A NEW CLASS OF MODULAR EQUATIONS IN RAMANUJAN S ALTERNATIVE THEORY OF ELLIPTIC FUNCTIONS OF SIGNATURE 4 AND SOME NEW P-Q ETA-FUNCTION IDENTITIES
|
|
- Άφροδίτη Φραγκούδης
- 6 χρόνια πριν
- Προβολές:
Transcript
1 A NEW CLASS OF MODULAR EQUATIONS IN RAMANUJAN S ALTERNATIVE THEORY OF ELLIPTIC FUNCTIONS OF SIGNATURE AND SOME NEW P-Q ETA-FUNCTION IDENTITIES S. Bhagava Chasheka Adiga M. S. Mahadeva Naika. Depatent of Studies in Matheatics Univesity of Mysoe Manasa Gangothi Mysoe (INDIA Abstact: In this pape we obtain a class of odula equations in Raanujan s altenative theoy of elliptic functions of signatue eploy the to obtain a new class of P-Q eta-function identities with fou oduli akin to Raanujan s. Key wods: Elliptic functions odula equations P-Q eta-functions. 000 AMS Matheatics Subject Classification: S D5 D0.. Intoduction In his faous pape Modula Equations Appoxiation to π [6] [ pp.-9] on pages 57-6 of his Second Notebook [7] Raanujan gives an outline of theoies of elliptic functions to altenative bases coesponding to the classical theoy by way of stateents of soe esults. Poofs of all these esults can be found in one of B. C. Bendt s books [ pp ]. Soe of the esults in altenative theoies wee also peviously exained by K. Venkatachalienga [9 pp.9-95] J. M. Bowein P. B. Bowien [5]. In Section of the pesent pape we establish a class of odula equations belonging to altenative theoy of signatue. These equations copleent the known classes of odula equations [7 pp.57 6] [ pp.9-6].
2 In enties 5 7 of Chapte 5 of his Second Notebook [7] Raanujan states twenty thee elegant so called P Q eta-function identities. Eleentay poofs of eighteen of these P Q identities eploying vaious odula equations of Raanujan have been given fo the fist tie in the woks of Bendt [ pp.0-7] Bendt L.-C. Zhang []. In Section we obtain a new class of P-Q identities on eploying the odula equations of theoy of signatue established in Section.. Soe odula equations in the theoy of signatue Let x F x Z Z ; ; : ; ( : ( ;; ;; : ( : x F x F csc exp x q q π π whee 6 0 < x <. Let n denote a fixed natual nube assue that ; ;; ;; ;; F F F F n (. whee o 6. Then a odula equation of degee n in theoy of elliptic functions of signatue is a elation between induced by (.. We often say that is of degee n ove ; ( ; ( : ( Z Z is called the ultiplie. We also use the notations ; ( : : Z Z Z Z n : Z n ( : Z ( ; to indicate that has degee n ove. When the context is clea we oit the aguent in q Z( (.
3 We now collect in the following theoe soe of Raanujan s odula equations belonging to the theoy of signatue (classical theoy. Theoe.. The following odula equations hold in the theoy of signatue (classical theoy. If ae of thid eleventh thity-thid degees ove espectively then (i. ( ( ( ( ( ( ( ( ( ( ( ( (. (ii. ( ( ( ( ( ( ( ( ( ( ( ( (. whee ae ultiplies associated with the pais espectively. If ae of thid ninth degees ove espectively then (iii ( ( ( ( ( ( (. ( ( ( ( (iv ( ( (.5 whee ae ultiplies associated with the pais espectively.
4 If ae of thid fifth fifteenth degees ove espectively then ( ( ( ( (v ( ( ( ( ( ( ( ( (vi ( ( ( ( (.6 (.7 (vii (viii ( ( ( ( ( ( ( ( 6 ( ( ( ( ( ( ( ( ( ( ( ( (. 6 ( ( 9 (.9 ( ( whee ae ultiplies associated with the pais espectively. If ae of thid seventh twentyfist degees ove espectively then (ix ( ( ( ( ( ( ( ( ( ( ( ( 6 (.0 (x ( ( ( ( ( ( ( ( ( ( ( ( 6 (.
5 (xi ( ( ( ( ( ( ( ( ( ( ( ( ZZ Z 7Z (. (xii ( ( ( ( ( ( ( ( ( ( ( ( Z 7Z 7 ZZ (. whee ae ultiplies associated with the pais espectively. If ae of fifth seventh thity-fifth degees ove espectively then ( ( ( ( (xiii ( ( ( ( ( ( ( ( (. (xiv ( ( ( ( ( ( ( ( ( ( ( ( (.5 whee ae ultiplies associated with the pais espectively. 5
6 If ae of thid thiteenth thity-nineth degees ove espectively then (xv ( ( ( ( ( ( ( ( ( ( ( ( (.6 (xvi ( ( ( ( ( ( ( ( ( ( ( ( (.7 whee ae ultiplies associated with the pais espectively. Poof. Fo poofs of (i (ii see [ Enty (i (ii p.0] ; fo poofs of (iii (iv see [ Enty (xii (xiii pp.5-5] : fo poofs of (v (vi (vii (viii see [ Enty (viii (ix (x (xi p.] ; fo poofs of (ix (x (xi (xii see [ Enty (i (ii (iii (iv p.0] ; fo poofs of (xiii (xiv see [ Enty (v (vi p.] ; lastly fo poofs of (xv (xvi see [ Enty 9 (iv p.6]. While outlining his theoy of signatue Raanujan indicates a device of deducing foulas in the theoy of signatue fo coesponding foulas in the classical theoy. In fact if we eplace then x x by x (. Z( ; x gets eplaced by x Z( ; x (.9 q ( x gets eplaced by q (x (.0 6
7 any foula Ω ( x q Z( 0 in the classical theoy yields the foula Ω x q x Z( x 0 in the theoy of signatue. One ay see [ pp. 5-6] fo details whee Bendt also establishes vaious Raanujan s odula equations in the theoy of signatue by this echanis. The odula equations in the theoy of signatue stated in the Theoe. below ae obtained in exactly the sae fashion stating fo the classical odula equations of Theoe.. Theoe.. The following odula equations hold in the theoy of signatue. If ae of thid eleventh thitythid degees ove espectively then (i ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( (. (ii ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( (. whee ae ultiplies associated with the pais espectively. 7
8 If ae of thid ninth degees ove espectively then (iii ( ( ( ( ( ( ( ( ( (. (iv ( ( ( ( ( ( ( ( ( (. whee ae ultiplies associated with the pais espectively. If ae of thid fifth fifteenth degees ove espectively then (v ( ( ( ( ( ( ( ( ( ( ( ( (.5 (vi ( ( ( ( ( ( ( ( ( ( ( ( (.6
9 9 (vii ( ( ( ( ( ( ( ( ' ( ( ( ( ( ( ( ( 6 (.7 (viii ( ( ( ( ( ( ( ( 9 ( ( ( ( ( ( ( ( 6 (. whee ae ultiplies associated with the pais espectively. If ae of thid seventh twentyfist degees ove espectively then (ix ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( 6 (.9 (x ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( 6 (.0 (xi ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( (.
10 (xii ( ( ( ( ( ( ( ( ( ( ( ( 7 ( ( ( ( (. whee ae ultiplies associated with the pais espectively. If ae of fifth seventh thity-fifth degees ove espectively then (xiii ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( (. (xiv ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( (. whee ae ultiplies associated with the pais espectively. If ae of thid thiteenth thity ninth degees ove espectively then (xv ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( (.5 0
11 (xvi ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( (.6 whee ae ultiplies associated with the pais espectively. Poof. In view of the eaks ade iediately peceeding the stateent of the theoe we deonstate the poof of only two of the identities (. (.6. Fo exaple to pove (. effect tansfoations (. (.9 (.0 epeatedly on (. of Theoe.. We then obtain ( '( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( (. (.7 ( ( Multiplying both sides of (.7 by we obtain ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( (. ( ( This copletes the poof of (..
12 To pove (. effect tansfoations (. (.9 (.0 epeatedly on (.5 of Theo.. We then obtain ( ( ( ( ( ( ( ( ( ( ( ( ( (. (. ( ( ( Multiplying both sides of (. by ( we obtain ( ( ( ( ( ( ( ( ( This copletes the poof of (.. (. (. Soe P-Q eta-function identities with fou oduli In this section we obtain algebaic identities between functions of the type. p n z nz z nz ( z : o z nz η ( z η ( nz Q n ( z : P n (z. Hee n ae cetain positive integes z sts as usual fo the Dedekind s eta-function defined by πiz η ( z : q f ( q q e I z > 0 (. whee f is the theta function in Raanujan s notations given by f ( q : Π( q n q <. (.
13 Ou poof consists in eleentay algebaic anipulations of the odula equations in the theoy of signatue stated in Theoe.. We will obtain identities (.-(.0 of which the fist six appea new to liteatue the last two (.9 (.0 ae due to Raanujan poofs eploying Raanujan s odula equations in the theoy of signatue can be found in Bundt s book [ pp.-] whee he also establishes seveal othe Raanujan s P-Q identities with two oduli. Theoe.. If f(-q z ae as defined in (. (. then the following P-Q identities hold with Q (q : P (q always. (i P Q PQ Q P ( P Q PQ whee z z f ( q f ( q P : z z qf ( q f ( q (. P Q P Q (ii PQ PQ Q P Q P whee z 7z P : (. z z (iii P Q 7PQ Q P ( P Q PQ whee z z P : (.5 7z z (iv P Q PQ Q P ( P Q PQ whee z z P : (.6 9z z (v P Q PQ Q P ( P Q PQ whee 7z z P : (.7 5z 5z
14 Q P (vi PQ PQ P Q whee z z P : (. z 9z Q P (vii PQ PQ P Q whee 5z z P : (.9 5z z 9 Q P Q P (viii PQ PQ P Q P Q whee z 5z P :. (.0 z 5z Poof. We epeatedly use the following elations of the theoy of signatue naely q f ( q Z x ( x (. q f ( q Z x ( x (. stated by Raanujan [7 p.60] poved in Bendt s book [ p.] whee x Z: Z ( q q ae elated as in Section. A geneal featue of ou poof is that each of (. (.0 is deived fo a suitable pai of identities taken fo (. (.6. Since the deivations ae siila we deonstate just two cases. Fo instance to pove (. we begin by ewiting P Q of (. as follows by epeated use of (. (.: ( ( P : (. ( (
15 ( ( Q : Q( q : P( q ( (. (. Fo (. (. we deduce that P Q ( ( ( ( (.5 Q P. (.6 Multiplying (. by obtain ( ( ( ( adding the esulting identity to (. we ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( (. (.7 Eploying (.5 (.6 in (.7 we obtain the algebaic elation (. between P Q. To pove (. ultiply (. by (. to obtain ( ( ( add the esulting identity to ( ( ( (. ( ' ( We ewite P Q of (. as follows by epeated use of (. (.: (. : ( ( ( P (.9 5
16 ( ( Q : Q( q : P( q (. (.0 Fo (.9 (.0 we deduce that P Q ' ( ( ( (. Q. (. P ' Eploying (. (. in (. we obtain the algebaic elation (. between P Q. Refeences. B. C. Bendt Raanujan s Notebooks Pat III Spinge-Velag New Yok 99.. B. C. Bendt Raanujan s Notebooks Pat IV Spinge-Velag New Yok 99.. B. C. Bendt Raanujan s Notebooks Pat V Spinge-Velag New Yok 99.. B. C. Bendt L.-C. Zhang Raanujan s identities fo eta-functions Math. Ann. 9 ( J. M. Bowein P. B. Bowien A cubic countepat of Jacobi s identity the AGM Tans. Ae. Math. Soc. ( S. Raanujan Modula equations appoxiation to π Quat J. Math. (Oxfod 5 ( S. Raanujan Notebooks ( volues Tata Institute of Fundaental Reseach Bobay S. Raanujan Collected Papes Chelsea New Yok K. Venkatachalienga Developent of Elliptic Functions Accoding to Raanujan Technical Repot Maduai Kaaaj Univesity Maduai 9. 6
Analytical Expression for Hessian
Analytical Expession fo Hessian We deive the expession of Hessian fo a binay potential the coesponding expessions wee deived in [] fo a multibody potential. In what follows, we use the convention that
Διαβάστε περισσότερα(a,b) Let s review the general definitions of trig functions first. (See back cover of your book) sin θ = b/r cos θ = a/r tan θ = b/a, a 0
TRIGONOMETRIC IDENTITIES (a,b) Let s eview the geneal definitions of tig functions fist. (See back cove of you book) θ b/ θ a/ tan θ b/a, a 0 θ csc θ /b, b 0 sec θ /a, a 0 cot θ a/b, b 0 By doing some
Διαβάστε περισσότεραSection 8.3 Trigonometric Equations
99 Section 8. Trigonometric Equations Objective 1: Solve Equations Involving One Trigonometric Function. In this section and the next, we will exple how to solving equations involving trigonometric functions.
Διαβάστε περισσότερα2 Composition. Invertible Mappings
Arkansas Tech University MATH 4033: Elementary Modern Algebra Dr. Marcel B. Finan Composition. Invertible Mappings In this section we discuss two procedures for creating new mappings from old ones, namely,
Διαβάστε περισσότεραCHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS
CHAPTER 5 SOLVING EQUATIONS BY ITERATIVE METHODS EXERCISE 104 Page 8 1. Find the positive root of the equation x + 3x 5 = 0, correct to 3 significant figures, using the method of bisection. Let f(x) =
Διαβάστε περισσότεραLaplace s Equation in Spherical Polar Coördinates
Laplace s Equation in Spheical Pola Coödinates C. W. David Dated: Januay 3, 001 We stat with the pimitive definitions I. x = sin θ cos φ y = sin θ sin φ z = cos θ thei inveses = x y z θ = cos 1 z = z cos1
Διαβάστε περισσότεραSection 7.6 Double and Half Angle Formulas
09 Section 7. Double and Half Angle Fmulas To derive the double-angles fmulas, we will use the sum of two angles fmulas that we developed in the last section. We will let α θ and β θ: cos(θ) cos(θ + θ)
Διαβάστε περισσότερα3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β
3.4 SUM AND DIFFERENCE FORMULAS Page Theorem cos(αβ cos α cos β -sin α cos(α-β cos α cos β sin α NOTE: cos(αβ cos α cos β cos(α-β cos α -cos β Proof of cos(α-β cos α cos β sin α Let s use a unit circle
Διαβάστε περισσότεραHomework 3 Solutions
Homework 3 Solutions Igor Yanovsky (Math 151A TA) Problem 1: Compute the absolute error and relative error in approximations of p by p. (Use calculator!) a) p π, p 22/7; b) p π, p 3.141. Solution: For
Διαβάστε περισσότεραFinite Field Problems: Solutions
Finite Field Problems: Solutions 1. Let f = x 2 +1 Z 11 [x] and let F = Z 11 [x]/(f), a field. Let Solution: F =11 2 = 121, so F = 121 1 = 120. The possible orders are the divisors of 120. Solution: The
Διαβάστε περισσότεραThe Neutrix Product of the Distributions r. x λ
ULLETIN u. Maaysia Math. Soc. Secod Seies 22 999 - of the MALAYSIAN MATHEMATICAL SOCIETY The Neuti Poduct of the Distibutios ad RIAN FISHER AND 2 FATMA AL-SIREHY Depatet of Matheatics ad Copute Sciece
Διαβάστε περισσότεραTrigonometry 1.TRIGONOMETRIC RATIOS
Trigonometry.TRIGONOMETRIC RATIOS. If a ray OP makes an angle with the positive direction of X-axis then y x i) Sin ii) cos r r iii) tan x y (x 0) iv) cot y x (y 0) y P v) sec x r (x 0) vi) cosec y r (y
Διαβάστε περισσότεραMatrix Hartree-Fock Equations for a Closed Shell System
atix Hatee-Fock Equations fo a Closed Shell System A single deteminant wavefunction fo a system containing an even numbe of electon N) consists of N/ spatial obitals, each occupied with an α & β spin has
Διαβάστε περισσότεραPARTIAL NOTES for 6.1 Trigonometric Identities
PARTIAL NOTES for 6.1 Trigonometric Identities tanθ = sinθ cosθ cotθ = cosθ sinθ BASIC IDENTITIES cscθ = 1 sinθ secθ = 1 cosθ cotθ = 1 tanθ PYTHAGOREAN IDENTITIES sin θ + cos θ =1 tan θ +1= sec θ 1 + cot
Διαβάστε περισσότεραAreas and Lengths in Polar Coordinates
Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the
Διαβάστε περισσότεραJesse Maassen and Mark Lundstrom Purdue University November 25, 2013
Notes on Average Scattering imes and Hall Factors Jesse Maassen and Mar Lundstrom Purdue University November 5, 13 I. Introduction 1 II. Solution of the BE 1 III. Exercises: Woring out average scattering
Διαβάστε περισσότεραAreas and Lengths in Polar Coordinates
Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the
Διαβάστε περισσότεραSrednicki Chapter 55
Srednicki Chapter 55 QFT Problems & Solutions A. George August 3, 03 Srednicki 55.. Use equations 55.3-55.0 and A i, A j ] = Π i, Π j ] = 0 (at equal times) to verify equations 55.-55.3. This is our third
Διαβάστε περισσότεραOrdinal Arithmetic: Addition, Multiplication, Exponentiation and Limit
Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit Ting Zhang Stanford May 11, 2001 Stanford, 5/11/2001 1 Outline Ordinal Classification Ordinal Addition Ordinal Multiplication Ordinal
Διαβάστε περισσότεραCoefficient Inequalities for a New Subclass of K-uniformly Convex Functions
International Journal of Computational Science and Mathematics. ISSN 0974-89 Volume, Number (00), pp. 67--75 International Research Publication House http://www.irphouse.com Coefficient Inequalities for
Διαβάστε περισσότερα4.6 Autoregressive Moving Average Model ARMA(1,1)
84 CHAPTER 4. STATIONARY TS MODELS 4.6 Autoregressive Moving Average Model ARMA(,) This section is an introduction to a wide class of models ARMA(p,q) which we will consider in more detail later in this
Διαβάστε περισσότεραω ω ω ω ω ω+2 ω ω+2 + ω ω ω ω+2 + ω ω+1 ω ω+2 2 ω ω ω ω ω ω ω ω+1 ω ω2 ω ω2 + ω ω ω2 + ω ω ω ω2 + ω ω+1 ω ω2 + ω ω+1 + ω ω ω ω2 + ω
0 1 2 3 4 5 6 ω ω + 1 ω + 2 ω + 3 ω + 4 ω2 ω2 + 1 ω2 + 2 ω2 + 3 ω3 ω3 + 1 ω3 + 2 ω4 ω4 + 1 ω5 ω 2 ω 2 + 1 ω 2 + 2 ω 2 + ω ω 2 + ω + 1 ω 2 + ω2 ω 2 2 ω 2 2 + 1 ω 2 2 + ω ω 2 3 ω 3 ω 3 + 1 ω 3 + ω ω 3 +
Διαβάστε περισσότεραCRASH COURSE IN PRECALCULUS
CRASH COURSE IN PRECALCULUS Shiah-Sen Wang The graphs are prepared by Chien-Lun Lai Based on : Precalculus: Mathematics for Calculus by J. Stuwart, L. Redin & S. Watson, 6th edition, 01, Brooks/Cole Chapter
Διαβάστε περισσότεραHOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:
HOMEWORK 4 Problem a For the fast loading case, we want to derive the relationship between P zz and λ z. We know that the nominal stress is expressed as: P zz = ψ λ z where λ z = λ λ z. Therefore, applying
Διαβάστε περισσότερα2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits.
EAMCET-. THEORY OF EQUATIONS PREVIOUS EAMCET Bits. Each of the roots of the equation x 6x + 6x 5= are increased by k so that the new transformed equation does not contain term. Then k =... - 4. - Sol.
Διαβάστε περισσότεραPractice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1
Conceptual Questions. State a Basic identity and then verify it. a) Identity: Solution: One identity is cscθ) = sinθ) Practice Exam b) Verification: Solution: Given the point of intersection x, y) of the
Διαβάστε περισσότερα4.2 Differential Equations in Polar Coordinates
Section 4. 4. Diffeential qations in Pola Coodinates Hee the two-dimensional Catesian elations of Chapte ae e-cast in pola coodinates. 4.. qilibim eqations in Pola Coodinates One wa of epesg the eqations
Διαβάστε περισσότεραC.S. 430 Assignment 6, Sample Solutions
C.S. 430 Assignment 6, Sample Solutions Paul Liu November 15, 2007 Note that these are sample solutions only; in many cases there were many acceptable answers. 1 Reynolds Problem 10.1 1.1 Normal-order
Διαβάστε περισσότεραHomomorphism in Intuitionistic Fuzzy Automata
International Journal of Fuzzy Mathematics Systems. ISSN 2248-9940 Volume 3, Number 1 (2013), pp. 39-45 Research India Publications http://www.ripublication.com/ijfms.htm Homomorphism in Intuitionistic
Διαβάστε περισσότεραSection 9.2 Polar Equations and Graphs
180 Section 9. Polar Equations and Graphs In this section, we will be graphing polar equations on a polar grid. In the first few examples, we will write the polar equation in rectangular form to help identify
Διαβάστε περισσότεραPhys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)
Phys460.nb 81 ψ n (t) is still the (same) eigenstate of H But for tdependent H. The answer is NO. 5.5.5. Solution for the tdependent Schrodinger s equation If we assume that at time t 0, the electron starts
Διαβάστε περισσότεραCongruence Classes of Invertible Matrices of Order 3 over F 2
International Journal of Algebra, Vol. 8, 24, no. 5, 239-246 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/.2988/ija.24.422 Congruence Classes of Invertible Matrices of Order 3 over F 2 Ligong An and
Διαβάστε περισσότεραInverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- -----------------
Inverse trigonometric functions & General Solution of Trigonometric Equations. 1. Sin ( ) = a) b) c) d) Ans b. Solution : Method 1. Ans a: 17 > 1 a) is rejected. w.k.t Sin ( sin ) = d is rejected. If sin
Διαβάστε περισσότεραSecond Order Partial Differential Equations
Chapter 7 Second Order Partial Differential Equations 7.1 Introduction A second order linear PDE in two independent variables (x, y Ω can be written as A(x, y u x + B(x, y u xy + C(x, y u u u + D(x, y
Διαβάστε περισσότεραUniform Convergence of Fourier Series Michael Taylor
Uniform Convergence of Fourier Series Michael Taylor Given f L 1 T 1 ), we consider the partial sums of the Fourier series of f: N 1) S N fθ) = ˆfk)e ikθ. k= N A calculation gives the Dirichlet formula
Διαβάστε περισσότεραA Note on Intuitionistic Fuzzy. Equivalence Relation
International Mathematical Forum, 5, 2010, no. 67, 3301-3307 A Note on Intuitionistic Fuzzy Equivalence Relation D. K. Basnet Dept. of Mathematics, Assam University Silchar-788011, Assam, India dkbasnet@rediffmail.com
Διαβάστε περισσότεραe t e r Cylindrical and Spherical Coordinate Representation of grad, div, curl and 2
Cylindical and Spheical Coodinate Repesentation of gad, div, cul and 2 Thus fa, we have descibed an abitay vecto in F as a linea combination of i, j and k, which ae unit vectos in the diection of inceasin,
Διαβάστε περισσότεραLecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3
Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3 1 State vector space and the dual space Space of wavefunctions The space of wavefunctions is the set of all
Διαβάστε περισσότεραOn a four-dimensional hyperbolic manifold with finite volume
BULETINUL ACADEMIEI DE ŞTIINŢE A REPUBLICII MOLDOVA. MATEMATICA Numbers 2(72) 3(73), 2013, Pages 80 89 ISSN 1024 7696 On a four-dimensional hyperbolic manifold with finite volume I.S.Gutsul Abstract. In
Διαβάστε περισσότεραIf we restrict the domain of y = sin x to [ π, π ], the restrict function. y = sin x, π 2 x π 2
Chapter 3. Analytic Trigonometry 3.1 The inverse sine, cosine, and tangent functions 1. Review: Inverse function (1) f 1 (f(x)) = x for every x in the domain of f and f(f 1 (x)) = x for every x in the
Διαβάστε περισσότεραCE 530 Molecular Simulation
C 53 olecular Siulation Lecture Histogra Reweighting ethods David. Kofke Departent of Cheical ngineering SUNY uffalo kofke@eng.buffalo.edu Histogra Reweighting ethod to cobine results taken at different
Διαβάστε περισσότεραDESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.
DESIGN OF MACHINERY SOLUTION MANUAL -7-1! PROBLEM -7 Statement: Design a double-dwell cam to move a follower from to 25 6, dwell for 12, fall 25 and dwell for the remader The total cycle must take 4 sec
Διαβάστε περισσότεραHomework 8 Model Solution Section
MATH 004 Homework Solution Homework 8 Model Solution Section 14.5 14.6. 14.5. Use the Chain Rule to find dz where z cosx + 4y), x 5t 4, y 1 t. dz dx + dy y sinx + 4y)0t + 4) sinx + 4y) 1t ) 0t + 4t ) sinx
Διαβάστε περισσότεραIf we restrict the domain of y = sin x to [ π 2, π 2
Chapter 3. Analytic Trigonometry 3.1 The inverse sine, cosine, and tangent functions 1. Review: Inverse function (1) f 1 (f(x)) = x for every x in the domain of f and f(f 1 (x)) = x for every x in the
Διαβάστε περισσότεραST5224: Advanced Statistical Theory II
ST5224: Advanced Statistical Theory II 2014/2015: Semester II Tutorial 7 1. Let X be a sample from a population P and consider testing hypotheses H 0 : P = P 0 versus H 1 : P = P 1, where P j is a known
Διαβάστε περισσότεραTridiagonal matrices. Gérard MEURANT. October, 2008
Tridiagonal matrices Gérard MEURANT October, 2008 1 Similarity 2 Cholesy factorizations 3 Eigenvalues 4 Inverse Similarity Let α 1 ω 1 β 1 α 2 ω 2 T =......... β 2 α 1 ω 1 β 1 α and β i ω i, i = 1,...,
Διαβάστε περισσότεραderivation of the Laplacian from rectangular to spherical coordinates
derivation of the Laplacian from rectangular to spherical coordinates swapnizzle 03-03- :5:43 We begin by recognizing the familiar conversion from rectangular to spherical coordinates (note that φ is used
Διαβάστε περισσότερα6.3 Forecasting ARMA processes
122 CHAPTER 6. ARMA MODELS 6.3 Forecasting ARMA processes The purpose of forecasting is to predict future values of a TS based on the data collected to the present. In this section we will discuss a linear
Διαβάστε περισσότεραSOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM
SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM Solutions to Question 1 a) The cumulative distribution function of T conditional on N n is Pr T t N n) Pr max X 1,..., X N ) t N n) Pr max
Διαβάστε περισσότεραOther Test Constructions: Likelihood Ratio & Bayes Tests
Other Test Constructions: Likelihood Ratio & Bayes Tests Side-Note: So far we have seen a few approaches for creating tests such as Neyman-Pearson Lemma ( most powerful tests of H 0 : θ = θ 0 vs H 1 :
Διαβάστε περισσότεραEvery set of first-order formulas is equivalent to an independent set
Every set of first-order formulas is equivalent to an independent set May 6, 2008 Abstract A set of first-order formulas, whatever the cardinality of the set of symbols, is equivalent to an independent
Διαβάστε περισσότεραSCITECH Volume 13, Issue 2 RESEARCH ORGANISATION Published online: March 29, 2018
Journal of rogressive Research in Mathematics(JRM) ISSN: 2395-028 SCITECH Volume 3, Issue 2 RESEARCH ORGANISATION ublished online: March 29, 208 Journal of rogressive Research in Mathematics www.scitecresearch.com/journals
Διαβάστε περισσότεραExample Sheet 3 Solutions
Example Sheet 3 Solutions. i Regular Sturm-Liouville. ii Singular Sturm-Liouville mixed boundary conditions. iii Not Sturm-Liouville ODE is not in Sturm-Liouville form. iv Regular Sturm-Liouville note
Διαβάστε περισσότεραThe Simply Typed Lambda Calculus
Type Inference Instead of writing type annotations, can we use an algorithm to infer what the type annotations should be? That depends on the type system. For simple type systems the answer is yes, and
Διαβάστε περισσότεραMath221: HW# 1 solutions
Math: HW# solutions Andy Royston October, 5 7.5.7, 3 rd Ed. We have a n = b n = a = fxdx = xdx =, x cos nxdx = x sin nx n sin nxdx n = cos nx n = n n, x sin nxdx = x cos nx n + cos nxdx n cos n = + sin
Διαβάστε περισσότεραq-analogues of Triple Series Reduction Formulas due to Srivastava and Panda with General Terms
Advances in Dynamical Systems and Applications ISSN 0973-5321, Volume 7, Numbe 1, pp 41 55 (2012 http://campusmstedu/adsa -analogues of Tiple Seies Reduction Fomulas due to Sivastava and Panda with Geneal
Διαβάστε περισσότεραFourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics
Fourier Series MATH 211, Calculus II J. Robert Buchanan Department of Mathematics Spring 2018 Introduction Not all functions can be represented by Taylor series. f (k) (c) A Taylor series f (x) = (x c)
Διαβάστε περισσότεραTrigonometric Formula Sheet
Trigonometric Formula Sheet Definition of the Trig Functions Right Triangle Definition Assume that: 0 < θ < or 0 < θ < 90 Unit Circle Definition Assume θ can be any angle. y x, y hypotenuse opposite θ
Διαβάστε περισσότεραExercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.
Exercises 0 More exercises are available in Elementary Differential Equations. If you have a problem to solve any of them, feel free to come to office hour. Problem Find a fundamental matrix of the given
Διαβάστε περισσότεραTL-Moments and L-Moments Estimation for the Generalized Pareto Distribution
Applied Mathematical Sciences, Vol. 3, 2009, no. 1, 43-52 TL-Moments L-Moments Estimation fo the Genealized Paeto Distibution Ibahim B. Abdul-Moniem Madina Highe Institute fo Management Technology Madina
Διαβάστε περισσότεραF19MC2 Solutions 9 Complex Analysis
F9MC Solutions 9 Complex Analysis. (i) Let f(z) = eaz +z. Then f is ifferentiable except at z = ±i an so by Cauchy s Resiue Theorem e az z = πi[res(f,i)+res(f, i)]. +z C(,) Since + has zeros of orer at
Διαβάστε περισσότεραSCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions
SCHOOL OF MATHEMATICAL SCIENCES GLMA Linear Mathematics 00- Examination Solutions. (a) i. ( + 5i)( i) = (6 + 5) + (5 )i = + i. Real part is, imaginary part is. (b) ii. + 5i i ( + 5i)( + i) = ( i)( + i)
Διαβάστε περισσότεραPartial Differential Equations in Biology The boundary element method. March 26, 2013
The boundary element method March 26, 203 Introduction and notation The problem: u = f in D R d u = ϕ in Γ D u n = g on Γ N, where D = Γ D Γ N, Γ D Γ N = (possibly, Γ D = [Neumann problem] or Γ N = [Dirichlet
Διαβάστε περισσότεραNowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in
Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in : tail in X, head in A nowhere-zero Γ-flow is a Γ-circulation such that
Διαβάστε περισσότεραFractional Colorings and Zykov Products of graphs
Fractional Colorings and Zykov Products of graphs Who? Nichole Schimanski When? July 27, 2011 Graphs A graph, G, consists of a vertex set, V (G), and an edge set, E(G). V (G) is any finite set E(G) is
Διαβάστε περισσότεραMATH 38061/MATH48061/MATH68061: MULTIVARIATE STATISTICS Solutions to Problems on Matrix Algebra
MATH 38061/MATH48061/MATH68061: MULTIVARIATE STATISTICS Solutios to Poblems o Matix Algeba 1 Let A be a squae diagoal matix takig the fom a 11 0 0 0 a 22 0 A 0 0 a pp The ad So, log det A t log A t log
Διαβάστε περισσότεραMathCity.org Merging man and maths
MathCity.org Merging man and maths Exercise 10. (s) Page Textbook of Algebra and Trigonometry for Class XI Available online @, Version:.0 Question # 1 Find the values of sin, and tan when: 1 π (i) (ii)
Διαβάστε περισσότεραSolution Series 9. i=1 x i and i=1 x i.
Lecturer: Prof. Dr. Mete SONER Coordinator: Yilin WANG Solution Series 9 Q1. Let α, β >, the p.d.f. of a beta distribution with parameters α and β is { Γ(α+β) Γ(α)Γ(β) f(x α, β) xα 1 (1 x) β 1 for < x
Διαβάστε περισσότεραforms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with
Week 03: C lassification of S econd- Order L inear Equations In last week s lectures we have illustrated how to obtain the general solutions of first order PDEs using the method of characteristics. We
Διαβάστε περισσότεραANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?
Teko Classes IITJEE/AIEEE Maths by SUHAAG SIR, Bhopal, Ph (0755) 3 00 000 www.tekoclasses.com ANSWERSHEET (TOPIC DIFFERENTIAL CALCULUS) COLLECTION # Question Type A.Single Correct Type Q. (A) Sol least
Διαβάστε περισσότεραConcrete Mathematics Exercises from 30 September 2016
Concrete Mathematics Exercises from 30 September 2016 Silvio Capobianco Exercise 1.7 Let H(n) = J(n + 1) J(n). Equation (1.8) tells us that H(2n) = 2, and H(2n+1) = J(2n+2) J(2n+1) = (2J(n+1) 1) (2J(n)+1)
Διαβάστε περισσότερα2. Μηχανικό Μαύρο Κουτί: κύλινδρος με μια μπάλα μέσα σε αυτόν.
Experiental Copetition: 14 July 011 Proble Page 1 of. Μηχανικό Μαύρο Κουτί: κύλινδρος με μια μπάλα μέσα σε αυτόν. Ένα μικρό σωματίδιο μάζας (μπάλα) βρίσκεται σε σταθερή απόσταση z από το πάνω μέρος ενός
Διαβάστε περισσότεραStatistical Inference I Locally most powerful tests
Statistical Inference I Locally most powerful tests Shirsendu Mukherjee Department of Statistics, Asutosh College, Kolkata, India. shirsendu st@yahoo.co.in So far we have treated the testing of one-sided
Διαβάστε περισσότεραReminders: linear functions
Reminders: linear functions Let U and V be vector spaces over the same field F. Definition A function f : U V is linear if for every u 1, u 2 U, f (u 1 + u 2 ) = f (u 1 ) + f (u 2 ), and for every u U
Διαβάστε περισσότεραCHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS
CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS EXERCISE 01 Page 545 1. Use matrices to solve: 3x + 4y x + 5y + 7 3x + 4y x + 5y 7 Hence, 3 4 x 0 5 y 7 The inverse of 3 4 5 is: 1 5 4 1 5 4 15 8 3
Διαβάστε περισσότεραMatrices and Determinants
Matrices and Determinants SUBJECTIVE PROBLEMS: Q 1. For what value of k do the following system of equations possess a non-trivial (i.e., not all zero) solution over the set of rationals Q? x + ky + 3z
Διαβάστε περισσότεραDerivations of Useful Trigonometric Identities
Derivations of Useful Trigonometric Identities Pythagorean Identity This is a basic and very useful relationship which comes directly from the definition of the trigonometric ratios of sine and cosine
Διαβάστε περισσότεραThe Laplacian in Spherical Polar Coordinates
Univesity of Connecticut DigitalCommons@UConn Chemisty Education Mateials Depatment of Chemisty -6-007 The Laplacian in Spheical Pola Coodinates Cal W. David Univesity of Connecticut, Cal.David@uconn.edu
Διαβάστε περισσότεραSpace Physics (I) [AP-3044] Lecture 1 by Ling-Hsiao Lyu Oct Lecture 1. Dipole Magnetic Field and Equations of Magnetic Field Lines
Space Physics (I) [AP-344] Lectue by Ling-Hsiao Lyu Oct. 2 Lectue. Dipole Magnetic Field and Equations of Magnetic Field Lines.. Dipole Magnetic Field Since = we can define = A (.) whee A is called the
Διαβάστε περισσότεραΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 6/5/2006
Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Ολοι οι αριθμοί που αναφέρονται σε όλα τα ερωτήματα είναι μικρότεροι το 1000 εκτός αν ορίζεται διαφορετικά στη διατύπωση του προβλήματος. Διάρκεια: 3,5 ώρες Καλή
Διαβάστε περισσότερα6.1. Dirac Equation. Hamiltonian. Dirac Eq.
6.1. Dirac Equation Ref: M.Kaku, Quantum Field Theory, Oxford Univ Press (1993) η μν = η μν = diag(1, -1, -1, -1) p 0 = p 0 p = p i = -p i p μ p μ = p 0 p 0 + p i p i = E c 2 - p 2 = (m c) 2 H = c p 2
Διαβάστε περισσότεραOn mixing generalized poison with Generalized Gamma distribution
34 WALFORD I.E. CHUKWU(*) and DEVENDRA GUPTA (**) On mixing genealized poison with Genealized Gamma distibution CONTENTS: Intoduction Mixtue. Refeences. Summay. Riassunto. Key wods (*) Walfod I.E. Chukwu
Διαβάστε περισσότεραStrain gauge and rosettes
Strain gauge and rosettes Introduction A strain gauge is a device which is used to measure strain (deformation) on an object subjected to forces. Strain can be measured using various types of devices classified
Διαβάστε περισσότεραΤΕΧΝΟΛΟ ΓΙ ΚΟ ΕΚΠΑ ΙΔ ΕΥ Τ ΙΚΟ Ι ΔΡΥ Μ Α 'ΠΕ Ι ΡΑ ΙΑ ΤΜΗΜΑ ΚΛΩΣΤΟΥΦΑΝΤΟΥΡΓΙΑΣ ΕΙΔΙΚΟΤΗΤΑ ΒΑΦΙΚΗΣ ΠΤΥΧΙΑΚΉ ΕΡΓ ΑΣΙΑ ΤΙΤΛΟΣ ΕΥΧΡΗΣΤΙΑ ΕΞΕΙΔΙΚΕΥΜΕΝΟΥ
515 ΤΕΧΝΟΛΟ ΓΙ ΚΟ ΕΚΠΑ ΙΔ ΕΥ Τ ΙΚΟ Ι ΔΡΥ Μ Α 'ΠΕ Ι ΡΑ ΙΑ ~ " ΤΜΗΜΑ ΚΛΩΣΤΟΥΦΑΝΤΟΥΡΓΙΑΣ ΕΙΔΙΚΟΤΗΤΑ ΒΑΦΙΚΗΣ ΠΤΥΧΙΑΚΉ ΕΡΓ ΑΣΙΑ ΤΙΤΛΟΣ ΕΥΧΡΗΣΤΙΑ ΕΞΕΙΔΙΚΕΥΜΕΝΟΥ ΠΡΟΣΤΑΤΕΥΤΙΚΟΥ ΙΜΑΤΙΣΜΟΥ ΑΡΓΥΡΟΠΟΥ ΛΟΣ ΘΕΜΙΣΤΟΚΛΗΣ
Διαβάστε περισσότεραSection 7.7 Product-to-Sum and Sum-to-Product Formulas
Section 7.7 Product-to-Sum and Sum-to-Product Fmulas Objective 1: Express Products as Sums To derive the Product-to-Sum Fmulas will begin by writing down the difference and sum fmulas of the cosine function:
Διαβάστε περισσότεραSecond Order RLC Filters
ECEN 60 Circuits/Electronics Spring 007-0-07 P. Mathys Second Order RLC Filters RLC Lowpass Filter A passive RLC lowpass filter (LPF) circuit is shown in the following schematic. R L C v O (t) Using phasor
Διαβάστε περισσότεραΝέος Αναπτυξιακός Νόµος - Επενδυτικός Νόµος 3299/2004
Νέος Αναπτυξιακός Νόµος - Επενδυτικός Νόµος 3299/2004 Business Unit: CON No of Pages: 10 Authors: AR Use: External Info Date: 17/09/2007 Τηλ.: 210 6545340, Fax: 210 6545342 email: info@abele.gr - www.abele.gr
Διαβάστε περισσότεραΔΙΑΤΜΗΜΑΤΙΚΟ ΠΡΟΓΡΑΜΜΑ ΜΕΤΑΠΤΥΧΙΑΚΩΝ ΣΠΟΥΔΩΝ ΣΤΗ ΔΙΟΙΚΗΣΗ ΕΠΙΧΕΙΡΗΣΕΩΝ ΘΕΜΕΛΙΩΔΗΣ ΚΛΑΔΙΚΗ ΑΝΑΛΥΣΗ ΤΩΝ ΕΙΣΗΓΜΕΝΩΝ ΕΠΙΧΕΙΡΗΣΕΩΝ ΤΗΣ ΕΛΛΗΝΙΚΗΣ ΑΓΟΡΑΣ
ΔΙΑΤΜΗΜΑΤΙΚΟ ΠΡΟΓΡΑΜΜΑ ΜΕΤΑΠΤΥΧΙΑΚΩΝ ΣΠΟΥΔΩΝ ΣΤΗ ΔΙΟΙΚΗΣΗ ΕΠΙΧΕΙΡΗΣΕΩΝ Διπλωματική Εργασία ΘΕΜΕΛΙΩΔΗΣ ΚΛΑΔΙΚΗ ΑΝΑΛΥΣΗ ΤΩΝ ΕΙΣΗΓΜΕΝΩΝ ΕΠΙΧΕΙΡΗΣΕΩΝ ΤΗΣ ΕΛΛΗΝΙΚΗΣ ΑΓΟΡΑΣ Του ΚΩΣΤΟΥΛΗ ΔΗΜΗΤΡΙΟΥ ΤΟΥ ΒΑΣΙΛΕΙΟΥ
Διαβάστε περισσότεραEE512: Error Control Coding
EE512: Error Control Coding Solution for Assignment on Finite Fields February 16, 2007 1. (a) Addition and Multiplication tables for GF (5) and GF (7) are shown in Tables 1 and 2. + 0 1 2 3 4 0 0 1 2 3
Διαβάστε περισσότερα9.09. # 1. Area inside the oval limaçon r = cos θ. To graph, start with θ = 0 so r = 6. Compute dr
9.9 #. Area inside the oval limaçon r = + cos. To graph, start with = so r =. Compute d = sin. Interesting points are where d vanishes, or at =,,, etc. For these values of we compute r:,,, and the values
Διαβάστε περισσότεραApproximation of distance between locations on earth given by latitude and longitude
Approximation of distance between locations on earth given by latitude and longitude Jan Behrens 2012-12-31 In this paper we shall provide a method to approximate distances between two points on earth
Διαβάστε περισσότεραD Alembert s Solution to the Wave Equation
D Alembert s Solution to the Wave Equation MATH 467 Partial Differential Equations J. Robert Buchanan Department of Mathematics Fall 2018 Objectives In this lesson we will learn: a change of variable technique
Διαβάστε περισσότεραΗ ΣΥΝΘΕΣΗ ΚΑΙ ΤΑ ΣΥΝΘΕΤΑ ΝΟΗΜΑΤΑ ΣΤΗΝ ΕΛΛΗΝΙΚΗ ΝΟΗΜΑΤΙΚΗ ΓΛΩΣΣΑ
ΠΑΝΕΠΙΣΤΗΜΙΟ ΠΑΤΡΩΝ Σχολή Ανθρωπιστικών & Κοινωνικών Επιστημών Παιδαγωγικό Τμήμα Δημοτικής Εκπαίδευσης ΤΙΤΛΟΣ ΔΙΔΑΚΤΟΡΙΚΗΣ ΔΙΑΤΡΙΒΗΣ Η ΣΥΝΘΕΣΗ ΚΑΙ ΤΑ ΣΥΝΘΕΤΑ ΝΟΗΜΑΤΑ ΣΤΗΝ ΕΛΛΗΝΙΚΗ ΝΟΗΜΑΤΙΚΗ ΓΛΩΣΣΑ ΕΙΡΗΝΗ
Διαβάστε περισσότεραΑπόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.
Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο The time integral of a force is referred to as impulse, is determined by and is obtained from: Newton s 2 nd Law of motion states that the action
Διαβάστε περισσότεραMock Exam 7. 1 Hong Kong Educational Publishing Company. Section A 1. Reference: HKDSE Math M Q2 (a) (1 + kx) n 1M + 1A = (1) =
Mock Eam 7 Mock Eam 7 Section A. Reference: HKDSE Math M 0 Q (a) ( + k) n nn ( )( k) + nk ( ) + + nn ( ) k + nk + + + A nk... () nn ( ) k... () From (), k...() n Substituting () into (), nn ( ) n 76n 76n
Διαβάστε περισσότεραSOLVING CUBICS AND QUARTICS BY RADICALS
SOLVING CUBICS AND QUARTICS BY RADICALS The purpose of this handout is to record the classical formulas expressing the roots of degree three and degree four polynomials in terms of radicals. We begin with
Διαβάστε περισσότεραExistence and Nonexistence of Weak Positive Solution for Classes of 3 3 P-Laplacian Elliptic Systems
Intenational Jounal of Patial Diffeential Euations Alications 03 Vol. No. 3-7 Aailable online at htt://ubs.scieub.co/ijdea///3 Science Education Publishing DOI:0.69/ijdea---3 Existence Nonexistence of
Διαβάστε περισσότερα( )( ) ( ) ( )( ) ( )( ) β = Chapter 5 Exercise Problems EX α So 49 β 199 EX EX EX5.4 EX5.5. (a)
hapter 5 xercise Problems X5. α β α 0.980 For α 0.980, β 49 0.980 0.995 For α 0.995, β 99 0.995 So 49 β 99 X5. O 00 O or n 3 O 40.5 β 0 X5.3 6.5 μ A 00 β ( 0)( 6.5 μa) 8 ma 5 ( 8)( 4 ) or.88 P on + 0.0065
Διαβάστε περισσότεραw o = R 1 p. (1) R = p =. = 1
Πανεπιστήµιο Κρήτης - Τµήµα Επιστήµης Υπολογιστών ΗΥ-570: Στατιστική Επεξεργασία Σήµατος 205 ιδάσκων : Α. Μουχτάρης Τριτη Σειρά Ασκήσεων Λύσεις Ασκηση 3. 5.2 (a) From the Wiener-Hopf equation we have:
Διαβάστε περισσότεραLecture 15 - Root System Axiomatics
Lecture 15 - Root System Axiomatics Nov 1, 01 In this lecture we examine root systems from an axiomatic point of view. 1 Reflections If v R n, then it determines a hyperplane, denoted P v, through the
Διαβάστε περισσότερα