Existence and Nonexistence of Weak Positive Solution for Classes of 3 3 P-Laplacian Elliptic Systems

Μέγεθος: px
Εμφάνιση ξεκινά από τη σελίδα:

Download "Existence and Nonexistence of Weak Positive Solution for Classes of 3 3 P-Laplacian Elliptic Systems"

Transcript

1 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 Weak Positie Solution fo Classes of 3 3 P-Lalacian Ellitic Systes Guefaifia Rafik Akout Kael * Saifia Wada LAMIS Laboatoy Tebessa Uniesity Tebessa Algeia LANOS Laboatoy Badji Mokhta Uniesity Annaba Algeia *Coesonding autho: akoutkael@gail.co Receied Noebe 03; Reised Noebe 9 03; Acceted Decebe 3 03 Abstact In this ok e ae inteested to obtain soe esult of existence nonexistence of lage ositie u = α x f u in u = µβ ( x g ( u in eak solution fo the folloing -lalacian syste hee = νγ ( x h ( u in u = = = 0 on σ σ z = di z z σ µ ν ae a ositie aaete is a bounded doain in N ith sooth bounday. The oof of the ain esults is based to the sub-suesolutions ethod. Keyods: Positie solutions Sub-suesolutions -Lalacian systes Cite This Aticle: Guefaifia Rafik Akout Kael Saifia Wada Existence Nonexistence of Weak Positie Solution fo Classes of 3 3 P-Lalacian Ellitic Systes. Intenational Jounal of Patial Diffeential Euations Alications no. (03: 3-7. doi: 0.69/ijdea Intoduction Pobles inoling the -Lalacian aise fo any banches of ue athe-atics as in the theoy of uasiegula uasiconfoal aing as ell as fo aious obles in atheatical hysics notably the flo of non-netonian fluids. Hai Shiaji [9] studied the existence of ositie solution fo the -Lalacian syste u = f in = g u in u = = 0 on (. hich f(s; g(s ae the inceasing functions in [0 satisfy M( gs li f = 0 M > 0 s + S the authos shoed that the oble (. has at least one ositie solution oided that > 0 is lage enough. In [6] the autho studied the existence nonexistence of ositie eak solution to the folloing uasilinea ellitic syste α γ u = u in δ β u = u in u = = 0 on (. The fist eigenfunction is used to constuct the subsolution of oble (.3 the ain esults ae as follos: (i If α β 0 γ δ > 0 θ = ( α (( β γδ > 0 then oble (.3 has a ositie eak solution fo each k > 0; (ii If = 0 γ= ( α then thee exists 0 > 0 such that fo 0 < < 0 then oble (.3 has no nontiial nonnegatie eak solution. In this ae e ae concened ith the existence nonexistence of ositie eak solution to the uasilinea ellitic syste u = α x f u in = µβ x g u in = νγ x h u in u = = = 0 on σ hee z di ( z σ z (.3 = σ µ ν ae a ositie aaete is a bounded doain in

2 4 Intenational Jounal of Patial Diffeential Euations Alications N ith sooth bounday. We oe the existence of a lage ositie eak solution fo µ ν lage hen ( ( ( f ttt gttt httt li 0 t t = t = + t =. Definitions Notations Definition. We called ositie eak solution (u; ; of (.3 such that satisfies u u. = α( x f ( u u. ω dx = µ β( x g ( u u3. = γ ( x h( u fo all ω Η 0 ( ith ω 0 Definition. We called ositie eak subsolution ( 3 suesolution (z z z 3 of (.3 such that i zi i= 3 satisfies 3. α x f 3. ω dx µ β x g γ x h z z. α( x f ( z z z3 z z. ω dx µ β( x g ( z z z3 z3 z3. γ ( x h( z z z3 fo all Η 0 ( ith 0. We suose that α β γ f g h eify the folloing assutions; (H f gh : ([ 0 [ ae C onotone functions such that = li f t t t3 li g t t t3 t t t3 + t t t3 + = li ht ( t t3 = + t t t3 + k0 > 0: f yz g yz h yz k0 fo all yz 0 ( x ( x ( x α0 α α α0 β0 γ0 α β γ > 0: β0 β β γ0 γ γ ( ( ( f ttt gttt httt (H li 0 t t = t = + t = ξ ξ ξ3 η η η3 3 > 0: f ( t t t3 ξt ηt t (H3 g( t t t3 ξt ηt t ht ( t t3 ξ3t + η3t + 33 t Let µ ν be the fist eigenalue of ith Diichlet bounday conditions the coesonding ositie eigenfunction ith = = = δ > 0 such that on δ = x d x µ { : ( δ} We denote by ( ( ( ( ( ( µ ξ η ξ ξ 0 = ( µ 0 = + ( µ η ξ η η µ 0 = + + ( ξ3 + η Existence Results Theoe. Let (H (H hold. Then fo lage the syste (.3 has a lage ositie solution (u : Poof. We shall eify that α = µβ = γ 3 = is a subsolution of (.3 fo lage: Let ω ω 0.A calculation shos that ω dx = H 0 ith k0 = dx σ σ σ ω k 0 σ σ ( σ ω dx = σ k0 = ( σ σ.

3 Intenational Jounal of Patial Diffeential Euations Alications 5 No on σ e hae α 3 α β γ ( x f ( ( α α( x 3 ( x f ( µ β ( β β( x ( γ ( x f ( 3 ( γ γ ( x Next on / σ e hae ρ fo soe ρ 0 theefoe fo µ ν lage f ( 3 g ( 3 µ µ ( 3 ( h Hence 3. f 3. ω dx µ g h i.e. ( 3 is a subsolution of (.3. Next let ae the solution of = in = in = in = 0 on. = 0 on. = 0 on. Let C z = z = µ g z3 = h Whee C > 0 is a lage nube to be chosen late: We shall eify that (z z z 3 is a suesolution of (.3 fo µ ν lage. To this end let ω H 0 ( ith ω 0. By (H (H e can choose C lage enough so that then g C C C µ µ g = z z h h = z3 then z3 hich ily that f C C C C f C C C f C C f ( z z z3 = Then e hae z z. C = C = f ( z z z3

4 6 Intenational Jounal of Patial Diffeential Euations Alications in anothe h z z. = µ g. C µ g ( µ g z z z siila z z. = h. C h ( h z z z 3 i.e (z z z 3 is a suesolution of (.3 ith z i i fo C lage i = 3. Thus thee exists a solution (u of (.3 ith u z z 3 ω z3. 4. Nonexistence Results Theoe. If f g h eify (H 3 the syste (.3 has not nontiial ositie solutions fo 0 < 0 < 0< µ 0 < µ 0 < 0 <. (4. Poof. Multilying the fist euation by u; e hae fo Young ineuality that u ( = f u udx ξ u + η + udx ( η ξ u u u dx η + ( ( ( ξ η + η + ξ + u + η + dx = + + u then e hae ( ( u ( ξ +η+ u + η + ( µ µ ξ u + ( ξ + η + µ + ( ( ( ξ 3 u + η Note that u = inf inf u inf = µ = ( ξ η Cobining (4. (4.3 e obtain ( ( µ µ 0 u (4. (4.3 hich is a contadiction if (4. hold. Thus (.3 has no nontiial nonnegatie eak solution. 5. Alications P Theoe 3. conside the folloing syste in W ( n l u = u in n l = µ u in 3 n3 l3 = u in u = = = 0 on the syste has a lage ositie solutions if In the case hee + n+ l < + n + l < 3 + n3 + l3 < ( + n+ l = + n + l = 3 + n3 + l3 = the syste has not non tiial ositie solutions if 0 (5. (5. (5.3 0 < < 0< µ < µ 0 < <. (5.4 Poof. (5. ily that (H. By using theoe the syste has a lage ositie solutions. The fist euation in (5.3 ily that + + = + + = 3 n l θ θ θ then the genealized Young ineuality gies (5.5

5 Intenational Jounal of Patial Diffeential Euations Alications 7 n l n lθ 3 f ( u = u θ u + θ + θ θ θ3 = u + + θ θ θ3 By the sae anne e conclude that the assution (H3 holds. Then he syste (5. has not nontiial ositie solutions if hich ily that 0 = ( ( < µ 0 = ( n+ ( n + + n3 < µ µ µ 0 = ( l+ µ l + l ( 3 + <. ( ( µ µ + + < (5.6 0 this ineuality hold if (5.4 hold. Theoe 4. The folloing oble has a lage ositie solution if lage 3 3 u x H u u u in = γ u = u = u = 0 on (5.7 hee is a bounded doain in N ith sooth bounday is a ositie aaete γ is a function of class L ( : ([ 0 [ 3 ( 3 ( H is of class C H t t t is inceasing ith esect to t t 3 H t t t 3 is deceasing ith esect to t ( H t t t li = 0 > + t t ([ [ k > 0: H t t t k t t t Poof. The oble (5.7 can be itten unde the folloing syste fo u = in = in = γ ( x H ( u in u = = = 0 on In this case the assutions of theoe (3. holds. Refeences [] S. Ala G. A. Afouzi Q. Zhang & A. Nikna Existence of ositie solutions fo aiable exonent ellitic systes Bounday Value Pobles 0 0:37. [] G. A. Afouzi & J. Vahidi On citical exonent fo the existence stability oeties of ositie eak solutions fo soe nonlinea ellitic systes inoling the ( -Lalacian indefinite eight function Poc. Indian Acad. Sci. (Math. Sci. Vol. No. Febuay [3] G. A. Afouzi & Z. Valinejad Nonexistence of esult fo soe - Lalacian Systes The Jounal of Matheatics Coute Science Vol. 3 No. (0-6. [4] J. Ali R. Shiaji Existence esults fo classes of Lalacian systes ith sign-changing eight Alied Matheatics Lettes 0 ( [5] J. Ali R. Shiaji Positie solutions fo a class of -Lalacian systes ith ultile aaetes J. Math. Anal. Al. 335 ( s [6] C. Chen On ositie eak solutions fo a class of uasilinea ellitic systes Nonlinea Analysis 6 ( [7] R. Dalasso Existence uniueness of ositie solutions of seilinea ellitic systes Nonlinea Analysis 39 ( [8] H. Dang S. Ouganti & R. Shiaji nonexistence of non ositie solutions fo a class of seilinea ellitic systes Rocky Mountain Jounal of atheatics Volue 36 Nube [9] D. D. Hai R. Shiaji An existence esult on ositie solutions fo a class of -Lalacian systes Nonlinea Analysis 56 ( [0] P. Dˆabek & J. Hen ez Existence uniueness of ositie solutions fo soe uasilinea ellitic obles Nonlinea Analysis 44 (00. [] S. Haghaieghi & G. A. Afouzi Sub-sue solutions fo (- Lalacian systes Bounday Value Pobles 0 0:5. [] R. Shiaji a & J. Ye Nonexistence esults fo classes of 3 3 ellitic systes Nonlinea Analysis 74 (

Example Sheet 3 Solutions

Example 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 περισσότερα

Laplace s Equation in Spherical Polar Coördinates

Laplace 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 περισσότερα

2 Composition. Invertible Mappings

2 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 περισσότερα

Finite Field Problems: Solutions

Finite 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 περισσότερα

Congruence Classes of Invertible Matrices of Order 3 over F 2

Congruence 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 περισσότερα

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

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 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

Διαβάστε περισσότερα

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

SOLUTIONS 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 περισσότερα

Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit

Ordinal 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 περισσότερα

The Pohozaev identity for the fractional Laplacian

The Pohozaev identity for the fractional Laplacian The Pohozaev identity for the fractional Laplacian Xavier Ros-Oton Departament Matemàtica Aplicada I, Universitat Politècnica de Catalunya (joint work with Joaquim Serra) Xavier Ros-Oton (UPC) The Pohozaev

Διαβάστε περισσότερα

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS

CHAPTER 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 περισσότερα

Statistical Inference I Locally most powerful tests

Statistical 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 περισσότερα

Example 1: THE ELECTRIC DIPOLE

Example 1: THE ELECTRIC DIPOLE Example 1: THE ELECTRIC DIPOLE 1 The Electic Dipole: z + P + θ d _ Φ = Q 4πε + Q = Q 4πε 4πε 1 + 1 2 The Electic Dipole: d + _ z + Law of Cosines: θ A B α C A 2 = B 2 + C 2 2ABcosα P ± = 2 ( + d ) 2 2

Διαβάστε περισσότερα

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

SOLUTIONS 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 περισσότερα

Inverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- -----------------

Inverse 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 περισσότερα

6.3 Forecasting ARMA processes

6.3 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 περισσότερα

Space 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-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 περισσότερα

Uniform Convergence of Fourier Series Michael Taylor

Uniform 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 περισσότερα

Section 8.3 Trigonometric Equations

Section 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 περισσότερα

Matrices and Determinants

Matrices 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 περισσότερα

Areas and Lengths in Polar Coordinates

Areas 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 περισσότερα

Areas and Lengths in Polar Coordinates

Areas 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 περισσότερα

Solutions to Exercise Sheet 5

Solutions to Exercise Sheet 5 Solutions to Eercise Sheet 5 jacques@ucsd.edu. Let X and Y be random variables with joint pdf f(, y) = 3y( + y) where and y. Determine each of the following probabilities. Solutions. a. P (X ). b. P (X

Διαβάστε περισσότερα

C.S. 430 Assignment 6, Sample Solutions

C.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 περισσότερα

Other Test Constructions: Likelihood Ratio & Bayes Tests

Other 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 περισσότερα

Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8 questions or comments to Dan Fetter 1

Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8  questions or comments to Dan Fetter 1 Eon : Fall 8 Suggested Solutions to Problem Set 8 Email questions or omments to Dan Fetter Problem. Let X be a salar with density f(x, θ) (θx + θ) [ x ] with θ. (a) Find the most powerful level α test

Διαβάστε περισσότερα

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions

SCHOOL 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 περισσότερα

D Alembert s Solution to the Wave Equation

D 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 περισσότερα

Every set of first-order formulas is equivalent to an independent set

Every 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 περισσότερα

Takeaki Yamazaki (Toyo Univ.) 山崎丈明 ( 東洋大学 ) Oct. 24, RIMS

Takeaki Yamazaki (Toyo Univ.) 山崎丈明 ( 東洋大学 ) Oct. 24, RIMS Takeaki Yamazaki (Toyo Univ.) 山崎丈明 ( 東洋大学 ) Oct. 24, 2017 @ RIMS Contents Introduction Generalized Karcher equation Ando-Hiai inequalities Problem Introduction PP: The set of all positive definite operators

Διαβάστε περισσότερα

Solution Series 9. i=1 x i and i=1 x i.

Solution 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 περισσότερα

ORDINAL ARITHMETIC JULIAN J. SCHLÖDER

ORDINAL ARITHMETIC JULIAN J. SCHLÖDER ORDINAL ARITHMETIC JULIAN J. SCHLÖDER Abstract. We define ordinal arithmetic and show laws of Left- Monotonicity, Associativity, Distributivity, some minor related properties and the Cantor Normal Form.

Διαβάστε περισσότερα

Homework 3 Solutions

Homework 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 περισσότερα

Intuitionistic Fuzzy Ideals of Near Rings

Intuitionistic Fuzzy Ideals of Near Rings International Mathematical Forum, Vol. 7, 202, no. 6, 769-776 Intuitionistic Fuzzy Ideals of Near Rings P. K. Sharma P.G. Department of Mathematics D.A.V. College Jalandhar city, Punjab, India pksharma@davjalandhar.com

Διαβάστε περισσότερα

ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?

ANSWERSHEET (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 περισσότερα

CE 530 Molecular Simulation

CE 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 περισσότερα

EE512: Error Control Coding

EE512: 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 περισσότερα

ST5224: Advanced Statistical Theory II

ST5224: 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 περισσότερα

4.6 Autoregressive Moving Average Model ARMA(1,1)

4.6 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 περισσότερα

Lecture 21: Properties and robustness of LSE

Lecture 21: Properties and robustness of LSE Lecture 21: Properties and robustness of LSE BLUE: Robustness of LSE against normality We now study properties of l τ β and σ 2 under assumption A2, i.e., without the normality assumption on ε. From Theorem

Διαβάστε περισσότερα

Second Order RLC Filters

Second 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 περισσότερα

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)

Phys460.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 περισσότερα

Global nonlinear stability of steady solutions of the 3-D incompressible Euler equations with helical symmetry and with no swirl

Global nonlinear stability of steady solutions of the 3-D incompressible Euler equations with helical symmetry and with no swirl Around Vortices: from Cont. to Quantum Mech. Global nonlinear stability of steady solutions of the 3-D incompressible Euler equations with helical symmetry and with no swirl Maicon José Benvenutti (UNICAMP)

Διαβάστε περισσότερα

The ε-pseudospectrum of a Matrix

The ε-pseudospectrum of a Matrix The ε-pseudospectrum of a Matrix Feb 16, 2015 () The ε-pseudospectrum of a Matrix Feb 16, 2015 1 / 18 1 Preliminaries 2 Definitions 3 Basic Properties 4 Computation of Pseudospectrum of 2 2 5 Problems

Διαβάστε περισσότερα

Tridiagonal matrices. Gérard MEURANT. October, 2008

Tridiagonal 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 περισσότερα

Homework 8 Model Solution Section

Homework 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 περισσότερα

forms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with

forms 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 περισσότερα

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

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 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 περισσότερα

DESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.

DESIGN 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 περισσότερα

Απόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.

Απόκριση 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 περισσότερα

Lecture 26: Circular domains

Lecture 26: Circular domains Introductory lecture notes on Partial Differential Equations - c Anthony Peirce. Not to be copied, used, or revised without eplicit written permission from the copyright owner. 1 Lecture 6: Circular domains

Διαβάστε περισσότερα

Math 446 Homework 3 Solutions. (1). (i): Reverse triangle inequality for metrics: Let (X, d) be a metric space and let x, y, z X.

Math 446 Homework 3 Solutions. (1). (i): Reverse triangle inequality for metrics: Let (X, d) be a metric space and let x, y, z X. Math 446 Homework 3 Solutions. (1). (i): Reverse triangle inequalit for metrics: Let (X, d) be a metric space and let x,, z X. Prove that d(x, z) d(, z) d(x, ). (ii): Reverse triangle inequalit for norms:

Διαβάστε περισσότερα

Fourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics

Fourier 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 περισσότερα

POSITIVE SOLUTIONS FOR A FUNCTIONAL DELAY SECOND-ORDER THREE-POINT BOUNDARY-VALUE PROBLEM

POSITIVE SOLUTIONS FOR A FUNCTIONAL DELAY SECOND-ORDER THREE-POINT BOUNDARY-VALUE PROBLEM Electronic Journal of Differential Equations, Vol. 26(26, No. 4, pp.. ISSN: 72-669. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp POSITIVE SOLUTIONS

Διαβάστε περισσότερα

Lecture 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 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 περισσότερα

Math221: HW# 1 solutions

Math221: 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 περισσότερα

SOME PROPERTIES OF FUZZY REAL NUMBERS

SOME PROPERTIES OF FUZZY REAL NUMBERS Sahand Communications in Mathematical Analysis (SCMA) Vol. 3 No. 1 (2016), 21-27 http://scma.maragheh.ac.ir SOME PROPERTIES OF FUZZY REAL NUMBERS BAYAZ DARABY 1 AND JAVAD JAFARI 2 Abstract. In the mathematical

Διαβάστε περισσότερα

Coefficient Inequalities for a New Subclass of K-uniformly Convex Functions

Coefficient 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 περισσότερα

Homomorphism of Intuitionistic Fuzzy Groups

Homomorphism of Intuitionistic Fuzzy Groups International Mathematical Forum, Vol. 6, 20, no. 64, 369-378 Homomorphism o Intuitionistic Fuzz Groups P. K. Sharma Department o Mathematics, D..V. College Jalandhar Cit, Punjab, India pksharma@davjalandhar.com

Διαβάστε περισσότερα

Product of two generalized pseudo-differential operators involving fractional Fourier transform

Product of two generalized pseudo-differential operators involving fractional Fourier transform J. Pseudo-Diffe. Ope. Appl. 2011 2:355 365 DOI 10.1007/s11868-011-0034-5 Poduct of two genealized pseudo-diffeential opeatos involving factional Fouie tansfom Akhilesh Pasad Manish Kuma eceived: 21 Febuay

Διαβάστε περισσότερα

17 Monotonicity Formula And Basic Consequences

17 Monotonicity Formula And Basic Consequences Lectues o Vaifols Leo Sio Zhag Zui 7 Mootoicity Foula A Basic Cosequeces I this sectio we assue that U is oe i R, V v( M,θ) has the geealize ea cuvatue H i U ( see 6.5), a we wite µ fo µ V ( H θ as i 5.).

Διαβάστε περισσότερα

EE101: Resonance in RLC circuits

EE101: Resonance in RLC circuits EE11: Resonance in RLC circuits M. B. Patil mbatil@ee.iitb.ac.in www.ee.iitb.ac.in/~sequel Deartment of Electrical Engineering Indian Institute of Technology Bombay I V R V L V C I = I m = R + jωl + 1/jωC

Διαβάστε περισσότερα

Chapter 6: Systems of Linear Differential. be continuous functions on the interval

Chapter 6: Systems of Linear Differential. be continuous functions on the interval Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations

Διαβάστε περισσότερα

Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1

Practice 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 περισσότερα

Second Order Partial Differential Equations

Second 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 περισσότερα

( y) Partial Differential Equations

( y) Partial Differential Equations Partial Dierential Equations Linear P.D.Es. contains no owers roducts o the deendent variables / an o its derivatives can occasionall be solved. Consider eamle ( ) a (sometimes written as a ) we can integrate

Διαβάστε περισσότερα

Approximation of distance between locations on earth given by latitude and longitude

Approximation 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 περισσότερα

Tutorial Note - Week 09 - Solution

Tutorial Note - Week 09 - Solution Tutoial Note - Week 9 - Solution ouble Integals in Pola Coodinates. a Since + and + 5 ae cicles centeed at oigin with adius and 5, then {,θ 5, θ π } Figue. f, f cos θ, sin θ cos θ sin θ sin θ da 5 69 5

Διαβάστε περισσότερα

SCITECH Volume 13, Issue 2 RESEARCH ORGANISATION Published online: March 29, 2018

SCITECH 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 περισσότερα

The Laplacian in Spherical Polar Coordinates

The 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 περισσότερα

Mean-Variance Analysis

Mean-Variance Analysis Mean-Variance Analysis Jan Schneider McCombs School of Business University of Texas at Austin Jan Schneider Mean-Variance Analysis Beta Representation of the Risk Premium risk premium E t [Rt t+τ ] R1

Διαβάστε περισσότερα

Iterated trilinear fourier integrals with arbitrary symbols

Iterated trilinear fourier integrals with arbitrary symbols Cornell University ICM 04, Satellite Conference in Harmonic Analysis, Chosun University, Gwangju, Korea August 6, 04 Motivation the Coifman-Meyer theorem with classical paraproduct(979) B(f, f )(x) :=

Διαβάστε περισσότερα

5. Choice under Uncertainty

5. Choice under Uncertainty 5. Choice under Uncertainty Daisuke Oyama Microeconomics I May 23, 2018 Formulations von Neumann-Morgenstern (1944/1947) X: Set of prizes Π: Set of probability distributions on X : Preference relation

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

(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 περισσότερα

2. Let H 1 and H 2 be Hilbert spaces and let T : H 1 H 2 be a bounded linear operator. Prove that [T (H 1 )] = N (T ). (6p)

2. Let H 1 and H 2 be Hilbert spaces and let T : H 1 H 2 be a bounded linear operator. Prove that [T (H 1 )] = N (T ). (6p) Uppsala Universitet Matematiska Institutionen Andreas Strömbergsson Prov i matematik Funktionalanalys Kurs: F3B, F4Sy, NVP 2005-03-08 Skrivtid: 9 14 Tillåtna hjälpmedel: Manuella skrivdon, Kreyszigs bok

Διαβάστε περισσότερα

Analytical Expression for Hessian

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

THE BLOWUP OF SOLUTIONS FOR 3-D AXISYMMETRIC COMPRESSIBLE EULER EQUATIONS

THE BLOWUP OF SOLUTIONS FOR 3-D AXISYMMETRIC COMPRESSIBLE EULER EQUATIONS H. Yin Q. Qiu Nagoya Math. J. Vol. 154 (1999, 157 169 THE BLOWUP OF SOLUTIONS FOR 3-D AXISYMMETRIC COMPRESSIBLE EULER EQUATIONS HUICHENG YIN QINGJIU QIU Abstact. In this pape, fo thee dimensional compessible

Διαβάστε περισσότερα

Matrix Hartree-Fock Equations for a Closed Shell System

Matrix 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 περισσότερα

Commutative Monoids in Intuitionistic Fuzzy Sets

Commutative Monoids in Intuitionistic Fuzzy Sets Commutative Monoids in Intuitionistic Fuzzy Sets S K Mala #1, Dr. MM Shanmugapriya *2 1 PhD Scholar in Mathematics, Karpagam University, Coimbatore, Tamilnadu- 641021 Assistant Professor of Mathematics,

Διαβάστε περισσότερα

Reminders: linear functions

Reminders: 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 περισσότερα

e t e r Cylindrical and Spherical Coordinate Representation of grad, div, curl and 2

e 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 περισσότερα

3.7 Governing Equations and Boundary Conditions for P-Flow

3.7 Governing Equations and Boundary Conditions for P-Flow .0 - Maine Hydodynaics, Sping 005 Lectue 10.0 - Maine Hydodynaics Lectue 10 3.7 Govening Equations and Bounday Conditions fo P-Flow 3.7.1 Govening Equations fo P-Flow (a Continuity φ = 0 ( 1 (b Benoulli

Διαβάστε περισσότερα

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007 Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Αν κάπου κάνετε κάποιες υποθέσεις να αναφερθούν στη σχετική ερώτηση. Όλα τα αρχεία που αναφέρονται στα προβλήματα βρίσκονται στον ίδιο φάκελο με το εκτελέσιμο

Διαβάστε περισσότερα

Numerical Analysis FMN011

Numerical Analysis FMN011 Numerical Analysis FMN011 Carmen Arévalo Lund University carmen@maths.lth.se Lecture 12 Periodic data A function g has period P if g(x + P ) = g(x) Model: Trigonometric polynomial of order M T M (x) =

Διαβάστε περισσότερα

М. I. Parolya, М. М. Sheremeta ESTIMATES FROM BELOW FOR CHARACTERISTIC FUNCTIONS OF PROBABILITY LAWS

М. I. Parolya, М. М. Sheremeta ESTIMATES FROM BELOW FOR CHARACTERISTIC FUNCTIONS OF PROBABILITY LAWS Математичнi Студiї. Т.39, Matematychni Studii. V.39, No. УДК 59.23.2+57.53 М. I. Paolya, М. М. Sheemeta ESTIMATES FROM BELOW FOR CHARACTERISTIC FUNCTIONS OF PROBABILITY LAWS M. I. Paolya, M. M. Sheemeta.

Διαβάστε περισσότερα

Boundary-Layer Flow over a Flat Plate Approximate Method

Boundary-Layer Flow over a Flat Plate Approximate Method Bounar-aer lo oer a lat Plate Approimate Metho Transition Turbulent aminar The momentum balance on a control olume o the bounar laer leas to the olloing equation: + () The approimate metho o bounar laer

Διαβάστε περισσότερα

Trigonometric Formula Sheet

Trigonometric 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 περισσότερα

Differential equations

Differential equations Differential equations Differential equations: An equation inoling one dependent ariable and its deriaties w. r. t one or more independent ariables is called a differential equation. Order of differential

Διαβάστε περισσότερα

12. Radon-Nikodym Theorem

12. Radon-Nikodym Theorem Tutorial 12: Radon-Nikodym Theorem 1 12. Radon-Nikodym Theorem In the following, (Ω, F) is an arbitrary measurable space. Definition 96 Let μ and ν be two (possibly complex) measures on (Ω, F). We say

Διαβάστε περισσότερα

Appendix to On the stability of a compressible axisymmetric rotating flow in a pipe. By Z. Rusak & J. H. Lee

Appendix to On the stability of a compressible axisymmetric rotating flow in a pipe. By Z. Rusak & J. H. Lee Appendi to On the stability of a compressible aisymmetric rotating flow in a pipe By Z. Rusak & J. H. Lee Journal of Fluid Mechanics, vol. 5 4, pp. 5 4 This material has not been copy-edited or typeset

Διαβάστε περισσότερα

A Note on Intuitionistic Fuzzy. Equivalence Relation

A 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 περισσότερα

Homomorphism in Intuitionistic Fuzzy Automata

Homomorphism 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 περισσότερα

DiracDelta. Notations. Primary definition. Specific values. General characteristics. Traditional name. Traditional notation

DiracDelta. Notations. Primary definition. Specific values. General characteristics. Traditional name. Traditional notation DiracDelta Notations Traditional name Dirac delta function Traditional notation x Mathematica StandardForm notation DiracDeltax Primary definition 4.03.02.000.0 x Π lim ε ; x ε0 x 2 2 ε Specific values

Διαβάστε περισσότερα

The Neutrix Product of the Distributions r. x λ

The 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 περισσότερα

ω 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

ω 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 περισσότερα

The Critical Exponent of Doubly Singular Parabolic Equations 1

The Critical Exponent of Doubly Singular Parabolic Equations 1 Jounal of Mathematical Analysis and Applications 257, 70 88 (200) doi:0.006/jmaa.2000.734, available online at http://www.idealibay.com on The Citical Exponent of Doubly Singula Paabolic Equations Xinfeng

Διαβάστε περισσότερα

Main source: "Discrete-time systems and computer control" by Α. ΣΚΟΔΡΑΣ ΨΗΦΙΑΚΟΣ ΕΛΕΓΧΟΣ ΔΙΑΛΕΞΗ 4 ΔΙΑΦΑΝΕΙΑ 1

Main source: Discrete-time systems and computer control by Α. ΣΚΟΔΡΑΣ ΨΗΦΙΑΚΟΣ ΕΛΕΓΧΟΣ ΔΙΑΛΕΞΗ 4 ΔΙΑΦΑΝΕΙΑ 1 Main source: "Discrete-time systems and computer control" by Α. ΣΚΟΔΡΑΣ ΨΗΦΙΑΚΟΣ ΕΛΕΓΧΟΣ ΔΙΑΛΕΞΗ 4 ΔΙΑΦΑΝΕΙΑ 1 A Brief History of Sampling Research 1915 - Edmund Taylor Whittaker (1873-1956) devised a

Διαβάστε περισσότερα

Jesse Maassen and Mark Lundstrom Purdue University November 25, 2013

Jesse 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 περισσότερα

Positive solutions for three-point nonlinear fractional boundary value problems

Positive solutions for three-point nonlinear fractional boundary value problems Electronic Journal of Qualitative Theory of Differential Equations 2, No. 2, -9; http://www.math.u-szeged.hu/ejqtde/ Positive solutions for three-point nonlinear fractional boundary value problems Abdelkader

Διαβάστε περισσότερα

Partial Differential Equations in Biology The boundary element method. March 26, 2013

Partial 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 περισσότερα

The Simply Typed Lambda Calculus

The 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 περισσότερα