Probabilistic Reasoning in Bayesian Networks: A Relational Database Approach

Size: px
Start display at page:

Download "Probabilistic Reasoning in Bayesian Networks: A Relational Database Approach"

Transcription

1 Probbilistic Resoning in Byesin Networks: A Reltionl Dtbse Approch S.K.M. Wong, D. Wu nd C.J. Butz Deprtment of Computer Science, University of Regin Regin Ssktchewn, Cnd S4S 0A2 Abstrct. Probbilistic resoning in Byesin networks is normlly conducted on junction tree by repetedly pplying the locl propgtion whenever new evidence is observed. In this pper, we suggest to tret probbilistic resoning s dtbse queries. We dpt method for nswering queries in dtbse theory to the setting of probbilistic resoning in Byesin networks. We show n effective method for probbilistic resoning without repeted ppliction of locl propgtion whenever evidence is observed. 1 Introduction Byesin networks [3] hve been well estblished s model for representing nd resoning with uncertin informtion using probbility. Probbilistic resoning simply mens computing the mrginl distribution for set of vribles, or the conditionl probbility distribution for set of vribles given evidence. A Byesin network is normlly trnsformed through morliztion nd tringultion into junction tree on which the probbilistic resoning is conducted. One of the most populr methods for performing probbilistic resoning is the so-clled locl propgtion method [2]. The locl propgtion method is pplied to the junction tree so tht the junction tree reches consistent stte, i.e., mrginl distribution is ssocited with ech node in the junction tree. Probbilistic resoning cn then be subsequently crried out on this consistent junction tree [2]. In this pper, by exploring the intriguing reltionship between Byesin networks nd reltionl dtbses [5], we propose new pproch for probbilistic resoning by treting it s dtbse query. This new pproch hs severl slient fetures. (1) It dvoctes using hypertree insted of junction tree for probbilistic resoning. By selectively pruning the hypertree, probbilistic resoning cn be performed by employing the locl propgtion method once nd cn then nswer ny queries without nother ppliction of locl propgtion. (2) The structure of fixed junction tree my be fvourble to some queries but not to others. By using the hypertree s the secondry structure, we cn dynmiclly prune the hypertree to obtin the best choice for nswering ech query. (3) Finlly, this dtbse perspective of probbilistic resoning provides mple opportunities for well developed techniques in dtbse theory, especilly

2 techniques in query optimiztion, to be dopted for chieving more efficient probbilistic resoning in prctice. The pper is orgnized s follows. We briefly review Byesin networks nd locl propgtion in Sect. 2. In Sect. 3, we first discuss the reltionship between hypertrees nd junction trees nd the notion of Mrkov network. We then present our proposed method. We discuss the dvntges of the proposed method in Sect. 4. We conclude our pper in Sect Byesin Networks nd the Locl Propgtion We use U = {x 1,..., x n } to represent set of discrete vribles. Ech x i tkes vlues from finite domin denoted V xi. We use cpitl letters such s X to represent subset of U nd its domin is denoted by V X. By XY we men X Y. We write x i = α, where α V xi, to indicte tht the vrible x i is instntited to the vlue α. Similrly, we write X = β, where β V X, to indicte tht X is instntited to the vlue β. For convenience, we write p(x i ) to represent p(x i = α) for ll α V xi. Similrly, we write p(x) to represent p(x = β) for ll β V X. A Byesin network (BN) defined over set U = {x 1,..., x n } of vribles is tuple (D, C). The D is directed cyclic grph (DAG) nd the C = {p(x i p(x i )) x i U} is set of conditionl probbility distributions (CPDs), where p(x i ) denotes the prents of node x i in D, such tht p(u) = n i=1 p(x i p(x i )). This fctoriztion of p(u) is referred to s BN fctoriztion. Probbilistic resoning in BN mens computing p(x) or p(x E = e), where X E =, X U, nd E U. The fct tht E is instntited to e, i.e., E = e, is clled the evidence. The DAG of BN is normlly trnsformed through morliztion nd tringultion into junction on which the locl propgtion method is pplied [1]. After the locl propgtion finishes its execution, mrginl distribution is ssocited with ech node in the junction tree. p(x) cn be esily computed by identifying node in the junction tree which contins X nd then do mrginliztion; the probbility of p(x E = e) cn be similrly obtined by first incorporting the evidence E = e into the junction tree nd then propgting the evidence so tht the junction tree reches n updted consistent stte from which the probbility p(x E = e) cn be computed in the sme fshion s we compute p(x). It is worth emphsizing tht this method for computing p(x E = e) needs to pply the locl propgtion procedure every time when new evidence is observed. Tht is, it involves lot of computtion to keep the knowledge bse consistent. It is lso worth mentioning tht it is not evident how to compute p(x) nd p(x E = e) when X is not subset of ny node in the junction tree [6]. A more forml technicl tretment on the locl propgtion method cn be found in [1]. The problem of probbilistic resoning, i.e., computing p(x E = e), cn then be equivlently stted s computing p(x, E) for the set X E of vribles [6]. Henceforth, probbilistic resoning mens computing the mrginl distribution p(w) for ny subset W of U.

3 3 Probbilistic Resoning s Dtbse Queries In this section, we show tht the tsk of computing p(x) for ny rbitrry subset X cn be conveniently expressed nd solved s dtbse query. 3.1 Hypertrees, Junction Trees, nd Mrkov Networks A hypergrph is pir (N, H), where N is finite set of nodes (ttributes) nd H is set of edges (hyperedges) which re rbitrry subsets of N [4]. If the nodes re understood, we will use H to denote the hypergrph (N, H). We sy n element h i in hypergrph H is twig if there exists nother element h j in H, distinct from h i, such tht ( (H {h i })) h i = h i h j. We cll ny such h j brnch for the twig h i. A hypergrph H is hypertree [4] if its elements cn be ordered, sy h 1, h 2,..., h n, so tht h i is twig in {h 1, h 2,..., h i }, for i = 2,..., n 1. We cll ny such ordering hypertree (tree) construction ordering for H. It is noted for given hypertree, there my exist multiple tree construction orderings. Given tree construction ordering h 1, h 2,..., h n, we cn choose, for ech i from 2 to N, n integer j(i) such tht 1 j(i) i 1 nd h j(i) is brnch for h i in {h 1, h 2,..., h i }. We cll function j(i) tht stisfies this condition brnching for the hypertree H with h 1, h 2,..., h n being the tree construction ordering. For given tree construction ordering, there might exist multiple choices of brnching functions. Given tree construction ordering h 1, h 2,..., h n for hypertree H nd brnching function j(i) for this ordering, we cn construct the following multiset: L(H) = {h j(2) h 2, h j(3) h 3,..., h j(n) h n }. The multiset L(H) is the sme for ny tree construction ordering nd brnching function of H [4]. We cll L(H) the seprtor set of the hypertree H. Let (N, H) be hypergrph. Its reduction (N, H ) is obtined by removing from H ech hyperedge tht is proper subset of nother hyperedge. A hypergrph is reduced if it equls its reduction. Let M N be set of nodes of the hypergrph (N, H). The set of prtil edges generted by M is defined to be the reduction of the hypergrph {h M h H}. Let H be hypertree nd X be set of nodes of H. The set of prtil edges generted by X is lso hypertree [7]. A hypergrph H is hypertree if nd only if its reduction is hypertree [4]. Henceforth, we will tret ech hypergrph s if it is reduced unless otherwise noted. It hs been shown in [4] tht given hypertree, there exists set of junction trees ech of which corresponds to prticulr tree construction ordering nd brnching function for this ordering. On the other hnd, given junction tree, there lwys exists unique corresponding hypertree representtion whose hyperedges re the nodes in the junction tree. Exmple 1. Consider the hypertree H shown in Fig 1 (i), it hs three corresponding junction trees shown in Fig 1 (ii), (iii) nd (iv), respectively. On the other hnd, ech of the junction trees in Fig 1 (ii), (iii) nd (iv) corresponds to the hypertree in Fig 1 (i). The hypertree in Fig 1 (v) will be explined lter.

4 b b b b b c d c d c d c d d (i) (ii) (iii) (iv) (v) Fig. 1. (i) A hypertree H, nd its three possible junction tree representtions in (ii), (iii), nd (iv). The pruned hypertree with respect to b, d is in (v). We now introduce the notion of Mrkov network. A (decomposble) Mrkov network (MN) [3] is pir (H, P), where () H = {h i i = 1,...,n} is hypertree defined over vrible set U where U = h i H h i with h 1,..., h n s tree construction ordering nd j(i) s the brnching function; together with (b) set P = {p(h) h H} of mrginls of p(u). The conditionl independencies encoded in H men tht the jpd p(u) cn be expressed s Mrkov fctoriztion: p(u) = p(h 1 ) p(h 2 )... p(h n ) p(h 2 h j(2) )... p(h n h j(n) ). (1) Recll the locl propgtion method for BNs in Sect. 2. After finishing the locl propgtion without ny evidence, we hve obtined mrginls for ech node in the junction tree. Since junction tree corresponds to unique hypertree, the hypertree nd the set of mrginls (for ech hyperedge) obtined by locl propgtion together define Mrkov network [1]. 3.2 An Illustrtive Exmple For Computing p(x) As mentioned before, the probbilistic resoning cn be stted s the problem of computing p(x) where X is n rbitrry set of vribles. Consider Mrkov network obtined from BN by locl propgtion nd let H be its ssocited hypertree. It is trivil to compute p(x) if X h for some h H, s p(x) = h X p(h). However, it is not evident how to compute p(x) in the cse tht X h. Using the Mrkov network obtined by locl propgtion, we use n exmple to demonstrte how to compute p(x) for ny rbitrry subset X U by selectively pruning the hypertree H. Exmple 2. Consider the Mrkov network whose ssocited hypertree H is shown in Fig 1 (i) nd its Mrkov fctoriztion s follows: p(bcd) = p(b) p(c) p(d) p() p(). (2) Suppose we wnt to compute p(bd) where the nodes b nd d re not contined by ny hyperedge of H. We cn compute p(bd) by mrginlizing out ll the

5 irrelevnt vribles in the Mrkov fctoriztion of the jpd p(bcd) in eqution (2). Notice tht the numertor p(c) in eqution (2) is the only fctor tht involves vrible c. (Grphiclly speking, the node c occurs only in the hyperedge c). Therefore, we cn sum it out s shown below. p(bd) =, c = p(b) p(c) p(d) p() p() p(b) p(d) p() = p() p() = p(b) p(d) p() p() p(c) c p(b) p(d). (3) p() Note tht p(b) p(d) p() = p(bd) nd this is Mrkov fctoriztion. The bove summtion process grphiclly corresponds to deleting the node c from the hypertree H in Fig 1 (i), which results in the hypertree in Fig 1 (iv). Note tht fter the vrible c hs been summed out, there exists p() both s term in the numertor nd term in the denomintor. The existence of the denomintor term p() is due to the fct tht is in L(H). Obviously, this pir of p() cn be cnceled. Therefore, our originl objective of computing p(bd) cn now be chieved by working with this pruned Mrkov fctoriztion p(bd) = p(b) p(d) p() whose hypertree is shown in Fig 1 (iv). 3.3 Selectively Pruning the Hypertree of the Mrkov Network The method demonstrted in Exmple 2 cn ctully be generlized to compute p(x) for ny X U. In the following, we introduce method for selectively pruning the hypertree H ssocited with Mrkov network to the exct portion needed for computing p(x). This method ws originlly developed in the dtbse theory for nswering dtbse queries [7]. Consider Mrkov network with its ssocited hypertree H nd suppose we wnt to compute p(x). In order to reduce the hypertree H to the exct portion tht fcilittes the computtion of p(x), we first mrk those nodes in X nd repet the following two opertions to prune the hypertree H until neither is pplicble: (op1): delete n unmrked node tht occurs in only one hyperedge; (op2): delete hyperedge tht is contined in nother hyperedge. We use H to denote the resulting hypergrph. Note tht the bove procedure possesses the Church-Rosser property, tht is, the finl result H is unique, regrdless of the order in which (op1) nd (op2) re pplied [4]. It is lso noted tht the opertors (op1) nd (op2) cn be implemented in liner time [7]. It is perhps worth mentioning tht (op1) nd (op2) re grphicl opertors pplying to H. On the other hnd, the method in [8] works with BN fctoriztion nd it sums out irrelevnt vribles numericlly. Let H 0, H 1,..., H j,..., H m represent the sequence of hypergrphs (not necessrily reduced) in the pruning process, where H 0 = H, H m = H, 1 j m, ech H j is obtined by pplying either (op1) or (op2) to H j 1.

6 Lemm 1. Ech hypergrph H i, 1 i m, is hypertree. Lemm 2. L(H ) L(H). Due to lck of spce, the detiled proofs of the bove lemms nd the following theorem will be reported in seprte pper. For ech h i H, there exists h j H such tht h i h j. We cn compute p(h i ) s p(h i ) = h j h p(h j ). In other words, the mrginl p(h i ) cn be i computed from the originl mrginl p(h) supplied with the Mrkov network H. Therefore, fter selectively pruning H, we hve obtined the hypertree H nd mrginls p(h i ) for ech h i H. Theorem 1. Let (H, P) be Mrkov network. Let H be the resulting pruned hypertree with respect to set X of vribles. The hypertree H ={h 1, h 2,..., h k } nd the set P = {p(h i ) 1 i k} of mrginls define Mrkov network. Theorem 1 indictes tht the originl problem of computing p(x) cn now be nswered by the new Mrkov network defined by the pruned hypertree H. It hs been proposed [5] tht ech mrginl p(h) where h H cn be stored s reltion in the dtbse fshion. Moreover, computing p(x) from H cn be implemented by dtbse SQL sttements [5]. It is noted tht the result of pplying (op1) nd (op2) to H lwys yields Mrkov network which is different thn the method in [8]. 4 Advntges One slient feture of the proposed method is tht it does not require ny repeted ppliction of locl propgtion. Since the problem of computing p(x E = e) cn be equivlently reduced to the problem of computing p(x, E), we cn uniformly tret probbilistic resoning s merely computing mrginl distributions. Moreover, computing mrginl distribution, sy, p(w), from the jpd p(u) defined by BN, cn be ccomplished by working with the Mrkov fctoriztion of p(u), whose estblishment only needs pplying the locl propgtion method once on the junction tree constructed from the BN. It is worth mentioning tht Xu in [6] reched the sme conclusion nd proved theorem similr to Theorem 1 bsed on the locl propgtion technique on the junction tree. Computing p(w) in our proposed pproch needs to prune the hypertree H to the exct portion needed for computing p(w) s Exmple 2 demonstrtes if W h for ny h H. A similr method ws suggested in [6] by pruning the junction tree insted. Using hypertrees s the secondry structure insted of junction trees hs vluble dvntges s the following exmple shows. Exmple 3. Consider the hypertree H shown in Fig 1 (i), it hs three corresponding junction trees shown in Fig 1 (ii), (iii) nd (iv), respectively. The method in [6] first fixes junction tree, for exmple, sy the one in Fig 1 (ii). Suppose we need to compute p(bd), the method in [6] will prune the junction tree so tht ny irrelevnt nodes will be removed s we do for pruning hypertree. However, in this

7 junction tree, nothing cn be pruned out ccording to [6]. In other words, p(bd) hs to be obtined by the following clcultion: p(bd) = p(b) p() c p(c) p(d) p(). However, if we prune the hypertree in Fig 1 (i), the resulting pruned hypertree is shown in Fig 1 (v), from which p(bd) cn be obtined by eqution (3). Obviously, the computtion involved is much less. Observing this, one might decide to dopt the junction tree in Fig 1 (iii) s the secondry structure. This chnge fcilittes the computtion of p(bd). However, in similr fshion, one cn esily be convinced tht computing p(bc) using the junction tree in (iii), computing p(cd) using the junction tree in (iv) suffer exctly the sme problem s computing p(bd) using junction tree in (ii). In other words, regrdless of the junction tree fixed in dvnce, there lwys exists some queries tht re not fvored by the pre-determined junction tree structure. On the other hnd, the hypertree structure lwys provides the optiml pruning result for computing mrginl [7]. 5 Conclusion In this pper, we hve suggested new pproch for conducting probbilistic resoning from the reltionl dtbse perspective. We demonstrted how to selectively reduce the hypertree structure so tht we cn void repeted ppliction of locl propgtion. This suggests possible dul purposes dtbse mngement systems for both dtbse storge, retrievl nd probbilistic resoning. ACKNOWLEDGMENT. The uthors would like to thnk one of the reviewers for his/her helpful suggestions nd comments. References [1] C. Hung nd A. Drwiche. Inference in belief networks: A procedurl guide. Interntionl Journl of Approximte Resoning, 15(3): , October [2] S.L. Luritzen nd D.J. Spiegelhlter. Locl computtion with probbilities on grphicl structures nd their ppliction to expert systems. Journl of the Royl Sttisticl Society, 50: , [3] J. Perl. Probbilistic Resoning in Intelligent Systems: Networks of Plusible Inference. Morgn Kufmnn Publishers, Sn Frncisco, Cliforni, [4] G. Shfer. An xiomtic study of computtion in hypertrees. School of Business Working Ppers 232, University of Knss, [5] S.K.M. Wong, C.J. Butz, nd Y. Xing. A method for implementing probbilistic model s reltionl dtbse. In Eleventh Conference on Uncertinty in Artificil Intelligence, pges Morgn Kufmnn Publishers, [6] H. Xu. Computing mrginls for rbitrry subsets from mrginl representtion in mrkov trees. Artificil Intelligence, 74: , [7] Mihlis Ynnkkis. Algorithms for cyclic dtbse schemes. In Very Lrge Dt Bses, 7th Interntionl Conference, September 9-11, 1981, Cnnes, Frnce, Proceedings, pges 82 94, [8] N. Zhng nd Poole.D. Exploiting cusl independence in byesin network inference. Journl of Artificil Intelligence Reserch, 5: , 1996.

ARITHMETIC OPERATIONS. The real numbers have the following properties: a b c ab ac

ARITHMETIC OPERATIONS. The real numbers have the following properties: a b c ab ac REVIEW OF ALGEBRA Here we review the bsic rules nd procedures of lgebr tht you need to know in order to be successful in clculus. ARITHMETIC OPERATIONS The rel numbers hve the following properties: b b

More information

New Expansion and Infinite Series

New Expansion and Infinite Series Interntionl Mthemticl Forum, Vol. 9, 204, no. 22, 06-073 HIKARI Ltd, www.m-hikri.com http://dx.doi.org/0.2988/imf.204.4502 New Expnsion nd Infinite Series Diyun Zhng College of Computer Nnjing University

More information

7.2 The Definite Integral

7.2 The Definite Integral 7.2 The Definite Integrl the definite integrl In the previous section, it ws found tht if function f is continuous nd nonnegtive, then the re under the grph of f on [, b] is given by F (b) F (), where

More information

Duality # Second iteration for HW problem. Recall our LP example problem we have been working on, in equality form, is given below.

Duality # Second iteration for HW problem. Recall our LP example problem we have been working on, in equality form, is given below. Dulity #. Second itertion for HW problem Recll our LP emple problem we hve been working on, in equlity form, is given below.,,,, 8 m F which, when written in slightly different form, is 8 F Recll tht we

More information

Reversals of Signal-Posterior Monotonicity for Any Bounded Prior

Reversals of Signal-Posterior Monotonicity for Any Bounded Prior Reversls of Signl-Posterior Monotonicity for Any Bounded Prior Christopher P. Chmbers Pul J. Hely Abstrct Pul Milgrom (The Bell Journl of Economics, 12(2): 380 391) showed tht if the strict monotone likelihood

More information

CS 188 Introduction to Artificial Intelligence Fall 2018 Note 7

CS 188 Introduction to Artificial Intelligence Fall 2018 Note 7 CS 188 Introduction to Artificil Intelligence Fll 2018 Note 7 These lecture notes re hevily bsed on notes originlly written by Nikhil Shrm. Decision Networks In the third note, we lerned bout gme trees

More information

Chapter 14. Matrix Representations of Linear Transformations

Chapter 14. Matrix Representations of Linear Transformations Chpter 4 Mtrix Representtions of Liner Trnsformtions When considering the Het Stte Evolution, we found tht we could describe this process using multipliction by mtrix. This ws nice becuse computers cn

More information

Physics 116C Solution of inhomogeneous ordinary differential equations using Green s functions

Physics 116C Solution of inhomogeneous ordinary differential equations using Green s functions Physics 6C Solution of inhomogeneous ordinry differentil equtions using Green s functions Peter Young November 5, 29 Homogeneous Equtions We hve studied, especilly in long HW problem, second order liner

More information

Review of Calculus, cont d

Review of Calculus, cont d Jim Lmbers MAT 460 Fll Semester 2009-10 Lecture 3 Notes These notes correspond to Section 1.1 in the text. Review of Clculus, cont d Riemnn Sums nd the Definite Integrl There re mny cses in which some

More information

Properties of Integrals, Indefinite Integrals. Goals: Definition of the Definite Integral Integral Calculations using Antiderivatives

Properties of Integrals, Indefinite Integrals. Goals: Definition of the Definite Integral Integral Calculations using Antiderivatives Block #6: Properties of Integrls, Indefinite Integrls Gols: Definition of the Definite Integrl Integrl Clcultions using Antiderivtives Properties of Integrls The Indefinite Integrl 1 Riemnn Sums - 1 Riemnn

More information

20 MATHEMATICS POLYNOMIALS

20 MATHEMATICS POLYNOMIALS 0 MATHEMATICS POLYNOMIALS.1 Introduction In Clss IX, you hve studied polynomils in one vrible nd their degrees. Recll tht if p(x) is polynomil in x, the highest power of x in p(x) is clled the degree of

More information

Improper Integrals. Type I Improper Integrals How do we evaluate an integral such as

Improper Integrals. Type I Improper Integrals How do we evaluate an integral such as Improper Integrls Two different types of integrls cn qulify s improper. The first type of improper integrl (which we will refer to s Type I) involves evluting n integrl over n infinite region. In the grph

More information

NUMERICAL INTEGRATION. The inverse process to differentiation in calculus is integration. Mathematically, integration is represented by.

NUMERICAL INTEGRATION. The inverse process to differentiation in calculus is integration. Mathematically, integration is represented by. NUMERICAL INTEGRATION 1 Introduction The inverse process to differentition in clculus is integrtion. Mthemticlly, integrtion is represented by f(x) dx which stnds for the integrl of the function f(x) with

More information

Decomposition of terms in Lucas sequences

Decomposition of terms in Lucas sequences Journl of Logic & Anlysis 1:4 009 1 3 ISSN 1759-9008 1 Decomposition of terms in Lucs sequences ABDELMADJID BOUDAOUD Let P, Q be non-zero integers such tht D = P 4Q is different from zero. The sequences

More information

Summary: Method of Separation of Variables

Summary: Method of Separation of Variables Physics 246 Electricity nd Mgnetism I, Fll 26, Lecture 22 1 Summry: Method of Seprtion of Vribles 1. Seprtion of Vribles in Crtesin Coordintes 2. Fourier Series Suggested Reding: Griffiths: Chpter 3, Section

More information

f(x) dx, If one of these two conditions is not met, we call the integral improper. Our usual definition for the value for the definite integral

f(x) dx, If one of these two conditions is not met, we call the integral improper. Our usual definition for the value for the definite integral Improper Integrls Every time tht we hve evluted definite integrl such s f(x) dx, we hve mde two implicit ssumptions bout the integrl:. The intervl [, b] is finite, nd. f(x) is continuous on [, b]. If one

More information

W. We shall do so one by one, starting with I 1, and we shall do it greedily, trying

W. We shall do so one by one, starting with I 1, and we shall do it greedily, trying Vitli covers 1 Definition. A Vitli cover of set E R is set V of closed intervls with positive length so tht, for every δ > 0 nd every x E, there is some I V with λ(i ) < δ nd x I. 2 Lemm (Vitli covering)

More information

SUMMER KNOWHOW STUDY AND LEARNING CENTRE

SUMMER KNOWHOW STUDY AND LEARNING CENTRE SUMMER KNOWHOW STUDY AND LEARNING CENTRE Indices & Logrithms 2 Contents Indices.2 Frctionl Indices.4 Logrithms 6 Exponentil equtions. Simplifying Surds 13 Opertions on Surds..16 Scientific Nottion..18

More information

Recitation 3: More Applications of the Derivative

Recitation 3: More Applications of the Derivative Mth 1c TA: Pdric Brtlett Recittion 3: More Applictions of the Derivtive Week 3 Cltech 2012 1 Rndom Question Question 1 A grph consists of the following: A set V of vertices. A set E of edges where ech

More information

UNIFORM CONVERGENCE. Contents 1. Uniform Convergence 1 2. Properties of uniform convergence 3

UNIFORM CONVERGENCE. Contents 1. Uniform Convergence 1 2. Properties of uniform convergence 3 UNIFORM CONVERGENCE Contents 1. Uniform Convergence 1 2. Properties of uniform convergence 3 Suppose f n : Ω R or f n : Ω C is sequence of rel or complex functions, nd f n f s n in some sense. Furthermore,

More information

Section 6.1 INTRO to LAPLACE TRANSFORMS

Section 6.1 INTRO to LAPLACE TRANSFORMS Section 6. INTRO to LAPLACE TRANSFORMS Key terms: Improper Integrl; diverge, converge A A f(t)dt lim f(t)dt Piecewise Continuous Function; jump discontinuity Function of Exponentil Order Lplce Trnsform

More information

The Regulated and Riemann Integrals

The Regulated and Riemann Integrals Chpter 1 The Regulted nd Riemnn Integrls 1.1 Introduction We will consider severl different pproches to defining the definite integrl f(x) dx of function f(x). These definitions will ll ssign the sme vlue

More information

Math 1B, lecture 4: Error bounds for numerical methods

Math 1B, lecture 4: Error bounds for numerical methods Mth B, lecture 4: Error bounds for numericl methods Nthn Pflueger 4 September 0 Introduction The five numericl methods descried in the previous lecture ll operte by the sme principle: they pproximte the

More information

MORE FUNCTION GRAPHING; OPTIMIZATION. (Last edited October 28, 2013 at 11:09pm.)

MORE FUNCTION GRAPHING; OPTIMIZATION. (Last edited October 28, 2013 at 11:09pm.) MORE FUNCTION GRAPHING; OPTIMIZATION FRI, OCT 25, 203 (Lst edited October 28, 203 t :09pm.) Exercise. Let n be n rbitrry positive integer. Give n exmple of function with exctly n verticl symptotes. Give

More information

Advanced Calculus: MATH 410 Notes on Integrals and Integrability Professor David Levermore 17 October 2004

Advanced Calculus: MATH 410 Notes on Integrals and Integrability Professor David Levermore 17 October 2004 Advnced Clculus: MATH 410 Notes on Integrls nd Integrbility Professor Dvid Levermore 17 October 2004 1. Definite Integrls In this section we revisit the definite integrl tht you were introduced to when

More information

State space systems analysis (continued) Stability. A. Definitions A system is said to be Asymptotically Stable (AS) when it satisfies

State space systems analysis (continued) Stability. A. Definitions A system is said to be Asymptotically Stable (AS) when it satisfies Stte spce systems nlysis (continued) Stbility A. Definitions A system is sid to be Asymptoticlly Stble (AS) when it stisfies ut () = 0, t > 0 lim xt () 0. t A system is AS if nd only if the impulse response

More information

p-adic Egyptian Fractions

p-adic Egyptian Fractions p-adic Egyptin Frctions Contents 1 Introduction 1 2 Trditionl Egyptin Frctions nd Greedy Algorithm 2 3 Set-up 3 4 p-greedy Algorithm 5 5 p-egyptin Trditionl 10 6 Conclusion 1 Introduction An Egyptin frction

More information

Self-similarity and symmetries of Pascal s triangles and simplices mod p

Self-similarity and symmetries of Pascal s triangles and simplices mod p Sn Jose Stte University SJSU ScholrWorks Fculty Publictions Mthemtics nd Sttistics Februry 2004 Self-similrity nd symmetries of Pscl s tringles nd simplices mod p Richrd P. Kubelk Sn Jose Stte University,

More information

Exam 2, Mathematics 4701, Section ETY6 6:05 pm 7:40 pm, March 31, 2016, IH-1105 Instructor: Attila Máté 1

Exam 2, Mathematics 4701, Section ETY6 6:05 pm 7:40 pm, March 31, 2016, IH-1105 Instructor: Attila Máté 1 Exm, Mthemtics 471, Section ETY6 6:5 pm 7:4 pm, Mrch 1, 16, IH-115 Instructor: Attil Máté 1 17 copies 1. ) Stte the usul sufficient condition for the fixed-point itertion to converge when solving the eqution

More information

Math& 152 Section Integration by Parts

Math& 152 Section Integration by Parts Mth& 5 Section 7. - Integrtion by Prts Integrtion by prts is rule tht trnsforms the integrl of the product of two functions into other (idelly simpler) integrls. Recll from Clculus I tht given two differentible

More information

Lecture Note 9: Orthogonal Reduction

Lecture Note 9: Orthogonal Reduction MATH : Computtionl Methods of Liner Algebr 1 The Row Echelon Form Lecture Note 9: Orthogonl Reduction Our trget is to solve the norml eution: Xinyi Zeng Deprtment of Mthemticl Sciences, UTEP A t Ax = A

More information

THE EXISTENCE-UNIQUENESS THEOREM FOR FIRST-ORDER DIFFERENTIAL EQUATIONS.

THE EXISTENCE-UNIQUENESS THEOREM FOR FIRST-ORDER DIFFERENTIAL EQUATIONS. THE EXISTENCE-UNIQUENESS THEOREM FOR FIRST-ORDER DIFFERENTIAL EQUATIONS RADON ROSBOROUGH https://intuitiveexplntionscom/picrd-lindelof-theorem/ This document is proof of the existence-uniqueness theorem

More information

Convert the NFA into DFA

Convert the NFA into DFA Convert the NF into F For ech NF we cn find F ccepting the sme lnguge. The numer of sttes of the F could e exponentil in the numer of sttes of the NF, ut in prctice this worst cse occurs rrely. lgorithm:

More information

Frobenius numbers of generalized Fibonacci semigroups

Frobenius numbers of generalized Fibonacci semigroups Frobenius numbers of generlized Fiboncci semigroups Gretchen L. Mtthews 1 Deprtment of Mthemticl Sciences, Clemson University, Clemson, SC 29634-0975, USA gmtthe@clemson.edu Received:, Accepted:, Published:

More information

A REVIEW OF CALCULUS CONCEPTS FOR JDEP 384H. Thomas Shores Department of Mathematics University of Nebraska Spring 2007

A REVIEW OF CALCULUS CONCEPTS FOR JDEP 384H. Thomas Shores Department of Mathematics University of Nebraska Spring 2007 A REVIEW OF CALCULUS CONCEPTS FOR JDEP 384H Thoms Shores Deprtment of Mthemtics University of Nebrsk Spring 2007 Contents Rtes of Chnge nd Derivtives 1 Dierentils 4 Are nd Integrls 5 Multivrite Clculus

More information

HW3, Math 307. CSUF. Spring 2007.

HW3, Math 307. CSUF. Spring 2007. HW, Mth 7. CSUF. Spring 7. Nsser M. Abbsi Spring 7 Compiled on November 5, 8 t 8:8m public Contents Section.6, problem Section.6, problem Section.6, problem 5 Section.6, problem 7 6 5 Section.6, problem

More information

Abstract inner product spaces

Abstract inner product spaces WEEK 4 Abstrct inner product spces Definition An inner product spce is vector spce V over the rel field R equipped with rule for multiplying vectors, such tht the product of two vectors is sclr, nd the

More information

Chapter 4 Contravariance, Covariance, and Spacetime Diagrams

Chapter 4 Contravariance, Covariance, and Spacetime Diagrams Chpter 4 Contrvrince, Covrince, nd Spcetime Digrms 4. The Components of Vector in Skewed Coordintes We hve seen in Chpter 3; figure 3.9, tht in order to show inertil motion tht is consistent with the Lorentz

More information

A BRIEF INTRODUCTION TO UNIFORM CONVERGENCE. In the study of Fourier series, several questions arise naturally, such as: c n e int

A BRIEF INTRODUCTION TO UNIFORM CONVERGENCE. In the study of Fourier series, several questions arise naturally, such as: c n e int A BRIEF INTRODUCTION TO UNIFORM CONVERGENCE HANS RINGSTRÖM. Questions nd exmples In the study of Fourier series, severl questions rise nturlly, such s: () (2) re there conditions on c n, n Z, which ensure

More information

AQA Further Pure 1. Complex Numbers. Section 1: Introduction to Complex Numbers. The number system

AQA Further Pure 1. Complex Numbers. Section 1: Introduction to Complex Numbers. The number system Complex Numbers Section 1: Introduction to Complex Numbers Notes nd Exmples These notes contin subsections on The number system Adding nd subtrcting complex numbers Multiplying complex numbers Complex

More information

1.9 C 2 inner variations

1.9 C 2 inner variations 46 CHAPTER 1. INDIRECT METHODS 1.9 C 2 inner vritions So fr, we hve restricted ttention to liner vritions. These re vritions of the form vx; ǫ = ux + ǫφx where φ is in some liner perturbtion clss P, for

More information

Riemann Sums and Riemann Integrals

Riemann Sums and Riemann Integrals Riemnn Sums nd Riemnn Integrls Jmes K. Peterson Deprtment of Biologicl Sciences nd Deprtment of Mthemticl Sciences Clemson University August 26, 2013 Outline 1 Riemnn Sums 2 Riemnn Integrls 3 Properties

More information

Riemann Sums and Riemann Integrals

Riemann Sums and Riemann Integrals Riemnn Sums nd Riemnn Integrls Jmes K. Peterson Deprtment of Biologicl Sciences nd Deprtment of Mthemticl Sciences Clemson University August 26, 203 Outline Riemnn Sums Riemnn Integrls Properties Abstrct

More information

A recursive construction of efficiently decodable list-disjunct matrices

A recursive construction of efficiently decodable list-disjunct matrices CSE 709: Compressed Sensing nd Group Testing. Prt I Lecturers: Hung Q. Ngo nd Atri Rudr SUNY t Bufflo, Fll 2011 Lst updte: October 13, 2011 A recursive construction of efficiently decodble list-disjunct

More information

1 Online Learning and Regret Minimization

1 Online Learning and Regret Minimization 2.997 Decision-Mking in Lrge-Scle Systems My 10 MIT, Spring 2004 Hndout #29 Lecture Note 24 1 Online Lerning nd Regret Minimiztion In this lecture, we consider the problem of sequentil decision mking in

More information

The First Fundamental Theorem of Calculus. If f(x) is continuous on [a, b] and F (x) is any antiderivative. f(x) dx = F (b) F (a).

The First Fundamental Theorem of Calculus. If f(x) is continuous on [a, b] and F (x) is any antiderivative. f(x) dx = F (b) F (a). The Fundmentl Theorems of Clculus Mth 4, Section 0, Spring 009 We now know enough bout definite integrls to give precise formultions of the Fundmentl Theorems of Clculus. We will lso look t some bsic emples

More information

The steps of the hypothesis test

The steps of the hypothesis test ttisticl Methods I (EXT 7005) Pge 78 Mosquito species Time of dy A B C Mid morning 0.0088 5.4900 5.5000 Mid Afternoon.3400 0.0300 0.8700 Dusk 0.600 5.400 3.000 The Chi squre test sttistic is the sum of

More information

Intuitionistic Fuzzy Lattices and Intuitionistic Fuzzy Boolean Algebras

Intuitionistic Fuzzy Lattices and Intuitionistic Fuzzy Boolean Algebras Intuitionistic Fuzzy Lttices nd Intuitionistic Fuzzy oolen Algebrs.K. Tripthy #1, M.K. Stpthy *2 nd P.K.Choudhury ##3 # School of Computing Science nd Engineering VIT University Vellore-632014, TN, Indi

More information

Introduction to Group Theory

Introduction to Group Theory Introduction to Group Theory Let G be n rbitrry set of elements, typiclly denoted s, b, c,, tht is, let G = {, b, c, }. A binry opertion in G is rule tht ssocites with ech ordered pir (,b) of elements

More information

Zero-Sum Magic Graphs and Their Null Sets

Zero-Sum Magic Graphs and Their Null Sets Zero-Sum Mgic Grphs nd Their Null Sets Ebrhim Slehi Deprtment of Mthemticl Sciences University of Nevd Ls Vegs Ls Vegs, NV 89154-4020. ebrhim.slehi@unlv.edu Abstrct For ny h N, grph G = (V, E) is sid to

More information

Markscheme May 2016 Mathematics Standard level Paper 1

Markscheme May 2016 Mathematics Standard level Paper 1 M6/5/MATME/SP/ENG/TZ/XX/M Mrkscheme My 06 Mthemtics Stndrd level Pper 7 pges M6/5/MATME/SP/ENG/TZ/XX/M This mrkscheme is the property of the Interntionl Bcclurete nd must not be reproduced or distributed

More information

The Algebra (al-jabr) of Matrices

The Algebra (al-jabr) of Matrices Section : Mtri lgebr nd Clculus Wshkewicz College of Engineering he lgebr (l-jbr) of Mtrices lgebr s brnch of mthemtics is much broder thn elementry lgebr ll of us studied in our high school dys. In sense

More information

Acceptance Sampling by Attributes

Acceptance Sampling by Attributes Introduction Acceptnce Smpling by Attributes Acceptnce smpling is concerned with inspection nd decision mking regrding products. Three spects of smpling re importnt: o Involves rndom smpling of n entire

More information

4 7x =250; 5 3x =500; Read section 3.3, 3.4 Announcements: Bell Ringer: Use your calculator to solve

4 7x =250; 5 3x =500; Read section 3.3, 3.4 Announcements: Bell Ringer: Use your calculator to solve Dte: 3/14/13 Objective: SWBAT pply properties of exponentil functions nd will pply properties of rithms. Bell Ringer: Use your clcultor to solve 4 7x =250; 5 3x =500; HW Requests: Properties of Log Equtions

More information

UNIT 1 FUNCTIONS AND THEIR INVERSES Lesson 1.4: Logarithmic Functions as Inverses Instruction

UNIT 1 FUNCTIONS AND THEIR INVERSES Lesson 1.4: Logarithmic Functions as Inverses Instruction Lesson : Logrithmic Functions s Inverses Prerequisite Skills This lesson requires the use of the following skills: determining the dependent nd independent vribles in n exponentil function bsed on dt from

More information

Math 426: Probability Final Exam Practice

Math 426: Probability Final Exam Practice Mth 46: Probbility Finl Exm Prctice. Computtionl problems 4. Let T k (n) denote the number of prtitions of the set {,..., n} into k nonempty subsets, where k n. Argue tht T k (n) kt k (n ) + T k (n ) by

More information

Math Lecture 23

Math Lecture 23 Mth 8 - Lecture 3 Dyln Zwick Fll 3 In our lst lecture we delt with solutions to the system: x = Ax where A is n n n mtrix with n distinct eigenvlues. As promised, tody we will del with the question of

More information

Research Article Moment Inequalities and Complete Moment Convergence

Research Article Moment Inequalities and Complete Moment Convergence Hindwi Publishing Corportion Journl of Inequlities nd Applictions Volume 2009, Article ID 271265, 14 pges doi:10.1155/2009/271265 Reserch Article Moment Inequlities nd Complete Moment Convergence Soo Hk

More information

Bernoulli Numbers Jeff Morton

Bernoulli Numbers Jeff Morton Bernoulli Numbers Jeff Morton. We re interested in the opertor e t k d k t k, which is to sy k tk. Applying this to some function f E to get e t f d k k tk d k f f + d k k tk dk f, we note tht since f

More information

KNOWLEDGE-BASED AGENTS INFERENCE

KNOWLEDGE-BASED AGENTS INFERENCE AGENTS THAT REASON LOGICALLY KNOWLEDGE-BASED AGENTS Two components: knowledge bse, nd n inference engine. Declrtive pproch to building n gent. We tell it wht it needs to know, nd It cn sk itself wht to

More information

IN GAUSSIAN INTEGERS X 3 + Y 3 = Z 3 HAS ONLY TRIVIAL SOLUTIONS A NEW APPROACH

IN GAUSSIAN INTEGERS X 3 + Y 3 = Z 3 HAS ONLY TRIVIAL SOLUTIONS A NEW APPROACH INTEGERS: ELECTRONIC JOURNAL OF COMBINATORIAL NUMBER THEORY 8 (2008), #A2 IN GAUSSIAN INTEGERS X + Y = Z HAS ONLY TRIVIAL SOLUTIONS A NEW APPROACH Elis Lmpkis Lmpropoulou (Term), Kiprissi, T.K: 24500,

More information

Improper Integrals, and Differential Equations

Improper Integrals, and Differential Equations Improper Integrls, nd Differentil Equtions October 22, 204 5.3 Improper Integrls Previously, we discussed how integrls correspond to res. More specificlly, we sid tht for function f(x), the region creted

More information

Variational Techniques for Sturm-Liouville Eigenvalue Problems

Variational Techniques for Sturm-Liouville Eigenvalue Problems Vritionl Techniques for Sturm-Liouville Eigenvlue Problems Vlerie Cormni Deprtment of Mthemtics nd Sttistics University of Nebrsk, Lincoln Lincoln, NE 68588 Emil: vcormni@mth.unl.edu Rolf Ryhm Deprtment

More information

a a a a a a a a a a a a a a a a a a a a a a a a In this section, we introduce a general formula for computing determinants.

a a a a a a a a a a a a a a a a a a a a a a a a In this section, we introduce a general formula for computing determinants. Section 9 The Lplce Expnsion In the lst section, we defined the determinnt of (3 3) mtrix A 12 to be 22 12 21 22 2231 22 12 21. In this section, we introduce generl formul for computing determinnts. Rewriting

More information

MAA 4212 Improper Integrals

MAA 4212 Improper Integrals Notes by Dvid Groisser, Copyright c 1995; revised 2002, 2009, 2014 MAA 4212 Improper Integrls The Riemnn integrl, while perfectly well-defined, is too restrictive for mny purposes; there re functions which

More information

Read section 3.3, 3.4 Announcements:

Read section 3.3, 3.4 Announcements: Dte: 3/1/13 Objective: SWBAT pply properties of exponentil functions nd will pply properties of rithms. Bell Ringer: 1. f x = 3x 6, find the inverse, f 1 x., Using your grphing clcultor, Grph 1. f x,f

More information

Overview of Calculus I

Overview of Calculus I Overview of Clculus I Prof. Jim Swift Northern Arizon University There re three key concepts in clculus: The limit, the derivtive, nd the integrl. You need to understnd the definitions of these three things,

More information

Convergence of Fourier Series and Fejer s Theorem. Lee Ricketson

Convergence of Fourier Series and Fejer s Theorem. Lee Ricketson Convergence of Fourier Series nd Fejer s Theorem Lee Ricketson My, 006 Abstrct This pper will ddress the Fourier Series of functions with rbitrry period. We will derive forms of the Dirichlet nd Fejer

More information

Lecture 3 ( ) (translated and slightly adapted from lecture notes by Martin Klazar)

Lecture 3 ( ) (translated and slightly adapted from lecture notes by Martin Klazar) Lecture 3 (5.3.2018) (trnslted nd slightly dpted from lecture notes by Mrtin Klzr) Riemnn integrl Now we define precisely the concept of the re, in prticulr, the re of figure U(, b, f) under the grph of

More information

Before we can begin Ch. 3 on Radicals, we need to be familiar with perfect squares, cubes, etc. Try and do as many as you can without a calculator!!!

Before we can begin Ch. 3 on Radicals, we need to be familiar with perfect squares, cubes, etc. Try and do as many as you can without a calculator!!! Nme: Algebr II Honors Pre-Chpter Homework Before we cn begin Ch on Rdicls, we need to be fmilir with perfect squres, cubes, etc Try nd do s mny s you cn without clcultor!!! n The nth root of n n Be ble

More information

Lecture 1. Functional series. Pointwise and uniform convergence.

Lecture 1. Functional series. Pointwise and uniform convergence. 1 Introduction. Lecture 1. Functionl series. Pointwise nd uniform convergence. In this course we study mongst other things Fourier series. The Fourier series for periodic function f(x) with period 2π is

More information

How do we solve these things, especially when they get complicated? How do we know when a system has a solution, and when is it unique?

How do we solve these things, especially when they get complicated? How do we know when a system has a solution, and when is it unique? XII. LINEAR ALGEBRA: SOLVING SYSTEMS OF EQUATIONS Tody we re going to tlk bout solving systems of liner equtions. These re problems tht give couple of equtions with couple of unknowns, like: 6 2 3 7 4

More information

Here we study square linear systems and properties of their coefficient matrices as they relate to the solution set of the linear system.

Here we study square linear systems and properties of their coefficient matrices as they relate to the solution set of the linear system. Section 24 Nonsingulr Liner Systems Here we study squre liner systems nd properties of their coefficient mtrices s they relte to the solution set of the liner system Let A be n n Then we know from previous

More information

Entropy and Ergodic Theory Notes 10: Large Deviations I

Entropy and Ergodic Theory Notes 10: Large Deviations I Entropy nd Ergodic Theory Notes 10: Lrge Devitions I 1 A chnge of convention This is our first lecture on pplictions of entropy in probbility theory. In probbility theory, the convention is tht ll logrithms

More information

Reinforcement learning II

Reinforcement learning II CS 1675 Introduction to Mchine Lerning Lecture 26 Reinforcement lerning II Milos Huskrecht milos@cs.pitt.edu 5329 Sennott Squre Reinforcement lerning Bsics: Input x Lerner Output Reinforcement r Critic

More information

Theoretical foundations of Gaussian quadrature

Theoretical foundations of Gaussian quadrature Theoreticl foundtions of Gussin qudrture 1 Inner product vector spce Definition 1. A vector spce (or liner spce) is set V = {u, v, w,...} in which the following two opertions re defined: (A) Addition of

More information

Chapter 3. Vector Spaces

Chapter 3. Vector Spaces 3.4 Liner Trnsformtions 1 Chpter 3. Vector Spces 3.4 Liner Trnsformtions Note. We hve lredy studied liner trnsformtions from R n into R m. Now we look t liner trnsformtions from one generl vector spce

More information

Exponentials - Grade 10 [CAPS] *

Exponentials - Grade 10 [CAPS] * OpenStx-CNX module: m859 Exponentils - Grde 0 [CAPS] * Free High School Science Texts Project Bsed on Exponentils by Rory Adms Free High School Science Texts Project Mrk Horner Hether Willims This work

More information

1 The Lagrange interpolation formula

1 The Lagrange interpolation formula Notes on Qudrture 1 The Lgrnge interpoltion formul We briefly recll the Lgrnge interpoltion formul. The strting point is collection of N + 1 rel points (x 0, y 0 ), (x 1, y 1 ),..., (x N, y N ), with x

More information

AQA Further Pure 2. Hyperbolic Functions. Section 2: The inverse hyperbolic functions

AQA Further Pure 2. Hyperbolic Functions. Section 2: The inverse hyperbolic functions Hperbolic Functions Section : The inverse hperbolic functions Notes nd Emples These notes contin subsections on The inverse hperbolic functions Integrtion using the inverse hperbolic functions Logrithmic

More information

Equations and Inequalities

Equations and Inequalities Equtions nd Inequlities Equtions nd Inequlities Curriculum Redy ACMNA: 4, 5, 6, 7, 40 www.mthletics.com Equtions EQUATIONS & Inequlities & INEQUALITIES Sometimes just writing vribles or pronumerls in

More information

SOLUTIONS FOR ADMISSIONS TEST IN MATHEMATICS, COMPUTER SCIENCE AND JOINT SCHOOLS WEDNESDAY 5 NOVEMBER 2014

SOLUTIONS FOR ADMISSIONS TEST IN MATHEMATICS, COMPUTER SCIENCE AND JOINT SCHOOLS WEDNESDAY 5 NOVEMBER 2014 SOLUTIONS FOR ADMISSIONS TEST IN MATHEMATICS, COMPUTER SCIENCE AND JOINT SCHOOLS WEDNESDAY 5 NOVEMBER 014 Mrk Scheme: Ech prt of Question 1 is worth four mrks which re wrded solely for the correct nswer.

More information

How to simulate Turing machines by invertible one-dimensional cellular automata

How to simulate Turing machines by invertible one-dimensional cellular automata How to simulte Turing mchines by invertible one-dimensionl cellulr utomt Jen-Christophe Dubcq Déprtement de Mthémtiques et d Informtique, École Normle Supérieure de Lyon, 46, llée d Itlie, 69364 Lyon Cedex

More information

A New Grey-rough Set Model Based on Interval-Valued Grey Sets

A New Grey-rough Set Model Based on Interval-Valued Grey Sets Proceedings of the 009 IEEE Interntionl Conference on Systems Mn nd Cybernetics Sn ntonio TX US - October 009 New Grey-rough Set Model sed on Intervl-Vlued Grey Sets Wu Shunxing Deprtment of utomtion Ximen

More information

Generalized Fano and non-fano networks

Generalized Fano and non-fano networks Generlized Fno nd non-fno networks Nildri Ds nd Brijesh Kumr Ri Deprtment of Electronics nd Electricl Engineering Indin Institute of Technology Guwhti, Guwhti, Assm, Indi Emil: {d.nildri, bkri}@iitg.ernet.in

More information

Riemann Integrals and the Fundamental Theorem of Calculus

Riemann Integrals and the Fundamental Theorem of Calculus Riemnn Integrls nd the Fundmentl Theorem of Clculus Jmes K. Peterson Deprtment of Biologicl Sciences nd Deprtment of Mthemticl Sciences Clemson University September 16, 2013 Outline Grphing Riemnn Sums

More information

Math 520 Final Exam Topic Outline Sections 1 3 (Xiao/Dumas/Liaw) Spring 2008

Math 520 Final Exam Topic Outline Sections 1 3 (Xiao/Dumas/Liaw) Spring 2008 Mth 520 Finl Exm Topic Outline Sections 1 3 (Xio/Dums/Liw) Spring 2008 The finl exm will be held on Tuesdy, My 13, 2-5pm in 117 McMilln Wht will be covered The finl exm will cover the mteril from ll of

More information

Riemann is the Mann! (But Lebesgue may besgue to differ.)

Riemann is the Mann! (But Lebesgue may besgue to differ.) Riemnn is the Mnn! (But Lebesgue my besgue to differ.) Leo Livshits My 2, 2008 1 For finite intervls in R We hve seen in clss tht every continuous function f : [, b] R hs the property tht for every ɛ >

More information

Coalgebra, Lecture 15: Equations for Deterministic Automata

Coalgebra, Lecture 15: Equations for Deterministic Automata Colger, Lecture 15: Equtions for Deterministic Automt Julin Slmnc (nd Jurrin Rot) Decemer 19, 2016 In this lecture, we will study the concept of equtions for deterministic utomt. The notes re self contined

More information

Solution to Fredholm Fuzzy Integral Equations with Degenerate Kernel

Solution to Fredholm Fuzzy Integral Equations with Degenerate Kernel Int. J. Contemp. Mth. Sciences, Vol. 6, 2011, no. 11, 535-543 Solution to Fredholm Fuzzy Integrl Equtions with Degenerte Kernel M. M. Shmivnd, A. Shhsvrn nd S. M. Tri Fculty of Science, Islmic Azd University

More information

13: Diffusion in 2 Energy Groups

13: Diffusion in 2 Energy Groups 3: Diffusion in Energy Groups B. Rouben McMster University Course EP 4D3/6D3 Nucler Rector Anlysis (Rector Physics) 5 Sept.-Dec. 5 September Contents We study the diffusion eqution in two energy groups

More information

Continuous Random Variables

Continuous Random Variables STAT/MATH 395 A - PROBABILITY II UW Winter Qurter 217 Néhémy Lim Continuous Rndom Vribles Nottion. The indictor function of set S is rel-vlued function defined by : { 1 if x S 1 S (x) if x S Suppose tht

More information

RELATIONAL MODEL.

RELATIONAL MODEL. RELATIONAL MODEL Structure of Reltionl Dtbses Reltionl Algebr Tuple Reltionl Clculus Domin Reltionl Clculus Extended Reltionl-Algebr- Opertions Modifiction of the Dtbse Views EXAMPLE OF A RELATION BASIC

More information

Section 14.3 Arc Length and Curvature

Section 14.3 Arc Length and Curvature Section 4.3 Arc Length nd Curvture Clculus on Curves in Spce In this section, we ly the foundtions for describing the movement of n object in spce.. Vector Function Bsics In Clc, formul for rc length in

More information

Chapter 5 : Continuous Random Variables

Chapter 5 : Continuous Random Variables STAT/MATH 395 A - PROBABILITY II UW Winter Qurter 216 Néhémy Lim Chpter 5 : Continuous Rndom Vribles Nottions. N {, 1, 2,...}, set of nturl numbers (i.e. ll nonnegtive integers); N {1, 2,...}, set of ll

More information

Integral points on the rational curve

Integral points on the rational curve Integrl points on the rtionl curve y x bx c x ;, b, c integers. Konstntine Zeltor Mthemtics University of Wisconsin - Mrinette 750 W. Byshore Street Mrinette, WI 5443-453 Also: Konstntine Zeltor P.O. Box

More information

Section 6.1 INTRO to LAPLACE TRANSFORMS

Section 6.1 INTRO to LAPLACE TRANSFORMS Section 6. INTRO to LAPLACE TRANSFORMS Key terms: Improper Integrl; diverge, converge A A f(t)dt lim f(t)dt Piecewise Continuous Function; jump discontinuity Function of Exponentil Order Lplce Trnsform

More information

SCHOOL OF ENGINEERING & BUILT ENVIRONMENT. Mathematics

SCHOOL OF ENGINEERING & BUILT ENVIRONMENT. Mathematics SCHOOL OF ENGINEERING & BUIL ENVIRONMEN Mthemtics An Introduction to Mtrices Definition of Mtri Size of Mtri Rows nd Columns of Mtri Mtri Addition Sclr Multipliction of Mtri Mtri Multipliction 7 rnspose

More information

Path product and inverse M-matrices

Path product and inverse M-matrices Electronic Journl of Liner Algebr Volume 22 Volume 22 (2011) Article 42 2011 Pth product nd inverse M-mtrices Yn Zhu Cheng-Yi Zhng Jun Liu Follow this nd dditionl works t: http://repository.uwyo.edu/el

More information

Jim Lambers MAT 169 Fall Semester Lecture 4 Notes

Jim Lambers MAT 169 Fall Semester Lecture 4 Notes Jim Lmbers MAT 169 Fll Semester 2009-10 Lecture 4 Notes These notes correspond to Section 8.2 in the text. Series Wht is Series? An infinte series, usully referred to simply s series, is n sum of ll of

More information