Vol. 40 No Journal of Jiangxi Normal University Natural Science Jul. 2016

Σχετικά έγγραφα
J. of Math. (PRC) u(t k ) = I k (u(t k )), k = 1, 2,, (1.6) , [3, 4] (1.1), (1.2), (1.3), [6 8]

Nonlinear Analysis: Modelling and Control, 2013, Vol. 18, No. 4,

Necessary and sufficient conditions for oscillation of first order nonlinear neutral differential equations

Positive solutions for a multi-point eigenvalue. problem involving the one dimensional

Linear singular perturbations of hyperbolic-parabolic type

r t te 2t i t Find the derivative of the vector function. 19. r t e t cos t i e t sin t j ln t k Evaluate the integral.

Vol. 38 No Journal of Jiangxi Normal University Natural Science Nov. 2014

Oscillation Criteria for Nonlinear Damped Dynamic Equations on Time Scales

J. of Math. (PRC) Banach, , X = N(T ) R(T + ), Y = R(T ) N(T + ). Vol. 37 ( 2017 ) No. 5

Multiple positive periodic solutions of nonlinear functional differential system with feedback control

A Control Method of Errors in Long-Term Integration

Oscillation criteria for two-dimensional system of non-linear ordinary differential equations

ACTA MATHEMATICAE APPLICATAE SINICA Sep., ( MR (2000) Õ È 32C17; 32F07; 35G30; 53C55

ER-Tree (Extended R*-Tree)

Nov Journal of Zhengzhou University Engineering Science Vol. 36 No FCM. A doi /j. issn

Reservoir modeling. Reservoir modelling Linear reservoirs. The linear reservoir, no input. Starting up reservoir modeling

High order interpolation function for surface contact problem

Pricing Asian option under mixed jump-fraction process

Existence of travelling wave solutions in delayed reaction diffusion systems with applications to diffusion competition systems

CorV CVAC. CorV TU317. 1

A research on the influence of dummy activity on float in an AOA network and its amendments

EXISTENCE OF POSITIVE SOLUTIONS FOR SINGULAR FRACTIONAL DIFFERENTIAL EQUATIONS

ACTA MATHEMATICAE APPLICATAE SINICA Nov., ( µ ) ( (

FENXI HUAXUE Chinese Journal of Analytical Chemistry. Savitzky-Golay. n = SG SG. Savitzky-Golay mmol /L 5700.

Apr Vol.26 No.2. Pure and Applied Mathematics O157.5 A (2010) (d(u)d(v)) α, 1, (1969-),,.

INDIRECT ADAPTIVE CONTROL

2 ~ 8 Hz Hz. Blondet 1 Trombetti 2-4 Symans 5. = - M p. M p. s 2 x p. s 2 x t x t. + C p. sx p. + K p. x p. C p. s 2. x tp x t.

Journal of Central South University (Science and Technology) May Bragg TU443 A (2011)

( ) ( t) ( 0) ( ) dw w. = = β. Then the solution of (1.1) is easily found to. wt = t+ t. We generalize this to the following nonlinear differential

Levin Lin(1992) Oh(1996),Wu(1996) Papell(1997) Im, Pesaran Shin(1996) Canzoneri, Cumby Diba(1999) Lee, Pesaran Smith(1997) FGLS SUR

I. Μητρώο Εξωτερικών Μελών της ημεδαπής για το γνωστικό αντικείμενο «Μη Γραμμικές Ελλειπτικές Διαφορικές Εξισώσεις»

L p approach to free boundary problems of the Navier-Stokes equation

2002 Journal of Software

No. 7 Modular Machine Tool & Automatic Manufacturing Technique. Jul TH166 TG659 A

Error ana lysis of P2wave non2hyperbolic m oveout veloc ity in layered media

A New Approach to Bounded Real Lemma Representation for Linear Neutral Systems

Center Manifold Theory and Computation Using a Forward Backward Approach

ΕΡΓΑΣΙΑ ΜΑΘΗΜΑΤΟΣ: ΘΕΩΡΙΑ ΒΕΛΤΙΣΤΟΥ ΕΛΕΓΧΟΥ ΦΙΛΤΡΟ KALMAN ΜΩΥΣΗΣ ΛΑΖΑΡΟΣ

J. of Math. (PRC) 6 n (nt ) + n V = 0, (1.1) n t + div. div(n T ) = n τ (T L(x) T ), (1.2) n)xx (nt ) x + nv x = J 0, (1.4) n. 6 n

Estimation of stability region for a class of switched linear systems with multiple equilibrium points

The Euler Equations! λ 1. λ 2. λ 3. ρ ρu. E = e + u 2 /2. E + p ρ. = de /dt. = dh / dt; h = h( T ); c p. / c v. ; γ = c p. p = ( γ 1)ρe. c v.

Representation of Five Dimensional Lie Algebra and Generating Relations for the Generalized Hypergeometric Functions

Motion analysis and simulation of a stratospheric airship

Analysis of optimal harvesting of a prey-predator fishery model with the limited sources of prey and presence of toxicity

Prey-Taxis Holling-Tanner

( ) ( ) ( ) Fourier series. ; m is an integer. r(t) is periodic (T>0), r(t+t) = r(t), t Fundamental period T 0 = smallest T. Fundamental frequency ω

University of Washington Department of Chemistry Chemistry 553 Spring Quarter 2010 Homework Assignment 3 Due 04/26/10

arxiv: v1 [math.ap] 10 Apr 2017

Stress Relaxation Test and Constitutive Equation of Saturated Soft Soil

Single-value extension property for anti-diagonal operator matrices and their square

ON LOCAL MOTION OF A COMPRESSIBLE BAROTROPIC VISCOUS FLUID WITH THE BOUNDARY SLIP CONDITION. Marek Burnat Wojciech M. ZajĄczkowski. 1.

Vol. 40 No Journal of Jiangxi Normal University Natural Science Jul p q -φ. p q

Approximation Expressions for the Temperature Integral

Analysis on construction application of lager diameter pile foundation engineering in Guangdong coastal areas

Evaluation on precision of occurrence measurement based on theory of errors

Χρονοσειρές Μάθημα 3

ΔΙΠΛΩΜΑΤΙΚΕΣ ΕΡΓΑΣΙΕΣ

Positive solutions for three-point nonlinear fractional boundary value problems

Studies on the Binding Mechanism of Several Antibiotics and Human Serum Albumin

LUO, Hong2Qun LIU, Shao2Pu Ξ LI, Nian2Bing

The Student s t and F Distributions Page 1

Vol. 31,No JOURNAL OF CHINA UNIVERSITY OF SCIENCE AND TECHNOLOGY Feb

Homomorphism in Intuitionistic Fuzzy Automata

The third moment for the parabolic Anderson model

Symmetric Complex Boundary Element Scheme for 2-D Stokes Mixed Boundary Value Problem

,,, (, ) , ;,,, ; -

Q L -BFGS. Method of Q through full waveform inversion based on L -BFGS algorithm. SUN Hui-qiu HAN Li-guo XU Yang-yang GAO Han ZHOU Yan ZHANG Pan

Riemann Hypothesis: a GGC representation

9.1 Introduction 9.2 Lags in the Error Term: Autocorrelation 9.3 Estimating an AR(1) Error Model 9.4 Testing for Autocorrelation 9.

arxiv: v3 [math.ca] 4 Jul 2013

(II) * PACS: a, Hj 300. ) [6 9] ) [10 23] ) [26 30]. . Deng [24,25] Acta Phys. Sin. Vol. 61, No. 15 (2012)

DOI /J. 1SSN

Vol. 41 No Journal of Jiangxi Normal University Natural Science May A DOI /j. cnki. issn

326. Dynamic synchronization of the unbalanced rotors for the excitation of longitudinal traveling waves

Product Innovation and Optimal Capital Investment under Uncertainty. by Chia-Yu Liao Advisor Ching-Tang Wu

Supporting Information

Matrices and Determinants

Congruence Classes of Invertible Matrices of Order 3 over F 2

Quick algorithm f or computing core attribute

Electronic Companion to Supply Chain Dynamics and Channel Efficiency in Durable Product Pricing and Distribution

Numerical Analysis FMN011

90 [, ] p Panel nested error structure) : Lagrange-multiple LM) Honda [3] LM ; King Wu, Baltagi, Chang Li [4] Moulton Randolph ANOVA) F p Panel,, p Z

Model updating experiment of space truss using global and local dynamic information HOU Ji-lin 1 OU Jin-ping 1 2 ukasz Jankowski 3

Supporting Information

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

: Monte Carlo EM 313, Louis (1982) EM, EM Newton-Raphson, /. EM, 2 Monte Carlo EM Newton-Raphson, Monte Carlo EM, Monte Carlo EM, /. 3, Monte Carlo EM

, P bkc (c[0, 1]) P bkc (L p [0, 1]) (1) 2 P bkc (X) O A (2012) Aumann. R. J., [3]. Feb Vol. 28 No.

Application of Statistical Process Control in Pretreatment Production Process of Gardenia jasminoides

Optimizing Microwave-assisted Extraction Process for Paprika Red Pigments Using Response Surface Methodology

Polyvinyl Chloride PVC, The effects of organotin thermal stabilizers on the dehydrochlorination of TPUΠPVC blends

Applying Markov Decision Processes to Role-playing Game

ΑΝΑΛΥΣΗ ΔΕΔΟΜΕΝΩΝ ΔΟΚΙΜΑΣΤΙΚΩΝ ΑΝΤΛΗΣΕΩΝ ΜΕ ΜΕΤΑΒΑΛΛΟΜΕΝΗ ΠΑΡΟΧΗ ΣΕ ΚΛΕΙΣΤΟΥΣ ΥΔΡΟΦΟΡΕΙΣ

Research on model of early2warning of enterprise crisis based on entropy

Research Article Existence of Positive Solutions for m-point Boundary Value Problems on Time Scales

ΔΗΜΟΣΙΕΥΣΕΙΣ σε περιοδικά με κριτές

On Strong Product of Two Fuzzy Graphs

= e 6t. = t 1 = t. 5 t 8L 1[ 1 = 3L 1 [ 1. L 1 [ π. = 3 π. = L 1 3s = L. = 3L 1 s t. = 3 cos(5t) sin(5t).

Research on real-time inverse kinematics algorithms for 6R robots

(, ) (SEM) [4] ,,,, , Legendre. [6] Gauss-Lobatto-Legendre (GLL) Legendre. Dubiner ,,,, (TSEM) Vol. 34 No. 4 Dec. 2017

HIV HIV HIV HIV AIDS 3 :.1 /-,**1 +332

Transcript:

4 4 Vol 4 No 4 26 7 Journal of Jiangxi Normal Universiy Naural Science Jul 26-5862 26 4-349-5 3 2 6 2 67 3 3 O 77 9 A DOI 6357 /j cnki issn-5862 26 4 4 C q x' x /q G s = { α 2 - s -9 2 β 2 2 s α 2 - s -6-3 2 β 2 - s 2 - s 2 2 2 G s q G s s 2-3 3 q = β 2 / 2 { x φ f x x' = P = x C q q x x x 2 x = x' = x P C q αx' βx = 3 x P x = x α β > φ 4 φ C R φ s ds < = = 7! F = G s φ s ds F P 7 ~ 4 7 6 3 4-5 5 5 Ω Banach E q = β 2 / 2 C q = x R x x' q x' <! x P E E θ Ω A Ω P P λax x x Ω P λ i A Ω P P = C q C q 6 Ω Banach E x = x x 2 x = x 2 = q x' P E A Ω P P Ax /x x Ω P / C q Banach x i A Ω P P = 26--5 647365 964-

35 26! H 2 g C!!! f x y g x q y x y! -!! H 3 c/ [ ( c! s) g x z ] > φ s d x c z c H 4 g C! -!!! f x y g x y x y! -!! lim g x y /x =! y x! H 5 g 2 C! -!!! f x y g 2 x y x y! -!! limg 2 x y /x =! y x x P A Ax = G s φ s f s x s x' s ds H H 2 A P P Ax = s φ s f s x s x' s ds G s φ s g x s q s x' s ds G g c c' <! φ s ds c x c' x q Ax ' = q α - s ( β ) φ s f s x s x' s ds - - s φ s f s x s x' s ds α - s β φ s f s x s x' s ds φ s f s x s x' s ds 2 φ s f s x s x' s ds Ax ' - Ax ' = 2 φ s ds g c c' <! lim x n = x lim x n ' = n! n! c x c' x x Ax ' f x n x n ' g x n 4 A P P q x n ' g x y x M y M α - s β φ s f s x s x' s ds - H φ C L φ > f C! -!! - s φ s f s x s x' s ds α - s β α β φ s f s x s x' s ds - s φ s f s x s x' s ds ( c x c' x c x c' x g c c' ) - Ax ' - Ax ' = α - s β φ s ds g c c' - s φ s ds α - s β φ s f s x s x' s ds - - s φ s f s x s x' s ds - α - s ( β - s) φ s f s x s x' s ds = α - s β α - s ( - - ) φ s f s x s x' s ds - - s φ s f s x s x' s ds = β - s αs - - s φ s f s x s x' s ds - - s φ s f s x s x' s ds = αs - - s φ s f s x s x' s ds - - s φ s f s x s x' s ds αs - - s - αs φ s f s φ s f s x s x' s ds x s x' s ds αs - - s φ s f s x s x' s ds Ax C x n P x P lim x n = x M > n! x n < M n 2 3

4 3 35 n! Ax n - Ax G s φ s f s x n s x n ' s f s x s = x ' s ds φ s f s x n s x n ' s f s x s x ' s ds Ax n - Ax 2 = Ax - Ax 2 ( q α - s β - - s φ s f s x m x n ' f s x x ' ds ε > δ > 2 - < δ α - s β ( ) φ s f s x n x n ' f s x x ' ds q [ ( s - αs Ax ' 2 < ε Ax x D Ax - Ax 2 < ε Ax ' - ) φ s Ax ' x D f s x n x n ' - f s x x ' ds ( - αs ) φ s Arzela-Ascoli A D C f s x n x n ' - f s x x ' d s ] Ax Ax = Ax A P P Ax ' D M > x D A P P x M H ~ H 4 Ax = 2 G s φ s f s x s H 3 R > x' s ds φ s ds g x y R / ( x M y M g x y φ s ds x R y R ) > 2 Ax 2 2 φ s ds g x y C q Ω = x C q x M y M x < R A D C q C μax x μ x P Ω 2 < 2 x D μ x P Ω G s - μ Ax = x x Ax = G s φ s f s G 2 s φ s d s ) Ax ' - Ax ' 2 = g x y x M y M α - s β φ s f s x s x' s ds - - s φ s f s x s x' s ds - 2 2 2 2 2 α 2 - s β 2 φ s f s x s x' s ds - s φ s f s x s x' s ds = - 2 ( - αs α ) β φ s f s - s φ s f s x s x' s ds - s φ s f s x s x' s ds - - s φ s f s x s x' s ds = x s x' s ds 2-2 ( - αs ) φ s f s x s x' s ds 2 - φ s f s x s x' s ds 2 - s φ s f s x s x' s ds ( 2 2 - φ s ds 2 φ s d s ) g x y x M y M x s x ' s ds G s φ s ds g x y y R x R g x y q x ' = u q φ s ds x R y R Ax ' φ s ds g x y x R y R R = x x 2 φ s ds g x y x R y R R / g x y φ s ds x R y R 2 5 i A Ω P P = 3 < a * < b * < N * = βa ( * 2 min a * b b* s φ s d s) * 2 a * G - H 4 R 2 ' > R g x y N * x

352 26 x R 2 ' y -!! R 2 = 2 α N ** x x R 3 y -!! C q β R 2 ' / βa * 2 R 2 > R C q Ω 3 = x C q x < R 3 Ω 2 = x C q x < R 2 Ax /x Ax /x x P Ω 3 x P Ω 2 x P Ω 2 x Ax a * b * x q x βa * 2 x / 2 = βa * 2 2 R 2 2 ' = R 2 ' βa * 2 x Ax = G s φ s f s x s b x ' s ds * G s φ s g x s x ' s ds a * b* G s φ s N * x s ds N * b R 2 ' a * G s φ s ds * a * i A Ω 2 \ Ω P P = i A Ω 2 P P i A Ω P P = - 5 A Ω 2 \ Ω P 2 μ x 2 H ~ H 槡 - 4 2 x' 5 2 x b = x = x' = < R < αx' βx = R 2 C q Ω Ω 2 = x C q x < R = x C q x < R 2 3 4 5 A Ω 2 \ Ω P < a ** < b ** < N ** = βa ( **2 min b** b** G s φ s d s) 2 H 5 R 3 - < R g 2 x y x P Ω 3 x Ax a ** b ** x q x βa **2 x / 2 = βa **2 R 3 / 2 x Ax = x ' s ds b** b** G s φ s N ** x s ds N ** β2 2 R 3 b** G s φ s f s x s G s φ s g 2 x s x ' s ds G s φ s ds N * R 2 ' min a * b b* G s φ s ds = * a * N * βa * 2 R 2 ' 2 min a * b b* N ( G s φ s d s ) 2 R 3 min a * b b** G s φ s ds > R 3 * * a * 2 2 α x β x > R 3 > R βa * 2 βa * 2 2 ' 6 x x > 2 R 2 ' / βa * 2 = i A Ω 3 P P = 6 R 2 x < R 2 6 i A Ω 2 P P = 4 3 6 i A Ω \ Ω 3 P P = i A Ω P P i A Ω 3 P P = A Ω \ Ω 3 P A P P 3 A Ω P 2 2 a β > α a > b > μ > 7 μ < c / π c a c b 8 c! 7 2 7 φ = μ / - 槡 f x y = 2 y /4 a x b H g x z = z a x b f x y g x q y H 2

4 3 353 c! c! c! c / φ s ds c / μπ x c y c x c y c g x y = y a x b = c / μπ c a c b 8 c! c / φ s ds x c y c g x y > H 3 4 Wei Zhongli Some necessary and sufficien condiions for g x y = g 2 x y = x b f x y exisence of posiive soluions for hird order singular sublinear muli-poin boundary value problems J Aca g x y = g 2 x y lim g x y /x = lim x b /x =! Mah Sci 24 34 6 795-8 x! x! limg 2 x y /x = lim x b 5 Zhang Haie Sun Jianping Exisence and ieraion of monoone posiive soluions for hird-order nonlocal BVPs in- /x =! x x y -!! H 4 H 5 volving inegral condiions J Elecronic Journal of Qualiaive Theory of Differenial Equaions 22 4 2 7 2 8-9 7 6 3 2 J 7 Agarwal Ravi P O Regan Donal Yan Baoqiang Muliple 3 posiive soluions of singular Dirichle second-order boundary-value problems wih derivaive dependence J Journal of Dynamical and Conrol Sysems 29 5-26 8 Li Yongxiang Shang Yaya An exisence resul of posiive 3 soluions for fully second-order boundary value problems H ~ H 4 J Journal of Funcion Spaces doi 55 /25 / 2 287253 x 9 Zhang Guowei Posiive soluions of wo-poin boundary Ω P x value problems for second-order differenial equaions wih R q he nonlineariy dependen on he derivaive J Nonlinear Anal 28 69 222-229 x ' R x 2 Ω 2 \ Ω P R x 2 R 2 Mousafa El-Shahed Posiive soluions for nonlinear singular hird order boundary value problem J Communica- R q x 2 ' R 2 ions in Nonlinear Science and Numerical Simulaion 2 H ~ H 5 29 4 2 424-429 2 3 J x Ω \ Ω 3 P R 3 2 34 3 277- x R R 3 q x ' R 279 2 M x 2 Ω 2 \ Ω P 27 3 M 4 Cheng Ming Nagumo heorems of hird-order singular nonlinear boundary value problems J Boundary Value Problems 25-2 Kelevedjiev P Popivanov N Bekesheva L Exisence of soluions for a class of hird-order nonlinear boundary value problem C AIP Conference Proceedings doi 63 / 4936723 3 Wei Zhongli Some necessary and sufficien condiions for exisence of posiive soluions for hird order singular er-linear muli-poin boundary value problems J J Appl Mah Compu 24 46 47-422 25 42 24-32 24 4 Deimling K Nonlinear funcional analysis M Berlin Springer-Verlag 985 5 M 3 25 368

368 26 9 J 25 39 69-72 CAT J 24 38 5 445-448 J 28 5 27-29 5 Chang Hua-Hua Qian Jiahe Ying Zhiliang Alpha-sraified mulisage compuerized adapive esing J Applied Psychological Measuremen 999 23 23 2-222 6 J 23 37-5 7 J 23 37 6 657-66 2 8 J 22 44 3 4- J 26 38 3 46-42 467 The Iem Selecion Sraegy of Raising Iem Pool Securiy HE Xiang LUO Fen GAN Dengwen * DING Shuliang WANG Wenyi College of Compuer Informaion and Engineering Jiangxi Normal Universiy Nanchang Jiangxi 3322 China Absrac The safey of iem pool is he key poin o he implemenaion of compuerized adapive es inspired by he original dynamic a-sraified mehod and mean inequaliy consrucing anoher iem selecion sraegy of he dynamic a-sraified The simulaion experimenal resuls showed ha he new iem selecion sraegy o keep he es precision of he original dynamic a-sraified mehod and furher improves he securiy of he es Key words iem informaion discriminaion iem selecion sraegy 353 The Posiive Soluions of a Class of Third-Order Boundary-Value Problems wih Derivaive Dependence LI Fengyan SHI Jinchuan 2 Deparmen of Business and Trade College of Liaoning Adminisraion Shenyang Liaoning 6 China 2 Keya College Shenyang Universiy of Chemical Technology Shenyang Liaoning 67 China Absrac By means of he mehods of fixed poin index compuaion he exisence of posiive soluions of a class of hird-order boundary-value problems wih derivaive dependence is proved The boundary-value problems considered possess differen order boundary condiions and singulariy from hose in previous works An example is given o apply he resuls obained Key words derivaive dependence hird-order boundary-value posiive soluion