Size: px
Start display at page:

Download ""

Transcription

1 Print of 1 2/3/ :12 AM On Monday, 2 Febrary :26 PM, Editor AJS <editor_ajs@rediffmail.com> wrote: Dear Prof. Uixit, I am glad to inform yo that yor paper entitled, Characterizations of the Pareto distribtion in the presence of otliers has been accepted for pblication in The Aligarh Jornal of Statistics. To expedite its pblication and also make it error free, the Editorial board of the AJS has decided that the accepted paper be sbmitted on a CD in the format given below*. It is, therefore, reqested to please send the paper as early as possible on a CD sing MS-Word alongwith a hard copy of it. Yor co-operation is solicited. With regards, Sincerely yors, (Prof. Qazi M. Ali) Editor *Paper size : A4 Line spacing : Single Font size : 11 Font style : Times New Roman Eqations : MS Eqation 3.0 Typing area : First page : 5.0 x 7.0 Other page: 5.0 x 8.0 Odd nmbered pages : Rnning title of the paper Even nmbered pages : Athors name Editor Aligarh Jornal of Statistics Dept. of Statistics & O.R. Aligarh Mslim University Aligarh , U.P. INDIA. Phone: editor_ajs@rediffmail.com Web site:

2 Characterizations of the Pareto distribtion in the presence of otliers U. J. Dixit 1 Department of Statistics, University of Mmbai, Mmbai-India M. Jabbari Nooghabi 2 Department of Statistics, Ferdowsi University of Mashhad, Mashhad-Iran Abstract Here we have given some characterizations for the Pareto distribtion in the presence of otliers. It is proved that a necessary and sfficient condition for f(x) to be a Pareto density fnction in the presence of otliers is that the statistics X (r) and X (s) X (1 r < s n) are independent. Frther, we have derived some another (r) characterizations of the Pareto distribtion in the presence of otliers. Key Words: Pareto distribtion, Power distribtion, Characterization, Order statistics, Otliers. 1 Introdction Ahsanllah and Kabir [2] proved that necessary and sfficient condition for f(x) to be a Pareto distribtion is that the statistics X (r) and X (s) X (r) (1 r < s n) are independent. Dallas [3] proved that for a cmlative distribtion fnction (CDF) G(y) (y β), if E(Y r Y > c) = E ( ) r Y c β holds then Y has a Pareto distribtion. In this paper, we assme that the random variables (X 1, X 2,..., X n ) are sch that k of them are distribted with probability density fnction (pdf) f 2 (x; α, β, ) = α()α, 0 < x, α > 0, β > 1, > 0, (1) xα+1 and remaining (n k) random variables are distribted as f 1 (x; α, ) = αα, 0 < x, α > 0. (2) xα+1 One shold note that two sets of the observation (i.e. k and n k) are independent. Bt X 1, X 2,..., X n are not independent becase of the model of otliers (for more details see [5, 7, 8]). Also, we may note that or assmptions are based of Dixit s model for 1 lhasdixit@yahoo.co.in 2 jabbarinm@yahoo.com, jabbarinm@m.ac.ir 1

3 the otliers problem and it is totaly different than the mixtre models which considers X 1, X 2,..., X n are independent. Here, we have extended the approaches of Ahsanllah and Kabir [2] and Dallas [3] for the homogenos case of the Pareto distribtion and derived some characterizations of the Pareto distribtion in the presence of otliers. 2 Prereqisite Reslts Assme that X (1) < X (2) <... < X (n) be the order statistics of a random sample of size n sch that k ot of n are coming from pdf f 2 (or CDF F 2 ) and the remaining (n k) follow the pdf f 1 (or CDF F 1 ). The CDF and pdf of r th (1 r n) order statistic are H X(r) (x) = n i=r m 6 j=m 5 C(k, j)[f 2 (x)] j [1 F 2 (x)] k j C(n k, i j)[f 1 (x)] i j [1 F 1 (x)] n k i+j, (3) where m 5 = max(0, i n + k) and m 6 = min(k, i) and m 2 h X(r) (x) = kf 2 (x) {C(k 1, j)[f 2 (x)] j [1 F 2 (x)] k j 1 C(n k, r 1 j) j=m 1 [F 1 (x)] r j 1 [1 F 1 (x)] n k r+j+1 } + (n k)f 1 (x) {C(k, j)[f 2 (x)] j j=m 3 [1 F 2 (x)] k j C(n k 1, r 1 j)[f 1 (x)] r j 1 [1 F 1 (x)] n k r+j }, (4) where m 1 = max(0, k + r n 1), m 2 = min(k 1, r 1), m 3 = max(0, k + r n), m 4 = min(k, r 1), respectively (for more details see [4, 5, 6, 8]). Frther, the joint CDF and pdf of (X (r), X (s) ) (1 r < s n) are H X(r),X (s) (x, y) = n j w 10 j=s i=r m=w 9 t 10 m 4 l=t 9 {C(k, m)c(k m, l)[f 2 (x)] m [F 2 (y) F 2 (x)] l [1 F 2 (y)] k m l C(n k, i m)c(n k i + m, j i l)[f 1 (x)] i m [F 1 (y) F 1 (x)] j i l [1 F 1 (y)] n k j+m+l }, (5) where w 9 = max(0, i n + k), w 10 = min(k, i), t 9 = max(0, j n + k m) and t 10 = min(k m, j i) and h X(r),X (s) (x, y) = k(k 1)f 2 (x)f 2 (y) w 2 j=w 1 t 2 i=t 1 {C(k 2, j)c(n k, r 1 j)[f 2 (x)] j [F 1 (x)] r 1 j C(k 2 j, i)c(n k r + j + 1, n s i)[1 F 2 (y)] i [1 F 1 (y)] n s i [F 2 (y) F 2 (x)] k j i 2 [F 1 (y) F 1 (x)] s r k+i+j+1 } + (n k)(n k 1)f 1 (x)f 1 (y) 2 w 4 j=w 3 t 4 i=t 3 {C(n k 2, j)c(k, r 1 j)

4 [F 1 (x)] j [F 2 (x)] r 1 j C(n k 2 j, i)c(k r + j + 1, n s i)[1 F 1 (y)] i [1 F 2 (y)] n s i [F 1 (y) F 1 (x)] n k 2 i j [F 2 (y) F 2 (x)] s r+k n+i+j+1 } + k(n k)f 1 (x)f 2 (y) w 6 j=w 5 t 6 i=t 5 {C(n k 1, j)c(k 1, r 1 j) [F 1 (x)] j [F 2 (x)] r 1 j C(n k j 1, i)c(k r + j, n s i)[1 F 1 (y)] i [1 F 2 (y)] n s i [F 1 (y) F 1 (x)] n k i j 1 [F 2 (y) F 2 (x)] s r n+k+i+j } + k(n k)f 2 (x)f 1 (y) w 8 j=w 7 t 8 i=t 7 {C(k 1, j)c(n k 1, r 1 j) [F 2 (x)] j [F 1 (x)] r 1 j C(k j 1, i)c(n k r + j, n s i)[1 F 2 (y)] i [1 F 1 (y)] n s i [F 2 (y) F 2 (x)] k i j 1 [F 1 (y) F 1 (x)] s r k+i+j }, (6) where w 1 = max(0, r n + k 1), w 2 = min(k 2, r 1), t 1 = max(0, k s + r j 1) and t 2 = min(k j 2, n s), w 3 = max(0, r k 1), w 4 = min(n k 2, r 1), t 3 = max(0, n s k + r j 1) and t 4 = min(n k j 2, n s), w 5 = max(0, r k), w 6 = min(n k 1, r 1), t 5 = max(0, n s k +r j 1), t 6 = min(n k j 1, n s), w 7 = max(0, r n + k), w 8 = min(k 1, r 1), t 7 = max(0, k s + r j 1), t 8 = min(k j 1, n s), respectively. One shold note that if k = 1 the joint pdf of (X (r), X (s) ) is given in Sinha [10]. Also, if we pt f 1 = f 2 and F 1 = F 2 then all pdfs and CDFs are redced to homogeneos cases. The following eqations are named as Pexider s eqations. and f(xy) = g(x) + h(y), (7) f(xy) = g(x)h(y). (8) For solving these eqations, the following Theorem has taken from Aczel [1] (Theorem 4. in p. 144) and Kczma [9] (Theorem in p. 358). Theorem 2.1. The general soltions, with f continos in a point of (7) and (8), respectively, both spposed for positive x and y, are and f(t) = c ln(αβt), g(t) = c ln(αt), h(t) = c ln(βt), (α > 0, β > 0, t > 0), (9) f(t) = abt c, g(t) = at c, h(t) = bt c, (t > 0), (10) respectively, spplemented with the following trivial soltions in case of (8). f(t) = 0, g(t) = 0, h(t) arbitrary, and f(t) = 0, g(t) arbitrary, h(t) = 0. (11) 3

5 3 Characterization of the Pareto distribtion in the presence of otliers Theorem 3.1. Let X be a random variable having an absoltely continos CDF F (x). A necessary and sfficient condition that X follows the Pareto distribtion in the presence of otliers as given by (1) and (2) is that for some r and s (1 r < s n) the statistics X (r) and X (s) X (r) are independent. Proof. Necessity: From (6) we can get the joint pdf of X (r) and X (s). Sbstitting U = X (r) and V = X (s) X (r) in (6), we can obtain the joint pdf of U and V as h U,V (, v) = h X(r),X (s) (, v). Then after some simplification (replace h U,V (, v) with h(, v)) h(, v) = α 2 α(n r+1) β αk v α(s n 1) 1 [1 v α ] s r 1 [ ( ) w2 α(r n 1) 1 k(k 1) t 2 α ] j [ ( ) α ] r 1 j A 1 β αj 1 1 j=w 1 i=t 1 [ ( ) w 4 + (n k)(n k 1)β α(r 1) t 4 α ] j [ ( ) α ] r 1 j A 2 β αj 1 1 j=w 3 i=t 3 [ ( ) w 6 + k(n k)β α(r 1) t 6 α ] j [ ( ) α ] r 1 j A 3 β αj 1 1 j=w 5 i=t 5 [ ( ) w 8 t 8 α ] j [ ( ) α ] r 1 j + k(n k) A 4 β αj 1 1 i=t 7, (12) j=w 7 where A 1 = C(k 2, j)c(n k, r 1 j)c(k 2 j, i)c(n k r + j + 1, n s i), A 2 = C(n k 2, j)c(k, r 1 j)c(n k 2 j, i)c(k r + j + 1, n s i), A 3 = C(n k 1, j)c(k 1, r 1 j)c(n k j 1, i)c(k r + j, n s i), (13) A 4 = C(k 1, j)c(n k 1, r 1 j)c(k j 1, i)c(n k r + j, n s i). Therefore, it establishes the independence of U and V. Sfficiency: Here we assme that U and V are independent. The joint pdf of U and V is h(, v) = k(k 1)f 2 ()f 2 (v) w 2 j=w 1 t 2 i=t 1 {A 1 [F 2 ()] j [F 1 ()] r 1 j [1 F 2 (v)] i 4

6 [1 F 1 (v)] n s i [F 2 (v) F 2 ()] k j i 2 [F 1 (v) F 1 ()] s r k+i+j+1 } + (n k)(n k 1)f 1 ()f 1 (v) w 4 j=w 3 t 4 i=t 3 {A 2 [F 1 ()] j [F 2 ()] r 1 j [1 F 1 (v)] i [1 F 2 (v)] n s i [F 1 (v) F 1 ()] n k 2 i j [F 2 (v) F 2 ()] s r+k n+i+j+1 } + k(n k)f 1 ()f 2 (v) w 6 j=w 5 t 6 i=t 5 {A 3 [F 1 ()] j [F 2 ()] r 1 j [1 F 1 (v)] i [1 F 2 (v)] n s i [F 1 (v) F 1 ()] n k i j 1 [F 2 (v) F 2 ()] s r n+k+i+j } + k(n k)f 2 ()f 1 (v) w 8 j=w 7 t 8 i=t 7 {A 4 [F 2 ()] j [F 1 ()] r 1 j [1 F 2 (v)] i [1 F 1 (v)] n s i [F 2 (v) F 2 ()] k i j 1 [F 1 (v) F 1 ()] s r k+i+j }, (14) where A 1, A 2, A 3 and A 4 are given in (13). By sing some elementary algebra we have h(, v) = k(k 1)f 2 ()f 2 (v)[f 1 ()] r 1 [1 F 1 (v)] n s [F 1 (v) F 1 ()] s r k+1 w 2 [F 2 (v) F 2 ()] k 2 t 2 j j [ F2 () 1 F1 () 1 F 2 (v) {A 1 i=t 1 F 1 () 1 F 2 () F 2 (v) F 2 () j=w 1 i j [ F1 (v) F 1 () F1 (v) F 1 () 1 F 1 (v) 1 F 1 () 1 F 2 () F 2 (v) F 2 () + (n k)(n k 1)f 1 ()f 1 (v)[f 2 ()] r 1 [1 F 2 (v)] n s [F 1 (v) F 1 ()] n k 2 w 4 [F 2 (v) F 2 ()] s r+k n+1 t 4 j j [ F1 () 1 F2 () 1 F 1 (v) {A 2 i=t 3 F 2 () 1 F 1 () F 1 (v) F 1 () i [ F2 (v) F 2 () 1 F 2 (v) j=w 3 1 F 1 () F 1 (v) F 1 () ] j } ] j j F2 (v) F 2 () } 1 F 2 () + k(n k)f 1 ()f 2 (v)[f 2 ()] r 1 [1 F 2 (v)] n s [F 1 (v) F 1 ()] n k 1 w 6 [F 2 (v) F 2 ()] s r+k n t 6 j j [ F1 () 1 F2 () 1 F 1 (v) {A 3 j=w 5 i=t 5 F 2 () 1 F 1 () F 1 (v) F 1 () i j [ ] j F2 (v) F 2 () F2 (v) F 2 () 1 F 1 () } 1 F 2 (v) 1 F 2 () F 1 (v) F 1 () + k(n k)f 2 ()f 1 (v)[f 1 ()] r 1 [1 F 1 (v)] n s [F 2 (v) F 2 ()] k 1 w 8 [F 1 (v) F 1 ()] s r k t 8 j j [ ] i F2 () 1 F1 () 1 F 2 (v) {A 4 j=w 7 i=t 7 F 1 () 1 F 2 () F 2 (v) F 2 () i j [ ] j F1 (v) F 1 () F1 (v) F 1 () 1 F 2 () }. (15) 1 F 1 (v) 1 F 1 () F 2 (v) F 2 () Also from (4) and after some simplification, the marginal pdf of U = X (r) is as h 1 (). h 1 () = [1 F 2 ()] k 1 [F 1 ()] r 1 [1 F 1 ()] n k r+1 D, (16) 5 ] i ] i ] i

7 where and D = kf 2 () m 2 j=m 1 B 1 + (n k)f 1 () j [ F2 () 1 F1 () F 1 () 1 F 2 () 1 F2 () m4 1 F 1 () j=m 3 B 2 ] j [ F2 () F 1 () B 1 = C(k 1, j)c(n k, r 1 j), B 2 = C(k, j)c(n k 1, r 1 j). ] j j 1 F1 (), 1 F 2 () (17) Therefore from independency of U and V, we can write h 2 (v) = h(, v) h 1 (), (18) where h 2 (v) is pdf of V. Letting p = p(, v) = 1 F 1(v) 1 F 1 () and q = q(, v) = 1 F 2(v) 1 F 2, we obtain () w 2 h 2 (v) = {k(k 1)p n s [1 p] s k r+1 [1 q] k 2 t 2 A 1 j=w 1 i=t 1 A 4 j=w 7 i=t 7 [ F2 () F 1 () ] j j 1 F1 () 1 F 2 () p i [1 p] i+j q i [1 q] i j f 2 () q v r 1 r 2 F2 () 1 F1 () + (n k)(n k 1) [1 p] n k 2 q n s [1 q] k+s r n+1 F 1 () 1 F 2 () w 4 t 4 j j F1 () 1 F2 () A 2 q i [1 q] i+j p i [1 p] i j f 1 () p j=w 3 i=t 3 F 2 () 1 F 1 () v r 1 r 2 F2 () 1 F1 () + k(n k) q n s [1 q] k+s r n [1 p] n k 1 F 1 () 1 F 2 () w 6 t 6 j j F1 () 1 F2 () A 3 p i [1 p] i j q i [1 q] i+j f 1 () q j=w 5 i=t 5 F 2 () 1 F 1 () v w 8 + k(n k)p n s [1 p] s k r [1 q] k 1 t 8 j j F2 () 1 F1 () F 1 () 1 F 2 () p i [1 p] i+j q i [1 q] i j f 2 () p v }D 1. (19) From the assmption, we know that U and V are independent. So h 2 (v) is independent of and by sing the lemma in Ahsanllah and Kabir [2] p = p(, v) = g 1 (v) and 6

8 q = q(, v) = g 2 (v) (we say fnctions of v only) and the remaining parts shold be constant. Therefore { 1 F1 (v) = [1 F 1 ()]g 1 (v),, 1 < v, > 0, (20) 1 F 2 (v) = [1 F 2 ()]g 2 (v),, 1 < v, > 0, β > 1. It is clear that these are version of Pexider s eqation. So from Theorem 2.1 we can solve them. Since F 1 (x) and F 2 (x) are CDFs continos for all x [, ) and x [, ), respectively. We may conclde that { 1 F1 (x) = c 1 x α, x, > 0, 1 F 2 (x) = c 2 x α, x, > 0, β > 1, (21) where c 1, c 2 and α are constant. After replacing these soltions in (19) and sing some simplification we get where h 2 (v) = αv α(n s+1) 1 [1 v α ] s r 1 H[c 2 D] 1, (22) w 2 H = k(k 1)c 2 t 2 A 1 j=w 1 i=t 1 w 4 + (n k)(n k 1)c 1 w 6 + k(n k)c 1 + k(n k)c 2 t 8 A 3 j=w 5 i=t 5 i=t 7 A 4 t 6 [ 1 c2 α 1 c 1 α t 4 A 2 j=w 3 i=t 3 [ 1 c2 α 1 c 1 α [ 1 c2 α 1 c 1 α ] j (c1 ) j c 2 [ 1 c2 α 1 c 1 α ] r 1 j (c1 ) r 2 j ] j (c1 ) j. c 2 c 2 ] r 1 j (c1 ) r 2 j We know that C(n, j) = 0 if j > n, then by sing some elementary algebra H[c 2 D] 1 = (n r)c(n r 1, n s) and the right side of (22) is only depend on v and it is pdf of V. Finally, from the property of CDF, α > 0, c 1 = α and c 2 = () α. Ths sfficiency is established and the proof is complete. Theorem 3.2. Let X be a random variable with CDF F (x) = bf 2 (x) + bf 1 (x) sch that F 1 (x) (x ) and F 2 (x) (x ) are CDFs, where b = k n, b = 1 b, > 0 and β > 1. If E(X α X > c) = be 2 ( Xc ) α + be ( ) Xc α 1, (23) holds for some α > 0 then F (x) is the Pareto distribtion in the presence of otliers. We assme that E(X α ) <. Proof. Proof is similar as given in Dallas [3]. In the process to prove the theorem, 7 c 2

9 we shold note that the soltion of the differential eqation cp (c) = γp (c) (P (c) = 1 F (c)) is P (c) = Ac α, where A is a constant, γ = αδ/(δ 1) > 0 and δ = b ( ) α X df 2 (x) + b ( X ) α df 1 (x). (24) Comparing the soltion with the assmption imply that A = b() α + b α and the proof is complete. 4 An actal example Here, we have given an example of motor insrance company from Dixit and Jabbari Nooghabi [7]. From the example, we know that the data follow the Preto distribtion in the presence of otliers. So by sing Theorem 3.1, we can check the sfficiency. Assming r = 3 and s = 12, we have x (r) =63000, and x (s) x (r) = So, sing the copla method and independent test by package copla in R, the reslt is as follows: Global Cramer-von Mises statistic: with p-vale Combined p-vales from the Mobis decomposition: from Fisher s rle, from Tippett s rle. Therefore, X (r) and X (s) X (r) are independent, becase of the p-vale is grater than 0.05, as significant level of the test. So, we can conclde that the data follow the Pareto distribtion in the presence of otliers. 5 Acknowledgements The athors are thankfl to the two referees for their valable comments and sggestions. This research was spported by a grant from Ferdowsi University of Mashhad, No. MS92299MEH. References [1] Aczel, J. (1966). Lectres on Fnctional Eqations and their Applications. Academic Press, New York. [2] Ahsanllah, M. and Kabir Ltfl A. B. M. (1973). A Characterization of the Pareto Distribtion. The Canadian Jornal of Statistics, 1(1), [3] Dallas, A. C. (1976). Characterizing the Pareto and power distribtions. Ann. Inst. Statist. Math., 28,

10 [4] Dixit, U. J. (1987). Characterization of the gamma distribtion in the presence of k otliers. Blletin Bombay Mathematical Colloqim, 4, [5] Dixit, U. J. (1989). Estimation of parameters of the Gamma Distribtion in the presence of Otliers. Commn. Statist. Theory and Meth., 18, [6] Dixit, U. J. (1994). Bayesian approach to prediction in the presence of otliers for Weibll distribtion, Metrika, 41, [7] Dixit, U. J. and Jabbari Nooghabi, M. (2011). Efficient estimation in the Pareto distribtion with the presence of otliers, Statistical Methodology, 8(4), [8] Dixit, U. J. and Jabbari Nooghabi, M. (2011). Efficient Estimation of the parameters of the Pareto Distribtion in the Presence of Otliers, Commnications of the Korean Statistical Society, 18(6), [9] Kczma M. (2008). An Introdction to the Theory of Fnctional Eqations and Ineqalities. Second edition, edited by Attila Gilányi, Birkhäser Verlag AG, Berlin. [10] Sinha, S. K. (1973). Distribtions of order statistics and estimation of mean life when an otlier may be present. The Canadian Jornal of Statistics, 1(1),

Characterizations of probability distributions via bivariate regression of record values

Characterizations of probability distributions via bivariate regression of record values Metrika (2008) 68:51 64 DOI 10.1007/s00184-007-0142-7 Characterizations of probability distribtions via bivariate regression of record vales George P. Yanev M. Ahsanllah M. I. Beg Received: 4 October 2006

More information

CHARACTERIZATIONS OF EXPONENTIAL DISTRIBUTION VIA CONDITIONAL EXPECTATIONS OF RECORD VALUES. George P. Yanev

CHARACTERIZATIONS OF EXPONENTIAL DISTRIBUTION VIA CONDITIONAL EXPECTATIONS OF RECORD VALUES. George P. Yanev Pliska Std. Math. Blgar. 2 (211), 233 242 STUDIA MATHEMATICA BULGARICA CHARACTERIZATIONS OF EXPONENTIAL DISTRIBUTION VIA CONDITIONAL EXPECTATIONS OF RECORD VALUES George P. Yanev We prove that the exponential

More information

Remarks on strongly convex stochastic processes

Remarks on strongly convex stochastic processes Aeqat. Math. 86 (01), 91 98 c The Athor(s) 01. This article is pblished with open access at Springerlink.com 0001-9054/1/010091-8 pblished online November 7, 01 DOI 10.1007/s00010-01-016-9 Aeqationes Mathematicae

More information

Essentials of optimal control theory in ECON 4140

Essentials of optimal control theory in ECON 4140 Essentials of optimal control theory in ECON 4140 Things yo need to know (and a detail yo need not care abot). A few words abot dynamic optimization in general. Dynamic optimization can be thoght of as

More information

MATH2715: Statistical Methods

MATH2715: Statistical Methods MATH275: Statistical Methods Exercises VI (based on lectre, work week 7, hand in lectre Mon 4 Nov) ALL qestions cont towards the continos assessment for this modle. Q. The random variable X has a discrete

More information

QUANTILE ESTIMATION IN SUCCESSIVE SAMPLING

QUANTILE ESTIMATION IN SUCCESSIVE SAMPLING Jornal of the Korean Statistical Society 2007, 36: 4, pp 543 556 QUANTILE ESTIMATION IN SUCCESSIVE SAMPLING Hosila P. Singh 1, Ritesh Tailor 2, Sarjinder Singh 3 and Jong-Min Kim 4 Abstract In sccessive

More information

RELIABILITY ASPECTS OF PROPORTIONAL MEAN RESIDUAL LIFE MODEL USING QUANTILE FUNC- TIONS

RELIABILITY ASPECTS OF PROPORTIONAL MEAN RESIDUAL LIFE MODEL USING QUANTILE FUNC- TIONS RELIABILITY ASPECTS OF PROPORTIONAL MEAN RESIDUAL LIFE MODEL USING QUANTILE FUNC- TIONS Athors: N.UNNIKRISHNAN NAIR Department of Statistics, Cochin University of Science Technology, Cochin, Kerala, INDIA

More information

Moment Generating Functions of Exponential-Truncated Negative Binomial Distribution based on Ordered Random Variables

Moment Generating Functions of Exponential-Truncated Negative Binomial Distribution based on Ordered Random Variables J. Stat. Appl. Pro. 3, No. 3, 413-423 2015 413 Jornal of Statistics Applications & Probability An International Jornal http://d.doi.org/10.12785/jsap/030312 oment Generating Fnctions of Eponential-Trncated

More information

The Replenishment Policy for an Inventory System with a Fixed Ordering Cost and a Proportional Penalty Cost under Poisson Arrival Demands

The Replenishment Policy for an Inventory System with a Fixed Ordering Cost and a Proportional Penalty Cost under Poisson Arrival Demands Scientiae Mathematicae Japonicae Online, e-211, 161 167 161 The Replenishment Policy for an Inventory System with a Fixed Ordering Cost and a Proportional Penalty Cost nder Poisson Arrival Demands Hitoshi

More information

Admissibility under the LINEX loss function in non-regular case. Hidekazu Tanaka. Received November 5, 2009; revised September 2, 2010

Admissibility under the LINEX loss function in non-regular case. Hidekazu Tanaka. Received November 5, 2009; revised September 2, 2010 Scientiae Mathematicae Japonicae Online, e-2012, 427 434 427 Admissibility nder the LINEX loss fnction in non-reglar case Hidekaz Tanaka Received November 5, 2009; revised September 2, 2010 Abstract. In

More information

ON OPTIMALITY CONDITIONS FOR ABSTRACT CONVEX VECTOR OPTIMIZATION PROBLEMS

ON OPTIMALITY CONDITIONS FOR ABSTRACT CONVEX VECTOR OPTIMIZATION PROBLEMS J. Korean Math. Soc. 44 2007), No. 4, pp. 971 985 ON OPTIMALITY CONDITIONS FOR ABSTRACT CONVEX VECTOR OPTIMIZATION PROBLEMS Ge Myng Lee and Kwang Baik Lee Reprinted from the Jornal of the Korean Mathematical

More information

Research Article Uniqueness of Solutions to a Nonlinear Elliptic Hessian Equation

Research Article Uniqueness of Solutions to a Nonlinear Elliptic Hessian Equation Applied Mathematics Volme 2016, Article ID 4649150, 5 pages http://dx.doi.org/10.1155/2016/4649150 Research Article Uniqeness of Soltions to a Nonlinear Elliptic Hessian Eqation Siyan Li School of Mathematics

More information

Approximate Solution of Convection- Diffusion Equation by the Homotopy Perturbation Method

Approximate Solution of Convection- Diffusion Equation by the Homotopy Perturbation Method Gen. Math. Notes, Vol. 1, No., December 1, pp. 18-114 ISSN 19-7184; Copyright ICSRS Pblication, 1 www.i-csrs.org Available free online at http://www.geman.in Approximate Soltion of Convection- Diffsion

More information

A new integral transform on time scales and its applications

A new integral transform on time scales and its applications Agwa et al. Advances in Difference Eqations 202, 202:60 http://www.advancesindifferenceeqations.com/content/202//60 RESEARCH Open Access A new integral transform on time scales and its applications Hassan

More information

Research Article Permanence of a Discrete Predator-Prey Systems with Beddington-DeAngelis Functional Response and Feedback Controls

Research Article Permanence of a Discrete Predator-Prey Systems with Beddington-DeAngelis Functional Response and Feedback Controls Hindawi Pblishing Corporation Discrete Dynamics in Natre and Society Volme 2008 Article ID 149267 8 pages doi:101155/2008/149267 Research Article Permanence of a Discrete Predator-Prey Systems with Beddington-DeAngelis

More information

An Isomorphism Theorem for Bornological Groups

An Isomorphism Theorem for Bornological Groups International Mathematical Form, Vol. 12, 2017, no. 6, 271-275 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/imf.2017.612175 An Isomorphism Theorem for Bornological rops Dinamérico P. Pombo Jr.

More information

Math 263 Assignment #3 Solutions. 1. A function z = f(x, y) is called harmonic if it satisfies Laplace s equation:

Math 263 Assignment #3 Solutions. 1. A function z = f(x, y) is called harmonic if it satisfies Laplace s equation: Math 263 Assignment #3 Soltions 1. A fnction z f(x, ) is called harmonic if it satisfies Laplace s eqation: 2 + 2 z 2 0 Determine whether or not the following are harmonic. (a) z x 2 + 2. We se the one-variable

More information

On Multiobjective Duality For Variational Problems

On Multiobjective Duality For Variational Problems The Open Operational Research Jornal, 202, 6, -8 On Mltiobjective Dality For Variational Problems. Hsain *,, Bilal Ahmad 2 and Z. Jabeen 3 Open Access Department of Mathematics, Jaypee University of Engineering

More information

Approximate Solution for the System of Non-linear Volterra Integral Equations of the Second Kind by using Block-by-block Method

Approximate Solution for the System of Non-linear Volterra Integral Equations of the Second Kind by using Block-by-block Method Astralian Jornal of Basic and Applied Sciences, (1): 114-14, 008 ISSN 1991-8178 Approximate Soltion for the System of Non-linear Volterra Integral Eqations of the Second Kind by sing Block-by-block Method

More information

THE HOHENBERG-KOHN THEOREM FOR MARKOV SEMIGROUPS

THE HOHENBERG-KOHN THEOREM FOR MARKOV SEMIGROUPS THE HOHENBERG-KOHN THEOREM FOR MARKOV SEMIGROUPS OMAR HIJAB Abstract. At the basis of mch of comptational chemistry is density fnctional theory, as initiated by the Hohenberg-Kohn theorem. The theorem

More information

Calculations involving a single random variable (SRV)

Calculations involving a single random variable (SRV) Calclations involving a single random variable (SRV) Example of Bearing Capacity q φ = 0 µ σ c c = 100kN/m = 50kN/m ndrained shear strength parameters What is the relationship between the Factor of Safety

More information

General solution and Ulam-Hyers Stability of Duodeviginti Functional Equations in Multi-Banach Spaces

General solution and Ulam-Hyers Stability of Duodeviginti Functional Equations in Multi-Banach Spaces Global Jornal of Pre and Applied Mathematics. ISSN 0973-768 Volme 3, Nmber 7 (07), pp. 3049-3065 Research India Pblications http://www.ripblication.com General soltion and Ulam-Hyers Stability of Dodeviginti

More information

Graphs and Networks Lecture 5. PageRank. Lecturer: Daniel A. Spielman September 20, 2007

Graphs and Networks Lecture 5. PageRank. Lecturer: Daniel A. Spielman September 20, 2007 Graphs and Networks Lectre 5 PageRank Lectrer: Daniel A. Spielman September 20, 2007 5.1 Intro to PageRank PageRank, the algorithm reportedly sed by Google, assigns a nmerical rank to eery web page. More

More information

Bayes and Naïve Bayes Classifiers CS434

Bayes and Naïve Bayes Classifiers CS434 Bayes and Naïve Bayes Classifiers CS434 In this lectre 1. Review some basic probability concepts 2. Introdce a sefl probabilistic rle - Bayes rle 3. Introdce the learning algorithm based on Bayes rle (ths

More information

Lecture 8: September 26

Lecture 8: September 26 10-704: Information Processing and Learning Fall 2016 Lectrer: Aarti Singh Lectre 8: September 26 Note: These notes are based on scribed notes from Spring15 offering of this corse. LaTeX template cortesy

More information

Conditions for Approaching the Origin without Intersecting the x-axis in the Liénard Plane

Conditions for Approaching the Origin without Intersecting the x-axis in the Liénard Plane Filomat 3:2 (27), 376 377 https://doi.org/.2298/fil7276a Pblished by Faclty of Sciences and Mathematics, University of Niš, Serbia Available at: http://www.pmf.ni.ac.rs/filomat Conditions for Approaching

More information

MATH2715: Statistical Methods

MATH2715: Statistical Methods MATH275: Statistical Methods Exercises III (based on lectres 5-6, work week 4, hand in lectre Mon 23 Oct) ALL qestions cont towards the continos assessment for this modle. Q. If X has a niform distribtion

More information

STEP Support Programme. STEP III Hyperbolic Functions: Solutions

STEP Support Programme. STEP III Hyperbolic Functions: Solutions STEP Spport Programme STEP III Hyperbolic Fnctions: Soltions Start by sing the sbstittion t cosh x. This gives: sinh x cosh a cosh x cosh a sinh x t sinh x dt t dt t + ln t ln t + ln cosh a ln ln cosh

More information

Asymptotics of dissipative nonlinear evolution equations with ellipticity: different end states

Asymptotics of dissipative nonlinear evolution equations with ellipticity: different end states J. Math. Anal. Appl. 33 5) 5 35 www.elsevier.com/locate/jmaa Asymptotics of dissipative nonlinear evoltion eqations with ellipticity: different end states enjn Dan, Changjiang Zh Laboratory of Nonlinear

More information

Sufficient Optimality Condition for a Risk-Sensitive Control Problem for Backward Stochastic Differential Equations and an Application

Sufficient Optimality Condition for a Risk-Sensitive Control Problem for Backward Stochastic Differential Equations and an Application Jornal of Nmerical Mathematics and Stochastics, 9(1) : 48-6, 17 http://www.jnmas.org/jnmas9-4.pdf JNM@S Eclidean Press, LLC Online: ISSN 151-3 Sfficient Optimality Condition for a Risk-Sensitive Control

More information

An Introduction to Geostatistics

An Introduction to Geostatistics An Introdction to Geostatistics András Bárdossy Universität Stttgart Institt für Wasser- nd Umweltsystemmodellierng Lehrsthl für Hydrologie nd Geohydrologie Prof. Dr. rer. nat. Dr.-Ing. András Bárdossy

More information

We automate the bivariate change-of-variables technique for bivariate continuous random variables with

We automate the bivariate change-of-variables technique for bivariate continuous random variables with INFORMS Jornal on Compting Vol. 4, No., Winter 0, pp. 9 ISSN 09-9856 (print) ISSN 56-558 (online) http://dx.doi.org/0.87/ijoc.046 0 INFORMS Atomating Biariate Transformations Jeff X. Yang, John H. Drew,

More information

ON THE SHAPES OF BILATERAL GAMMA DENSITIES

ON THE SHAPES OF BILATERAL GAMMA DENSITIES ON THE SHAPES OF BILATERAL GAMMA DENSITIES UWE KÜCHLER, STEFAN TAPPE Abstract. We investigate the for parameter family of bilateral Gamma distribtions. The goal of this paper is to provide a thorogh treatment

More information

FREQUENCY DOMAIN FLUTTER SOLUTION TECHNIQUE USING COMPLEX MU-ANALYSIS

FREQUENCY DOMAIN FLUTTER SOLUTION TECHNIQUE USING COMPLEX MU-ANALYSIS 7 TH INTERNATIONAL CONGRESS O THE AERONAUTICAL SCIENCES REQUENCY DOMAIN LUTTER SOLUTION TECHNIQUE USING COMPLEX MU-ANALYSIS Yingsong G, Zhichn Yang Northwestern Polytechnical University, Xi an, P. R. China,

More information

Some extensions of Alon s Nullstellensatz

Some extensions of Alon s Nullstellensatz Some extensions of Alon s Nllstellensatz arxiv:1103.4768v2 [math.co] 15 Ag 2011 Géza Kós Compter and Atomation Research Institte, Hngarian Acad. Sci; Dept. of Analysis, Eötvös Loránd Univ., Bdapest kosgeza@szta.h

More information

UNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL

UNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL 8th International DAAAM Baltic Conference "INDUSTRIAL ENGINEERING - 19-1 April 01, Tallinn, Estonia UNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL Põdra, P. & Laaneots, R. Abstract: Strength analysis is a

More information

A Note on Irreducible Polynomials and Identity Testing

A Note on Irreducible Polynomials and Identity Testing A Note on Irrecible Polynomials an Ientity Testing Chanan Saha Department of Compter Science an Engineering Inian Institte of Technology Kanpr Abstract We show that, given a finite fiel F q an an integer

More information

Linear System Theory (Fall 2011): Homework 1. Solutions

Linear System Theory (Fall 2011): Homework 1. Solutions Linear System Theory (Fall 20): Homework Soltions De Sep. 29, 20 Exercise (C.T. Chen: Ex.3-8). Consider a linear system with inpt and otpt y. Three experiments are performed on this system sing the inpts

More information

Lecture 2: CENTRAL LIMIT THEOREM

Lecture 2: CENTRAL LIMIT THEOREM A Theorist s Toolkit (CMU 8-859T, Fall 3) Lectre : CENTRAL LIMIT THEOREM September th, 3 Lectrer: Ryan O Donnell Scribe: Anonymos SUM OF RANDOM VARIABLES Let X, X, X 3,... be i.i.d. random variables (Here

More information

Math 116 First Midterm October 14, 2009

Math 116 First Midterm October 14, 2009 Math 116 First Midterm October 14, 9 Name: EXAM SOLUTIONS Instrctor: Section: 1. Do not open this exam ntil yo are told to do so.. This exam has 1 pages inclding this cover. There are 9 problems. Note

More information

SUBORDINATION RESULTS FOR A CERTAIN SUBCLASS OF NON-BAZILEVIC ANALYTIC FUNCTIONS DEFINED BY LINEAR OPERATOR

SUBORDINATION RESULTS FOR A CERTAIN SUBCLASS OF NON-BAZILEVIC ANALYTIC FUNCTIONS DEFINED BY LINEAR OPERATOR italian jornal of pre and applied mathematics n. 34 215 375 388) 375 SUBORDINATION RESULTS FOR A CERTAIN SUBCLASS OF NON-BAZILEVIC ANALYTIC FUNCTIONS DEFINED BY LINEAR OPERATOR Adnan G. Alamosh Maslina

More information

L 1 -smoothing for the Ornstein-Uhlenbeck semigroup

L 1 -smoothing for the Ornstein-Uhlenbeck semigroup L -smoothing for the Ornstein-Uhlenbeck semigrop K. Ball, F. Barthe, W. Bednorz, K. Oleszkiewicz and P. Wolff September, 00 Abstract Given a probability density, we estimate the rate of decay of the measre

More information

Optimal Control of a Heterogeneous Two Server System with Consideration for Power and Performance

Optimal Control of a Heterogeneous Two Server System with Consideration for Power and Performance Optimal Control of a Heterogeneos Two Server System with Consideration for Power and Performance by Jiazheng Li A thesis presented to the University of Waterloo in flfilment of the thesis reqirement for

More information

The Cryptanalysis of a New Public-Key Cryptosystem based on Modular Knapsacks

The Cryptanalysis of a New Public-Key Cryptosystem based on Modular Knapsacks The Cryptanalysis of a New Pblic-Key Cryptosystem based on Modlar Knapsacks Yeow Meng Chee Antoine Jox National Compter Systems DMI-GRECC Center for Information Technology 45 re d Ulm 73 Science Park Drive,

More information

Formulas for stopped diffusion processes with stopping times based on drawdowns and drawups

Formulas for stopped diffusion processes with stopping times based on drawdowns and drawups Stochastic Processes and their Applications 119 (009) 563 578 www.elsevier.com/locate/spa Formlas for stopped diffsion processes with stopping times based on drawdowns and drawps Libor Pospisil, Jan Vecer,

More information

BLOOM S TAXONOMY. Following Bloom s Taxonomy to Assess Students

BLOOM S TAXONOMY. Following Bloom s Taxonomy to Assess Students BLOOM S TAXONOMY Topic Following Bloom s Taonomy to Assess Stdents Smmary A handot for stdents to eplain Bloom s taonomy that is sed for item writing and test constrction to test stdents to see if they

More information

i=1 y i 1fd i = dg= P N i=1 1fd i = dg.

i=1 y i 1fd i = dg= P N i=1 1fd i = dg. ECOOMETRICS II (ECO 240S) University of Toronto. Department of Economics. Winter 208 Instrctor: Victor Agirregabiria SOLUTIO TO FIAL EXAM Tesday, April 0, 208. From 9:00am-2:00pm (3 hors) ISTRUCTIOS: -

More information

Discussion Papers Department of Economics University of Copenhagen

Discussion Papers Department of Economics University of Copenhagen Discssion Papers Department of Economics University of Copenhagen No. 10-06 Discssion of The Forward Search: Theory and Data Analysis, by Anthony C. Atkinson, Marco Riani, and Andrea Ceroli Søren Johansen,

More information

Optimal control of a stochastic network driven by a fractional Brownian motion input

Optimal control of a stochastic network driven by a fractional Brownian motion input Optimal control of a stochastic network driven by a fractional Brownian motion inpt arxiv:88.299v [math.pr] 8 Ag 28 Arka P. Ghosh Alexander Roitershtein Ananda Weerasinghe Iowa State University Agst 5,

More information

Subcritical bifurcation to innitely many rotating waves. Arnd Scheel. Freie Universitat Berlin. Arnimallee Berlin, Germany

Subcritical bifurcation to innitely many rotating waves. Arnd Scheel. Freie Universitat Berlin. Arnimallee Berlin, Germany Sbcritical bifrcation to innitely many rotating waves Arnd Scheel Institt fr Mathematik I Freie Universitat Berlin Arnimallee 2-6 14195 Berlin, Germany 1 Abstract We consider the eqation 00 + 1 r 0 k2

More information

A Characterization of Interventional Distributions in Semi-Markovian Causal Models

A Characterization of Interventional Distributions in Semi-Markovian Causal Models A Characterization of Interventional Distribtions in Semi-Markovian Casal Models Jin Tian and Changsng Kang Department of Compter Science Iowa State University Ames, IA 50011 {jtian, cskang}@cs.iastate.ed

More information

Integration of Basic Functions. Session 7 : 9/23 1

Integration of Basic Functions. Session 7 : 9/23 1 Integration o Basic Fnctions Session 7 : 9/3 Antiderivation Integration Deinition: Taking the antiderivative, or integral, o some nction F(), reslts in the nction () i ()F() Pt simply: i yo take the integral

More information

FUZZY BOUNDARY ELEMENT METHODS: A NEW MULTI-SCALE PERTURBATION APPROACH FOR SYSTEMS WITH FUZZY PARAMETERS

FUZZY BOUNDARY ELEMENT METHODS: A NEW MULTI-SCALE PERTURBATION APPROACH FOR SYSTEMS WITH FUZZY PARAMETERS MODELOWANIE INŻYNIERSKIE ISNN 896-77X 3, s. 433-438, Gliwice 6 FUZZY BOUNDARY ELEMENT METHODS: A NEW MULTI-SCALE PERTURBATION APPROACH FOR SYSTEMS WITH FUZZY PARAMETERS JERZY SKRZYPCZYK HALINA WITEK Zakład

More information

Lecture: Corporate Income Tax - Unlevered firms

Lecture: Corporate Income Tax - Unlevered firms Lectre: Corporate Income Tax - Unlevered firms Ltz Krschwitz & Andreas Löffler Disconted Cash Flow, Section 2.1, Otline 2.1 Unlevered firms Similar companies Notation 2.1.1 Valation eqation 2.1.2 Weak

More information

Tamsui Oxford Journal of Information and Mathematical Sciences 29(2) (2013) Aletheia University

Tamsui Oxford Journal of Information and Mathematical Sciences 29(2) (2013) Aletheia University Tamsui Oxford Journal of Information and Mathematical Sciences 292 2013 219-238 Aletheia University Relations for Marginal and Joint Moment Generating Functions of Extended Type I Generalized Logistic

More information

Uttam Ghosh (1), Srijan Sengupta (2a), Susmita Sarkar (2b), Shantanu Das (3)

Uttam Ghosh (1), Srijan Sengupta (2a), Susmita Sarkar (2b), Shantanu Das (3) Analytical soltion with tanh-method and fractional sb-eqation method for non-linear partial differential eqations and corresponding fractional differential eqation composed with Jmarie fractional derivative

More information

FINITE TRAVELING WAVE SOLUTIONS IN A DEGENERATE CROSS-DIFFUSION MODEL FOR BACTERIAL COLONY. Peng Feng. ZhengFang Zhou. (Communicated by Congming Li)

FINITE TRAVELING WAVE SOLUTIONS IN A DEGENERATE CROSS-DIFFUSION MODEL FOR BACTERIAL COLONY. Peng Feng. ZhengFang Zhou. (Communicated by Congming Li) COMMUNICATIONS ON Website: http://aimsciences.org PURE AND APPLIED ANALYSIS Volme 6, Nmber 4, December 27 pp. 45 65 FINITE TRAVELING WAVE SOLUTIONS IN A DEGENERATE CROSS-DIFFUSION MODEL FOR BACTERIAL COLONY

More information

Stability of Model Predictive Control using Markov Chain Monte Carlo Optimisation

Stability of Model Predictive Control using Markov Chain Monte Carlo Optimisation Stability of Model Predictive Control sing Markov Chain Monte Carlo Optimisation Elilini Siva, Pal Golart, Jan Maciejowski and Nikolas Kantas Abstract We apply stochastic Lyapnov theory to perform stability

More information

A Survey of the Implementation of Numerical Schemes for Linear Advection Equation

A Survey of the Implementation of Numerical Schemes for Linear Advection Equation Advances in Pre Mathematics, 4, 4, 467-479 Pblished Online Agst 4 in SciRes. http://www.scirp.org/jornal/apm http://dx.doi.org/.436/apm.4.485 A Srvey of the Implementation of Nmerical Schemes for Linear

More information

Fixed points for discrete logarithms

Fixed points for discrete logarithms Fixed points for discrete logarithms Mariana Levin 1, Carl Pomerance 2, and and K. Sondararajan 3 1 Gradate Grop in Science and Mathematics Edcation University of California Berkeley, CA 94720, USA levin@berkeley.ed

More information

ON THE CHARACTERIZATION OF GENERALIZED DHOMBRES EQUATIONS HAVING NON CONSTANT LOCAL ANALYTIC OR FORMAL SOLUTIONS

ON THE CHARACTERIZATION OF GENERALIZED DHOMBRES EQUATIONS HAVING NON CONSTANT LOCAL ANALYTIC OR FORMAL SOLUTIONS Annales Univ. Sci. Bdapest., Sect. Comp. 4 203 28 294 ON THE CHARACTERIZATION OF GENERALIZED DHOMBRES EQUATIONS HAVING NON CONSTANT LOCAL ANALYTIC OR FORMAL SOLUTIONS Ldwig Reich Graz, Astria Jörg Tomaschek

More information

On averaged expected cost control as reliability for 1D ergodic diffusions

On averaged expected cost control as reliability for 1D ergodic diffusions On averaged expected cost control as reliability for 1D ergodic diffsions S.V. Anlova 5 6, H. Mai 7 8, A.Y. Veretennikov 9 10 Mon Nov 27 10:24:42 2017 Abstract For a Markov model described by a one-dimensional

More information

Discussion of The Forward Search: Theory and Data Analysis by Anthony C. Atkinson, Marco Riani, and Andrea Ceroli

Discussion of The Forward Search: Theory and Data Analysis by Anthony C. Atkinson, Marco Riani, and Andrea Ceroli 1 Introdction Discssion of The Forward Search: Theory and Data Analysis by Anthony C. Atkinson, Marco Riani, and Andrea Ceroli Søren Johansen Department of Economics, University of Copenhagen and CREATES,

More information

Department of Industrial Engineering Statistical Quality Control presented by Dr. Eng. Abed Schokry

Department of Industrial Engineering Statistical Quality Control presented by Dr. Eng. Abed Schokry Department of Indstrial Engineering Statistical Qality Control presented by Dr. Eng. Abed Schokry Department of Indstrial Engineering Statistical Qality Control C and U Chart presented by Dr. Eng. Abed

More information

MAXIMUM AND ANTI-MAXIMUM PRINCIPLES FOR THE P-LAPLACIAN WITH A NONLINEAR BOUNDARY CONDITION. 1. Introduction. ν = λ u p 2 u.

MAXIMUM AND ANTI-MAXIMUM PRINCIPLES FOR THE P-LAPLACIAN WITH A NONLINEAR BOUNDARY CONDITION. 1. Introduction. ν = λ u p 2 u. 2005-Ojda International Conference on Nonlinear Analysis. Electronic Jornal of Differential Eqations, Conference 14, 2006, pp. 95 107. ISSN: 1072-6691. URL: http://ejde.math.txstate.ed or http://ejde.math.nt.ed

More information

Non-coherent Rayleigh fading MIMO channels: Capacity and optimal input

Non-coherent Rayleigh fading MIMO channels: Capacity and optimal input Non-coherent Rayleigh fading MIMO channels: Capacity and optimal inpt Rasika R. Perera, Tony S. Pollock*, and Thshara D. Abhayapala* Department of Information Engineering Research School of Information

More information

Chapter 2 Introduction to the Stiffness (Displacement) Method. The Stiffness (Displacement) Method

Chapter 2 Introduction to the Stiffness (Displacement) Method. The Stiffness (Displacement) Method CIVL 7/87 Chater - The Stiffness Method / Chater Introdction to the Stiffness (Dislacement) Method Learning Objectives To define the stiffness matrix To derive the stiffness matrix for a sring element

More information

Modelling by Differential Equations from Properties of Phenomenon to its Investigation

Modelling by Differential Equations from Properties of Phenomenon to its Investigation Modelling by Differential Eqations from Properties of Phenomenon to its Investigation V. Kleiza and O. Prvinis Kanas University of Technology, Lithania Abstract The Panevezys camps of Kanas University

More information

Generalized Jinc functions and their application to focusing and diffraction of circular apertures

Generalized Jinc functions and their application to focusing and diffraction of circular apertures Qing Cao Vol. 20, No. 4/April 2003/J. Opt. Soc. Am. A 66 Generalized Jinc fnctions and their application to focsing and diffraction of circlar apertres Qing Cao Optische Nachrichtentechnik, FernUniversität

More information

Nonlinear parametric optimization using cylindrical algebraic decomposition

Nonlinear parametric optimization using cylindrical algebraic decomposition Proceedings of the 44th IEEE Conference on Decision and Control, and the Eropean Control Conference 2005 Seville, Spain, December 12-15, 2005 TC08.5 Nonlinear parametric optimization sing cylindrical algebraic

More information

Convergence to diffusion waves for nonlinear evolution equations with different end states

Convergence to diffusion waves for nonlinear evolution equations with different end states J. Math. Anal. Appl. 338 8) 44 63 www.elsevier.com/locate/jmaa Convergence to diffsion waves for nonlinear evoltion eqations with different end states Walter Allegretto, Yanping Lin, Zhiyong Zhang Department

More information

Trace-class Monte Carlo Markov Chains for Bayesian Multivariate Linear Regression with Non-Gaussian Errors

Trace-class Monte Carlo Markov Chains for Bayesian Multivariate Linear Regression with Non-Gaussian Errors Trace-class Monte Carlo Markov Chains for Bayesian Mltivariate Linear Regression with Non-Gassian Errors Qian Qin and James P. Hobert Department of Statistics University of Florida Janary 6 Abstract Let

More information

OPTIMUM EXPRESSION FOR COMPUTATION OF THE GRAVITY FIELD OF A POLYHEDRAL BODY WITH LINEARLY INCREASING DENSITY 1

OPTIMUM EXPRESSION FOR COMPUTATION OF THE GRAVITY FIELD OF A POLYHEDRAL BODY WITH LINEARLY INCREASING DENSITY 1 OPTIMUM EXPRESSION FOR COMPUTATION OF THE GRAVITY FIEL OF A POLYHERAL BOY WITH LINEARLY INCREASING ENSITY 1 V. POHÁNKA2 Abstract The formla for the comptation of the gravity field of a polyhedral body

More information

CHANNEL SELECTION WITH RAYLEIGH FADING: A MULTI-ARMED BANDIT FRAMEWORK. Wassim Jouini and Christophe Moy

CHANNEL SELECTION WITH RAYLEIGH FADING: A MULTI-ARMED BANDIT FRAMEWORK. Wassim Jouini and Christophe Moy CHANNEL SELECTION WITH RAYLEIGH FADING: A MULTI-ARMED BANDIT FRAMEWORK Wassim Joini and Christophe Moy SUPELEC, IETR, SCEE, Avene de la Bolaie, CS 47601, 5576 Cesson Sévigné, France. INSERM U96 - IFR140-

More information

On the Total Duration of Negative Surplus of a Risk Process with Two-step Premium Function

On the Total Duration of Negative Surplus of a Risk Process with Two-step Premium Function Aailable at http://pame/pages/398asp ISSN: 93-9466 Vol, Isse (December 7), pp 7 (Preiosly, Vol, No ) Applications an Applie Mathematics (AAM): An International Jornal Abstract On the Total Dration of Negatie

More information

Uncertainty Evaluation of Toluene Determination in Room Air by Thermal Desorption Gas Chromatography

Uncertainty Evaluation of Toluene Determination in Room Air by Thermal Desorption Gas Chromatography International Conference on Civil, Transportation and Environment (ICCTE 06) ncertainty Evalation of Tolene Determination in Room Air by Thermal Desorption Gas Chromatography Xiaoyan Wen, a,yanhi Gao,

More information

MEAN VALUE ESTIMATES OF z Ω(n) WHEN z 2.

MEAN VALUE ESTIMATES OF z Ω(n) WHEN z 2. MEAN VALUE ESTIMATES OF z Ωn WHEN z 2 KIM, SUNGJIN 1 Introdction Let n i m pei i be the prime factorization of n We denote Ωn by i m e i Then, for any fixed complex nmber z, we obtain a completely mltiplicative

More information

1 The space of linear transformations from R n to R m :

1 The space of linear transformations from R n to R m : Math 540 Spring 20 Notes #4 Higher deriaties, Taylor s theorem The space of linear transformations from R n to R m We hae discssed linear transformations mapping R n to R m We can add sch linear transformations

More information

Lecture 17 Errors in Matlab s Turbulence PSD and Shaping Filter Expressions

Lecture 17 Errors in Matlab s Turbulence PSD and Shaping Filter Expressions Lectre 7 Errors in Matlab s Trblence PSD and Shaping Filter Expressions b Peter J Sherman /7/7 [prepared for AERE 355 class] In this brief note we will show that the trblence power spectral densities (psds)

More information

This Topic follows on from Calculus Topics C1 - C3 to give further rules and applications of differentiation.

This Topic follows on from Calculus Topics C1 - C3 to give further rules and applications of differentiation. CALCULUS C Topic Overview C FURTHER DIFFERENTIATION This Topic follows on from Calcls Topics C - C to give frther rles applications of differentiation. Yo shold be familiar with Logarithms (Algebra Topic

More information

CRITERIA FOR TOEPLITZ OPERATORS ON THE SPHERE. Jingbo Xia

CRITERIA FOR TOEPLITZ OPERATORS ON THE SPHERE. Jingbo Xia CRITERIA FOR TOEPLITZ OPERATORS ON THE SPHERE Jingbo Xia Abstract. Let H 2 (S) be the Hardy space on the nit sphere S in C n. We show that a set of inner fnctions Λ is sfficient for the prpose of determining

More information

Study of the diffusion operator by the SPH method

Study of the diffusion operator by the SPH method IOSR Jornal of Mechanical and Civil Engineering (IOSR-JMCE) e-issn: 2278-684,p-ISSN: 2320-334X, Volme, Isse 5 Ver. I (Sep- Oct. 204), PP 96-0 Stdy of the diffsion operator by the SPH method Abdelabbar.Nait

More information

Analysis of the fractional diffusion equations with fractional derivative of non-singular kernel

Analysis of the fractional diffusion equations with fractional derivative of non-singular kernel Al-Refai and Abdeljawad Advances in Difference Eqations 217 217:315 DOI 1.1186/s13662-17-1356-2 R E S E A R C H Open Access Analysis of the fractional diffsion eqations with fractional derivative of non-singlar

More information

Lecture: Corporate Income Tax

Lecture: Corporate Income Tax Lectre: Corporate Income Tax Ltz Krschwitz & Andreas Löffler Disconted Cash Flow, Section 2.1, Otline 2.1 Unlevered firms Similar companies Notation 2.1.1 Valation eqation 2.1.2 Weak atoregressive cash

More information

The Linear Quadratic Regulator

The Linear Quadratic Regulator 10 The Linear Qadratic Reglator 10.1 Problem formlation This chapter concerns optimal control of dynamical systems. Most of this development concerns linear models with a particlarly simple notion of optimality.

More information

Control Systems Design

Control Systems Design ELEC4410 Control Systems Design Lectre 16: Controllability and Observability Canonical Decompositions Jlio H. Braslavsky jlio@ee.newcastle.ed.a School of Electrical Engineering and Compter Science Lectre

More information

A Note on the Strong Law of Large Numbers

A Note on the Strong Law of Large Numbers JIRSS (2005) Vol. 4, No. 2, pp 107-111 A Note on the Strong Law of Large Numbers V. Fakoor, H. A. Azarnoosh Department of Statistics, School of Mathematical Sciences, Ferdowsi University of Mashhad, Iran.

More information

Using Min-max Method to Solve a Full Fuzzy Linear Programming

Using Min-max Method to Solve a Full Fuzzy Linear Programming Astralian Jornal of Basic and Applied Sciences, 5(7): 44-449, ISSN 99-878 Using Min-max Method to Solve a Fll Fzzy inear Programming. Ezzati, E. Khorram, A. Mottaghi. Enayati Department of Mathematics,

More information

Gravitational Instability of a Nonrotating Galaxy *

Gravitational Instability of a Nonrotating Galaxy * SLAC-PUB-536 October 25 Gravitational Instability of a Nonrotating Galaxy * Alexander W. Chao ;) Stanford Linear Accelerator Center Abstract Gravitational instability of the distribtion of stars in a galaxy

More information

Sensitivity Analysis in Bayesian Networks: From Single to Multiple Parameters

Sensitivity Analysis in Bayesian Networks: From Single to Multiple Parameters Sensitivity Analysis in Bayesian Networks: From Single to Mltiple Parameters Hei Chan and Adnan Darwiche Compter Science Department University of California, Los Angeles Los Angeles, CA 90095 {hei,darwiche}@cs.cla.ed

More information

entropy ISSN by MDPI

entropy ISSN by MDPI Entropy, 007, 9, 113-117 Letter to the Editor entropy ISSN 1099-4300 007 by MDPI www.mdpi.org/entropy Entropy of Relativistic Mono-Atomic Gas and Temperatre Relativistic Transformation in Thermodynamics

More information

Math 273b: Calculus of Variations

Math 273b: Calculus of Variations Math 273b: Calcls of Variations Yacob Kreh Homework #3 [1] Consier the 1D length fnctional minimization problem min F 1 1 L, or min 1 + 2, for twice ifferentiable fnctions : [, 1] R with bonary conitions,

More information

BIOSTATISTICAL METHODS

BIOSTATISTICAL METHODS BIOSTATISTICAL METHOS FOR TRANSLATIONAL & CLINICAL RESEARCH ROC Crve: IAGNOSTIC MEICINE iagnostic tests have been presented as alwas having dichotomos otcomes. In some cases, the reslt of the test ma be

More information

On the Representation theorems of Riesz and Schwartz

On the Representation theorems of Riesz and Schwartz On the Representation theorems of Riesz and Schwartz Yves Hpperts Michel Willem Abstract We give simple proofs of the representation theorems of Riesz and Schwartz. 1 Introdction According to J.D. Gray

More information

POWER GENERALIZED WEIBULL DISTRIBUTION BASED ON GENERALISED ORDER STATISTICS

POWER GENERALIZED WEIBULL DISTRIBUTION BASED ON GENERALISED ORDER STATISTICS Jornal of Data Science 621-646, DOI: 1.6339/JDS.2187_16(3).1 POWER GENERALIZED WEIBULL DISTRIBUTION BASED ON GENERALISED ORDER STATISTICS Devendra Kmar 1 and Neet Jain 2 1 Department of Statistics, Central

More information

Section 7.4: Integration of Rational Functions by Partial Fractions

Section 7.4: Integration of Rational Functions by Partial Fractions Section 7.4: Integration of Rational Fnctions by Partial Fractions This is abot as complicated as it gets. The Method of Partial Fractions Ecept for a few very special cases, crrently we have no way to

More information

RESGen: Renewable Energy Scenario Generation Platform

RESGen: Renewable Energy Scenario Generation Platform 1 RESGen: Renewable Energy Scenario Generation Platform Emil B. Iversen, Pierre Pinson, Senior Member, IEEE, and Igor Ardin Abstract Space-time scenarios of renewable power generation are increasingly

More information

A Computational Study with Finite Element Method and Finite Difference Method for 2D Elliptic Partial Differential Equations

A Computational Study with Finite Element Method and Finite Difference Method for 2D Elliptic Partial Differential Equations Applied Mathematics, 05, 6, 04-4 Pblished Online November 05 in SciRes. http://www.scirp.org/jornal/am http://d.doi.org/0.46/am.05.685 A Comptational Stdy with Finite Element Method and Finite Difference

More information

Reflections on a mismatched transmission line Reflections.doc (4/1/00) Introduction The transmission line equations are given by

Reflections on a mismatched transmission line Reflections.doc (4/1/00) Introduction The transmission line equations are given by Reflections on a mismatched transmission line Reflections.doc (4/1/00) Introdction The transmission line eqations are given by, I z, t V z t l z t I z, t V z, t c z t (1) (2) Where, c is the per-nit-length

More information