Analysis of a deteriorating cold standby system with priority

Size: px
Start display at page:

Download "Analysis of a deteriorating cold standby system with priority"

Transcription

1 Lixia Ma, Genqi Xu, Nikos E. Mastoakis Analysis of a deteioating cold standby system with pioity Lixia Ma Tianjin Univesity Depatment of Mathematics Tianjin, 372 P. R. China lixiama@tju.edu.cn Genqi Xu Tianjin Univesity Depatment of Mathematics Tianjin, 372 P. R. China gqxu@tju.edu.cn Nikos E. Mastoakis Militay Institutes of Univesity Education Hellenic Naval Academy Tema Hatzikyiakou, Piaeus, Geece masto@hna.g Abstact: A deteioating cold standby epaiable system consisting of two dissimila components and one epaiman is studied in this pape. Suppose that the life of each component satisfies the exponentially distibution and epai time of the component satisfies the geneal distibution, the component 1 has pioity in use and epai. Fistly, a mathematical model is built via the diffeential and patial diffeential equations. And then using the C -semigoup theoy of bounded linea opeatos, the existence and uniqueness of the solution, the non-negative steady-state solution and the exponential stability of the system ae deived. Based on the stability esult, some eliability indices of the system and an optimization poblem ae pesented at the end of the pape. Key Wods: C Semigoup, Well-Posedness, Asymptotic Stability, Exponential Stability, Availability. 1 Intoduction With the development of the moden technology and extensive use of electonic poducts, the eliability poblem of the epaable systems has become a hot topic. It is well known that the edundancy can enhance the eliability of the system. In the ealie study, the standby component doesn t fail in its standby peiod since they ae machine system. Howeve, the electonic poduct doesn t satisfy this popety. In fact, fo an electonic poduct, it has less failue ate if it is in use, othewise, it has geate failue ate afte cetain time, which means that it deteioates. Theefoe, in this pape we will discuss the eliability of a system consisting of the electonic poduct with epai. Fo the eliability poblem of system, it has been a hot topic in engineeing and Mathematics. Using mathematical model and Makov enewal theoy, one studied the indices of eliability of the epaable system, fo example, see [1], [2], [3]. Notice that, in the ealie eseach, the component afte epai is as good as new, only ecent a deteioating case is consideed in ([8]). Although some nice esults have been obtained, thee exists cetain difficulty to obtain some index of the system, fo instance, how long time one can see the stable state of the system. The mainly difficulty comes fom the mathematical model; this is because one cannot give an exact solution to the model. To ovecome this difficulty, many authos have woked on the analysis of the epaable systems using functional analysis method (see [4]-[6], etc), moe pecisely, semigoup theoy of bounded linea opeatos ([7]) to pove the well-posedness and the stability of the system. In this pape, we will give a new model about a cold standby epaiable system, and then discuss the system by functional analysis method. The est is oganized as follows. In section 2, a mathematical model fo the system unde consideation is established. And then in section 3, the existence and uniqueness of nonnegative time-dependent solution of the system ae pesented via C semigoup theoy. In section 4, by analyzing spectal distibution of the system opeato, the main esults on stability of the system ae obtained. In section 5 some indices of stationay state of the system and the estimation of instantaneous availability of the system ae given. Finally, an optimal epai ate poblem is studied. 2 Modeling fo a system with pioity Fistly, we descibe the system unde consideation. Suppose that a system consists of two dissimila components and one epaiman, the component 1 is the main woking unit and the component 2 is cold standby unit. The component 1 has pioity in use and epai. The system satisfies the following assumptions: Assumption 1. Initially, the two components ae both new, and component 1 is in a woking state while component 2 is in a standby state. Assumption 2. Assume that both components afte epai ae as good as new. ISSN: Issue 2, Volume 1, Febuay 211

2 Lixia Ma, Genqi Xu, Nikos E. Mastoakis Assumption 3. The component 1 has pioity in woking and epai. When both components ae good, the component 1 has the highe use pioity than the component 2, even if component 2 is woking, it must be switched immediately into the standby state as soon as component 1 afte epaied so that the component 1 becomes the woking state; When both components fail (i.e. the system is down), component 1 has the highe epai pioity than component 2, even if the epaiman is epaiing component 2, he must switch to epai the component 1. He will wok on the epai of component 2 afte completing the epai on component 1. Assumption 4. The standby component will pehaps fail in the standby time fo some eason. The failue and epai times of both components follow exponential distibution and geneal distibution espectively. λ j and ε denote the failue ate of component j(j 1, 2) and the standby component; µ j (x) denote the epai ate of component j(j 1, 2). Assumption 5. All failues ae independent of each othe. Unde these assumptions, we can divide the system into the following states: : The components 1 and 2 ae in good condition; 1: The component 1 is failue unde epai and the component 2 is woking; 2: The component 1 is woking and component 2 is failue unde epaiing; 3: The components 1 and 2 ae failue unde epai. P (t) denotes the pobability that component 1 is in woking state and component 2 is in cold standby state at time t; p 1 (t, x) epesents the pobability that the epaiman is dealing with component 1 with the elapsed time lying in [x, x + ) and component 2 is in wok at time t; p 2 (t, x) epesents the pobability that the epaiman is dealing with component 2 with the elapsed time lying in [x, x + ) and component 1 is in wok at time t; p 3 (t, x) epesents the pobability that the epaiman is dealing with component 1 with the elapsed time lying in [x, x + ) and component 2 is waiting fo epai at time t. By the supplementay vaiables technique, the model of the system can be fomulated as dp (t) dt (λ 1 + ε)p (t) + µ 1 (x)p 1 (x, t) + µ 2 (x)p 2 (x, t), p 1 (x,t) t p 1(x,t) x (µ 1 (x) + λ 2 )p 1 (x, t), p 2 (x,t) t p 2(x,t) x (µ 2 (x) + λ 1 )p 2 (x, t), p 3 (x,t) t p 3(x,t) x µ 1 (x)p 3 (x, t). (1) The bounday conditions ae p 1 (, t) λ 1 P (t), p 2 (, t) εp (t) + µ 1 (x)p 3 (x, t), p 3 (, t) λ 1 p 2 (x, t) + λ 2 p 1 (x, t), (2) whee (x, t) R + R +. 3 The well-possedness of the system solution In this section, we will discuss the well-posed-ness of the system. To this end, we fomulate the system (1) into a suitable Banach space. Based on the pactical backgound of ou model, we can assume that µ j (x)(j 1, 2) satisfy M sup x R + µ j (x) < ; µ j (s)ds. (3) In the sequel, we denote by R + [, ). Fom the physical meaning of the poblem, we take the s- tate space X R [L 1 (R + )] 3, equipped with the nom P P + 3 p j L 1, fo each P (P, p 1, p 2, p 3 ) X. Obviously, X is a Banach space. Define an opeato A : X X by A P p 1 (x) p 2 (x) p 3 (x) with domain D(A) P X (λ 1 + ε)p + 2 µ j(x)p j (x) ( d µ 1(x) λ 2 )p 1 (x), ( d µ 2(x) λ 1 )p 2 (x), ( d µ 1(x))p 3 (x) (4) p j (x) is absolutely continuous, p j (x), p j (x) L1 (R + ), p 1 () λ 1 P, p 2 () εp + µ 1(x)p 3 (x), p 3 () λ 1 p 2(x) + λ 2 p 1(x), j 1, 2, 3, (5) Obviously, A is a linea opeato in X. By the definition of A, the system (1) can be ewitten as an abstact Cauchy poblem in Banach s- pace X: { dp (t) dt AP (t), t, (6) P () (1,,, ). ISSN: Issue 2, Volume 1, Febuay 211

3 Lixia Ma, Genqi Xu, Nikos E. Mastoakis whee P (t) (P (t), p 1 (x, t), p 2 (x, t), p 3 (x, t)). By Theoem II 6.7 and Definition II 6.8 of [9], we know that the well-possedness of the system (1) is equivalent to the opeato A being the geneato of some C semigoup T (t). Theefoe, the main task of this section is to veify that the opeato A geneates a C semigoup. In paticula, the semigoup T (t) geneated by the opeato A is also positive and contactive. Theoem 1. Let A be defined by (4) and (5). Then the system opeato A is a closed and densely linea opeato in X. The poof is a diect veification (fo example, see [?]), so we omit. Theoem 2. A is a dissipative opeato in X, and γ ρ(a) fo Rγ >. Poof: We know that the dual space of X is X R (L (R + )) 3 by the diect veification, and the nom fo Q X is given by Q max{ q 1, q j, j 2, 3, 4}. Step I. We show A is dissipative. Fo any P D(A), we choose Q P ( P sign(p ), P sign(p 1 (x)), P sign(p 2 (x)), P sign(p 3 (x)) X Obviously, Q P F(P ) {Q X (P, Q P ) Q P 2 P 2 }. Moeove, (AP, Q P ) P { (λ 1 + ε) P + sign(p ) 2 3 µ j (x)p j (x) p j (x)sign(p j(x)) (µ 1(x)+λ 2 ) p 1 (x) (µ 2(x) + λ 1 ) p 2 (x) µ 1 (x) p 3 (x) }, while sign(p ) µ j (x)p j (x) µ j (x) p j (x), p j (x)sign(p j(x)) p j (), (j 1, 2) we have (AP,Q P ) P (λ 1 + ε) P + 3 p j () λ 2 p 1 (x) λ 1 p 2 (x) µ 1 (x) p 3 (x) (λ 1 + ε) P + λ 1 P + εp + µ 1 (x)p 3 (x) + λ 1 p 2 (x) +λ 2 p 1 (x) λ 2 p 1 (x) λ 1 p 2 (x) µ 1 (x) p 3 (x), i.e., A is dissipative. Step II. We pove that {γ C Rγ > } ρ(a). Fo any F (f, f 1, f 2, f 3 ) X, we conside the esolvent equation (γi A)P F, that is (γ + λ 1 + ε)p µ 1 (x)p 1 (x) µ 2 (x)p 2 (x) f, dp 1 (x) + (γ + µ 1 (x) + λ 2 )p 1 (x) f 1 (x), dp 2 (x) + (γ + µ 2 (x) + λ 1 )p 2 (x) f 2 (x), dp 3 (x) + (γ + µ 1 (x))p 3 (x) f 3 (x), p 1 () λ 1 P, p 2 () εp + µ 1 (x)p 3 (x), p 3 () λ 1 p 2 (x)+λ 2 p 1 (x). Solving the diffeential equations in (7) yields p 1 (x) p 1 () (γ+µ 1(s)+λ 2 )ds + f 1() p 2 (x) p 2 () (γ+µ 2(s)+λ 1 )ds + f 2() p 3 (x) p 3 () (γ+µ 1(s))ds + f 3() (γ+µ 1(s))ds d. By assumption to µ j (x), we have f 1 () (γ+µ 1(s)+λ 2 )ds d, (γ+µ 2(s)+λ 1 )ds d, (γ+µ 1(s)+λ 2 )ds d f 1 () (γ+µ 1(s)+λ 2 )ds d f 1 () d (γ+µ 1(s)+λ 2 )ds 1 Rγ + λ 2 f 1 L 1 1 Rγ f 1 L 1, (7) (8) so, p 1 L 1 (R + ) and µ 1 (x)p 1 (x) f 1 (x) + p 1 () (γ + λ 2 ) p 1 (x) is finite. Similaly, we can pove that p 2, p 3 L 1 (R + ) and µ 2 (x)p 2 (x) < +. Now we substitute (8) into (7) into bounday conditions (2) and get algebaic equations about (P, p 1 (), p 2 (), p 3 ()): (γ + λ 1 + ε)p p 1 ()G 1 (γ) p 2 ()G 2 (γ) f + H 1 (γ) + H 2 (γ), λ 1 P + p 1 (), εp + p 2 () p 3 ()G 3 (γ) H 3 (γ) λ 2 G 4 (γ)p 1 () λ 1 G 5 (γ)p 2 () + p 3 () λ 2 H 4 (γ) λ 1 H 5 (γ), (9) ISSN: Issue 2, Volume 1, Febuay 211

4 Lixia Ma, Genqi Xu, Nikos E. Mastoakis whee G 1 (γ) µ 1 (x) (γ+µ 1(s)+λ 2 )ds, H 1 (γ) µ 1 (x) f 1() G 2 (γ) µ 2 (x) (γ+µ 1(s)+λ 2 )ds d, (γ+µ 2(s)+λ 1 )ds, H 2 (γ) µ 2 (x) f 2() G 3 (γ) µ 1 (x) (γ+µ 1(s))ds, H 3 (γ) µ 1 (x) f 3() G 4 (γ) H 4 (γ) G 5 (γ) H 5 (γ) (γ+µ 2(s)+λ 1 )ds d, (γ+µ 1(x))ds d, (γ+µ 1(s)+λ 2 )ds, f 1() (γ+µ 1(s)+λ 2 )ds d, (γ+µ 2(s)+λ 1 )ds, (γ+µ 2(s)+λ 1 )ds d, f 2() (1) Denote the coefficient matix of (9) by (γ) and the deteminant by D(γ), then (γ) γ+λ 1 +ε G 1 (γ) G 2 (γ) λ 1 1 ε 1 G 3 (γ) λ 2 G 4 (γ) λ 1 G 5 (γ) 1 When Rγ >, it holds that G 1 (γ) + λ 2 G 4 (γ) (µ 1(x) + λ 2 ) (γ+µ 1(s)+λ 2 )ds < 1, G 2 (γ) + λ 1 G 5 (γ) (µ 2(x) + λ 1 ) (γ+µ 2(s)+λ 1 )ds < 1. (11) This shows that (γ) is column stictly diagonal dominant, so D(γ) and linea equations (9) has a unique solution (P, p 1 (), p 2 (), p 3 ()). Thus, it can be deived fom (8) that the esolvent equations (7) has a unique solution (P, p 1 (x), p 2 (x), p 3 (x)) D(A), which means γi A is sujection. Because γi A is closed and D(A) is dense in X, then (γi A) 1 exists and is bounded by Invese Opeato Theoem. So γ ρ(a). As a diect esult of Lume-Phillips Theoem (see, [7]), we have the following esult. Theoem 3. Let A and X be defined as befoe. Then A geneates a C -semigoup of contactions on X. Hence the equation (6) has a unique solution. Next, we will pove the existence of positive solutions to (1) since it is a pactical poblem. We complete the poof by showing A geneates a positive semigoup on X. Theoem 4. A geneates a positive C -semigoup of contactions on X. Poof: Accoding to the positive semigoup theoy (see [11]), A geneates a positive C -semigoup of contactions if and only if A is a dispesive and R(I A) X. Since Theoem 2 has asseted that R(I A) X, we only need to pove A is a dispesive opeato. Take Φ (sign + (P ), sign + (p 1 (x)), sign + (p 2 (x)), sign + (p 3 (x))) { 1, p > ; instead of Q P, whee sign + (P ), p. The othes is simila to the pocess of poving the dissipativity of the opeato A, so we omit. Theoem 5. The semigoup T (t) geneated by A is andom one. Poof: It is sufficient to pove that T (t) is positive consevative accoding to definition of andom semigoup. Fo any positive vecto P D(A), P (P,, p 1 (x), p 2 (x), p 3 (x)), we have T (t)p > and T (t)p D(A), since T (t) is positive. Set P (t, ) (P (t), p 1 (x, t), p 2 (x, t), p 3 (x, t)), obviously, T (t)p dt (t)p satisfies the equation dt AP, t >. Integating the diffeential equations in (1) fom to with espect to x, we have dp (t) dt + 3 d dt which shows that P (t) + 3 p j (x, t), p j (x, t) is a constant. Since T (t)p is continuous in t, we obtain T (t)p P (t) + 3 p j (x, t) P. So T (t) is a andom semigoup, which coincides with the physical meaning. 4 Stability of the system 4.1 Asymptotical stability In this section, we will discuss the stability of the system by analyzing the specta of the system opeato A. Lemma 6. Set µ γ µ(x) (iγ+µ(ξ))dξ, then{ µγ 1, if γ, and µ µ γ 1, if γ, γ < 1, γ. Theoem 7. γ is a simple eigenvalue of A. Moeove if fo any ξ R +, sup ξ ξ ξ µ 1(s)ds <. (12) Thee is no othe spectum of A besides zeo in the imaginay axis. ISSN: Issue 2, Volume 1, Febuay 211

5 Lixia Ma, Genqi Xu, Nikos E. Mastoakis Poof: Let us conside the equation AP, i.e., (λ 1 + ε)p µ 1 (x)p 1 (x) µ 2 (x)p 2 (x), dp 1 (x) + (µ 1 (x) + λ 2 )p 1 (x), dp 2 (x) + (µ 2 (x) + λ 1 )p 2 (x), dp 3 (x) + µ 1 (x)p 3 (x), p 1 () λ 1 P, p 2 () εp + µ 1 (x)p 3 (x), p 3 () λ 1 p 2 (x)+λ 2 p 1 (x). (13) Since 1 λ 1 G 5 () >, diectly solving the equations we get and p 1 () λ 1 P, p 2 () ε+λ 1λ 2 G 4 () 1 λ 1 G 5 () P, p 3 () ελ 1G 5 ()+λ 1 λ 2 G 4 () 1 λ 1 G 5 () P, p 1 (x) λ 1 P (µ 1(s)+λ 2 )ds, ε+λ p 2 (x) P 1 λ 2 G 4 () 1 λ 1 G 5 () e p 3 (x) P ελ 1 G 5 ()+λ 1 λ 2 G 4 () 1 λ 1 G 5 () (µ 2(s)+λ 1 )ds, (14) µ 1(s)ds. (15) So is an eigenvalue of A with geometic multiplicity one and P (P, p 1 (x), p 2 (x), p 3 (x)) given by (15) is the eigenvecto of A coesponding to. Next, we will pove that the algebaic multiplicity of is one. Obviously, the dual space of X is X R [L (R + )] 3. Let A be the dual opeato of A. By the definition of the dual opeato, we can obtain A Q (λ 1 + ε)q + λ 1 q + εq 2 () µ 1 (x)q + q 1 (x) (µ 1(x) + λ 2 )q 1 (x) + λ 2 q 3 () µ 2 (x)q + q 2 (x) (µ 2(x) + λ 1 )q 2 (x) + λ 1 q 3 () q 3 (x) µ 1(x)q 3 (x) + µ 1 (x)q 2 () whee Q (q, q 1 (x), q 2 (x), q 3 (x)) and D(A ) { Q X q j (x), q j (x) L (R + ) j 1, 2, 3 }. Clealy, Q (1, 1,, 1) D(A ) and A Q, so is an eigenvalue of A and Q (1, 1, 1, 1, 1, 1) is a coesponding eigenvecto. Let P be an eigenfunction of A given by (15), then(p, Q) 1. Theefoe, is a simple eigenvalue of A. Now, we show that {ib b } ρ(a). Fo b R, b, F X, let us conside the equation (ibi A)P F, (i.e., eplace γ with ib in (7)) and solving the diffeential equation in (7) yields p 1 (x) p 1 () (ib+µ 1(s)+λ 2 )ds + f 1() (ib+µ 1(s)+λ 2 )ds d, p 2 (x) p 2 () (ib+µ 2(s)+λ 1 )ds + f 2() (ib+µ 2(s)+λ 1 )ds (16) d, p 3 (x) p 3 ()e (ib+µ 1(s))ds + f 3() (ib+µ 1(s)ds d. It is easy to see that p 1, p 2 L 1 (R + ). Fo p 3, p 3 (x) p 3 () + f 3 () d By the assumption (12), we have f 3 () d µ 1(s)ds µ 1(s)ds µ 1(s)ds < (17) fo any f 3 L 1 (R + ), so p 3 L 1 (R + ). Accoding to the poof of Theoem 2, the algebaic equation about (P, p 1 (), p 2 (), p 3 ()) and the coefficient matix is (ib) having the same fom with (26). When b, fom Lemma 6 we know that G 1 (ib) + λ 2 G 4 (ib) (µ 1 (x) + λ 2 ) (ib+µ 1(s)+λ 2 )ds < 1 and G 2 (ib) + λ 1 G 5 (ib) < 1, G 3 (ib) < 1. Thus, (ib) is also column stictly diagonal dominant, so D(ib) and by the same method in Theoem 2, ib ρ(a). That is ir\{} ρ(a). Remak 8. The condition (12) is necessay fo ir\{} ρ(a), othewise the estimate (17) doesn t hold evidently. Let us conside a counteexample. Fom this example we also see that the existence of expectation of the epai time does not ensue the condition (12). If (12) doesn t hold, maybe we have ir σ(a). α 2+x Example 4.1. Let us conside function µ(x) with α > 1. We have e x µ(s)ds (2 + ) α (2 + x) α 2 + α 1. So sup µ(s)ds. Fo f() 1 e ib L 1 (R + ), we have (2+) 4 3 (ib+µ(s))ds f()d d (2 + ) (2 + ) d. α 1 α 2+s ds ISSN: Issue 2, Volume 1, Febuay 211

6 Lixia Ma, Genqi Xu, Nikos E. Mastoakis Summay discussion above, we have the following assetion. Theoem 9. Let space X and opeato A be defined as befoe, the condition (12) hold. Then the following statements ae tue 1)A geneates a positive C -semigoup of contactions T (t); 2) Thee exists a unique dynamic solution P (t) fo any initial value P (). In paticula, when the initial value is nonnegative, the dynamic solution P (t) is positive. 3) The system (1) has a positive steady-state ˆP (P, p 1 (x), p 2 (x), p 3 (x)) which is given by (15) with P 1 Z, whee Z 1 + λ 1 + ε+λ 1λ 2 G 4 () 1 λ 1 G 5 () + ελ 1G 5 ()+λ 1 λ 2 G 4 () 1 λ 1 G 5 () (µ 1(s)+λ 2 )ds (µ 2(s)+λ 1 )ds µ 1(s)ds (18) Futhemoe, the dynamic solution P (t) conveges to the nonnegative steady-state ˆP in the sense of nom, i.e. lim P (t) lim T (t)p () (P (), Q) ˆP. t t Poof: Recalling [1], the eigenfunction coesponding to eigenvalue of the system opeato defined by (15) is the stable solution the system (1), we denote it by ˆP. Note that ˆP 1, then the esult is deived immediately. 4.2 The exponential convegence In the pevious subsection we see that the dynamic solution of the system conveges to the steady state when condition (12) holds. In this subsection, we conside the ate of convegence unde some conditions about µ j (x)(j 1, 2) stonge than (12). Since sup µ 1(s)ds sup µ 1(s+)ds, we define non-negative eal numbe µ 1 by µ 1 sup{η sup e ηx µ 1(s+)ds < }. (19) In what follows, we always assume that µ 1 >, which implies that condition (12) holds. Obviously, when η < µ 1, the integal fo, sup (µ 1(s+) η)ds <, (2) while fo η > µ 1, it must be Set (µ 1(s) η)ds. µ min{ µ 1, λ 1 }. (21) Theoem 1. Let X, A and µ be defined as befoe. Then we have (I) The half-plane {γ C Rγ + µ < } ae in the spectum of A; (II) The set {γ C Rγ + µ >, D(γ) } is in the esolvent set of A and the set {γ C Rγ + µ >, D(γ) } consists of all eigenvalues of A; (III) δ >, thee ae at most finitely many eigenvalues of A in the egion {γ C Rγ + µ δ}; (IV) Thee exists a constant ω 1 > such that the egion {γ C Rγ > ω1 } has only one eigenvalue γ, thus it is stictly dominant. Poof Fo any γ and F (f, f 1 (x), f 2 (x), f 3 (x)) X, we conside the esolvent equation (γi A)P F, that is (γ + λ 1 + ε)p µ 1 (x)p 1 (x) µ 2 (x)p 2 (x) f, dp 1 (x) + (γ + µ 1 (x) + λ 2 )p 1 (x) f 1 (x), dp 2 (x) + (γ + µ 2 (x) + λ 1 )p 2 (x) f 2 (x), dp 3 (x) + (γ + µ 1 (x))p 3 (x) f 3 (x), p 1 () λ 1 P, p 2 () εp + µ 1 (x)p 3 (x), p 3 () λ 1 p 2 (x) + λ 2 p 1 (x). (22) Solving the diffeential equations in (22) yields p 1 (x) p 1 () (γ+µ 1(s)+λ 2 )ds + f 1() (γ+µ 1(s)+λ 2 )ds d, p 2 (x) p 2 () (γ+µ 2(s)+λ 1 )ds + f 2() (γ+µ 2(s)+λ 1 )ds d, p 3 (x) p 3 ()e (γ+µ 1(s))ds + f 3() (γ+µ 1(s))ds d, (23) When Rγ + µ >, using (2) the fist pat in the expession p 1 (x), p 2 (x), p 3 (x) ae bounded. Fo the second tems in the expession p 1 (x), p 2 (x) ae also bounded. Fo the second tem of p 3 (x), f 3 () (γ+µ 1(s))ds d f 3 () d M 2 (Rγ) f 3 L 1, (Rγ+µ 1(s))ds ISSN: Issue 2, Volume 1, Febuay 211

7 Lixia Ma, Genqi Xu, Nikos E. Mastoakis whee M 2 (Rγ) sup (Rγ+µ 1(s+))ds <. Theefoe, p j L 1 (R + ), j 1, 2, 3. Obviously, when Rγ + µ <, at least p 3 (x) in (23) is not in L 1 (R + ). Thus (I) follows. (II) Now we substitute (23) into bounday conditions in (22) and get the algebaic equations about (P, p 1 (), p 2 (), p 3 ()): (γ + λ 1 + ε)p p 1 ()G 1 (γ) p 2 ()G 2 (γ) f + H 1 (γ) + H 2 (γ), λ 1 P + p 1 (), εp + p 2 () p 3 ()G 3 (γ) H 3 (γ) λ 2 G 4 (γ)p 1 () λ 1 G 5 (γ)p 2 () + p 3 () λ 2 H 4 (γ) λ 1 H 5 (γ), (24) The coefficient deteminant of the equations (24) is D(γ) γ+λ 1 +ε G 1 (γ) G 2 (γ) λ 1 1 ε 1 G 3 (γ) λ 2 G 4 (γ) λ 1 G 5 (γ) 1 Then the algebaic equations have solution if and only if D(γ). When D(γ), the equations (24) has unique solution (P, p 1 (), p 2 (), p 3 ()), futhemoe, the vecto detemined by (23) (P, p 1 (x), p 2 (x), p 3 (x)) D(A), and (γi A)P F, so γ ρ(a). When D(γ), the equations (24) has nonzeo solution (P, p 1 (), p 2 (), p 3 ()), futhemoe, the vecto (P, p 1 (x), p 2 (x), p 3 (x)) D(A), and AP γp, so γ is an eigenvalues of A. (III) Note that G 1 (γ) + λ 2 G 4 (γ) (µ 1(x) + λ 2 ) (γ+µ 1(s)+λ 2 )ds, 1 γ (γ+µ 1(s)+λ 2 )ds 1 γg 4 (γ) G 2 (γ) + λ 1 G 5 (γ) 1 γ (γ+µ 2(s)+λ 1 )ds 1 γg 5 (γ), G 3 (γ) 1 γ (γ+µ 1(s))ds. (25) and whee D(γ) γ γg 4 (γ) γg 5 (γ) γπ(γ) λ 1 1 ε 1 G 3 (γ), λ 2 G 4 (γ) λ 1 G 5 (γ) 1 Π(γ) (γ+µ1(ξ))dξ. (26) So, fo all µ + δ Rγ, by condition (3) G 3 (γ) µ 1 (x)e (Rγ+ µ)x iiγx M e (Rγ+ µ)x (µ1(ξ) µ)dξ By Riemman Lemma, we have Similaly, G 4 (γ) e (Rγ+λ 2+ µ)x iiγx G 5 (γ) e (Rγ+λ 1+ µ)x iiγx Π(γ) e (Rγ+ µ)x iiγx The Riemman Lemma assets that lim G 4(γ), Iγ lim Iγ (µ 1(ξ) µ)dξ lim G 3(γ). Iγ (µ 1(ξ) µ)dξ (µ 2(ξ) µ)dξ (µ 1(ξ) µ)dξ lim Iγ lim G 5(γ). Hence, Iγ D(γ) γ 1 λ 1 1 ε (27) (28) Π(γ), The limit is unifomly in the egion µ+δ Rγ <. Moeove D(γ) is analytic function. So D(γ) has at most finite numbe of zeos in µ + δ Rγ <. Thus A has at most finite numbe eigenvalue in the egion µ + δ Rγ <. Moeove, thee is no othe spectum of A besides zeo in the imaginay axis accoding to Theoem 11. Thus (III) is tue. (IV) Set H 1 (γ) D(γ) γ. So γ is a zeo of D(γ) if and only if it is that of H 1 (γ). Since H 1 (γ) H 1 (γ), its zeos ae symmetically with espect to the eal axis. Note that µ > implies H 1 (ib), b R. Let the zeos of H 1 (γ) in the egion µ+δ Rγ be γ k, k 1, 2,, m. We can set ω 1 min Rγ k. 1 k m Thee is no zeo of H 1 (γ) as Rs > ω 1. Hence thee is only one eigenvalue γ of A in the egion {γ C Rγ > ω 1 }. Accoding to the finite expansion theoem of semigoups, we have the following esult. Theoem 11. Let X and A be defined as befoe, and let T (t) be the semigoup geneated by A. Suppose that µ > and < ω 1 < Rγ 1. Then fo any initial P (), we have P (t) P (), Q P 2e ω 1t P () (29) whee P (t) T (t)p (). ISSN: Issue 2, Volume 1, Febuay 211

8 Lixia Ma, Genqi Xu, Nikos E. Mastoakis Poof: Since the Riesz spectal poject coesponding to γ is given by E(γ, A)F 1 R(s, A)F ds F, Q 2πi P s ε fo F X. This leads to E(γ, A) 1. Since T (t) is a dissipative semigoup in (I E(γ, A))X, and the condition µ > ensues that the esolvent R(γ, A)F (P, p 1 (x), p 2 (x), p 3 (x) is bounded u- nifomly in the egion µ + δ Rγ when γ is lage enough. So we have The esult is deived. P (t) P (), Q P T (t)(i E(γ, A))P () e ω1t (I E(γ, A))P () 2e ω1t P (). 4.3 Special case In this subsection we discuss the special case that µ 1 (x), µ 2 (x) ae the constant functions. In this case, G 3 (s) µ 1 (γ+µ 1 ),G µ 4(γ) 1 (γ+µ 1 +λ 2 ) and G 5(γ) µ 2 (γ+µ 2 +λ 1 ). Hence and D(γ) whee γh 2 (γ) (γ + µ 1 )(γ + µ 1 + λ 2 )(γ + µ 2 + λ 1 ) H 2 (γ) γ 3 + a 2 γ 2 + a 1 γ + a a µ 1 µ 2 (λ 1 + λ 2 ) + λ 1 λ 2 (µ 1 µ 2 ) λ 2 1 λ 2 +µ 2 1 µ 2 + ε(µ λ 2µ 1 λ 1 µ 1 λ 1 λ 2 ), a 1 µ λ 1µ 1 + µ 2 λ 1 + λ 2 µ 1 + λ 2 µ 2 +2µ 1 µ 2 + 2εµ 1 + ελ 2 ελ 1, a 2 2λ 1 + 2λ 2 + 2µ 1 + µ 2 + ε, ae eal coefficients. Clealy, H 2 (γ) has thee zeos. 5 Reliability analysis of the system 5.1 Some indices deiving fom Steady-State Fom Theoem 9, we obtain the steady state of the system. Based on this, some indices of eliability can be deived. Theoem 12. The nomal steady-state availability of the system is A N v whee Z is given by (18). 1 Z (3) Poof: By the expession of steady state (18) and definition of the nomal availability A N v P, we know the esult holds. Accoding to the definition of abnomal availability we have A U v p 1 (x) + p 2 (x), Theoem 13. The abnomal steady-state availability of the system is A U v p 1 (x) + p 2 (x) λ 1 Z [ (µ 1(s)+λ 2 )ds + ε+λ 1 λ 2 G 4 () 1 λ 1 G 5 () e whee G 4 (), G 5 () is given by (1). (µ 2(s)+λ 1 )ds ] The steady-state availability of the system is A v A N v + A U v 1 Z + λ 1 Z [ + (µ 1(s)+λ 2 )ds ε+λ 1 λ 2 G 4 () 1 λ 1 G 5 () e (µ 2(s)+λ 1 )ds ] (31) (32) Remak : Fom the expession of Z, we can know if the system has stonge epai ate µ j (x), then µ j(s)ds has a smalle value, thus the nomal steady-state availability of the system will be lage, the failue pobability of the system p 3 (x) will be smalle, and system nomal eliability be enhanced. The aveage failue numbe of the system at time t is called the instantaneous failue fequency, denoted by W f (t), and its limit as t is called steady-state failue fequency of the system, denoted by W f. Fom [2] and the model of the system, we know We immediately have W f lim t p 3 (t, ) p 3 () (33) Theoem 14. The steady-state failue fequency of the system is W f ελ 1G 5 () + λ 1 λ 2 G 4 (). [1 λ 1 G 5 ()]Z 5.2 The estimation of instantaneous availability The instantaneous availability of the system is the pobability of the system being in wok, which is defined by A v (t) P (t) + p 1 (x, t) + p 2 (x, t). Fom Theoem 11, A v (t) A v P (t) P 2e ω t, ISSN: Issue 2, Volume 1, Febuay 211

9 Lixia Ma, Genqi Xu, Nikos E. Mastoakis whee A v is given by (32), we have A v (t) A v (t) A v + A v A v (t) A v + A v P (t) P + A v 2e ω t + A v. 3 ln 1 ln 5 Because when t > ω, P (t) P.1. So, we have A v (t).1 + A v. Obviously, the failue pobability of the system is p 3 (x, t) 1 A v (t). It has an estimate1 3 ln 1 ln 5 A v (t).99 A v, when t > ω. 6 Optimal epai ate fo steadystate eliability In this section, we shall conside a optimization poblem fo the epai ate µ(x) (µ 1 (x), µ 2 (x)). Suppose P is the expectable pobability of zeo state in steady-state and P (µ) is the fist component of solution of system coesponding to µ(x). Take the index functional S(µ) P (µ)) P 2. Ou aim is to find µ(x) (µ 1 (x), µ 2 (x)) such that it minimizes S(µ). Accoding to the assumptions (3), we let the admissible set be U { (µ1 (x), µ 2 (x)) [L (R + )] } 3 U ln(1+x) 1+x µ 1 (x), µ 2 (x) M Clealy U is a closed and convex set in [L (R + )] 3. Ou object is to find µ U such that S(µ ) inf µ U S(µ). (34) µ is said to be optimal epai ate of the system. To solve the poblem (34), let P R µ U such that (P, p 1 (x), p 2 (x), p 3 (x)) R (L 1 (R + )) 3 W is a nonnegative solution coesponding to µ(x) P +. p 1 (x) + p 2 (x) + p 3 (x) 1 (35) We fistly pove that thee exists a P W satisfying S(P ) inf S(P ) inf P P 2. (36) P W P W Theoem 15. W is a bounded and w -closed set in R. Poof: Fom the pevious section we know W is a bounded set. Now we pove that W is a closed set. Let P (n) W, and P (n) P. Then thee exist a sequence µ (n) (x) U such that P (n) (x) ae the nonnegative solution to (1) with bounday conditions (2). Since U [L (R + )] 3 is bounded and then w -sequence compact, thee exist a subsequence of µ (n) (x) without loss geneality itself such that µ (n) (x) w µ(x) ( µ 1 (x), µ 2 (x)). It is easy to see that µ 1 (x) and µ 2 (x) ae nonnegative functions. Fo any x R + fixed, the function χ [,x] (s) L 1 (R + ), the w convegence of µ (n) deduces that lim n lim n Since (µ (n) χ [,x] (s)µ (n) 1 (s)ds µ 1(s)ds, χ [,x] (s)µ (n) 2 (s)ds µ 2(s)ds. 1, µ(n) [ln(1 + x)]2 so it holds that 1 2 [ln(1 + x)]2 ) U implies that x µ (n) 1 (s)ds, x Mx, µ (n) 2 (s)ds µ 1 (s)ds, µ 2 (s)ds Mx. Theefoe, µ(x) U. On the othe hands, fom (15) we get that p (n) 1 (x) λ 1P (n) (µ(n) (n) ε+λ (x) P 1 λ 2 G 4 () p (n) 2 p (n) 3 (x) P (n) 1 (s)+λ2)ds, 1 λ 1 G 5 () e (µ(n) 2 (s)+λ1)ds, ελ 1 G (n) 5 ()+λ 1λ 2 G (n) 4 () e 1 λ 1 G (n) 5 () µ(n) 1 (s)ds. (37) The convegence of P (n) implies that fo each x R +, p (n) 1 (x), p(n) 2 (x) and p(n) 3 (x) ae convegent and the limit ae espectively p 1 (x) λ 1 ( µ 1(s)+λ 2 )ds P, p 2 (x) ε+λ 1λ 2 G 4 () 1 λ 1 G 5 () e ( µ 2(s)+λ 1 )ds P, p 3 (x) ελ 1G 5 ()+λ 1 λ 2 G 4 () 1 λ 1 G 5 () µ 1(s)ds P. Clealy, it holds that p 1 () λ 1 P p 2 () ε P + µ 1 (x) p 3 (x), p 3 () λ 1 p 2 (x, t) + λ 2 p 1 (x). Fom above expession we see that p 1 (x), p 2 (x) and p 3 (x) ae absolute continuous and P, p 1, p 2, p 3 (x), satisfy the diffeential equations in (1). ISSN: Issue 2, Volume 1, Febuay 211

10 Lixia Ma, Genqi Xu, Nikos E. Mastoakis Finally, we pove that the integal µ 1(s)ds is finite. Note that the elation 1 2 [ln(1 + x)]2 µ 1(s)ds Mx, we have µ(n) 1 (s)ds e 1 2 [ln(1+x)]2 <. The Fatou lemma assets that µ 1(s)ds e 1 2 [ln(1+x)]2. Thus, Z 1 + λ 1 + ε+λ 1λ 2 G 4 () 1 λ 1 G 5 () + ελ 1G 5 ()+λ 1 λ 2 G 4 () 1 λ 1 G 5 () ( µ 1(s)+λ 2 )ds ( µ 2(s)+λ 1 )ds µ 1(s)ds (38) has meaning. Theefoe, ( P, p 1 (x), p 2 (x), p 3 (x)) is a nonnegative solution of (1) coesponding to µ(x) ( µ 1 (x), µ 2 (x)), and satisfies condition P ( µ) + 3 p j (x) 1. So P W, and W is a closed set. Theoem 16. W is a convex set, and S(P ) is a stictly convex functional on W. Poof: Let P (1), P (2) W and P (1) P (2). By the definition of W thee exist µ (i) (µ (i) 1, µ(i) 2 ), i 1, 2 coesponding to P (i). Fo any < τ < 1, we set P (i) (P (i) (x), p(i) (x)) and, p(i) 1 (x), p(i) 2 P τ (x) τp (1) (x) + (1 τ)p (2) (x). A diect veification shows that P τ satisfy the diffeential equation (1) coesponding to µ τ τµ (1) +(1 τ)µ (2). So W is a convex set. Futhe, we have S(τP (1) + (1 τ)p (2) ) τp (1) + (1 τ)p (2) P 2 < τ P (1) P 2 + (1 τ) P (2) P 2 τs(p (1) ) + (1 τ)s(p (2) ). Theefoe, S(P ) is a stictly convex functional in W. Theoem 17. Thee exists a unique P that S(P ) inf S(P ). p W 3 W such Poof: Since W R + is a bounded and closed set, the existence and uniqueness of P W follows fom the theoy of the convex function on convex set. Theoem 18. If P W, then thee exists a unique µ U such that S(µ ) inf µ U S(µ). Poof: Note that S(P ) P P 2, S(µ) P (µ) P 2 and P (µ) 1 Z(µ) whee Z 1 + λ 1 + ε+λ 1λ 2 G 4 () 1 λ 1 G 5 () + ελ 1G 5 ()+λ 1 λ 2 G 4 () 1 λ 1 G 5 () (µ 1(s)+λ 2 )ds (µ 2(s)+λ 1 )ds µ 1(s)ds (39) whee G 4 () (µ 1(s)+λ 2 )ds, G 5 () (µ 2(s)+λ 1 )ds. Obviously, Z(µ) depends continuously on (µ 1, µ 2 ) U. In paticula, it holds that Z(µ) 1 + λ 1 M+λ 2 + ε(m+λ 2)+λ 1 λ 2 M(M+λ 2 ) + ελ 1(M+λ 2 )+λ 1 λ 2 (M+λ 1 ) M 2 ((M+λ 2 ) whee M is defined as in U. Theefoe, µ U, P (µ) 1 Z(µ) (4) M 2 (M+λ 2 ) M 2 ((M+λ 2 )+λ 1 M 2 +ε(m+λ 1 )(M+λ 2 )+λ 1 λ 2 M+λ 1 λ 2 (M+λ 1 ). Theefoe, when P W, it must have P > M 2 (M+λ 2 ) M 2 ((M+λ 2 )+λ 1 M 2 +ε(m+λ 1 )(M+λ 2 )+λ 1 λ 2 M+λ 1 λ 2 (M+λ 1 ). so S(µ) aives minimum at µ M(1, 1). Acknowledgements: The eseach is suppoted by the National Science Natual Foundation in China (NSFC ). Refeences: [1] K. C. Who, A Repaable Multistate Device With Abitaily Distibuted Repai Times, Micoelectonics and Reliability, 21(1981),2, pp [2] J. H. Cao and K. Cheng, Intoduction to Reliability Mathematics, Science Pess, Beijing, China, [3] R. B. Liu, Y. H. Tang and C. Y. Luo, A new kind of N-unit seies epaiable system and its eliability analysis. Applied Mathematical Modelling, 2 (27), 1,pp ISSN: Issue 2, Volume 1, Febuay 211

11 Lixia Ma, Genqi Xu, Nikos E. Mastoakis [4] W. L. Wang, and G. Q. Xu, Stability analysis of a complex standby system with constant waiting and diffeent epaiman citeia incopoating envionmental failue, Applied Mathematical Modelling, 33 (29), pp [5] L. N. Guo, H. B. Xu, C. Gao and G. T. Zhu, Stability analysis of a new kind seies system. IMA Jounal of Applied Mathematics, 75(21), pp [6] Z. F. Shen et al. Exponential asymptotic popety of a paallel epaiable system with wam standby unde common-cause failue. Mathematical Analysis and applications, 341(28), 1, pp [7] A. Pazy, Semigoup of linea opeatos and application to patial diffeential equations, Spinge-Velag, Belin, New Yok,1982. [8] Z. Y. Lin and G. J. Wang, A geometic pocess epai model fo a epaiable cold standby system with pioity in use and epai. Reliability Engineeing and System Safety, 94(29), pp [9] K. J. Engel and R. Nagel, One-paamete Semigoups fo Linea Evolution Equations, Gaduate Texts in Math, Vol.194, Spinge-Velag, 2. [1] G. Gupu, X. Z. Li and G. T. Zhu, Functional Analysis Method in Queuing Theoy, Hetfodshie, Reseach Infomation Ltd, United Kingdom, 21. [11] R. Nagel, One-Paamete Semigoup of Positive Opeatos, Lectue Notes in Mathematics, Spinge, New Yok, ISSN: Issue 2, Volume 1, Febuay 211

New problems in universal algebraic geometry illustrated by boolean equations

New problems in universal algebraic geometry illustrated by boolean equations New poblems in univesal algebaic geomety illustated by boolean equations axiv:1611.00152v2 [math.ra] 25 Nov 2016 Atem N. Shevlyakov Novembe 28, 2016 Abstact We discuss new poblems in univesal algebaic

More information

SOME SOLVABILITY THEOREMS FOR NONLINEAR EQUATIONS

SOME SOLVABILITY THEOREMS FOR NONLINEAR EQUATIONS Fixed Point Theoy, Volume 5, No. 1, 2004, 71-80 http://www.math.ubbcluj.o/ nodeacj/sfptcj.htm SOME SOLVABILITY THEOREMS FOR NONLINEAR EQUATIONS G. ISAC 1 AND C. AVRAMESCU 2 1 Depatment of Mathematics Royal

More information

SOME GENERAL NUMERICAL RADIUS INEQUALITIES FOR THE OFF-DIAGONAL PARTS OF 2 2 OPERATOR MATRICES

SOME GENERAL NUMERICAL RADIUS INEQUALITIES FOR THE OFF-DIAGONAL PARTS OF 2 2 OPERATOR MATRICES italian jounal of pue and applied mathematics n. 35 015 (433 44) 433 SOME GENERAL NUMERICAL RADIUS INEQUALITIES FOR THE OFF-DIAGONAL PARTS OF OPERATOR MATRICES Watheq Bani-Domi Depatment of Mathematics

More information

3.1 Random variables

3.1 Random variables 3 Chapte III Random Vaiables 3 Random vaiables A sample space S may be difficult to descibe if the elements of S ae not numbes discuss how we can use a ule by which an element s of S may be associated

More information

Journal of Inequalities in Pure and Applied Mathematics

Journal of Inequalities in Pure and Applied Mathematics Jounal of Inequalities in Pue and Applied Mathematics COEFFICIENT INEQUALITY FOR A FUNCTION WHOSE DERIVATIVE HAS A POSITIVE REAL PART S. ABRAMOVICH, M. KLARIČIĆ BAKULA AND S. BANIĆ Depatment of Mathematics

More information

Lecture 28: Convergence of Random Variables and Related Theorems

Lecture 28: Convergence of Random Variables and Related Theorems EE50: Pobability Foundations fo Electical Enginees July-Novembe 205 Lectue 28: Convegence of Random Vaiables and Related Theoems Lectue:. Kishna Jagannathan Scibe: Gopal, Sudhasan, Ajay, Swamy, Kolla An

More information

ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION. 1. Introduction. 1 r r. r k for every set E A, E \ {0},

ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION. 1. Introduction. 1 r r. r k for every set E A, E \ {0}, ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION E. J. IONASCU and A. A. STANCU Abstact. We ae inteested in constucting concete independent events in puely atomic pobability

More information

Perturbation to Symmetries and Adiabatic Invariants of Nonholonomic Dynamical System of Relative Motion

Perturbation to Symmetries and Adiabatic Invariants of Nonholonomic Dynamical System of Relative Motion Commun. Theo. Phys. Beijing, China) 43 25) pp. 577 581 c Intenational Academic Publishes Vol. 43, No. 4, Apil 15, 25 Petubation to Symmeties and Adiabatic Invaiants of Nonholonomic Dynamical System of

More information

A Multivariate Normal Law for Turing s Formulae

A Multivariate Normal Law for Turing s Formulae A Multivaiate Nomal Law fo Tuing s Fomulae Zhiyi Zhang Depatment of Mathematics and Statistics Univesity of Noth Caolina at Chalotte Chalotte, NC 28223 Abstact This pape establishes a sufficient condition

More information

THE CONE THEOREM JOEL A. TROPP. Abstract. We prove a fixed point theorem for functions which are positive with respect to a cone in a Banach space.

THE CONE THEOREM JOEL A. TROPP. Abstract. We prove a fixed point theorem for functions which are positive with respect to a cone in a Banach space. THE ONE THEOEM JOEL A. TOPP Abstact. We pove a fixed point theoem fo functions which ae positive with espect to a cone in a Banach space. 1. Definitions Definition 1. Let X be a eal Banach space. A subset

More information

KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS

KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS Jounal of Applied Analysis Vol. 14, No. 1 2008), pp. 43 52 KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS L. KOCZAN and P. ZAPRAWA Received Mach 12, 2007 and, in evised fom,

More information

Absorption Rate into a Small Sphere for a Diffusing Particle Confined in a Large Sphere

Absorption Rate into a Small Sphere for a Diffusing Particle Confined in a Large Sphere Applied Mathematics, 06, 7, 709-70 Published Online Apil 06 in SciRes. http://www.scip.og/jounal/am http://dx.doi.og/0.46/am.06.77065 Absoption Rate into a Small Sphee fo a Diffusing Paticle Confined in

More information

10/04/18. P [P(x)] 1 negl(n).

10/04/18. P [P(x)] 1 negl(n). Mastemath, Sping 208 Into to Lattice lgs & Cypto Lectue 0 0/04/8 Lectues: D. Dadush, L. Ducas Scibe: K. de Boe Intoduction In this lectue, we will teat two main pats. Duing the fist pat we continue the

More information

6 PROBABILITY GENERATING FUNCTIONS

6 PROBABILITY GENERATING FUNCTIONS 6 PROBABILITY GENERATING FUNCTIONS Cetain deivations pesented in this couse have been somewhat heavy on algeba. Fo example, detemining the expectation of the Binomial distibution (page 5.1 tuned out to

More information

Measure Estimates of Nodal Sets of Polyharmonic Functions

Measure Estimates of Nodal Sets of Polyharmonic Functions Chin. Ann. Math. Se. B 39(5), 08, 97 93 DOI: 0.007/s40-08-004-6 Chinese Annals of Mathematics, Seies B c The Editoial Office of CAM and Spinge-Velag Belin Heidelbeg 08 Measue Estimates of Nodal Sets of

More information

On the integration of the equations of hydrodynamics

On the integration of the equations of hydrodynamics Uebe die Integation de hydodynamischen Gleichungen J f eine u angew Math 56 (859) -0 On the integation of the equations of hydodynamics (By A Clebsch at Calsuhe) Tanslated by D H Delphenich In a pevious

More information

RADIAL POSITIVE SOLUTIONS FOR A NONPOSITONE PROBLEM IN AN ANNULUS

RADIAL POSITIVE SOLUTIONS FOR A NONPOSITONE PROBLEM IN AN ANNULUS Electonic Jounal of Diffeential Equations, Vol. 04 (04), o. 9, pp. 0. ISS: 07-669. UL: http://ejde.math.txstate.edu o http://ejde.math.unt.edu ftp ejde.math.txstate.edu ADIAL POSITIVE SOLUTIOS FO A OPOSITOE

More information

Gradient-based Neural Network for Online Solution of Lyapunov Matrix Equation with Li Activation Function

Gradient-based Neural Network for Online Solution of Lyapunov Matrix Equation with Li Activation Function Intenational Confeence on Infomation echnology and Management Innovation (ICIMI 05) Gadient-based Neual Netwok fo Online Solution of Lyapunov Matix Equation with Li Activation unction Shiheng Wang, Shidong

More information

Research Article On Alzer and Qiu s Conjecture for Complete Elliptic Integral and Inverse Hyperbolic Tangent Function

Research Article On Alzer and Qiu s Conjecture for Complete Elliptic Integral and Inverse Hyperbolic Tangent Function Abstact and Applied Analysis Volume 011, Aticle ID 697547, 7 pages doi:10.1155/011/697547 Reseach Aticle On Alze and Qiu s Conjectue fo Complete Elliptic Integal and Invese Hypebolic Tangent Function Yu-Ming

More information

ONE-POINT CODES USING PLACES OF HIGHER DEGREE

ONE-POINT CODES USING PLACES OF HIGHER DEGREE ONE-POINT CODES USING PLACES OF HIGHER DEGREE GRETCHEN L. MATTHEWS AND TODD W. MICHEL DEPARTMENT OF MATHEMATICAL SCIENCES CLEMSON UNIVERSITY CLEMSON, SC 29634-0975 U.S.A. E-MAIL: GMATTHE@CLEMSON.EDU, TMICHEL@CLEMSON.EDU

More information

Mean Curvature and Shape Operator of Slant Immersions in a Sasakian Space Form

Mean Curvature and Shape Operator of Slant Immersions in a Sasakian Space Form Mean Cuvatue and Shape Opeato of Slant Immesions in a Sasakian Space Fom Muck Main Tipathi, Jean-Sic Kim and Son-Be Kim Abstact Fo submanifolds, in a Sasakian space fom, which ae tangential to the stuctue

More information

Internet Appendix for A Bayesian Approach to Real Options: The Case of Distinguishing Between Temporary and Permanent Shocks

Internet Appendix for A Bayesian Approach to Real Options: The Case of Distinguishing Between Temporary and Permanent Shocks Intenet Appendix fo A Bayesian Appoach to Real Options: The Case of Distinguishing Between Tempoay and Pemanent Shocks Steven R. Genadie Gaduate School of Business, Stanfod Univesity Andey Malenko Gaduate

More information

Do Managers Do Good With Other People s Money? Online Appendix

Do Managers Do Good With Other People s Money? Online Appendix Do Manages Do Good With Othe People s Money? Online Appendix Ing-Haw Cheng Haison Hong Kelly Shue Abstact This is the Online Appendix fo Cheng, Hong and Shue 2013) containing details of the model. Datmouth

More information

Temporal-Difference Learning

Temporal-Difference Learning .997 Decision-Making in Lage-Scale Systems Mach 17 MIT, Sping 004 Handout #17 Lectue Note 13 1 Tempoal-Diffeence Leaning We now conside the poblem of computing an appopiate paamete, so that, given an appoximation

More information

Bifurcation Analysis for the Delay Logistic Equation with Two Delays

Bifurcation Analysis for the Delay Logistic Equation with Two Delays IOSR Jounal of Mathematics (IOSR-JM) e-issn: 78-578, p-issn: 39-765X. Volume, Issue 5 Ve. IV (Sep. - Oct. 05), PP 53-58 www.iosjounals.og Bifucation Analysis fo the Delay Logistic Equation with Two Delays

More information

Multiple Criteria Secretary Problem: A New Approach

Multiple Criteria Secretary Problem: A New Approach J. Stat. Appl. Po. 3, o., 9-38 (04 9 Jounal of Statistics Applications & Pobability An Intenational Jounal http://dx.doi.og/0.785/jsap/0303 Multiple Citeia Secetay Poblem: A ew Appoach Alaka Padhye, and

More information

Solution to HW 3, Ma 1a Fall 2016

Solution to HW 3, Ma 1a Fall 2016 Solution to HW 3, Ma a Fall 206 Section 2. Execise 2: Let C be a subset of the eal numbes consisting of those eal numbes x having the popety that evey digit in the decimal expansion of x is, 3, 5, o 7.

More information

STUDY OF SOLUTIONS OF LOGARITHMIC ORDER TO HIGHER ORDER LINEAR DIFFERENTIAL-DIFFERENCE EQUATIONS WITH COEFFICIENTS HAVING THE SAME LOGARITHMIC ORDER

STUDY OF SOLUTIONS OF LOGARITHMIC ORDER TO HIGHER ORDER LINEAR DIFFERENTIAL-DIFFERENCE EQUATIONS WITH COEFFICIENTS HAVING THE SAME LOGARITHMIC ORDER UNIVERSITATIS IAGELLONICAE ACTA MATHEMATICA doi: 104467/20843828AM170027078 542017, 15 32 STUDY OF SOLUTIONS OF LOGARITHMIC ORDER TO HIGHER ORDER LINEAR DIFFERENTIAL-DIFFERENCE EQUATIONS WITH COEFFICIENTS

More information

Results on the Commutative Neutrix Convolution Product Involving the Logarithmic Integral li(

Results on the Commutative Neutrix Convolution Product Involving the Logarithmic Integral li( Intenational Jounal of Scientific and Innovative Mathematical Reseach (IJSIMR) Volume 2, Issue 8, August 2014, PP 736-741 ISSN 2347-307X (Pint) & ISSN 2347-3142 (Online) www.acjounals.og Results on the

More information

Using Laplace Transform to Evaluate Improper Integrals Chii-Huei Yu

Using Laplace Transform to Evaluate Improper Integrals Chii-Huei Yu Available at https://edupediapublicationsog/jounals Volume 3 Issue 4 Febuay 216 Using Laplace Tansfom to Evaluate Impope Integals Chii-Huei Yu Depatment of Infomation Technology, Nan Jeon Univesity of

More information

Failure Probability of 2-within-Consecutive-(2, 2)-out-of-(n, m): F System for Special Values of m

Failure Probability of 2-within-Consecutive-(2, 2)-out-of-(n, m): F System for Special Values of m Jounal of Mathematics and Statistics 5 (): 0-4, 009 ISSN 549-3644 009 Science Publications Failue Pobability of -within-consecutive-(, )-out-of-(n, m): F System fo Special Values of m E.M.E.. Sayed Depatment

More information

Lacunary I-Convergent Sequences

Lacunary I-Convergent Sequences KYUNGPOOK Math. J. 52(2012), 473-482 http://dx.doi.og/10.5666/kmj.2012.52.4.473 Lacunay I-Convegent Sequences Binod Chanda Tipathy Mathematical Sciences Division, Institute of Advanced Study in Science

More information

ESSENTIAL NORM OF AN INTEGRAL-TYPE OPERATOR ON THE UNIT BALL. Juntao Du and Xiangling Zhu

ESSENTIAL NORM OF AN INTEGRAL-TYPE OPERATOR ON THE UNIT BALL. Juntao Du and Xiangling Zhu Opuscula Math. 38, no. 6 (8), 89 839 https://doi.og/.7494/opmath.8.38.6.89 Opuscula Mathematica ESSENTIAL NORM OF AN INTEGRAL-TYPE OPERATOR FROM ω-bloch SPACES TO µ-zygmund SPACES ON THE UNIT BALL Juntao

More information

arxiv: v1 [math.co] 4 May 2017

arxiv: v1 [math.co] 4 May 2017 On The Numbe Of Unlabeled Bipatite Gaphs Abdullah Atmaca and A Yavuz Ouç axiv:7050800v [mathco] 4 May 207 Abstact This pape solves a poblem that was stated by M A Haison in 973 [] This poblem, that has

More information

Central Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution

Central Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution Statistics Reseach Lettes Vol. Iss., Novembe Cental Coveage Bayes Pediction Intevals fo the Genealized Paeto Distibution Gyan Pakash Depatment of Community Medicine S. N. Medical College, Aga, U. P., India

More information

An Exact Solution of Navier Stokes Equation

An Exact Solution of Navier Stokes Equation An Exact Solution of Navie Stokes Equation A. Salih Depatment of Aeospace Engineeing Indian Institute of Space Science and Technology, Thiuvananthapuam, Keala, India. July 20 The pincipal difficulty in

More information

Goodness-of-fit for composite hypotheses.

Goodness-of-fit for composite hypotheses. Section 11 Goodness-of-fit fo composite hypotheses. Example. Let us conside a Matlab example. Let us geneate 50 obsevations fom N(1, 2): X=nomnd(1,2,50,1); Then, unning a chi-squaed goodness-of-fit test

More information

Bounds for Codimensions of Fitting Ideals

Bounds for Codimensions of Fitting Ideals Ž. JOUNAL OF ALGEBA 194, 378 382 1997 ATICLE NO. JA966999 Bounds fo Coensions of Fitting Ideals Michał Kwiecinski* Uniwesytet Jagiellonski, Instytut Matematyki, ul. eymonta 4, 30-059, Kakow, Poland Communicated

More information

Banach Journal of Mathematical Analysis ISSN: (electronic)

Banach Journal of Mathematical Analysis ISSN: (electronic) Banach J. Math. Anal. 4 200), no., 87 9 Banach Jounal of Mathematical Analysis ISSN: 75-8787 electonic) www.emis.de/jounals/bjma/ ON A REVERSE OF ANDO HIAI INEQUALITY YUKI SEO This pape is dedicated to

More information

arxiv: v1 [math.co] 1 Apr 2011

arxiv: v1 [math.co] 1 Apr 2011 Weight enumeation of codes fom finite spaces Relinde Juius Octobe 23, 2018 axiv:1104.0172v1 [math.co] 1 Ap 2011 Abstact We study the genealized and extended weight enumeato of the - ay Simplex code and

More information

GROWTH ESTIMATES THROUGH SCALING FOR QUASILINEAR PARTIAL DIFFERENTIAL EQUATIONS

GROWTH ESTIMATES THROUGH SCALING FOR QUASILINEAR PARTIAL DIFFERENTIAL EQUATIONS Annales Academiæ Scientiaum Fennicæ Mathematica Volumen 32, 2007, 595 599 GROWTH ESTIMATES THROUGH SCALING FOR QUASILINEAR PARTIAL DIFFERENTIAL EQUATIONS Teo Kilpeläinen, Henik Shahgholian and Xiao Zhong

More information

A THREE CRITICAL POINTS THEOREM AND ITS APPLICATIONS TO THE ORDINARY DIRICHLET PROBLEM

A THREE CRITICAL POINTS THEOREM AND ITS APPLICATIONS TO THE ORDINARY DIRICHLET PROBLEM A THREE CRITICAL POINTS THEOREM AND ITS APPLICATIONS TO THE ORDINARY DIRICHLET PROBLEM DIEGO AVERNA AND GABRIELE BONANNO Abstact. The aim of this pape is twofold. On one hand we establish a thee citical

More information

A Relativistic Electron in a Coulomb Potential

A Relativistic Electron in a Coulomb Potential A Relativistic Electon in a Coulomb Potential Alfed Whitehead Physics 518, Fall 009 The Poblem Solve the Diac Equation fo an electon in a Coulomb potential. Identify the conseved quantum numbes. Specify

More information

Weighted least-squares estimators of parametric functions of the regression coefficients under a general linear model

Weighted least-squares estimators of parametric functions of the regression coefficients under a general linear model Ann Inst Stat Math (2010) 62:929 941 DOI 10.1007/s10463-008-0199-8 Weighted least-squaes estimatos of paametic functions of the egession coefficients unde a geneal linea model Yongge Tian Received: 9 Januay

More information

SPECTRAL SEQUENCES. im(er

SPECTRAL SEQUENCES. im(er SPECTRAL SEQUENCES MATTHEW GREENBERG. Intoduction Definition. Let a. An a-th stage spectal (cohomological) sequence consists of the following data: bigaded objects E = p,q Z Ep,q, a diffeentials d : E

More information

PROBLEM SET #1 SOLUTIONS by Robert A. DiStasio Jr.

PROBLEM SET #1 SOLUTIONS by Robert A. DiStasio Jr. POBLM S # SOLUIONS by obet A. DiStasio J. Q. he Bon-Oppenheime appoximation is the standad way of appoximating the gound state of a molecula system. Wite down the conditions that detemine the tonic and

More information

Application of Parseval s Theorem on Evaluating Some Definite Integrals

Application of Parseval s Theorem on Evaluating Some Definite Integrals Tukish Jounal of Analysis and Numbe Theoy, 4, Vol., No., -5 Available online at http://pubs.sciepub.com/tjant/// Science and Education Publishing DOI:.69/tjant--- Application of Paseval s Theoem on Evaluating

More information

Pearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms

Pearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms Peason s Chi-Squae Test Modifications fo Compaison of Unweighted and Weighted Histogams and Two Weighted Histogams Univesity of Akueyi, Bogi, v/noduslód, IS-6 Akueyi, Iceland E-mail: nikolai@unak.is Two

More information

Boundedness for Marcinkiewicz integrals associated with Schrödinger operators

Boundedness for Marcinkiewicz integrals associated with Schrödinger operators Poc. Indian Acad. Sci. (Math. Sci. Vol. 24, No. 2, May 24, pp. 93 23. c Indian Academy of Sciences oundedness fo Macinkiewicz integals associated with Schödinge opeatos WENHUA GAO and LIN TANG 2 School

More information

Enumerating permutation polynomials

Enumerating permutation polynomials Enumeating pemutation polynomials Theodoulos Gaefalakis a,1, Giogos Kapetanakis a,, a Depatment of Mathematics and Applied Mathematics, Univesity of Cete, 70013 Heaklion, Geece Abstact We conside thoblem

More information

Conservative Averaging Method and its Application for One Heat Conduction Problem

Conservative Averaging Method and its Application for One Heat Conduction Problem Poceedings of the 4th WSEAS Int. Conf. on HEAT TRANSFER THERMAL ENGINEERING and ENVIRONMENT Elounda Geece August - 6 (pp6-) Consevative Aveaging Method and its Application fo One Heat Conduction Poblem

More information

Vanishing lines in generalized Adams spectral sequences are generic

Vanishing lines in generalized Adams spectral sequences are generic ISSN 364-0380 (on line) 465-3060 (pinted) 55 Geomety & Topology Volume 3 (999) 55 65 Published: 2 July 999 G G G G T T T G T T T G T G T GG TT G G G G GG T T T TT Vanishing lines in genealized Adams spectal

More information

Construction and Analysis of Boolean Functions of 2t + 1 Variables with Maximum Algebraic Immunity

Construction and Analysis of Boolean Functions of 2t + 1 Variables with Maximum Algebraic Immunity Constuction and Analysis of Boolean Functions of 2t + 1 Vaiables with Maximum Algebaic Immunity Na Li and Wen-Feng Qi Depatment of Applied Mathematics, Zhengzhou Infomation Engineeing Univesity, Zhengzhou,

More information

LET a random variable x follows the two - parameter

LET a random variable x follows the two - parameter INTERNATIONAL JOURNAL OF MATHEMATICS AND SCIENTIFIC COMPUTING ISSN: 2231-5330, VOL. 5, NO. 1, 2015 19 Shinkage Bayesian Appoach in Item - Failue Gamma Data In Pesence of Pio Point Guess Value Gyan Pakash

More information

Solving Some Definite Integrals Using Parseval s Theorem

Solving Some Definite Integrals Using Parseval s Theorem Ameican Jounal of Numeical Analysis 4 Vol. No. 6-64 Available online at http://pubs.sciepub.com/ajna///5 Science and Education Publishing DOI:.69/ajna---5 Solving Some Definite Integals Using Paseval s

More information

On the Quasi-inverse of a Non-square Matrix: An Infinite Solution

On the Quasi-inverse of a Non-square Matrix: An Infinite Solution Applied Mathematical Sciences, Vol 11, 2017, no 27, 1337-1351 HIKARI Ltd, wwwm-hikaicom https://doiog/1012988/ams20177273 On the Quasi-invese of a Non-squae Matix: An Infinite Solution Ruben D Codeo J

More information

On Computing Optimal (Q, r) Replenishment Policies under Quantity Discounts

On Computing Optimal (Q, r) Replenishment Policies under Quantity Discounts Annals of Opeations Reseach manuscipt No. will be inseted by the edito) On Computing Optimal, ) Replenishment Policies unde uantity Discounts The all - units and incemental discount cases Michael N. Katehakis

More information

This aticle was oiginally published in a jounal published by Elsevie, the attached copy is povided by Elsevie fo the autho s benefit fo the benefit of the autho s institution, fo non-commecial eseach educational

More information

A pathway to matrix-variate gamma and normal densities

A pathway to matrix-variate gamma and normal densities Linea Algeba and its Applications 396 005 317 38 www.elsevie.com/locate/laa A pathway to matix-vaiate gamma and nomal densities A.M. Mathai Depatment of Mathematics and Statistics, McGill Univesity, 805

More information

arxiv: v1 [math.nt] 28 Oct 2017

arxiv: v1 [math.nt] 28 Oct 2017 ON th COEFFICIENT OF DIVISORS OF x n axiv:70049v [mathnt] 28 Oct 207 SAI TEJA SOMU Abstact Let,n be two natual numbes and let H(,n denote the maximal absolute value of th coefficient of divisos of x n

More information

QIP Course 10: Quantum Factorization Algorithm (Part 3)

QIP Course 10: Quantum Factorization Algorithm (Part 3) QIP Couse 10: Quantum Factoization Algoithm (Pat 3 Ryutaoh Matsumoto Nagoya Univesity, Japan Send you comments to yutaoh.matsumoto@nagoya-u.jp Septembe 2018 @ Tokyo Tech. Matsumoto (Nagoya U. QIP Couse

More information

Duality between Statical and Kinematical Engineering Systems

Duality between Statical and Kinematical Engineering Systems Pape 00, Civil-Comp Ltd., Stiling, Scotland Poceedings of the Sixth Intenational Confeence on Computational Stuctues Technology, B.H.V. Topping and Z. Bittna (Editos), Civil-Comp Pess, Stiling, Scotland.

More information

ON LACUNARY INVARIANT SEQUENCE SPACES DEFINED BY A SEQUENCE OF MODULUS FUNCTIONS

ON LACUNARY INVARIANT SEQUENCE SPACES DEFINED BY A SEQUENCE OF MODULUS FUNCTIONS STUDIA UNIV BABEŞ BOLYAI, MATHEMATICA, Volume XLVIII, Numbe 4, Decembe 2003 ON LACUNARY INVARIANT SEQUENCE SPACES DEFINED BY A SEQUENCE OF MODULUS FUNCTIONS VATAN KARAKAYA AND NECIP SIMSEK Abstact The

More information

On a quantity that is analogous to potential and a theorem that relates to it

On a quantity that is analogous to potential and a theorem that relates to it Su une quantité analogue au potential et su un théoème y elatif C R Acad Sci 7 (87) 34-39 On a quantity that is analogous to potential and a theoem that elates to it By R CLAUSIUS Tanslated by D H Delphenich

More information

On the Poisson Approximation to the Negative Hypergeometric Distribution

On the Poisson Approximation to the Negative Hypergeometric Distribution BULLETIN of the Malaysian Mathematical Sciences Society http://mathusmmy/bulletin Bull Malays Math Sci Soc (2) 34(2) (2011), 331 336 On the Poisson Appoximation to the Negative Hypegeometic Distibution

More information

Analytical Solutions for Confined Aquifers with non constant Pumping using Computer Algebra

Analytical Solutions for Confined Aquifers with non constant Pumping using Computer Algebra Poceedings of the 006 IASME/SEAS Int. Conf. on ate Resouces, Hydaulics & Hydology, Chalkida, Geece, May -3, 006 (pp7-) Analytical Solutions fo Confined Aquifes with non constant Pumping using Compute Algeba

More information

Moment-free numerical approximation of highly oscillatory integrals with stationary points

Moment-free numerical approximation of highly oscillatory integrals with stationary points Moment-fee numeical appoximation of highly oscillatoy integals with stationay points Sheehan Olve Abstact We pesent a method fo the numeical quadatue of highly oscillatoy integals with stationay points.

More information

JENSEN S INEQUALITY FOR DISTRIBUTIONS POSSESSING HIGHER MOMENTS, WITH APPLICATION TO SHARP BOUNDS FOR LAPLACE-STIELTJES TRANSFORMS

JENSEN S INEQUALITY FOR DISTRIBUTIONS POSSESSING HIGHER MOMENTS, WITH APPLICATION TO SHARP BOUNDS FOR LAPLACE-STIELTJES TRANSFORMS J. Austal. Math. Soc. Se. B 40(1998), 80 85 JENSEN S INEQUALITY FO DISTIBUTIONS POSSESSING HIGHE MOMENTS, WITH APPLICATION TO SHAP BOUNDS FO LAPLACE-STIELTJES TANSFOMS B. GULJAŠ 1,C.E.M.PEACE 2 and J.

More information

A new approach in classical electrodynamics to protect principle of causality

A new approach in classical electrodynamics to protect principle of causality A new appoach in classical electodynamics to potect pinciple of causality Biswaanjan Dikshit * Lase and Plasma Technology Division Bhabha Atomic Reseach Cente, Mumbai-400085 INDIA * Coesponding autho E-mail:

More information

q i i=1 p i ln p i Another measure, which proves a useful benchmark in our analysis, is the chi squared divergence of p, q, which is defined by

q i i=1 p i ln p i Another measure, which proves a useful benchmark in our analysis, is the chi squared divergence of p, q, which is defined by CSISZÁR f DIVERGENCE, OSTROWSKI S INEQUALITY AND MUTUAL INFORMATION S. S. DRAGOMIR, V. GLUŠČEVIĆ, AND C. E. M. PEARCE Abstact. The Ostowski integal inequality fo an absolutely continuous function is used

More information

Integral operator defined by q-analogue of Liu-Srivastava operator

Integral operator defined by q-analogue of Liu-Srivastava operator Stud. Univ. Babeş-Bolyai Math. 582013, No. 4, 529 537 Integal opeato defined by q-analogue of Liu-Sivastava opeato Huda Aldweby and Maslina Daus Abstact. In this pape, we shall give an application of q-analogues

More information

Functions Defined on Fuzzy Real Numbers According to Zadeh s Extension

Functions Defined on Fuzzy Real Numbers According to Zadeh s Extension Intenational Mathematical Foum, 3, 2008, no. 16, 763-776 Functions Defined on Fuzzy Real Numbes Accoding to Zadeh s Extension Oma A. AbuAaqob, Nabil T. Shawagfeh and Oma A. AbuGhneim 1 Mathematics Depatment,

More information

Information Retrieval Advanced IR models. Luca Bondi

Information Retrieval Advanced IR models. Luca Bondi Advanced IR models Luca Bondi Advanced IR models 2 (LSI) Pobabilistic Latent Semantic Analysis (plsa) Vecto Space Model 3 Stating point: Vecto Space Model Documents and queies epesented as vectos in the

More information

6 Matrix Concentration Bounds

6 Matrix Concentration Bounds 6 Matix Concentation Bounds Concentation bounds ae inequalities that bound pobabilities of deviations by a andom vaiable fom some value, often its mean. Infomally, they show the pobability that a andom

More information

Some Remarks on the Boundary Behaviors of the Hardy Spaces

Some Remarks on the Boundary Behaviors of the Hardy Spaces Soe Reaks on the Bounday Behavios of the Hady Spaces Tao Qian and Jinxun Wang In eoy of Jaie Kelle Abstact. Soe estiates and bounday popeties fo functions in the Hady spaces ae given. Matheatics Subject

More information

Localization of Eigenvalues in Small Specified Regions of Complex Plane by State Feedback Matrix

Localization of Eigenvalues in Small Specified Regions of Complex Plane by State Feedback Matrix Jounal of Sciences, Islamic Republic of Ian (): - () Univesity of Tehan, ISSN - http://sciencesutaci Localization of Eigenvalues in Small Specified Regions of Complex Plane by State Feedback Matix H Ahsani

More information

Mitscherlich s Law: Sum of two exponential Processes; Conclusions 2009, 1 st July

Mitscherlich s Law: Sum of two exponential Processes; Conclusions 2009, 1 st July Mitschelich s Law: Sum of two exponential Pocesses; Conclusions 29, st July Hans Schneebege Institute of Statistics, Univesity of Elangen-Nünbeg, Gemany Summay It will be shown, that Mitschelich s fomula,

More information

A Backward Identification Problem for an Axis-Symmetric Fractional Diffusion Equation

A Backward Identification Problem for an Axis-Symmetric Fractional Diffusion Equation Mathematical Modelling and Analysis Publishe: Taylo&Fancis and VGTU Volume 22 Numbe 3, May 27, 3 32 http://www.tandfonline.com/tmma https://doi.og/.3846/3926292.27.39329 ISSN: 392-6292 c Vilnius Gediminas

More information

A STABILITY RESULT FOR p-harmonic SYSTEMS WITH DISCONTINUOUS COEFFICIENTS. Bianca Stroffolini. 0. Introduction

A STABILITY RESULT FOR p-harmonic SYSTEMS WITH DISCONTINUOUS COEFFICIENTS. Bianca Stroffolini. 0. Introduction Electonic Jounal of Diffeential Equations, Vol. 2001(2001), No. 02, pp. 1 7. ISSN: 1072-6691. URL: http://ejde.math.swt.edu o http://ejde.math.unt.edu ftp ejde.math.swt.edu (login: ftp) A STABILITY RESULT

More information

Identification of the degradation of railway ballast under a concrete sleeper

Identification of the degradation of railway ballast under a concrete sleeper Identification of the degadation of ailway ballast unde a concete sleepe Qin Hu 1) and Heung Fai Lam ) 1), ) Depatment of Civil and Achitectual Engineeing, City Univesity of Hong Kong, Hong Kong SAR, China.

More information

A PROOF OF THE INF-SUP CONDITION FOR THE STOKES EQUATIONS ON LIPSCHITZ DOMAINS

A PROOF OF THE INF-SUP CONDITION FOR THE STOKES EQUATIONS ON LIPSCHITZ DOMAINS A PROOF OF THE INF-SUP CONDITION FOR THE STOKES EQUATIONS ON LIPSCHITZ DOMAINS JAMES H. BRAMBLE Abstact. The pupose of this pape is to pesent a athe simple poof of an inequality of Nečas [9] which is equivalent

More information

On the Comparison of Stability Analysis with Phase Portrait for a Discrete Prey-Predator System

On the Comparison of Stability Analysis with Phase Portrait for a Discrete Prey-Predator System Intenational Jounal of Applied Engineeing Reseach ISSN 0973-4562 Volume 12, Nume 24 (2017) pp. 15273-15277 Reseach India Pulications. http://www.ipulication.com On the Compaison of Staility Analysis with

More information

Mathematical Model of Magnetometric Resistivity. Sounding for a Conductive Host. with a Bulge Overburden

Mathematical Model of Magnetometric Resistivity. Sounding for a Conductive Host. with a Bulge Overburden Applied Mathematical Sciences, Vol. 7, 13, no. 7, 335-348 Mathematical Model of Magnetometic Resistivity Sounding fo a Conductive Host with a Bulge Ovebuden Teeasak Chaladgan Depatment of Mathematics Faculty

More information

Analytical solutions to the Navier Stokes equations

Analytical solutions to the Navier Stokes equations JOURAL OF MATHEMATICAL PHYSICS 49, 113102 2008 Analytical solutions to the avie Stokes equations Yuen Manwai a Depatment of Applied Mathematics, The Hong Kong Polytechnic Univesity, Hung Hom, Kowloon,

More information

Asymptotically Lacunary Statistical Equivalent Sequence Spaces Defined by Ideal Convergence and an Orlicz Function

Asymptotically Lacunary Statistical Equivalent Sequence Spaces Defined by Ideal Convergence and an Orlicz Function "Science Stays Tue Hee" Jounal of Mathematics and Statistical Science, 335-35 Science Signpost Publishing Asymptotically Lacunay Statistical Equivalent Sequence Spaces Defined by Ideal Convegence and an

More information

Method for Approximating Irrational Numbers

Method for Approximating Irrational Numbers Method fo Appoximating Iational Numbes Eic Reichwein Depatment of Physics Univesity of Califonia, Santa Cuz June 6, 0 Abstact I will put foth an algoithm fo poducing inceasingly accuate ational appoximations

More information

Compactly Supported Radial Basis Functions

Compactly Supported Radial Basis Functions Chapte 4 Compactly Suppoted Radial Basis Functions As we saw ealie, compactly suppoted functions Φ that ae tuly stictly conditionally positive definite of ode m > do not exist The compact suppot automatically

More information

Chromatic number and spectral radius

Chromatic number and spectral radius Linea Algeba and its Applications 426 2007) 810 814 www.elsevie.com/locate/laa Chomatic numbe and spectal adius Vladimi Nikifoov Depatment of Mathematical Sciences, Univesity of Memphis, Memphis, TN 38152,

More information

MATH 220: SECOND ORDER CONSTANT COEFFICIENT PDE. We consider second order constant coefficient scalar linear PDEs on R n. These have the form

MATH 220: SECOND ORDER CONSTANT COEFFICIENT PDE. We consider second order constant coefficient scalar linear PDEs on R n. These have the form MATH 220: SECOND ORDER CONSTANT COEFFICIENT PDE ANDRAS VASY We conside second ode constant coefficient scala linea PDEs on R n. These have the fom Lu = f L = a ij xi xj + b i xi + c i whee a ij b i and

More information

Hua Xu 3 and Hiroaki Mukaidani 33. The University of Tsukuba, Otsuka. Hiroshima City University, 3-4-1, Ozuka-Higashi

Hua Xu 3 and Hiroaki Mukaidani 33. The University of Tsukuba, Otsuka. Hiroshima City University, 3-4-1, Ozuka-Higashi he inea Quadatic Dynamic Game fo Discete-ime Descipto Systems Hua Xu 3 and Hioai Muaidani 33 3 Gaduate School of Systems Management he Univesity of suuba, 3-9- Otsua Bunyo-u, oyo -0, Japan xuhua@gssm.otsua.tsuuba.ac.jp

More information

COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS

COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS Pogess In Electomagnetics Reseach, PIER 73, 93 105, 2007 COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS T.-X. Song, Y.-H. Liu, and J.-M. Xiong School of Mechanical Engineeing

More information

Application of homotopy perturbation method to the Navier-Stokes equations in cylindrical coordinates

Application of homotopy perturbation method to the Navier-Stokes equations in cylindrical coordinates Computational Ecology and Softwae 5 5(): 9-5 Aticle Application of homotopy petubation method to the Navie-Stokes equations in cylindical coodinates H. A. Wahab Anwa Jamal Saia Bhatti Muhammad Naeem Muhammad

More information

arxiv: v1 [math.na] 8 Feb 2013

arxiv: v1 [math.na] 8 Feb 2013 A mixed method fo Diichlet poblems with adial basis functions axiv:1302.2079v1 [math.na] 8 Feb 2013 Nobet Heue Thanh Tan Abstact We pesent a simple discetization by adial basis functions fo the Poisson

More information

15 Solving the Laplace equation by Fourier method

15 Solving the Laplace equation by Fourier method 5 Solving the Laplace equation by Fouie method I aleady intoduced two o thee dimensional heat equation, when I deived it, ecall that it taes the fom u t = α 2 u + F, (5.) whee u: [0, ) D R, D R is the

More information

A method for solving dynamic problems for cylindrical domains

A method for solving dynamic problems for cylindrical domains Tansactions of NAS of Azebaijan, Issue Mechanics, 35 (7), 68-75 (016). Seies of Physical-Technical and Mathematical Sciences. A method fo solving dynamic poblems fo cylindical domains N.B. Rassoulova G.R.

More information

DonnishJournals

DonnishJournals DonnishJounals 041-1189 Donnish Jounal of Educational Reseach and Reviews. Vol 1(1) pp. 01-017 Novembe, 014. http:///dje Copyight 014 Donnish Jounals Oiginal Reseach Pape Vecto Analysis Using MAXIMA Savaş

More information

Math 124B February 02, 2012

Math 124B February 02, 2012 Math 24B Febuay 02, 202 Vikto Gigoyan 8 Laplace s equation: popeties We have aleady encounteed Laplace s equation in the context of stationay heat conduction and wave phenomena. Recall that in two spatial

More information

Appraisal of Logistics Enterprise Competitiveness on the Basis of Fuzzy Analysis Algorithm

Appraisal of Logistics Enterprise Competitiveness on the Basis of Fuzzy Analysis Algorithm Appaisal of Logistics Entepise Competitiveness on the Basis of Fuzzy Analysis Algoithm Yan Zhao, Fengge Yao, Minming She Habin Univesity of Commece, Habin, Heilongjiang 150028, China, zhaoyan2000@yahoo.com.cn

More information

On absence of solutions of a semi-linear elliptic equation with biharmonic operator in the exterior of a ball

On absence of solutions of a semi-linear elliptic equation with biharmonic operator in the exterior of a ball Tansactions of NAS of Azebaijan, Issue Mathematics, 36, 63-69 016. Seies of Physical-Technical and Mathematical Sciences. On absence of solutions of a semi-linea elliptic euation with bihamonic opeato

More information

working pages for Paul Richards class notes; do not copy or circulate without permission from PGR 2004/11/3 10:50

working pages for Paul Richards class notes; do not copy or circulate without permission from PGR 2004/11/3 10:50 woking pages fo Paul Richads class notes; do not copy o ciculate without pemission fom PGR 2004/11/3 10:50 CHAPTER7 Solid angle, 3D integals, Gauss s Theoem, and a Delta Function We define the solid angle,

More information