. CONTINUOUS TIME RANDOM WALK The continuou time random walk (CTRW) wa introduced by Montroll and Wei 1. Unlike dicrete time random walk treated o far, in the CTRW the number of jump n made by the walker

More information

Chapter 4. The Laplace Transform Method

Chapter 4. The Laplace Transform Method Chapter 4. The Laplace Tranform Method The Laplace Tranform i a tranformation, meaning that it change a function into a new function. Actually, it i a linear tranformation, becaue it convert a linear combination

More information

A Simplified Methodology for the Synthesis of Adaptive Flight Control Systems

A Simplified Methodology for the Synthesis of Adaptive Flight Control Systems A Simplified Methodology for the Synthei of Adaptive Flight Control Sytem J.ROUSHANIAN, F.NADJAFI Department of Mechanical Engineering KNT Univerity of Technology 3Mirdamad St. Tehran IRAN Abtract- A implified

More information

TRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL

TRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL GLASNIK MATEMATIČKI Vol. 38583, 73 84 TRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL p-laplacian Haihen Lü, Donal O Regan and Ravi P. Agarwal Academy of Mathematic and Sytem Science, Beijing, China, National

More information

GNSS Solutions: What is the carrier phase measurement? How is it generated in GNSS receivers? Simply put, the carrier phase

GNSS Solutions: What is the carrier phase measurement? How is it generated in GNSS receivers? Simply put, the carrier phase GNSS Solution: Carrier phae and it meaurement for GNSS GNSS Solution i a regular column featuring quetion and anwer about technical apect of GNSS. Reader are invited to end their quetion to the columnit,

More information

The Hassenpflug Matrix Tensor Notation

The Hassenpflug Matrix Tensor Notation The Haenpflug Matrix Tenor Notation D.N.J. El Dept of Mech Mechatron Eng Univ of Stellenboch, South Africa e-mail: dnjel@un.ac.za 2009/09/01 Abtract Thi i a ample document to illutrate the typeetting of

More information

Theoretical Computer Science. Optimal algorithms for online scheduling with bounded rearrangement at the end

Theoretical Computer Science. Optimal algorithms for online scheduling with bounded rearrangement at the end Theoretical Computer Science 4 (0) 669 678 Content lit available at SciVere ScienceDirect Theoretical Computer Science journal homepage: www.elevier.com/locate/tc Optimal algorithm for online cheduling

More information

LTV System Modelling

LTV System Modelling Helinki Univerit of Technolog S-72.333 Potgraduate Coure in Radiocommunication Fall 2000 LTV Stem Modelling Heikki Lorentz Sonera Entrum O heikki.lorentz@onera.fi Januar 23 rd 200 Content. Introduction

More information

Molecular Dynamics Simulations of Nonequilibrium Effects Associated with Thermally Activated Exothermic Reactions

Molecular Dynamics Simulations of Nonequilibrium Effects Associated with Thermally Activated Exothermic Reactions Original Paper orma, 5, 9 7, Molecular Dynamic Simulation of Nonequilibrium Effect ociated with Thermally ctivated Exothermic Reaction Jerzy GORECKI and Joanna Natalia GORECK Intitute of Phyical Chemitry,

More information

Z a>2 s 1n = X L - m. X L = m + Z a>2 s 1n X L = The decision rule for this one-tail test is

Z a>2 s 1n = X L - m. X L = m + Z a>2 s 1n X L = The decision rule for this one-tail test is M09_BERE8380_12_OM_C09.QD 2/21/11 3:44 PM Page 1 9.6 The Power of a Tet 9.6 The Power of a Tet 1 Section 9.1 defined Type I and Type II error and their aociated rik. Recall that a repreent the probability

More information

Lecture 9: Shor s Algorithm

Lecture 9: Shor s Algorithm Quantum Computation (CMU 8-859BB, Fall 05) Lecture 9: Shor Algorithm October 7, 05 Lecturer: Ryan O Donnell Scribe: Sidhanth Mohanty Overview Let u recall the period finding problem that wa et up a a function

More information

White Rose Research Online URL for this paper: Version: Accepted Version

White Rose Research Online URL for this paper:   Version: Accepted Version Thi i a repoitory copy of Identification of nonlinear ytem with non-peritent excitation uing an iterative forward orthogonal leat quare regreion algorithm. White Roe Reearch Online URL for thi paper: http://eprint.whiteroe.ac.uk/107314/

More information

μ + = σ = D 4 σ = D 3 σ = σ = All units in parts (a) and (b) are in V. (1) x chart: Center = μ = 0.75 UCL =

μ + = σ = D 4 σ = D 3 σ = σ = All units in parts (a) and (b) are in V. (1) x chart: Center = μ = 0.75 UCL = Our online Tutor are available 4*7 to provide Help with Proce control ytem Homework/Aignment or a long term Graduate/Undergraduate Proce control ytem Project. Our Tutor being experienced and proficient

More information

NOTE: The items d) and e) of Question 4 gave you bonus marks.

NOTE: The items d) and e) of Question 4 gave you bonus marks. MAE 40 Linear ircuit Summer 2007 Final Solution NOTE: The item d) and e) of Quetion 4 gave you bonu mark. Quetion [Equivalent irciut] [4 mark] Find the equivalent impedance between terminal A and B in

More information

An Inequality for Nonnegative Matrices and the Inverse Eigenvalue Problem

An Inequality for Nonnegative Matrices and the Inverse Eigenvalue Problem An Inequality for Nonnegative Matrice and the Invere Eigenvalue Problem Robert Ream Program in Mathematical Science The Univerity of Texa at Dalla Box 83688, Richardon, Texa 7583-688 Abtract We preent

More information

CHAPTER 6. Estimation

CHAPTER 6. Estimation CHAPTER 6 Etimation Definition. Statitical inference i the procedure by which we reach a concluion about a population on the bai of information contained in a ample drawn from that population. Definition.

More information

4.6 Principal trajectories in terms of amplitude and phase function

4.6 Principal trajectories in terms of amplitude and phase function 4.6 Principal trajectorie in term of amplitude and phae function We denote with C() and S() the coinelike and inelike trajectorie relative to the tart point = : C( ) = S( ) = C( ) = S( ) = Both can be

More information

Relationship between surface velocity divergence and gas transfer in open-channel flows with submerged simulated vegetation

Relationship between surface velocity divergence and gas transfer in open-channel flows with submerged simulated vegetation IOP Conference Serie: Earth and Environmental Science PAPER OPEN ACCESS Relationhip between urface velocity divergence and ga tranfer in open-channel flow with ubmerged imulated vegetation To cite thi

More information

Microblog Hot Spot Mining Based on PAM Probabilistic Topic Model

Microblog Hot Spot Mining Based on PAM Probabilistic Topic Model MATEC Web of Conference 22, 01062 ( 2015) DOI: 10.1051/ matecconf/ 2015220106 2 C Owned by the author, publihed by EDP Science, 2015 Microblog Hot Spot Mining Baed on PAM Probabilitic Topic Model Yaxin

More information

HELICAL TUBES TOUCHING ONE ANOTHER OR THEMSELVES

HELICAL TUBES TOUCHING ONE ANOTHER OR THEMSELVES 15 TH INTERNATIONAL CONFERENCE ON GEOMETRY AND GRAPHICS 0 ISGG 1-5 AUGUST, 0, MONTREAL, CANADA HELICAL TUBES TOUCHING ONE ANOTHER OR THEMSELVES Peter MAYRHOFER and Dominic WALTER The Univerity of Innbruck,

More information