Research Article Existence of Positive Solutions for Fourth-Order Three-Point Boundary Value Problems
|
|
- Ἀγαμέμνων Ζυγομαλάς
- 7 χρόνια πριν
- Προβολές:
Transcript
1 Hindawi Publihing Corporation Boundary Value Problem Volume 27, Article ID 68758, 1 page doi:1.1155/27/68758 Reearch Article Exitence of Poitive Solution for Fourth-Order Three-Point Boundary Value Problem Chuanzhi Bai Received 11 July 27; Accepted 7 November 27 Recommended by Jean Mawhin We are concerned with the nonlinear fourth-order three-point boundary value problem u (4) (t) = a(t) f (u(t)), <t<1, u() = u(1) =, αu () βu () =, γu (1) + δu (1) =. By uing Kranoelkii fixed point theorem in a cone, we get ome exitence reult of poitive olution. Copyright 27 Chuanzhi Bai. Thi i an open acce article ditributed under the Creative Common Attribution Licene, which permit unretricted ue, ditribution, and reproduction in any medium, provided the original work i properly cited. 1. Introduction A i pointed out in [1, 2, boundary value problem for econd- and higher-order differential equation play a very important role in both theory and application. Recently, an increaing interet in tudying the exitence of olution and poitive olution to boundary value problem for fourth-order differential equation i oberved; ee, for example, [3 8. In thi paper, we are concerned with the exitence of poitive olution for the following fourth-order three-point boundary value problem (BVP): u (4) (t) = a(t) f ( u(t) ), <t<1, u() = u(1) =, αu () βu () =, γu (1) + δu (1) =, (1.1) where α, β, γ, andδ are nonnegative contant atifying αδ + βγ + αγ > ; <<1, a C[,1, and f C([, ),[, )). We ue Kranoelkii fixed point theorem in cone to etablih ome imple criteria for the exitence of at leat one poitive olution to BVP (1.1). To the bet of our knowledge, no paper in the literature ha invetigated the exitence of poitive olution for BVP (1.1).
2 2 Boundary Value Problem The paper i formulated a follow. In Section 2, ome definition and lemma are given. In Section 3, we prove ome exitence theorem of the poitive olution for BVP (1.1). 2. Preliminarie and lemma In thi ection, we introduce ome neceary definition and preliminary reult that will be ued to prove our main reult. Firt, we lit the following notation and aumption: f (u) f = lim u u, f f (u) = lim u u. (2.1) (H 1 ) f :[, ) [, )icontinuou; (H 2 ) a C[,1, a(t), for all t [,, a(t), for all t [,1, and a(t), for all t (p,) (,q)(<p<<q<1). By routine calculation, we eaily obtain the following lemma. Lemma 2.1. Suppoe that α, β, γ, δ are nonnegative contant atifying αδ + βγ + αγ >. If h C[,1, then the boundary value problem v (t) = h(t), t [,1, αv() βv () =, γv(1) + δv (1) = (2.2) ha a unique olution t v(t) = )h()d+ (t 1 where = αδ + βγ + αγ(1 ) >. Let G(t,) be the Green functionof the differential equation ubject to the boundary condition In particular, ( α( t) β )( γ(1 )+δ ) h()d, (2.3) u (t) =, t (,1), (2.4) u() = u(1) =. (2.5) (1 t), t 1, G(t,) = t(1 ), t< 1. (2.6)
3 Chuanzhi Bai 3 It i rather traightforward that G(t,) G(,), t, 1, (2.7) G(t,) mg(,), t [p,q, [,1, (2.8) where <p<q<1, and <m= min{p,1 q} < 1. Let X be the Banach pace C[,1 endowed with the norm We define the operator T : X X by u =max u(t). (2.9) t 1 [ Tu(t) = G(t,) (τ )a(τ) f + 1 ( )( ) ( ) β α( ) γ(1 τ)+δ a(τ) f u(τ d, (2.1) where G(t,) ain(2.6). From Lemma 2.1, we eaily know that u(t) i a olution of the fourth-order three-point boundary value problem (1.1)ifandonlyifu(t)iafixedpoint of the operator T. Define the cone K in X by K = { u X u, min u(t) m u t [p,q }, (2.11) where <p<<q<1, and <m= max{p,1 q} < 1. (2.12) Lemma 2.2. Aume that (H 1 ) and (H 2 ) hold. If β α, then T : K K i completely continuou. Proof. For any u K,weknowfrom(2.1), (H 1 ), (H 2 ), and β α that [ (Tu)(t) = G(t,) ( τ)a(τ) f + 1 ( )( ) ( ) β α( ) γ(1 τ)+δ a(τ) f u(τ d [ + G(t,) (τ )a(τ) f + 1 ( )( ) ( ) β α( ) γ(1 τ)+δ a(τ) f u(τ + 1 ( )( ) ( ) β α( ) γ(1 τ)+δ a(τ) f u(τ d
4 4 Boundary Value Problem [ = G(t,) ( τ)a(τ) f + 1 ( )( ) ( ) β α( ) γ(1 τ)+δ a(τ) f u(τ d [ 1 + G(t,), t [, [ αδ(τ )+βγ(1 )+αγ(1 )(τ )+βδ a(τ) f ( β + α( ) ) d (2.13) Hence, in view of (2.13)and(2.7), we have [ Tu = max (Tu)(t) G(,) ( τ)a(τ) f t [,1 + 1 ( )( ) ( ) β α( ) γ(1 τ)+δ a(τ) f u(τ d [ 1 + G(,) + 1 Thu from (2.8), (2.13), and (2.14), we get min t [p,q (Tu)(t) m [ αδ(τ )+βγ(1 )+αγ(1 )(τ )+βδ a(τ) f ( β + α( ) ) d. [ G(,) ( τ)a(τ) f ( )( ) ( ) β α( ) γ(1 τ)+δ a(τ) f u(τ d + 1 [ 1 + m G(,) + 1 (2.14) [ αδ(τ )+βγ(1 )+αγ(1 )(τ )+βδ a(τ) f ( β + α( ) ) d = m Tu, (2.15) where m a in (2.12). So T : K K. Moreover, it i eay to check by the Arzela-Acoli theorem that the operator T i completely continuou. Remark 2.3. By = αδ + βγ + αγ(1 ) > andβ α,wehaveβ>. Recently, Kranoelkii theorem of cone expanion/compreion type ha been ued to tudy the exitence of poitive olution of boundary value problem in many paper;
5 Chuanzhi Bai 5 ee, for example, Liu [7, Ma [9, Torre [1, and the reference contained therein. The following lemma (Kranoelkii fixed point theorem) will play an important role in the proofofourtheorem. Lemma 2.4 [11. Let X be a Banach pace, and let K X beaconeinx. Aume that Ω 1, Ω 2 are open ubet of X with Ω 1, Ω 1 Ω 2 and let A : K (Ω 2 \ Ω 1 ) K be a completely operator uch that either (i) Au u, u K Ω 1 and Au u, u K Ω 2 ;or (ii) Au u, u K Ω 1 and Au u, u K Ω 2. Then A ha a fixed point in K (Ω 2 \ Ω 1 ). 3. Main reult We are now in a poition to preent and prove our main reult. Theorem 3.1. Let β α. Aume that (H 1 )-(H 2 ) hold. If f = and f =, then(1.1) ha at leat a poitive olution. Proof. Since f =,wecanchooer>ufficiently mall o that where ε atifie ε f (u) εu for u r, (3.1) 6 m(1 ) a(τ)τ3 dτ, if a( ) t <, for ome t (p,), βm (τ )(1 τ) ) a(τ)dτ, if a( t 1 ) >, for ome t1 (,q). (3.2) Set Ω r ={u K u <r}. From condition (H 2 ), we conider two cae a follow. Cae 1. If a(t ) < foromet (p,), then, for u Ω r,wehavefrom(2.13), (3.1), and (3.2)that [ (Tu)() G(,) ( τ)a(τ) f + 1 ( )( ) ( ) β α( ) γ(1 τ)+δ a(τ) f u(τ d G(,) ( τ)a(τ) f ) dτ d ε G(,) ( τ)a(τ)u(τ)dτ d mε u G(,) = mε u a(τ)dτ τ ( τ)a(τ)dτ d = mε u (1 )( τ)d = mε u 1 6 a(τ)dτ τ G(,)( τ)d a(τ)τ 3 dτ u, (3.3)
6 6 Boundary Value Problem which implie Tu u, u Ω r. (3.4) Cae 2. If a(t 1 ) > foromet 1 (,q), then, for u Ω r,wehavefrom(2.13), (3.1), and (3.2)that [ [ ( ) (Tu)() G(,) αδ(τ )+βγ(1 )+αγ(1 )(τ )+βδ a(τ) f u(τ + 1 ( )( ) ( ) β + α( ) γ(1 τ)+δ a(τ) f u(τ d that i, 1 β G(,) G(,) εβm u = εβm u = εβm u εβm u ( β + α( ) ) d d G(,)d ) a(τ)dτ ( ) τ γ(1 τ)+δ a(τ)dτ (1 )d ( (τ ) 1 1 ) (γ(1 2 (τ + ) ) τ)+δ a(τ)dτ (τ )(1 τ) ) a(τ)dτ u, Next, define a function f (v):[, ) [, )by (3.5) Tu u, u Ω r. (3.6) f (v) = max f (u). (3.7) u v It i eay to ee that f (v) inondecreaing.since f =, we have lim v f (v)/v =. Thu, thereexitr>ruch that f (R) θr, (3.8) where θ atifie [ θ a(τ)τ 3 dτ + 1 [ ( (1 ) + βδ 1 2 ) a(τ)dτ ( ) ( ) β + α(1 ) γ(1 τ)+δ a(τ)dτ 1. 6 (3.9)
7 Chuanzhi Bai 7 Hence, we obtain Thu from (2.14)and(3.1), for all u Ω R,wehave f (u) f (R) θr, u R. (3.1) [ [ Tu θr G(,) ( τ)a(τ)dτ + 1 (β α + α) ) a(τ)dτ d [ [ + G(,) αδ(τ )+βγ(1 )+αγ(1 )(τ )+βδ a(τ)dτ + 1 ( )( ) β + α( ) γ(1 τ)+δ a(τ)dτ d [ τ θr a(τ)dτ (1 )( τ)d+ β ( ) γ(1 τ)+δ a(τ)dτ (1 )d + 1 [ (1 )d αδ(1 )+βγ(1 )+αγ(1 ) 2 + βδ a(τ)dτ + 1 ( )( ) (1 )d β + α(1 ) γ(1 τ)+δ a(τ)dτ that i, [ = θr a(τ)τ 3 dτ + β ( ) ( ) γ(1 τ)+δ a(τ)dτ [ ( (1 ) + βδ ) a(τ)dτ + 1 ( )( β + α(1 ) ) ( ) γ(1 τ)+δ a(τ)dτ 6 [ θr a(τ)τ 3 dτ + 1 [ ( (1 ) + βδ 1 2 ) a(τ)dτ ( ) ( ) β + α(1 ) γ(1 τ)+δ a(τ)dτ R = u, 6 (3.11) Tu u, foru Ω R. (3.12) Hence, from (3.6), (3.12), and Lemma 2.4, T ha a fixed point u Ω R \ Ω r, which mean that u i a poitive olution of BVP (1.1). Theorem 3.2. Let β α. Aume that (H 1 )-(H 2 )hold.if f = and f =,then(1.1) ha at leat a poitive olution.
8 8 Boundary Value Problem Proof. Since f =,wecanchooer 1 > ufficiently large o that f (u) Au, u R 1, (3.13) where A atifie 6 m(1 ) p a(τ)(τ p)( τ 2 + τp τp 2, A βm q (τ )(1 τ) ) a(τ)dτ, if a( t ) <, for ome t (p,), if a( t 1 ) >, for ome t1 (,q). (3.14) Chooe R R 1 m, (3.15) where m>ain(2.12). Let u Ω R.Sinceu(t) m u =mr R 1 for t [p,q, from (3.13), we ee that f ( u(t) ) Au(t) AmR, t [p,q, u Ω R. (3.16) For u Ω R, we conider two cae a follow. Cae 1. If a(t ) < foromet (p,), then we have from (3.3), (3.14), and (3.16)that (Tu)() p G(,) ( τ)a(τ) f d G(,) ( τ)a(τ) f d AmR G(,) ( τ)a(τ)dτ d p p τ = AmR(1 ) a(τ)dτ ( τ)d p = 1 p 6 AmR(1 ) a(τ)(τ p) ( τ 2 + τp 2p 2 R = u, (3.17) which implie Tu u, u Ω R. (3.18)
9 Chuanzhi Bai 9 Cae 2. If a(t 1 ) > foromet 1 (,q), then we have from (3.5), (3.14), and (3.16)that (Tu)() β which implie β q AmR β G(,) G(,) q q q G(,) d d q ) a(τ)dτ d = AmR β ( ) τ γ(1 τ)+δ a(τ)dτ (1 )d AmR β q (τ )(1 τ) ) a(τ)dτ R = u, (3.19) Tu u, u Ω R. (3.2) Since f =,wecanchooe<r<ruch that f (u) θu, u r, (3.21) where θ a in (3.9). For u Ω r,wehavefrom(3.11)and(3.21)that So, [ Tu θ u a(τ)τ 3 dτ + 1 [ ( (1 ) + βδ 1 2 ) a(τ)dτ ( β + α(1 ) ) ) a(τ)dτ u. (3.22) Tu u, u Ω r. (3.23) Therefore, from (3.2), (3.23), and Lemma 2.4, T haafixedpointu Ω R \ Ω r, which mean u i a poitive olution of BVP (1.1). Finally, we conclude thi paper with the following example. Example 3.3. Conider the following fourth-order three-point boundary value problem: u (4) (t) = inπ(1 + 2t)u r (t), <t<1, αu ( 1 2 u() = u(1) =, ) ( ) 1 βu =, γu 2 (1) + δu (1) =, (3.24) where <r<1, α, β, γ, andδ are nonnegative contant atifying αδ + βγ + αγ > and β (1/2)α.ThenBVP(3.24) ha at leat one poitive olution.
10 1 Boundary Value Problem To ee thi, we will apply Theorem 3.1.Set f (u) = u r, a(t) = inπ(1 + 2t), = 1 2. (3.25) With the above function f and a,weeethat(h 1 )and(h 2 )hold.moreover,itieayto ee that The reult now follow from Theorem 3.1. Acknowledgment f =, f =, β α. (3.26) Thi work i upported by the National Natural Science Foundation of China ( ) and the Natural Science Foundation of Jiangu Education Office (6KJB111). The author i grateful to the referee for their valuable uggetion and comment. Reference [1 R. P. Agarwal, Focal Boundary Value problem for Differential and Difference Equation, vol. 436 of MathematicandItApplication, Kluwer Academic Publiher, Dordrecht, The Netherland, [2 D. G. Zill and M. R. Cullen, Differential Equation with Boundary-Value Problem, Brook/Cole, Belmont, Calif, USA, 5th edition, 21. [3 Z. Bai and H. Wang, On poitive olution of ome nonlinear fourth-order beam equation, Journal of Mathematical Analyi and Application, vol. 27, no. 2, pp , 22. [4 J. R. Graef and B. Yang, On a nonlinear boundary value problem for fourth order equation, Applicable Analyi, vol. 72, no. 3 4, pp , [5 Z. Hao, L. Liu, and L. Debnath, A neceary and ufficient condition for the exitence of poitive olution of fourth-order ingular boundary value problem, Applied Mathematic Letter, vol. 16, no. 3, pp , 23. [6 F. Li, Q. Zhang, and Z. Liang, Exitence and multiplicity of olution of a kind of fourth-order boundary value problem, Nonlinear Analyi: Theory, Method & Application,vol.62,no.5,pp , 25. [7 B. Liu, Poitive olution of fourth-order two point boundary value problem, Applied Mathematic and Computation, vol. 148, no. 2, pp , 24. [8 D. Yang, H. Zhu, and C. Bai, Poitive olution for emipoitone fourth-order two-point boundary value problem, Electronic Journal of Differential Equation, no. 16, pp. 1 8, 27. [9 R. Ma, Poitive olution of fourth-order two-point boundary value problem, Annal of Differential Equation, vol. 15, no. 3, pp , [1 P. J. Torre, Exitence of one-igned periodic olution of ome econd-order differential equation via a Kranoel kii fixed point theorem, JournalofDifferential Equation, vol. 19, no. 2, pp , 23. [11 M. A. Kranoel kii, Poitive Solution of Operator Equation, P. Noordhoff, Groningen, The Netherland, Chuanzhi Bai: Department of Mathematic, Huaiyin Teacher College, Huaian 2233, China addre: czbai8@ohu.com
EXISTENCE AND UNIQUENESS THEOREM FOR FRACTIONAL DIFFERENTIAL EQUATION WITH INTEGRAL BOUNDARY CONDITION
Journal of Fractional Calculu and Application, Vol. 3, July 212, No. 6, pp. 1 9. ISSN: 29-5858. http://www.fcaj.web.com/ EXISTENCE AND UNIQUENESS THEOREM FOR FRACTIONAL DIFFERENTIAL EQUATION WITH INTEGRAL
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
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
Deterministic Policy Gradient Algorithms: Supplementary Material
Determinitic Policy Gradient lgorithm: upplementary Material. Regularity Condition Within the text we have referred to regularity condition on the MDP: Regularity condition.1: p(, a), a p(, a), µ θ (),
SURVEY AND NEW RESULTS ON BOUNDARY-VALUE PROBLEMS OF SINGULAR FRACTIONAL DIFFERENTIAL EQUATIONS WITH IMPULSE EFFECTS
Electronic Journal of Differential Equation, Vol. 26 26, No. 296, pp. 77. ISSN: 72-669. URL: http://ejde.math.txtate.edu or http://ejde.math.unt.edu SURVEY AND NEW RESULTS ON BOUNDARY-VALUE PROBLEMS OF
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
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,
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
Research Article Existence of Positive Solutions for m-point Boundary Value Problems on Time Scales
Hindawi Publishing Corporation Discrete Dynamics in Nature and Society Volume 29, Article ID 189768, 12 pages doi:1.1155/29/189768 Research Article Existence of Positive Solutions for m-point Boundary
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
Exercises 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
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
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.
( ) ( 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
Periodic oluion of van der Pol differenial equaion. by A. Arimoo Deparmen of Mahemaic Muahi Iniue of Technology Tokyo Japan in Seminar a Kiami Iniue of Technology January 8 9. Inroducion Le u conider a
( P) det. constitute the cofactor matrix, or the matrix of the cofactors: com P = c. ( 1) det
Aendix C Tranfer Matrix Inverion To invert one matrix P, the variou te are a follow: calculate it erminant ( P calculate the cofactor ij of each element, tarting from the erminant of the correonding minor
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
EXISTENCE OF POSITIVE SOLUTIONS FOR SINGULAR FRACTIONAL DIFFERENTIAL EQUATIONS
Electronic Journal of Differential Equations, Vol. 28(28), No. 146, pp. 1 9. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp) EXISTENCE
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
HOMEWORK 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
3.4 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
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
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
On mean-field stochastic maximum principle for near-optimal controls for Poisson jump diffusion with applications
Int. J. Dynam. Control 04) :6 84 DOI 0.007/40435-03-0040-y On mean-field tochatic maximum principle for near-optimal control for Poion jump diffuion with application Mokhtar Hafayed Abdelmadjid Abba Syed
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
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
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
Mellin transforms and asymptotics: Harmonic sums
Mellin tranform and aymptotic: Harmonic um Phillipe Flajolet, Xavier Gourdon, Philippe Duma Die Theorie der reziproen Funtionen und Integrale it ein centrale Gebiet, welche manche anderen Gebiete der Analyi
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,
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
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 :
MINIMAL CLOSED SETS AND MAXIMAL CLOSED SETS
MINIMAL CLOSED SETS AND MAXIMAL CLOSED SETS FUMIE NAKAOKA AND NOBUYUKI ODA Received 20 December 2005; Revised 28 May 2006; Accepted 6 August 2006 Some properties of minimal closed sets and maximal closed
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
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
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)
On Numerical Radius of Some Matrices
International Journal of Mathematical Analysis Vol., 08, no., 9-8 HIKARI Ltd, www.m-hikari.com https://doi.org/0.988/ijma.08.75 On Numerical Radius of Some Matrices Shyamasree Ghosh Dastidar Department
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
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
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
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
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
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
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
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
Section 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)
The Negative Neumann Eigenvalues of Second Order Differential Equation with Two Turning Points
Applied Mathematical Sciences, Vol. 3, 009, no., 6-66 The Negative Neumann Eigenvalues of Second Order Differential Equation with Two Turning Points A. Neamaty and E. A. Sazgar Department of Mathematics,
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) =
PROPERTIES OF CERTAIN INTEGRAL OPERATORS. a n z n (1.1)
GEORGIAN MATHEMATICAL JOURNAL: Vol. 2, No. 5, 995, 535-545 PROPERTIES OF CERTAIN INTEGRAL OPERATORS SHIGEYOSHI OWA Abstract. Two integral operators P α and Q α for analytic functions in the open unit disk
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
arxiv: v3 [math.ca] 4 Jul 2013
POSITIVE SOLUTIONS OF NONLINEAR THREE-POINT INTEGRAL BOUNDARY-VALUE PROBLEMS FOR SECOND-ORDER DIFFERENTIAL EQUATIONS arxiv:125.1844v3 [math.ca] 4 Jul 213 FAOUZI HADDOUCHI, SLIMANE BENAICHA Abstract. We
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
A Two-Sided Laplace Inversion Algorithm with Computable Error Bounds and Its Applications in Financial Engineering
Electronic Companion A Two-Sie Laplace Inversion Algorithm with Computable Error Bouns an Its Applications in Financial Engineering Ning Cai, S. G. Kou, Zongjian Liu HKUST an Columbia University Appenix
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
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) =
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:
w 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:
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
The k-α-exponential Function
Int Journal of Math Analysis, Vol 7, 213, no 11, 535-542 The --Exponential Function Luciano L Luque and Rubén A Cerutti Faculty of Exact Sciences National University of Nordeste Av Libertad 554 34 Corrientes,
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.
Approximation of the Lerch zeta-function
Approximaion of he Lerch zea-funcion Ramūna Garunkši Deparmen of Mahemaic and Informaic Vilniu Univeriy Naugarduko 4 035 Vilniu Lihuania ramunagarunki@mafvul Abrac We conider uniform in parameer approximaion
Turkish Journal of I N E Q U A L I T I E S
Turkih J Ineq, ) 7), Page 6 37 Turkih Journal of I N E Q U A L I T I E S Available online at wwwtjinequalitycom PARAMETERIZED HERMITE-HADAMARD TYPE INEQUALITIES FOR FRACTIONAL INTEGRALS M ADIL KHAN AND
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
ES440/ES911: CFD. Chapter 5. Solution of Linear Equation Systems
ES440/ES911: CFD Chapter 5. Solution of Linear Equation Systems Dr Yongmann M. Chung http://www.eng.warwick.ac.uk/staff/ymc/es440.html Y.M.Chung@warwick.ac.uk School of Engineering & Centre for Scientific
Problem Set 3: Solutions
CMPSCI 69GG Applied Information Theory Fall 006 Problem Set 3: Solutions. [Cover and Thomas 7.] a Define the following notation, C I p xx; Y max X; Y C I p xx; Ỹ max I X; Ỹ We would like to show that C
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
New bounds for spherical two-distance sets and equiangular lines
New bounds for spherical two-distance sets and equiangular lines Michigan State University Oct 8-31, 016 Anhui University Definition If X = {x 1, x,, x N } S n 1 (unit sphere in R n ) and x i, x j = a
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
Fractional 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
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
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
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
derivation 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
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
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
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
On the Galois Group of Linear Difference-Differential Equations
On the Galois Group of Linear Difference-Differential Equations Ruyong Feng KLMM, Chinese Academy of Sciences, China Ruyong Feng (KLMM, CAS) Galois Group 1 / 19 Contents 1 Basic Notations and Concepts
A Bonus-Malus System as a Markov Set-Chain. Małgorzata Niemiec Warsaw School of Economics Institute of Econometrics
A Bonus-Malus System as a Markov Set-Chain Małgorzata Niemiec Warsaw School of Economics Institute of Econometrics Contents 1. Markov set-chain 2. Model of bonus-malus system 3. Example 4. Conclusions
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
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
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
2. 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.
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
TMA4115 Matematikk 3
TMA4115 Matematikk 3 Andrew Stacey Norges Teknisk-Naturvitenskapelige Universitet Trondheim Spring 2010 Lecture 12: Mathematics Marvellous Matrices Andrew Stacey Norges Teknisk-Naturvitenskapelige Universitet
BOUNDARY VALUE PROBLEMS FOR DISCRETE FRACTIONAL EQUATIONS
University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln Dissertations, Theses, and Student Research Papers in Mathematics Mathematics, Department of 8-212 BOUNDARY VALUE PROBLEMS
Finite difference method for 2-D heat equation
Finite difference method for 2-D heat equation Praveen. C praveen@math.tifrbng.res.in Tata Institute of Fundamental Research Center for Applicable Mathematics Bangalore 560065 http://math.tifrbng.res.in/~praveen
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
Arithmetical applications of lagrangian interpolation. Tanguy Rivoal. Institut Fourier CNRS and Université de Grenoble 1
Arithmetical applications of lagrangian interpolation Tanguy Rivoal Institut Fourier CNRS and Université de Grenoble Conference Diophantine and Analytic Problems in Number Theory, The 00th anniversary
( )( ) ( ) ( )( ) ( )( ) 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
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 +
The challenges of non-stable predicates
The challenges of non-stable predicates Consider a non-stable predicate Φ encoding, say, a safety property. We want to determine whether Φ holds for our program. The challenges of non-stable predicates
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
( 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
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
k A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +
Chapter 3. Fuzzy Arithmetic 3- Fuzzy arithmetic: ~Addition(+) and subtraction (-): Let A = [a and B = [b, b in R If x [a and y [b, b than x+y [a +b +b Symbolically,we write A(+)B = [a (+)[b, b = [a +b
Quadratic Expressions
Quadratic Expressions. The standard form of a quadratic equation is ax + bx + c = 0 where a, b, c R and a 0. The roots of ax + bx + c = 0 are b ± b a 4ac. 3. For the equation ax +bx+c = 0, sum of the roots
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
Section 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
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
= 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).
Worked Soluion 95 Chaper 25: The Invere Laplace Tranform 25 a From he able: L ] e 6 6 25 c L 2 ] ] L! + 25 e L 5 2 + 25] ] L 5 2 + 5 2 in(5) 252 a L 6 + 2] L 6 ( 2)] 6L ( 2)] 6e 2 252 c L 3 8 4] 3L ] 8L
Differentiation exercise show differential equation
Differentiation exercise show differential equation 1. If y x sin 2x, prove that x d2 y 2 2 + 2y x + 4xy 0 y x sin 2x sin 2x + 2x cos 2x 2 2cos 2x + (2 cos 2x 4x sin 2x) x d2 y 2 2 + 2y x + 4xy (2x cos
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