Discrete Bernoulli s Formula and its Applications Arising from Generalized Difference Operator
|
|
- Angela Dean
- 5 years ago
- Views:
Transcription
1 Int. Journa of Math. Anaysis, Vo. 7, 2013, no. 5, Discrete Bernoui s Formua and its Appications Arising from Generaized Difference Operator G. Britto Antony Xavier 1 Department of Mathematics, Sacred Heart Coege Tirupattur , Veore District, Tami Nadu, S.India shcbritto@yahoo.co.in H. Nasira Begum Department of Mathematics, Sacred Heart Coege Tirupattur , Veore District, Tami Nadu, S.India Abstract In this paper, the authors derive discrete Bernoui s formua of the form, [u(k)v(k)] = ( 1) t u (t) (k)v t+1 (k + t) t=0 for the rea vaued rea variabe functions u(k) and v(k) using the generaized differences, u (t) (k) =Δ t u(k) and its inverses, v t(k) =Δ t v(k) and obtain severa formuae on finite and infinite series as appication of the discrete Bernoui s formua in number theory. Suitabe exampes are provided to iustrate the main resuts. Mathematics Subject Cassification: 39A70, 47B39, 39A10 Keywords: Generaized difference operator, Discrete Bernoui s Formua, Partia sums 1 Introduction The theory and some appications of the generaized difference operator Δ defined as Δ u(k) =u(k + ) u(k), k [0, ) and (0, ) had been deveoped in [2]. The generaized versions of Leibnitz, Binomia, Montmorte s Theorems, Newton s formua aong with formuae for the sums and partia sums of the n th powers of an arithmetic progression, the sums and partia 1 Research Supported by University Grants Commission, SERO, Hyderabad, India.
2 230 G. Britto Antony Xavier and H. Nasira Begum sums of the products of n consecutive terms of an arithmetic progression and the sums and partia sums of an arithmetic-geometric progression using the generaized difference operators of the first, second and n th kinds and their inverses were obtained in ([2], [7], [8], [9]). Generaized Bernoui poynomias B n (k, ±) with appications using Δ ± and its inverses ([4, 5]), quaitative and rotatory properties of certain cass of generaized difference equations ([3, 6]) are some of the appications of difference equations invoving Δ. In this paper, we derive the discrete version of the Bernoui s formua and some appications in number theory which are not obtained earier. A the resuts are iustrated with suitabe exampes. 2 Preiminaries Before stating and proving our resuts, we present some notations, basic definitions and preiminary resuts which wi be used in the subsequent discussions. Let > 0, k [0, ), j = k [k/], where [k/] denotes the integer part of k/, N (j) ={j, + j, 2 + j, }, N 1 (j) =N(j) and c j is a constant for a k N (j). For m N(1), we denote Δ m u(k) k ( (m 1)+j = 1 ( Δ Δ 1 u(k) k ) j k ) +j k (m 1)+j,Δ 1 u(k) k j = u 1(k) = u(k) ( u(j), Δ 1 u(k) k ) j k +j = u 2(k) = u 1 (k) u 1 ( + j), and so on. Definition 2.1 [2] For a rea vaued function u(k), the generaized difference operator Δ and its inverse are respectivey defined as Δ u(k) =u(k + ) u(k), k [0, ), (0, ), (1) if Δ v(k) =u(k), then v(k) = u(k)+c j. (2) Definition 2.2 [11] For k, n (0, ), the -factoria function is defined by k (n) = n Γ( k +1) (3) +1 n), where Γ is the Euer gamma function and k (n) 1 = k (n). Remark 2.3 When n N(1), (3) and its Δ -difference become Γ( k k (n) n 1 = (k t), and Δ k (n) t=0 =(n)k (n 1). (4) Theorem 2.4 [2] Let u(k), k [0, ) be rea vaued function. Then for k [, ), [k/] u(k) k j = u(k r). (5)
3 Discrete Bernoui s formua 231 Lemma 2.5 [2] For n N(0), and for n N(2), 1 k (n) k j k (n) k j = k(n+1) = 1 (n +1) (n 1)(j ) (n 1) j(n+1) (n +1) 1 (n 1)(k ) (n 1) In particuar, when =1, k =(r 1) N(1), j =0, then (6) becomes (6). (7) k (n) r 1 0 = (r 1)(n+1). (8) (n +1) Lemma 2.6 Let n N(0) and r N(3). Then, k (n) r 1 0 =(r 2) (n) +(r 3) (n) + + (1) (n) = (r 1)(n+1). (9) (n +1) Proof. The proof foows by taking =1,u(k) =k (n) in (5) and (6). Theorem 2.7 Let m N(1), (0, ) and k [m, ). Then, Δ m Proof. Taking ( [k/] u(k) k (m 1)+j = r=m (r 1) (m 1) u(k r). (10) (m 1)! on (5), and appying (5) for u(k r), we get [k/] u(k) k j ) k +j = u(k r) = [k/] [k r/] s=1 u(k r s). From the notation given this section and ordering the terms u(k r), we find Δ 2 [k/] u(k) k +j = (r 1) (1) u(k r). (11) 1! Again, taking on (11), by (5) for u(k r), we arrive Δ 3 [k/] u(k) k 2+j = [ (r 2) (1) 1! which yieds by (9), r=3 + (r 3)(1) 1! + + (1)(1) ] u(k r), 1! Δ 3 [k/] u(k) k 2+j = r=3 (r 1) (2) u(k r). (12) 2! Now, (10) wi be obtained by continuing this process and using (9).
4 232 G. Britto Antony Xavier and H. Nasira Begum Theorem 2.8 Let k [0, ) and im k u(k) =0. Then, u(k) k = u(k + r). (13) Proof. From (5), and expressing its terms in reverse order, we find r=0 u(k) k j +Δ 1 u(k) k = u(j)+u(+j)+ +u(k )+u(k)+u(k+)+ +u( ) which is same as u(k) j = u(j + r). (14) r=0 Now, (13) foows by given condition u( ) = 0 and then repacing j by k. Lemma 2.9 [2] Let Sr n s are the stiring numbers of the second kind. Then n k n = Sr n n r k (r). (15) Lemma 2.10 Let u(k) and v(k) be two rea vaued functions. Then [u(k)v(k)] = u(k) Proof. From (1), we find v(k) [ v(k + )Δ u(k)]. (16) Δ [u(k)w(k)] = w(k + )Δ u(k)+u(k)δ w(k). (17) Appying (4) in (17), we obtain [u(k)δ w(k)] = u(k)w(k) [w(k + )Δ u(k)]. (18) The proof foows from the reation v(k) =Δ w(k) and (18). 3 Main Resuts and Appications In this section, we present the discrte version of Bernoui s Formua and deveop reative resuts of it in number theory. Theorem 3.1 (Discrete Bernoui s Formua) Let u(k) and v(k) be two rea vaued functions, u (t) (k) =Δ t u(k), v t (k) =Δ t v(k) for t =1, 2, and u (0) (k) =u(k). Then [u(k)v(k)] = ( 1) t u (t) (k)v t+1 (k + t). (19) t=0
5 Discrete Bernoui s formua 233 Proof. Taking v(k) =v 1 (k) and Δ u(k) =u (1) (k) in (16), we have [u(k)v(k)] = u(k)v 1 (k) [v 1 (k + )u (1) (k)] (20) Appying the equation (16) again and again in (20) we get proof. Theorem 3.2 Let m N(1) and t be any integer. Then, [k/] r=m where F (n) m F (n) (r 1) (m 1) (m 1)! 1 (k) = (k) =Δ m [k (n) a tk ]. (k r) (n) Proof. From (16), we find [k (n) a t(k r) = F (n) m (k) F (n) m ((m 1) + j), (21) [ F (n) m 1(k) F (n) m 1((m 2) + j) ], m =2, 3,... and a tk ]=k (n) Appying (10) in (22), we get [k/] (k r) (n) a tk (a t 1) Δ 1 { a t(k+) a t 1 (n)k(n 1) a t(k r) = F (n) 1 (k) F (n) 1 (j), F (n) 1 (k) = }. (22) [k (n) a tk ]. Again operating on both sides and appying (10), we obtain [k/] where F (n) 2 (k) = (r 1)(k r) (n) F (n) a t(k r) = F (n) 2 (k) F (n) 2 ( + j), 1 (k). By continuing this process, we get the proof. Coroary 3.3 Let k [2, ), a 1and j = k [k/]. Then, [k/] where F (n) 2 (k) = (r 1)(k r) (n) n r=0 ( ) r n (r) r!(a 1) a k r = F (n) 2 (k) F (n) 2 ( + j), (23) (r + 1)!k (n r) a k+r r!j(n r) (a 1) r+1 Proof. The proof foows by taking m = 2 and t = 1 in (21). Exampe 3.4 Putting n =3in (23), we obtain [k/] (r 1)(k r) (3) a k r = F (3) 2 (k) F (3) a j+r k (1) (a 1) r. 2 ( + j), (24)
6 234 G. Britto Antony Xavier and H. Nasira Begum where F (3) 2 (k) = k(3) a k (a 1) 2 6k(2) a k+ (a 1) k (1) a k+2 (a 1) a k+3 (a 1) 5 (j) (3) a j (a 1) 3(j)(2) a +j (a 1) (j) (1) a 2+j 63 a 3+j k (1) (a 1) 3 (a 1) 4. In particuar, when k =16.4,=2.4,a=2and j =2in (24), we get [ 16.4] 2.4 (r 1)( r) (3) r = F (3) 2 (16.4) F (3) 2 (4.4) = Coroary 3.5 If a 1, then [k/] here F (n) 2 (k) = (r 1)(k r) (n) n r=0 ( ) r n (r) r!(a 1) a (k r) = F (n) 2 (k) F (n) 2 ( + j), (25) (r + 1)!k (n r) a (k+r) r!j(n r) (a 1) r+1 a (j+r) k (1) (a 1) r. Proof. The proof foows by taking m = 2 and t = 1 in (21). Exampe 3.6 Taking n =2in (25), we get [k/] (r 1)(k r) (2) a (k r) = F (2) 2 (k) F (2) a k a (k+) 2 ( + j), (26) where F (2) 2 (k) = k(2) (a 1) 4k(1) + 62 a (k+2) 2 (a 1) 3 (a 1) 4 (j) (2) a j (a 1) 2(j)(1) a (j+) + 22 a (j+2) k (1) (a 1) 2 (a 1) 3. In particuar, when k =28.9,=10.9,a=2and j =7.1 in (26), we obtain [ 28.9] 10.9 (r 1)( r) (2) ( r) = F (2) 2 (28.9) F (2) 2 (18) = Coroary 3.7 Let p, q N(1), q p +2 and k (q) [k/] (k +(s r))(p) = F (k r) (q) 1 (k) F 1 (j), F 1 (k) = 0. Then, (k + s)(p) k (q) (27) Proof. The vaue of F 1 (k) can be obtained by substituting u(k) =(k + s) (p) and v(k) = 1 in (16) and using (6), (7). The proof foows by (10). k (q)
7 Discrete Bernoui s formua 235 Exampe 3.8 Taking p =2, q =4in (27), and by (6), (7),(16), we get [k/] (k +(s r))(2) = F (k r) (4) 1 (k) F 1 (j), (28) (k + s)(2) (k + s)(1) 1 where F 1 (k) =. 3(k ) (3) 3(k ) (2) 3(k ) (1) In particuar, when k =60.5,=20.5,s=2and j =19.5 in (28), we have [ 60.5] 20.5 (60.5+(2 r)20.5)(2) 20.5 = F ( r) (4) 1 (60.5) F 1 (19.5) = Theorem 3.9 If q p +3, then [k/] (k +(s r))(p) (r 1) = F (k r) (q) 2 (k) F 2 ( + j), (29) where F 2 (k) = [F 1 (k) F 1 (j)] and F 1 (k) = (k + s)(p). k (q) Proof. Cosed form expression of F 1 (k) and hence F 2 (k) can be obtained by taking u(k) =(k + s) (p) and v(k) = 1 in (16) and using (6) and (7). The k (q) proof foows from (10). Exampe 3.10 In (29), by taking p =3and q =6, we have [k/] (k +(s r))(3) (r 1) = F (k r) (6) 2 (k) F 2 ( + j), (30) (k + s)(3) (k + s)(2) 3(k + s)(1) 1 F 2 (k) = (k 2) (4) 10 2 (k 2) (3) 20 2 (k 2) (2) 5 2 (k 2) (1) (j + s) (3) 3(j + s)(2) (j + s)(1) 1 k (1) (j ) (5) 20(j ) (4) 10(j ) (3) 20(j ) (2). 2 In particuar, when k =9,=2,s=2and j =1in (30), we obtain [ 9] 2 (9 + (2 r)2)(3) (r 1) 2 = F (9 2r) (6) 2 (9) F 2 (3) = Coroary 3.11 If q p +2, then (k +(s 1) + r)(p) = (k + s)(p) (k +(r 1)) (q) (31) k (q) k
8 236 G. Britto Antony Xavier and H. Nasira Begum Proof. The proof foows by (13) and the cosed form expression of F 1 (k) can be obtained from (16). Exampe 3.12 Substituting p =2and q =4in (31), we obtain (k +(s 1) + r) (2) (k +(r 1)) (4) = (k + s)(2) + 3(k ) (3) (k + s)(1) + 3(k ) (2) In particuar, when k =11, =2, s =3in (32), we get (11 + (3 1)2 + 2r)(2) 2 = (11 + 2(r 1)) (4) 2 1 3(k ) (1). (32) Coroary 3.13 Let p, q N(1), q p +3. Then, (k +(s 2) + r)(p) (r 1) = F (k +(r 2)) (q) 2 (k), (33) where F 2 (k) = F 1 (k) and F 1 (k) = u(k). Proof. The proof foows by (13) and the cosed form expression of F 1 (k) and hence F 2 (k) can be obtained by taking u(k) =(k + s) (p), v(k) = 1 in (16) k (q) and using (6) and (7). Exampe 3.14 Put p =3and q =6in (33), we get (k +(s 2) + r)(3) (r 1) = F (k +(r 2)) (6) 2 (k), (34) (k + s)(3) (k + s)(2) 3(k + s)(1) F 2 (k) = (k 2) (4) 10 2 (k 2) (3) 20 2 (k 2) (2) (j + s) (3) 3(j + s)(2) (j + s)(1) 1 k (1) (j ) (5) 20(j ) (4) 10(j ) (3) 20(j ) (2). 2 In particuar, when k =5, =2, s =2and j =1in (34), we get (r 1) = (5 + (2 2)2 + 2r)(3) 2 (5 + (r 2)2) (6) 2 Theorem 3.15 Let (0, ), a 1, t =1and k>. Then, [k/] where F n 1 (k) = (k n a k ) (k 2) (1) (k r) n a k r = F1 n (k) F 1 n (j), (35)
9 Discrete Bernoui s formua 237 Proof. From (15), we have where (k n a k )= n Sr n n r [k (r) a k ], (36) [k (r) a k ] wi be obtained from (22), by taking n = r and t = 1. The proof foows from (10). The foowing coroary iustrates Theorem 3.15, when n = 3. Coroary 3.16 Let k [, ), (0, ) and a 1. Then, F 3 1 (k) = [k/] (k r) 3 a k r = F 3 1 (k) F 3 1 (j), (37) a k [ (3) k (a +3k (2) + 2 k (1) ] a k+ [ 3 +3k (2) 1) (a 1) k (1) ] + 62 a k+2 [ ] (1) 6 3 a k+3 + k (a 1) 3 (a 1). (38) 4 Exampe 3.17 In (37), by taking k =35.5, =20.5, a =2and j =15, we obtain [ 35.5] 20.5 ( r) r = F2 3 (35.5) F 2 3 (15) = , where F2 3 (35.5) is obtained by substituting k =35.5 in (38). Theorem 3.18 Let k [2, ), (0, ) and a 1. Then, where F n 2 [k/] (k) =Δ 1 (r 1)(k r) n a k r = F2 n (k) F 2 n ( + j), (39) [F n 1 (k) F n 1 (j)] and F n 1 (k) =Δ 1 (k n a k ). Proof. The proof foows from (4), (10) and (37). The foowing coroary iustrates Theorem 3.18, when n = 3. Coroary 3.19 If k [2, ) and a 1, then [k/] (r 1)(k r) 3 a k r = F2 3 (k) F 2 3 ( + j), (40)
10 238 G. Britto Antony Xavier and H. Nasira Begum where F 3 2 (k) = k(1) a j a k (a 1) 2 [k(3) +3k (2) + 2 k (1) ] 2ak+ (a 1) 3 [2 +3k (2) +6k (1) ] (a 1) [(j)(3) +3(j) (2) + 2 (j) (1) ]+ k(1) a +j (a 1) 2 [2 +3(j) (2) +6(j) (1) ] (41) a k+2 [ + (a k(1) 1) 4 ] 6k(1) a 2+j [ (a +(j)(1) 1) 3 ]+ 62 k (1) a 3+j 243 a k+3 (a 1) 4 (a 1) 5 and F2 3 (k) is given in (38). Exampe 3.20 Putting k =9, =2, a =2and j =1in (40), we get [ 9] 2 (r 1)(9 2r) r = F2 3 (9) F 2 3 (3) = Theorem 3.21 If is a positive rea number, a 1, t = 1 and k>, then [k/] (k r) n a (k r) = F1 n (k) F 1 n (j), (42) where Proof. From (15), we have F n 1 (k n a k )= (k) =Δ 1 (k n a k ). (43) n Sr n n r [k (r) a k ]. (44) The proof foows from (10), (16) and (44). The foowing coroary iustrates Theorem 3.21, when n = 3. Coroary 3.22 If k [, ), (0, ) and a 1, then F 3 1 (k) = [k/] (k r) 3 a (k r) = F1 3 (k) F 1 3 (j), (45) a k [ (3) k (a +3k (2) + 2 k (1) ] a (k+) [ 3 +3k (2) 1) (a 1) k (1) ] + 62 a (k+2) [ ] (1) 6 3 a (k+3) + k (a 1) 3 (a 1). (46) 4 Exampe 3.23 In (45), by substituting k =62.1, =12.1, a =2and j =1.6, we obtain [ 62.1] 12.1 ( r) r = F1 3 (62.1) F 1 3 (1.6) = where F1 3 (62.1) is obtained by putting k =62.1.
11 Discrete Bernoui s formua 239 Theorem 3.24 If k [2, ), t = 1 and a 1, then where F n 2 [k/] (r 1)(k r) n a (k r) = F n 2 (k) F n 2 ( + j), (47) (k) =Δ 1 F1 n(k) and F 1 n (k) is given in (43). Proof. The proof foows from (10) and (42). Coroary 3.25 If k [2, ) and a 1, then [k/] (r 1)(k r) 3 a (k r) = F2 3 (k) F 2 3 ( + j), (48) F2 3 (k) = [k(3) +3k (2) + 2 k (1) ] 2[2 +3k (2) a k (a 1) 2 a (k+) (a 1) 3 +6k (1) ] k(1) [(j) (3) +3(j) (2) + 2 (j) (1) ] + k(1) [ 2 +3(j) (2) +6(j) (1) ] (49) a j (a 1) a (+j) (a 1) [ + k (1) ] a (k+2) (a 1) 6k(1) [ +(j) (1) ] 4 a (2+j) (a 1) + 62 k (1) a (3+j) 243 a (k+3) 3 (a 1) 4 (a 1) 5 and F1 3 (k) is given in (46). Proof. The proof foows by taking n = 3 in (47). Exampe 3.26 Putting k =9, =2, a =2and j =1in (40), we get 4 (r 1)(9 2r) r = F2 3 (9) F 2 3 (3) = , where F2 3 (9) is obtained by substituting k =9in (49). References [1] R.P Agarwa, Difference Equations and Inequaities, Marce Dekker, New York, [2] M.Maria Susai Manue, G.Britto Antony Xavier and E.Thandapani, Theory of Generaized Difference Operator and Its Appications, Far East Journa of Mathematica Sciences, 20(2) (2006), [3] M.Maria Susai Manue, G.Britto Antony Xavier and E.Thandapani, Quaitative Properties of Soutions of Certain Cass of Difference Equations, Far East Journa of Mathematica Sciences, 23(3) (2006),
12 240 G. Britto Antony Xavier and H. Nasira Begum [4] M.Maria Susai Manue, G.Britto Antony Xavier and E.Thandapani, Generaized Bernoui Poynomias Through Weighted Pochhammer Symbos, Far East Journa of Appied Mathematics, 26(3) (2007), [5] M. Maria Susai Manue, A. George Maria Sevam and G. Britto Antony Xavier, On the soutions and appications of some cass of generaized difference equations, Far East Journa of Appied Mathematics 28(2)(2007), [6] M.Maria Susai Manue and G.Britto Antony Xavier, Recessive, Dominant and Spira Behaviours of Soutions of Certain Cass of Generaized Difference Equations, Internationa Journa of Differentia Equations and Appications, 10(4) (2007), [7] M.Maria Susai Manue, G.Britto Antony Xavier and V.Chandrasekar, Generaized Difference Operator of the Second Kind and Its Appication to Number Theory, Internationa Journa of Pure and Appied Mathematics, 47(1) (2008), [8] M.Maria Susai Manue, G.Britto Antony Xavier and V.Chandrasekar, Theory and Appication of the Generaized Difference Operator of the n th Kind (Part - I), Demonstratio Mathematica, 45(1) (2012), [9] M.Maria Susai Manue, G.Britto Antony Xavier and V.Chandrasekar, Some Appications of the Generaized Difference Operator of the n th Kind, Far East Journa of Appied Mathematics, 66(2) (2012), [10] Ronad E.Mickens, Difference Equations, Van Nostrand Reinhod Company, New York, [11] Ruta.C.Ferreira and Defim F.M.Jorres,Fractiona h-difference equations arising from the Cacuus of variations, Journa of Appicabe Anaysis and Discrete Mathematics, (2011). Received: September, 2012
Theory of Generalized k-difference Operator and Its Application in Number Theory
Internationa Journa of Mathematica Anaysis Vo. 9, 2015, no. 19, 955-964 HIKARI Ltd, www.m-hiari.com http://dx.doi.org/10.12988/ijma.2015.5389 Theory of Generaized -Difference Operator and Its Appication
More informationLaplace - Fibonacci transform by the solution of second order generalized difference equation
Nonauton. Dyn. Syst. 017; 4: 30 Research Artice Open Access Sandra Pineas*, G.B.A Xavier, S.U. Vasantha Kumar, and M. Meganathan Lapace - Fibonacci transform by the soution of second order generaized difference
More informationSummation of p-adic Functional Series in Integer Points
Fiomat 31:5 (2017), 1339 1347 DOI 10.2298/FIL1705339D Pubished by Facuty of Sciences and Mathematics, University of Niš, Serbia Avaiabe at: http://www.pmf.ni.ac.rs/fiomat Summation of p-adic Functiona
More informationarxiv: v1 [math.nt] 12 Feb 2019
Degenerate centra factoria numbers of the second ind Taeyun Kim, Dae San Kim arxiv:90.04360v [math.nt] Feb 09 In this paper, we introduce the degenerate centra factoria poynomias and numbers of the second
More informationDual Integral Equations and Singular Integral. Equations for Helmholtz Equation
Int.. Contemp. Math. Sciences, Vo. 4, 9, no. 34, 1695-1699 Dua Integra Equations and Singuar Integra Equations for Hemhotz Equation Naser A. Hoshan Department of Mathematics TafiaTechnica University P.O.
More informationSome Applications on Generalized Hypergeometric and Confluent Hypergeometric Functions
Internationa Journa of Mathematica Anaysis and Appications 0; 5(): 4-34 http://www.aascit.org/journa/ijmaa ISSN: 375-397 Some Appications on Generaized Hypergeometric and Confuent Hypergeometric Functions
More informationDifferential equations associated with higher-order Bernoulli numbers of the second kind
Goba Journa of Pure and Appied Mathematics. ISS 0973-768 Voume 2, umber 3 (206), pp. 2503 25 Research India Pubications http://www.ripubication.com/gjpam.htm Differentia equations associated with higher-order
More informationExtended central factorial polynomials of the second kind
Kim et a. Advances in Difference Equations 09 09:4 https://doi.org/0.86/s366-09-963- R E S E A R C H Open Access Extended centra factoria poynomias of the second ind Taeyun Kim,DaeSanKim,Gwan-WooJang and
More informationORTHOGONAL MULTI-WAVELETS FROM MATRIX FACTORIZATION
J. Korean Math. Soc. 46 2009, No. 2, pp. 281 294 ORHOGONAL MLI-WAVELES FROM MARIX FACORIZAION Hongying Xiao Abstract. Accuracy of the scaing function is very crucia in waveet theory, or correspondingy,
More informationGeneralized Bell polynomials and the combinatorics of Poisson central moments
Generaized Be poynomias and the combinatorics of Poisson centra moments Nicoas Privaut Division of Mathematica Sciences Schoo of Physica and Mathematica Sciences Nanyang Technoogica University SPMS-MAS-05-43,
More informationWeek 6 Lectures, Math 6451, Tanveer
Fourier Series Week 6 Lectures, Math 645, Tanveer In the context of separation of variabe to find soutions of PDEs, we encountered or and in other cases f(x = f(x = a 0 + f(x = a 0 + b n sin nπx { a n
More informationFinite Fourier Decomposition of Signals Using Generalized Difference Operator
SCIENTIFIC PUBLICATIONS OF THE STATE UNIVERSITY OF NOVI PAZAR SER. A: APPL. ATH. INFOR. AND ECH. vo. 9, (27, 47-57. Finite Fourier Decoosition of Signas Using Generaized Difference Oerator G. B. A. Xavier,
More informationEstablishment of Weak Conditions for Darboux- Goursat-Beudon Theorem
Georgia Southern University Digita Commons@Georgia Southern Mathematica Sciences Facuty Pubications Department of Mathematica Sciences 2009 Estabishment of Weak Conditions for Darboux- Goursat-Beudon Theorem
More informationResearch Article Building Infinitely Many Solutions for Some Model of Sublinear Multipoint Boundary Value Problems
Abstract and Appied Anaysis Voume 2015, Artice ID 732761, 4 pages http://dx.doi.org/10.1155/2015/732761 Research Artice Buiding Infinitey Many Soutions for Some Mode of Subinear Mutipoint Boundary Vaue
More informationJENSEN S OPERATOR INEQUALITY FOR FUNCTIONS OF SEVERAL VARIABLES
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Voume 128, Number 7, Pages 2075 2084 S 0002-99390005371-5 Artice eectronicay pubished on February 16, 2000 JENSEN S OPERATOR INEQUALITY FOR FUNCTIONS OF
More informationResearch Article On the Lower Bound for the Number of Real Roots of a Random Algebraic Equation
Appied Mathematics and Stochastic Anaysis Voume 007, Artice ID 74191, 8 pages doi:10.1155/007/74191 Research Artice On the Lower Bound for the Number of Rea Roots of a Random Agebraic Equation Takashi
More informationQUADRATIC FORMS AND FOUR PARTITION FUNCTIONS MODULO 3
QUADRATIC FORMS AND FOUR PARTITION FUNCTIONS MODULO 3 JEREMY LOVEJOY AND ROBERT OSBURN Abstract. Recenty, Andrews, Hirschhorn Seers have proven congruences moduo 3 for four types of partitions using eementary
More informationON THE POSITIVITY OF SOLUTIONS OF SYSTEMS OF STOCHASTIC PDES
ON THE POSITIVITY OF SOLUTIONS OF SYSTEMS OF STOCHASTIC PDES JACKY CRESSON 1,2, MESSOUD EFENDIEV 3, AND STEFANIE SONNER 3,4 On the occasion of the 75 th birthday of Prof. Dr. Dr.h.c. Wofgang L. Wendand
More informationOn the New q-extension of Frobenius-Euler Numbers and Polynomials Arising from Umbral Calculus
Adv. Studies Theor. Phys., Vo. 7, 203, no. 20, 977-99 HIKARI Ltd, www.m-hiari.com http://dx.doi.org/0.2988/astp.203.390 On the New -Extension of Frobenius-Euer Numbers and Poynomias Arising from Umbra
More informationGaussian Curvature in a p-orbital, Hydrogen-like Atoms
Advanced Studies in Theoretica Physics Vo. 9, 015, no. 6, 81-85 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.1988/astp.015.5115 Gaussian Curvature in a p-orbita, Hydrogen-ike Atoms Sandro-Jose Berrio-Guzman
More informationOn the Number of Limit Cycles for Discontinuous Generalized Liénard Polynomial Differential Systems
Internationa Journa of Bifurcation and Chaos Vo. 25 No. 10 2015 1550131 10 pages c Word Scientific Pubishing Company DOI: 10.112/S02181271550131X On the Number of Limit Cyces for Discontinuous Generaized
More informationC. Fourier Sine Series Overview
12 PHILIP D. LOEWEN C. Fourier Sine Series Overview Let some constant > be given. The symboic form of the FSS Eigenvaue probem combines an ordinary differentia equation (ODE) on the interva (, ) with a
More informationCourse 2BA1, Section 11: Periodic Functions and Fourier Series
Course BA, 8 9 Section : Periodic Functions and Fourier Series David R. Wikins Copyright c David R. Wikins 9 Contents Periodic Functions and Fourier Series 74. Fourier Series of Even and Odd Functions...........
More informationarxiv: v1 [math.ca] 6 Mar 2017
Indefinite Integras of Spherica Besse Functions MIT-CTP/487 arxiv:703.0648v [math.ca] 6 Mar 07 Joyon K. Boomfied,, Stephen H. P. Face,, and Zander Moss, Center for Theoretica Physics, Laboratory for Nucear
More informationMaejo International Journal of Science and Technology
Fu Paper Maejo Internationa Journa of Science and Technoogy ISSN 1905-7873 Avaiabe onine at www.mijst.mju.ac.th A study on Lucas difference sequence spaces (, ) (, ) and Murat Karakas * and Ayse Metin
More informationALGORITHMIC SUMMATION OF RECIPROCALS OF PRODUCTS OF FIBONACCI NUMBERS. F. = I j. ^ = 1 ^ -, and K w = ^. 0) n=l r n «=1 -*/!
ALGORITHMIC SUMMATIO OF RECIPROCALS OF PRODUCTS OF FIBOACCI UMBERS Staney Rabinowitz MathPro Press, 2 Vine Brook Road, Westford, MA 0886 staney@tiac.net (Submitted May 997). ITRODUCTIO There is no known
More informationOn Some Basic Properties of Geometric Real Sequences
On Some Basic Properties of eometric Rea Sequences Khirod Boruah Research Schoar, Department of Mathematics, Rajiv andhi University Rono His, Doimukh-791112, Arunacha Pradesh, India Abstract Objective
More informationMARKOV CHAINS AND MARKOV DECISION THEORY. Contents
MARKOV CHAINS AND MARKOV DECISION THEORY ARINDRIMA DATTA Abstract. In this paper, we begin with a forma introduction to probabiity and expain the concept of random variabes and stochastic processes. After
More informationInvestigation on spectrum of the adjacency matrix and Laplacian matrix of graph G l
Investigation on spectrum of the adjacency matrix and Lapacian matrix of graph G SHUHUA YIN Computer Science and Information Technoogy Coege Zhejiang Wani University Ningbo 3500 PEOPLE S REPUBLIC OF CHINA
More information4 1-D Boundary Value Problems Heat Equation
4 -D Boundary Vaue Probems Heat Equation The main purpose of this chapter is to study boundary vaue probems for the heat equation on a finite rod a x b. u t (x, t = ku xx (x, t, a < x < b, t > u(x, = ϕ(x
More informationSome identities of Laguerre polynomials arising from differential equations
Kim et a. Advances in Difference Equations 2016) 2016:159 DOI 10.1186/s13662-016-0896-1 R E S E A R C H Open Access Some identities of Laguerre poynomias arising from differentia equations Taekyun Kim
More informationComponentwise Determination of the Interval Hull Solution for Linear Interval Parameter Systems
Componentwise Determination of the Interva Hu Soution for Linear Interva Parameter Systems L. V. Koev Dept. of Theoretica Eectrotechnics, Facuty of Automatics, Technica University of Sofia, 1000 Sofia,
More informationExplicit overall risk minimization transductive bound
1 Expicit overa risk minimization transductive bound Sergio Decherchi, Paoo Gastado, Sandro Ridea, Rodofo Zunino Dept. of Biophysica and Eectronic Engineering (DIBE), Genoa University Via Opera Pia 11a,
More informationAn explicit Jordan Decomposition of Companion matrices
An expicit Jordan Decomposition of Companion matrices Fermín S V Bazán Departamento de Matemática CFM UFSC 88040-900 Forianópois SC E-mai: fermin@mtmufscbr S Gratton CERFACS 42 Av Gaspard Coriois 31057
More informationTHE REACHABILITY CONES OF ESSENTIALLY NONNEGATIVE MATRICES
THE REACHABILITY CONES OF ESSENTIALLY NONNEGATIVE MATRICES by Michae Neumann Department of Mathematics, University of Connecticut, Storrs, CT 06269 3009 and Ronad J. Stern Department of Mathematics, Concordia
More informationADELIC ANALYSIS AND FUNCTIONAL ANALYSIS ON THE FINITE ADELE RING. Ilwoo Cho
Opuscua Math. 38, no. 2 208, 39 85 https://doi.org/0.7494/opmath.208.38.2.39 Opuscua Mathematica ADELIC ANALYSIS AND FUNCTIONAL ANALYSIS ON THE FINITE ADELE RING Iwoo Cho Communicated by.a. Cojuhari Abstract.
More information6 Wave Equation on an Interval: Separation of Variables
6 Wave Equation on an Interva: Separation of Variabes 6.1 Dirichet Boundary Conditions Ref: Strauss, Chapter 4 We now use the separation of variabes technique to study the wave equation on a finite interva.
More informationStrauss PDEs 2e: Section Exercise 2 Page 1 of 12. For problem (1), complete the calculation of the series in case j(t) = 0 and h(t) = e t.
Strauss PDEs e: Section 5.6 - Exercise Page 1 of 1 Exercise For probem (1, compete the cacuation of the series in case j(t = and h(t = e t. Soution With j(t = and h(t = e t, probem (1 on page 147 becomes
More informationCS229 Lecture notes. Andrew Ng
CS229 Lecture notes Andrew Ng Part IX The EM agorithm In the previous set of notes, we taked about the EM agorithm as appied to fitting a mixture of Gaussians. In this set of notes, we give a broader view
More informationConvergence Property of the Iri-Imai Algorithm for Some Smooth Convex Programming Problems
Convergence Property of the Iri-Imai Agorithm for Some Smooth Convex Programming Probems S. Zhang Communicated by Z.Q. Luo Assistant Professor, Department of Econometrics, University of Groningen, Groningen,
More informationWAVELET LINEAR ESTIMATION FOR DERIVATIVES OF A DENSITY FROM OBSERVATIONS OF MIXTURES WITH VARYING MIXING PROPORTIONS. B. L. S.
Indian J. Pure App. Math., 41(1): 275-291, February 2010 c Indian Nationa Science Academy WAVELET LINEAR ESTIMATION FOR DERIVATIVES OF A DENSITY FROM OBSERVATIONS OF MIXTURES WITH VARYING MIXING PROPORTIONS
More informationBinomial Transform and Dold Sequences
1 2 3 47 6 23 11 Journa of Integer Sequences, Vo. 18 (2015), Artice 15.1.1 Binomia Transform and Dod Sequences Kaudiusz Wójcik Department of Mathematics and Computer Science Jagieonian University Lojasiewicza
More informationAn Extension of Almost Sure Central Limit Theorem for Order Statistics
An Extension of Amost Sure Centra Limit Theorem for Order Statistics T. Bin, P. Zuoxiang & S. Nadarajah First version: 6 December 2007 Research Report No. 9, 2007, Probabiity Statistics Group Schoo of
More informationDo Schools Matter for High Math Achievement? Evidence from the American Mathematics Competitions Glenn Ellison and Ashley Swanson Online Appendix
VOL. NO. DO SCHOOLS MATTER FOR HIGH MATH ACHIEVEMENT? 43 Do Schoos Matter for High Math Achievement? Evidence from the American Mathematics Competitions Genn Eison and Ashey Swanson Onine Appendix Appendix
More informationProblem set 6 The Perron Frobenius theorem.
Probem set 6 The Perron Frobenius theorem. Math 22a4 Oct 2 204, Due Oct.28 In a future probem set I want to discuss some criteria which aow us to concude that that the ground state of a sef-adjoint operator
More informationGeneral Decay of Solutions in a Viscoelastic Equation with Nonlinear Localized Damping
Journa of Mathematica Research with Appications Jan.,, Vo. 3, No., pp. 53 6 DOI:.377/j.issn:95-65...7 Http://jmre.dut.edu.cn Genera Decay of Soutions in a Viscoeastic Equation with Noninear Locaized Damping
More informationUniprocessor Feasibility of Sporadic Tasks with Constrained Deadlines is Strongly conp-complete
Uniprocessor Feasibiity of Sporadic Tasks with Constrained Deadines is Strongy conp-compete Pontus Ekberg and Wang Yi Uppsaa University, Sweden Emai: {pontus.ekberg yi}@it.uu.se Abstract Deciding the feasibiity
More informationHomogeneity properties of subadditive functions
Annaes Mathematicae et Informaticae 32 2005 pp. 89 20. Homogeneity properties of subadditive functions Pá Burai and Árpád Száz Institute of Mathematics, University of Debrecen e-mai: buraip@math.kte.hu
More informationNOISE-INDUCED STABILIZATION OF STOCHASTIC DIFFERENTIAL EQUATIONS
NOISE-INDUCED STABILIZATION OF STOCHASTIC DIFFERENTIAL EQUATIONS TONY ALLEN, EMILY GEBHARDT, AND ADAM KLUBALL 3 ADVISOR: DR. TIFFANY KOLBA 4 Abstract. The phenomenon of noise-induced stabiization occurs
More informationarxiv: v1 [math.nt] 17 Jul 2015
ON THE DEGENERATE FROBENIUS-EULER POLYNOMIALS arxiv:1507.04846v1 [math.nt] 17 Ju 2015 TAEKYUN KIM, HYUCK-IN KWON, AND JONG-JIN SEO Abstract. In this paper, we consider the degenerate Frobenius-Euer poynomias
More informationConsistent linguistic fuzzy preference relation with multi-granular uncertain linguistic information for solving decision making problems
Consistent inguistic fuzzy preference reation with muti-granuar uncertain inguistic information for soving decision making probems Siti mnah Binti Mohd Ridzuan, and Daud Mohamad Citation: IP Conference
More informationImproving the Reliability of a Series-Parallel System Using Modified Weibull Distribution
Internationa Mathematica Forum, Vo. 12, 217, no. 6, 257-269 HIKARI Ltd, www.m-hikari.com https://doi.org/1.12988/imf.217.611155 Improving the Reiabiity of a Series-Parae System Using Modified Weibu Distribution
More informationResearch Article Some Applications of Second-Order Differential Subordination on a Class of Analytic Functions Defined by Komatu Integral Operator
ISRN Mathematia Anaysis, Artie ID 66235, 5 pages http://dx.doi.org/1.1155/214/66235 Researh Artie Some Appiations of Seond-Order Differentia Subordination on a Cass of Anayti Funtions Defined by Komatu
More informationarxiv: v4 [math.nt] 20 Jan 2015
arxiv:3.448v4 [math.nt] 20 Jan 205 NEW IDENTITIES ON THE APOSTOL-BERNOULLI POLYNOMIALS OF HIGHER ORDER DERIVED FROM BERNOULLI BASIS ARMEN BAGDASARYAN, SERKAN ARACI, MEHMET ACIKGOZ, AND YUAN HE Abstract.
More information(f) is called a nearly holomorphic modular form of weight k + 2r as in [5].
PRODUCTS OF NEARLY HOLOMORPHIC EIGENFORMS JEFFREY BEYERL, KEVIN JAMES, CATHERINE TRENTACOSTE, AND HUI XUE Abstract. We prove that the product of two neary hoomorphic Hece eigenforms is again a Hece eigenform
More informationarxiv: v1 [math.ap] 8 Nov 2014
arxiv:1411.116v1 [math.ap] 8 Nov 014 ALL INVARIANT REGIONS AND GLOBAL SOLUTIONS FOR m-component REACTION-DIFFUSION SYSTEMS WITH A TRIDIAGONAL SYMMETRIC TOEPLITZ MATRIX OF DIFFUSION COEFFICIENTS SALEM ABDELMALEK
More informationPath planning with PH G2 splines in R2
Path panning with PH G2 spines in R2 Laurent Gajny, Richard Béarée, Eric Nyiri, Oivier Gibaru To cite this version: Laurent Gajny, Richard Béarée, Eric Nyiri, Oivier Gibaru. Path panning with PH G2 spines
More informationThe numerical radius of a weighted shift operator
Eectronic Journa of Linear Agebra Voume 30 Voume 30 2015 Artice 60 2015 The numerica radius of a weighted shift operator Batzorig Undrah Nationa University of Mongoia, batzorig_u@yahoo.com Hiroshi Naazato
More informationTHE PARTITION FUNCTION AND HECKE OPERATORS
THE PARTITION FUNCTION AND HECKE OPERATORS KEN ONO Abstract. The theory of congruences for the partition function p(n depends heaviy on the properties of haf-integra weight Hecke operators. The subject
More informationNumerical solution of one dimensional contaminant transport equation with variable coefficient (temporal) by using Haar wavelet
Goba Journa of Pure and Appied Mathematics. ISSN 973-1768 Voume 1, Number (16), pp. 183-19 Research India Pubications http://www.ripubication.com Numerica soution of one dimensiona contaminant transport
More informationStatistical Learning Theory: A Primer
Internationa Journa of Computer Vision 38(), 9 3, 2000 c 2000 uwer Academic Pubishers. Manufactured in The Netherands. Statistica Learning Theory: A Primer THEODOROS EVGENIOU, MASSIMILIANO PONTIL AND TOMASO
More informationKing Fahd University of Petroleum & Minerals
King Fahd University of Petroeum & Mineras DEPARTMENT OF MATHEMATICAL SCIENCES Technica Report Series TR 369 December 6 Genera decay of soutions of a viscoeastic equation Saim A. Messaoudi DHAHRAN 3161
More informationOn formulas for moments of the Wishart distributions as weighted generating functions of matchings
FPSAC 2010, San Francisco, USA DMTCS proc. AN, 2010, 821 832 On formuas for moments of the Wishart distributions as weighted generating functions of matchings Yasuhide NUMATA 1,3 and Satoshi KURIKI 2,3
More informationAssignment 7 Due Tuessday, March 29, 2016
Math 45 / AMCS 55 Dr. DeTurck Assignment 7 Due Tuessday, March 9, 6 Topics for this week Convergence of Fourier series; Lapace s equation and harmonic functions: basic properties, compuations on rectanges
More informationFirst-Order Corrections to Gutzwiller s Trace Formula for Systems with Discrete Symmetries
c 26 Noninear Phenomena in Compex Systems First-Order Corrections to Gutzwier s Trace Formua for Systems with Discrete Symmetries Hoger Cartarius, Jörg Main, and Günter Wunner Institut für Theoretische
More informationOn the Goal Value of a Boolean Function
On the Goa Vaue of a Booean Function Eric Bach Dept. of CS University of Wisconsin 1210 W. Dayton St. Madison, WI 53706 Lisa Heerstein Dept of CSE NYU Schoo of Engineering 2 Metrotech Center, 10th Foor
More informationA Two-Parameter Trigonometric Series
A Two-Parameter Trigonometric Series Xiang-Qian Chang Xiang.Chang@bos.mcphs.edu Massachusetts Coege of Pharmacy and Heath Sciences Boston MA 25 Let us consider the foowing dua questions. A. Givenafunction
More informationPartial permutation decoding for MacDonald codes
Partia permutation decoding for MacDonad codes J.D. Key Department of Mathematics and Appied Mathematics University of the Western Cape 7535 Bevie, South Africa P. Seneviratne Department of Mathematics
More informationarxiv: v1 [math.co] 12 May 2013
EMBEDDING CYCLES IN FINITE PLANES FELIX LAZEBNIK, KEITH E. MELLINGER, AND SCAR VEGA arxiv:1305.2646v1 [math.c] 12 May 2013 Abstract. We define and study embeddings of cyces in finite affine and projective
More informationDisturbance decoupling by measurement feedback
Preprints of the 19th Word Congress The Internationa Federation of Automatic Contro Disturbance decouping by measurement feedback Arvo Kadmäe, Üe Kotta Institute of Cybernetics at TUT, Akadeemia tee 21,
More informationSmoothness equivalence properties of univariate subdivision schemes and their projection analogues
Numerische Mathematik manuscript No. (wi be inserted by the editor) Smoothness equivaence properties of univariate subdivision schemes and their projection anaogues Phiipp Grohs TU Graz Institute of Geometry
More informationResearch Article New Iterative Method: An Application for Solving Fractional Physical Differential Equations
Abstract and Appied Anaysis Voume 203, Artice ID 6700, 9 pages http://d.doi.org/0.55/203/6700 Research Artice New Iterative Method: An Appication for Soving Fractiona Physica Differentia Equations A. A.
More information2M2. Fourier Series Prof Bill Lionheart
M. Fourier Series Prof Bi Lionheart 1. The Fourier series of the periodic function f(x) with period has the form f(x) = a 0 + ( a n cos πnx + b n sin πnx ). Here the rea numbers a n, b n are caed the Fourier
More informationLegendre Polynomials - Lecture 8
Legendre Poynomias - Lecture 8 Introduction In spherica coordinates the separation of variabes for the function of the poar ange resuts in Legendre s equation when the soution is independent of the azimutha
More informationResearch Article Numerical Range of Two Operators in Semi-Inner Product Spaces
Abstract and Appied Anaysis Voume 01, Artice ID 846396, 13 pages doi:10.1155/01/846396 Research Artice Numerica Range of Two Operators in Semi-Inner Product Spaces N. K. Sahu, 1 C. Nahak, 1 and S. Nanda
More informationarxiv: v1 [math.nt] 13 Jan 2009
NOTE ON THE GENERALIZATION OF THE HIGHER ORDER -GENOCCHI NUMBERS AND -EULER NUMBERS arxiv:09011697v1 [athnt] 13 Jan 2009 TAEKYUN KIM, YOUNG-HEE KIM, AND KYUNG-WON HWANG Abstract Cangu-Ozden-Sisek[1] constructed
More informationOPERATORS WITH COMMON HYPERCYCLIC SUBSPACES
OPERATORS WITH COMMON HYPERCYCLIC SUBSPACES R. ARON, J. BÈS, F. LEÓN AND A. PERIS Abstract. We provide a reasonabe sufficient condition for a famiy of operators to have a common hypercycic subspace. We
More informationMat 1501 lecture notes, penultimate installment
Mat 1501 ecture notes, penutimate instament 1. bounded variation: functions of a singe variabe optiona) I beieve that we wi not actuay use the materia in this section the point is mainy to motivate the
More informationUmbral calculus and Sheffer sequences of polynomials. Taekyun Kim, 1, a) Dae San Kim, 2, b) Toufik Mansour, 3, c) Seog-Hoon Rim, 4, d) and
Umbra cacuus and Sheffer sequences of poynomias Taeyun Kim, 1, a Dae San Kim, 2, b Toufi Mansour, 3, c Seog-Hoon Rim, 4, d and 5, e Matthias Schor 1 Department of Mathematics, Kwangwoon University, Seou,
More informationTHINKING IN PYRAMIDS
ECS 178 Course Notes THINKING IN PYRAMIDS Kenneth I. Joy Institute for Data Anaysis and Visuaization Department of Computer Science University of Caifornia, Davis Overview It is frequenty usefu to think
More informationRestricted weak type on maximal linear and multilinear integral maps.
Restricted weak type on maxima inear and mutiinear integra maps. Oscar Basco Abstract It is shown that mutiinear operators of the form T (f 1,..., f k )(x) = R K(x, y n 1,..., y k )f 1 (y 1 )...f k (y
More informationODE Homework 2. Since M y N x, the equation is not exact. 2. Determine whether the following equation is exact. If it is exact, M y N x 1 x.
ODE Homework.6. Exact Equations and Integrating Factors 1. Determine whether the foowing equation is exact. If it is exact, find the soution pe x sin qdx p3x e x sin qd 0 [.6 #8] So. Let Mpx, q e x sin,
More informationDavid Eigen. MA112 Final Paper. May 10, 2002
David Eigen MA112 Fina Paper May 1, 22 The Schrodinger equation describes the position of an eectron as a wave. The wave function Ψ(t, x is interpreted as a probabiity density for the position of the eectron.
More informationA NOTE ON QUASI-STATIONARY DISTRIBUTIONS OF BIRTH-DEATH PROCESSES AND THE SIS LOGISTIC EPIDEMIC
(January 8, 2003) A NOTE ON QUASI-STATIONARY DISTRIBUTIONS OF BIRTH-DEATH PROCESSES AND THE SIS LOGISTIC EPIDEMIC DAMIAN CLANCY, University of Liverpoo PHILIP K. POLLETT, University of Queensand Abstract
More informationLecture 6: Moderately Large Deflection Theory of Beams
Structura Mechanics 2.8 Lecture 6 Semester Yr Lecture 6: Moderatey Large Defection Theory of Beams 6.1 Genera Formuation Compare to the cassica theory of beams with infinitesima deformation, the moderatey
More informationLecture Notes for Math 251: ODE and PDE. Lecture 34: 10.7 Wave Equation and Vibrations of an Elastic String
ecture Notes for Math 251: ODE and PDE. ecture 3: 1.7 Wave Equation and Vibrations of an Eastic String Shawn D. Ryan Spring 212 ast Time: We studied other Heat Equation probems with various other boundary
More information4 Separation of Variables
4 Separation of Variabes In this chapter we describe a cassica technique for constructing forma soutions to inear boundary vaue probems. The soution of three cassica (paraboic, hyperboic and eiptic) PDE
More informationSome Properties Related to the Generalized q-genocchi Numbers and Polynomials with Weak Weight α
Appied Mathematica Sciences, Vo. 6, 2012, no. 118, 5851-5859 Some Properties Reated to the Generaized q-genocchi Numbers and Poynomias with Weak Weight α J. Y. Kang Department of Mathematics Hannam University,
More informationFORECASTING TELECOMMUNICATIONS DATA WITH AUTOREGRESSIVE INTEGRATED MOVING AVERAGE MODELS
FORECASTING TEECOMMUNICATIONS DATA WITH AUTOREGRESSIVE INTEGRATED MOVING AVERAGE MODES Niesh Subhash naawade a, Mrs. Meenakshi Pawar b a SVERI's Coege of Engineering, Pandharpur. nieshsubhash15@gmai.com
More informationPRIME TWISTS OF ELLIPTIC CURVES
PRIME TWISTS OF ELLIPTIC CURVES DANIEL KRIZ AND CHAO LI Abstract. For certain eiptic curves E/Q with E(Q)[2] = Z/2Z, we prove a criterion for prime twists of E to have anaytic rank 0 or 1, based on a mod
More informationMIXING AUTOMORPHISMS OF COMPACT GROUPS AND A THEOREM OF SCHLICKEWEI
MIXING AUTOMORPHISMS OF COMPACT GROUPS AND A THEOREM OF SCHLICKEWEI KLAUS SCHMIDT AND TOM WARD Abstract. We prove that every mixing Z d -action by automorphisms of a compact, connected, abeian group is
More informationRELATIONSHIP BETWEEN QUATERNION LINEAR CANONICAL AND QUATERNION FOURIER TRANSFORMS
Proceedings of the 04 Internationa Conference on Waveet Anaysis and Pattern ecognition, Lanzhou, 3-6 Juy, 04 ELATIONSHIP BETWEEN QUATENION LINEA CANONICAL AND QUATENION FOUIE TANSFOMS MAWADI BAHI, YUICHI
More informationTRIPLE FACTORIZATION OF SOME RIORDAN MATRICES. Paul Peart* Department of Mathematics, Howard University, Washington, D.C
Pau Peart* Department of Mathematics, Howard University, Washington, D.C. 59 Leon Woodson Department of Mathematicss, Morgan State University, Batimore, MD 39 (Submitted June 99). INTRODUCTION When examining
More informationSome Measures for Asymmetry of Distributions
Some Measures for Asymmetry of Distributions Georgi N. Boshnakov First version: 31 January 2006 Research Report No. 5, 2006, Probabiity and Statistics Group Schoo of Mathematics, The University of Manchester
More informationSeparation of Variables and a Spherical Shell with Surface Charge
Separation of Variabes and a Spherica She with Surface Charge In cass we worked out the eectrostatic potentia due to a spherica she of radius R with a surface charge density σθ = σ cos θ. This cacuation
More informationEffect of transport ratio on source term in determination of surface emission coefficient
Internationa Journa of heoretica & Appied Sciences, (): 74-78(9) ISSN : 975-78 Effect of transport ratio on source term in determination of surface emission coefficient Sanjeev Kumar and Apna Mishra epartment
More informationFitting affine and orthogonal transformations between two sets of points
Mathematica Communications 9(2004), 27-34 27 Fitting affine and orthogona transformations between two sets of points Hemuth Späth Abstract. Let two point sets P and Q be given in R n. We determine a transation
More informationGeneral Certificate of Education Advanced Level Examination June 2010
Genera Certificate of Education Advanced Leve Examination June 2010 Human Bioogy HBI6T/Q10/task Unit 6T A2 Investigative Skis Assignment Task Sheet The effect of using one or two eyes on the perception
More informationAALBORG UNIVERSITY. The distribution of communication cost for a mobile service scenario. Jesper Møller and Man Lung Yiu. R June 2009
AALBORG UNIVERSITY The distribution of communication cost for a mobie service scenario by Jesper Møer and Man Lung Yiu R-29-11 June 29 Department of Mathematica Sciences Aaborg University Fredrik Bajers
More informationThe functional variable method for solving the fractional Korteweg de Vries equations and the coupled Korteweg de Vries equations
PRAMANA c Indian Academy of Sciences Vo. 85, No. 4 journa of October 015 physics pp. 583 59 The functiona variabe method for soving the fractiona Korteweg de Vries equations and the couped Korteweg de
More information