Cheeger Gromoll type metrics on the tangent bundle
|
|
- Verity Holland
- 5 years ago
- Views:
Transcription
1 Cheege Gomoll type metics on the tngent bundle Min Ion MUNTEANU Abstct In this ppe we study Riemnin metic on the tngent bundle T M) of Riemnnin mnifold M which genelizes the Cheege Gomoll metic nd comptible lmost complex stuctue which togethe with the metic confes to T M) stuctue of loclly confoml lmost Kählein mnifold. We found conditions unde which T M) is lmost Kählein, loclly confoml Kählein o Kählein o when T M) hs constnt sectionl cuvtue o constnt scl cuvtue MSC: 53B35, 53C07, 53C25, 53C55. Key wods: Riemnnin mnifold, Sski metic, Cheege Gomoll metic, tngent bundle, loclly confoml lmost) Kählein mnifold. 1 Peliminies Given Riemnnin mnifold M, g) one cn define sevel Riemnnin metics on the tngent bundle T M) of M. Mybe the best known exmple is the Sski metic g S intoduced in [20]. Although the Sski metic is ntully defined, it is vey igid. Fo exmple, the Sski metic is not, genelly, Einstein. O, the tngent bundle T M) with the Sski metic is neve loclly symmetic unless the metic g on the bse mnifold is flt see [12]). E.Musso & F.Ticei [15] hve poved tht the Sski metic hs constnt scl cuvtue if nd only if M, g) is loclly Euclidin. In the sme ppe, they hve given n explicit expession of positive definite Riemnnin metic intoduced by J.Cheege nd D.Gomoll in [9] nd clled this metic the Cheege-Gomoll metic. M.Sekizw see [21]), computed geometic objects elted to this metic. Lte, S.Gudmundson nd E.Kppos in [11], hve completed these esults nd hve shown tht the scl cuvtue of the Cheege Gomoll metic is neve constnt if the metic on the bse mnifold hs constnt sectionl cuvtue. Futhemoe, M.T.K.Abbssi & M.Sih hve poved tht T M) with the Cheege Gomoll metic is neve spce of constnt sectionl cuvtue cf. [2]). It is lso known tht the tngent bundle T M) of Riemnnin mnifold M, g) cn be ognized s n lmost Kählein mnifold see [10]) by using the decomposition of the tngent bundle to T M) into the veticl nd hoizontl distibutions, V T M nd HT M espectively the lst one being defined by the Levi Civit connection on M), the Sski metic nd n lmost complex stuctue defined by the bove splitting. A moe genel metic is given by M.Anstsiei in [6] which genelizes both of the Sski nd Cheege Gomoll metics: it peseves the othogonlity of the veticl 1
2 2 nd hoizontl distibutions, on the hoizontl distibution it is the sme s on the bse mnifold, nd finlly the Sski nd the Cheege Gomoll metic cn be obtined s pticul cses of this metic. A comptible lmost complex stuctue is lso intoduced nd hence T M) becomes loclly confoml lmost Kähein mnifold. On the othe hnd, V.Opoiu nd his collbotos constucted fmily of Riemnnin metics on the tngent bundles of Riemnnin mnifolds which possess inteesting geometic popeties cf. [16, 17, 18, 19]) fo exmple, the scl cuvtue of T M) cn be constnt lso fo non-flt bse mnifold with constnt sectionl cuvtue). Then M.T.K.Abbssi & M.Sih poved in [3] tht the consideed metics by Opoiu fom pticul subclss of the so-clled g-ntul metics on the tngent bundle see lso [1, 3, 4, 5, 13]). In this ppe we descibed fmily g of Riemnnin metics of Cheege Gomoll type, on the tngent bundle T M) of the Riemnnin mnifold M, g) nd comptible lmost complex stuctue J which bestow to T M) stuctue of loclly confoml lmost Kählein mnifold. We found n lmost Kählein stuctue on T M) nd we poved tht thee is no Cheege Gomoll type stuctue on T M) such tht the mnifold T M), g, J ) is Kählein. We studied the possibility fo the sectionl cuvtue on T M) to be constnt nd we found flt metic on T M) of couse of Cheege Gomoll type). Finlly, if M is el spce fom, we wee inteested to find when T M) endowed with the metic g hs constnt scl cuvtue. 2 On the Geomety of the Tngent Bundle T M) Let M, g) be Riemnnin mnifold nd let be its Levi Civit connection. Let τ : T M) M be the tngent bundle. If u T M) it is well known the following decomposition of the tngent spce T u T M) in u t T M)) T u T M) = V u T M) H u T M) whee V u T M) = ke τ,u is the veticl spce nd H u T M) is the hoizontl spce in u obtined by using. A cuve γ : I T M), t γt), V t)) is hoizontl if the vecto field V t) is pllel long γ = γ τ. A vecto on T M) is hoizontl if it is tngent to n hoizontl cuve nd veticl if it is tngent to fibe. Loclly, if U, x i ), i = 1,..., m, m = dim M, is locl cht in p M, conside τ 1 U), x i, y i ) locl cht on T M). If Γ k ij x) e the Chistoffel symbols, then δ i = x i Γ k ij x)yj in u, i = 1,..., m spn the spce H y k u T M), while y, i = 1,..., m spn i the veticl spce V u T M).) We hve obtined the hoizontl veticl) distibution HT M V T M) nd diect sum decomposition T T M = HT M V T M of the tngent bundle of T M). If X χm), denote by X H nd X V, espectively) the hoizontl lift nd the veticl lift, espectively) of X to T M). If u T M) then we conside the enegy density in u on T M), nmely t = 1 2 g τu)u, u).
3 3 2.1 The Cheege-Gomoll Stuctue The Cheege-Gomoll metic on T M) is given by g CGp,u) X H, Y H ) = g p X, Y ), g CGp,u) X H, Y V ) = 0 g CGp,u) X V, Y V ) = t g px, Y ) + g p X, u)g p Y, u)) 2.1) fo ny vectos X nd Y tngent to M. Moeove, n lmost complex stuctue J CG, comptible with the Chegee-Gomoll metic, cn be defined by the fomuls { JCG Xp,u) H = XV 1 1+ g px, u)u V J CG Xp,u) V = 1 XH 1 1+) g 2.2) px, u)u H whee = 1 + 2t nd X T p M). Remk tht J CG u H = u V nd J CG u V = u H. We get n lmost Hemitin mnifold T M), J CG, g CG ). If we denote by Ω CG the Kehle 2-fom nmely Ω CG U, V ) = g CG U, J CG V ), U, V χt M))) one cn pove the following Poposition 2.1 We hve whee ω Λ 1 T M)) is defined by ω p,u) X H ) = 0 nd ω p,u) X V ) = dω CG = ω Ω CG, 2.3) ) g p X, u), X T p M). 1 + Poof. A simple computtion gives the diffeentil of Ω CG : dω CG X H, Y H, Z H ) = dω CG X H, Y) H, Z V ) = dω CG X V, Y V, Z V ) = 0 dω CG X H, Y V, Z V ) = [gx, Y )gz, u) gx, Z)gY, u)] fo ny X, Y, Z χm). Hence the sttement. Remk 2.2 The lmost Hemitin mnifold T M), J CG, g CG ) is neve lmost Kehlein i.e. dω CG 0). Finlly, necessy condition fo the integbility of J CG is tht the bse mnifold M, g) is loclly Euclidin. 2.2 The Cheege Gomoll Type Stuctue A genel metic, let s cll it g, is in fct fmily of Riemnnin metics, depending on pmete, nd the Cheege-Gomoll metic is obtined by tking t) = 1 1+2t. It is defined by the following fomuls see lso [6]) g p,u) X H, Y H ) = g p X, Y ) g p,u) X H, Y V ) = 0 g p,u) X V, Y V ) = t) g p X, Y ) + g p X, u)g p Y, u) ), fo ll X, Y χm), whee : [0, + ) 0, + ). 2.4)
4 4 Poposition 2.3 see lso [14]) The metic defined bove cn be constuct by using the method descibed by Musso nd Ticei in [15]. We intend to find n lmost complex stuctue on T M), cll it J, comptible with the metic g. Inspied fom the pevious cses we look fo the lmost complex stuctue J in the following wy { J Xp,u) H = αxv + βg p X, u)u V J Xp,u) V = 2.5) γxh + ρg p X, u)u H whee X χm) nd α, β, γ nd ρ e smooth functions on T M) which will be detemined fom J 2 = I nd fom the comptibility conditions with the metic g. Following the computtions mde in [6] we get fist α = ± 1 nd γ =. Without lost of the genelity we cn tke α = 1 nd γ =. Then one ) obtins β = ) 2t + ɛ +2bt nd ρ = 1 2t + ɛ + 2bt whee ɛ = ±1. Remk 2.4 In this genel cse J is defined on T M) \ 0 the bundle of non zeo tngent vectos), but if we conside ɛ = 1 the pevious eltions define J on ll T M). Fom now on we will wok with ɛ = 1. We hve the lmost complex stuctue J J X H = 1 X V 1 J X V = ) 1+) gx, u)uv ) X H gx, u)uh. 2.6) One obtins n lmost Hemitin mnifold T M), g, J ). If we denote by Ω the Kähle 2-fom, Ω U, V ) = g U, J V ), U, V χt M)) one obtins Poposition 2.5 see lso [6]) The lmost Hemitin mnifold T M), g, J ) is loclly confoml lmost Kählein, tht is dω = ω Ω 2.7) whee ω is closed nd globlly defined 1 fom on T M) given by ωx H ) = 0 nd ωx V ) = 1 ) gx, u). 1 + As consequence one cn stte the following Theoem 2.6 The lmost Hemitin mnifold T M), g, J ) is lmost Kählein if nd only if t) = const e 1+2t t. 2.8) Poof. The esult is obtined by integting the eqution = We will tke ) = 2e 1 1+ if we sk 0) = 1.
5 5 2.3 The Integbility of J. In ode to hve n integble stuctue J on T M) we hve to compute the Nijenhuis tenso N J of J nd to sk tht it vnishes identiclly. Fo the integbility tenso N J we hve the following eltions N J X H, Y H ) ) = ) ) V gx, u)y gy, u)x + RXY u) V N J X V, Y V ) = R XY u 1+ gy, u)r Xuu + 1+ gx, u)r Y uu ) V gy, 2 1+) ) 1 V u)x gx, u)y. 2.9) The expession fo N J X H, Y V ) is vey complicted. Thus if J is integble then R XY u = ) ) gy, u)x gx, u)y ) fo evey X, Y χm) nd fo evey point u T M). It follows tht M is spce fom Mc) c is the constnt sectionl cuvtue of M). Consequently, ) = e ) ce 2 1) + k1 + )) with k positive el constnt nd c must be nonnegtive. Question: Cn T M), g, J ) be Kähle mnifold? If this hppens then we hve to find n ppopite constnt in 2.8) such tht the expession 2 1+) ) is lso constnt. Theoem 2.7 Thee is no Cheege Gomoll type stuctue on T M) such tht the mnifold T M), g, J ) is Kählein. Now we give Poposition 2.8 Let M, g) be Riemnnin mnifold nd let T M) be its tngent bundle equipped with the metic g. Then, the coesponding Levi Civit connection stisfies the following eltions: X H Y H = X Y ) H 1 2 R XY u) V X H Y V = X Y ) V + 2 R uy X) H X V Y H = 2 R uxy ) H 2.10) X Y V = L gx, u)y V + gy, u)x ) V + 1 L V 2 L gx, u)gy, u)u V, 2 gx, Y )u V whee L = t) 2t).
6 6 Poof. The sttement follows fom Koszul fomul mking usul computtions. Hving detemined Levi Civit connection, we cn compute now the Riemnnin cuvtue tenso R on T M). We give Poposition 2.9 The cuvtue tenso is given by R X H Y H Z H = R XY Z) H + 4 [R ur XZ uy R ury Z ux + 2R urxy uz] H [ ZR) XY u] V R X H Y Z V = [ R H XY Z + 4 R Y R uz Xu R XRuZ Y u) ] V + LgZ, u)rxy u) V L gr 2 XY u, Z)u V + 2 [ XR) uz Y Y R) uz X] H R X H Y Z H = V 2 [ XR) uy Z] H + [ RXZ Y 2 R XR uy Zu + LgY, u)r XZ u + 1 L gr 2 XZ u, Y )u ] V R X H Y Z V = V 2 R Y ZX) H 2 4 R uy R uz X) H + [ gz, u)ruy X) H gy, u)r uz X) H] + 4 R X V Y Z H = R V XY Z) H + 2 [gx, u)r uy Z gy, u)r ux Z] H [R uxr uy Z R uy R ux Z] H 2.11) R X V Y V Z V = F 1 t)gz, u) [ gx, u)y V gy, u)x V ] + +F 2 t) [ gx, Z)Y V gy, Z)X V ] + +F 3 t) [gx, Z)gY, u) gy, Z)gX, u)] u V, whee F 1 = L + L1 L), F 2 2 = L 2 1 L)2 nd F 2 3 = L L L 2. 4 In the following let Q U, V ) denote the sque of the e of the pllelogm with sides U nd V fo U, V χt M)), We hve Q U, V ) = g U, U)g V, V ) g U, V ) 2. Lemm 2.10 Let X, Y T p M be two othonoml vectos. Then { Q X H, Y H ) = 1, Q X H, Y V ) = t) 1 + gy, u) 2) Q X V, Y V ) = t) gx, u) 2 + gy, u) 2). 2.12) We compute now the sectionl cuvtue of the Riemnnin mnifold T M), g ), nmely K U, V ) = g R UV V,U) fo U, V χt M)). Q U,V ) Denote by T 0 M) = T M) \ 0 the tngent bundle of non-zeo vectos tngent to M. Fo given point p, u) T 0 M) conside n othonoml bsis {e i } i=1,m fo the tngent spce T p M) of M such tht e 1 = u u. Conside on T p,u)t M) the following vectos E i = e H i, i = 1, m, E m+1 = 1 ev 1, E m+k = 1 e V k, k = 2, m. 2.13)
7 7 It is esy to check tht {E 1,..., E 2m } is n othonoml bsis in T p,u) T M) with espect to the metic g ). We will wite the expessions of the sectionl cuvtue K in tems of this bsis. We hve K E i, E j ) = Ke i, e j ) 3t) 4 R eie j u 2, K E i, E m+1 ) = 0, K E i, E m+k ) = 1 4 R ue k e i 2, 2.14) K E m+1 E m+k ) = F2+2tF3 t), K E m+k E m+l ) = F 2 t), i, j = 1,..., m; k, l = 2,..., m. Hee denotes the nom of the vecto with espect to the metic g in point). Question: Cn we hve constnt sectionl cuvtue c on T M)? If this hppens, then it must be 0, so T M) is flt. One gets esily tht M is loclly Eucliden. Then, we should lso hve F 2 t) = 0. It follows, F 3 t) = 0 nd F 1 t) = 0. On the othe hnd n odiny diffeentil eqution occus: A simple computtion shows tht t) t) = t. e 2 1+2t t) = 0 1 +, 1 + 2t) 2 0 > ) Remk 2.11 The mnifold T M) equipped with the Cheege Gomoll hs non constnt sectionl cuvtue. Putting 0, such tht 0) = 1 we cn stte the following Theoem 2.12 Conside g 1 on T M) given by g 1 X H, Y H ) = gx, Y ), g 1 X H, Y V ) = 0 ) 2.16) g 1 X V, Y V ) = 4e2 1) 1+) gx, Y ) + gx, u)gy, u) 2 The mnifold T M), g 1 ) is flt. Let us now compe the scl cuvtues of M, g) nd T M), g ). Poposition 2.13 Let M, g) be Riemnnin mnifold nd endow the tngent bundle T M) with the metic g. Let scl nd scl be the scl cuvtues of g nd g espectively. The following eltion holds: scl = scl R ei e j u m mf 2 + 4tF 3 ), 2.17) whee {e i } i=1,...,m is locl othonoml fme on T M). i<j Poof. Using tht scl = i j Ke i, e j ) nd the fomul
8 8 we get the conclusion. m i,j=1 R ei ue j 2 = m i,j=1 R ei e j u 2 Conside M el spce fom with c the constnt sectionl cuvtue. Question: Could we find functions such tht T M) equipped with the metic g hs constnt scl cuvtue? Then T M), g ) hs constnt scl cuvtue if nd only if stisfies the following ODE: t) 2 t) 3 2 m m) t) t) 2 4 t c + 2 c t) 2 t) t c + 2 c t) 2 t) m) t t) t) t) m m) t) t) + 2 t t) t)) ) = const. which seems to be vey complicted to solve. Acknowledgements. This wok ws ptilly suppoted by Gnt CNCSIS 1463/ n.18/2005. Refeences [1] Abbssi M., Note on the Clssifiction Theoems of g-ntul Metics on the Tngent Bundle of Riemnnin Mnifold M, g), Commnet.Mth.Univ.Coline, 45 4)2004), [2] Abbssi M. nd Sih M., Killing Vecto Fields on Tngent Bundles with Cheege Gomoll Metic, Tsukub J. Mth., 272)2003) [3] Abbssi M. nd Sih M., On Some Heedity Popeties of Riemnnin g- Ntul Metics on Tngent Bundles of Riemnnin Mnifolds, Diffeentil Geomety nd Its Applictions ), [4] Abbssi M. nd Sih M., On Ntul Metics on Tngent Bundles of Riemnnin Mnifolds, Achivum Mthemticum Bno), ) 1, [5] Abbssi M. nd Sih M., On Riemnnin g-mtul Metics of the Fom.g s + b.g h + c.g v on the Tngent Bundle of Riemnnin Mnifold M, g), Medite. J. Mth., ), [6] Anstsiei M., Loclly Confoml Kehle Stuctues on Tngent Mnifold of Spce Fom, Libets Mth., ) [7] Bli D., Riemnnin Geomety of Contct nd Symplectic Mnifolds, Pogess in Mthemtics, Bikhäuse Boston, [8] Boeckx E. nd Vnhecke L., Hmonic nd Miniml Vecto Fields on Tngent nd Unit Tngent Bundles, Diffeentil Geomety nd Its Applictions, ),
9 9 [9] Cheege J. nd Gomoll D., On the Stuctue of Complete Mnifolds of Nonnegtive Cuvtue, Ann. of Mth., ), [10] P.Dombowski, On the Geomety of the Tngent Bundle, J. Reine Angew. Mthemtik, ), [11] Gudmundson S. nd Kppos E., On the Geomety of the Tngent Bundle with the Cheege-Gomoll Metic, Tokyo J. Mth., ) 1, [12] Kowlski O., Cuvtue of the Induced Riemnnin Metic of the Tngent Bundle of Riemnnin Mnifold, J.Reine Angew. Mth., ), [13] Kowlski O. nd Sekizw M., Ntul Tnsfomtions of Riemnnin Metics on Mnifolds to Metics on Tngent Bundles - Clssifiction -, Bull. Tokyo Gkuei Univ. 4) ), [14] Muntenu M.I., Old nd New Stuctues on the Tngent Bundle, to ppe in Poceedings of the Eighth Intentionl Confeence on Geomety, Integbility nd Quntiztion, June 9-14, 2006, Vn, Bulgi, I. M. Mldenov & M. de Leon, Editos, SOFTEX, Sofi 2006, 14pp. [15] Musso E. nd Ticei F., Riemnnin Metics on Tngent Bundles, Ann. Mt. Pu Appl. 4) ), [16] Opoiu V., Some new Geometic Stuctues on the Tngent Bundle, Publ. Mth Debecen, ) 3-4, [17] Opoiu V., A Loclly Symmetic Kehle Einstein Stuctue on the Tngent Bundle of Spce Fom, Beitäge Zu Algeb und Geometie / Contibutions to Algeb nd Geomety, ) [18] Opoiu V., A Kähle Einstein Stuctue on the Tngent Bundle of Spce Fom, Int. J. Mth. Mth. Sci ) 3, [19] Opoiu V. nd Ppghiuc N., Some Clsses of Almost Anti-Hemitin Stuctues on the Tngent Bundle, Medite. J. Mth ) [20] Sski S., On the Diffeentil Geomety of Tngent Bundles of Riemnnin Mnifolds, Tôhoku Mth. J., ), [21] Sekizw M., Cuvtues of Tngent Bundles with Cheege-Gomoll Metic, Tokyo J. Mth., ) 2, Min Ion MUNTEANU Fculty of Mthemtics Al.I.Cuz Univesity of Işi, Bd. Col I, n Işi, ROMANIA e-mil: muntenu@uic.o
RELATIVE KINEMATICS. q 2 R 12. u 1 O 2 S 2 S 1. r 1 O 1. Figure 1
RELAIVE KINEMAICS he equtions of motion fo point P will be nlyzed in two diffeent efeence systems. One efeence system is inetil, fixed to the gound, the second system is moving in the physicl spce nd the
More informationOn Natural Partial Orders of IC-Abundant Semigroups
Intentionl Jounl of Mthemtics nd Computtionl Science Vol. No. 05 pp. 5-9 http://www.publicsciencefmewok.og/jounl/ijmcs On Ntul Ptil Odes of IC-Abundnt Semigoups Chunhu Li Bogen Xu School of Science Est
More informationFI 2201 Electromagnetism
FI 1 Electomgnetism Alexnde A. Isknd, Ph.D. Physics of Mgnetism nd Photonics Resech Goup Electosttics ELECTRIC PTENTIALS 1 Recll tht we e inteested to clculte the electic field of some chge distiution.
More information10 Statistical Distributions Solutions
Communictions Engineeing MSc - Peliminy Reding 1 Sttisticl Distiutions Solutions 1) Pove tht the vince of unifom distiution with minimum vlue nd mximum vlue ( is ) 1. The vince is the men of the sques
More informationThe Formulas of Vector Calculus John Cullinan
The Fomuls of Vecto lculus John ullinn Anlytic Geomety A vecto v is n n-tuple of el numbes: v = (v 1,..., v n ). Given two vectos v, w n, ddition nd multipliction with scl t e defined by Hee is bief list
More informationClass Summary. be functions and f( D) , we define the composition of f with g, denoted g f by
Clss Summy.5 Eponentil Functions.6 Invese Functions nd Logithms A function f is ule tht ssigns to ech element D ectly one element, clled f( ), in. Fo emple : function not function Given functions f, g:
More informationFriedmannien equations
..6 Fiedmnnien equtions FLRW metic is : ds c The metic intevl is: dt ( t) d ( ) hee f ( ) is function which detemines globl geometic l popety of D spce. f d sin d One cn put it in the Einstein equtions
More informationPhysics 505 Fall 2005 Midterm Solutions. This midterm is a two hour open book, open notes exam. Do all three problems.
Physics 55 Fll 5 Midtem Solutions This midtem is two hou open ook, open notes exm. Do ll thee polems. [35 pts] 1. A ectngul ox hs sides of lengths, nd c z x c [1] ) Fo the Diichlet polem in the inteio
More informationOptimization. x = 22 corresponds to local maximum by second derivative test
Optimiztion Lectue 17 discussed the exteme vlues of functions. This lectue will pply the lesson fom Lectue 17 to wod poblems. In this section, it is impotnt to emembe we e in Clculus I nd e deling one-vible
More informationIntegrals and Polygamma Representations for Binomial Sums
3 47 6 3 Jounl of Intege Sequences, Vol. 3 (, Aticle..8 Integls nd Polygmm Repesenttions fo Binomil Sums Anthony Sofo School of Engineeing nd Science Victoi Univesity PO Box 448 Melboune City, VIC 8 Austli
More informationOn the Eötvös effect
On the Eötvös effect Mugu B. Răuţ The im of this ppe is to popose new theoy bout the Eötvös effect. We develop mthemticl model which loud us bette undestnding of this effect. Fom the eqution of motion
More informationMath 4318 : Real Analysis II Mid-Term Exam 1 14 February 2013
Mth 4318 : Rel Anlysis II Mid-Tem Exm 1 14 Febuy 2013 Nme: Definitions: Tue/Flse: Poofs: 1. 2. 3. 4. 5. 6. Totl: Definitions nd Sttements of Theoems 1. (2 points) Fo function f(x) defined on (, b) nd fo
More informationTwo dimensional polar coordinate system in airy stress functions
I J C T A, 9(9), 6, pp. 433-44 Intentionl Science Pess Two dimensionl pol coodinte system in iy stess functions S. Senthil nd P. Sek ABSTRACT Stisfy the given equtions, boundy conditions nd bihmonic eqution.in
More informationRadial geodesics in Schwarzschild spacetime
Rdil geodesics in Schwzschild spcetime Spheiclly symmetic solutions to the Einstein eqution tke the fom ds dt d dθ sin θdϕ whee is constnt. We lso hve the connection components, which now tke the fom using
More informationMichael Rotkowitz 1,2
Novembe 23, 2006 edited Line Contolles e Unifomly Optiml fo the Witsenhusen Counteexmple Michel Rotkowitz 1,2 IEEE Confeence on Decision nd Contol, 2006 Abstct In 1968, Witsenhusen intoduced his celebted
More informationAbout Some Inequalities for Isotonic Linear Functionals and Applications
Applied Mthemticl Sciences Vol. 8 04 no. 79 8909-899 HIKARI Ltd www.m-hiki.com http://dx.doi.og/0.988/ms.04.40858 Aout Some Inequlities fo Isotonic Line Functionls nd Applictions Loedn Ciudiu Deptment
More informationChapter 7. Kleene s Theorem. 7.1 Kleene s Theorem. The following theorem is the most important and fundamental result in the theory of FA s:
Chpte 7 Kleene s Theoem 7.1 Kleene s Theoem The following theoem is the most impotnt nd fundmentl esult in the theoy of FA s: Theoem 6 Any lnguge tht cn e defined y eithe egul expession, o finite utomt,
More informationRight-indefinite half-linear Sturm Liouville problems
Computes nd Mthemtics with Applictions 55 2008) 2554 2564 www.elsevie.com/locte/cmw Right-indefinite hlf-line Stum Liouville poblems Lingju Kong, Qingki Kong b, Deptment of Mthemtics, The Univesity of
More information13.5. Torsion of a curve Tangential and Normal Components of Acceleration
13.5 osion of cuve ngentil nd oml Components of Acceletion Recll: Length of cuve '( t) Ac length function s( t) b t u du '( t) Ac length pmetiztion ( s) with '( s) 1 '( t) Unit tngent vecto '( t) Cuvtue:
More informationπ,π is the angle FROM a! TO b
Mth 151: 1.2 The Dot Poduct We hve scled vectos (o, multiplied vectos y el nume clled scl) nd dded vectos (in ectngul component fom). Cn we multiply vectos togethe? The nswe is YES! In fct, thee e two
More informationarxiv: v1 [hep-th] 6 Jul 2016
INR-TH-2016-021 Instbility of Sttic Semi-Closed Wolds in Genelized Glileon Theoies Xiv:1607.01721v1 [hep-th] 6 Jul 2016 O. A. Evseev, O. I. Melichev Fculty of Physics, M V Lomonosov Moscow Stte Univesity,
More informationu(r, θ) = 1 + 3a r n=1
Mth 45 / AMCS 55. etuck Assignment 8 ue Tuesdy, Apil, 6 Topics fo this week Convegence of Fouie seies; Lplce s eqution nd hmonic functions: bsic popeties, computions on ectngles nd cubes Fouie!, Poisson
More informationPROPER CURVATURE COLLINEATIONS IN SPECIAL NON STATIC AXIALLY SYMMETRIC SPACE-TIMES
POPE CUVATUE COLLINEATIONS IN SPECIAL NON STATIC AXIALLY SYMMETIC SPACE-TIMES GHULAM SHABBI, M. AMZAN Fculty of Engineeing Sciences, GIK Institute of Engineeing Sciences nd Technology, Toi, Swbi, NWFP,
More informationDiscrete Model Parametrization
Poceedings of Intentionl cientific Confeence of FME ession 4: Automtion Contol nd Applied Infomtics Ppe 9 Discete Model Pmetition NOKIEVIČ, Pet Doc,Ing,Cc Deptment of Contol ystems nd Instumenttion, Fculty
More informationEECE 260 Electrical Circuits Prof. Mark Fowler
EECE 60 Electicl Cicuits Pof. Mk Fowle Complex Numbe Review /6 Complex Numbes Complex numbes ise s oots of polynomils. Definition of imginy # nd some esulting popeties: ( ( )( ) )( ) Recll tht the solution
More information440-2 Geometry/Topology: Differentiable Manifolds Northwestern University Solutions of Practice Problems for Final Exam
440-2 Geometry/Topology: Differentible Mnifolds Northwestern University Solutions of Prctice Problems for Finl Exm 1) Using the cnonicl covering of RP n by {U α } 0 α n, where U α = {[x 0 : : x n ] RP
More information( ) D x ( s) if r s (3) ( ) (6) ( r) = d dr D x
SIO 22B, Rudnick dpted fom Dvis III. Single vile sttistics The next few lectues e intended s eview of fundmentl sttistics. The gol is to hve us ll speking the sme lnguge s we move to moe dvnced topics.
More informationTopics for Review for Final Exam in Calculus 16A
Topics fo Review fo Finl Em in Clculus 16A Instucto: Zvezdelin Stnkov Contents 1. Definitions 1. Theoems nd Poblem Solving Techniques 1 3. Eecises to Review 5 4. Chet Sheet 5 1. Definitions Undestnd the
More informationQualitative Analysis for Solutions of a Class of. Nonlinear Ordinary Differential Equations
Adv. Theo. Appl. Mech., Vol. 7, 2014, no. 1, 1-7 HIKARI Ltd, www.m-hiki.com http://dx.doi.og/10.12988/tm.2014.458 Qulittive Anlysis fo Solutions of Clss of Nonline Odiny Diffeentil Equtions Juxin Li *,
More informationThis immediately suggests an inverse-square law for a "piece" of current along the line.
Electomgnetic Theoy (EMT) Pof Rui, UNC Asheville, doctophys on YouTube Chpte T Notes The iot-svt Lw T nvese-sque Lw fo Mgnetism Compe the mgnitude of the electic field t distnce wy fom n infinite line
More informationr a + r b a + ( r b + r c)
AP Phsics C Unit 2 2.1 Nme Vectos Vectos e used to epesent quntities tht e chcteized b mgnitude ( numeicl vlue with ppopite units) nd diection. The usul emple is the displcement vecto. A quntit with onl
More informationSurfaces of Constant Retarded Distance and Radiation Coordinates
Apeion, Vol. 9, No., Apil 00 6 Sufces of Constnt Retded Distnce nd Rdition Coodintes J. H. Cltenco, R. Lines y M., J. López-Bonill Sección de Estudios de Posgdo e Investigción Escuel Supeio de Ingenieí
More informationdefined on a domain can be expanded into the Taylor series around a point a except a singular point. Also, f( z)
08 Tylo eie nd Mcluin eie A holomophic function f( z) defined on domin cn be expnded into the Tylo eie ound point except ingul point. Alo, f( z) cn be expnded into the Mcluin eie in the open dik with diu
More informationMean Curvature and Shape Operator of Slant Immersions in a Sasakian Space Form
Mean Cuvatue and Shape Opeato of Slant Immesions in a Sasakian Space Fom Muck Main Tipathi, Jean-Sic Kim and Son-Be Kim Abstact Fo submanifolds, in a Sasakian space fom, which ae tangential to the stuctue
More information9.4 The response of equilibrium to temperature (continued)
9.4 The esponse of equilibium to tempetue (continued) In the lst lectue, we studied how the chemicl equilibium esponds to the vition of pessue nd tempetue. At the end, we deived the vn t off eqution: d
More informationEXISTENCE OF THREE SOLUTIONS FOR A KIRCHHOFF-TYPE BOUNDARY-VALUE PROBLEM
Electonic Jounl of Diffeentil Eutions, Vol. 20 (20, No. 9, pp.. ISSN: 072-669. URL: http://ejde.mth.txstte.edu o http://ejde.mth.unt.edu ftp ejde.mth.txstte.edu EXISTENCE OF THREE SOLUTIONS FOR A KIRCHHOFF-TYPE
More information1 Using Integration to Find Arc Lengths and Surface Areas
Novembe 9, 8 MAT86 Week Justin Ko Using Integtion to Find Ac Lengths nd Sufce Aes. Ac Length Fomul: If f () is continuous on [, b], then the c length of the cuve = f() on the intevl [, b] is given b s
More informationWeek 8. Topic 2 Properties of Logarithms
Week 8 Topic 2 Popeties of Logithms 1 Week 8 Topic 2 Popeties of Logithms Intoduction Since the esult of ithm is n eponent, we hve mny popeties of ithms tht e elted to the popeties of eponents. They e
More informationLecture 10. Solution of Nonlinear Equations - II
Fied point Poblems Lectue Solution o Nonline Equtions - II Given unction g : R R, vlue such tht gis clled ied point o the unction g, since is unchnged when g is pplied to it. Whees with nonline eqution
More informationAlgebra Based Physics. Gravitational Force. PSI Honors universal gravitation presentation Update Fall 2016.notebookNovember 10, 2016
Newton's Lw of Univesl Gvittion Gvittionl Foce lick on the topic to go to tht section Gvittionl Field lgeb sed Physics Newton's Lw of Univesl Gvittion Sufce Gvity Gvittionl Field in Spce Keple's Thid Lw
More informationA comparison principle for nonlinear heat Rockland operators on graded groups
Bull. London Mth. Soc. 00 2018 1 6 doi:10.1112/blms.12178 A compison pinciple fo nonline het ocklnd opetos on gded goups Michel uzhnsky nd Duvudkhn Sugn Abstct In this note we show compison pinciple fo
More informationPhysics 11b Lecture #11
Physics 11b Lectue #11 Mgnetic Fields Souces of the Mgnetic Field S&J Chpte 9, 3 Wht We Did Lst Time Mgnetic fields e simil to electic fields Only diffeence: no single mgnetic pole Loentz foce Moving chge
More informationThe Area of a Triangle
The e of Tingle tkhlid June 1, 015 1 Intodution In this tile we will e disussing the vious methods used fo detemining the e of tingle. Let [X] denote the e of X. Using se nd Height To stt off, the simplest
More informationChapter 6 Thermoelasticity
Chpte 6 Themoelsticity Intoduction When theml enegy is dded to n elstic mteil it expnds. Fo the simple unidimensionl cse of b of length L, initilly t unifom tempetue T 0 which is then heted to nonunifom
More informationMath 6455 Oct 10, Differential Geometry I Fall 2006, Georgia Tech
Mth 6455 Oct 10, 2006 1 Differentil Geometry I Fll 2006, Georgi Tech Lecture Notes 12 Riemnnin Metrics 0.1 Definition If M is smooth mnifold then by Riemnnin metric g on M we men smooth ssignment of n
More informationElectric Potential. and Equipotentials
Electic Potentil nd Euipotentils U Electicl Potentil Review: W wok done y foce in going fom to long pth. l d E dl F W dl F θ Δ l d E W U U U Δ Δ l d E W U U U U potentil enegy electic potentil Potentil
More informationSchool of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007
School of Electicl nd Compute Engineeing, Conell Univesity ECE 303: Electomgnetic Fields nd Wves Fll 007 Homewok 3 Due on Sep. 14, 007 by 5:00 PM Reding Assignments: i) Review the lectue notes. ii) Relevnt
More informationPreviously. Extensions to backstepping controller designs. Tracking using backstepping Suppose we consider the general system
436-459 Advnced contol nd utomtion Extensions to bckstepping contolle designs Tcking Obseves (nonline dmping) Peviously Lst lectue we looked t designing nonline contolles using the bckstepping technique
More informationarxiv: v1 [math.co] 1 Apr 2011
Weight enumeation of codes fom finite spaces Relinde Juius Octobe 23, 2018 axiv:1104.0172v1 [math.co] 1 Ap 2011 Abstact We study the genealized and extended weight enumeato of the - ay Simplex code and
More informationAvailable online at ScienceDirect. Procedia Engineering 91 (2014 ) 32 36
Aville online t wwwsciencediectcom ScienceDiect Pocedi Engineeing 91 (014 ) 3 36 XXIII R-S-P semin Theoeticl Foundtion of Civil Engineeing (3RSP) (TFoCE 014) Stess Stte of Rdil Inhomogeneous Semi Sphee
More informationChapter 4: Christoffel Symbols, Geodesic Equations and Killing Vectors Susan Larsen 29 October 2018
Content 4 Chistoffel Symbols, Geodesic Equtions nd illing Vectos... 4. Chistoffel symbols.... 4.. Definitions... 4.. Popeties... 4..3 The Chistoffel Symbols of digonl metic in Thee Dimensions... 4. Cylindicl
More information6. Numbers. The line of numbers: Important subsets of IR:
6. Nubes We do not give n xiotic definition of the el nubes hee. Intuitive ening: Ech point on the (infinite) line of nubes coesponds to el nube, i.e., n eleent of IR. The line of nubes: Ipotnt subsets
More informationarxiv: v1 [physics.pop-ph] 3 Jun 2013
A note on the electostatic enegy of two point chages axiv:1306.0401v1 [physics.pop-ph] 3 Jun 013 A C Tot Instituto de Física Univesidade Fedeal do io de Janeio Caixa Postal 68.58; CEP 1941-97 io de Janeio,
More informationThe Clamped Plate Equation for the Limaçon
A. Dll Acqu G. Swees The Clmped Plte Eqution fo the Limçon Received: dte / in finl fom: dte Abstct. Hdmd climed in 907 tht the clmped plte eqution is positivity peseving fo domins which e bounded by Limçon
More informationGeneral Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface
Genel Physics II Chpte 3: Guss w We now wnt to quickly discuss one of the moe useful tools fo clculting the electic field, nmely Guss lw. In ode to undestnd Guss s lw, it seems we need to know the concept
More informationData Structures. Element Uniqueness Problem. Hash Tables. Example. Hash Tables. Dana Shapira. 19 x 1. ) h(x 4. ) h(x 2. ) h(x 3. h(x 1. x 4. x 2.
Element Uniqueness Poblem Dt Stuctues Let x,..., xn < m Detemine whethe thee exist i j such tht x i =x j Sot Algoithm Bucket Sot Dn Shpi Hsh Tbles fo (i=;i
More informationSchool of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007
School of Electicl nd Compute Engineeing, Conell Univesity ECE 303: Electomgnetic Fields nd Wves Fll 007 Homewok 4 Due on Sep. 1, 007 by 5:00 PM Reding Assignments: i) Review the lectue notes. ii) Relevnt
More informationON A CLASS OF N(k)-CONTACT METRIC MANIFOLDS
ON A CLASS OF N(k)-CONTACT METRIC MANIFOLDS UDAY CHAND DE, AHMET YILDIZ and SUJIT GHOSH Communicated by the fome editoial boad The object of the pesent pape is to study ξ-conciculaly flat and φ-conciculaly
More informationdx was area under f ( x ) if ( ) 0
13. Line Integls Line integls e simil to single integl, f ( x) dx ws e unde f ( x ) if ( ) 0 Insted of integting ove n intevl [, ] (, ) f xy ds f x., we integte ove cuve, (in the xy-plne). **Figue - get
More informationD-STABLE ROBUST RELIABLE CONTROL FOR UNCERTAIN DELTA OPERATOR SYSTEMS
Jounl of Theoeticl nd Applied nfomtion Technology 8 th Febuy 3. Vol. 48 No.3 5-3 JATT & LLS. All ights eseved. SSN: 99-8645 www.jtit.og E-SSN: 87-395 D-STABLE ROBUST RELABLE CONTROL FOR UNCERTAN DELTA
More informationTheoretical foundations of Gaussian quadrature
Theoreticl foundtions of Gussin qudrture 1 Inner product vector spce Definition 1. A vector spce (or liner spce) is set V = {u, v, w,...} in which the following two opertions re defined: (A) Addition of
More informationDeterministic simulation of a NFA with k symbol lookahead
Deteministic simultion of NFA with k symbol lookhed SOFSEM 7 Bl Rvikum, Clifoni Stte Univesity (joint wok with Nic Snten, Univesity of Wteloo) Oveview Definitions: DFA, NFA nd lookhed DFA Motivtion: utomted
More informationMATHEMATICS IV 2 MARKS. 5 2 = e 3, 4
MATHEMATICS IV MARKS. If + + 6 + c epesents cicle with dius 6, find the vlue of c. R 9 f c ; g, f 6 9 c 6 c c. Find the eccenticit of the hpeol Eqution of the hpeol Hee, nd + e + e 5 e 5 e. Find the distnce
More informationSTUDY OF THE UNIFORM MAGNETIC FIELD DOMAINS (3D) IN THE CASE OF THE HELMHOLTZ COILS
STUDY OF THE UNIFORM MAGNETIC FIED DOMAINS (3D) IN THE CASE OF THE HEMHOTZ COIS FORIN ENACHE, GHEORGHE GAVRIĂ, EMI CAZACU, Key wods: Unifom mgnetic field, Helmholt coils. Helmholt coils e used to estblish
More informationSPA7010U/SPA7010P: THE GALAXY. Solutions for Coursework 1. Questions distributed on: 25 January 2018.
SPA7U/SPA7P: THE GALAXY Solutions fo Cousewok Questions distibuted on: 25 Jnuy 28. Solution. Assessed question] We e told tht this is fint glxy, so essentilly we hve to ty to clssify it bsed on its spectl
More informationPROGRESSION AND SERIES
INTRODUCTION PROGRESSION AND SERIES A gemet of umbes {,,,,, } ccodig to some well defied ule o set of ules is clled sequece Moe pecisely, we my defie sequece s fuctio whose domi is some subset of set of
More informationApproximation of functions belonging to the class L p (ω) β by linear operators
ACTA ET COMMENTATIONES UNIVERSITATIS TARTUENSIS DE MATHEMATICA Volume 3, 9, Approximtion of functions belonging to the clss L p ω) β by liner opertors W lodzimierz Lenski nd Bogdn Szl Abstrct. We prove
More informationInternational Jour. of Diff. Eq. and Appl., 3, N1, (2001),
Interntionl Jour. of Diff. Eq. nd Appl., 3, N1, (2001), 31-37. 1 New proof of Weyl s theorem A.G. Rmm Mthemtics Deprtment, Knss Stte University, Mnhttn, KS 66506-2602, USA rmm@mth.ksu.edu http://www.mth.ksu.edu/
More informationWHEN IS A FUNCTION NOT FLAT? 1. Introduction. {e 1 0, x = 0. f(x) =
WHEN IS A FUNCTION NOT FLAT? YIFEI PAN AND MEI WANG Abstrct. In this pper we prove unique continution property for vector vlued functions of one vrible stisfying certin differentil inequlity. Key words:
More informationElectric Field F E. q Q R Q. ˆ 4 r r - - Electric field intensity depends on the medium! origin
1 1 Electic Field + + q F Q R oigin E 0 0 F E ˆ E 4 4 R q Q R Q - - Electic field intensity depends on the medium! Electic Flux Density We intoduce new vecto field D independent of medium. D E So, electic
More informationNote 16. Stokes theorem Differential Geometry, 2005
Note 16. Stokes theorem ifferentil Geometry, 2005 Stokes theorem is the centrl result in the theory of integrtion on mnifolds. It gives the reltion between exterior differentition (see Note 14) nd integrtion
More informationImportant design issues and engineering applications of SDOF system Frequency response Functions
Impotnt design issues nd engineeing pplictions of SDOF system Fequency esponse Functions The following desciptions show typicl questions elted to the design nd dynmic pefomnce of second-ode mechnicl system
More informationVariational Techniques for Sturm-Liouville Eigenvalue Problems
Vritionl Techniques for Sturm-Liouville Eigenvlue Problems Vlerie Cormni Deprtment of Mthemtics nd Sttistics University of Nebrsk, Lincoln Lincoln, NE 68588 Emil: vcormni@mth.unl.edu Rolf Ryhm Deprtment
More informationFourier-Bessel Expansions with Arbitrary Radial Boundaries
Applied Mthemtics,,, - doi:./m.. Pulished Online My (http://www.scirp.og/jounl/m) Astct Fouie-Bessel Expnsions with Aity Rdil Boundies Muhmmd A. Mushef P. O. Box, Jeddh, Sudi Ai E-mil: mmushef@yhoo.co.uk
More informationSolution to HW 3, Ma 1a Fall 2016
Solution to HW 3, Ma a Fall 206 Section 2. Execise 2: Let C be a subset of the eal numbes consisting of those eal numbes x having the popety that evey digit in the decimal expansion of x is, 3, 5, o 7.
More informationElectricity & Magnetism Lecture 6: Electric Potential
Electicity & Mgnetism Lectue 6: Electic Potentil Tody s Concept: Electic Potenl (Defined in tems of Pth Integl of Electic Field) Electicity & Mgnesm Lectue 6, Slide Stuff you sked bout:! Explin moe why
More informationHomework # 3 Solution Key
PHYSICS 631: Geneal Relativity Homewok # 3 Solution Key 1. You e on you hono not to do this one by hand. I ealize you can use a compute o simply look it up. Please don t. In a flat space, the metic in
More informationContinuous Charge Distributions
Continuous Chge Distibutions Review Wht if we hve distibution of chge? ˆ Q chge of distibution. Q dq element of chge. d contibution to due to dq. Cn wite dq = ρ dv; ρ is the chge density. = 1 4πε 0 qi
More informationElectronic Supplementary Material
Electonic Supplementy Mteil On the coevolution of socil esponsiveness nd behvioul consistency Mx Wolf, G Snde vn Doon & Fnz J Weissing Poc R Soc B 78, 440-448; 0 Bsic set-up of the model Conside the model
More informationPerturbation to Symmetries and Adiabatic Invariants of Nonholonomic Dynamical System of Relative Motion
Commun. Theo. Phys. Beijing, China) 43 25) pp. 577 581 c Intenational Academic Publishes Vol. 43, No. 4, Apil 15, 25 Petubation to Symmeties and Adiabatic Invaiants of Nonholonomic Dynamical System of
More informationNotes on length and conformal metrics
Notes on length nd conforml metrics We recll how to mesure the Eucliden distnce of n rc in the plne. Let α : [, b] R 2 be smooth (C ) rc. Tht is α(t) (x(t), y(t)) where x(t) nd y(t) re smooth rel vlued
More informationON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION. 1. Introduction. 1 r r. r k for every set E A, E \ {0},
ON INDEPENDENT SETS IN PURELY ATOMIC PROBABILITY SPACES WITH GEOMETRIC DISTRIBUTION E. J. IONASCU and A. A. STANCU Abstact. We ae inteested in constucting concete independent events in puely atomic pobability
More informationLanguage Processors F29LP2, Lecture 5
Lnguge Pocessos F29LP2, Lectue 5 Jmie Gy Feuy 2, 2014 1 / 1 Nondeteministic Finite Automt (NFA) NFA genelise deteministic finite utomt (DFA). They llow sevel (0, 1, o moe thn 1) outgoing tnsitions with
More informationS. S. Dragomir. 2, we have the inequality. b a
Bull Koren Mth Soc 005 No pp 3 30 SOME COMPANIONS OF OSTROWSKI S INEQUALITY FOR ABSOLUTELY CONTINUOUS FUNCTIONS AND APPLICATIONS S S Drgomir Abstrct Compnions of Ostrowski s integrl ineulity for bsolutely
More informationB.A. (PROGRAMME) 1 YEAR MATHEMATICS
Gdute Couse B.A. (PROGRAMME) YEAR MATHEMATICS ALGEBRA & CALCULUS PART B : CALCULUS SM 4 CONTENTS Lesson Lesson Lesson Lesson Lesson Lesson Lesson : Tngents nd Nomls : Tngents nd Nomls (Pol Co-odintes)
More informationON THE EXISTENCE OF NEARLY QUASI-EINSTEIN MANIFOLDS. 1. Introduction. Novi Sad J. Math. Vol. 39, No. 2, 2009,
Novi Sad J. Math. Vol. 39, No. 2, 2009, 111-117 ON THE EXISTENCE OF NEARLY QUASI-EINSTEIN MANIFOLDS Abul Kalam Gazi 1, Uday Chand De 2 Abstact. The objective of the pesent pape is to establish the existence
More informationSelf-similarity and symmetries of Pascal s triangles and simplices mod p
Sn Jose Stte University SJSU ScholrWorks Fculty Publictions Mthemtics nd Sttistics Februry 2004 Self-similrity nd symmetries of Pscl s tringles nd simplices mod p Richrd P. Kubelk Sn Jose Stte University,
More informationThe Schwartzchild Geometry
UNIVERSITY OF ROCHESTER The Schwatzchild Geomety Byon Osteweil Decembe 21, 2018 1 INTRODUCTION In ou study of geneal elativity, we ae inteested in the geomety of cuved spacetime in cetain special cases
More informationSTURM-LIOUVILLE BOUNDARY VALUE PROBLEMS
STURM-LIOUVILLE BOUNDARY VALUE PROBLEMS Throughout, we let [, b] be bounded intervl in R. C 2 ([, b]) denotes the spce of functions with derivtives of second order continuous up to the endpoints. Cc 2
More informationKOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS
Jounal of Applied Analysis Vol. 14, No. 1 2008), pp. 43 52 KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS L. KOCZAN and P. ZAPRAWA Received Mach 12, 2007 and, in evised fom,
More information7.2 The Definite Integral
7.2 The Definite Integrl the definite integrl In the previous section, it ws found tht if function f is continuous nd nonnegtive, then the re under the grph of f on [, b] is given by F (b) F (), where
More informationJournal of Inequalities in Pure and Applied Mathematics
Jounal of Inequalities in Pue and Applied Mathematics COEFFICIENT INEQUALITY FOR A FUNCTION WHOSE DERIVATIVE HAS A POSITIVE REAL PART S. ABRAMOVICH, M. KLARIČIĆ BAKULA AND S. BANIĆ Depatment of Mathematics
More informationMark Scheme (Results) January 2008
Mk Scheme (Results) Jnuy 00 GCE GCE Mthemtics (6679/0) Edecel Limited. Registeed in Englnd nd Wles No. 4496750 Registeed Office: One90 High Holbon, London WCV 7BH Jnuy 00 6679 Mechnics M Mk Scheme Question
More information3.1 Magnetic Fields. Oersted and Ampere
3.1 Mgnetic Fields Oested nd Ampee The definition of mgnetic induction, B Fields of smll loop (dipole) Mgnetic fields in mtte: ) feomgnetism ) mgnetiztion, (M ) c) mgnetic susceptiility, m d) mgnetic field,
More informationTRAPEZOIDAL TYPE INEQUALITIES FOR n TIME DIFFERENTIABLE FUNCTIONS
TRAPEZOIDAL TYPE INEQUALITIES FOR n TIME DIFFERENTIABLE FUNCTIONS S.S. DRAGOMIR AND A. SOFO Abstrct. In this pper by utilising result given by Fink we obtin some new results relting to the trpezoidl inequlity
More informationPX3008 Problem Sheet 1
PX38 Poblem Sheet 1 1) A sphee of dius (m) contins chge of unifom density ρ (Cm -3 ). Using Guss' theoem, obtin expessions fo the mgnitude of the electic field (t distnce fom the cente of the sphee) in
More informationDEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3
DEPATMENT OF CIVIL AND ENVIONMENTAL ENGINEEING FLID MECHANICS III Solutions to Poblem Sheet 3 1. An tmospheic vote is moelle s combintion of viscous coe otting s soli boy with ngul velocity Ω n n iottionl
More informationSPECTRAL SEQUENCES. im(er
SPECTRAL SEQUENCES MATTHEW GREENBERG. Intoduction Definition. Let a. An a-th stage spectal (cohomological) sequence consists of the following data: bigaded objects E = p,q Z Ep,q, a diffeentials d : E
More informationComputing the first eigenpair of the p-laplacian in annuli
J. Mth. Anl. Appl. 422 2015277 1307 Contents lists vilble t ScienceDiect Jounl of Mthemticl Anlysis nd Applictions www.elsevie.com/locte/jm Computing the fist eigenpi of the p-lplcin in nnuli Gey Ecole,,
More informationA STUDY OF HAMMING CODES AS ERROR CORRECTING CODES
AGU Intenational Jounal of Science and Technology A STUDY OF HAMMING CODES AS ERROR CORRECTING CODES Ritu Ahuja Depatment of Mathematics Khalsa College fo Women, Civil Lines, Ludhiana-141001, Punjab, (India)
More information