Uncertain Dynamic Systems on Time Scales
|
|
- Winfred Fisher
- 5 years ago
- Views:
Transcription
1 Journl of Uncertin Sytem Vol.9, No.1, pp.17-30, 2015 Online t: Uncertin Dynmic Sytem on Time Scle Umber Abb Hhmi, Vile Lupulecu, Ghu ur Rhmn Abdu Slm School of Mthemticl Science, GCU Lhore Univerity Contntin Brncui, Str. Genev, Nr. 3, Trgu Jiu, Romni Received 28 Jnury 2013; Revied 13 Augut 2013 Abtrct In thi pper we tudy the exitence nd uniquene of the olution for the dynmic ytem on time cle with uncertin prmeter. For thi im, we introduced the notion of uncertin proce on time cle. In ddition, the liner dynmic ytem on time cle with uncertin prmeter re lo tudied. c 2015 World Acdemic Pre, UK. All right reerved. Keyword: differentil eqution, time cle, uncertin meure, uncertin proce, exitence nd uniquene, finnce, uncertin inference 1 Introduction The uncertin theory w introduced by Liu [14] n importnt tool for the tudy of ome rel world phenomen which cnnot be modeled by fuzzine. The min tge on the development of thi theory nd ome fundmentl reult cn be found in work [7, 14, 15, 16, 22]. The concept of uncertin differentil eqution w lo introduced in [14], but the exitence nd uniquene of the olution of thi kind of differentil eqution w obtined by Chen nd Liu in the work [6]. The theory of dynmic ytem on time cle imultneouly llow u to tudy continuou nd dicrete dynmic ytem. Since Hilger initil work [10] there h been ignificnt growth in the theory of dynmic ytem on time cle, covering vriety of different qulittive pect. The clculu of time cle w initited by B. Aulbch nd S. Hilger in order to crete theory tht cn unify dicrete nd continuou nlyi. We refer to the book [4, 5], nd the pper [1, 2, 21] which re more pecific with repect to our trget. Hoffcker [12], Ahlbrndt nd Morin [3] re known tht hve been worked nd demontrted the relted ide to the multivrite ce nd the tudy of prtil dynmic eqution (PDE), however, thee ide re lredy known for univrite ce of dynmic eqution [13]. The uncertin dynmic ytem re widely ued for olving different problem, nd thi technique i rther well developed. A lot of cientific work re dedicted to the development of thi method [2, 4, 5, 6, 10, 11]. Mny intereting nd importnt reult hve been obtined in thi field by different uthor. Depite of thi fct there till remin lot of unolved problem. For filling thee gp, in thi rticle we conider problem of uncertin dynmic ytem on time cle. It i well known tht the mthemticl model re necery to be ble to tudy the rel world ytem. Thee model involve different prmeter whoe vlue re determined by meurement. Even when the meurement re mde by modern technologie the end reult i tht the vlue of the prmeter re different from one meurement to nother. Depending on the nture of the vlue obtined from the meurement, the vrition of the prmeter cn be conidered to be rndom vrible, fuzzy rndom vrible or uncertin vrible. Moreover, the time vrition of the prmeter cn be continuou, dicrete, or my lternte from one time intervl to nother. In the ltter ce, the mthemticl model on time cle pper nturl one. The purpoe of thi pper i to prove the exitence nd uniquene of olution for the dynmic ytem on time cle with uncertin prmeter. The orgniztion of thi pper i follow. Section 2 preent few definition nd concept of time cle. Alo, the notion of uncertin proce on time cle i introduced. In Section 3 we prove the exitence nd uniquene of olution for the dynmic ytem on time cle with Correponding uthor. Emil: umberbb@yhoo.com (U.A. Hhmi).
2 18 U.A. Hhmi et l.: Uncertin Dynmic Sytem on Time Scle uncertin prmeter. In the lt ection, we tudy the liner dynmic ytem on time cle with uncertin prmeter. 2 Preliminry 2.1 Time Scle By time cle T we men ny cloed ubet of R. Then T i complete metric pce with the metric defined by d(t, ) := t for t, T. Since we know tht for working into the different connected component of the time cle T, we need the concept of jump opertor. The forwrd jump opertor σ : T T i defined by σ(t) := inf T : > t}, while the bckwrd jump opertor ρ : T T i defined by ρ(t) := up T : < t}. In thi definition we put inf = up T nd up = inf T. The grinine function µ : T [0, ) i defined by µ(t) := σ(t) t. If σ(t) > t, we y t i right-cttered point, while if ρ(t) < t, we y t i left-cttered point. Point tht re right-cttered nd left-cttered t the me time will be clled iolted point. A point t T uch tht t < up T nd σ(t) = t, i clled right-dene point. A point t T uch tht t > inf T nd ρ(t) = t, i clled left-dene point. Point tht re right-dene nd left-dene t the me time will be clled dene point. The et T κ i defined to be T κ = T\m} if T h left-cttered mximum m, otherwie T κ = T. To undertnd the notion we hve to conider ome exmple for clering the btrction of the itution. Given time cle intervl [, b] T := t T : t b}, then [, b] κ T denoted the intervl [, b] T if < ρ(b) = b nd denote the intervl [, b) T if < ρ(b) < b. In fct, [, b) T = [, ρ(b)] T. Alo, for T, we define [, ) T = [, ) T. If T i bounded time cle, then T cn be identified with [inf T, up T] T. If T nd δ > 0, then we define the following neighborhood of : U T (, δ) := ( δ, + δ) T, U + T (, δ) := [, + δ) T, nd U T (, δ) := ( δ, ] T. Let R m be the pce of m-dimenionl column vector x = col(x 1, x 2,..., x m ) with norm. Definition 2. 1 ([4]) A function f : T R m i clled regulted if it right-ided limit exit (finite) t ll right-dene point in T, nd itleft-ided limit exit (finite) t ll left-dene point in T. A function f : T R m i clled rd-continuou if it i continuou t ll right-dene point in T nd it left-ided limit exit (finite) t ll left-dene point in T. Denote by C rd (T, R m ) the et of ll rd-continuou function from T into R m. Obviouly, continuou function i rd-continuou, nd rd-continuou function i regulted ([4, Theorem 1.60]). Definition 2. 2 ([4]) A function f : [, b] T R m R m i clled Hilger continuou if f i continuou t ech point (t, x) where t i right-dene, nd the limit lim f(, y) nd (,y) (t,x) both exit nd re finite t ech point (t, x) where t i left-dene. lim f(t, y) y x Definition 2. 3 ([4]) Let f : T R m nd t T κ. Let f (t) R m (provided it exit) with the property tht for every ε > 0, there exit δ > 0 uch tht f(σ(t)) f() f (t)[σ(t) ] ε σ(t) (1) for ll U T (t, δ). We cll f (t) the delt (or Hilger) derivtive ( -derivtive for hort) of f t t. Moreover, we y tht f i delt differentible ( -differentible for hort) on T κ provided f(t) exit for ll t T κ. The following reult will be very ueful. Propoition 2. 1 ([4, Theorem 1.16]) Aume tht f : T R m nd t T κ. (i) If f i -differentible t t, then f i continuou t t. (ii) If f i continuou t t nd t i right-cttered, then f i -differentible t t with f (t) = f(σ(t)) f(t). σ(t) t
3 Journl of Uncertin Sytem, Vol.9, No.1, pp.17-30, (iii) If f i -differentible t t nd t i right-dene, then f f(t) f() (t) = lim. t t (iv) If f i -differentible t t, then f(σ(t)) = f(t) + µ(t)f (t). It i known [9] tht for every δ > 0 there exit t let one prtition P : = < t 1 < < t n = b of [, b) T uch tht for ech i 1, 2,..., n} either t i t i 1 δ or t i t i 1 > δ nd ρ(t i ) = t i 1. For given δ > 0 we denote by P([, b) T, δ) the et of ll prtition P : = < t 1 < < t n = b tht poe the bove property. Let f : T R m be bounded function on [, b) T, nd let P : = < t 1 < < t n = b be prtition of [, b) T. In ech intervl [t i 1, t i ) T,where 1 i n, we chooe n rbitrry point ξ i nd form the um S = n (t i t i 1 )f(ξ i ). We cll S Riemnn -um of f correponding to the prtition P. i=1 Definition 2. 4 ([8]) We y tht f i Riemnn -integrble from to b (or on [, b) T ) if there exit vector I R m with the following property: for ech ε > 0 there exit δ > 0 uch tht S I < ε for every Riemnn -um S of f correponding to prtition P P([, b) T, δ) independent of the wy in which we chooe ξ i [t i 1, t i ) T, i = 1, 2,..., n. It i eily een tht uch vector I i unique. The vector I R m i the Riemnn -integrl of f from to b, nd we will denote it by b f(t) t. Propoition 2. 2 ([8, Theorem 5.8]) A bounded function f : [, b) T R m i Riemnn -integrble on [, b) T if nd only if the et of ll right-dene point of [, b) T t which f i dicontinuou i et of meure zero. Since every regulted function on compct intervl i bounded (ee [4, Theorem 1.65]), o, we get tht every regulted function f : [, b] T R m, i Riemnn -integrble from to b. Propoition 2. 3 ([11, Theorem 5.8]) Aume tht, b T, < b nd f : T R m i rd-continuou. Then the integrl h the following propertie. (i) If T = R, then b f(t) t = b f(t)dt, where the integrl on the right-hnd ide i the Riemnn integrl. (ii) If T conit of iolted point, then b f(t) t = t [,b) T µ(t)f(t). Definition 2. 5 ([4]) A function g : T R m i clled -ntiderivtive of f : T R m if g (t) = f(t) for ll t T κ. Bohner exclimed tht ech rd-continuou function h -ntiderivtive [4, Theorem 1.74]. Propoition 2. 4 ([8, Theorem 4.1]) Let f : T R m be Riemnn -integrble function on [, b) T. If f h -ntiderivtive g : [, b] T R m, then b f(t) t = g(b) g(). In prticulr, σ(t) f() = µ(t)f(t) for t ll t [, b) T (ee [4, Theorem 1.75]). Propoition 2. 5 ([8, Theorem 4.3]) Let f : T R m be function which i Riemnn -integrble from to b. For t [, b] T, let g(t) = f(t) t. Then g i continuou on [, b] T. Further, let [, b) T nd let f be rbitrry t if i right-cttered, nd let f be continuou t if i right-dene. Then g i -differentible t nd g ( ) = f( ). Lemm 2. 1 ([21]) Let g : R R be continuou nd nondecreing function. If, t T with t, then g(τ) τ g(τ)dτ. Severl of the propertie of the Riemnn -integrl re dicued in [1, 4].
4 20 U.A. Hhmi et l.: Uncertin Dynmic Sytem on Time Scle 2.2 Uncertin Proce on Time Scle Let Γ be n nonempty et nd let L be σ-lgebr of et of Γ. A mpping M : L [0, 1] i clled uncertin meure if it tifie the following xiom: (A1) M(Γ) = 1; (A2) M(A) M(B) for ll A, B L with A B; (A3) M(A) + M(A c ) = 1 for ll A L, where A c := Γ\A; (A4) For every countble equence A n } of element of L, we hve ( ) M A n = M (A n ). n=1 n=1 Let Γ be nonempty et, L σ-lgebr on Γ, nd M n uncertin meure. T he triplet (Γ, L, M) i clled n uncertin pce. Exmple 2. 1 Let u conider Γ = (0, 1), L the σ-lgebr of ll Borel ubet of Γ. Let λ : (0, 1) R + be defined by λ(x) = x 1 2, x (0, 1). Then the mpping M : L [0, 1] defined by M(A) = upλ(x), x A 1 up x A c λ(x), if upλ(x) < 1/2 x A if upλ(x) 1/2, x A i n uncertin meure on (0, 1). Denote by B the σ-lgebr of ll Borel ubet of R m. A function X( ) : Γ R m i clled n uncertin vrible if X i meurble function from (Γ, F) into (R m, B), tht i, X 1 (B) := γ Γ; X(γ) B} L for ll B B. A time cle uncertin proce i function X(, ) : [, b] T Γ R m uch tht X(t, ) : Γ R m i uncertin vrible for ech t T. For ech point γ Γ, the function on T given by t X(t, γ) i will be clled mple pth of the time cle uncertin proce X(, ) correponding to γ. A time cle uncertin proce X(, ) i id to be regulted (rd-continuou, continuou) if the trjectory t X(t, γ) i regulted (rd-continuou, continuou) function on [, b] T for ech γ Γ. Lemm 2. 2 Let X(, ) : [, b] T Γ R m be time cle uncertin proce. If the mple pth t X(t, γ) i Riemnn -integrble on [, b) T for every γ Γ, then the function Y (, ) : [, b] T Γ R m given by Y (t, γ) = i continuou time cle uncertin proce. X(, γ), t [, b] T Proof: From Propoition 2.5, it follow tht the function t X(, γ) i continuou for ech γ Γ. Since the Riemnn -integrl i limit of the finite um S (γ) = n i=1 (t i t i 1 )X(ξ i, γ) of meurble function, we hve tht γ X(, γ) i meurble function. Therefore, Y (, ) i continuou time cle uncertin proce.
5 Journl of Uncertin Sytem, Vol.9, No.1, pp.17-30, Uncertin Initil Vlue Problem In the following, conider n initil vlue problem of the form X (t, γ) = F (t, X(t, γ), γ), t [, b] κ T X(, γ) = X 0 (γ), (2) where X 0 : Γ R m i uncertin vrible nd F : [, b] κ T Rm Γ R m tifie the following umption: (H1) F (t, x, ) : Γ R m i uncertin vrible for ll (t, x) [, b] κ T Rm, (H2) for ech γ Γ, the function F (,, γ) : [, b] κ T Rm R m i Hilger continuou function t every point (t, x) [, b] κ T Rm. By olution of (2) we men time cle uncertin proce X(, ) : [, b] κ T Γ Rm tht tifie condition in (2). Remrk 1: Conider the uncertin differentil Eqution (2) fmily (with repect to prmeter γ) of determinitic differentil eqution, nmely X (t, γ) = F (t, X(t, γ), γ), t [, b] κ T, γ Γ, (3) X(, γ) = X 0 (γ). Then i not correct to olve ech problem (3) to obtin the olution of (2). Let u give two exmple. Exmple 3. 1 Let (Γ, L, M) be n uncertin pce. Conider n initil vlue problem of the form X (t, γ) = K(γ)X 2 (t, γ), t [0, ) R, γ Γ, X(0, γ) = 1, (4) where K : Γ (0, ) i uncertin vrible. It i ey to ee tht, for ech γ Γ, X(t, γ) = 1/(1 K(γ)t) i olution of (4) on the intervl [0, 1/K(γ)]. Since for ech 0 we hve tht M(1/K(γ) > ) < 1, it follow tht not ll olution X(, γ) re well defined on ome common intervl [0, ). Exmple 3. 2 Let (Γ, L, M) be n uncertin pce nd let Γ 0 / L. It i ey to check tht, for ech γ Γ, the function X(, ) : [0, 1] R Γ R, given by 0 if γ Γ0 X(t, γ) = t 3/2 if γ Γ\Γ 0, i olution of the initil vlue problem X (t, γ) = 3 2 X(t, γ), t [0, ) R, γ Γ, X(0, γ) = 0. But X(, ) i not uncertin proce. Indeed, we hve tht tht i, γ X(1, γ) i not meurble function. γ Γ; X(1, γ) [ 1 2, 1 2 ]} = Γ 0 / L, Uing the Propoition 4 nd 5 nd [21, Lemm 2.3], it i ey to prove the following reult. Lemm 3. 3 A time cle uncertin proce X(, ) : [, b] κ T Γ Rm i the olution of the problem (2) if nd only if X(, ) i continuou time cle uncertin proce nd it tifie the following uncertin integrl eqution X(t, γ) = X 0 (γ) + F (, X(, γ), γ), t [, b] T, γ Γ. (5) The following reult i known Gronwll inequlity on time cle nd will be ued in thi pper.
6 22 U.A. Hhmi et l.: Uncertin Dynmic Sytem on Time Scle Lemm 3. 4 ([21, Lemm 3.1]) Let rd-continuou time cle uncertin procee X(, ), Y (, ) : [, b] κ T Γ R + be uch tht X(t, γ) Y (t, γ) + where 1 + µ(t)p(t) > 0, for ll t [, b] T. Then we hve X(t, γ) Y (t, γ) + q()x(, γ), t [, b] T, γ Γ, e p (t, σ()p()y (, γ), t [, b] T, γ Γ. Theorem 3. 1 Let F : [, b] κ T Rm Γ R m tifie (H1)-(H2) nd ume tht there exit rd-continuou time cle uncertin proce L(, ) : [, b] κ T Γ R + uch tht F (t, x, γ) F (t, y, γ) L(t, γ) x y (6) for every t [, b] κ T, x, y Rm nd γ Γ. Let X 0 : Γ R m uncertin vrible uch tht F (t, X 0 (γ), γ) M, t [, b] κ T, γ Γ, (7) where M > 0 i contnt. Then the problem (2) h unique olution. Proof: To prove the theorem we pply the method of ucceive pproximtion (ee [21]). For thi, we define equence of function X n (, ) : [, b] κ T Γ Rm, n N, follow: X 0 (t, γ) = X 0 (γ) X n (t, γ) = X 0 (γ) + F (, X n 1 (, γ), γ), n 1, for every t [, b] κ T nd every γ Γ. Firt, uing (7) nd the Lemm 2.1, we oberve tht (8) X 1 (t, γ) X 0 (t, γ) F (, X 0 (γ), γ) M(t ) M(b ), t [, b] T, γ Γ. We prove by induction tht for ech integer n 2 the following etimte hold (t )n (b )n X n (t, γ) X n 1 (t, γ) M L(γ) M L(γ), t [, b] T, γ Γ, (9) n! n! where L(γ) = up L(t, γ). Suppoe tht (9) hold for n = k 2. Then, uing (6), (7) nd Lemm 2.1, we [,b] T obtin X k+1 (t, γ) X k (t, γ) L(γ) X k (, γ) X k 1 (, γ) L(γ) M k! L(γ) M k! F (, X k (, γ), γ) F (, X k 1 (, γ), γ) ( ) k ( ) k (t )k+1 (b )k+1 d = M L(γ) (k+1)! M L(γ) (k+1)!, for ll t [, b] T nd γ Γ. Thu, (9) i true for n = k + 1 nd o (9) hold for ll n 2. Further, we how tht for every n N the function X n (, γ) : [, b] T R re continuou for ech γ Γ. Let ε > 0 nd t, [, b] T be uch tht t < ε/m. We hve X 1 (t, γ) X 1 (, γ) = F (τ, X 0 (γ), γ) τ F (τ, X 0 (γ), γ) τ = t F (τ, X 0 (γ), γ) τ F (τ, X 0 (γ), γ) τ F (τ, X 0 (γ), γ) dτ M t < ε
7 Journl of Uncertin Sytem, Vol.9, No.1, pp.17-30, nd o t X 1 (t, γ) i continuou on [, b] T for ech γ Γ. Since for ech n 2 X n (t, γ) X n (, γ) + + n 1 F (τ, X n 1 (τ, γ), γ) τ F (τ, X n 1 (τ, γ), γ) F (τ, X 0 (γ), γ) τ k=1 then, by induction, we obtin F (τ, X k (τ, γ), γ) F (τ, X k 1 (τ, γ), γ) τ, X n (t, γ) X n (, γ) M ( 1 + n 1 k=1 L(γ) k 1 (b ) k k! F (τ, X 0 (γ), γ) τ F (τ, X 0 (γ), γ) τ ) t 0 t. Therefore, for every n N the function X n (, γ) : [, b] T Γ R m i continuou for ech γ Γ. Now, uing Lemm 3.3 nd (8), we deduce tht the function X n (t, ) : Γ R m re meurble. Conequently, it follow tht for every n N the function X n (, ) : [, b] T Γ R i time cle uncertin proce. Further, we hll how tht the equence (X n (t, )) n N i uniformly convergent. Denote Since Y n (t, γ) = X n+1 (t, γ) X n (t, γ), n N, γ Γ. Y n (t, γ) Y n (, γ) L(γ) X n (τ, γ) X n 1 (τ, γ) τ then, reoning bove, we deduce tht the function t Y n (t, γ) re continuou on [, b] T for ech γ Γ. Now, uing (9), we obtin n 1 up X n (t, γ) X m (t, γ) t [,b] T for ll n > m > 0. Since the erie uch tht n=1 k=m up Y k (t, γ) M t [,b] T n 1 k=m L(γ) k (b ) k+1 (k + 1)! L(γ) n 1 (b ) n /n! converge, then for ech ε > 0 there exit n 0 N up X n (t, γ) X m (t, γ) ε for ll n, m n 0 nd γ Γ. (10) t [,b] T Hence, ince ([, b] T, ) i complete metric pce, it follow tht the equence (X n (t, )) n N i uniformly convergent on [, b] T. Denote X(t, γ) = lim X n(t, γ), t [, b] T, γ Γ. Obviouly, t X(t, γ) i continuou n on [, b] T for ech γ Γ. Since, by Lemm 2.2 nd (8), the function γ X n (, γ) re meurble nd X(t, γ) = lim X n(t, γ) for every t [, b] T nd γ Γ, we deduce tht γ X(t, γ) i meurble for every n t [, b] T. Therefore, X(, ) : [, b] T Γ R m i continuou time cle uncertin proce. We how tht X(, ) tifie the uncertin integrl eqution (5). For ech n N we put G n (t, γ) = F (t, X n (t, γ), γ), t [, b] T, γ Γ. Then G n (t, γ) i rd-continuou time cle uncertin proce, nd we hve tht up G n (t, γ) G m (t, γ) L(γ) up X n (t, γ) X m (t, γ), t [, b] T, γ Γ, t [,b] T t [,b] T for ll n, m n 0. Uing (10) we infer tht the equence (G n (, γ)) n N i uniformly convergent on [, b] T for ech γ Γ. If we tke m, then for ech ε > 0 there exit n 0 N uch tht for every n n 0 we hve up G n (t, γ) F (t, X(t, γ), γ) L(γ) up X n (t, γ) X(t, γ), t [, b] T, γ Γ, t [,b] T t [,b] T nd o lim G n(t, γ) F (t, X(t, γ), γ) = 0 for ll t [, b] T nd γ Γ. Alo, it ey to ee tht n up G n (, γ) F (, X(, γ), γ) t [,b] T L(γ) X n (, γ) X(, γ), γ Γ.
8 24 U.A. Hhmi et l.: Uncertin Dynmic Sytem on Time Scle Since X(t, γ) = lim n X n(t, γ) uniformly on [, b] T, then it follow tht Now, we hve lim n G n (, γ) = F (, X(, γ), γ) for ll t [, b] nd γ Γ. up X(t, γ) X 0(γ) F (, X(, γ), γ) up X(t, γ) X n (t, γ) t [,b] T t [,b] T + up X n(t, γ) X 0 (γ) F (, X n 1 (, γ), γ) t [,b] T + up F (, X n 1 (, γ), γ) F (, X(, γ), γ). t [,b] T Uing the two previou convergence X(t, γ) = X 0 (γ) + F (, X(, γ), γ) for ll t [, b] T nd γ Γ, tht i, X(, ) tifie the uncertin integrl Eqution (5). Then, by Lemm 3.3, it follow tht X(, ) i the olution of the problem (2). Finlly, we how the uniquene of the olution. For thi, we ume tht X(, ), Y (, ) : [, b] T Γ R m re two olution of (5). Since X(t, γ) Y (t, γ) L(γ) X(, γ) Y (, γ) d, t [, b] T, γ Γ, from Lemm 3.4 it follow tht X(t, γ) Y (t, γ) 0, t [, b] T, γ Γ, nd o, the proof i complete. Let T be upper unbounded time cle. Under uitble condition we cn extend the notion of the olution of (2) from [, b] κ T to [, ) T := [, ) T, if we define F on [, ) T R m Γ nd how tht the olution exit on ech [, b] T where b (, ) T, < ρ(b). Theorem 3. 2 Aume tht F : [, ) T R m Γ R m tifie the umption of the Theorem 3.1 on ech intervl [, b] T with b (, ) T, < ρ(b). If there i contnt M > 0 uch tht F (t, x, γ) M for ll (t, x) [, b) T R m then the problem (2) h unique olution on [, ) T. Proof: Let X(, ) be the olution of (2) which exit on [, b) T with b (, ) T, < ρ(b), nd the vlue of b cnnot be increed. Firt, we oberve tht b i left-cttered point, then ρ(b) (, b) T nd the olution X(, ) exit on [, ρ(b)] T. But then the olution X(, ) exit lo on [, b] T, nmely by putting X(b, γ) = X(ρ(b), γ) + µ(b)x (ρ(b), γ) = X(ρ(b), γ) + µ(b)f (ρ(b), X(ρ(b), γ), γ). If b i left-dene point, then their neighborhood contin infinitely mny point to the left of b. Then, for ny t, (, b) T uch tht < t, we hve X(t, γ) X(, γ) F (τ, X(τ, γ), γ) τ M t. Tking limit, t b nd uing Cuchy criterion for convergence, it follow lim t b X(t, γ) exit nd i finite. Further, we define X b (γ) = lim X(t, γ) nd conider the initil vlue problem t b X (t, γ) = F (τ, X(τ, γ), γ), t [b, b 1 ] T, b 1 > σ(b), X(b, γ) = X b (γ). By Theorem 3.1, one get tht X(t, γ) cn be continued beyond b, contrdicting our umption. Hence every olution X(t, γ) of (2) exit on [, ) T nd the proof i complete.
9 Journl of Uncertin Sytem, Vol.9, No.1, pp.17-30, Uncertin Liner Sytem Let : Γ R be poitively regreive uncertin vrible, tht i, 1 + µ(t)(γ) > 0 for ll γ Γ. Then, by Lemm 2.2, the function (t, γ) e (γ) (t, ) defined by ( ) log(1 + µ(τ)(γ)) e (γ) (t, ) = τ,, t T, γ Γ, µ(τ) i continuou time cle uncertin proce. For ech fixed γ Γ, the mple pth t e (γ) (t, ) i the exponentil function on time cle (ee [4]). It ey to check tht the uncertin proce (t, γ) e (γ) (t, ) i olution of the initil vlue problem (for determinitic ce, ee [4, Theorem 2.33]): X (t, γ) = (γ)x(t, γ), t [, b] κ T, γ Γ, (11) X(, γ) = 1. If : Γ R i bounded then, by the Theorem 3.1 nd 3.2, it follow tht (11) h unique olution on [, ) T. Let u denote by M m (R) the pce of ll m m mtrice. We recll tht A := up Ax ; x 1} define norm on M m (R) nd the following inequlity Ax A x hold for ll A M m (R) nd x R m. A mpping A : Γ M m (R) i clled n uncertin mtrix if ll it component ij : Γ R, i, j = 1, 2,..., m, re uncertin vrible. An uncertin mtrix A i id to be regreive if I +µ(t)a(γ) i invertible for ll t T nd γ Γ, where I i the m m identity mtrix. Moreover, the et R m = R(Γ, M m (R)) of ll regreive uncertin mtrice i group with repect to the ddition opertion define A B = A + B + µ(t)ab for ll t T. The invere element of A R m i given by A = [I + µ(t)a 1 ]A = A[I + µ(t)a] 1 for ll t T. Now conider the following homogeneou liner uncertin initil vlue problem X (t, γ) = A(γ)X(t, γ), t T, γ Γ, X(, γ) = X 0 (γ). (12) where A R m. The correponding nonhomogeneou liner uncertin initil vlue problem i X (t, γ) = A(γ)X(t, γ) + H(t, γ), t T, γ Γ, X(, γ) = X 0 (γ). (13) where H : T Γ R m i n uncertin proce. Theorem 4. 1 Suppoe tht A : Γ M m (R) i regreive nd bounded uncertin mtrix, X 0 : Γ R m i bounded uncertin vrible, nd H(, ) : [, ) T Γ R m i rd-continuou time cle uncertin proce. If there i contnt ν > 0 uch tht H(t, γ) ν for ll t [, b) T with b (, ) T, < ρ(b), then the initil vlue problem (13) h unique olution on [, ) T. Proof: Firt, we oberve tht we put F (t, x, γ) := A(γ)x + H(t, γ), then F tifie the condition (H 1 ) nd (H 2 ). Moreover, F (t, x, γ) F (t, y, γ) A(γ) x y for every t [, ) T, x, y R m nd γ Γ. Therefore, by the Theorem 3.1, it follow tht (13) h unique olution on [, b] κ T. Further, let X(t, ) be the olution of (13) which exit on [, b) T with b (, ) T, < ρ(b). Alo, let N > 0 be uch tht A(γ) N. Then we hve X(t, γ) X(, γ) ν(t ) + N A(γ)X(, γ) + X(, γ). H(, γ)
10 26 U.A. Hhmi et l.: Uncertin Dynmic Sytem on Time Scle Then, by the Corollry 6.8 in [4], it follow tht X(t, γ) (1 + ν N )e N(t, ) ν N (1 + ν N )e N(b, ). Hence F (t, X(t, γ), γ) M := ν +(1+ ν N )e N (b, ). Proceeding in the proof of the Theorem 3.2 it follow tht the unique olution of (13) exit on [, ) T. A mpping Ψ : T Γ M m (R) i clled n uncertin mtrix proce if ll it component ψ ij : T Γ R, i, j = 1, 2,..., m, re uncertin proce. An uncertin mtrix proce Ψ i id to be regreive if Ψ(t, ) R m for ll t T. In the following, uppoe tht A : Γ M m (R) i regreive nd bounded uncertin mtrix. An uncertin mtrix proce Ψ A i id to be n uncertin mtrix olution of the the following homogeneou liner uncertin differentil eqution X (t, γ) = A(γ)X(t, γ), t T, γ Γ, (14) if ech column of Ψ A tifie (14). An uncertin fundmentl mtrix of (14) i n uncertin mtrix olution Ψ A of (14) uch tht det Ψ A (t, γ) 0 for ll t T nd γ Γ. An uncertin trnition mtrix of (14) t initil time T i n uncertin fundmentl mtrix Ψ A uch tht Ψ A (, γ) = I for ll γ Γ. The uncertin trnition mtrix of (14) t initil time T will be denoted by U A (t, ). Therefore, the uncertin trnition mtrix of (14) t initil time T i the unique olution of the following uncertin mtrix initil vlue problem Φ (t, γ) = A(γ)Φ(t, γ), Φ(, γ) = I, (15) nd X(t, γ) = U A (t, )X(, γ), t, i the unique olution of the following uncertin initil vlue problem X (t, γ) = A(γ)X(t, γ), t T, γ Γ, X(, γ) = X 0 (γ). The exitence nd uniquene of the olution of (15) follow from the Theorem 3.1. The uncertin trnition mtrix of (14) t initil time T i lo clled the uncertin mtrix exponentil function (t ), nd it i denoted by e A(γ) (t, ) or e A (t, ). In the following theorem we give ome propertie of the uncertin trnition mtrix. The proof of the theorem i the me tht in [4, Theorem 5.21]. Theorem 4. 2 If A : Γ M m (R) i regreive nd bounded uncertin mtrix, then (1) U A (t, t) = I; (2) U A (σ(t), ) = [I + µ(t)a(γ)]u A (t, ); (3) U 1 A (t, ) = U T A (t, ); T (4) U A (t, ) = U 1 A (, t) = U T A (, t); T (5) U A (t, )U A (, r) = U A (t, r), for ll t,, r T with t > > r nd ll γ Γ. Theorem 4. 3 (Vrition of Contnt). Suppoe tht the umption of the Theorem 4.1 hold. Then the unique olution X(, ) : [, ) T Γ R m of the uncertin initil vlue problem (13) i given by X(t, γ) = U A (t, )X 0 (γ) + U A (t, σ())h(, γ), t [, ) T, γ Γ. (16) Proof: Indeed, we cn rewritten (16) [ ] X(t, γ) = U A (t, ) X 0 (γ) + U A (, σ())h(, γ).
11 Journl of Uncertin Sytem, Vol.9, No.1, pp.17-30, Uing the product rule to differentite X(t, ), we infer [ ] X (t, γ) = A(γ)U A (t, ) X 0 (γ) + U A (, σ())h(, γ) +U A (σ(t), )U A (, σ(t))h(t, γ) = A(γ)X(t, γ) + H(t, γ) Obviouly, X(, γ) = X 0 (γ). Therefore, X(t, γ) i the olution of (16). Corollry 4. 1 Let X 0 : Γ R m be bounded uncertin vrible. If A : Γ M m (R) i regreive nd bounded uncertin mtrix, then the unique olution of the uncertin initil vlue problem (12) i given by X(t, γ) = U A (t, )X 0 (γ), t [, ) T, γ Γ. Theorem 4. 4 (Vrition of Contnt). Suppoe tht the umption of the Theorem 4.1 hold. Then the unique olution X(, ) : [, ) T Γ R m of the following uncertin initil vlue problem X (t, γ) = A T (γ)x σ (t, γ) + H(t, γ), t [, ) T, γ Γ, (17) X(, γ) = X 0 (γ), on [, ) T given by X(t, γ) = Ψ A T (γ)(t, )X 0 (γ) + Proof: Indeed, we cn rewrite (17) tht i, Ψ A T (γ)(t, )H(, γ), t [, ) T, γ Γ. (18) X (t, γ) = A T (γ)[x(t, γ) + µ(t)x (t, γ)] + H(t, γ) = A T (γ)x(t, γ) µ(t)a T (γ)x (t, γ) + H(t, γ), [I + µ(t)a T (γ)]x (t, γ) = A T (γ)x(t, γ) + H(t, γ). Since the mtrix A(γ) i regreive, then A T (γ) i lo regreive, nd hence we infer tht tht i, X (t, γ) = [I + µ(t)a T (γ)] 1 A T (γ)x(t, γ) + [I + µ(t)a T (γ)] 1 H(t, γ) = A T (γ)x(t, γ) + [I + µ(t)a T (γ)] 1 H(t, γ), X (t, γ) = A T (γ)x(t, γ) + [I + µ(t)a T (γ)] 1 H(t, γ). Now, uing the Theorem 4.3 nd the propertie of the uncertin trnition mtrix, we obtin tht tht i (18). X(t, γ) = U A T (t, )X 0 (γ) + = U A T (t, )X 0 (γ) + = U A T (t, )X 0 (γ) + = U A T (t, )X 0 (γ) + U A T (t, σ())[i + µ(t)a T (γ)] 1 H(, γ) U T A (t, σ())[i + µ(t)a T (γ)] 1 H(, γ) [I + µ(t)a(γ)] 1 U A (σ(), t)} T H(, γ) U A (, t)h(, γ), Corollry 4. 2 Let X 0 : Γ R be bounded uncertin vrible. If A : Γ M m (R) i regreive nd bounded uncertin mtrix, then the unique olution of the following uncertin initil vlue problem X (t, γ) = A(γ)X σ (t, γ), t [, ) T, γ Γ, i given by X(, γ) = X 0 (γ), X(t, γ) = U A T (t, )X 0 (γ), t [, ) T, γ Γ.
12 28 U.A. Hhmi et l.: Uncertin Dynmic Sytem on Time Scle Exmple 4. 1 Let u conider Γ = (0, 1), L the σ-lgebr of ll Borel ubet of Γ, M the uncertin meure on Γ defined in Exmple 2.1, nd the following initil vlue problem X (t, γ) = γx(t, γ) + e γ (t, 0), t [0, ) T, γ Γ, (19) X(0, γ) = γ. Then, by the Theorem 4.1 nd 4.3, the initil vlue problem (19) h unique olution on [0, ) T, given by tht i, Next, conider two prticulr ce. X(t, γ) = γe γ (t, 0) + 0 e γ (t, σ())e γ (, 0), ( ) 1 X(t, γ) = e γ (t, 0) γ µ()γ, t [0, ) T. If T = R, then µ(t) = 0 for ll t N, nd e γ (t, 0) = e γt. Moreover, in thi ce we hve µ()γ = 0 d = t. It follow tht the initil vlue problem X (t, γ) = γx(t, γ) + e γt, t [0, ) X(0, γ) = γ, h the olution X(t, γ) = (γ + t)e γt, t [0, ). If T = N, then µ(n) = 1 for ll n N, nd e γ (n, 0) = (1 + γ) n. Moreover, in thi ce we hve µ()γ = [0,n) γ = n 1 + γ. It follow tht the difference initil vlue problem Xn+1 (γ) = (1 + γ)x n (γ) + (1 + γ) n, n N X 0 (γ) = γ, h the olution X n (γ) = (γ + n 1 + γ )(1 + γ)n, n N. Exmple 4. 2 Let u conider Γ = (0, 1),L the σ-lgebr of ll Borel ubet of Γ, M the uncertin meure on Γ defined in Exmple 2.1, nd the following initil vlue problem X (t, γ) = γx σ (t, γ) + e γ (t, ), t [0, ) T, γ Γ, (20) X(0, γ) = γ. The initil vlue problem (20) h unique olution on [, ) T, given by tht i, X(t, γ) = γe γ (t, ) + 0 e γ (t, )e γ (, 0), X(t, γ) = (γ + t) e γ (t, 0), t [0, ) T, γ (0, 1). If T = R, then µ(t) = 0 for ll t R, nd e γ (t, 0) = e γt. It follow tht X(t, γ) = (γ + t) = e γt, t [0, ) T, γ (0, 1).
13 Journl of Uncertin Sytem, Vol.9, No.1, pp.17-30, If T = hn with h > 0, then µ(t) = h for ll t hn, nd e γ (t, 0) = (1 + γh) t/h. It follow tht the h-difference initil vlue problem Xt+h (γ) = 1 1+γh X t(γ) + h(1 + γh) t/h 1, t hn X 0 (γ) = γ, h the unique olution X t (γ) = (γ + t) (1 + γh) t/h, t hn. If T = 2 N, then µ(t) = t for ll t 2 N, nd e γ (t, 0) = initil vlue problem Xt (γ) = (1 + γt)x 2t (γ) t X 1 (γ) = γ, h the unique olution X t (γ) = (γ + t) [1,t) [1,t) [0,t) (1 + γ) 1, t 2 N. (1 + γ) 1. It follow tht the 2-difference (1 + γ) 1, t 2 N Exmple 4. 3 Let u conider Γ = (0, 1), L the σ lgebr of ll Borel ubet of Γ, M the uncertin meure on Γ defined in Exmple 2.1, nd the following initil vlue problem X (t, γ) = [ 1 γ 0 1 ] [ γ X(t, γ), X(0, γ) = 1 ], t [0, ) T, (21) [ ] 1 γ where 1 µ(t) 0 for t [0, ) T. The mtrix A = h the eigenvlue λ = 1, λ 2 = 1 with the [ ] [ ] 1 1 correponding eigenvector v 1 =, v 0 1 =, repectively. Then Ψ A (t, γ) = γ 2 [ e 1 (t, 0) e 1 (t, 0) 0 2 γ e 1(t, 0) ] [, Ψ 1 A (, γ) = e1 (, 0) 0 nd therefore, the uncertin trnition mtrix for (21) i given by [ γ e 1 (t, ) U A (t, ) = 2 e 1(t, ) γ 2 e 1(t, ) 0 e 1 (t, ) It follow tht the olution of the initil vlue problem (21) i given by X(t, γ) = U A (t, 0)X(0, γ) = [ 3γ 2 e 1(t, 0) γ 2 e 1(t, 0) e 1 (t, 0) ]. γ 2 e ] 1(, 0) γ 2 e 1(, 0) ] t [0, ) T, γ (0, 1). 5 Concluion The theory of dynmicl ytem with uncertin prmeter cn be uccefully pplied to modeling mny rel-world phenomen uch in biology to tudy the popultion growth, in epecilly of microorgnim uch bcteri, in phyicl ytem where heterogeneou micro-cle tructure re preent, in the propgtion of electromgnetic wve through dielectric mteril with vribility in the relxtion time nd o on. Some of thee ppliction will be the ubject of future work. Acknowledgment Thi work w upported by Higher Eduction Commiion of Pkitn.
14 30 U.A. Hhmi et l.: Uncertin Dynmic Sytem on Time Scle Reference [1] Agrwl, R.P., nd M. Bohner, Bic clculu on time cle nd ome of it ppliction, Reult Mth, vol.35, pp.3 22, [2] Agrwl, R.P., Bohner., M., O Regn, D., nd A. Peteron, Dynmic eqution on time cle: urvey, Journl of Computtionl nd Applied Mthemtic, vol.141, no.1-2, pp.1 26, [3] Ahlbrndt, C.D., nd C. Morin, Prtil differentil eqution on time cle, Journl of Computtionl nd Applied Mthemtic, vol.141, pp.35 55, [4] Bohner, M., nd A. Peteron, Dynmic Eqution on Time Scle: An Introduction with Appliction, Birkhuer, Boton, [5] Bohner, M., nd A. Peteron, Advnce in Dynmic Eqution on Time Scle, Birkhuer, Boton, [6] Chen, X., nd B. Liu, Exitence nd uniquene theorem for uncertin differentil eqution, Fuzzy Optimiztion nd Deciion Mking, vol.9, no.1, pp.69 81, [7] Go, X., Some propertie of continuou uncertin meure, Interntionl Journl of Uncertinty, Fuzzine nd Knowledge-Bed Sytem, vol.17, no.3, pp , [8] Gueinov, G.S., Integrtion on time cle, Journl of Mthemticl Anlyi nd Appliction, vol.285, pp , [9] Gueinov, G.S., nd B. Kymkln, Bic of Riemnn delt nd nbl integrtion on time cle, Journl of Differentil Eqution nd Appliction, vol.8, pp , [10] Hilger, S., Ein Mkettenklkl mit Anwendung uf Zentrummnnigfltigkeiten, Ph.D. Thei, Univerität Würzburg, [11] Hilger, S., Anlyi on meure chin- unified pproch to continuou nd dicrete clculu, Reult Mth, vol.18, pp.18 56, [12] Hoffcker, J., Bic prtil dynmic eqution on time cle, Journl of Difference Eqution nd Appliction, vol.8, no.4, pp , [13] Jckon, B., Prtil dynmic eqution on time cle, Journl of Computtionl nd Applied Mthemtic, vol.186, pp , [14] Liu, B., Uncertinty Theory, 2nd Edition, Springer-Verlg, Berlin, [15] Liu, B., Fuzzy proce, hybrid proce nd uncertin proce, Journl of Uncertin Sytem, vol.2, no.1, pp.3 16, [16] Liu, B., Some reerch problem in uncertin theory, Journl of Uncertin Sytem, vol.2, no.4, pp.3 10, [17] Lungn, C., nd V. Lupulecu, Rndom dynmicl ytem on time cle, Electronic Journl of Differentil Eqution, vol.2012, no.86, pp.1 14, [18] Mlinowki, M.T., On rndom fuzzy differentil eqution, Fuzzy Set nd Sytem, vol.160, pp , [19] Mlinowki, M.T., Exitence theorem for olution to rndom fuzzy differentil eqution, Nonliner Anlyi, vol.73, pp , [20] Sngl, S., Stochtic Differentil Eqution, Ph.D. Dierttion, Miouri Univerity of Science nd Technology, [21] Tidell, C.C., nd A.H. Zidi, Succeive pproximtion to olution of dynmic eqution on time cle, Communiction on Applied Nonliner Anlyi, vol.16, no.1, pp.61 87, [22] You, C., Some convergence theorem of uncertin equence, Mthemticl nd Computer Modelling, vol.49, no.3-4, pp , 2009.
FRACTIONAL DYNAMIC INEQUALITIES HARMONIZED ON TIME SCALES
FRACTIONAL DYNAMIC INEQUALITIES HARMONIZED ON TIME SCALES M JIBRIL SHAHAB SAHIR Accepted Mnuscript Version This is the unedited version of the rticle s it ppered upon cceptnce by the journl. A finl edited
More informationTAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES
TAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES DOUGLAS R. ANDERSON Abtract. We are concerned with the repreentation of polynomial for nabla dynamic equation on time cale. Once etablihed,
More informationAPPENDIX 2 LAPLACE TRANSFORMS
APPENDIX LAPLACE TRANSFORMS Thi ppendix preent hort introduction to Lplce trnform, the bic tool ued in nlyzing continuou ytem in the frequency domin. The Lplce trnform convert liner ordinry differentil
More informationReview on Integration (Secs ) Review: Sec Origins of Calculus. Riemann Sums. New functions from old ones.
Mth 20B Integrl Clculus Lecture Review on Integrtion (Secs. 5. - 5.3) Remrks on the course. Slide Review: Sec. 5.-5.3 Origins of Clculus. Riemnn Sums. New functions from old ones. A mthemticl description
More informationWENJUN LIU AND QUÔ C ANH NGÔ
AN OSTROWSKI-GRÜSS TYPE INEQUALITY ON TIME SCALES WENJUN LIU AND QUÔ C ANH NGÔ Astrct. In this pper we derive new inequlity of Ostrowski-Grüss type on time scles nd thus unify corresponding continuous
More informationThe Regulated and Riemann Integrals
Chpter 1 The Regulted nd Riemnn Integrls 1.1 Introduction We will consider severl different pproches to defining the definite integrl f(x) dx of function f(x). These definitions will ll ssign the sme vlue
More informationARCHIVUM MATHEMATICUM (BRNO) Tomus 47 (2011), Kristína Rostás
ARCHIVUM MAHEMAICUM (BRNO) omu 47 (20), 23 33 MINIMAL AND MAXIMAL SOLUIONS OF FOURH ORDER IERAED DIFFERENIAL EQUAIONS WIH SINGULAR NONLINEARIY Kritín Rotá Abtrct. In thi pper we re concerned with ufficient
More informationA General Dynamic Inequality of Opial Type
Appl Mth Inf Sci No 3-5 (26) Applied Mthemtics & Informtion Sciences An Interntionl Journl http://dxdoiorg/2785/mis/bos7-mis A Generl Dynmic Inequlity of Opil Type Rvi Agrwl Mrtin Bohner 2 Donl O Regn
More informationExpected Value of Function of Uncertain Variables
Journl of Uncertin Systems Vol.4, No.3, pp.8-86, 2 Online t: www.jus.org.uk Expected Vlue of Function of Uncertin Vribles Yuhn Liu, Minghu H College of Mthemtics nd Computer Sciences, Hebei University,
More informationHenstock Kurzweil delta and nabla integrals
Henstock Kurzweil delt nd nbl integrls Alln Peterson nd Bevn Thompson Deprtment of Mthemtics nd Sttistics, University of Nebrsk-Lincoln Lincoln, NE 68588-0323 peterso@mth.unl.edu Mthemtics, SPS, The University
More informationf(x)dx . Show that there 1, 0 < x 1 does not exist a differentiable function g : [ 1, 1] R such that g (x) = f(x) for all
3 Definite Integrl 3.1 Introduction In school one comes cross the definition of the integrl of rel vlued function defined on closed nd bounded intervl [, b] between the limits nd b, i.e., f(x)dx s the
More informationMATH34032: Green s Functions, Integral Equations and the Calculus of Variations 1
MATH34032: Green s Functions, Integrl Equtions nd the Clculus of Vritions 1 Section 1 Function spces nd opertors Here we gives some brief detils nd definitions, prticulrly relting to opertors. For further
More information20.2. The Transform and its Inverse. Introduction. Prerequisites. Learning Outcomes
The Trnform nd it Invere 2.2 Introduction In thi Section we formlly introduce the Lplce trnform. The trnform i only pplied to cul function which were introduced in Section 2.1. We find the Lplce trnform
More informationThe inequality (1.2) is called Schlömilch s Inequality in literature as given in [9, p. 26]. k=1
THE TEACHING OF MATHEMATICS 2018, Vol XXI, 1, pp 38 52 HYBRIDIZATION OF CLASSICAL INEQUALITIES WITH EQUIVALENT DYNAMIC INEQUALITIES ON TIME SCALE CALCULUS Muhmmd Jibril Shhb Shir Abstrct The im of this
More informationTP 10:Importance Sampling-The Metropolis Algorithm-The Ising Model-The Jackknife Method
TP 0:Importnce Smpling-The Metropoli Algorithm-The Iing Model-The Jckknife Method June, 200 The Cnonicl Enemble We conider phyicl ytem which re in therml contct with n environment. The environment i uully
More information(4.1) D r v(t) ω(t, v(t))
1.4. Differentil inequlities. Let D r denote the right hnd derivtive of function. If ω(t, u) is sclr function of the sclrs t, u in some open connected set Ω, we sy tht function v(t), t < b, is solution
More information2. The Laplace Transform
. The Lplce Trnform. Review of Lplce Trnform Theory Pierre Simon Mrqui de Lplce (749-87 French tronomer, mthemticin nd politicin, Miniter of Interior for 6 wee under Npoleon, Preident of Acdemie Frncie
More informationMath Advanced Calculus II
Mth 452 - Advnced Clculus II Line Integrls nd Green s Theorem The min gol of this chpter is to prove Stoke s theorem, which is the multivrible version of the fundmentl theorem of clculus. We will be focused
More information1.2. Linear Variable Coefficient Equations. y + b "! = a y + b " Remark: The case b = 0 and a non-constant can be solved with the same idea as above.
1 12 Liner Vrible Coefficient Equtions Section Objective(s): Review: Constnt Coefficient Equtions Solving Vrible Coefficient Equtions The Integrting Fctor Method The Bernoulli Eqution 121 Review: Constnt
More information2π(t s) (3) B(t, ω) has independent increments, i.e., for any 0 t 1 <t 2 < <t n, the random variables
2 Brownin Motion 2.1 Definition of Brownin Motion Let Ω,F,P) be probbility pce. A tochtic proce i meurble function Xt, ω) defined on the product pce [, ) Ω. In prticulr, ) for ech t, Xt, ) i rndom vrible,
More informationAdvanced Calculus: MATH 410 Notes on Integrals and Integrability Professor David Levermore 17 October 2004
Advnced Clculus: MATH 410 Notes on Integrls nd Integrbility Professor Dvid Levermore 17 October 2004 1. Definite Integrls In this section we revisit the definite integrl tht you were introduced to when
More informationResearch Article On Existence and Uniqueness of Solutions of a Nonlinear Integral Equation
Journl of Applied Mthemtics Volume 2011, Article ID 743923, 7 pges doi:10.1155/2011/743923 Reserch Article On Existence nd Uniqueness of Solutions of Nonliner Integrl Eqution M. Eshghi Gordji, 1 H. Bghni,
More informationMath 2142 Homework 2 Solutions. Problem 1. Prove the following formulas for Laplace transforms for s > 0. a s 2 + a 2 L{cos at} = e st.
Mth 2142 Homework 2 Solution Problem 1. Prove the following formul for Lplce trnform for >. L{1} = 1 L{t} = 1 2 L{in t} = 2 + 2 L{co t} = 2 + 2 Solution. For the firt Lplce trnform, we need to clculte:
More informationMath 554 Integration
Mth 554 Integrtion Hndout #9 4/12/96 Defn. A collection of n + 1 distinct points of the intervl [, b] P := {x 0 = < x 1 < < x i 1 < x i < < b =: x n } is clled prtition of the intervl. In this cse, we
More informationRegulated functions and the regulated integral
Regulted functions nd the regulted integrl Jordn Bell jordn.bell@gmil.com Deprtment of Mthemtics University of Toronto April 3 2014 1 Regulted functions nd step functions Let = [ b] nd let X be normed
More informationCommunications inmathematicalanalysis Volume 6, Number 2, pp (2009) ISSN
Communictions inmthemticlanlysis Volume 6, Number, pp. 33 41 009) ISSN 1938-9787 www.commun-mth-nl.org A SHARP GRÜSS TYPE INEQUALITY ON TIME SCALES AND APPLICATION TO THE SHARP OSTROWSKI-GRÜSS INEQUALITY
More informationSet Integral Equations in Metric Spaces
Mthemtic Morvic Vol. 13-1 2009, 95 102 Set Integrl Equtions in Metric Spces Ion Tişe Abstrct. Let P cp,cvr n be the fmily of ll nonempty compct, convex subsets of R n. We consider the following set integrl
More informationCHOOSING THE NUMBER OF MODELS OF THE REFERENCE MODEL USING MULTIPLE MODELS ADAPTIVE CONTROL SYSTEM
Interntionl Crpthin Control Conference ICCC 00 ALENOVICE, CZEC REPUBLIC y 7-30, 00 COOSING TE NUBER OF ODELS OF TE REFERENCE ODEL USING ULTIPLE ODELS ADAPTIVE CONTROL SYSTE rin BICĂ, Victor-Vleriu PATRICIU
More informationWirtinger s Integral Inequality on Time Scale
Theoreticl themtics & pplictions vol.8 no.1 2018 1-8 ISSN: 1792-9687 print 1792-9709 online Scienpress Ltd 2018 Wirtinger s Integrl Inequlity on Time Scle Ttjn irkovic 1 bstrct In this pper we estblish
More informationSome estimates on the Hermite-Hadamard inequality through quasi-convex functions
Annls of University of Criov, Mth. Comp. Sci. Ser. Volume 3, 7, Pges 8 87 ISSN: 13-693 Some estimtes on the Hermite-Hdmrd inequlity through qusi-convex functions Dniel Alexndru Ion Abstrct. In this pper
More informationLyapunov-type inequality for the Hadamard fractional boundary value problem on a general interval [a; b]; (1 6 a < b)
Lypunov-type inequlity for the Hdmrd frctionl boundry vlue problem on generl intervl [; b]; ( 6 < b) Zid Ldjl Deprtement of Mthemtic nd Computer Science, ICOSI Lbortory, Univerity of Khenchel, 40000, Algeri.
More informationDefinite integral. Mathematics FRDIS MENDELU
Definite integrl Mthemtics FRDIS MENDELU Simon Fišnrová Brno 1 Motivtion - re under curve Suppose, for simplicity, tht y = f(x) is nonnegtive nd continuous function defined on [, b]. Wht is the re of the
More informationMath 360: A primitive integral and elementary functions
Mth 360: A primitive integrl nd elementry functions D. DeTurck University of Pennsylvni October 16, 2017 D. DeTurck Mth 360 001 2017C: Integrl/functions 1 / 32 Setup for the integrl prtitions Definition:
More informationII. Integration and Cauchy s Theorem
MTH6111 Complex Anlysis 2009-10 Lecture Notes c Shun Bullett QMUL 2009 II. Integrtion nd Cuchy s Theorem 1. Pths nd integrtion Wrning Different uthors hve different definitions for terms like pth nd curve.
More informationODE: Existence and Uniqueness of a Solution
Mth 22 Fll 213 Jerry Kzdn ODE: Existence nd Uniqueness of Solution The Fundmentl Theorem of Clculus tells us how to solve the ordinry differentil eqution (ODE) du = f(t) dt with initil condition u() =
More informationCzechoslovak Mathematical Journal, 55 (130) (2005), , Abbotsford. 1. Introduction
Czechoslovk Mthemticl Journl, 55 (130) (2005), 933 940 ESTIMATES OF THE REMAINDER IN TAYLOR S THEOREM USING THE HENSTOCK-KURZWEIL INTEGRAL, Abbotsford (Received Jnury 22, 2003) Abstrct. When rel-vlued
More information7.2 Riemann Integrable Functions
7.2 Riemnn Integrble Functions Theorem 1. If f : [, b] R is step function, then f R[, b]. Theorem 2. If f : [, b] R is continuous on [, b], then f R[, b]. Theorem 3. If f : [, b] R is bounded nd continuous
More information1 The Riemann Integral
The Riemnn Integrl. An exmple leding to the notion of integrl (res) We know how to find (i.e. define) the re of rectngle (bse height), tringle ( (sum of res of tringles). But how do we find/define n re
More informationDefinite integral. Mathematics FRDIS MENDELU. Simona Fišnarová (Mendel University) Definite integral MENDELU 1 / 30
Definite integrl Mthemtics FRDIS MENDELU Simon Fišnrová (Mendel University) Definite integrl MENDELU / Motivtion - re under curve Suppose, for simplicity, tht y = f(x) is nonnegtive nd continuous function
More informationA REVIEW OF CALCULUS CONCEPTS FOR JDEP 384H. Thomas Shores Department of Mathematics University of Nebraska Spring 2007
A REVIEW OF CALCULUS CONCEPTS FOR JDEP 384H Thoms Shores Deprtment of Mthemtics University of Nebrsk Spring 2007 Contents Rtes of Chnge nd Derivtives 1 Dierentils 4 Are nd Integrls 5 Multivrite Clculus
More information1. On some properties of definite integrals. We prove
This short collection of notes is intended to complement the textbook Anlisi Mtemtic 2 by Crl Mdern, published by Città Studi Editore, [M]. We refer to [M] for nottion nd the logicl stremline of the rguments.
More informationJournal of Inequalities in Pure and Applied Mathematics
Journl of Inequlities in Pure nd Applied Mthemtics MOMENTS INEQUALITIES OF A RANDOM VARIABLE DEFINED OVER A FINITE INTERVAL PRANESH KUMAR Deprtment of Mthemtics & Computer Science University of Northern
More informationThe Banach algebra of functions of bounded variation and the pointwise Helly selection theorem
The Bnch lgebr of functions of bounded vrition nd the pointwise Helly selection theorem Jordn Bell jordn.bell@gmil.com Deprtment of Mthemtics, University of Toronto Jnury, 015 1 BV [, b] Let < b. For f
More informationDynamics and stability of Hilfer-Hadamard type fractional differential equations with boundary conditions
Journl Nonliner Anlyi nd Appliction 208 No. 208 4-26 Avilble online t www.ipc.com/jn Volume 208, Iue, Yer 208 Article ID jn-00386, 3 Pge doi:0.5899/208/jn-00386 Reerch Article Dynmic nd tbility of Hilfer-Hdmrd
More informationMATH 409 Advanced Calculus I Lecture 19: Riemann sums. Properties of integrals.
MATH 409 Advnced Clculus I Lecture 19: Riemnn sums. Properties of integrls. Drboux sums Let P = {x 0,x 1,...,x n } be prtition of n intervl [,b], where x 0 = < x 1 < < x n = b. Let f : [,b] R be bounded
More informationFourier series. Preliminary material on inner products. Suppose V is vector space over C and (, )
Fourier series. Preliminry mteril on inner products. Suppose V is vector spce over C nd (, ) is Hermitin inner product on V. This mens, by definition, tht (, ) : V V C nd tht the following four conditions
More informationAdvanced Calculus: MATH 410 Uniform Convergence of Functions Professor David Levermore 11 December 2015
Advnced Clculus: MATH 410 Uniform Convergence of Functions Professor Dvid Levermore 11 December 2015 12. Sequences of Functions We now explore two notions of wht it mens for sequence of functions {f n
More informationThe Kurzweil integral and hysteresis
Journl of Phyic: Conference Serie The Kurzweil integrl nd hyterei To cite thi rticle: P Krejcí 2006 J. Phy.: Conf. Ser. 55 144 View the rticle online for updte nd enhncement. Relted content - Outwrd pointing
More informationThe Delta-nabla Calculus of Variations for Composition Functionals on Time Scales
Interntionl Journl of Difference Equtions ISSN 973-669, Volume 8, Number, pp. 7 47 3) http://cmpus.mst.edu/ijde The Delt-nbl Clculus of Vritions for Composition Functionls on Time Scles Monik Dryl nd Delfim
More informationPHYS 601 HW 5 Solution. We wish to find a Fourier expansion of e sin ψ so that the solution can be written in the form
5 Solving Kepler eqution Conider the Kepler eqution ωt = ψ e in ψ We wih to find Fourier expnion of e in ψ o tht the olution cn be written in the form ψωt = ωt + A n innωt, n= where A n re the Fourier
More informationPrinciples of Real Analysis I Fall VI. Riemann Integration
21-355 Principles of Rel Anlysis I Fll 2004 A. Definitions VI. Riemnn Integrtion Let, b R with < b be given. By prtition of [, b] we men finite set P [, b] with, b P. The set of ll prtitions of [, b] will
More informationResearch Article Generalized Hyers-Ulam Stability of the Second-Order Linear Differential Equations
Hindwi Publihing Corportion Journl of Applied Mthemtic Volume 011, Article ID 813137, 10 pge doi:10.1155/011/813137 Reerch Article Generlized Hyer-Ulm Stbility of the Second-Order Liner Differentil Eqution
More informationNew Expansion and Infinite Series
Interntionl Mthemticl Forum, Vol. 9, 204, no. 22, 06-073 HIKARI Ltd, www.m-hikri.com http://dx.doi.org/0.2988/imf.204.4502 New Expnsion nd Infinite Series Diyun Zhng College of Computer Nnjing University
More information1.1. Linear Constant Coefficient Equations. Remark: A differential equation is an equation
1 1.1. Liner Constnt Coefficient Equtions Section Objective(s): Overview of Differentil Equtions. Liner Differentil Equtions. Solving Liner Differentil Equtions. The Initil Vlue Problem. 1.1.1. Overview
More informationMA 124 January 18, Derivatives are. Integrals are.
MA 124 Jnury 18, 2018 Prof PB s one-minute introduction to clculus Derivtives re. Integrls re. In Clculus 1, we lern limits, derivtives, some pplictions of derivtives, indefinite integrls, definite integrls,
More informationGreen s function. Green s function. Green s function. Green s function. Green s function. Green s functions. Classical case (recall)
Green s functions 3. G(t, τ) nd its derivtives G (k) t (t, τ), (k =,..., n 2) re continuous in the squre t, τ t with respect to both vribles, George Green (4 July 793 3 My 84) In 828 Green privtely published
More informationM. A. Pathan, O. A. Daman LAPLACE TRANSFORMS OF THE LOGARITHMIC FUNCTIONS AND THEIR APPLICATIONS
DEMONSTRATIO MATHEMATICA Vol. XLVI No 3 3 M. A. Pthn, O. A. Dmn LAPLACE TRANSFORMS OF THE LOGARITHMIC FUNCTIONS AND THEIR APPLICATIONS Abtrct. Thi pper del with theorem nd formul uing the technique of
More informationKRASNOSEL SKII TYPE FIXED POINT THEOREM FOR NONLINEAR EXPANSION
Fixed Point Theory, 13(2012), No. 1, 285-291 http://www.mth.ubbcluj.ro/ nodecj/sfptcj.html KRASNOSEL SKII TYPE FIXED POINT THEOREM FOR NONLINEAR EXPANSION FULI WANG AND FENG WANG School of Mthemtics nd
More informationJournal of Inequalities in Pure and Applied Mathematics
Journl of Inequlities in Pure nd Applied Mthemtics http://jipm.vu.edu.u/ Volume 3, Issue, Article 4, 00 ON AN IDENTITY FOR THE CHEBYCHEV FUNCTIONAL AND SOME RAMIFICATIONS P. CERONE SCHOOL OF COMMUNICATIONS
More informationUNIFORM CONVERGENCE. Contents 1. Uniform Convergence 1 2. Properties of uniform convergence 3
UNIFORM CONVERGENCE Contents 1. Uniform Convergence 1 2. Properties of uniform convergence 3 Suppose f n : Ω R or f n : Ω C is sequence of rel or complex functions, nd f n f s n in some sense. Furthermore,
More informationLINEAR STOCHASTIC DIFFERENTIAL EQUATIONS WITH ANTICIPATING INITIAL CONDITIONS
Communiction on Stochtic Anlyi Vol. 7, No. 2 213 245-253 Seril Publiction www.erilpubliction.com LINEA STOCHASTIC DIFFEENTIAL EQUATIONS WITH ANTICIPATING INITIAL CONDITIONS NAJESS KHALIFA, HUI-HSIUNG KUO,
More informationA PROOF OF THE FUNDAMENTAL THEOREM OF CALCULUS USING HAUSDORFF MEASURES
INROADS Rel Anlysis Exchnge Vol. 26(1), 2000/2001, pp. 381 390 Constntin Volintiru, Deprtment of Mthemtics, University of Buchrest, Buchrest, Romni. e-mil: cosv@mt.cs.unibuc.ro A PROOF OF THE FUNDAMENTAL
More informationEXISTENCE OF SOLUTIONS TO INFINITE ELASTIC BEAM EQUATIONS WITH UNBOUNDED NONLINEARITIES
Electronic Journl of Differentil Eqution, Vol. 17 (17), No. 19, pp. 1 11. ISSN: 17-6691. URL: http://ejde.mth.txtte.edu or http://ejde.mth.unt.edu EXISTENCE OF SOLUTIONS TO INFINITE ELASTIC BEAM EQUATIONS
More informationThe presentation of a new type of quantum calculus
DOI.55/tmj-27-22 The presenttion of new type of quntum clculus Abdolli Nemty nd Mehdi Tourni b Deprtment of Mthemtics, University of Mzndrn, Bbolsr, Irn E-mil: nmty@umz.c.ir, mehdi.tourni@gmil.com b Abstrct
More informationTHE EXISTENCE-UNIQUENESS THEOREM FOR FIRST-ORDER DIFFERENTIAL EQUATIONS.
THE EXISTENCE-UNIQUENESS THEOREM FOR FIRST-ORDER DIFFERENTIAL EQUATIONS RADON ROSBOROUGH https://intuitiveexplntionscom/picrd-lindelof-theorem/ This document is proof of the existence-uniqueness theorem
More informationMA FINAL EXAM INSTRUCTIONS
MA 33 FINAL EXAM INSTRUCTIONS NAME INSTRUCTOR. Intructor nme: Chen, Dong, Howrd, or Lundberg 2. Coure number: MA33. 3. SECTION NUMBERS: 6 for MWF :3AM-:2AM REC 33 cl by Erik Lundberg 7 for MWF :3AM-:2AM
More informationChapter 6. Riemann Integral
Introduction to Riemnn integrl Chpter 6. Riemnn Integrl Won-Kwng Prk Deprtment of Mthemtics, The College of Nturl Sciences Kookmin University Second semester, 2015 1 / 41 Introduction to Riemnn integrl
More informationReview of Riemann Integral
1 Review of Riemnn Integrl In this chpter we review the definition of Riemnn integrl of bounded function f : [, b] R, nd point out its limittions so s to be convinced of the necessity of more generl integrl.
More informationSection 6.1 INTRO to LAPLACE TRANSFORMS
Section 6. INTRO to LAPLACE TRANSFORMS Key terms: Improper Integrl; diverge, converge A A f(t)dt lim f(t)dt Piecewise Continuous Function; jump discontinuity Function of Exponentil Order Lplce Trnsform
More informationNew Integral Inequalities of the Type of Hermite-Hadamard Through Quasi Convexity
Punjb University Journl of Mthemtics (ISSN 116-56) Vol. 45 (13) pp. 33-38 New Integrl Inequlities of the Type of Hermite-Hdmrd Through Qusi Convexity S. Hussin Deprtment of Mthemtics, College of Science,
More informationAdvanced Calculus I (Math 4209) Martin Bohner
Advnced Clculus I (Mth 4209) Spring 2018 Lecture Notes Mrtin Bohner Version from My 4, 2018 Author ddress: Deprtment of Mthemtics nd Sttistics, Missouri University of Science nd Technology, Roll, Missouri
More informationUNIFORM CONVERGENCE MA 403: REAL ANALYSIS, INSTRUCTOR: B. V. LIMAYE
UNIFORM CONVERGENCE MA 403: REAL ANALYSIS, INSTRUCTOR: B. V. LIMAYE 1. Pointwise Convergence of Sequence Let E be set nd Y be metric spce. Consider functions f n : E Y for n = 1, 2,.... We sy tht the sequence
More informationLecture 1. Functional series. Pointwise and uniform convergence.
1 Introduction. Lecture 1. Functionl series. Pointwise nd uniform convergence. In this course we study mongst other things Fourier series. The Fourier series for periodic function f(x) with period 2π is
More informationResearch Article On New Inequalities via Riemann-Liouville Fractional Integration
Abstrct nd Applied Anlysis Volume 202, Article ID 428983, 0 pges doi:0.55/202/428983 Reserch Article On New Inequlities vi Riemnn-Liouville Frctionl Integrtion Mehmet Zeki Sriky nd Hsn Ogunmez 2 Deprtment
More information. The set of these fractions is then obviously Q, and we can define addition and multiplication on it in the expected way by
50 Andre Gthmnn 6. LOCALIZATION Locliztion i very powerful technique in commuttive lgebr tht often llow to reduce quetion on ring nd module to union of mller locl problem. It cn eily be motivted both from
More information63. Representation of functions as power series Consider a power series. ( 1) n x 2n for all 1 < x < 1
3 9. SEQUENCES AND SERIES 63. Representtion of functions s power series Consider power series x 2 + x 4 x 6 + x 8 + = ( ) n x 2n It is geometric series with q = x 2 nd therefore it converges for ll q =
More informationLecture 1: Introduction to integration theory and bounded variation
Lecture 1: Introduction to integrtion theory nd bounded vrition Wht is this course bout? Integrtion theory. The first question you might hve is why there is nything you need to lern bout integrtion. You
More informationMAT612-REAL ANALYSIS RIEMANN STIELTJES INTEGRAL
MAT612-REAL ANALYSIS RIEMANN STIELTJES INTEGRAL DR. RITU AGARWAL MALVIYA NATIONAL INSTITUTE OF TECHNOLOGY, JAIPUR, INDIA-302017 Tble of Contents Contents Tble of Contents 1 1. Introduction 1 2. Prtition
More informationCalculus in R. Chapter Di erentiation
Chpter 3 Clculus in R 3.1 Di erentition Definition 3.1. Suppose U R is open. A function f : U! R is di erentible t x 2 U if there exists number m such tht lim y!0 pple f(x + y) f(x) my y =0. If f is di
More informationSTEP FUNCTIONS, DELTA FUNCTIONS, AND THE VARIATION OF PARAMETERS FORMULA. 0 if t < 0, 1 if t > 0.
STEP FUNCTIONS, DELTA FUNCTIONS, AND THE VARIATION OF PARAMETERS FORMULA STEPHEN SCHECTER. The unit step function nd piecewise continuous functions The Heviside unit step function u(t) is given by if t
More informationSection 6.1 INTRO to LAPLACE TRANSFORMS
Section 6. INTRO to LAPLACE TRANSFORMS Key terms: Improper Integrl; diverge, converge A A f(t)dt lim f(t)dt Piecewise Continuous Function; jump discontinuity Function of Exponentil Order Lplce Trnsform
More informationExistence and Uniqueness of Solution for a Fractional Order Integro-Differential Equation with Non-Local and Global Boundary Conditions
Applied Mthetic 0 9-96 doi:0.436/.0.079 Pulihed Online Octoer 0 (http://www.scirp.org/journl/) Eitence nd Uniquene of Solution for Frctionl Order Integro-Differentil Eqution with Non-Locl nd Glol Boundry
More informationTaylor Polynomial Inequalities
Tylor Polynomil Inequlities Ben Glin September 17, 24 Abstrct There re instnces where we my wish to pproximte the vlue of complicted function round given point by constructing simpler function such s polynomil
More informationW. We shall do so one by one, starting with I 1, and we shall do it greedily, trying
Vitli covers 1 Definition. A Vitli cover of set E R is set V of closed intervls with positive length so tht, for every δ > 0 nd every x E, there is some I V with λ(i ) < δ nd x I. 2 Lemm (Vitli covering)
More informationMath 113 Fall Final Exam Review. 2. Applications of Integration Chapter 6 including sections and section 6.8
Mth 3 Fll 0 The scope of the finl exm will include: Finl Exm Review. Integrls Chpter 5 including sections 5. 5.7, 5.0. Applictions of Integrtion Chpter 6 including sections 6. 6.5 nd section 6.8 3. Infinite
More informationThe Henstock-Kurzweil integral
fculteit Wiskunde en Ntuurwetenschppen The Henstock-Kurzweil integrl Bchelorthesis Mthemtics June 2014 Student: E. vn Dijk First supervisor: Dr. A.E. Sterk Second supervisor: Prof. dr. A. vn der Schft
More informationx = b a n x 2 e x dx. cdx = c(b a), where c is any constant. a b
CHAPTER 5. INTEGRALS 61 where nd x = b n x i = 1 (x i 1 + x i ) = midpoint of [x i 1, x i ]. Problem 168 (Exercise 1, pge 377). Use the Midpoint Rule with the n = 4 to pproximte 5 1 x e x dx. Some quick
More informationAn inequality related to η-convex functions (II)
Int. J. Nonliner Anl. Appl. 6 (15) No., 7-33 ISSN: 8-68 (electronic) http://d.doi.org/1.75/ijn.15.51 An inequlity relted to η-conve functions (II) M. Eshghi Gordji, S. S. Drgomir b, M. Rostmin Delvr, Deprtment
More informationHYERS-ULAM STABILITY OF HIGHER-ORDER CAUCHY-EULER DYNAMIC EQUATIONS ON TIME SCALES
Dynmic Systems nd Applictions 23 (2014) 653-664 HYERS-ULAM STABILITY OF HIGHER-ORDER CAUCHY-EULER DYNAMIC EQUATIONS ON TIME SCALES DOUGLAS R. ANDERSON Deprtment of Mthemtics, Concordi College, Moorhed,
More informationTheoretical foundations of Gaussian quadrature
Theoreticl foundtions of Gussin qudrture 1 Inner product vector spce Definition 1. A vector spce (or liner spce) is set V = {u, v, w,...} in which the following two opertions re defined: (A) Addition of
More informationA Convergence Theorem for the Improper Riemann Integral of Banach Space-valued Functions
Interntionl Journl of Mthemticl Anlysis Vol. 8, 2014, no. 50, 2451-2460 HIKARI Ltd, www.m-hikri.com http://dx.doi.org/10.12988/ijm.2014.49294 A Convergence Theorem for the Improper Riemnn Integrl of Bnch
More informationA HELLY THEOREM FOR FUNCTIONS WITH VALUES IN METRIC SPACES. 1. Introduction
Ttr Mt. Mth. Publ. 44 (29), 159 168 DOI: 1.2478/v1127-9-56-z t m Mthemticl Publictions A HELLY THEOREM FOR FUNCTIONS WITH VALUES IN METRIC SPACES Miloslv Duchoň Peter Mličký ABSTRACT. We present Helly
More informationRiemann Sums and Riemann Integrals
Riemnn Sums nd Riemnn Integrls Jmes K. Peterson Deprtment of Biologicl Sciences nd Deprtment of Mthemticl Sciences Clemson University August 26, 2013 Outline 1 Riemnn Sums 2 Riemnn Integrls 3 Properties
More informationOn Stability of Nonlinear Slowly Time-Varying and Switched Systems
2018 IEEE Conference on Decision nd Control CDC) Mimi Bech, FL, USA, Dec. 17-19, 2018 On Stbility of Nonliner Slowly Time-Vrying nd Switched Systems Xiobin Go, Dniel Liberzon, nd Tmer Bşr Abstrct In this
More information11 An introduction to Riemann Integration
11 An introduction to Riemnn Integrtion The PROOFS of the stndrd lemms nd theorems concerning the Riemnn Integrl re NEB, nd you will not be sked to reproduce proofs of these in full in the exmintion in
More informationMultiple Positive Solutions for the System of Higher Order Two-Point Boundary Value Problems on Time Scales
Electronic Journl of Qulittive Theory of Differentil Equtions 2009, No. 32, -3; http://www.mth.u-szeged.hu/ejqtde/ Multiple Positive Solutions for the System of Higher Order Two-Point Boundry Vlue Problems
More informationFor a continuous function f : [a; b]! R we wish to define the Riemann integral
Supplementry Notes for MM509 Topology II 2. The Riemnn Integrl Andrew Swnn For continuous function f : [; b]! R we wish to define the Riemnn integrl R b f (x) dx nd estblish some of its properties. This
More informationMath Solutions to homework 1
Mth 75 - Solutions to homework Cédric De Groote October 5, 07 Problem, prt : This problem explores the reltionship between norms nd inner products Let X be rel vector spce ) Suppose tht is norm on X tht
More informationFundamental Theorem of Calculus and Computations on Some Special Henstock-Kurzweil Integrals
Fundmentl Theorem of Clculus nd Computtions on Some Specil Henstock-Kurzweil Integrls Wei-Chi YANG wyng@rdford.edu Deprtment of Mthemtics nd Sttistics Rdford University Rdford, VA 24142 USA DING, Xiofeng
More informationAccelerator Physics. G. A. Krafft Jefferson Lab Old Dominion University Lecture 5
Accelertor Phyic G. A. Krfft Jefferon L Old Dominion Univerity Lecture 5 ODU Accelertor Phyic Spring 15 Inhomogeneou Hill Eqution Fundmentl trnvere eqution of motion in prticle ccelertor for mll devition
More information