|
|
- Debra Turner
- 5 years ago
- Views:
Transcription
1 Tis article was originally publised in a journal publised by Elsevier, and te attaced copy is provided by Elsevier for te autor s benefit and for te benefit of te autor s institution, for non-commercial researc and educational use including witout limitation use in instruction at your institution, sending it to specific colleagues tat you know, and providing a copy to your institution s administrator. ll oter uses, reproduction and distribution, including witout limitation commercial reprints, selling or licensing copies or access, or posting on open internet sites, your personal or institution s website or repository, are proibited. For exceptions, permission may be sougt for suc use troug Elsevier s permissions site at: ttp://
2 pplied Matematics and Computation 90 (2007) bstract Generalized LM-inverse of a matrix augmented by a column vector Firdaus E. Udwadia a, *, Pailaung Poomsiri b a erospace and Mecanical Engineering, Civil Engineering, Systems rcitecture Engineering, and Information and Operation Management, 430 K Olin Hall of Engineering, University of Soutern California, Los ngeles, C , US b Postdoctoral Researc ssociate, erospace and Mecanical Engineering, University of Soutern California, Los ngeles, C , US Tis paper presents a direct proof of te recursive formulae for te generalized LM- inverse of a matrix augmented by a column vector. Te recursive relations are proved by direct verification of te four conditions of te generalized LM-inverse. Several auxiliary results pertaining to generalized inverses are also provided. Ó 2006 Elsevier Inc. ll rigts reserved. Keywords: Generalized inverse; Moore Penrose M-Inverse; Moore Penrose LM-Inverse; Recursive formulae; Least squares problem. Introduction Let us begin by considering a set of linear equations Bx b; were B is an m by n matrix, b is an m-vector, and x is an n-vector. Te generalized LM-inverse of te matrix B is te matrix suc tat te solution x B þ LM b minimizes bot G L =2 ðbx bþ 2 kbx bk 2 L ð3þ and H M =2 x 2 kk x 2 M ; were L is an m by m symmetric positive definite matrix and M is an n by n symmetric positive definite matrix. ðþ ð2þ ð4þ * Corresponding autor. address: fudwadia@usc.edu (F.E. Udwadia) /$ - see front matter Ó 2006 Elsevier Inc. ll rigts reserved. doi:0.06/j.amc
3 000 F.E. Udwadia, P. Poomsiri / pplied Matematics and Computation 90 (2007) Below are te four conditions for te generalized LM-inverse []. ðiþ BB þ LM B B; ðiiþ B þ LM BBþ LM Bþ LM ; ðiiiþ LBB þ LM is symmetric; ð7þ ðivþ MB þ LMB is symmetric: ð8þ We note tat te generalized LM-inverse is te more general kind of te Moore Penrose inverse. Te concept of Moore Penrose (MP) inverses was first introduced by Moore [2] in 920 and later independently by Penrose [3] in 955. In 960, Greville [4] gave te first formulae for recursively determining te Moore Penrose inverse of a matrix. His algoritm provides an update of te MP inverse of a matrix wenever new information becomes available. s a result, te recursive formulae ave found extensive use in many areas of applications. mong tem are statistical inference [5], filtering teory, estimation teory [6], system identification [7], optimization and control, and most recently analytical dynamics [8,9]. In 997 Udwadia and Kalaba [0] provided an alternative and simple constructive proof of Greville s formulae, and later [,2] developed recursive relations for different types of generalized inverses of a matrix including te least-squares generalized inverse, te minimum-norm generalized inverse, and te Moore Penrose (MP) inverse of a matrix. Recently, te recursive formulae for te generalized M-inverse [3,4] and for te generalized LM-inverse were obtained. Tose for te generalized LM-inverse were proved constructively [5]. In tis paper, we provide a muc simpler and alternative proof for te recursive formulae of te generalized LM-inverse, B þ LM,of any given matrix, B, partitioned as B ½ j a Š, were is an m by n matrix and a is a column vector of m components. We sow tat te four conditions of te generalized LM-inverse of te recursive formulae are satisfied. Besides its inerent simplicity, our proof requires several subsidiary properties of te generalized LM-inverse of a matrix, many of wic appear to be ereto unknown; tey are presented in te ppendix. More general tan te generalized M-inverse, te generalized LM-inverse finds use in an even wider range of application areas tan te Moore Penrose inverse areas ranging from system teory, statistics, filtering, control teory, and optimization, to signal processing and mecanics. 2. Recursive formulae of te generalized LM-inverse of a matrix augmented by a column vector 2.. Result For any given matrix B ½ j a Š ð9þ its generalized LM-inverse formulae are given by B þ LM ½ j a Šþ LM þ þ ad þ L ; wen d ði þ d þ Þa 6 0; ð0þ L þ þ a p ; wen d ði þ LM Þa 0; ðþ were is an m by (n ) matrix, a is a column vector of m components, d þ L dt L=ðd T LdÞ, b qt MU, b = q T Mq, U þ, q v þ p, p ði þ 0 m ÞM ~m; and v þ M a. Note tat L is a symmetric positive definite m by m matrix, and M M ~m ~m T ; ð2þ m were M is a symmetric positive definite n by n matrix, M is te symmetric positive definite (n ) by (n ), ~m is te column vector of (n ) components, and m is te scalar. ð5þ ð6þ
4 F.E. Udwadia, P. Poomsiri / pplied Matematics and Computation 90 (2007) It sould be noted tat te formulae are given in two separate cases; wen d 5 0 and wen d = 0. Wen d 5 0, te added column vector a is not a linear combination of te columns of, and wen d = 0, te added column vector a is a linear combination of te columns of (see ppendix in Ref. [5] for a proof). Proof. Case : (wen d 5 0) Because te BB þ M and Bþ MB are repetitively used to verify all four properties of te generalized LM-inverse, we sall first evaluate BB þ M and Bþ MB. By Eqs. (9) and (0), we ave BB þ LM ½ j a Š þ þ ad þ L þ d þ þ ad þ L ðpþdþ L þ adþ L : ð3þ L Since p = 0 (see Property in ppendix) and d ði þ Þa, we get BB þ LM þ þ ad þ L þ adþ L þ þði þ Þad þ L þ þ dd þ L : ð4þ gain by Eqs. (9) and (0), we obtain B þ LM B þ þ ad þ L ½ j a Š ð5þ d þ L þ þ aðd þ L Þpðdþ L Þ þ a þ aðd þ L aþpðdþ L aþ d þ L d þ L a : ð6þ Using te relations d þ L 0 and dþ L a (see Properties 4 and 5 in ppendix), we ave B þ LM B þ þ a þ a p 0 þ p 0 : ð7þ We now verify te four properties of te generalized LM-inverse. Generalized LM-inverse condition : BB þ LM B B Using Eqs. (9) and (4), we obtain BB þ LM B ðbbþ LM ÞB ðþ þ dd þ L Þ½ j a Š ½þ þ dðd þ L Þ j þ a þ dðd þ L aþ Š: ð8þ Because þ, d þ L 0, dþ L a (see Properties 4 and 5 in ppendix), and d ði þ Þa, we ave BB þ LM B þ a þði þ Þa ½ j a Š B: Generalized LM-inverse condition 2: B þ LM BBþ LM Bþ LM Using Eqs. () and (4), we get B þ LM BBþ LM Bþ LM ðbbþ LM Þ þ þ ad þ L ½ þ d þ þ dd þ L Š; ð9þ L " þ þ þð þ dþd þ L þ aðd þ L Þþ þ ad þ L ddþ L # pðdþ L Þþ pd þ L ddþ L ðd þ L Þþ þ d þ : ð20þ L ddþ L Since þ þ þ, þ d 0, d þ L 0 (see Properties 3 and 4 in ppendix), and dþ L ddþ L dþ L,we obtain B þ LM BBþ LM þ þ ad þ L B þ LM : d þ L Generalized LM-inverse condition 3: LðBB þ LMÞ is symmetric Since L þ and Ldd þ L are symmetric, using Eq. (4), we ave LðBB þ LM ÞLðþ þ dd þ L ÞLþ þ Ldd þ L ; wic is symmetric.
5 002 F.E. Udwadia, P. Poomsiri / pplied Matematics and Computation 90 (2007) Generalized LM-inverse condition 4: MðB þ LMBÞ is symmetric Using Eqs. (2) and (7), we obtain MðB þ LM BÞ M ~m þ ~m T m 0 " p M þ # M p þ ~m ~m T þ ~m T p þ m E ; E ;2 ; ð2þ E 2; E 2;2 were E,, E,2, E 2,, ande 2,2 represent te elements (,), (, 2), (2,), and (2, 2) of te matrix MðB þ LM BÞ, respectively. Note tat E, is te (n ) by (n ) matrix, E,2 is te column vector of (n ) components, E 2, is te row vector of (n ) components, and E 2,2 is te scalar. We see tat E ; M ð þ Þ is symmetric since þ is te generalized -inverse of, wile E 2,2 is a scalar, and is terefore symmetric. Tus, for MðB þ LM BÞ to be symmetric, we need to sow tat E,2 is te transpose of E 2,. Using p ði þ ÞM ~m, te element E,2 can be written as M p þ ~m M ði þ ÞM ~m þ ~m M ð þ ÞM ~m ðþ Þ T ~m; ð22þ wic is te transpose of te element E 2,. Hence, MðB þ LMBÞ is symmetric. We ave sown tat all four generalized LM-inverse conditions are satisfied. Hence, te formula (0) is verified. Case 2: (wen d =0) We begin again by evaluating BB þ LM and Bþ LMB quantities tat we will need furter along. Using Eqs. (9) and (), weave BB þ LM ½ j a Š þ þ a p ½ þ LM ð þ aþ ðpþ þ aš: ð23þ Since þ a a and p = 0 (see Properties and 2 in ppendix), we get BB þ LM ½þ a þ aš þ : Using Eqs. (9) and (), weave B þ LM B þ þ a p ½ j a Š þ þ a p þ a þ aa pa : a ð25þ We next verify te four properties of te Generalized LM-inverse. Generalized LM-inverse condition : BB þ LM B B Using te fact tat þ and þ a a (see Property 2 in ppendix), by Eqs. (9) and (24) we obtain BB þ LM B ðbbþ LM ÞB þ ½ j a Š ½ þ þ a Š½ j a Š B: Generalized LM-inverse condition 2: B þ LM BBþ LM Bþ LM By Eqs. () and (24), we ave B þ LM BBþ LM Bþ LM ðbbþ LM Þ þ þ " # a p þ þ LM LM þ þ að þ Þpð þ Þ þ : ð26þ Since þ þ þ and þ (see Property 9 in ppendix), we ave B þ LM BBþ LM þ þ a p B þ LM : ð24þ
6 F.E. Udwadia, P. Poomsiri / pplied Matematics and Computation 90 (2007) Generalized LM-inverse condition 3: LðBB þ LMÞ is symmetric Because L þ is symmetric, by Eq. (24) we ave ðbb þ LM ÞT ð þ Þ T L þ L LBB þ LM L : Generalized LM-inverse condition 4: MðB þ LMBÞ is symmetric. Using Eqs. (2), (25), andv þ a, we obtain MðB þ LM BÞ M ~m þ v p v va pa ~m T m ; a " M ð þ # v pþþ~mðþ M ðv va paþþ~mðaþ ~m T ð þ v pþþmðþ ~m T ðv va paþþmðaþ E ; E ;2 ; ð27þ E 2; E 2;2 were E,, E,2, E 2,,andE 2,2 represent te elements (,), (, 2), (2,), and (2,2) of te matrix MðB þ LM BÞ, respectively. Note tat E, is te (n ) by (n ) square matrix, E,2 is te column vector of (n ) components, E 2, is te row vector of (n ) components, and E 2,2 is te scalar. For MðB þ LMBÞ to be symmetric, we need to sow tat E, is symmetric and E,2 is te transpose of E 2,. Let us first sow tat E, is symmetric. We can rewrite E, as E ; M þ ðm v þ M p ~mþðþ: Since M v þ M p ~m bðþ T (see Property 2 in ppendix), we get E ; M þ bðþ T ðþ: Because M þ and b() T () are symmetric, E, is symmetric. Next, we will sow tat E,2 is te transpose of E 2,. Let us rewrite E,2 as E ;2 M v ðm v þ M p ~mþðaþ: Using a b ðvt M v ~m T vþ and M p ~m ð þ Þ T ~m (see Properties 0 and in ppendix) in Eq. (30), we obtain i E ;2 M v M v ð þ Þ T ~m v T M v ~m T v b : ð3þ On te oter and, E 2, can be written as E 2; ~m T þ ~m T v þ ~m T p m ðþ: ð32þ Using b ðvt M ~m T þ Þ and ~m T v þ ~m T p m v T M v v T ~m b (see Properties 8 and 4 in ppendix) in Eq. (32), we get E 2; ~m T ð þ Þ v T M v v T ~m b v T M ~m T þ b ; ð33þ wic can be simplified to E 2; v T M v T M v v T ~m v T M ~m T þ b : ð28þ ð29þ ð30þ ð34þ It can be seen from Eqs. (3) and (34) tat E,2 is te transpose of E 2,. Since we ave already sown tat E, is symmetric and since E 2,2 is scalar wic is symmetric, te symmetry of MðB þ LMBÞ is verified. We ave sown tat all four generalized LM-inverse conditions are satisfied. Hence, te formula () is verified.
7 004 F.E. Udwadia, P. Poomsiri / pplied Matematics and Computation 90 (2007) Conclusions Te recursive formulae for obtaining te generalized LM-inverse of any general matrix augmented by a column vector were first given in Ref. 5. Tere tey were derived in a constructive manner. We erein provide an alternative proof of teir formulae by directly verifying tat te four conditions of te generalized LM-inverse are satisfied, tereby confirming te validity of te formulae, and providing several new auxiliary results related to tese generalized inverses. ppendix Tis section provides some properties tat are used for verifying te recursive formulae for determining of te generalized LM-inverse of a matrix. Property. p = 0. Proof. Since p ði þ ÞM ~m, we ave p ði þ ÞM ~m 0: Property 2. a þ a (wen d = 0). Proof. Because d ði þ Þa 0, we get a þ a: Property 3. þ d 0. Proof. Since d ði þ Þa, we obtain þ d þ ði þ Þa 0: Property 4. d þ L 0. Proof. Since d ði þ Þa and d þ L ðdt LdÞ d T L, we ave d þ L ðdt LdÞ d T L ðd T LdÞ ði þ T Þa L ðd T LdÞ a T ði þ Þ T L ðd T LdÞ a T LðI þ ÞL L 0: Property 5. d þ L a. Proof. Using d þ L ðdt LdÞ d T L and d ði þ Þa, weave d þ L a dt La d T Ld ½ðI þ ÞaŠ T La ½ðI þ ÞaŠ T L½ðI þ ÞaŠ a T þ LðI ÞL La a T LðI þ ÞL LðI þ Þa at LðI þ Þa a T LðI þ Þa : Property 6. b ðvt M ~m T Þ þ. Proof. Since b qt MU, were b = q T Mq, q and U,weave þ 0 m v þ p, v þ a, p ði þ ÞM ~m, M M ~m ~m T m,
8 F.E. Udwadia, P. Poomsiri / pplied Matematics and Computation 90 (2007) b qt MU T v þ p M ~m þ b ~m T m 0 m b vt M þ þ p T M þ ~m T þ : b vt þ p T j " # M þ ~m T þ ; Because p T M þ ½~m T M ði þ Þ T ŠM þ ~m T M M ði þ ÞM M þ 0, we obtain b ðvt M þ ~m T þ Þ b ðvt M ~m T Þ þ : Property 7. v T M þ v T M. Proof. Since v þ a and M þ ð þ Þ T M, we ave v T M þ ð þ aþ T ð þ Þ T M ð þ þ aþ T M ð þ aþ T M v T M : Property 8. b ðvt M ~m T þ Þ. Proof. Since b ðvt M ~m T Þ þ b ðvt M þ ~m T þ Þ b ðvt M ~m T þ Þ: Property 9. þ. and v T M þ v T M (see Properties 6 and 7 above), we ave Proof. Since b ðvt M ~m T Þ þ (see Property 6 above) and þ þ þ, we get þ b ðvt M ~m T Þ þ þ b ðvt M ~m T Þ þ : Property 0. a b ðvt M v ~m T vþ. Proof. Because þ a v and b ðvt M ~m T Þ þ a b ðvt M þ a ~m T þ aþ b ðvt M v ~m T vþ: Property. M p ~m ð þ Þ T ~m. Proof. Since p ði þ ÞM ~m, we get (see Property 6 above), we ave M p ~m M ½ðI þ ÞM ~mš~m M þ M ~m ðþ Þ T ~m: Property 2. M v þ M p ~m ½M v ð þ Þ T ~mš T bðþ T. Proof. Since M p ~m ð þ Þ T ~m and v T M ~m T þ b (see Properties 8 and above), we get M v þ M p ~m M v ð þ Þ T ~m ½v T M ~m T þ Š T bðþ T : Property 3. p T M ~m T ði þ Þ. Proof. Because p ði þ ÞM ~m and v þ a,weave p T M ½ðI þ ÞM ~mšt M ~m T M ½M ði þ ÞM ŠM ~m T ði þ Þ:
9 006 F.E. Udwadia, P. Poomsiri / pplied Matematics and Computation 90 (2007) Property 4. ~m T v þ ~m T p m v T M v v T ~m b. Proof. Since q v þ p, and M M ~m ~m T, we ave m b q T Mq v þ p T M ~m v þ p ~m T v T M v þ 2p T M v 2~m T v þ p T M p 2~m T p þ m; m were we ave used p T Mv = v T Mp, ~m T v v T ~m, and ~m T p p T ~m since tey are scalars. Using p T M ~m T ði þ Þ (see Property 3 above), we ave p T M v ~m T ði þ Þ þ a 0 and p T M p ½~m T ði þ ÞŠ½ðI þ ÞM ~mš ~mt ½ðI þ ÞM ~mš ~mt p. Tus, we obtain b v T M v 2~m T v ~m T p þ m, wic gives m b v T M v þ 2~m T v þ ~m T p: Using te relation above and again te fact tat ~m T v v T ~m, we ave ~m T v þ ~m T p m ~m T v þ ~m T p ðbv T M v þ 2~m T v þ ~m T pþv T M v v T ~m b: References [] C.R. Rao, S.K. Mitra, Generalized Inverses of Matrices and Its pplications, Wiley, New York, 97. [2] E.H. Moore, On te reciprocal of te general algebraic matrix, Bulletin of te merican Matematical Society 26 (920) [3] R.. Penrose, Generalized inverse for matrices, Proceedings of te Cambridge Pilosopical Society 5 (955) [4] T.N.E. Greville, Some applications of te pseudoinverse of a matrix, SIM Review 2 (960) [5] C.R. Rao, note on a generalized inverse of a matrix wit applications to problems in matematical statistics, Journal of te Royal Statistical Society Series B 24 (962) [6] F. Graybill, Matrices and pplications to Statistics, second ed., Wadswort, Belmont, California, 983. [7] R.E. Kalaba, F.E. Udwadia, ssociative memory approac to te identification of structural and mecanical systems, Journal of Optimization Teory and pplications 76 (993) [8] F.E. Udwadia, R.E. Kalaba, nalytical Dynamics: New pproac, Cambridge University Press, Cambridge, England, 996. [9] J. Franklin, Least-squares solution of equations of motion under inconsistent constraints, Linear lgebra and Its pplications 222 (995) 9 3. [0] F.E. Udwadia, R.E. Kalaba, n alternative proof of te Greville formula, Journal of Optimization Teory and pplications 94 (997) [] F.E. Udwadia, R.E. Kalaba, unified approac for te recursive determination of generalized inverses, Computers and Matematics wit pplications 37 (999) [2] F.E. Udwadia, R.E. Kalaba, Sequential determination of te {,4}-inverse of a matrix, Journal of Optimization Teory and pplications 7 (2003) 7. [3] F.E. Udwadia, P. Poomsiri, Te recursive determination of te generalized Moore Penrose M-inverse of a matrix, Journal of Optimization Teory and pplications 27 (3) (2005) [4] P. Poomsiri, B. Han, n alternative proof for te recursive formulae for computing te Moore Penrose M-inverse of a matrix, pplied Matematics and Computation 74 (2006) [5] F.E. Udwadia, P. Poomsiri, Recursive formulae for te generalized LM-inverse of a matrix, Journal of Optimization Teory and pplications 3 () (2006) 6.
More on generalized inverses of partitioned matrices with Banachiewicz-Schur forms
More on generalized inverses of partitioned matrices wit anaciewicz-scur forms Yongge Tian a,, Yosio Takane b a Cina Economics and Management cademy, Central University of Finance and Economics, eijing,
More informationRecursive Determination of the Generalized Moore Penrose M-Inverse of a Matrix
journal of optimization theory and applications: Vol. 127, No. 3, pp. 639 663, December 2005 ( 2005) DOI: 10.1007/s10957-005-7508-7 Recursive Determination of the Generalized Moore Penrose M-Inverse of
More informationAn Alternative Proof of the Greville Formula
JOURNAL OF OPTIMIZATION THEORY AND APPLICATIONS: Vol. 94, No. 1, pp. 23-28, JULY 1997 An Alternative Proof of the Greville Formula F. E. UDWADIA1 AND R. E. KALABA2 Abstract. A simple proof of the Greville
More informationChaos, Solitons & Fractals Nonlinear Science, and Nonequilibrium and Complex Phenomena
Caos, Solitons & Fractals 5 (0) 77 79 Contents lists available at SciVerse ScienceDirect Caos, Solitons & Fractals Nonlinear Science, and Nonequilibrium and Complex Penomena journal omepage: www.elsevier.com/locate/caos
More information1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point
MA00 Capter 6 Calculus and Basic Linear Algebra I Limits, Continuity and Differentiability Te concept of its (p.7 p.9, p.4 p.49, p.55 p.56). Limits Consider te function determined by te formula f Note
More informationThe derivative function
Roberto s Notes on Differential Calculus Capter : Definition of derivative Section Te derivative function Wat you need to know already: f is at a point on its grap and ow to compute it. Wat te derivative
More informationInternational Journal of Approximate Reasoning
International Journal of Approximate Reasoning 49 (2008) 422 435 Contents lists available at ScienceDirect International Journal of Approximate Reasoning journal omepage: www.elsevier.com/locate/ijar Modus
More informationch (for some fixed positive number c) reaching c
GSTF Journal of Matematics Statistics and Operations Researc (JMSOR) Vol. No. September 05 DOI 0.60/s4086-05-000-z Nonlinear Piecewise-defined Difference Equations wit Reciprocal and Cubic Terms Ramadan
More informationMAT Calculus for Engineers I EXAM #1
MAT 65 - Calculus for Engineers I EXAM # Instructor: Liu, Hao Honor Statement By signing below you conrm tat you ave neiter given nor received any unautorized assistance on tis eam. Tis includes any use
More informationMathematics 5 Worksheet 11 Geometry, Tangency, and the Derivative
Matematics 5 Workseet 11 Geometry, Tangency, and te Derivative Problem 1. Find te equation of a line wit slope m tat intersects te point (3, 9). Solution. Te equation for a line passing troug a point (x
More informationSymmetry Labeling of Molecular Energies
Capter 7. Symmetry Labeling of Molecular Energies Notes: Most of te material presented in tis capter is taken from Bunker and Jensen 1998, Cap. 6, and Bunker and Jensen 2005, Cap. 7. 7.1 Hamiltonian Symmetry
More informationA = h w (1) Error Analysis Physics 141
Introduction In all brances of pysical science and engineering one deals constantly wit numbers wic results more or less directly from experimental observations. Experimental observations always ave inaccuracies.
More informationTHE IDEA OF DIFFERENTIABILITY FOR FUNCTIONS OF SEVERAL VARIABLES Math 225
THE IDEA OF DIFFERENTIABILITY FOR FUNCTIONS OF SEVERAL VARIABLES Mat 225 As we ave seen, te definition of derivative for a Mat 111 function g : R R and for acurveγ : R E n are te same, except for interpretation:
More informationOn convexity of polynomial paths and generalized majorizations
On convexity of polynomial pats and generalized majorizations Marija Dodig Centro de Estruturas Lineares e Combinatórias, CELC, Universidade de Lisboa, Av. Prof. Gama Pinto 2, 1649-003 Lisboa, Portugal
More informationElectron transport through a strongly correlated monoatomic chain
Surface Science () 97 7 www.elsevier.com/locate/susc Electron transport troug a strongly correlated monoatomic cain M. Krawiec *, T. Kwapiński Institute of Pysics and anotecnology Center, M. Curie-Skłodowska
More information232 Calculus and Structures
3 Calculus and Structures CHAPTER 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS FOR EVALUATING BEAMS Calculus and Structures 33 Copyrigt Capter 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS 17.1 THE
More informationQuantum Mechanics Chapter 1.5: An illustration using measurements of particle spin.
I Introduction. Quantum Mecanics Capter.5: An illustration using measurements of particle spin. Quantum mecanics is a teory of pysics tat as been very successful in explaining and predicting many pysical
More informationDifferentiation in higher dimensions
Capter 2 Differentiation in iger dimensions 2.1 Te Total Derivative Recall tat if f : R R is a 1-variable function, and a R, we say tat f is differentiable at x = a if and only if te ratio f(a+) f(a) tends
More informationPre-Calculus Review Preemptive Strike
Pre-Calculus Review Preemptive Strike Attaced are some notes and one assignment wit tree parts. Tese are due on te day tat we start te pre-calculus review. I strongly suggest reading troug te notes torougly
More informationREVIEW LAB ANSWER KEY
REVIEW LAB ANSWER KEY. Witout using SN, find te derivative of eac of te following (you do not need to simplify your answers): a. f x 3x 3 5x x 6 f x 3 3x 5 x 0 b. g x 4 x x x notice te trick ere! x x g
More informationMaterial for Difference Quotient
Material for Difference Quotient Prepared by Stepanie Quintal, graduate student and Marvin Stick, professor Dept. of Matematical Sciences, UMass Lowell Summer 05 Preface Te following difference quotient
More informationlecture 26: Richardson extrapolation
43 lecture 26: Ricardson extrapolation 35 Ricardson extrapolation, Romberg integration Trougout numerical analysis, one encounters procedures tat apply some simple approximation (eg, linear interpolation)
More informationNONLINEAR SYSTEMS IDENTIFICATION USING THE VOLTERRA MODEL. Georgeta Budura
NONLINEAR SYSTEMS IDENTIFICATION USING THE VOLTERRA MODEL Georgeta Budura Politenica University of Timisoara, Faculty of Electronics and Telecommunications, Comm. Dep., georgeta.budura@etc.utt.ro Abstract:
More information4. The slope of the line 2x 7y = 8 is (a) 2/7 (b) 7/2 (c) 2 (d) 2/7 (e) None of these.
Mat 11. Test Form N Fall 016 Name. Instructions. Te first eleven problems are wort points eac. Te last six problems are wort 5 points eac. For te last six problems, you must use relevant metods of algebra
More informationNonlinear correction to the bending stiffness of a damaged composite beam
Van Paepegem, W., Decaene, R. and Degrieck, J. (5). Nonlinear correction to te bending stiffness of a damaged composite beam. Nonlinear correction to te bending stiffness of a damaged composite beam W.
More informationTHE STURM-LIOUVILLE-TRANSFORMATION FOR THE SOLUTION OF VECTOR PARTIAL DIFFERENTIAL EQUATIONS. L. Trautmann, R. Rabenstein
Worksop on Transforms and Filter Banks (WTFB),Brandenburg, Germany, Marc 999 THE STURM-LIOUVILLE-TRANSFORMATION FOR THE SOLUTION OF VECTOR PARTIAL DIFFERENTIAL EQUATIONS L. Trautmann, R. Rabenstein Lerstul
More informationMath 31A Discussion Notes Week 4 October 20 and October 22, 2015
Mat 3A Discussion Notes Week 4 October 20 and October 22, 205 To prepare for te first midterm, we ll spend tis week working eamples resembling te various problems you ve seen so far tis term. In tese notes
More information7.1 Using Antiderivatives to find Area
7.1 Using Antiderivatives to find Area Introduction finding te area under te grap of a nonnegative, continuous function f In tis section a formula is obtained for finding te area of te region bounded between
More information3.4 Worksheet: Proof of the Chain Rule NAME
Mat 1170 3.4 Workseet: Proof of te Cain Rule NAME Te Cain Rule So far we are able to differentiate all types of functions. For example: polynomials, rational, root, and trigonometric functions. We are
More informationBlueprint End-of-Course Algebra II Test
Blueprint End-of-Course Algebra II Test for te 2001 Matematics Standards of Learning Revised July 2005 Tis revised blueprint will be effective wit te fall 2005 administration of te Standards of Learning
More informationBifurcation Analysis of a Vaccination Model of Tuberculosis Infection
merican Journal of pplied and Industrial Cemistry 2017; 1(1): 5-9 ttp://www.sciencepublisinggroup.com/j/ajaic doi: 10.11648/j.ajaic.20170101.12 Bifurcation nalysis of a Vaccination Model of Tuberculosis
More informationHow to Find the Derivative of a Function: Calculus 1
Introduction How to Find te Derivative of a Function: Calculus 1 Calculus is not an easy matematics course Te fact tat you ave enrolled in suc a difficult subject indicates tat you are interested in te
More informationPolynomial Interpolation
Capter 4 Polynomial Interpolation In tis capter, we consider te important problem of approximatinga function fx, wose values at a set of distinct points x, x, x,, x n are known, by a polynomial P x suc
More informationChapter 4 Derivatives [ ] = ( ) ( )= + ( ) + + = ()= + ()+ Exercise 4.1. Review of Prerequisite Skills. 1. f. 6. d. 4. b. lim. x x. = lim = c.
Capter Derivatives Review of Prerequisite Skills. f. p p p 7 9 p p p Eercise.. i. ( a ) a ( b) a [ ] b a b ab b a. d. f. 9. c. + + ( ) ( + ) + ( + ) ( + ) ( + ) + + + + ( ) ( + ) + + ( ) ( ) ( + ) + 7
More informationIntroduction to Derivatives
Introduction to Derivatives 5-Minute Review: Instantaneous Rates and Tangent Slope Recall te analogy tat we developed earlier First we saw tat te secant slope of te line troug te two points (a, f (a))
More informationGELFAND S PROOF OF WIENER S THEOREM
GELFAND S PROOF OF WIENER S THEOREM S. H. KULKARNI 1. Introduction Te following teorem was proved by te famous matematician Norbert Wiener. Wiener s proof can be found in is book [5]. Teorem 1.1. (Wiener
More informationNumerical Analysis MTH603. dy dt = = (0) , y n+1. We obtain yn. Therefore. and. Copyright Virtual University of Pakistan 1
Numerical Analysis MTH60 PREDICTOR CORRECTOR METHOD Te metods presented so far are called single-step metods, were we ave seen tat te computation of y at t n+ tat is y n+ requires te knowledge of y n only.
More informationWYSE Academic Challenge 2004 Sectional Mathematics Solution Set
WYSE Academic Callenge 00 Sectional Matematics Solution Set. Answer: B. Since te equation can be written in te form x + y, we ave a major 5 semi-axis of lengt 5 and minor semi-axis of lengt. Tis means
More informationChapter 1 Functions and Graphs. Section 1.5 = = = 4. Check Point Exercises The slope of the line y = 3x+ 1 is 3.
Capter Functions and Graps Section. Ceck Point Exercises. Te slope of te line y x+ is. y y m( x x y ( x ( y ( x+ point-slope y x+ 6 y x+ slope-intercept. a. Write te equation in slope-intercept form: x+
More informationExam 1 Review Solutions
Exam Review Solutions Please also review te old quizzes, and be sure tat you understand te omework problems. General notes: () Always give an algebraic reason for your answer (graps are not sufficient),
More informationSection 2.7 Derivatives and Rates of Change Part II Section 2.8 The Derivative as a Function. at the point a, to be. = at time t = a is
Mat 180 www.timetodare.com Section.7 Derivatives and Rates of Cange Part II Section.8 Te Derivative as a Function Derivatives ( ) In te previous section we defined te slope of te tangent to a curve wit
More informationThe entransy dissipation minimization principle under given heat duty and heat transfer area conditions
Article Engineering Termopysics July 2011 Vol.56 No.19: 2071 2076 doi: 10.1007/s11434-010-4189-x SPECIAL TOPICS: Te entransy dissipation minimization principle under given eat duty and eat transfer area
More informationVolume 29, Issue 3. Existence of competitive equilibrium in economies with multi-member households
Volume 29, Issue 3 Existence of competitive equilibrium in economies wit multi-member ouseolds Noriisa Sato Graduate Scool of Economics, Waseda University Abstract Tis paper focuses on te existence of
More information5.1 We will begin this section with the definition of a rational expression. We
Basic Properties and Reducing to Lowest Terms 5.1 We will begin tis section wit te definition of a rational epression. We will ten state te two basic properties associated wit rational epressions and go
More informationf a h f a h h lim lim
Te Derivative Te derivative of a function f at a (denoted f a) is f a if tis it exists. An alternative way of defining f a is f a x a fa fa fx fa x a Note tat te tangent line to te grap of f at te point
More informationBrazilian Journal of Physics, vol. 29, no. 1, March, Ensemble and their Parameter Dierentiation. A. K. Rajagopal. Naval Research Laboratory,
Brazilian Journal of Pysics, vol. 29, no. 1, Marc, 1999 61 Fractional Powers of Operators of sallis Ensemble and teir Parameter Dierentiation A. K. Rajagopal Naval Researc Laboratory, Wasington D. C. 2375-532,
More informationPreface. Here are a couple of warnings to my students who may be here to get a copy of what happened on a day that you missed.
Preface Here are my online notes for my course tat I teac ere at Lamar University. Despite te fact tat tese are my class notes, tey sould be accessible to anyone wanting to learn or needing a refreser
More information(a) At what number x = a does f have a removable discontinuity? What value f(a) should be assigned to f at x = a in order to make f continuous at a?
Solutions to Test 1 Fall 016 1pt 1. Te grap of a function f(x) is sown at rigt below. Part I. State te value of eac limit. If a limit is infinite, state weter it is or. If a limit does not exist (but is
More informationClose-packed dimers on nonorientable surfaces
4 February 2002 Pysics Letters A 293 2002 235 246 wwwelseviercom/locate/pla Close-packed dimers on nonorientable surfaces Wentao T Lu FYWu Department of Pysics orteastern University Boston MA 02115 USA
More informationResearch Article Error Analysis for a Noisy Lacunary Cubic Spline Interpolation and a Simple Noisy Cubic Spline Quasi Interpolation
Advances in Numerical Analysis Volume 204, Article ID 35394, 8 pages ttp://dx.doi.org/0.55/204/35394 Researc Article Error Analysis for a Noisy Lacunary Cubic Spline Interpolation and a Simple Noisy Cubic
More informationFinding and Using Derivative The shortcuts
Calculus 1 Lia Vas Finding and Using Derivative Te sortcuts We ave seen tat te formula f f(x+) f(x) (x) = lim 0 is manageable for relatively simple functions like a linear or quadratic. For more complex
More informationMATH1131/1141 Calculus Test S1 v8a
MATH/ Calculus Test 8 S v8a October, 7 Tese solutions were written by Joann Blanco, typed by Brendan Trin and edited by Mattew Yan and Henderson Ko Please be etical wit tis resource It is for te use of
More informationDerivatives and Rates of Change
Section.1 Derivatives and Rates of Cange 2016 Kiryl Tsiscanka Derivatives and Rates of Cange Measuring te Rate of Increase of Blood Alcool Concentration Biomedical scientists ave studied te cemical and
More informationSome Review Problems for First Midterm Mathematics 1300, Calculus 1
Some Review Problems for First Midterm Matematics 00, Calculus. Consider te trigonometric function f(t) wose grap is sown below. Write down a possible formula for f(t). Tis function appears to be an odd,
More informationETNA Kent State University
Electronic Transactions on Numerical Analysis. Volume 34, pp. 14-19, 2008. Copyrigt 2008,. ISSN 1068-9613. ETNA A NOTE ON NUMERICALLY CONSISTENT INITIAL VALUES FOR HIGH INDEX DIFFERENTIAL-ALGEBRAIC EQUATIONS
More informationLIMITS AND DERIVATIVES CONDITIONS FOR THE EXISTENCE OF A LIMIT
LIMITS AND DERIVATIVES Te limit of a function is defined as te value of y tat te curve approaces, as x approaces a particular value. Te limit of f (x) as x approaces a is written as f (x) approaces, as
More informationLecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator.
Lecture XVII Abstract We introduce te concept of directional derivative of a scalar function and discuss its relation wit te gradient operator. Directional derivative and gradient Te directional derivative
More informationThe Verlet Algorithm for Molecular Dynamics Simulations
Cemistry 380.37 Fall 2015 Dr. Jean M. Standard November 9, 2015 Te Verlet Algoritm for Molecular Dynamics Simulations Equations of motion For a many-body system consisting of N particles, Newton's classical
More informationChapter 2. Limits and Continuity 16( ) 16( 9) = = 001. Section 2.1 Rates of Change and Limits (pp ) Quick Review 2.1
Capter Limits and Continuity Section. Rates of Cange and Limits (pp. 969) Quick Review..... f ( ) ( ) ( ) 0 ( ) f ( ) f ( ) sin π sin π 0 f ( ). < < < 6. < c c < < c 7. < < < < < 8. 9. 0. c < d d < c
More informationMath 1210 Midterm 1 January 31st, 2014
Mat 110 Midterm 1 January 1st, 01 Tis exam consists of sections, A and B. Section A is conceptual, wereas section B is more computational. Te value of every question is indicated at te beginning of it.
More informationPolynomial Interpolation
Capter 4 Polynomial Interpolation In tis capter, we consider te important problem of approximating a function f(x, wose values at a set of distinct points x, x, x 2,,x n are known, by a polynomial P (x
More informationQuantum mechanical effects in internal photoemission THz detectors
Infrared Pysics & Tecnology 50 (007) 199 05 www.elsevier.com/locate/infrared Quantum mecanical effects in internal potoemission THz detectors M.B. Rinzan, S. Matsik, A.G.U. Perera * Department of Pysics
More informationUNIVERSITY OF MANITOBA DEPARTMENT OF MATHEMATICS MATH 1510 Applied Calculus I FIRST TERM EXAMINATION - Version A October 12, :30 am
DEPARTMENT OF MATHEMATICS MATH 1510 Applied Calculus I October 12, 2016 8:30 am LAST NAME: FIRST NAME: STUDENT NUMBER: SIGNATURE: (I understand tat ceating is a serious offense DO NOT WRITE IN THIS TABLE
More informationGlobal Existence of Classical Solutions for a Class Nonlinear Parabolic Equations
Global Journal of Science Frontier Researc Matematics and Decision Sciences Volume 12 Issue 8 Version 1.0 Type : Double Blind Peer Reviewed International Researc Journal Publiser: Global Journals Inc.
More informationChapter 2 Limits and Continuity
4 Section. Capter Limits and Continuity Section. Rates of Cange and Limits (pp. 6) Quick Review.. f () ( ) () 4 0. f () 4( ) 4. f () sin sin 0 4. f (). 4 4 4 6. c c c 7. 8. c d d c d d c d c 9. 8 ( )(
More informationSECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY
(Section 3.2: Derivative Functions and Differentiability) 3.2.1 SECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY LEARNING OBJECTIVES Know, understand, and apply te Limit Definition of te Derivative
More information1. Consider the trigonometric function f(t) whose graph is shown below. Write down a possible formula for f(t).
. Consider te trigonometric function f(t) wose grap is sown below. Write down a possible formula for f(t). Tis function appears to be an odd, periodic function tat as been sifted upwards, so we will use
More informationEfficient algorithms for for clone items detection
Efficient algoritms for for clone items detection Raoul Medina, Caroline Noyer, and Olivier Raynaud Raoul Medina, Caroline Noyer and Olivier Raynaud LIMOS - Université Blaise Pascal, Campus universitaire
More informationSFU UBC UNBC Uvic Calculus Challenge Examination June 5, 2008, 12:00 15:00
SFU UBC UNBC Uvic Calculus Callenge Eamination June 5, 008, :00 5:00 Host: SIMON FRASER UNIVERSITY First Name: Last Name: Scool: Student signature INSTRUCTIONS Sow all your work Full marks are given only
More informationDepartment of Statistics & Operations Research, Aligarh Muslim University, Aligarh, India
Open Journal of Optimization, 04, 3, 68-78 Publised Online December 04 in SciRes. ttp://www.scirp.org/ournal/oop ttp://dx.doi.org/0.436/oop.04.34007 Compromise Allocation for Combined Ratio Estimates of
More information= 0 and states ''hence there is a stationary point'' All aspects of the proof dx must be correct (c)
Paper 1: Pure Matematics 1 Mark Sceme 1(a) (i) (ii) d d y 3 1x 4x x M1 A1 d y dx 1.1b 1.1b 36x 48x A1ft 1.1b Substitutes x = into teir dx (3) 3 1 4 Sows d y 0 and states ''ence tere is a stationary point''
More informationProblem Solving. Problem Solving Process
Problem Solving One of te primary tasks for engineers is often solving problems. It is wat tey are, or sould be, good at. Solving engineering problems requires more tan just learning new terms, ideas and
More informationMVT and Rolle s Theorem
AP Calculus CHAPTER 4 WORKSHEET APPLICATIONS OF DIFFERENTIATION MVT and Rolle s Teorem Name Seat # Date UNLESS INDICATED, DO NOT USE YOUR CALCULATOR FOR ANY OF THESE QUESTIONS In problems 1 and, state
More informationPreconditioning in H(div) and Applications
1 Preconditioning in H(div) and Applications Douglas N. Arnold 1, Ricard S. Falk 2 and Ragnar Winter 3 4 Abstract. Summarizing te work of [AFW97], we sow ow to construct preconditioners using domain decomposition
More informationWhy gravity is not an entropic force
Wy gravity is not an entropic force San Gao Unit for History and Pilosopy of Science & Centre for Time, SOPHI, University of Sydney Email: sgao7319@uni.sydney.edu.au Te remarkable connections between gravity
More informationarxiv:cond-mat/ v3 [cond-mat.stat-mech] 18 Feb 2002
Close-packed dimers on nonorientable surfaces arxiv:cond-mat/00035v3 cond-mat.stat-mec 8 Feb 2002 Wentao T. Lu and F. Y. Wu Department of Pysics orteastern University, Boston, Massacusetts 025 Abstract
More informationNumerical Differentiation
Numerical Differentiation Finite Difference Formulas for te first derivative (Using Taylor Expansion tecnique) (section 8.3.) Suppose tat f() = g() is a function of te variable, and tat as 0 te function
More informationUniversity Mathematics 2
University Matematics 2 1 Differentiability In tis section, we discuss te differentiability of functions. Definition 1.1 Differentiable function). Let f) be a function. We say tat f is differentiable at
More informationNumerical Experiments Using MATLAB: Superconvergence of Nonconforming Finite Element Approximation for Second-Order Elliptic Problems
Applied Matematics, 06, 7, 74-8 ttp://wwwscirporg/journal/am ISSN Online: 5-7393 ISSN Print: 5-7385 Numerical Experiments Using MATLAB: Superconvergence of Nonconforming Finite Element Approximation for
More informationCalculus I Practice Exam 1A
Calculus I Practice Exam A Calculus I Practice Exam A Tis practice exam empasizes conceptual connections and understanding to a greater degree tan te exams tat are usually administered in introductory
More informationContinuity and Differentiability Worksheet
Continuity and Differentiability Workseet (Be sure tat you can also do te grapical eercises from te tet- Tese were not included below! Typical problems are like problems -3, p. 6; -3, p. 7; 33-34, p. 7;
More information5 Ordinary Differential Equations: Finite Difference Methods for Boundary Problems
5 Ordinary Differential Equations: Finite Difference Metods for Boundary Problems Read sections 10.1, 10.2, 10.4 Review questions 10.1 10.4, 10.8 10.9, 10.13 5.1 Introduction In te previous capters we
More informationDistribution of reynolds shear stress in steady and unsteady flows
University of Wollongong Researc Online Faculty of Engineering and Information Sciences - Papers: Part A Faculty of Engineering and Information Sciences 13 Distribution of reynolds sear stress in steady
More information3. Using your answers to the two previous questions, evaluate the Mratio
MASSACHUSETTS INSTITUTE OF TECHNOLOGY DEPARTMENT OF MECHANICAL ENGINEERING CAMBRIDGE, MASSACHUSETTS 0219 2.002 MECHANICS AND MATERIALS II HOMEWORK NO. 4 Distributed: Friday, April 2, 2004 Due: Friday,
More informationCombining functions: algebraic methods
Combining functions: algebraic metods Functions can be added, subtracted, multiplied, divided, and raised to a power, just like numbers or algebra expressions. If f(x) = x 2 and g(x) = x + 2, clearly f(x)
More informationTaylor Series and the Mean Value Theorem of Derivatives
1 - Taylor Series and te Mean Value Teorem o Derivatives Te numerical solution o engineering and scientiic problems described by matematical models oten requires solving dierential equations. Dierential
More informationDerivation Of The Schwarzschild Radius Without General Relativity
Derivation Of Te Scwarzscild Radius Witout General Relativity In tis paper I present an alternative metod of deriving te Scwarzscild radius of a black ole. Te metod uses tree of te Planck units formulas:
More information2.11 That s So Derivative
2.11 Tat s So Derivative Introduction to Differential Calculus Just as one defines instantaneous velocity in terms of average velocity, we now define te instantaneous rate of cange of a function at a point
More informationSpatial models with spatially lagged dependent variables and incomplete data
J Geogr Syst (2010) 12:241 257 DOI 10.1007/s10109-010-0109-5 ORIGINAL ARTICLE Spatial models wit spatially lagged dependent variables and incomplete data Harry H. Kelejian Ingmar R. Pruca Received: 23
More information1. Questions (a) through (e) refer to the graph of the function f given below. (A) 0 (B) 1 (C) 2 (D) 4 (E) does not exist
Mat 1120 Calculus Test 2. October 18, 2001 Your name Te multiple coice problems count 4 points eac. In te multiple coice section, circle te correct coice (or coices). You must sow your work on te oter
More informationALGEBRA AND TRIGONOMETRY REVIEW by Dr TEBOU, FIU. A. Fundamental identities Throughout this section, a and b denotes arbitrary real numbers.
ALGEBRA AND TRIGONOMETRY REVIEW by Dr TEBOU, FIU A. Fundamental identities Trougout tis section, a and b denotes arbitrary real numbers. i) Square of a sum: (a+b) =a +ab+b ii) Square of a difference: (a-b)
More informationKnowledge-Based Systems
Knowledge-Based Systems 27 (22) 443 45 Contents lists available at SciVerse ScienceDirect Knowledge-Based Systems journal omepage: www.elsevier.com/locate/knosys Uncertainty measurement for interval-valued
More informationPacking polynomials on multidimensional integer sectors
Pacing polynomials on multidimensional integer sectors Luis B Morales IIMAS, Universidad Nacional Autónoma de México, Ciudad de México, 04510, México lbm@unammx Submitted: Jun 3, 015; Accepted: Sep 8,
More informationFractional Derivatives as Binomial Limits
Fractional Derivatives as Binomial Limits Researc Question: Can te limit form of te iger-order derivative be extended to fractional orders? (atematics) Word Count: 669 words Contents - IRODUCIO... Error!
More informationDiffraction. S.M.Lea. Fall 1998
Diffraction.M.Lea Fall 1998 Diffraction occurs wen EM waves approac an aperture (or an obstacle) wit dimension d > λ. We sall refer to te region containing te source of te waves as region I and te region
More informationDedicated to the 70th birthday of Professor Lin Qun
Journal of Computational Matematics, Vol.4, No.3, 6, 4 44. ACCELERATION METHODS OF NONLINEAR ITERATION FOR NONLINEAR PARABOLIC EQUATIONS Guang-wei Yuan Xu-deng Hang Laboratory of Computational Pysics,
More information1 Calculus. 1.1 Gradients and the Derivative. Q f(x+h) f(x)
Calculus. Gradients and te Derivative Q f(x+) δy P T δx R f(x) 0 x x+ Let P (x, f(x)) and Q(x+, f(x+)) denote two points on te curve of te function y = f(x) and let R denote te point of intersection of
More informationThe Convergence of a Central-Difference Discretization of Rudin-Osher-Fatemi Model for Image Denoising
Te Convergence of a Central-Difference Discretization of Rudin-Oser-Fatemi Model for Image Denoising Ming-Jun Lai 1, Bradley Lucier 2, and Jingyue Wang 3 1 University of Georgia, Atens GA 30602, USA mjlai@mat.uga.edu
More informationA Reconsideration of Matter Waves
A Reconsideration of Matter Waves by Roger Ellman Abstract Matter waves were discovered in te early 20t century from teir wavelengt, predicted by DeBroglie, Planck's constant divided by te particle's momentum,
More informationTime (hours) Morphine sulfate (mg)
Mat Xa Fall 2002 Review Notes Limits and Definition of Derivative Important Information: 1 According to te most recent information from te Registrar, te Xa final exam will be eld from 9:15 am to 12:15
More information