New Cartan s Tensors and Pseudotensors in a Generalized Finsler Space
|
|
- Isabella Parrish
- 6 years ago
- Views:
Transcription
1 Flomat 8: 04, 07 7 DOI 0.98/FIL4007C Publhed by Faculty of Scence and Mathematc, Unverty of Nš, Serba valable at: htt:// New Cartan Tenor and Peudotenor n a Generalzed Fnler Sace Mlca D. Cvetkovć a, Mlan Lj. Zlatanovć b a Unverty of Nš, Faculty of Scence and Mathematc, 8000 Nš, Serba, and College for led Techncal Scence, 8000 Nš, Serba, b Unverty of Nš, Faculty of Scence and Mathematc, 8000 Nš, Serba btract. In th work we defned a generalzed Fnler ace GF N a N-dmenonal dfferentable manfold wth a non-ymmetrc bac tenor j x, ẋ, whch ale that j θmx, ẋ = 0, θ =,. Baed on non-ymmetry of bac tenor, we obtaned ten Rcc tye dentte, comarng to two knd of covarant dervatve of a tenor n Rund ene. There aear two new curvature tenor and ffteen magntude, we called curvature eudotenor.. Introducton Fnler geometry a natural and fundamental generalzaton of Remann geometry. It wa frt uggeted by Remann a early a 854 [5], and tuded ytematcally by Fnler n 98 [5]. The name Fnler Geometry wa frt gven by J. Taylor n 97. The non-ymmetrc connecton wa nteretng to many author:. Yano [],.C. Shamhoke [7], S.Mnčć [8]-[0], S. Manoff [6], C.. Mhra[] and many other: [7], [0], []. Fnler [5] ace F N are N-dmenonal manfold the nfntemal dtance between two neghborng ont x, x + dx gven by: d = Fx, dx, =,..., N, F requred to atfy ome roerte [6]: Fx, dx > 0; Fx, λdx = λfx, dx, for any λ > 0; 3 The quadrc form F x, dx dx dx j ξ ξ j > 0, for all vector ξ and any x, dx. Then, the metrc tenor defned from a: j = F x, ẋ, ẋ ẋ j 3 00 Mathematc Subject Clafcaton. Prmary 5345; Secondary 53B05, 53B40 eyword. The generalzed Fnler ace, Rcc tye dentte, h-dfferentaton. Receved: 6 May 03; cceted: Setember 03 Communcated by Ljubca Velmrovć Reearch uorted by the reearch roject 740 of the Serban Mntry of Scence Emal addree: mlcacvetkovc@bb.r Mlca D. Cvetkovć, zlatmlan@mf.n.ac.r Mlan Lj. Zlatanovć
2 M. Cvetkovć, M. Zlatanovć / Flomat 8: 04, ẋ = dx dt are the tangent vector to a curve C : x = x t n the manfold ace, or element of the tangent ace T n x at ont x. Ung the econd condton n, j are homogeneou of degree zero n the other et of varable and we can wrte: d = j x k, dx k dx dx j. 4 Defnton.. The generalzed Fnler ace GF N a dfferentable manfold wth non-ymmetrc bac tenor j x, ẋ, j x, ẋ j x, ẋ, = det j 0. 5 Baed on 5, t can be defned the ymmetrc, reectvely, antymmetrc art of j : j = j + j, j = j j, 6, followng [7], t true that: a j = F x, ẋ j, b ẋ ẋ j ẋ = 0, 7 k F a metrc functon n GF N, havng the roerte known from the theory of uual Fnler ace. In the aer [8 0, 3, 4] we tuded generalzed Fnler ace. Introducng a Cartan tenor C jk, mlar a n F N, we have: C jk x, ẋ de = f j,ẋ = k 7b j,ẋ = k 4 F, 8 ẋ ẋ j ẋ k = 7b gnfe equal baed on 7b. We can conclude that C jk ymmetrc n relaton to each ar of ndce. lo, we have: C jk de f = h C jk = 8 h C jk = h C jk = C kj. 9 In GF N the next equaton are vald: C jk ẋ = C jk ẋ j = C jk ẋ k = 0. 0 One obtan coeffcent of non-ymmetrc affne connecton n the Cartan ene []: Γ jk = γ jk hl C jl Γ k + C klγ j C jkγ l ẋ Γ kj, Γ.jk = Γ r jk r = γ.jk C j Γ k + C kγ j C jkγ ẋ Γ.kj. We defned the coeffcent: Γ jk = γ jk hl C kl Γ j + C jlγ k C kjγ l ẋ Γ kj, 3 Γ.jk = Γ r jk r = γ.jk C k Γ j + C jγ k C kjγ ẋ Γ.kj. 4 Let u denote: T jk x, ẋ = Γ jk Γ kj, T jk x, ẋ = Γ jk Γ kj, Γ jk = Γ jk + Γ kj, Γ jk = Γ jk + Γ kj,
3 M. Cvetkovć, M. Zlatanovć / Flomat 8: 04, a toron tenor of the connecton Γ, Γ, reectvely. Baed on non-ymmetry of the coeffcent of the connecton, t can be defned two knd of h-covarant dervatve: T j m = T j,m + T j Γ m TΓ jm T j,ṡ Γrmẋr, T j m = T j,m + T j Γ m T Γ mj T j,ṡ Γmrẋr. By the rocedure that mlar n a Fnler ace, t can be roved that covarant dervatve 5 of a tenor alo a tenor. Theorem.. For the tenor j x, ẋ baed on both knd of dervatve 5 n GF N t vald: 5 j θmx, ẋ = 0, θ =,. 6 Proof. Startng from 5, we get: j mx, ẋ = j,m j,ṗ Γ rmẋ r Γ m j Γ jm = = j,m C j Γ rmẋ r Γ.jm + 8, Γ j.m = 0. 7 The ame reult one obtan for j m : j mx, ẋ = j,m j,ṗ Γ mrẋ r Γ m j Γ mj = = j,m C j Γ mrẋ r Γ j.m + Γ.mj = 0, 8 8, and we have roved 6.. Rcc tye dentte for h-dfferentaton n GF N It known that n Fnler ace there only one Rcc dentty for h-dfferentaton, correondng to alternated covarant dervatve of the nd order. In the cae of non-ymmetrc affne connecton there are 0 oblte to form the dfference: a r r u t t v m n ar r u t t v m λ µ ν ω n λ, µ, ν, ω =,, 9, denote two knd of covarant dervatve baed on.7,.8, and we can obtan ten Rcc tye dentte and two tenor of curvature. Correondng dentte n GF N may be roved by total nducton method. The mentoned oblte are obtaned for thee combnaton: λ, µ; ν, ω {, ;,,, ;,,, ;,,, ;,,, ;,,, ;,,, ;,,, ;,,, ;,,, ;, }. 0 For fndng the general cae baed on., we frtly oberve the cae of a tenor a x, ξ. Let u obtan the cae when the vector feld ξ l tatonary comarng to the frt knd of covarant dervatve,.e. ξ l h x, ξ = 0, ξl h x, ξ 0.
4 M. Cvetkovć, M. Zlatanovć / Flomat 8: 04, nd we have: ξ l,h = ξl x h = Γ l rh ξr = Gl x, ξ ẋ h = G l,ḣ. Then, we obtaned, for examle, a j mn =a j m,n + a j m,ṡξ ș n + Γ na j m Γ jn a m Γ mna j = =a j,mn + a j,nṡ ξș m + a j,ṡ ξș mn + Γ m,na j + Γ ma j,n Γ jm,n a Γ jm a,n+ + a j,mṡ ξș n + a j, lṡ ξl,mξ ș n + a j, l ξl,mṡ ξș n + Γ m,ṡ a j ξș n + Γ ma j,ṡ ξș n Γ jm,ṡ a ξ ș n Γ jm a,ṡ ξș n+ + Γ na j,m + Γ na j,ṡ ξș m + Γ nγ ma j Γ nγ jm a Γ jn a,m Γ jn a,ṡ ξș m Γ jn Γ ma + Γ jn Γ ma Γ mna j. 3 nd mlar: a j m n = a j,mn + a j,nṡ ξș m + a j,ṡ ξș mn + Γ m,na j + Γ ma j,n Γ jm,n a Γ jm a,n+ + a j,mṡ ξș n + a j, lṡ ξl,mξ ș n + a j, l ξl,mṡ ξș n + Γ m,ṡ a j ξș n + Γ ma j,ṡ ξș n Γ jm,ṡ a ξ ș n Γ jm a,ṡ ξș n+ + Γ na j,m + Γ na j,ṡ ξș m + Γ nγ ma j Γ nγ jm a Γ nj a,m Γ nj a,ṡ ξș m Γ nj Γ ma + Γ nj Γ ma Γ nma j. 4 a j m n = a j,mn + a j,nṡ ξș m + a j,ṡ ξș mn + Γ m,na j + Γ ma j,n Γ mj,n a Γ mj a,n+ + a j,mṡ ξș n + a j, lṡ ξl,mξ ș n + a j, l ξl,mṡ ξș n + Γ m,ṡ a j ξș n + Γ ma j,ṡ ξș n Γ mj,ṡ a ξ ș n Γ mj a,ṡ ξș n+ + Γ na j,m + Γ na j,ṡ ξș m + Γ n Γ ma j Γ n Γ mj a Γ jn a,m Γ jn a,ṡ ξș m Γ jn Γ ma + Γ jn Γ ma Γ mna j. 5 a j mn = a j,mn + a j,nṡ ξș m + a j,ṡ ξș mn + Γ m,na j + Γ ma j,n Γ mj,n a Γ mj a,n+ + a j,mṡ ξș n + a j, lṡ ξl,mξ ș n + a j, l ξl,mṡ ξș n + Γ m,ṡ a j ξș n + Γ ma j,ṡ ξș n Γ mj,ṡ a ξ ș n Γ mj a,ṡ ξș n+ + Γ na j,m + Γ na j,ṡ ξș m + Γ n Γ ma j Γ n Γ mj a Γ nj a,m Γ nj a,ṡ ξș m Γ nj Γ ma + Γ nj Γ ma Γ nma j. 6 lo, we have a j,ṡ ξș mn + a j, l ξl,mṡ ξș n = a G j,ṡ + a G l G x n ẋ m j, l ẋ ẋ m ẋ n = Γ = a rm j,ṡ x n ẋr Γ lm + Γ rm ẋ r G l ẋ l,ṅ = = a j,ṡ Γ rm,n Γ lm Γ l rn Γ l ẋr rm, l Gl,ṅ. 7
5 M. Cvetkovć, M. Zlatanovć / Flomat 8: 04, We condered the dfference: a j mn a j nm = a j,mn + a j,nṡ ξș m + a j,ṡ ξș mn + Γ m,na j + Γ ma j,n Γ jm,n a Γ jm a,n+ + a j,mṡ ξș n + a j, lṡ ξl,mξ ș n + a j, l ξl,mṡ ξș n + Γ m,ṡ a j ξș n + Γ ma j,ṡ ξș n Γ jm,ṡ a ξ ș n Γ jm a,ṡ ξș n+ + Γ na j,m + Γ na j,ṡ ξș m + Γ nγ ma j Γ nγ jm a Γ jn a,m Γ jn a,ṡ ξș m Γ jn Γ ma + Γ jn Γ ma Γ mna j a j,nm a j,mṡ ξș n a j,ṡ ξș nm Γ n,ma j Γ na j,m + Γ jn,m a + Γ jn a,m a j,nṡ ξș m a j, lṡ ξl,nξ ș m a j, l ξl,nṡ ξș m Γ n,ṡ a j ξș m Γ na j,ṡ ξș m + Γ jn,ṡ a ξ ș m + Γ jn a,ṡ ξș m Γ ma j,n Γ ma j,ṡ ξș n Γ mγ na j + Γ mγ jn a + + Γ jm a,n + Γ jm a,ṡ ξș n + Γ jm Γ na Γ jm Γ na + Γ = mn a j jmn a a j,ṡ rmn ẋ r T mna j, nma j = 8 mn = Γ m,n Γ n,m + Γ mγ n Γ nγ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ. 9 Theorem.. In the generalzed Fnler ace GF N, for h-dfferentaton, the frt Rcc tye dentty exreed: mn a nm = r αmn, ṡ rmn ẋ r Tmna, 30 α= β= gven by 9 and = a r + r u t t v, = a r r u t t β r β+ t v. 3 Ung.6 t eay to rove that: mn ẋ r = We condered: G x n ẋ m G x m ẋ n + G G m ẋ n G G n ẋ m = G,nṁ G,ṅm + G mg ș ṅ G ng ș ṁ, 3 G mn = a j mn a j nm = mn a j jmn a a j,ṡ rmn ẋ r T and fnally, we get: = mn + rmn l r a j a j mn a j nm = R mn a j R jmn a j a j rmn l r T G ẋ n ẋ m = G nm. mna j = jmn + j rmn l r a a j rmn l r T mna j mna j, 33, 34 we denoted the thrd tenor of Cartan, our the frt new curvature tenor ee Rund: R mn = mn + C rmn ẋ r = = Γ m,n Γ n,m + Γ mγ n Γ nγ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ + C G ș nṁ G ș ṅm + G qmg q,ṅ 35 G qng q,ṁ,
6 M. Cvetkovć, M. Zlatanovć / Flomat 8: 04, 07 7 and alo t vald: R mn ẋ = mn ẋ. 36. For the next dfference, we got: a j mn a j nm = mn a j jmn a + a j,ṡ rmn ẋ r + T = mn + rmn l r a j = R mn a j R jmn a j a j rmn l r + T mna j = jmn + j rmn l r a a j rmn l r + T mna j, mna j = 37 jmn = Γ mj,n Γ nj,m + Γ mj Γ n Γ nj Γ m Γ mj,ṡ Gș ṅ + Γ nj,ṡ Gș ṁ, 38 and the econd curvature tenor gven wth: R mn = mn + C rmn ẋ r = = Γ mj,n Γ nj,m + Γ mj Γ n Γ nj Γ m Γ mj,ṡ Gș ṅ + Γ nj,ṡ Gș ṁ + C G ș nṁ G ș ṅm + G qmg q,ṅ 39 G qng q,ṁ. It eay to rove that: R mn ẋ = mn ẋ. 40 Theorem.. In the generalzed Fnler ace GF N, for h-dfferentaton, the econd Rcc tye dentty exreed: mn a nm = r αmn, ṡ rmn ẋ r + T mna, 4 gven by 38. α= β= 3. For the dfference, we can get: a j m n a j n m = mn a j jmn a + a j<mn> + a j mn a,ṡ rmn ẋ r + T = mn + rmn l r a j + a j<mn> + a j mn a,ṡ rmn ẋ r + T = B mn a j B mna j = jmn + j rmn l r a a j rmn l r + mna j = jmn a j a j rmn l r + a j<mn> + a j mn a,ṡ rmn ẋ r + T mna j, 4 mn = Γ m,n Γ n,m + Γ m Γ n Γ n Γ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ, 43 mn = Γ m,n Γ n,m + Γ mγ n Γ nγ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ, 44 B mn = mn + C rmn ẋ r, B mn = mn + C rmn ẋ r, 45 a j<mn> = M ma j,n + a j,ṡ ξș n M jm a,n + a,ṡ ξș n, 46
7 M. Cvetkovć, M. Zlatanovć / Flomat 8: 04, a j mn = Γ mγ jn Γ m Γ nj a. It eay to rove that: 47 B mn ẋ = mn ẋ, B mn ẋ = mn ẋ. 48 Theorem.3. In GF N, for h-dfferentaton, the 3 rd Rcc tye dentty exreed by: m n a n m = r αmn, ṡ rmn ẋ r + α= β= + <mn> + mn + T mn and are gven by equaton 43, 44 and <mn> = α= M m,n +,ṡ ξș n β=, 49 M t β m,n +,ṡ ξș n, 50 u a r r u t t v mn = α= β= α<β v + α= β= α<β Γ [m Γ [t α m Γ r β n ] Γ tα nt β ] r β, α= β= Γ Γ [m nt β ] + 5 = a r + r u t t β r β+ t v. 4. We alo condered the dfference: a j m n a j n m = mn a 3 j 4 jmn a a j<mn> a j mn + a,ṡ rmn ẋ r T mna j, 5 3 mn = Γ m,n Γ n,m + Γ mγ n Γ nγ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ, 53 4 mn = Γ m,n Γ n,m + Γ m Γ n Γ n Γ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ. 54 Theorem.4. lyng the two knd of covarant dervatve n an nvere order than uual, we obtaned the 4 th Rcc tye dentty n GF N for h-dfferentaton: m n a n m = r αmn 3 4, ṡ rmn ẋ r α= β= 55 <mn> mn T mn, 3 and 4 are gven by 53, 54.
8 5. We condered the dfference: M. Cvetkovć, M. Zlatanovć / Flomat 8: 04, a j mn a j nm = mn a 5 j 6 jmn a + a j<mn> + a j mn a,ṡ rmn ẋ r Γ mna j + Γ mna j, 56 5 mn = Γ m,n Γ n,m + Γ mγ n Γ n Γ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ, 57 6 mn = Γ m,n Γ n,m + Γ m Γ n Γ nγ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ. 58 Theorem.5. In GF N, for h-dfferentaton, there the 5 th Rcc tye dentty: mn a nm = r αmn 5 6, ṡ rmn ẋ r + α= β= + <mn> + mn Γ 5 and 6 are gven by 57, 58. u a r r u t t v mn = α= β= α<β v + α= β= α<β Γ [m Γ [t α m Γ r β n ] Γ tα t β n] t β. mn α= β= 59 + Γ mn, Γ Γ [m t β n] r α In the next dfference we got: a j mn a j n m = mn a 7 j 8 jmn a + a j<mn> a j mn + a,ṡ rmn ẋ r M mna j, 6 7 mn = Γ m,n Γ n,m + Γ mγ n Γ n Γ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ, 6 8 mn = Γ m,n Γ n,m + Γ mγ n Γ nγ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ. 63 Theorem.6. In GF N for h-dfferentaton, there the 6 th Rcc tye dentty: r αmn 7 mn a n m = α= β= 8 7 and 8 are gven by equaton 6, 63 and u a r r u t t v mn = α= β= α<β α= β= Γ [m] Γ r β n + Γ n Γ r β [m] r β Γ [m] Γ t β n + Γ n Γ [t β n], ṡ rmn ẋ r + <mn> + mn, v + α= β= α<β Γ [t α m] Γ t β n + Γ t α n Γ [t β n] tα.
9 7. Then, we condered the dfference: a j mn a j n m = 9 M. Cvetkovć, M. Zlatanovć / Flomat 8: 04, mn a j 0 jmn a + a j<nm> a j nm + a,ṡ rmn ẋ r Γ mna j + Γ nma j, 66 9 mn = Γ m,n Γ n,m + Γ mγ n Γ nγ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ, 67 0 mn = Γ m,n Γ n,m + Γ m Γ n Γ nγ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ. 68 Theorem.7. In GF N, for h-dfferentaton, the 7 th Rcc tye dentty vald: mn a n m = r αmn 9 0, ṡ rmn ẋ r + α= β= + <nm> + nm Γ 9 and 0 are gven by equaton 67, 68. mn Γ nm, nd, we condered the dfference: a j mn a j n m = mn a j jmn a a j<nm> + a j nm + a,ṡ rmn ẋ r + Γ mna j Γ nma j, 70 mn = Γ m,n Γ n,m + Γ m Γ n Γ n Γ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ, 7 mn = Γ m,n Γ n,m + Γ mγ n Γ n Γ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ. 7 Theorem.8. In GF N, for h-dfferentaton, there the 8 th Rcc tye dentty: mn a n m = r αmn, ṡ rmn ẋ r α= β= <nm> + mn + Γ mn and are gven by equaton 7, 7 and u a r r u t t v mn = α= β= α<β α= β= Γ mγ r β [n] + Γ [n] Γ r β m 9. In the next dfference, we got: a j mn a j n Γ Γ mγ [nt β ] + Γ [n] Γ mt β nm r β, m = mn a 3 j 4 jmn a a j<mn> + a j nm + a,ṡ v + α= β= α<β rmn ẋ r + M Γ mt α Γ [nt β ] + Γ [nt α ] Γ mt β nma j tα., 75 3 mn = Γ m,n Γ n,m + Γ m Γ n Γ nγ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ, 76 4 mn = Γ m,n Γ n,m + Γ m Γ n Γ n Γ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ. 77
10 M. Cvetkovć, M. Zlatanovć / Flomat 8: 04, Theorem.9. In GF N, for h-dfferentaton, there the 9 th Rcc tye dentty: mn a n m = α= 3 mn β= <mn> + nm + M 3 and 4 are gven by equaton 76, nma j, ṡ rmn ẋ r, t lat, we condered the dfference: a j m n a j n m = mn a 5 j 5 jmn a + a,ṡ rmn ẋ r + Γ nma j Γ nma j, 79 5 mn = Γ m,n Γ n,m + Γ m Γ n Γ nγ m Γ m,ṡ Gș ṅ + Γ n,ṡ Gș ṁ. 80 Theorem.0. In GF N, for h-dfferentaton, the 0 th Rcc tye dentty vald: m n a n m = α= 5 gven by equaton mn β= 5, ṡ rmn ẋ r Γ nm Γ nm, 8 The dentty.64 can be wrtten n another form: a r r u t t v m n ar r u t t v n m = α= 3 mn β= 3, ṡ rmn ẋ r, 3 jmn = 5 jmn + Γ nmt j = Γ jm,n Γ nj,m + Γ jm Γ n Γ nj Γ m + Γ nmγ j Γ j + +P jm,ṡ ξș n Γ nj,ṡ ξș m Concluon Baed on non-ymmetry of bac tenor n generalzed Fnler ace, ung h-dfferentaton, we defned two knd of covarant dervatve of a tenor n Rund ene and obtaned ten Rcc tye dentte, two new curvature tenor and ffteen magntude, we called eudotenor. art from attemt at a theoretcal unfcaton of gravtaton and electromagnetc henomena n a ngle geometrcal framework, Fnler ace were alo condered ether a formal rooton of new theoretcal tructure and feld equaton, or more drectly concerned wth exlorng oble obervatonal conequence. Fnler geometry doe have many feld of alcaton, bede geometrcal extenon of theore of gravty. lo, comuter algebra can be very helful to gve Fnler exreon from a choen metrc or connecton.
11 M. Cvetkovć, M. Zlatanovć / Flomat 8: 04, Reference [] S. Bochner,. Yano, Tenor-feld n non-ymmetrc connecton, nnal of mathematc, Vol.56, No [] E. Cartan, Le Eace de Fnler, Par, 934. [3]. Enten, generalzaton of the relatvtc theory of gravtaton, nnal of Mathematc, Vol.46, No [4] L. P. Eenhart, Generalzed Remannan Sace, Proceedng of the Natonal cademy of Scence of the Unted State of merca, Vol.37, No [5] P. Fnler, Uber urven und Flachen n llgemenen Raumen, Dertaton, Gottngen, 98. [6] S. Manoff, Devaton oerator and devaton equaton over ace wth affne connecton and metrc, Journal of Geometry and Phyc, Vol.39, No [7] S. M. Mnčć, Lj. S. Velmrovć, M. S. Stankovć, On ace wth non-ymmetrc affne connecton, contanng ubace wthout toron, led Mathematc and Comutaton 9 9 0/03, [8] S. M. Mnčć, M. Lj. Zlatanovć, New commutaton formula for δ-dfferentaton n a generalzed Fnler ace, Dfferental Geometry-Dynamcal Sytem, Vol [9] S. M. Mnčć, M. Lj. Zlatanovć, Commutaton formula for δ-dfferentaton n a generalzed Fnler ace, ragujevac Journal of Mathematc, Vol.35, No [0] S. M. Mnčć, M. Lj. Zlatanovć, Derved curvature tenor n generalzed Fnler ace, Dfferental Geometry-Dynamcal Sytem, Vol [] C.. Mhra, On C h Recurrent and C v -Recurrent Fnler Sace of Second Order, Int. J. Contem. Math. Scence, Vol.3, No [] R. B. Mra, Bac Concet of Fnleran Geometry, Internatonal Centre For Theoretcal Phc, Trete, Italy [3] C. Ntecu, Banch Identte n a Non-ymmetrc Connecton Sace, Bul. Int. Polteh. Ia N.S. 04, Fac. -, Sect. I [4] H. D. Pande,.. Guta, Banch Identte n a Fnler Sace wth Non-ymmetrc Connecton, Bulletn T. LXIV de l cademe erbe de Scence et de rt No [5] B. Remann, ber de Hyotheen, welche der Geometre zugrunde legen 854, Ge. Math. Werke,.7-87, Lezg 89, reroduced by Dover Publcaton 953. [6] H. Rund, The Dfferental Geometry of Fnler Sace, Mokow 98, n Ruan. [7]. C. Shamhoke, Note on a Curvature Tenor n a Generalzed Fnler Sace, Tenor, N.S [8] U. P. Sngh, On Relatve Curvature Tenor n the Subace of a Remannan Sace, Unverty of Itanbul Faculty of Scence the Journal of Mathematc, Phyc and tronomy Vol [9] U. P. Sngh, On Relatve Gau Charactertc Equaton and Relatve Rcc Prncal Drecton of a Remannan Hyerurface, Unverdad Naconal de Tucumn, Sere, Matemtca y fca terca, Vol [0] M. S. Stankovć, S. M. Mnčć, Lj. S. Velmrovć, On equtoron holomorhcally rojectve mang of generalzed ahleran ace, Czecholovak Mathematcal Journal 54 9, 004, No.3, [] Lj. S. Velmrovć, S. M. Mnčć, M. S. Stankovć, Infntemal rgdty and flexblty of a non-ymmetrc affne connecton ace, Eur. J. Comb , [] N. L. Youef,. M. hmed, Lnear connecton and curvature tenor n the geometry of arallelzable manfold, Reort on mathematcal hyc, Vol.60, No [3] M. Lj. Zlatanovć, S. M. Mnčć, Identte for curvature tenor n generalzed Fnler ace, Flomat, Vol.3, No [4] M. Lj. Zlatanovć, S. M. Mnčć, Banch tye dentte n Generalzed Fnler Sace, Hyercomlex Number n geometry and Phyc 4, Vol
RICCI TYPE IDENTITIES FOR BASIC DIFFERENTIATION AND CURVATURE TENSORS IN OTSUKI SPACES 1
wnov Sad J. Math. wvol., No., 00, 7-87 7 RICCI TYPE IDENTITIES FOR BASIC DIFFERENTIATION AND CURVATURE TENSORS IN OTSUKI SPACES Svetlav M. Mnčć Abtract. In the Otuk ace ue made of two non-ymmetrc affne
More informationApplied Mathematics Letters. On equitorsion geodesic mappings of general affine connection spaces onto generalized Riemannian spaces
Appled Mathematcs Letters (0) 665 67 Contents lsts avalable at ScenceDrect Appled Mathematcs Letters journal homepage: www.elsever.com/locate/aml On equtorson geodesc mappngs of general affne connecton
More informationGeodesic mappings of equiaffine and anti-equiaffine general affine connection spaces preserving torsion
Flomat 6: (0) 9 DOI 0.98/FIL09S Publshed by Faculty of Scences and Mathematcs Unversty of Nš Serba Avalable at: http://www.pmf.n.ac.rs/flomat Geodesc mappngs of equaffne and ant-equaffne general affne
More informationInfinitesimal Rigidity and Flexibility at Non Symmetric Affine Connection Space
ESI The Erwn Schrödnger Internatonal Boltzmanngasse 9 Insttute for Mathematcal Physcs A-9 Wen, Austra Infntesmal Rgdty and Flexblty at Non Symmetrc Affne Connecton Sace Ljubca S. Velmrovć Svetslav M. Mnčć
More informationChapter 6 The Effect of the GPS Systematic Errors on Deformation Parameters
Chapter 6 The Effect of the GPS Sytematc Error on Deformaton Parameter 6.. General Beutler et al., (988) dd the frt comprehenve tudy on the GPS ytematc error. Baed on a geometrc approach and aumng a unform
More informationUNIT 7. THE FUNDAMENTAL EQUATIONS OF HYPERSURFACE THEORY
UNIT 7. THE FUNDAMENTAL EQUATIONS OF HYPERSURFACE THEORY ================================================================================================================================================================================================================================================
More information2-π STRUCTURES ASSOCIATED TO THE LAGRANGIAN MECHANICAL SYSTEMS UDC 531.3: (045)=111. Victor Blãnuţã, Manuela Gîrţu
FACTA UNIVERSITATIS Seres: Mechancs Automatc Control and Robotcs Vol. 6 N o 1 007 pp. 89-95 -π STRUCTURES ASSOCIATED TO THE LAGRANGIAN MECHANICAL SYSTEMS UDC 531.3:53.511(045)=111 Vctor Blãnuţã Manuela
More informationRICCI COEFFICIENTS OF ROTATION OF GENERALIZED FINSLER SPACES
Mskolc Mathematcal Notes HU e-issn 787- Vol. 6 (05), No., pp. 05 09 DOI: 0.85/MMN.05.05 RICCI COEFFICIENTS OF ROTATION OF GENERALIZED FINSLER SPACES SVETISLAV M. MINČIĆ, MIĆA S. STANKOVIĆ, AND MILAN LJ.
More informationDesign of Recursive Digital Filters IIR
Degn of Recurve Dgtal Flter IIR The outut from a recurve dgtal flter deend on one or more revou outut value, a well a on nut t nvolve feedbac. A recurve flter ha an nfnte mule reone (IIR). The mulve reone
More informationBinomial transforms of the modified k-fibonacci-like sequence
Internatonal Journal of Mathematcs and Computer Scence, 14(2019, no. 1, 47 59 M CS Bnomal transforms of the modfed k-fbonacc-lke sequence Youngwoo Kwon Department of mathematcs Korea Unversty Seoul, Republc
More informationAffine and Riemannian Connections
Affne and Remannan Connectons Semnar Remannan Geometry Summer Term 2015 Prof Dr Anna Wenhard and Dr Gye-Seon Lee Jakob Ullmann Notaton: X(M) space of smooth vector felds on M D(M) space of smooth functons
More informationRanders Space with Special Nonlinear Connection
ISSN 1995-0802, obachevsk Journal of Mathematcs, 2008, Vol. 29, No. 1, pp. 27 31. c Pleades Publshng, td., 2008. Rers Space wth Specal Nonlnear Connecton H. G. Nagaraja * (submtted by M.A. Malakhaltsev)
More informationCausal Diamonds. M. Aghili, L. Bombelli, B. Pilgrim
Causal Damonds M. Aghl, L. Bombell, B. Plgrm Introducton The correcton to volume of a causal nterval due to curvature of spacetme has been done by Myrhem [] and recently by Gbbons & Solodukhn [] and later
More informationSOME RESULTS ON TRANSFORMATIONS GROUPS OF N-LINEAR CONNECTIONS IN THE 2-TANGENT BUNDLE
STUDIA UNIV. BABEŞ BOLYAI MATHEMATICA Volume LIII Number March 008 SOME RESULTS ON TRANSFORMATIONS GROUPS OF N-LINEAR CONNECTIONS IN THE -TANGENT BUNDLE GHEORGHE ATANASIU AND MONICA PURCARU Abstract. In
More informationProjective change between two Special (α, β)- Finsler Metrics
Internatonal Journal of Trend n Research and Development, Volume 2(6), ISSN 2394-9333 www.jtrd.com Projectve change between two Specal (, β)- Fnsler Metrcs Gayathr.K 1 and Narasmhamurthy.S.K 2 1 Assstant
More informationImprovements on Waring s Problem
Imrovement on Warng Problem L An-Png Bejng 85, PR Chna al@nacom Abtract By a new recurve algorthm for the auxlary equaton, n th aer, we wll gve ome mrovement for Warng roblem Keyword: Warng Problem, Hardy-Lttlewood
More informationScattering of two identical particles in the center-of. of-mass frame. (b)
Lecture # November 5 Scatterng of two dentcal partcle Relatvtc Quantum Mechanc: The Klen-Gordon equaton Interpretaton of the Klen-Gordon equaton The Drac equaton Drac repreentaton for the matrce α and
More informationarxiv: v1 [math.ho] 18 May 2008
Recurrence Formulas for Fbonacc Sums Adlson J. V. Brandão, João L. Martns 2 arxv:0805.2707v [math.ho] 8 May 2008 Abstract. In ths artcle we present a new recurrence formula for a fnte sum nvolvng the Fbonacc
More informationCONDITIONS FOR INVARIANT SUBMANIFOLD OF A MANIFOLD WITH THE (ϕ, ξ, η, G)-STRUCTURE. Jovanka Nikić
147 Kragujevac J. Math. 25 (2003) 147 154. CONDITIONS FOR INVARIANT SUBMANIFOLD OF A MANIFOLD WITH THE (ϕ, ξ, η, G)-STRUCTURE Jovanka Nkć Faculty of Techncal Scences, Unversty of Nov Sad, Trg Dosteja Obradovća
More informationBULLETIN OF MATHEMATICS AND STATISTICS RESEARCH
Vol.6.Iue..8 (July-Set.) KY PUBLICATIONS BULLETIN OF MATHEMATICS AND STATISTICS RESEARCH A Peer Revewed Internatonal Reearch Journal htt:www.bor.co Eal:edtorbor@gal.co RESEARCH ARTICLE A GENERALISED NEGATIVE
More informationA Simple Proof of Sylvester s (Determinants) Identity
Appled Mathematcal Scences, Vol 2, 2008, no 32, 1571-1580 A Smple Proof of Sylvester s (Determnants) Identty Abdelmalek Salem Department of Mathematcs and Informatques, Unversty Centre Chekh Larb Tebess
More informationTensor Analysis. For orthogonal curvilinear coordinates, ˆ ˆ (98) Expanding the derivative, we have, ˆ. h q. . h q h q
For orthogonal curvlnear coordnates, eˆ grad a a= ( aˆ ˆ e). h q (98) Expandng the dervatve, we have, eˆ aˆ ˆ e a= ˆ ˆ a h e + q q 1 aˆ ˆ ˆ a e = ee ˆˆ ˆ + e. h q h q Now expandng eˆ / q (some of the detals
More informationPHYS 705: Classical Mechanics. Calculus of Variations II
1 PHYS 705: Classcal Mechancs Calculus of Varatons II 2 Calculus of Varatons: Generalzaton (no constrant yet) Suppose now that F depends on several dependent varables : We need to fnd such that has a statonary
More informationNMT EE 589 & UNM ME 482/582 ROBOT ENGINEERING. Dr. Stephen Bruder NMT EE 589 & UNM ME 482/582
NMT EE 589 & UNM ME 48/58 ROBOT ENGINEERING Dr. Stephen Bruder NMT EE 589 & UNM ME 48/58 7. Robot Dynamcs 7.5 The Equatons of Moton Gven that we wsh to fnd the path q(t (n jont space) whch mnmzes the energy
More informationMA 323 Geometric Modelling Course Notes: Day 13 Bezier Curves & Bernstein Polynomials
MA 323 Geometrc Modellng Course Notes: Day 13 Bezer Curves & Bernsten Polynomals Davd L. Fnn Over the past few days, we have looked at de Casteljau s algorthm for generatng a polynomal curve, and we have
More informationWeak McCoy Ore Extensions
Internatonal Mathematcal Forum, Vol. 6, 2, no. 2, 75-86 Weak McCoy Ore Extenon R. Mohammad, A. Mouav and M. Zahr Department of Pure Mathematc, Faculty of Mathematcal Scence Tarbat Modare Unverty, P.O.
More informationSpecification -- Assumptions of the Simple Classical Linear Regression Model (CLRM) 1. Introduction
ECONOMICS 35* -- NOTE ECON 35* -- NOTE Specfcaton -- Aumpton of the Smple Clacal Lnear Regreon Model (CLRM). Introducton CLRM tand for the Clacal Lnear Regreon Model. The CLRM alo known a the tandard lnear
More informationThe Jacobsthal and Jacobsthal-Lucas Numbers via Square Roots of Matrices
Internatonal Mathematcal Forum, Vol 11, 2016, no 11, 513-520 HIKARI Ltd, wwwm-hkarcom http://dxdoorg/1012988/mf20166442 The Jacobsthal and Jacobsthal-Lucas Numbers va Square Roots of Matrces Saadet Arslan
More informationThe multivariate Gaussian probability density function for random vector X (X 1,,X ) T. diagonal term of, denoted
Appendx Proof of heorem he multvarate Gauan probablty denty functon for random vector X (X,,X ) px exp / / x x mean and varance equal to the th dagonal term of, denoted he margnal dtrbuton of X Gauan wth
More informationPower-sum problem, Bernoulli Numbers and Bernoulli Polynomials.
Power-sum roblem, Bernoull Numbers and Bernoull Polynomals. Arady M. Alt Defnton 1 Power um Problem Fnd the sum n : 1... n where, n N or, usng sum notaton, n n n closed form. Recurrence for n Exercse Usng
More information9 Characteristic classes
THEODORE VORONOV DIFFERENTIAL GEOMETRY. Sprng 2009 [under constructon] 9 Characterstc classes 9.1 The frst Chern class of a lne bundle Consder a complex vector bundle E B of rank p. We shall construct
More informationFrom Biot-Savart Law to Divergence of B (1)
From Bot-Savart Law to Dvergence of B (1) Let s prove that Bot-Savart gves us B (r ) = 0 for an arbtrary current densty. Frst take the dvergence of both sdes of Bot-Savart. The dervatve s wth respect to
More informationENERGY-DEPENDENT MINKOWSKI METRIC IN SPACE-TIME
ENERGY-DEPENDENT MINKOWSKI METRIC IN SPACE-TIME R. Mron, A. Jannusss and G. Zet Abstract The geometrcal propertes of the space-tme endowed wth a metrc dependng on the energy E of the consdered process
More informationNATURAL 2-π STRUCTURES IN LAGRANGE SPACES
AALELE ŞTIIŢIFICE ALE UIVERSITĂŢII AL.I. CUZA DI IAŞI (S.. MATEMATICĂ, Tomul LIII, 2007, Suplment ATURAL 2-π STRUCTURES I LAGRAGE SPACES Y VICTOR LĂUŢA AD VALER IMIEŢ Dedcated to Academcan Radu Mron at
More informationHarmonic oscillator approximation
armonc ocllator approxmaton armonc ocllator approxmaton Euaton to be olved We are fndng a mnmum of the functon under the retrcton where W P, P,..., P, Q, Q,..., Q P, P,..., P, Q, Q,..., Q lnwgner functon
More informationDeterminants Containing Powers of Generalized Fibonacci Numbers
1 2 3 47 6 23 11 Journal of Integer Sequences, Vol 19 (2016), Artcle 1671 Determnants Contanng Powers of Generalzed Fbonacc Numbers Aram Tangboonduangjt and Thotsaporn Thanatpanonda Mahdol Unversty Internatonal
More informationA Fuzzy Optimization Method for Multi-criteria Decisionmaking Problem Based on the Inclusion Degrees of Intuitionistic Fuzzy Sets
SSN 746-7659 England UK Journal of nformaton and omutng Scence Vol. No. 008. 46-5 Fuzzy Otmzaton ethod for ult-crtera Deconmang Problem aed on the ncluon Degree of ntutontc Fuzzy Set Yan Luo and hangru
More informationOn Finite Rank Perturbation of Diagonalizable Operators
Functonal Analyss, Approxmaton and Computaton 6 (1) (2014), 49 53 Publshed by Faculty of Scences and Mathematcs, Unversty of Nš, Serba Avalable at: http://wwwpmfnacrs/faac On Fnte Rank Perturbaton of Dagonalzable
More informationarxiv: v1 [gr-qc] 31 Oct 2007
Covarant Theory of Gravtaton n the Spacetme wth nsler Structure Xn-Bng Huang Shangha Unted Center for Astrophyscs (SUCA), arxv:0710.5803v1 [gr-qc] 31 Oct 2007 Shangha Normal Unversty, No.100 Guln Road,
More informationBeyond Zudilin s Conjectured q-analog of Schmidt s problem
Beyond Zudln s Conectured q-analog of Schmdt s problem Thotsaporn Ae Thanatpanonda thotsaporn@gmalcom Mathematcs Subect Classfcaton: 11B65 33B99 Abstract Usng the methodology of (rgorous expermental mathematcs
More informationDifferential Polynomials
JASS 07 - Polynomals: Ther Power and How to Use Them Dfferental Polynomals Stephan Rtscher March 18, 2007 Abstract Ths artcle gves an bref ntroducton nto dfferental polynomals, deals and manfolds and ther
More informationIterative Methods for Searching Optimal Classifier Combination Function
htt://www.cub.buffalo.edu Iteratve Method for Searchng Otmal Clafer Combnaton Functon Sergey Tulyakov Chaohong Wu Venu Govndaraju Unverty at Buffalo Identfcaton ytem: Alce Bob htt://www.cub.buffalo.edu
More informationThe binomial transforms of the generalized (s, t )-Jacobsthal matrix sequence
Int. J. Adv. Appl. Math. and Mech. 6(3 (2019 14 20 (ISSN: 2347-2529 Journal homepage: www.jaamm.com IJAAMM Internatonal Journal of Advances n Appled Mathematcs and Mechancs The bnomal transforms of the
More informationONE EXPRESSION FOR THE SOLUTIONS OF SECOND ORDER DIFFERENCE EQUATIONS JERZY POPENDA
proceedngs of the amercan mathematcal socety Volume 100, Number 1, May 1987 ONE EXPRESSION FOR THE SOLUTIONS OF SECOND ORDER DIFFERENCE EQUATIONS JERZY POPENDA ABSTRACT. Explct formulas for the general
More informationThree views of mechanics
Three vews of mechancs John Hubbard, n L. Gross s course February 1, 211 1 Introducton A mechancal system s manfold wth a Remannan metrc K : T M R called knetc energy and a functon V : M R called potental
More informationSome congruences related to harmonic numbers and the terms of the second order sequences
Mathematca Moravca Vol. 0: 06, 3 37 Some congruences related to harmonc numbers the terms of the second order sequences Neşe Ömür Sbel Koaral Abstract. In ths aer, wth hels of some combnatoral denttes,
More informationLecture 13 APPROXIMATION OF SECOMD ORDER DERIVATIVES
COMPUTATIONAL FLUID DYNAMICS: FDM: Appromaton of Second Order Dervatves Lecture APPROXIMATION OF SECOMD ORDER DERIVATIVES. APPROXIMATION OF SECOND ORDER DERIVATIVES Second order dervatves appear n dffusve
More informationBezier curves. Michael S. Floater. August 25, These notes provide an introduction to Bezier curves. i=0
Bezer curves Mchael S. Floater August 25, 211 These notes provde an ntroducton to Bezer curves. 1 Bernsten polynomals Recall that a real polynomal of a real varable x R, wth degree n, s a functon of the
More informationSmall signal analysis
Small gnal analy. ntroducton Let u conder the crcut hown n Fg., where the nonlnear retor decrbed by the equaton g v havng graphcal repreentaton hown n Fg.. ( G (t G v(t v Fg. Fg. a D current ource wherea
More informationVariable Structure Control ~ Basics
Varable Structure Control ~ Bac Harry G. Kwatny Department of Mechancal Engneerng & Mechanc Drexel Unverty Outlne A prelmnary example VS ytem, ldng mode, reachng Bac of dcontnuou ytem Example: underea
More informationTANGENT DIRAC STRUCTURES OF HIGHER ORDER. P. M. Kouotchop Wamba, A. Ntyam, and J. Wouafo Kamga
ARCHIVUM MATHEMATICUM BRNO) Tomus 47 2011), 17 22 TANGENT DIRAC STRUCTURES OF HIGHER ORDER P. M. Kouotchop Wamba, A. Ntyam, and J. Wouafo Kamga Abstract. Let L be an almost Drac structure on a manfold
More informationABOUT THE GROUP OF TRANSFORMATIONS OF METRICAL SEMISYMMETRIC N LINEAR CONNECTIONS ON A GENERALIZED HAMILTON SPACE OF ORDER TWO
Bulletn of the Translvana Unversty of Braşov Vol 554 No. 2-202 Seres III: Mathematcs Informatcs Physcs 75-88 ABOUT THE GROUP OF TRANSFORMATIONS OF METRICAL SEMISYMMETRIC N LINEAR CONNECTIONS ON A GENERALIZED
More informationUsing T.O.M to Estimate Parameter of distributions that have not Single Exponential Family
IOSR Journal of Mathematcs IOSR-JM) ISSN: 2278-5728. Volume 3, Issue 3 Sep-Oct. 202), PP 44-48 www.osrjournals.org Usng T.O.M to Estmate Parameter of dstrbutons that have not Sngle Exponental Famly Jubran
More informationRandić Energy and Randić Estrada Index of a Graph
EUROPEAN JOURNAL OF PURE AND APPLIED MATHEMATICS Vol. 5, No., 202, 88-96 ISSN 307-5543 www.ejpam.com SPECIAL ISSUE FOR THE INTERNATIONAL CONFERENCE ON APPLIED ANALYSIS AND ALGEBRA 29 JUNE -02JULY 20, ISTANBUL
More informationRoot Locus Techniques
Root Locu Technque ELEC 32 Cloed-Loop Control The control nput u t ynthezed baed on the a pror knowledge of the ytem plant, the reference nput r t, and the error gnal, e t The control ytem meaure the output,
More informationChapter 11. Supplemental Text Material. The method of steepest ascent can be derived as follows. Suppose that we have fit a firstorder
S-. The Method of Steepet cent Chapter. Supplemental Text Materal The method of teepet acent can be derved a follow. Suppoe that we have ft a frtorder model y = β + β x and we wh to ue th model to determne
More informationAdditional File 1 - Detailed explanation of the expression level CPD
Addtonal Fle - Detaled explanaton of the expreon level CPD A mentoned n the man text, the man CPD for the uterng model cont of two ndvdual factor: P( level gen P( level gen P ( level gen 2 (.).. CPD factor
More information1 Matrix representations of canonical matrices
1 Matrx representatons of canoncal matrces 2-d rotaton around the orgn: ( ) cos θ sn θ R 0 = sn θ cos θ 3-d rotaton around the x-axs: R x = 1 0 0 0 cos θ sn θ 0 sn θ cos θ 3-d rotaton around the y-axs:
More informationLinear, affine, and convex sets and hulls In the sequel, unless otherwise specified, X will denote a real vector space.
Lnear, affne, and convex sets and hulls In the sequel, unless otherwse specfed, X wll denote a real vector space. Lnes and segments. Gven two ponts x, y X, we defne xy = {x + t(y x) : t R} = {(1 t)x +
More informationVanishing S-curvature of Randers spaces
Vanshng S-curvature of Randers spaces Shn-ch OHTA Department of Mathematcs, Faculty of Scence, Kyoto Unversty, Kyoto 606-850, JAPAN (e-mal: sohta@math.kyoto-u.ac.jp) December 31, 010 Abstract We gve a
More informationDifferentiating Gaussian Processes
Dfferentatng Gaussan Processes Andrew McHutchon Aprl 17, 013 1 Frst Order Dervatve of the Posteror Mean The posteror mean of a GP s gven by, f = x, X KX, X 1 y x, X α 1 Only the x, X term depends on the
More informationThe internal structure of natural numbers and one method for the definition of large prime numbers
The nternal structure of natural numbers and one method for the defnton of large prme numbers Emmanul Manousos APM Insttute for the Advancement of Physcs and Mathematcs 3 Poulou str. 53 Athens Greece Abstract
More informationIntroduction to Interfacial Segregation. Xiaozhe Zhang 10/02/2015
Introducton to Interfacal Segregaton Xaozhe Zhang 10/02/2015 Interfacal egregaton Segregaton n materal refer to the enrchment of a materal conttuent at a free urface or an nternal nterface of a materal.
More informationGEOMETRIC INTERPRETATIONS OF CURVATURE. Contents 1. Notation and Summation Conventions 1
GEOMETRIC INTERPRETATIONS OF CURVATURE ZHENGQU WAN Abstract. Ths s an exostory aer on geometrc meanng of varous knds of curvature on a Remann manfold. Contents 1. Notaton and Summaton Conventons 1 2. Affne
More informationCALCULUS CLASSROOM CAPSULES
CALCULUS CLASSROOM CAPSULES SESSION S86 Dr. Sham Alfred Rartan Valley Communty College salfred@rartanval.edu 38th AMATYC Annual Conference Jacksonvlle, Florda November 8-, 202 2 Calculus Classroom Capsules
More informationModelli Clamfim Equazione del Calore Lezione ottobre 2014
CLAMFIM Bologna Modell 1 @ Clamfm Equazone del Calore Lezone 17 15 ottobre 2014 professor Danele Rtell danele.rtell@unbo.t 1/24? Convoluton The convoluton of two functons g(t) and f(t) s the functon (g
More informationSpecial Relativity and Riemannian Geometry. Department of Mathematical Sciences
Tutoral Letter 06//018 Specal Relatvty and Reannan Geoetry APM3713 Seester Departent of Matheatcal Scences IMPORTANT INFORMATION: Ths tutoral letter contans the solutons to Assgnent 06. BAR CODE Learn
More information(δr i ) 2. V i. r i 2,
Cartesan coordnates r, = 1, 2,... D for Eucldean space. Dstance by Pythagoras: (δs 2 = (δr 2. Unt vectors ê, dsplacement r = r ê Felds are functons of poston, or of r or of {r }. Scalar felds Φ( r, Vector
More informationNUMERICAL DIFFERENTIATION
NUMERICAL DIFFERENTIATION 1 Introducton Dfferentaton s a method to compute the rate at whch a dependent output y changes wth respect to the change n the ndependent nput x. Ths rate of change s called the
More informationarxiv: v1 [math.dg] 15 Jun 2007
arxv:0706.2313v1 [math.dg] 15 Jun 2007 Cohomology of dffeologcal spaces and folatons E. Macías-Vrgós; E. Sanmartín-Carbón Abstract Let (M, F) be a folated manfold. We study the relatonshp between the basc
More informationBernoulli Numbers and Polynomials
Bernoull Numbers and Polynomals T. Muthukumar tmk@tk.ac.n 17 Jun 2014 The sum of frst n natural numbers 1, 2, 3,..., n s n n(n + 1 S 1 (n := m = = n2 2 2 + n 2. Ths formula can be derved by notng that
More informationPROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 125, Number 7, July 1997, Pages 2119{2125 S (97) THE STRONG OPEN SET CONDITION
PROCDINGS OF TH AMRICAN MATHMATICAL SOCITY Volume 125, Number 7, July 1997, Pages 2119{2125 S 0002-9939(97)03816-1 TH STRONG OPN ST CONDITION IN TH RANDOM CAS NORBRT PATZSCHK (Communcated by Palle. T.
More informationAGC Introduction
. Introducton AGC 3 The prmary controller response to a load/generaton mbalance results n generaton adjustment so as to mantan load/generaton balance. However, due to droop, t also results n a non-zero
More informationLecture 10 Support Vector Machines II
Lecture 10 Support Vector Machnes II 22 February 2016 Taylor B. Arnold Yale Statstcs STAT 365/665 1/28 Notes: Problem 3 s posted and due ths upcomng Frday There was an early bug n the fake-test data; fxed
More informationTransfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system
Transfer Functons Convenent representaton of a lnear, dynamc model. A transfer functon (TF) relates one nput and one output: x t X s y t system Y s The followng termnology s used: x y nput output forcng
More informationExtended Prigogine Theorem: Method for Universal Characterization of Complex System Evolution
Extended Prgogne Theorem: Method for Unveral Characterzaton of Complex Sytem Evoluton Sergey amenhchkov* Mocow State Unverty of M.V. Lomonoov, Phycal department, Rua, Mocow, Lennke Gory, 1/, 119991 Publhed
More informationarxiv: v1 [math.co] 12 Sep 2014
arxv:1409.3707v1 [math.co] 12 Sep 2014 On the bnomal sums of Horadam sequence Nazmye Ylmaz and Necat Taskara Department of Mathematcs, Scence Faculty, Selcuk Unversty, 42075, Campus, Konya, Turkey March
More informationPerfect Fluid Cosmological Model in the Frame Work Lyra s Manifold
Prespacetme Journal December 06 Volume 7 Issue 6 pp. 095-099 Pund, A. M. & Avachar, G.., Perfect Flud Cosmologcal Model n the Frame Work Lyra s Manfold Perfect Flud Cosmologcal Model n the Frame Work Lyra
More informationPhysics 5153 Classical Mechanics. D Alembert s Principle and The Lagrangian-1
P. Guterrez Physcs 5153 Classcal Mechancs D Alembert s Prncple and The Lagrangan 1 Introducton The prncple of vrtual work provdes a method of solvng problems of statc equlbrum wthout havng to consder the
More informationElectromagnetic scattering. Graduate Course Electrical Engineering (Communications) 1 st Semester, Sharif University of Technology
Electromagnetc catterng Graduate Coure Electrcal Engneerng (Communcaton) 1 t Semeter, 1390-1391 Sharf Unverty of Technology Content of lecture Lecture : Bac catterng parameter Formulaton of the problem
More informationOne-sided finite-difference approximations suitable for use with Richardson extrapolation
Journal of Computatonal Physcs 219 (2006) 13 20 Short note One-sded fnte-dfference approxmatons sutable for use wth Rchardson extrapolaton Kumar Rahul, S.N. Bhattacharyya * Department of Mechancal Engneerng,
More informationHomework & Solution. Contributors. Prof. Lee, Hyun Min. Particle Physics Winter School. Park, Ye
Homework & Soluton Prof. Lee, Hyun Mn Contrbutors Park, Ye J(yej.park@yonse.ac.kr) Lee, Sung Mook(smlngsm0919@gmal.com) Cheong, Dhong Yeon(dhongyeoncheong@gmal.com) Ban, Ka Young(ban94gy@yonse.ac.kr) Ro,
More informationOn the U-WPF Acts over Monoids
Journal of cence, Ilamc Republc of Iran 8(4): 33-38 (007) Unverty of Tehran, IN 06-04 http://jcence.ut.ac.r On the U-WPF ct over Monod. Golchn * and H. Mohammadzadeh Department of Mathematc, Unverty of
More informationImprovements on Waring s Problem
Improvement on Warng Problem L An-Png Bejng, PR Chna apl@nacom Abtract By a new recurve algorthm for the auxlary equaton, n th paper, we wll gve ome mprovement for Warng problem Keyword: Warng Problem,
More informationBy Samuel Schechter. (1) H = i-î -1 with 1 ^ i,j g n. [a, b,j
On tne Inverson of Certan Matrces By Samuel Schechter 1. Introducton. Let a, a2,, an ; 61, 62,, 6 be 2n dstnct, but otherwse arbtrary, complex numbers. For the matrx H, of order n, (1) H = -î -1 wth 1
More informationLorentz Group. Ling Fong Li. 1 Lorentz group Generators Simple representations... 3
Lorentz Group Lng Fong L ontents Lorentz group. Generators............................................. Smple representatons..................................... 3 Lorentz group In the dervaton of Drac
More informationSupplementary Material for Spectral Clustering based on the graph p-laplacian
Sulementary Materal for Sectral Clusterng based on the grah -Lalacan Thomas Bühler and Matthas Hen Saarland Unversty, Saarbrücken, Germany {tb,hen}@csun-sbde May 009 Corrected verson, June 00 Abstract
More informationAPPENDIX A Some Linear Algebra
APPENDIX A Some Lnear Algebra The collecton of m, n matrces A.1 Matrces a 1,1,..., a 1,n A = a m,1,..., a m,n wth real elements a,j s denoted by R m,n. If n = 1 then A s called a column vector. Smlarly,
More informationUncertainty in measurements of power and energy on power networks
Uncertanty n measurements of power and energy on power networks E. Manov, N. Kolev Department of Measurement and Instrumentaton, Techncal Unversty Sofa, bul. Klment Ohrdsk No8, bl., 000 Sofa, Bulgara Tel./fax:
More informationActa Mathematica Academiae Paedagogicae Nyíregyháziensis 24 (2008), ISSN
Acta Mathematca Academae Paedagogcae Nyíregyházenss 24 (2008), 65 74 www.ems.de/journals ISSN 1786-0091 ON THE RHEONOMIC FINSLERIAN MECHANICAL SYSTEMS CAMELIA FRIGIOIU Abstract. In ths paper t wll be studed
More informationSolutions to Exercises in Astrophysical Gas Dynamics
1 Solutons to Exercses n Astrophyscal Gas Dynamcs 1. (a). Snce u 1, v are vectors then, under an orthogonal transformaton, u = a j u j v = a k u k Therefore, u v = a j a k u j v k = δ jk u j v k = u j
More informationand decompose in cycles of length two
Permutaton of Proceedng of the Natona Conference On Undergraduate Reearch (NCUR) 006 Domncan Unverty of Caforna San Rafae, Caforna Apr - 4, 007 that are gven by bnoma and decompoe n cyce of ength two Yeena
More informationM-LINEAR CONNECTION ON THE SECOND ORDER REONOM BUNDLE
STUDIA UNIV. AEŞ OLYAI, MATHEMATICA, Volume XLVI, Number 3, September 001 M-LINEAR CONNECTION ON THE SECOND ORDER REONOM UNDLE VASILE LAZAR Abstract. The T M R bundle represents the total space of a tme
More informationOn the correction of the h-index for career length
1 On the correcton of the h-ndex for career length by L. Egghe Unverstet Hasselt (UHasselt), Campus Depenbeek, Agoralaan, B-3590 Depenbeek, Belgum 1 and Unverstet Antwerpen (UA), IBW, Stadscampus, Venusstraat
More informationSMARANDACHE-GALOIS FIELDS
SMARANDACHE-GALOIS FIELDS W. B. Vasantha Kandasamy Deartment of Mathematcs Indan Insttute of Technology, Madras Chenna - 600 036, Inda. E-mal: vasantak@md3.vsnl.net.n Abstract: In ths aer we study the
More informationA Result on a Cyclic Polynomials
Gen. Math. Note, Vol. 6, No., Feruary 05, pp. 59-65 ISSN 9-78 Copyrght ICSRS Pulcaton, 05.-cr.org Avalale free onlne at http:.geman.n A Reult on a Cyclc Polynomal S.A. Wahd Department of Mathematc & Stattc
More informationare called the contravariant components of the vector a and the a i are called the covariant components of the vector a.
Non-Cartesan Coordnates The poston of an arbtrary pont P n space may be expressed n terms of the three curvlnear coordnates u 1,u,u 3. If r(u 1,u,u 3 ) s the poston vector of the pont P, at every such
More informationALGORITHM FOR THE CALCULATION OF THE TWO VARIABLES CUBIC SPLINE FUNCTION
ANALELE ŞTIINŢIFICE ALE UNIVERSITĂŢII AL.I. CUZA DIN IAŞI (S.N.) MATEMATICĂ, Tomul LIX, 013, f.1 DOI: 10.478/v10157-01-00-y ALGORITHM FOR THE CALCULATION OF THE TWO VARIABLES CUBIC SPLINE FUNCTION BY ION
More informationA new Approach for Solving Linear Ordinary Differential Equations
, ISSN 974-57X (Onlne), ISSN 974-5718 (Prnt), Vol. ; Issue No. 1; Year 14, Copyrght 13-14 by CESER PUBLICATIONS A new Approach for Solvng Lnear Ordnary Dfferental Equatons Fawz Abdelwahd Department of
More informationFinslerian Nonholonomic Frame For Matsumoto (α,β)-metric
Internatonal Journal of Mathematcs and Statstcs Inventon (IJMSI) E-ISSN: 2321 4767 P-ISSN: 2321-4759 ǁ Volume 2 ǁ Issue 3 ǁ March 2014 ǁ PP-73-77 Fnsleran Nonholonomc Frame For Matsumoto (α,)-metrc Mallkarjuna
More information