Analyse complexe et problèmes de Dirichlet dans le plan : équation de Weinstein et autres conductivités non-bornées
|
|
- Φιλύρη Αλεξόπουλος
- 7 χρόνια πριν
- Προβολές:
Transcript
1 Analyse complexe et problèmes de Dirichlet dans le plan : équation de Weinstein et autres conductivités non-bornées Slah Chaabi To cite this version: Slah Chaabi. Analyse complexe et problèmes de Dirichlet dans le plan : équation de Weinstein et autres conductivités non-bornées. Équations aux dérivées partielles [math.ap]. Aix-Marseille Université, 03. Français. <tel > HAL Id: tel Submitted on 9 Dec 03 HAL is a multi-disciplinary open access archive for the deposit and dissemination of scientific research documents, whether they are published or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers. L archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.
2 ttr é r t èq r t r r t r rs rs té é té t é t q s ré ré tr t é t q s t r t q t à t s s r t r ér t é t q s t r t q rs rés té t s t q t r é r tr s t r è s r t s éq t st t tr s t tés r é s r t r t ès r t r t rt r t r t ès r r rès s s r rt rs t t P rt t r r t r t rt r t r r r r t r r r Pr ss r rs rs té r t r r r r Pr ss r rs té r é s Prés t t s Pr ss r rs té r t r r t r r r P t q rt r té t îtr ér s rs rs té r t ss Pr ss r r t r r s îtr ér s rs rs té t r
3
4 és é éq t st à ts s st éq t ré ss t s P t t s à étr P q s é r t L m [u] = u + (m/x x u = 0 ù m C tt éq t t r t t t r é s t r s s r m = r st rsq m = é éq t r st é r sé éq t r tt t r t t s s t s éq t s st é ér s s rés t ts s r m R s m C s r ss s t s s t s t s ér t rs st t rs st t s s s s r tés s é tr r r r s P s r t H + r m < r t é rè é s t s P s s s r s q q s r m C t s é étr r rt èr s t t r r s r é s r s r t rs r m C q s t s s P t r s t s r ss é s r èr t s s è r èt r ét q s sé r té s r s t r s r r r tt t r r s P s s r sér t rsq m R tr q tt st ê s s3 s rt s à r r r tr q s è rt r ét q st à s s s r té r t s r s s P s r r r t H + s s ù r ètr m st t r r t s r rés t t s s t t s r rés t r è rt s r s r s r à ts s r té t m s r s t t r r ç t s s é s r t t s P tr ss q tt ét s q à t s s s s t H + à r ré r s r èr rt ét ss t s q s P s t s t s s r s s s t s éq t w = αw α L r r < rés t t q s êtr t t r r s r été t st t s ré r té r s r té é s t s t s r s s r e s F s s rt s t ès s ré r tés t ù F st t r t ré r q r q t à r étr t q tt ss t s s s r t q r = P s t s t tr s t s s r s t s s t s éq t tr é rés r è r t à é s L p éré s s r s s ss s r s éq t s t t té à t t rt t à s W,
5 str t st q t t ts s t q t r s tr t t s P r tt s L m [u] = u+(m/x x u = 0 r m C s q t s s rt r r t s s t r r t t r m = r t s m = t r 3 r st q t s s t t s t s t st q t s r r 3 r s ts r m R t m C t r ss s t s t s r st r t rs t r st t s r s r t s t r r s r r P t r t H + r m < st s s t t r r t P r s r m C rt r s r r t s r r s r m C t t s t s r P q t t r s ss t r t s rst s s t t t r sts q s s r t r s s r r s s r m R s t t t s s s3 s s s tr r r s t s rt s t t s t t r r r s r P r r t r t H + m s t r s r r s t t s r t s rt r t r s r t t s ts r t t r t m s r s t r t r t t t t P q st t st rt st ss t s s t P t s r t s s t s t q t w = αw t α L r r < t t rs s r t r s t s r t s t r e s F r s r r t ss t s t r F rs t s r t t r t r r t s r = s t t t s r t s s t s t t t tr q t s s ss r t r s t s t t L p r t r s tr t t q t s s ts r t t s W,
6 s t èr s és é str t s t èr s tr t t s t s s ér t rs st à r ètr é s t s t t s à s étr Pré r s s t s t s t s t st t s s s r t é r s str t s t t s t é t s t s t s s s r té r r m t r r t t s t s r m C é rè é s t s P és t ts ré r s é rè é s t s P r m C r P ss r H + q Re m < t s r s r é s r s s xoy t s P r é s r s s t s r ss é s r èr t è s è s s s3 P r m ré é t t r r été s s3 s s t s t r r r s és t r è r t r ét s tr t éq t r éq t s r sq té Pr è r t r s P tr t t r rés t ts P r s t r s ér t s r é s r tér s t r r è rt
7 P r étr t q s t s s r s à s t r t q tr t t t s t é t s Pr rés t ts Ps r t s t t r t t r
8 tr t ét s ér t rs st L m := +(m/x x r tr st rt t s q r s rs é è s s t é sés r s P t t s à étr P q s t s t éq t st P r t r r èr s P r ètr m = rr s t s t s éq t r st é r sé éq t q st t sé r rés r s éq t s st s P r ètr m = s t r és t s 3 sé r s t r é r s r r t r ï P s ré sé t à rt r tr t s é s ét q s s r r t èr r r tér s r t èr s r ï u s t éq t (/x u = 0 rès t ès s étr r s r st q ï st r q s t r st t t rs s s s st s st s t éq t r r q st éq t é r s q é r t s t s s t s s s s rt s t s r q s s t r s s t s q s s t s s t s P m = t é étr q s st s r s t t s r ts és tr é r st r s t r ss s s é t s r è r t ét t é s s s r s u, n u s r r tér r t u st t s r r tér r r st t ét t t t é ér té r str r P u s t t r y u,? n u u, n u O x L (u = 0 t r è t êtr tt q é èr t s t ét s st q s r s tr t rés t r è r t r éq t ér é s rt s
9 té r r t à r t t à rés t rt r ér t r é r rt r è rt ét r r t t r t t r s s r s t r è r t sé ét s s t à r è rt st r étr r s t s s t t r s s P q t tr s t r r tr tt t ès ù ét s ss s r s r sq té éq t ré ss t s t s s t q s w = αw α L r r < tt t s st s é ér t s P s é s ss s r rs s q s r q t é r é st té t s tr tr q s t s tt t s tr s s r r té T t tr rt q r è r t r éq t w = αw ù s rt ré w s L p (T s t q s G p α s rés t ts é ér s t t s r L r (D (r > ré t r t ss t r t rt t s s tr t st r èr s r t q s r = st s éré P r éq t t té σ expw, st à r q σ s é r t σ = e h h s s s t s L t s ér é s r r s s s str t s s t r s t s L rr s w f Ref ù w ér éq t w = αw α = logσ / f ér éq t tr é f = ν f ν = σ t ù u = f ér éq t (σ u = 0 +σ s s t s r è r t à ts r és rt r éq t t té s éré st s str t t t q r σ = e h h W, st s ré r st t str t t s t P r rs t s t t té str t st ss r tré s tr sq s P ét és s t s t s s H + = {z C, Rez > 0} (x m u = 0 t q t z = x + iy H + x m st ré r é t ré r é t r st t str t t s t
10 tr t s t s s ér t rs st à r ètr é s t s t t s à s étr s tr s r s ét r ss ér t rs ér t s L m = + m x x m C é s s r r t H + = {(x,y R, x > 0} = {z C, Rez > 0} tt ss ér t rs és ér t rs ré ss t s P t t s à étr r ér t rs st été ét é èr ss 3 t s s s s m N m R s s s tér ss r s s tr s t s ù m C r s q q s ss s ù s rs m s r t r str t s à N Z R s s t s éq t s H + q s r s P r q t ré ss t s P t t s à étr L m u = 0 (EPSA s r t é s P t t s à étr ré é P s tér ss r ss s t s éq t L m u = δ (x,y ùδ (x,y és ss r (x,y H + t ss s t s éq t L m u = g ù g és r t ré èr é s rt H + s tr s r str r t r t s s s r rés t ts s ét t r t t s s s ér r st à r ér t rs n k= x i + m x n xn
11 P P P P P P s s H + n = {x R n, x n > 0} r r à r tr t tt ss ér t rs été st s ù ét s m N t t rt r r s r s P t t s à étr q s r t èr t à H + s t π u(0, 0 sin m θdθ = π π π u(re iθ sin m θdθ (PM t r ss s t t t r s t s ss t t r t t r té r s t q s r t s r é s ét t r rs tr s P r m N t s t s r q s R m+ q s r r s s r s t s st t 3 st ét ss t r rr s q s r r s tr s P rr s ts à m t r r s ts à m r s t s é s t r ss s t t t s r é s r s rs ré s m t t tr P t s éq t s r t rs s t s t s s r t t r t P ss é ér s t P s tér ss ss r ts s P r st s tér ss ss r r étés é t s s r tés s P s t r r rés t t str t s P s t s s r q st é ér sé r r t s P r rs é r r s s t s t s s éq t s t q s à ts t q s à s t s tr t s s ssé r r s r r q ré q é ér sé r t q râ ér t rs s z t z s t r s r st q s ê èr q t r q t r q st rt ré t r r s t r t t t r r t q s s t s éq t s t q s t rt r s P s é r t s t s q é à t r q q t tr q é à t t r ss q q s t s s é r t t t t r t s q s t t à s t s r é étr q s r à ér t s r t r s s r tr t très tér ss t tr P s ré t à s tr s s s r sér s t t ér t r ˆLu = u+a x u+b y u+cu t ét r tt sér ss t à éq t t3 s rt s èr s P è s r m 0 r rés t t s s r té r s s t s s éq t s t rt r s t t rsq s r é q s r q r s t r è r q s st à r str r P s H + à rt r s ss s s rs t s s ér é s r r rt r st s t q s r s r rt tt t ès st ét é s s ù P st é s r s x s st ss ét é s s ù
12 P P P P P P st H + \[0,a] {0} a > 0 s tr t r r tr s q s t r q s s s rés t t rés t ts q ê s s s t s t t r m ré st rés t t t t t s t s t q s ér t s s t sé s s s tr ré é t tés s rés t ts r s rs s m s t r tr à tr ss s rés t ts st ê s rés t ts s r r s t rés t t r st t é rè é s t q r q t t P s r H + st à r r Ω \ K ù Ω st rt H + t K st t Ω êtr s P s Ω tr s H + \ K t t t rs r H + s t s ss t é rè t q r q s P s r H + t rs à t s r s r é s rs st t q t rq s q rés t t st s é t r P st éq t t q é é éré sq st t t té t rs s s r é s s rés t ts r r ét t rt t s r s rs rt èr s m m = ± tr ss r r s t Pré r s s t s t s t s t st t s s s r t é r s str t s t s s t s ér q s s r t à rs s s t t s t t r H + = {(x,y R, x > 0} r t R Ω st rt R n n N D(Ω és r s s t s C à s rt t s r Ω s rt t f é s r Ω s r té suppf := {x Ω, f(x 0} P r K t s s Ω t r D K (Ω s s ϕ D(Ω t s q s ϕ K rsq u st t é t ér t s rt Ω R n s ér é s rt s u s r t t r à t r té s u x i xi u r u xi i,n rsq α = (α,...,α n N n st t t r α = α + +α n α := α x αn x n = α x α x αn n r q str t T s r Ω st r é r s r D(Ω t s s s s t r t t t K Ω st N N t st C > 0 t s q ϕ D K (Ω, T(ϕ C sup α N n α N sup α ϕ. K t r r s T(ϕ =: T,ϕ t r D (Ω s t r s str t s s r Ω P P
13 P P P P P P a Ω é t str t δ a r a r ϕ D(Ω, δ a,ϕ = ϕ(a. f : Ω C t t té r té r s r t t t Ω r r rt à s r s dm n é t str t T f ss é à f r ϕ D(Ω, T f,ϕ = fϕdm n. r q s α N n st t t s T st str t s r Ω ér é α T st r é t str t s r Ω é r Ω ϕ D(Ω, α T,ϕ := ( α T, α ϕ. s té r t s r rt s tr t q s T f st str t ss é à t ss C N t s α N n st t q α N rs α T f = T α f. f C (Ω t T D (Ω é t str t ft r ϕ D(Ω, ft,ϕ := T,fϕ. t L ér t r ér t s r Ω r L = a α α α N ù N N s t ré é t st t é s r s t s α r α s t t q N t s t s a α s t s t s s C (Ω P r é t s T st str t LT s r str t LT = α N a α α T ér t r t L L s s s str t s ér t r q à str t T ss str t L T = ( α α (a α T. α N r rq q s f,g s t t s D(Ω rs t t T f f t T g g Lf,g := LT f,g = T f,l g = f,l g. t t t a Ω t L ér t r ér t s r Ω s t t L s r Ω a Ω t t str t é ér q T a t q LT a = δ a ù é té ré é t st é té s s s str t s s r Ω tt é té s réé r t ss ϕ D(Ω, ϕ(a = LT a,ϕ = T a,l ϕ. P P
14 P P P P P P s s st s s r t q s tt é t s s t s t s rt Ω rô r t s r L = s R st q s a = (a,a H + T a = 4π ln( (x a +(y a st s t t s D(R a str t U a é r U a = T a T ( a,a = ( 4π ln (x a +(y a (x+a +(y a s r rs s t t a s D(H + s s s D(R r s ϕ D(R t s q s ϕ D(H + U a,ϕ = ϕ(a ϕ( a,a U a,ϕ = ϕ(a ϕ( a,a = ϕ(a. rt r s r a Ω T a st s t t L a s Ω t s g D(Ω st t q g = L(ϕ ϕ D(Ω rs a Ω, ϕ(a = T a,g. t s s a Ω, ϕ(a = δ a,ϕ = L T a,ϕ = T a,lϕ = T a,g. s s t s t s r tt t rés r éq t Lϕ = g s D(Ω s g D(Ω t t s t é t s m N s R m s r té m s s t q m = P r m C L m st ér t r é s t r t t t u C (H + t r t t (x,y H + L m u(x,y = u(x,y+ m x u x (x,y. t s r r s t t s t s f(x,y = (f (x,y,f (x,y st t t r ss C s rt R t à rs s C rs div(f := f x + f y. ê s f : R C st t s r ss C s rt R t à rs s C rs f := ( f x, f. y P P
15 P P P P P P s t t s ér t r L m st ér t r q à t u C (H + ss t é s r H + r L m u(x,y = x m div(x m u(x,y. rés t rè r3 q s u st t é s rt s t H + t q div(σ u = 0 ù σ : H + R + st ss C rs st t v s t sstè éq t s é ér sé v x = σ u y v y = σ u x t v ér éq t é div( v = 0 tt r rq st t q σ s r s L m r m C ér t r é L m t L m ér t r é r r t t t u C (H + t r t t (x,y H + L mu(x,y = u(x,y x t sq ( mu(x,y = u(x,y m x x u x (x,y+ m x u(x,y L m u(x,yv(x,y dxdy = u(x,yl mv(x,y dxdy u, v D(H +, H + H + L m st ér t r t L m s s s str t s s r H + tt é t é s H + s tr s s sé t s rt Ω H + s s ù s t s q é s é t tr s r s q x t y é r r L m,x,y L m q s q s ér é s rt s s t é s r s x t y t q s tr s r s s t s éré s ét t é s s s é r s ér t rs R m S m t D ç s t P r u D(H + é t S m u t D(H + r (S m u(x,y = x m u(x,y. P r u D(H + é t Du t D(H + r (Du(x,y = u x (x,y. s ér t rs s é s ér t r s t s t Pr s t S m L m t L m D L m t L m q t r q S m L m = L m S m, L md = DL m. P P
16 P P P P P P Pr t r èr r t s (S m u x = mx m u+x m u x, (S m u xx = m(m+x m u mx m u x +x m u xx, (S m u yy = x m u yy. t t rs L m S m u = (S m u xx +(S m u yy + m x (S mu x = x m ( u m x u x + m x u. L m S m u = S m L mu è r t s t s ér t rs t L mdu = u x +m x x L mdu = x ( u x x t t t t ( u+ m x r é s r t s s rq s u = DL m u, x m C S m t L m S m s t s ér t rs t ts S m = S m t L m S m = (L m S m s s rés t t s é ér s r s s ér t rs L m t L m s ér s r σ : Ω C t ss C q s s ér t r s r C (Ω é r r u C (Ω P σ u(x,y = ù Ω st rt R rs σ(x,y div(σ(x,y u(x,y, ( ( Pσ = div σ. σ t s u,v D(Ω s s t s t ér t s s s str t s P σ u,v = Ω σ(x,y div(σ(x,y u(x,yv(x,ydxdy ( v = σ u dxdy Ω σ ( ( v = udiv σ σ Ω P P
17 P P P P P P = u,p σv é t S σ ér t r q à u C (Ω ss (S σ u(x,y = σ(x,y u(x,y. rs S σ P σ t Pσ ù P σ = div ( σ ( σ sq èr é t s s S σ P σ = P σ S σ s s é tés ré é t s s t r s r t èr s r ss t s r s t s u v s q r ér é s s t à s rt t s rt Ω s s s s r s t s s t s q tr s s tr st Pr s t Pr st Ω st rt r t t t H + t s u : Ω C st ss C rs r t t m C L m u = x m L m [x m u]. Pr t α C t s s u(x,y = x α v(x,y t u x = αx α v +x α v x, u xx = α(α x α v +αx α v x +x α v xx u yy = x α v yy. ( L m u = x α v + m+α v x + α(m+α v x x t s ss t α := m t t é té s s ù t t m st t r s t tr t ér t r T m q à t u é s rt Ω H + ss t v é s r s {x R m+, ( x +x m+,x m+ Ω} r v(x,...,x m+ = u( x + +x m+,x m+. ré é t é t s rés t t s t Pr s t P r u ss C s rt r t t t H + t m N m+ (T m u = T m (L m u Pr P s s v = T m u P r t t i,m+ v x i = x i u x +...+x x, +m v x m+ = u y t v x i ( x i = x +...+x ( +m x +...+x 3/ +m u x + x i x +...+x +m u x. P P
18 P P P P P P m+ v = u+ m u x +...+x x, +m ù rés t t s r s t s t s r ttr r s s t s t s r L m t L m r m N t t r s r m Z r s t s st t s s r ss s r ttr t tr r q s r ss s t s r ss t t s s t s t s L m t L m r m C t s t s s s r té r r m t r r t r q s (x,y R δ (x,y st str t é r ϕ D(R, δ (x,y,ϕ = ϕ(x,y. t m t r s t Pr s t rt t s t m N P r (x,y H + t (ξ,η H + π E m (x,y,ξ,η = ξm π θ=0 [ (x ξ +4xξsin ( θ sin m θdθ ] +(y η m/ st s t t s H + r ér t r L m,ξ,η H + q s s s s str t s s H + t é (x,y L m,ξ,ηe m (x,y,ξ,η = δ (x,y (ξ,η. s s (ξ,η H + st é rs s s s str t s s H + L m,x,y E m (x,y,ξ,η = δ (ξ,η (x,y, q s q E m st s t t s H + ér t r L m,x,y t (ξ,η H + é Pr R m+ st t m N r q s t t s E(x = mω m+ x m, x Rm+, s s s str t s m+ E = δ 0 ω m+ ét t s r s èr té R m+ r t t t v D(R m+ v(t,...,t m+ = dτ dτ...dτ m+ m+ v(τ mω m+ τ R m+ ((τ t + +(τ m+ t m+ m/ ù τ = (τ,...,τ m+ P P
19 P P P P P P q t tt r t à v = T m u ù u D(H + s t s râ à r s t r t t (x,y H + u(x,y = (L m u( ξ + +xi m+,ξ m+ dξ dξ m+ ( mω m+ R m+ (ξ x +ξ + +ξm+ +(ξ m+ y m/ P r s r tt r ss té r s èr s r é s r s é r q s s t s ξ = ξcosθ ξ = ξsinθ cosθ = ξ m = ξsinθ sinθ m cosθ m ξ m = ξsinθ sinθ m cosθ m ξ m+ = ξsinθ sinθ m ù ξ = ξ + +ξ m+ θ m ] π,π[ t θ,...,θ m ]0,π[ r s ét r t tr é r stè r é s st t t rs r t t (x,y H + u(x,y = E m (x,y,ξ,η = ξm mω m+ r s t q I := π ξ m sinθ m sin θ m sin m θ η= π θ m= π ξ=0 π L m (u(ξ,ηe m (x,y,ξ,ηdξdη θ,...,θ m =0 θ m= π st s r s èr té s R m sq π π ω m = S m dσ = θ m = π t E m s é r t E m (x,y,ξ,η = ω mξ m sinθ m sin θ m sin m θ dθ...dθ m (ξ xξcosθ +x +(y η m/ π θ,...,θ m =0 sinθ m sin θ m sin m θ dθ...dθ m dθ m θ,...,θ m =0 mω m+ π θ=0 r t s t t q ω m = πm Γ( m π E m (x,y,ξ,η = ξm π θ=0 t t t r ss sinθ m sin θ m 3 sin m θ dθ...dθ m. sin m θdθ (ξ xξcosθ+x +(y η m/ ( (x ξ +4xξsin ( θ sin m θdθ +(y η m/ P P
20 P P P P P P s r t t (x,y H + t r t t (ξ,η H + ( m x E m (x,y,ξ,η = E m (ξ,η,x,y ξ t r r s t S m L m t L m rs s s s str t s ( (x m ( m x L m,x,y E m (x,y,ξ,η = L m,x,y E m (ξ,η,x,y = L ξ ξ m,x,ye m (ξ,η,x,y, t t r r L m,x,y E m (x,y,ξ,η = ( m x δ (ξ,η(x,y = δ (ξ,η, ξ P r m t r é t r s t ré é t é r st s r t t r s t s t Pr s t rt t s t m Z \ N P r (x,y H + t (ξ,η H + ( m ξ E m (x,y,ξ,η = E m(x,y,ξ,η x π = ξx m sin m θdθ [ π θ=0 (x ξ +4xξsin ( ] θ +(y η m st s t t s H + r ér t r L m,ξ,η t é (x,y H + t st s t t s H + ér t r L m,x,y t (ξ,η H + é Pr r t t m N u D(H + t (x,y H + u(x,y = (L m ue m (x,y,ξ,ηdξdη, (ξ,η H + t r r st r s t u(x,y = ξ m L m (ξ m ue m (x,y,ξ,ηdξdη. H + t t v(x,y = x m u(x,y t t x m v(x,y = ξ m (L m ve m (x,y,ξ,ηdξdη, H + s r t t m Z\N v D(H + t (x,y H + s t m = m ( m ξ v(x,y = (L m v E m (x,y,ξ,ηdξdη. H x + r s t st P P
21 P P P P P P t s t s r m C s r s s r r tr r q s r ss s ré é t s é ss t t s s t s t s s ér t rs L m r m s t r r t s r m C P s ré sé t s m rs E m = ξm π π θ=0 t t s q s m < rs t E m = ξx m π π θ=0 sin m θdθ [(x ξ +4xξsin ( θ +(y η ] m/ sin m θdθ [ (x ξ +4xξsin ( ] θ +(y η m s t t q s t E m és r t rs r rr s t s t q m m < Pr s t P r m C t (ξ,η H + és t r (x,y H + é (x,y H + \{(ξ,η} L m,x,y E m (x,y,ξ,η = 0. (ξ,η H + \{(x,y} L m,ξ,ηe m (x,y,ξ,η = 0. Pr P r té r s s t s f m (x,y,ξ,η,θ = [(x ξ +4xξsin ( θ +(y η ] m. P r tr r r èr é té r s t s t tr r q π θ=0 s s ér é s t f m L m,x,y f m (x,y,ξ,η,θsin m θdθ = 0. x f m = m (x ξ+4ξsin θ [(x ξ +4xξsin ( (= m(x ξcosθf θ +(y η ] m + m+ t xx f m = m [(x ξ +4xξsin ( θ +(y η ] m ++ s yy f m = + m ( m + ((x ξ+4ξsin θ [(x ξ +4xξsin ( θ +(y η ] m + m [(x ξ +4xξsin ( θ +(y η ] m ++ P P
22 P P P P P P t t f m = + m ( m + ((y η [(x ξ +4xξsin ( θ +(y η ] m + m [(x ξ +4xξsin ( θ +(y η ] m ++ + m ( m ((x ξ+4ξsin θ + +((y η [(x ξ +4xξsin ( θ +(y η ] m +. r ( (x ξ+4ξsin θ [ ( ] θ +((y η = 4 (x ξ +4xξsin +(y η 4ξ sin θ f m = r rq t q f m+ θ m [(x ξ +4xξsin ( θ +(y η ] m + m(m+ξ sin θ [(x ξ +4xξsin ( θ +(y η ]. m + xξsinθ = (m+ [(x ξ +4xξsin ( θ +(y η ], m + f m = m f m+ +m ξ x sinθ f m+ θ t r té r t r rt s t t π θ=0 f m sin m θdθ = m π = m x π θ=0 = m x θ=0f m+ sin m θdθ+m ξ x π θ=0 m(x ξcosθf m+ sin m θdθ π θ=0 x f m sin m θdθ, f m+ θ sin m θdθ ù rés t t s m r st t t t s r s m < è é té r s t é é t t t q S m L m t L m r s t r s t s t rt t s t s rès r s r té t s r t r tr r q s t t t s s t s t s r t t s s rs m C t s s t s rs t èr s rt r s tr s q rt t s s t s t s st r rt t s s t s t s t st r s ér t rs t q s s s s st s s r t q s r tt r s t s st t s q s s s té r s t q s P P
23 P P P P P P s t s st t s t t t é é t r s t s t t é rè r é t ér t s s st t s ss q s q é t st t s t s r é étr q s t f t g t s é s s r rt Ω R t à rs s t s t (x,y t ér t à Ω t q f st éq t à g (x,y t é r t f (x,y g f(ξ,η (ξ,η (x,y g(ξ,η s ér f g st é t g (x,y st à r r t t ε > 0 st α > 0 t q r t t (η,ξ Ω s (ξ x +(η y α rs f(ξ,η g(ξ,η ε g(ξ,η Pr s t t m C P r (x,y H + é E m (x,y,ξ,η (ξ,η (x,y π ln (x ξ +(y η Pr r tr t r s ù m st ré s ér r é à s s t s r ss s t r s t t = π E m (x,y,ξ,η = ξm π ( m ξ π d θ=0 π θ=0 sin m θdθ (+ksin θ m/ rq s q q d 0 k + s s r s t s t Pr s t rsq k + t m C Pr π θ=0 (+ksin θ m/ sin m θdθ [ (x ξ +4xξsin ( ] θ +(y η m/ sin m θdθ P s t u = sin θ tt té r t r 0 m 0 u m ( u m du (+ku m/ u m ( u m du ( k +u m/ 0 t r r t k + 0 u m d = (x ξ +(y η t k = 4xξ d. k + = m k m/ 0 u m du ( k +u = m/ 0 (u m/( ( u m m lnk. km/ du = t r u = k s t s 0 u m ( u m du ( k +u m/. u m du r s k ( k +u = th m tdt m/ 0 u m ( k +u m/ ( ( u m du 0 ( u m P P u du
24 P P P P P P th m t t rs q t + t q 0 dt r é t q q k + r s k 0 r s t rés t râ à r s t s s s m < st s r r s k th m dt dt = r s k k + 0 k + lnk. E m (x,y,ξ,η ( x m d 0+ π d m lnk km/ d 0+ π lnd. é rè t m C P r (x,y H + t (ξ,η H + π E m (x,y,ξ,η = ξm π θ=0 [ (x ξ +4xξsin ( θ sin m θdθ ] +(y η m/ s m ( m ξ t E m (x,y,ξ,η = E m(x,y,ξ,η x = ξx m π π θ=0 sin m θdθ [ (x ξ +4xξsin ( ] θ +(y η m s m < st s t t s H + r ér t r L m,ξ,η t é (x,y H + q s s s s str t s s H + L m,ξ,ηe m (x,y,ξ,η = δ (x,y (ξ,η. s s (ξ,η H + st é rs s s s str t s s H + L m,x,y E m (x,y,ξ,η = δ (ξ,η (x,y, q s q E m st s t t s H + ér t r L m,x,y t (ξ,η H + é Pr t m C t u D(H + t (x,y H + t ε > 0 t q D((x,y,ε H + ù D((x,y,ε st sq tr (x,y t r ε P s s I ε := L m (u(ξ,ηe m (x,y,ξ,ηdξdη = = H + \D((x,y,ε H + \D((x,y,ε (L m (u(ξ,ηe m (x,y,ξ,η u(ξ,ηl m(e m (x,y,ξ,ηdξdη r L m(e m = 0 s H + \D((x,y,ε é é t r s L m (ue m ul m(e = ξ (( ξ ue m u( ξ E m + m ξ ue m + η (( η ue m u( η E m. P P
25 P P P P P P s r r s r q s êtr t t Ω rt R t r st ss C r r t t n t r t r r s rt t à Ω t ds é é t r s r Ω r té ss t tér r Ω s r s X = (X,X : Ω C st t rs C rs Ω divx(x,ydxdy = Ω X(x,y n(x,yds râ à r q é à rt Ω = U\D((x,y,ε ùu st rt ré r H + t t s rt u s t s I ε = t [0,π] (ξ,η=(x,y+ε(cos t,sin t r s t tr q t [0,π] (ξ,η=(x,y+ε(cos t,sin t (( ( ξ ue m u( ξ E m + m ξ ue m [ [( ξ u+ m ξ u]cost+( ηusint cost+ +(( η ue m u( η E m sint εdt ] E m εdt ε 0+ 0 r lim ε 0 εlnε = 0 s t r r q lim ε 0 I ε st t tr r st lim ε 0 t [0,π] (ξ,η=(x,y+ε(cos t,sin t t tt t s r é à t I ε s s à rt r t t q m u(( ξ E m cost+( η E m sintεdt, t s J ε té r r t s é té ré é t s J ε = m u ξm sin m θdθ π t [0,π] ε m ( 0 (ξ,η=(x,y+ε(cos t,sin t +ksin θ m/ εcostdt+ }{{} π + m u ξm sin m θdθ π t [0,π] ε m+ ( 0 (ξ,η=(x,y+ε(cos t,sin t +ksin θ m/+ ε dt+ }{{} J ε, π J ε, π + m u ξm xsin θ sinm θdθ π t [0,π] ε m+ ( 0 (ξ,η=(x,y+ε(cos t,sin t +ksin θ m/+ εcostdt }{{} t ù r q k = 4xξ ε s s s r s t s s t s J ε,3 P P
26 P P P P P P Pr s t rsq k + t m C π sin θ sinm θdθ m θ=0 (+ksin θ m/+ k + k m + lnk. Pr P s t u = sin θ tt té r t r 0 m 0 u m+ ( u m du (+ku m/+ u m+ ( u m du ( k +u m/+ 0 k + 0 u m+ = m k m/+ 0 u m+ du ( k +u = m/+ 0 (u m/+( ( u m du = t r u = k s t s u m+ ( u m du ( k +u m/+. u m+ ( k +u m/+ ( ( u m du 0 ( u m u du. 0 u m+ du r s k ( k +u = th m+ tdt m/+ 0 th m+ t t rs q t + t q 0 dt r é t q q k + r s k 0 r s t rés t r s k th m+ dt dt = r s k k + 0 k + lnk. Pr s t rsq k + t m C π sin m θdθ m θ=0 (+ksin θ m/+ k + mk m Pr P s t ré é t u = sin θ tt té r t m 0 u m ( u m du (+ku m/+ = m k m/+ 0 u m ( u m du ( k +u m/+. r 0 u m ( u m du ( k +u m/+ 0 u m du ( k +u = m/+ 0 u m ( k +u m/+ ( ( u m du s s st r r r r t tt é té P P
27 P P P P P P 0 u m ( ( +u m/+ ( ( u m u m m du ( 0 +u u du m/+ k k = 0 k + 0 ( u m ( +u m/+ k u m (u m/+ = 0 ( m u ( u m du m u ( u m du s r r s t m u ( u m du. ( u 3 m 0 u m+ ( k +u m +du m lnk. k + 4 ( t t rs râ à t 0 u m ( +u m/+ ( ( u m m du lnk. k + 4 k t r u = k s t s 0 u m du r s k ( k +u = k th m t m/+ 0 dt = k t m th ( r m s k. é t q q k + 0 u m du ( k +u m/+ k + k m. t t t t r s t rés t s à r t é rè r s t tr q J ε, ε 0+ m π 0 u m ( u m du k ( k +u m/+ k + m. π sin m θdθ m θ=0 (+ksin θ m/+ k + mk m t [0,π] (ξ,η=(x,y+ε(cos t,sin t u xm ε m m k m/(lnkεcostdt ( + m ε 0+ πx εlnε u(x+εcost,y +εsintcostdt t [0,π] (ξ,η=(x,y+ε(cos t,sin t P P
28 P P P P P P q t rs r s t tr q m J ε,3 ε 0+ π t [0,π] (ξ,η=(x,y+ε(cos t,sin t u xm m εm+(x k m/+(lnkεcostdt ( m ε 0+ 4πx εlnε u(x+εcost,y +εsintcostdt t [0,π] (ξ,η=(x,y+ε(cos t,sin t q t ss rs r s t tr q ε 0+ π m J ε, ε 0+ π t [0,π] (ξ,η=(x,y+ε(cos t,sin t t [0,π] (ξ,η=(x,y+ε(cos t,sin t u xm ε m+ m mk m/ε dt u(x+εcost,y +εsintdt ε 0+ u(x,y. r é q r t t m C t rt ré st str t t s t lim L m (u(ξ,ηe m (x,y,ξ,ηdξdη = ε 0+ H + \D((x,y,ε = L m (u(ξ,ηe m (x,y,ξ,ηdξdη = u(x,y H + q E m st t t s t t L m q q s t m C t rt ré st str t t s t r r m C t rt ré st str t t ér r à st t t t ss s ss rt s s r s s t s t s L m q q s t m C r s t s t st s s séq t é rè ré é t Pr s t t m C t Ω rt r t t t s H + t r st ss C r r rs r (x,y Ω t u ss C s Ω t t n t r t r r s rt t à Ω t ds é é t r s r Ω r té ss t tér r Ω s r s s u(x,y = Ω L m (ue m dξdη [ ( ξ ue m u( ξ E m + m ] Ω ξ ue m, ( η ue m u( η E m nds t ù té s s té r s u := u(ξ,η t E m := E m (x,y,ξ,η P P
29 P P P P P P Pr t s u st s C (Ω s s r (x,y Ω t ε > 0 t q D((x,y,ε Ω L m (ue m dξdη = (L m (ue m L m(e m udξdη. Ω\D((x,y,ε Ω\D((x,y,ε rès r r ré é t té tt r èr té r st é à Ω t [0,π] (ξ,η=(x,y+ε(cos t,sin t [ ( ξ ue m u( ξ E m + m ] ξ ue m, ( η ue m u( η E m (( ( ξ ue m u( ξ E m + m ξ ue m cost+ nds +(( η ue m u( η E m sint εdt, t rès q s s s r ré é t tt r èr r ss t q ε 0 rs [ ( ξ ue m u( ξ E m + m ] ξ ue m, ( η ue m u( η E m nds+u(x,y. Ω r tèr té r E m s (x,y tr q L m (ue m dξdη = L m (ue m dξdη, lim ε 0 Ω\D((x,y,ε t r s t st r é Ω é rè é s t s P s r s s r r tr r q t t P s r H + st à r r Ω\K ù Ω st rt H + t K st t Ω êtr s P s Ω tr s H + \ K t t t rs r H + r ss t s t s t s s êtr t r t r t t é rè é s t s s r q s s r ss s ér t s s s t s t s s t s rs m P r s t s r ss s r s rt ts ér ts s t r m s s s r r r sé ré t s s m < t m P s ré sé t s s r s s t s t s q s t s s r r H + st à r s s r s r é s t s à P r m < r ss E m (x,y,ξ,η = ξx m π π θ=0 sin m θdθ [ (x ξ +4xξsin ( ] θ +(y η m tr q E m ér tt r r été E m (x,y,, t rs q x 0+ t (x,y + P P
30 P P P P P P P r m π E m (x,y,ξ,η = ξm π θ=0 ér s tt r r été P r tr [(x ξ +4xξsin ( θ E m (x,y,ξ,η E m ( x,y,ξ,η sin m θdθ +(y η ] m/ st t rs s t t s H + t q ér tt r r été s s r s P r m < P r m F m (x,y,ξ,η = E m (x,y,ξ,η F m (x,y,ξ,η = E m (x,y,ξ,η E m ( x,y,ξ,η. és t ts ré r s u D(H + t s r (x,y H + é t U(x,y = u(ξ,ηf m (x,y,ξ,ηdξdη, H + rs lim U = 0 t r t t y R lim U = 0 (x,y + (0,y s U st ss C s r H + \ s u t r t t (x,y s u L m,x,y U(x,y = 0 Pr r rq q q (ξ, η st é F m (x,y,ξ,η = ξx m π π θ=0 sin m θdθ [ (x ξ +4xξsin ( ] θ +(y η m r m < rs F m (x,y,ξ,η 0 t r r rés t t (x,y + é ê s m [ π F m (x,y,ξ,η = ξm sin m θ [ π θ=0 (x ξ +4xξsin ( θ +(y η ]m [ (x+ξ 4xξsin ( θ +(y η ]m F m (x,y,ξ,η 0 t r r rés t t é (x,y + P P ] dθ
31 P P P P P P P r s t s t r rq r q r m < F m (x,y,ξ,η (x,y (0,y q q rés t t és ré ξx m π[ξ +(y η ] m/ π 0 sin m θdθ s s t t m (ξ,η s s rt u q st t s H + rt r st M > 0 t α > 0 é t q u t s q (ξ,η M t ξ α t y s R P s s r x [ α,α] f m (x = [ (x ξ +4xξsin ( θ +(y η ]m. é té s r ss ts s tr q r x > 0 ss 3 r t rt r f m (x f m (0 xsup f m [0,α] f m ( x f m (0 x sup f m. [ α,0] f m (x f m ( x x sup f 3M +α m x m [ α,α] α. Rem+ sup F m (x,y = O(x (ξ,η supp u y R q x 0+ è t é rs r r t rés t t q s s s (x,y (ξ,η s t t s s s H + rs L m,x,y F m (x,y,ξ,η = 0. rq rq s q s U st s D(H + rs L m,x,y U = u s q tt t té st s é ss r t r s U D(H + rt r t s r s q L m U = u s r s é t s é t t r s t q s t é t t u : H + R t s r H + é r t s t s t s lim H +u = 0 ε > 0, N N, n N, (x,y H +, x n (x,y n = u(x,y ε. P P
32 P P P P P P tr s t r s r t à s ér r q r H + H + st st t é s ts s r é s t s ts à t à r q t r rs s r r H + st rt s s t r r rs t s s tr r q tt t r r st s s rt q t r t rs t t t H + P s ré sé t s s r s t s t Pr s t t u : H + C s t s t s lim H +u = 0 lim u(x,y = 0 t y R, lim u = 0. (x,y + (0,y Pr s s r t st é t s s t t q t t tr s q lim H + u = 0 lim u(x,y = 0 t y R, lim u = 0 (x,y + (0,y t ε > 0 st A > 0 t q r t t (ξ,η H + ξ +η A u(ξ,η ε. ê r t t y R st α y ]0,[ t q r t t (ξ,η H + ξ +(η y < α y u(ξ,η ε. s t [ A, A] st t râ r r t s st α > 0 t q r t t y [ A,A] B(y,α s t s s s s B(y,α y y [ A,A] rt r s (ξ,η H + st t q 0 < ξ < α rs rs u(ξ,η ε q η s t s [ A,A] t r r r s t s ç s r tr r q s s t u L m (u = 0 s s r H + rs st t q t t r r rq s q rés t t st é é t r s m st t r t r str t t s t t s tr t t v é s r (R m+ R r v(x,...,x m+ = u( x + +x m+,x m+, rs r s t tr q v st r q s (R m+ R lim H + u = 0 lim {(0,...,0} R v = 0 r s t tr q v s r t r q s r R m+ t t t r t q lim H + u = 0 s tr s q lim x + v(x = 0 rés t q v st t q t t q u ss s é ér s s é è s ù m r s rs s q q s P P
33 P P P P P P Pr s t t u C (H + t q L m u = 0 t lim H +u = 0 rs u 0 s r H + Pr P r (ξ,η H + s r N N φ N (ξ,η = θ (Nξθ ( ξ N ( η θ N ù θ t θ s t s t s C s r R à rs s [0,] t t s q θ (t = r t θ (t = 0 r t θ (t = r t [, ] t θ (t = 0 r t R\],[ s s s q t t s s ér é s s t s θ t θ ts {,,,} s t s θ θ u st t C s r r t H + s t L m u = 0 rs uφ N st t ss C t à s rt t s r H + t (x,y H + q s r é s t t s t r P r N ss 3 r râ à r s t s E m st r é r F m u(x,y = u(x,yφ N (x,y = L m (uφ N F m dξdη H + r t L m (uφ N st t q t s s r té F m u(x,y = [L m (uφ N +ul m (φ N + u φ N ]F m dξdη H + = u[l m (φ N F m div (F m φ N ]dξdη H + = u[l m (φ N F m div (F m φ N ]dξdη D D 8 = u[l m (φ N F m + F m φ N ]dξdη D D 8 ù D,...,D 8 s t s s é ts s ts [ D = N, ] [ N N, N ] [, D = N, N ] [ ] N,N, P P
34 P P P P P P [ ] N D 3 =,N [ D 5 = N, ] N [ ] N D 7 =,N N [ N, N ] [, D 4 = [ N, N η [ ] N,N, D 6 = ] et D 8 = N, N ] [ ] [ N N,N,N [ N, ] N [ N, N, ], ], [ N, N ]. N/ D 5 D D 6 ND φ N D 3 ξ N N/ N D 8 D 4 D 7 N/ N r s D i lim H + u t 0 rs u N := sup (ξ,η D D 8 u(ξ,η N + 0. s s r r s té r s rt t s r D,...,D 8 P r s s r s s s s ts q t s r s st t s s t r s t N r D s s sup φ N ξ = O(N t sup φ N η = 0. r D D 4 s s ( sup φ N ξ = 0 t sup φ N η = O N r D 3 s s sup φ N ξ ( = O N t sup φ N η. = 0. P P
35 P P P P P P r D 5 D 8 s s ( sup φ N ξ = O(N t sup φ N η = O N. r D 6 D 7 s s ( sup φ N ξ = O N r D D 5 D 8 s s t sup φ N η ( = O N. r D D 3 D 4 D 6 D 7 s s sup L m (φ N = O(N. sup L m (φ N = O (. N Pr P r (ξ,η D φ N (ξ,η = θ (Nξ t φ N ξ (ξ,η = Nθ (Nξ φ N η (ξ,η = 0, q s sup D φ N ξ L m φ N (ξ,η = N θ (Nξ mn θ ξ (Nξ, = O(N, sup D φ N η = 0, sup D L m (φ N = O(N sq s ér é s θ s t r é s t q r (ξ,η D ξ N P r (ξ,η D φ N (ξ,η = θ ( η N t q s sup D φ N ξ = 0, φ N ξ (ξ,η = 0 φ N η (ξ,η = η N ( θ, N sup D st ê s r D 4 L m φ N (ξ,η = ( η N θ, N φ N η ( = O N (, sup L m (φ N = O D N P r (ξ,η D 3 φ N (ξ,η = θ ( ξ N t φ N ξ (ξ,η = ( ξ N θ N φ N η (ξ,η = 0, P P
36 P P P P P P q s sup D 3 φ N ξ L m φ N (ξ,η = ( ξ N θ ( m ξ N N ξ θ, N ( = O N, sup D 3 φ N η = 0, P r (ξ,η D 5 φ N (ξ,η = θ (Nξθ ( η N t φ ( N η ξ (ξ,η = Nθ (Nξθ N L m φ N (ξ,η = N θ (Nξθ ( η N q s sup D 5 φ N ξ = O(N, st ê s r D 8 sup D 5 φ N η ( sup L m (φ N = O D 3 N φ N η (ξ,η = η N θ (Nξθ (, N + ( η N θ (Nξθ N m ( η ξ Nθ (Nξθ N ( = O N, sup D 5 L m (φ N = O(N. ( P r (ξ,η D 6 φ N (ξ,η = θ ξ ( η N θ N t φ N ξ (ξ,η = ( ξ ( η φ N N θ θ N N η (ξ,η = ( ξ N θ N L m φ N (ξ,η = ( ξ ( η N θ θ + ( ξ ( η N N N θ θ N N m Nξ θ q s sup D 6 φ N ξ ( = O N, sup D 6 φ N η ( = O N st ê s r D 7 ù ( η θ N, ( ξ ( η θ N N (, sup L m (φ N = O. D 6 N s s t t st r s q t tés s t s r i {,..., 8} F m dξdη, ξ F m dξdη et η F m dξdη. D i D i D i P r Re m < s s r i = : ( F m dξdη = O, D i N r i =,4 : D i F m dξdη = O ( N, D i D i ( F m ξ dξdη = O N F m η dξdη = O(N. P P.
37 P P P P P P r i = 3 : D i F m dξdη = O ( N, D i D i F m ξ dξdη = O(N. r i = 5,8 : ( ( F m dξdη = O, F m D i N D i ξ dξdη = O N ( F m η dξdη = O. N r i = 6,7 : F m dξdη = O ( N, F m D i D i ξ dξdη = O(N, F m η dξdη = O(N. Pr P r m < s s D i, F m (ξ,η = ξx m π π θ=0 sin m θdθ [ (x ξ +4xξsin ( ] θ +(y η m. st st t C t q r t t (ξ,η H + t F m (ξ,η C ξ [(x ξ +(η y ] Rem. ê s s F m ξ = F π m ξ ξx m π (m θ=0 [(ξ x+xsin θ ]sin m θdθ [ (x ξ +4xξsin ( ] θ +(y η m, t r t θ [0,π], [(ξ x+xsin θ ]sin m θ ] +(y η m [ (x ξ +4xξsin ( θ (ξ x+xsin θ ( (x ξ +(η y Rem = ξ xcosθ ( (x ξ +(η y Rem ξ +x ( (x ξ +(η y, Rem st st t C t q r t t N ss 3 r t r t t (ξ,η H + t F m ξ C [ (x ξ +(η y ] Rem + ξ(x+ξ (. (x ξ +(η y Rem P P
38 P P P P P P F m η = ( m(η yξx m π π θ=0 sin m θ [ (x ξ +4xξsin ( ] θ +(y η m, st st t C 3 t q r t t N ss 3 r t r t t (ξ,η H + t F m η C 3 ξ η y 3 Rem. râ à s é tés s s st r s té r s s ér t s t s s r s s D i r D é té D F m dξdη = O( ξ= N ξ= N η= N η= N ξdξdη [(x ξ +(η y ] Rem η= N = O(/N η= N P s st t D F m ξ= ξ dξdη = O( N ξ= N dη [ (x N +(η y ] = O(/N. Rem η= N η= N [ (x ξ +(η y ] Rem ξ(x+ξ + ( dξdη (x ξ +(η y Rem η= N = O(/N η= N dη [ (x N +(η y ] +O(/N = O(/N. Rem r D é té D F m dξdη = O( N ξ= N N η= N ξdξdη [(x ξ +(η y ] Rem N N = O( ξ= η= N N [ = O(N P s é té D ξ N η y dξdη = Rem O(N η= N ] (N y Rem ( N y Rem N F m η dξdη = O( ξ= N N η= N dη η y Rem = O(N Rem+. ξ η y 3 Remdξdη P P
39 P P P P P P N = O(N η= N dη η y 3 Rem = O(NRem r D 3 é té D 3 F m dξdη = O( N ξ= N N η= N ξdξdη [(x ξ +(η y ] Rem N = O( ξ= N N η= N N = O(N η= N N = O(N η= N P s é té D 3 F m N ξ dξdη = O( ξ= N N η= N ξdξdη [ (x N +(η y ] Rem dη [ (x N +(η y ] Rem dη [+(η y ] Rem = O(N. [ (x ξ +(η y ] Rem ξ(x+ξ + ( dξdη (x ξ +(η y Rem N = O(N η= N dη [ (x N +(η y ] Rem = O(N+O(N 3 N N +O(N 3 η= N η= N dη (x N 4 Rem dη [ (x N +(η y ] Rem = O(N+O(N Rem = O(N. r D 4 s st s D r D 5 é té D 5 F m dξdη = O( N ξ= N N η= N ξdξdη [(x ξ +(η y ] Rem = O(/N [ N = O(/N η= N dη (η y Rem (N y Rem ( N y Rem ] = O(/N 3 Rem. P P
40 P P P P P P P s é té D 5 F m ξ= ξ dξdη = O( N ξ= N ξ= N η=n = O( ξ= η= N N é té D 5 η=n η= N [ (x N F m ξ= η dξdη = O( [ (x ξ +(η y ] Rem ξ(x+ξ + ( dξdη (x ξ +(η y Rem Rem +(η y ] + ( = O N N ξ= N ( (x N η=n η= N ξ(x+ξ Rem +(η y ( ξdξdη η y = O 3 Rem N dξdη r D 6 é té D 6 F m dξdη = O( N ξ= N N η= N ξdξdη [(x ξ +(η y ] Rem = O(N [ P s é té D 6 F m ξ=n ξ dξdη = O( N = O(N η= N dη (η y Rem (N y Rem ( N y Rem ξ= N η=n η= N ξ=n η=n [ = O( ξ= N η= N ] = O(N +Rem. [ (x ξ +(η y ] Rem ξ(x+ξ + ( dξdη (x ξ +(η y Rem ξ(x+ξ + (η y Rem (η y 4 Rem ] dξdη P P
41 P P P P P P N = O(N+O(N 3 η= N é té D 6 F m ξ=n η dξdη = O( ξ= N dη (η y 4 Rem = O(N+O(NRem = O(N. η=n η= N ξdξdη η=n η y = 3 Rem O(N η= N = O(N Rem. dη η y 3 Rem r D 7 s st s D 6 r D 8 s st s D 5 P r m t t s s st t s t s s s t s Pr P r m s s ( π F m (x,y,ξ,η = ξm sin m θ π θ=0 [(x ξ +4xξsin θ +(y η ] m/ [(x+ξ 4xξsin θ +(y dθ. η ] m/ r t t (ξ,η H + [ (x+ξ 4xξsin θ ] m/ +(y η = [ x +ξ +xξcosθ+(y η ] m/, rs r t t (ξ,η H + [ (x+ξ 4xξsin θ ] m/ +(y η ( (x ξ +(y η Rem t st st t C t q r t t (ξ,η H+ t F m C ξ Rem ((x ξ +(y η Rem. tt st t st r s t s s t r r r s t r s rt ts s r D s s r é té s t réé r t F m F m (x,y,ξ,η = ξm π π θ=0 sin m θk m (x,y,ξ,η,θdθ ù K m (x,y,ξ,η,θ = [(x ξ +4xξsin θ +(y η ] m/ P P
42 P P P P P P [(x+ξ 4xξsin θ +(y η ] m/. P r (x,y H + é θ [0,π] é t η R é é t t g m s r [ /N,/N] /N < x r g m (ξ = [(x ξ +4xξsin θ +(y η ] m/. tt t st é sq rt (x ξ +4xξsin θ +(y η = x +ξ xξcosθ+(y η (x ξ +(y η t q r r t r st ss ré r (x /N > 0 s s K m (x,y,ξ,η,θ = g m (ξ g m ( ξ K m (x,y,ξ,η,θ ξ sup g ξ x +x m m ξ [ ξ,ξ] [(x ξ +(y η ] Rem, + q q q st st t c t q ξ Rem+ (ξ,η D, F m c [ (x ξ +(η y ] + Rem. ê s s F m ξ = mf m + mξm ξ π t r t θ [0,π], = t râ à θ [0,π], = π θ=0 ( sin m (ξ x+xsin θ θ [(x ξ +4xξsin θ +(y η ] m + [(ξ x+xsin θ ]sinm θ [(x ξ +4xξsin θ +(y η ] m + (ξ +x xsin θ [(x+ξ 4xξsin θ +(y η ] m + ξ xcosθ [(x ξ +(y η ] ξ +x Rem + [(x ξ +(y η ] Rem [(ξ +x xsin θ ]sinm θ [(x+ξ 4xξsin θ +(y η ] m + ξ +xcosθ [(x ξ +(y η ] ξ +x Rem + [(x ξ +(y η ] Rem (ξ x+xsin θ [(x ξ +(y η ] Rem + + (ξ +x xsin θ [(x ξ +(y η ] Rem + +. P P dθ.
43 P P P P P P s st t s é s r t é té tr t q st st t C H + t ( F m ξ ξ Rem C [(x ξ +(y η ] Rem t q r t t N ss 3 r t r t t (ξ,η + ξ Rem (ξ +x [(x ξ +(y η ] Rem +. s s é r r tt é té s r D t s t é té t s t s q st s st t s C t C é t s N t s q r t t (ξ,η D ( F m ξ ξ Rem C F m η = m(η yξm π [(x ξ +(y η ] +Rem π θ=0 C ξ Rem + [(x ξ +(y η ] +Rem ξ Rem (ξ +x [(x ξ +(y η ] Rem + ( sin m θ [(x ξ +4xξsin θ +(y η ] m + [(x+ξ 4xξsin θ +(y dθ. η ] m + ê st st t C 3 t q r t t N ss 3 r t r t t (ξ,η H + t F m η η y ξ Rem C 3 ((x ξ +(y η. Rem + râ à s é tés s s st r s té r s s ér t s t s s r s s D i r D é té D F m dξdη = O( ξ= N ξ= N η= N η= N ξ Rem+ dξdη [ (x ξ +(η y ] + Rem [ ξ= ( Rem+ ( ] Rem+ N = O(N ξ Rem+ dξ = O(N ξ= N N N P s st t D F m ξ= ξ dξdη = O( = O(/N Rem+. N ξ= N η= N η= N ξ Rem dξdη [ (x ξ +(η y ] + Rem. P P
44 P P P P P P ξ= N = O(N ξ Rem dξ = O(/N Rem. ξ= N r D é té D F m dξdη = O( N ξ= N N η= N ξ Rem dξdη ((x ξ +(y η Rem N N = O( ξ= η= N N ξ Rem dξdη y N Rem = O(N, r q t té té ré st ré t ré é t N s t s r st O(N P s é té D N F m η dξdη = O( ξ= N N η= N η y ξ Rem dξdη ((x ξ +(y η Rem + N N = O( ξ= η= N N ξ Rem N dξdη N = O( y η Rem+ ξ= η= N N N Rem dξdη = O(N. y Rem+ N r D 3 é té D 3 F m dξdη = O( N ξ= N N η= N ξ Rem dξdη ((x ξ +(y η Rem N = O( ξ= N N = O(N Rem+ η= N P s é té D 3 F m N ξ dξdη = O( ξ= N N N η= N η= N ξ Rem dξdη ( (x N +(y η Rem dη ( = O(N. (x N +(y η Rem ( ξ Rem [(x ξ +(y η ] Rem + ξ Rem (ξ +x [(x ξ +(y η ] Rem + dξdη N = O(N Rem η= N dη [(x N +(y η ] Rem +O(N Rem+ N η= N = O(N+O(N = O(N. dη [(x N +(y η ] Rem + P P
45 P P P P P P r D 4 s st s D r D 5 é té D 5 F m dξdη = O( N ξ= N N η= N ξ Rem dξdη ((x ξ +(y η Rem P s é té D 5 N = O(/N Rem+ η= N F m ξ= ξ dξdη = O( N ξ= N η=n η= N ( dη y N Rem = O(/NRem. ξ Rem [(x ξ +(y η ] Rem + ξ Rem (ξ +x [(x ξ +(y η ] Rem + ξ= N η=n ( ξ Rem = O( ξ= η= N y η + ξrem (ξ +x Rem y η Rem+ N = O(/N Rem. dξdη dξdη é té D 5 F m ξ= η dξdη = O( N ξ= N η=n η= N η y ξ Rem dξdη ((x ξ +(y η Rem + ξ= N η=n = O( ξ= η= N N ξ Rem dξdη y η Rem+ = O(/NRem+ r D 6 é té D 6 F m dξdη = O( N ξ= N N η= N ξ Rem dξdη ((x ξ +(y η Rem P s é té D 6 N = O(N Rem+ η= N F m ξ=n ξ dξdη = O( ξ= N η=n η= N + dη ( N yrem = O(N. ( ξ Rem [(x ξ +(y η ] Rem ξ Rem (ξ +x [(x ξ +(y η ] Rem + ξ=n η=n ( ξ Rem = O( ξ= N η= N y η + ξrem (ξ +x Rem y η Rem+ dξdη dξdη P P
46 P P P P P P η=n = O(N+O(N Rem+ η= N dη = O(N. y η Rem+ é té D 6 F m ξ=n η dξdη = O( ξ= N η=n η= N η y ξ Rem dξdη ((x ξ +(y η Rem + η=n = O(N Rem+ η= N dη = O(N. y η Rem+ r D 7 s st s D 6 r D 8 s st s D 5 s t s t ré t s rés t ts t s s s s ré é ts i sup Di L m φ N D i F m dξdη ( ξ φ N, η φ N D i ξ F m D i η F m O(N O(/N (O(N,0 O( N O(/N O(N (0,O( N O(N O(/N O(N (O(,0 N O(N O(/N O(N (0,O( N O(N O(N O(/N (O(N,O( N O( N O( N O(/N O(N (O(,O( N N O(N O(N O(/N O(N (O(,O( N N O(N O(N O(N O(/N (O(N,O( N O( N O( N t sé t ér r q r q i {,..., 8} s q t tés sup L m φ N F m, sup ξ φ N ξ F m et sup η φ N η F m D i D i D i D i D i D i r st t r é s rés t q q N + s u(x,y = o( u 0 t r r s t P P
47 P P P P P P é rè é s t s P r m C s r s t é rè é s t s P s s r t r é s é rè s t s s r t t ér t sq s tr t té st ré é à tr rs r Ω é rè é s t t Ω rt H + t K s s s t Ω t u C (Ω \ K st s t L m u = 0 s Ω\K rs u q é s t r u = v +w ù v C (Ω st s t L m v = 0 s Ω t w C (H + \K st s t L m w = 0 s H + \K lim H +w = 0 Pr P r t t s s s E C tρ > 0 é te ρ = {x C, d(x,e < ρ} E ρ st s E t r s s q Ω st rt r t t t H + s t ρ ss 3 t t t s rt q K ρ t ( Ω ρ s t s ts st t ϕ ρ D(H + à s rt s Ω\K t q ϕ ρ s s Ω\(K ρ ( Ω ρ y K ρ Ω ( Ω ρ K ρ Ω\{K ρ ( Ω ρ } ρ x r ϕ ρ s rt r s t r é r P r z = x+iy Ω\(K ρ ( Ω ρ t t F z (ζ := F m (x,y,ξ,η t L ζ := L m,ξ,η pour ζ = ξ +iη, râ à r s t u(z = uϕ ρ (z = F z (ζl ζ (uϕ ρ (ζdξdη Ω ρ P P
48 P P P P P P = F z (ζl ζ (uϕ ρ (ζdξdη + F z (ζl ζ (uϕ ρ (ζdξdη ( Ω ρ K ρ = v ρ (z+w ρ (z. r r t tr rs q v ρ st s t L m v ρ = 0 s r Ω\( Ω ρ t q w ρ st s t L m w ρ = 0 s r H + \K ρ ss lim H + w ρ = 0 s s t t q σ < ρ rs ré é t t t é s t u = v σ +w σ s r Ω\(K σ ( Ω σ s r s q v ρ = v σ s r Ω\( Ω ρ t w ρ = w σ s r H + \K ρ P r r r rq s q s z Ω\(K ρ ( Ω ρ rs v ρ (z+w ρ (z = v σ (z+w σ (z t r ( éq t L m u = 0 s w ρ w σ st s t ( s H + \K ρ q st é à v σ v ρ s Ω\(K ρ ( Ω ρ t v σ v ρ s r s t ( s r Ω\( Ω ρ s w ρ w σ s r s t ( s H + t lim H +w ρ w σ = 0 r s t s rs t r s t v ρ = v σ w ρ = w σ, P r z Ω t é r v(z = v ρ (z r t t ρ ss 3 t t t s rt q z Ω\( Ω ρ ê èr r z H + \K s w(z = w ρ (z r ρ t t s s s rr és à é s t s té u = v +w s s t t q Ω s t H + q q t q u st s t L m u = 0 s r Ω\K s t a H + t R ss 3 r r q K D(a,R t q D(a,R s t r t t t s H + t ω = Ω D(a,R r rq q K st s s s t rt ω r t t t s H + t q u st s t ( s ω \K q t rés t t é tré r s s s rts r t t ts s s u(z = ṽ(z+ w(z r z ω\k ù ṽ st s t ( s ω t w st s t ( s H + \K s t s s t lim H + w = 0 t s q ér V = u w st s t ( s Ω\K t q s r s t ( s K r st é à ṽ s ω s u = V + w r t é s t s té u ré é t s tr é s t u = v +w v C (Ω L m v = 0 t w C (H + \ K L m w = 0 t lim H + w = 0 rs V v = w w s Ω \ K t w w s r à H + st s t L m (w w = 0 s H + t ér lim H +(w w = 0 râ à r s t t t w = w s V = v q è r r t é rè é s t r P ss r H + q Re m < P r Re m < t r r s t à rt Ω = H + r t r r r rés t t té r t r ss u s t L m (u = 0 s H + ss t s rs u s r s r é s P P H + RE M <
49 P P P P P P s rés t ts t t t t été t s r s s s s é èr t ér ts H + \ (0,a] {0} a > 0 r s t s s s ù m = ± s t q s q s r r r s s tr P s ré sé t s s Pr s t t m C t q Re m < t u : R R t t t r é rs st q P U ss C s r H + t q lim (x,y + U(x,y = 0 t t q r t t y R lim (0,y U = u(y. s s s r t t (x,y H + ù C m = m π U(x,y = C m x m η= π θ=0 sin m θdθ = Γ ( m m π Γ( m Pr t s f(x,y = x m u(η dη (x +(y η m P r tr r r r t r (x +(y η m s t s t tr r q L m f = 0 r ér t s s s té r t x f = ( mx m (x +(y η m ( mx m (x +(y η m xx f = m( mx m (x +(y η m ( m(3 mx m (x +(y η m + ( m(4 mx3 m (x +(y η 3 m s yy f = ( mx m (x +(y η m f = m( mx m (x +(y η m t é t q L m f(x,y = 0 U(x,y = C m x m η= u(η dη (x +(y η m P r t r t = y η t t x U(x,y = C m + ( m(4 m(y η x m. (x +(y η 3 m t= m( mx m (x +(y η m = C m x u(y txdt (+t m η= P r t é rè r é s t tr r q u(η dη (+( y η x m C m t= dt (+t m = m π π θ=0 sin m θdθ t= dt (+t m =. P P H + RE M <
50 P P P P P P P r r r rq s rès q t= dt (+t m ù B st t êt r t q m π π θ=0 ( = B, m = Γ(/Γ( m Γ ( m sin m θdθ = m ( π m B m, m = m P s t s t r t r t Γ ( Γ(z = π / z Γ(zΓ z + π mγ ( m Γ( m. t r ré rr Γ(z + = zγ(z t t rés t t st à r q Γ(/Γ ( m Γ ( m m π mγ ( m Γ( m =. té é r s t r é r s t rq rr t s s r q st st t r r r s t s Re m t s m st t r t r t s u C (H + s t L m (u = 0 s H + rs t v é s r R m+ r v(x,...,x m+ = u(0,x m+ t v(x,...,x m+ = u ( x + +x m+,x m+ st t r q s r (R m+ R rt r s m r s t tr q v s r t r q s r R m+ q t rs à é t q v st t t q t q u 0 q r q r è ét r t s t L m (u = 0 s t q u t rs 0 à t q s rs u s t s s r s r é s st r è q s s s s s s s t r è r t st séq rt t té éq t L m u = 0 r H + s tr t r s s s Rem s r r tt r s t s r t s s t s q s t s t r t t sé s s q s à tr ss s s s tr é ts r r s r t é t q s s r r s t t s s é t s t r s t s s s r é s r s s xoy s tr s s sstè r é s t sé r s s s r t rt èr t té à ét L t L s s ù ét é st sq tré H + PP
51 P P P P P P s t s ér q s s r s r è s tré r és t s t èr èt s r é s r s t été ré sé s s ré t t ès s r t α > 0 s ér s r s t é A = ( α,0 t r é t é B = (α,0 r s s r s ét t t q s t t ré r sstè r s t M st à st t t t rès ln ( MA MB P r é t r èr r é r st s r é r st τ := ln MA MB. θ = ÂMB. y M(x, y A( α, 0 θ O B(α, 0 x r r é s r s s r é s r s s t rs r é s r é s rtés s (x, y xoy r t q (α x iy ( α x iy = e τ+iθ (x α+iy = e τ+iθ [(x+α+iy] q s rès t t s rt s ré s t r s r x α = e τ [(α+xcosθ ysinθ] y = e τ [(α+xsinθ+ycosθ] x[ e τ cosθ]+ysinθ = α[e τ cosθ+] xe τ sinθ+y[ e τ cosθ] = αe τ sinθ. rés t sstè éq t s s r t t r é t t x = α s τ τ cosθ, y = αsinθ τ cosθ. r R > 0 t s s a = R +α sq tr (a,0 t r R rr s à ( a a τ τ 0 = ln R + R = arg ch a R. PP
52 P P P P P P s r t st H + = {(τ,θ : τ ]0+ ], θ [0,π[}. s s τ = τ 0 s t s r s tr (αcothτ 0,0 t r α/s τ 0 q q r t t τ 0,τ t s q 0 < τ 0 < τ s {τ τ 0 } st sq r é t s 0 < τ < τ st é t r s H + sq r é {τ τ } y τ = /3 θ = π/6 τ = /3 τ = / θ = π/3 τ = / θ = 0 τ = θ = π τ = x θ = 0 θ = 5π/3 θ = π/6 τ = 0 r s α = t s P r é s r s s q s t s t r s s t s r é s rtés s s t s r é s r s t é rè s t st r m = r s s s s ét s rs m s q q s é rè u ér L m u = 0 s rt H + t s s s s v m (τ,θ = s m τ( τ cosθ m/ u(τ,θ ù r é t s m τ( τ cosθ m/ = exp ( m ln s τ m ln( τ cosθ rs ( v m τ + v m θ +cothτ v m τ + 4 (m 4 s v m = 0. τ Pr s s u τ = α [ ] τ cosθ u s τ sinθ u ( τ cosθ x ( τ cosθ y PP
53 P P P P P P t s t s s s [ ] u s τ sinθ θ = α u τ cosθ u +. ( τ cosθ x ( τ cosθ y u x = α u τ = α ( τ cosθ 4 α + ( τ cosθ 3 t ( ( τ cosθ u s τ sinθ u, τ θ [ ( τ cosθ u x + s τ sin θ u y ] ( τ cosθs τ sinθ u x y [ s τ(cos θ+ τ cosθ u x +sinθ( τ +cosθ τ ] u y [ u θ = α ( τ cosθ 4 s τ sin θ u x +( τ u cosθ y ] +( τ cosθs τ sinθ u x y [ α + s τ( cos θ cosθ τ u ( τ cosθ 3 x +sinθ( τ τ cosθ u ] y t rt r s s t t q ( ( τ cosθ u L m,x,y u = α P s s t t u τ + u θ = α ( τ cosθ [ ] u x + u. y τ + u m( τ cosθ + θ s τ( τ cosθ u(τ,θ = ( τ cosθm/ v m (τ,θ s m τ t s L m,x,y u t F(τ,θ t t u τ msinθ τ cosθ u. θ t r m θ = r m (τ,θ = r m θ = m ( τ cosθm/, s m τ sinθ τ cosθ r m m 4( τ cosθ ( cosθ τ +msin θ r m PP
54 P P P P P P s t r m τ = ( τ cosθs τ ( τ +(m τ cosθ m r m r m τ = 4( τ cosθ s τ [ 4 τ 3 τ cosθ+(m τ cos θ+ +(m τ +(4 m τ cosθ+(m cos θ+m(m ] r m. éq t L m,x,y u = 0 s réé r t ( v m r m τ + v m θ t + v m τ + v m θ ( r m τ + m τ cosθ s τ τ cosθ r m + ( r m θ msinθ τ cosθ r m ( r m +v m τ + r m m( τ cosθ + θ s τ( τ cosθ r m τ + r m m( τ cosθ + θ s τ( τ cosθ è r tr t é rè r m τ msinθ τ cosθ r m τ + m τ cosθ s τ τ cosθ r m = r m cothτ, r m θ msinθ τ cosθ r m = 0 r m = 0 θ r m τ msinθ ( r m τ cosθ θ = 4 (m 4s r m. τ t t r v m s s r v m (τ,θ = A m (τb m (θ s t à r s sé ré s rt r éq t s t s t r v m t t A m A m +cothτ A m A m + 4 (m 4 s τ = B m B m. t r r t ét t t θ t t τ é t q s t r s s t st ts t n C t q tt st t s t é à n rs ( A m +cothτa m + 4 (m 4s n A m = 0, τ B m +n B m = 0. t B m ét t t r t π ér q r θ st é étr q t st t n t é ss r t êtr r t r PP
55 P P P P P P P r ét r éq t s t s t r A m s t s t t t C m ér rs éq t s τc m( τ+ τ C m( τ+ q t s réé r r s s r A m (τ = C m ( τ. ( τc m( τ τ C m( τ+ (n ( 4 n (m 4s C m ( τ = 0 τ 4 ((m / C m ( τ = 0. τ (LAH tt éq t st é éq t r ss é r q rq s q s s s s z = τ t u(z = C m ( τ rs ù ] ( z u zu + [ν(ν + µ u = 0 z (LA ν = n t µ = m. tt éq t st é éq t r ss é s ré t r µ = 0 à éq t r ( z u zu +ν(ν +u = 0. (L s s é r ss s s t s é t s tt éq t q s t s t s r ss é s r èr t è s è s t s r ss é s r èr t è s è s s s r s r s r rés t t té r s t s r r èr t è s è r z = τ > P µ ν ( τ = ν s µ τ Γ( µ νγ(ν + ν > t (µ+ν < 0 0 ( τ + θ µ ν s ν+ θdθ P ν µ ( τ = µ s µ τ π ( πγ µ 0 ( τ + s τ cosθ µ+ν sin µ dθ θ µ < µ < P µ ν ( τ = π s µ τ Γ ( µ τ 0 [( ] ν + θ ( τ θ µ+/dθ PP
56 P P P P P P Q µ ν( τ = eiπµ π s µ τγ(ν +µ+ s µ θ µ Γ(ν µ+γ(µ+/ 0 ( τ + s τ θ ν+µ+dθ µ > (µ ν < 0 t µ+ν + / Z µ < Q µ ν( τ = Q µ ν( τ = e iπµ π s µ τ eiπµ Γ ( e (ν+ θ µ τ ( θ τ µ+/dθ t (µ+ν + > 0 ν Γ(ν +µ+ Γ(ν + s µ τ π 0 ( τ +cosθ µ ν sin ν+ θdθ ν > t µ+ν + Z r s t s s s s r t s s t s ér é s r s t s r r t r P µ ν = P µ ν. Q µ ν (z = πeiπµ cos(πνp µ ν +sin[π(ν +µ]q µ ν sin[π(ν µ] r ν µ Z rt r r ν = n n Z s s q q s t µ C P µ ν Γ(ν µ+ Γ(ν +µ+ Q µ ν = Q µ ν e iπµ Γ(ν +µ+q µ ν = e iπµ Γ(ν µ+q µ ν, [ = P ν µ π e iπµ sin(πµq µ ν s s s s r s r t s t s r ss é s r èr t è s è r ], π Q µ ν( τ = e iπµ Γ(µ+ν + P ν (cothτ, s τ µ P µ ν ( τ = ie iπν Γ( ν µ π Q ν s τ µ (cothτ. s s ss s r s ré rr r s t P ν µ+ ( τ = (ν µ τ Pµ ν ( τ (ν +µp ν ( τ µ s τ (ν µ+p µ ν+( τ = (ν + τ P µ ν ( τ (ν +µp µ ν ( τ. (z dpµ ν (z dz = (ν +µ(ν µ+(z / P ν µ (z µzp ν µ (z. (z dpµ ν (z dz = νzp µ ν (z (ν +µp µ ν (z. PP
57 P P P P P P t s s r s r tt t r t t s rs P µ ν ( τ t Q µ ν( τ r t t τ > 0 t t s (µ,ν C r s t s t r ss à µ t τ és rt t s t s r ss é s r èr t è s è rsq ν st r ν = n n Z t q n + Pr s t t τ > 0 t µ C és t s s rs s ν st r ν = n n Z s s q ν +, P µ ν ( τ eτ/ π s τ ν µ / e τν q ν, P µ ν ( τ e τ/ π s τ ( ν µ / e τν q ν +, q ν, Q µ ν( τ e iπµ e τ/ π s τ νµ / e τν Q µ ν( τ e iπµ e τ/ π s τ ( νµ / e τν. s éq s s t s t r s r r rt à τ st à r r s s t t t r [τ 0,τ ] 0 < τ 0 < τ Pr P µ ν ( τ = s s r t t ν q st r n n N r Γ(ν + [ e (ν+ τ +e πi(µ (ν+ τ] [ +O Γ(ν µ+ π(ν +s τ t r t r tr q q ν + Γ(ν + Γ(ν µ+ ( πν ν+/ e ν ν+/ ν π(ν µ ν µ+/ e = (ν µ µ e µ ν+µ ν µ ( ( = (ν µ µ e µ exp ν + ( ln µ ν µ ν ( ]. ν P µ ν ( τ ν µ πνs τ e τ e τν = eτ/ πs τ ν µ / e τν, q s r èr st t s s t t r t t à rt r r t P µ ν = P µ ν tr s è st t é r t t r Q µ ν( τ π s τ νµ / e iπµ e τ(ν+/ t r èr é t q r ν = n n Z s s Q µ ν = Q µ ν. PP
58 P P P P P P r tèr r s éq ts é s r s s r ss s t s s P ν µ tqµ ν à s t s r é étr q s t s t s st t s s t s r é étr q s t r s r r rt à rs r ètr s s s s r r t t q t é ( τ cosθm/ s m τ { cos(nθ sin(nθ } P m ( τ n Q m ( τ n st s s s s t s à tér r sq τ τ t tr t é st s s s s t s s τ τ 0 q st é t r s H + sq t ù 0 < τ 0 < τ t st r m = st à r r µ = s ét s s ù m st q q n Z. é rè t m C t 0 < τ 0 t u s t ss L m u = 0 s sq τ τ 0 t s t v s t ss L m v = 0 s H + \ {τ > τ 0 } q st é t r s H + sq {τ > τ 0 } q s s r r H + lim H + v = 0 rs st s t s (a n n Z t (b n n Z s l (Z q s t ê à é r ss r t s q u = + n= a n Q m n ( τs m τ( τ cosθ m e inθ t v = + n= b n P m n ( τs m τ( τ cosθ m e inθ. s t (a n st q s r r èr sér st r s t t t [τ,τ ] τ 0 τ < τ sq τ > τ 0 t r s sér st r s t t t [τ 3,τ 4 ] 0 < τ 3 < τ 4 τ 0 é t r sq τ > τ 0 s H + s m st ré t m < rs s t (b n st q Pr t é s t θ u(τ 0,θ( τ 0 cosθ m/ s m τ 0 sér r r r r rt à θ é t r r r u(τ 0, u(τ 0,θ = s m τ 0 ( τ 0 cosθ m ù a n st s t l (Z q s t s t a n = π π 0 + n= a n e inθ, ( τ 0 cosθ m/ s m τ 0 u(τ 0,se ins ds. PP
59 P P P P P P tt t ét t ss r r rt à θ é t q s t (a n n st à é r ss r q n + t ũ(τ,θ = s m τ( τ cosθ m + n= Q m ( τ n a n Q m ( τ n 0 ï u s r r τ = τ 0 s râ à r s t s s q n + Q m ( τ n Q m ( τ n 0 s τ 0 s τ e n (τ 0 τ t t éq t st r s r t t t [τ,τ ] 0 < τ 0 τ < τ rés t q sér t s é ss t ũ r r t s r t s s ts [τ,τ ] sq τ τ 0 st ê s ér é s r r rt à τ t θ q s r t s ss à s t s r ss é s r é ré é t rt r t ũ st t é s r sq τ τ 0 t q ï u s r r τ = τ 0 râ t q s t éq t t q st ét r é èr q r s s rs r é r é t q ũ st q P s sq τ τ 0 q ï u s r r τ = τ 0 P r t v r st t t t t é s t θ v(τ 0,θ( τ 0 cosθ m/ s m τ 0 e inθ sér r r r r rt à θ é t r r r v(τ 0, v(τ 0,θ = s m τ 0 ( τ 0 cosθ m ù b n st s t l (Z q s t s t b n = π π 0 + n= b n e inθ, ( τ 0 cosθ m/ s m τ 0 v(τ 0,se ins ds. tt t ét t ss r r rt à θ é t q s t (b n n st à é r ss r q n + t ṽ(τ,θ = s m τ( τ cosθ m ï v s r r τ = τ 0 + n= P m ( τ n b n P m ( τ n 0 e inθ PP
60 P P P P P P s râ à r s t s s q n + P m ( τ n P m ( τ n 0 s τ 0 s τ e n (τ τ 0 t t éq t st r s r t t t [τ,τ ] 0 < τ < τ τ 0 rés t q sér t s é ss t ṽ r r t s r t s s ts [τ,τ ] é t r sq τ > τ 0 st ê s ér é s r r rt à τ t θ q s r t s ss à s t s r ss é s r é ré é t rt r t ṽ st t é s r é t r sq τ > τ 0 t q ï v s r r τ = τ 0 s s r r q lim τ 0+ṽ = 0. m < s s q n N t râ à P m ( τ = n m πγ ( m s m τ π 0 lim P m ( τ = 0 τ 0+ n t s r n > Rem s s P m n Rem s Rem Rem ( τ π Γ ( m τ π s Rem τ π Γ ( m 0 π 0 ( τ + s τ cosθ n+m sin m θdθ ( τ + s τ cosθ n+rem sin Rem θdθ ( τ + s τ n+rem sin Rem θdθ C m s Rem τe (n+rem τ n> Rem sup τ [0, τ 0 ] P m ( τ n b n P m ( τ n 0 râ t q r s t s P m ( τ n 0 n + e inθ < + n m π s τ0 e nτ 0. s s é r q lim τ 0+ ṽ = 0 r st à r r té é s t ré é t s s ù m R m < é r r r s t q ét r t q Q m ( τ n ( τ cosθ m/ A := Q m ( τ n 0 s m τ e inθ n Z := (a n n Z PP
61 P P P P P P B := r s s3 P m ( τ n P m ( τ n ( τ cosθ m/ s m τ e inθ n Z := (b n n Z r r s t r è r t L m u = 0 s D((a,0,R ù u = ϕ s r D((a,0,R st é r u(τ,θ = s m τ( τ cosθ m + n= Q m ( τ n c n Q m ( τ n 0 ù {τ = τ 0 } rr s r tr (a,0 t r R t ù ê c n = π π 0 e inθ ( τ 0 cosθ m/ s m τ 0 ϕ(a+rcoss,rsinse ins ds. v(τ,θ = s m τ( τ cosθ m + n= P m ( τ n c n P m ( τ n 0 st s t L m v = 0 s H + \D((a,0,R é à ϕ s r D((a,0,R ù c n = π π 0 e inθ ( τ 0 cosθ m/ s m τ 0 ϕ(a+rcoss,rsinse ins ds. s m st ré t ér m < rs v ér lim H + v = 0 t t v ré é t str t st s s t r è r t L m v = 0 s H + \D((a,0,R q s s r H + s s s3 P r m ré s s t ré é t q s s t s t r r r L m u = 0 r t èt s tt s t tr r q r m ré tt st ê s s3 rt s rt é t t r r été s r s é t é ér t r r été s s s s3 r é t t X s rt t (x n n N s t X P P M
62 P P P P P P t q st s t q s rt s t s3 s st st t s c, C > 0 t s q r t t s t (a n n Z t r t r s s c a n a n x n C a n. n n n s s ù (x n n Z st èt r s s3 tr s r t s r { x i,x j } i,j st é tr r ss é à {x i } i s t s r q s t {x i } i s t s s3 t é t êtr r é t tr r Pr r été {x i } i st s s3 r s rt s {x i } i st èt s t s rt t q s tr r é t ér t r rs t r é s r l (N s s3 s s t s t r r r ta tb s s s t s éq t L m [u] = 0 r s t t à tér r sq τ > τ 0 t à tér r tr sq τ > τ 0 < τ 0 < τ Q m ( τ n A := ( τ cosθ m/ e inθ := (a Q m ( τ n 0 s m n n Z τ B := P m ( τ n P m ( τ n ( τ cosθ m/ s m τ t C ré s s ré é t s e inθ n Z n Z := (b n n Z C := (c n n Z := (c n = a n t c n+ = b n n Z é t s r é s r s r {0 < τ 0 < τ < τ } s r té A t C r t s r s t r f,g L ( A f,g = π π 0 s m τ 0 f(τ 0,θg(τ 0,θ ( τ 0 cosθ θ m r s t s t + π π 0 s m τ f(τ,θg(τ,θ ( τ cosθ θ. m Pr s t C r s s3 r s rt L ( A P P M
Couplage dans les applications interactives de grande taille
Couplage dans les applications interactives de grande taille Jean-Denis Lesage To cite this version: Jean-Denis Lesage. Couplage dans les applications interactives de grande taille. Réseaux et télécommunications
Physique des réacteurs à eau lourde ou légère en cycle thorium : étude par simulation des performances de conversion et de sûreté
Physique des réacteurs à eau lourde ou légère en cycle thorium : étude par simulation des performances de conversion et de sûreté Alexis Nuttin To cite this version: Alexis Nuttin. Physique des réacteurs
Annulations de la dette extérieure et croissance. Une application au cas des pays pauvres très endettés (PPTE)
Annulations de la dette extérieure et croissance. Une application au cas des pays pauvres très endettés (PPTE) Khadija Idlemouden To cite this version: Khadija Idlemouden. Annulations de la dette extérieure
Transformations d Arbres XML avec des Modèles Probabilistes pour l Annotation
Transformations d Arbres XML avec des Modèles Probabilistes pour l Annotation Florent Jousse To cite this version: Florent Jousse. Transformations d Arbres XML avec des Modèles Probabilistes pour l Annotation.
Radio détection des rayons cosmiques d ultra-haute énergie : mise en oeuvre et analyse des données d un réseau de stations autonomes.
Radio détection des rayons cosmiques d ultra-haute énergie : mise en oeuvre et analyse des données d un réseau de stations autonomes. Diego Torres Machado To cite this version: Diego Torres Machado. Radio
Émergence des représentations perceptives de la parole : Des transformations verbales sensorielles à des éléments de modélisation computationnelle
Émergence des représentations perceptives de la parole : Des transformations verbales sensorielles à des éléments de modélisation computationnelle Anahita Basirat To cite this version: Anahita Basirat.
ACI sécurité informatique KAA (Key Authentification Ambient)
ACI sécurité informatique KAA (Key Authentification Ambient) Samuel Galice, Veronique Legrand, Frédéric Le Mouël, Marine Minier, Stéphane Ubéda, Michel Morvan, Sylvain Sené, Laurent Guihéry, Agnès Rabagny,
Consommation marchande et contraintes non monétaires au Canada ( )
Consommation marchande et contraintes non monétaires au Canada (1969-2008) Julien Boelaert, François Gardes To cite this version: Julien Boelaert, François Gardes. Consommation marchande et contraintes
Forêts aléatoires : aspects théoriques, sélection de variables et applications
Forêts aléatoires : aspects théoriques, sélection de variables et applications Robin Genuer To cite this version: Robin Genuer. Forêts aléatoires : aspects théoriques, sélection de variables et applications.
Robust Segmentation of Focal Lesions on Multi-Sequence MRI in Multiple Sclerosis
Robust Segmentation of Focal Lesions on Multi-Sequence MRI in Multiple Sclerosis Daniel García-Lorenzo To cite this version: Daniel García-Lorenzo. Robust Segmentation of Focal Lesions on Multi-Sequence
Transfert sécurisé d Images par combinaison de techniques de compression, cryptage et de marquage
Transfert sécurisé d Images par combinaison de techniques de compression, cryptage et de marquage José Marconi Rodrigues To cite this version: José Marconi Rodrigues. Transfert sécurisé d Images par combinaison
Jeux d inondation dans les graphes
Jeux d inondation dans les graphes Aurélie Lagoutte To cite this version: Aurélie Lagoutte. Jeux d inondation dans les graphes. 2010. HAL Id: hal-00509488 https://hal.archives-ouvertes.fr/hal-00509488
Langages dédiés au développement de services de communications
Langages dédiés au développement de services de communications Nicolas Palix To cite this version: Nicolas Palix. Langages dédiés au développement de services de communications. Réseaux et télécommunications
Modèles de représentation multi-résolution pour le rendu photo-réaliste de matériaux complexes
Modèles de représentation multi-résolution pour le rendu photo-réaliste de matériaux complexes Jérôme Baril To cite this version: Jérôme Baril. Modèles de représentation multi-résolution pour le rendu
Vers un assistant à la preuve en langue naturelle
Vers un assistant à la preuve en langue naturelle Thévenon Patrick To cite this version: Thévenon Patrick. Vers un assistant à la preuve en langue naturelle. Autre [cs.oh]. Université de Savoie, 2006.
Contribution à l évolution des méthodologies de caractérisation et d amélioration des voies ferrées
Contribution à l évolution des méthodologies de caractérisation et d amélioration des voies ferrées Noureddine Rhayma To cite this version: Noureddine Rhayma. Contribution à l évolution des méthodologies
Multi-GPU numerical simulation of electromagnetic waves
Multi-GPU numerical simulation of electromagnetic waves Philippe Helluy, Thomas Strub To cite this version: Philippe Helluy, Thomas Strub. Multi-GPU numerical simulation of electromagnetic waves. ESAIM:
E fficient computational tools for the statistical analysis of shape and asymmetryof 3D point sets
E fficient computational tools for the statistical analysis of shape and asymmetryof 3D point sets Benoît Combès To cite this version: Benoît Combès. E fficient computational tools for the statistical
Analysis of a discrete element method and coupling with a compressible fluid flow method
Analysis of a discrete element method and coupling with a compressible fluid flow method Laurent Monasse To cite this version: Laurent Monasse. Analysis of a discrete element method and coupling with a
P r s r r t. tr t. r P
P r s r r t tr t r P r t s rés t t rs s r s r r t é ér s r q s t r r r r t str t q q s r s P rs t s r st r q r P P r s r r t t s rés t t r t s rés t t é ér s r q s t r r r r t r st r q rs s r s r r t str
Points de torsion des courbes elliptiques et équations diophantiennes
Points de torsion des courbes elliptiques et équations diophantiennes Nicolas Billerey To cite this version: Nicolas Billerey. Points de torsion des courbes elliptiques et équations diophantiennes. Mathématiques
Network Neutrality Debate and ISP Inter-Relations: Traffi c Exchange, Revenue Sharing, and Disconnection Threat
Network Neutrality Debate and ISP Inter-Relations: Traffi c Exchange, Revenue Sharing, and Disconnection Threat Pierre Coucheney, Patrick Maillé, runo Tuffin To cite this version: Pierre Coucheney, Patrick
Hygromécanique des panneaux en bois et conservation du patrimoine culturel. Des pathologies... aux outils pour la conservation
Hygromécanique des panneaux en bois et conservation du patrimoine culturel. Des pathologies... aux outils pour la conservation Bertrand Marcon To cite this version: Bertrand Marcon. Hygromécanique des
Résolution de problème inverse et propagation d incertitudes : application à la dynamique des gaz compressibles
Résolution de problème inverse et propagation d incertitudes : application à la dynamique des gaz compressibles Alexandre Birolleau To cite this version: Alexandre Birolleau. Résolution de problème inverse
Logique et Interaction : une Étude Sémantique de la
Logique et Interaction : une Étude Sémantique de la Totalité Pierre Clairambault To cite this version: Pierre Clairambault. Logique et Interaction : une Étude Sémantique de la Totalité. Autre [cs.oh].
Chemical and biological evaluations of an (111)in-labeled RGD-peptide targeting integrin alpha(v) beta(3) in a preclinical tumor model.
Chemical and biological evaluations of an (111)in-labeled RGD-peptide targeting integrin alpha(v) beta(3) in a preclinical tumor model. Mitra Ahmadi, Lucie Sancey, Arnaud Briat, Laurent Riou, Didier Boturyn,
Microscopie photothermique et endommagement laser
Microscopie photothermique et endommagement laser Annelise During To cite this version: Annelise During. Microscopie photothermique et endommagement laser. Physique Atomique [physics.atom-ph]. Université
Traitement STAP en environnement hétérogène. Application à la détection radar et implémentation sur GPU
Traitement STAP en environnement hétérogène. Application à la détection radar et implémentation sur GPU Jean-François Degurse To cite this version: Jean-François Degurse. Traitement STAP en environnement
Solving an Air Conditioning System Problem in an Embodiment Design Context Using Constraint Satisfaction Techniques
Solving an Air Conditioning System Problem in an Embodiment Design Context Using Constraint Satisfaction Techniques Raphael Chenouard, Patrick Sébastian, Laurent Granvilliers To cite this version: Raphael
r t t r t t à ré ér t é r t st é é t r s s2stè s t rs ts t s
r t r r é té tr q tr t q t t q t r t t rrêté stér ût Prés té r ré ér ès r é r r st P t ré r t érô t 2r ré ré s r t r tr q t s s r t t s t r tr q tr t q t t q t r t t r t t r t t à ré ér t é r t st é é
Stéphane Bancelin. Imagerie Quantitative du Collagène par Génération de Seconde Harmonique.
Imagerie Quantitative du Collagène par Génération de Seconde Harmonique Stéphane Bancelin To cite this version: Stéphane Bancelin. Imagerie Quantitative du Collagène par Génération de Seconde Harmonique.
Mesh Parameterization: Theory and Practice
Mesh Parameterization: Theory and Practice Kai Hormann, Bruno Lévy, Alla Sheffer To cite this version: Kai Hormann, Bruno Lévy, Alla Sheffer. Mesh Parameterization: Theory and Practice. This document is
Fusion de données multicapteurs pour la construction incrémentale du modèle tridimensionnel texturé d un environnement intérieur par un robot mobile
Fusion de données multicapteurs pour la construction incrémentale du modèle tridimensionnel texturé d un environnement intérieur par un robot mobile Ayman Zureiki To cite this version: Ayman Zureiki. Fusion
DYNAMICS OF CHANGE WITHIN LIVESTOCK SUB-SECTOR IN CHAD : a key-study of raw milk commodity chain in N Djamena
DYNAMICS OF CHANGE WITHIN LIVESTOCK SUB-SECTOR IN CHAD : a key-study of raw milk commodity chain in N Djamena Koussou Mian Oudanang To cite this version: Koussou Mian Oudanang. DYNAMICS OF CHANGE WITHIN
Conditions aux bords dans des theories conformes non unitaires
Conditions aux bords dans des theories conformes non unitaires Jerome Dubail To cite this version: Jerome Dubail. Conditions aux bords dans des theories conformes non unitaires. Physique mathématique [math-ph].
Coupling strategies for compressible - low Mach number flows
Coupling strategies for compressible - low Mach number flows Yohan Penel, Stéphane Dellacherie, Bruno Després To cite this version: Yohan Penel, Stéphane Dellacherie, Bruno Després. Coupling strategies
La naissance de la cohomologie des groupes
La naissance de la cohomologie des groupes Nicolas Basbois To cite this version: Nicolas Basbois. La naissance de la cohomologie des groupes. Mathématiques [math]. Université Nice Sophia Antipolis, 2009.
Profiterole : un protocole de partage équitable de la bande passante dans les réseaux ad hoc
Profiterole : un protocole de partage équitable de la bande passante dans les réseaux ad hoc Rémi Vannier To cite this version: Rémi Vannier. Profiterole : un protocole de partage équitable de la bande
Three essays on trade and transfers: country heterogeneity, preferential treatment and habit formation
Three essays on trade and transfers: country heterogeneity, preferential treatment and habit formation Jean-Marc Malambwe Kilolo To cite this version: Jean-Marc Malambwe Kilolo. Three essays on trade and
Développement d un nouveau multi-détecteur de neutrons
Développement d un nouveau multi-détecteur de neutrons M. Sénoville To cite this version: M. Sénoville. Développement d un nouveau multi-détecteur de neutrons. Physique Nucléaire Expérimentale [nucl-ex].
Une Théorie des Constructions Inductives
Une Théorie des Constructions Inductives Benjamin Werner To cite this version: Benjamin Werner. Une Théorie des Constructions Inductives. Génie logiciel [cs.se]. Université Paris- Diderot - Paris VII,
Transformation automatique de la parole - Etude des transformations acoustiques
Transformation automatique de la parole - Etude des transformations acoustiques Larbi Mesbahi To cite this version: Larbi Mesbahi. Transformation automatique de la parole - Etude des transformations acoustiques.
Algorithmique et télécommunications : Coloration et multiflot approchés et applications aux réseaux d infrastructure
Algorithmique et télécommunications : Coloration et multiflot approchés et applications aux réseaux d infrastructure Hervé Rivano To cite this version: Hervé Rivano. Algorithmique et télécommunications
Voice over IP Vulnerability Assessment
Voice over IP Vulnerability Assessment Humberto Abdelnur To cite this version: Humberto Abdelnur. Voice over IP Vulnerability Assessment. Networking and Internet Architecture [cs.ni]. Université Henri
Segmentation d IRM cérébrales multidimensionnelles par coupe de graphe
Segmentation d IRM cérébrales multidimensionnelles par coupe de graphe Jérémy Lecoeur To cite this version: Jérémy Lecoeur. Segmentation d IRM cérébrales multidimensionnelles par coupe de graphe. Informatique
Pathological synchronization in neuronal populations : a control theoretic perspective
Pathological synchronization in neuronal populations : a control theoretic perspective Alessio Franci To cite this version: Alessio Franci. Pathological synchronization in neuronal populations : a control
SPFC: a tool to improve water management and hay production in the Crau region
SPFC: a tool to improve water management and hay production in the Crau region J.C. Mailhol, A. Merot To cite this version: J.C. Mailhol, A. Merot. SPFC: a tool to improve water management and hay production
Interaction hydrodynamique entre deux vésicules dans un cisaillement simple
Interaction hydrodynamique entre deux vésicules dans un cisaillement simple Pierre-Yves Gires To cite this version: Pierre-Yves Gires. Interaction hydrodynamique entre deux vésicules dans un cisaillement
Pierre Grandemange. To cite this version: HAL Id: tel https://tel.archives-ouvertes.fr/tel
Piégeage et accumulation de positons issus d un faisceau pulsé produit par un accélérateur pour l étude de l interaction gravitationnelle de l antimatière Pierre Grandemange To cite this version: Pierre
Les gouttes enrobées
Les gouttes enrobées Pascale Aussillous To cite this version: Pascale Aussillous. Les gouttes enrobées. Fluid Dynamics. Université Pierre et Marie Curie - Paris VI,. French. HAL Id: tel-363 https://tel.archives-ouvertes.fr/tel-363
Statistical analysis of extreme events in a nonstationary context via a Bayesian framework. Case study with peak-over-threshold data
Statistical analysis of extreme events in a nonstationary context via a Bayesian framework. Case study with peak-over-threshold data B. Renard, M. Lang, P. Bois To cite this version: B. Renard, M. Lang,
Jie He. To cite this version: HAL Id: halshs https://halshs.archives-ouvertes.fr/halshs
Pollution haven hypothesis and Environmental impacts of foreign direct investment: The Case of Industrial Emission of Sulfur Dioxide (SO2) in Chinese provinces Jie He To cite this version: Jie He. Pollution
Mohamed-Salem Louly. To cite this version: HAL Id: tel https://tel.archives-ouvertes.fr/tel
Deux modèles matématiques de l évolution d un bassin sédimentaire. Pénomènes d érosion-sédimentation-transport en géologie. Application en prospection pétrolière Moamed-Salem Louly To cite tis version:
UNIVERSITE DE PERPIGNAN VIA DOMITIA
Délivré par UNIVERSITE DE PERPIGNAN VIA DOMITIA Préparée au sein de l école doctorale Energie et Environnement Et de l unité de recherche Procédés, Matériaux et Énergie Solaire (PROMES-CNRS, UPR 8521)
ss rt çã r s t Pr r Pós r çã ê t çã st t t ê s 1 t s r s r s r s r q s t r r t çã r str ê t çã r t r r r t r s
P P P P ss rt çã r s t Pr r Pós r çã ê t çã st t t ê s 1 t s r s r s r s r q s t r r t çã r str ê t çã r t r r r t r s r t r 3 2 r r r 3 t r ér t r s s r t s r s r s ér t r r t t q s t s sã s s s ér t
A Convolutional Neural Network Approach for Objective Video Quality Assessment
A Convolutional Neural Network Approach for Objective Video Quality Assessment Patrick Le Callet, Christian Viard-Gaudin, Dominique Barba To cite this version: Patrick Le Callet, Christian Viard-Gaudin,
Modélisation de la réaction d alkylation du motif zinc-thiolate
Modélisation de la réaction d alkylation du motif zinc-thiolate Delphine Picot To cite this version: Delphine Picot. Modélisation de la réaction d alkylation du motif zinc-thiolate. Chimie. Ecole Polytechnique
Enzymatic Synthesis of Dithiolopyrrolone Antibiotics Using Cell-Free Extract of Saccharothrix
Enzymatic Synthesis of Dithiolopyrrolone Antibiotics Using Cell-Free Extract of Saccharothrix algeriensis NRRL B-24137 and Biochemical Characterization of Two Pyrrothine N-Acyltransferases in This Extract.
Développement de virus HSV-1 (virus de l herpes simplex de type 1) oncolytiques ciblés pour traiter les carcinomes hépatocellulaires
Développement de virus HSV-1 (virus de l herpes simplex de type 1) oncolytiques ciblés pour traiter les carcinomes hépatocellulaires Aldo Decio Pourchet To cite this version: Aldo Decio Pourchet. Développement
Measurement-driven mobile data traffic modeling in a large metropolitan area
Measurement-driven mobile data traffic modeling in a large metropolitan area Eduardo Mucelli Rezende Oliveira, Aline Carneiro Viana, Kolar Purushothama Naveen, Carlos Sarraute To cite this version: Eduardo
Geometric Tomography With Topological Guarantees
Geometric Tomography With Topological Guarantees Omid Amini, Jean-Daniel Boissonnat, Pooran Memari To cite this version: Omid Amini, Jean-Daniel Boissonnat, Pooran Memari. Geometric Tomography With Topological
Inflation Bias after the Euro: Evidence from the UK and Italy
Inflation Bias after the Euro: Evidence from the UK and Italy Pasquale Scaramozzino, Giancarlo Marini, Alessandro Piergallini To cite this version: Pasquale Scaramozzino, Giancarlo Marini, Alessandro Piergallini.
Des données anatomiques à la simulation de la locomotion : application à l homme, au chimpanzé, et à Lucy (A.L )
Des données anatomiques à la simulation de la locomotion : application à l homme, au chimpanzé, et à Lucy (A.L. 288-1) Guillaume Nicolas To cite this version: Guillaume Nicolas. Des données anatomiques
Analyse de modèles pour ITER ; Traitement des conditions aux limites de systèmes modélisant le plasma de bord dans un tokamak
Analyse de modèles pour ITER ; Traitement des conditions aux limites de systèmes modélisant le plasma de bord dans un tokamak Thomas Auphan To cite this version: Thomas Auphan. Analyse de modèles pour
P P Ó P. r r t r r r s 1. r r ó t t ó rr r rr r rí st s t s. Pr s t P r s rr. r t r s s s é 3 ñ
P P Ó P r r t r r r s 1 r r ó t t ó rr r rr r rí st s t s Pr s t P r s rr r t r s s s é 3 ñ í sé 3 ñ 3 é1 r P P Ó P str r r r t é t r r r s 1 t r P r s rr 1 1 s t r r ó s r s st rr t s r t s rr s r q s
Pax8 and Pax2 are specifically required at different steps of Xenopus pronephros development
Pax8 and Pax2 are specifically required at different steps of Xenopus pronephros development Isabelle Buisson, Ronan Le Bouffant, Mélinée Futel, Jean-François Riou, Muriel Umbhauer To cite this version:
r r t r r t t r t P s r t r P s r s r r rs tr t r r t s ss r P s s t r t t tr r r t t r t r r t t s r t rr t Ü rs t 3 r r r 3 rträ 3 röÿ r t
r t t r t ts r3 s r r t r r t t r t P s r t r P s r s r P s r 1 s r rs tr t r r t s ss r P s s t r t t tr r 2s s r t t r t r r t t s r t rr t Ü rs t 3 r t r 3 s3 Ü rs t 3 r r r 3 rträ 3 röÿ r t r r r rs
Modélisation / Contrôle de la chaîne d air des moteurs HCCI pour euro 7.
Modélisation / Contrôle de la chaîne d air des moteurs HCCI pour euro 7. Felipe Castillo Buenaventura To cite this version: Felipe Castillo Buenaventura. Modélisation / Contrôle de la chaîne d air des
Stratégies Efficaces et Modèles d Implantation pour les Langages Fonctionnels.
Stratégies Efficaces et Modèles d Implantation pour les Langages Fonctionnels. François-Régis Sinot To cite this version: François-Régis Sinot. Stratégies Efficaces et Modèles d Implantation pour les Langages
Approximation de haute précision des problèmes de diffraction.
Approximation de haute précision des problèmes de diffraction. Sophie Laurens To cite this version: Sophie Laurens. Approximation de haute précision des problèmes de diffraction.. Mathématiques [math].
rs r r â t át r st tíst Ó P ã t r r r â
rs r r â t át r st tíst P Ó P ã t r r r â ã t r r P Ó P r sã rs r s t à r çã rs r st tíst r q s t r r t çã r r st tíst r t r ú r s r ú r â rs r r â t át r çã rs r st tíst 1 r r 1 ss rt q çã st tr sã
AVERTISSEMENT. D'autre part, toute contrefaçon, plagiat, reproduction encourt une poursuite pénale. LIENS
AVERTISSEMENT Ce document est le fruit d'un long travail approuvé par le jury de soutenance et mis à disposition de l'ensemble de la communauté universitaire élargie. Il est soumis à la propriété intellectuelle
Alterazioni del sistema cardiovascolare nel volo spaziale
POLITECNICO DI TORINO Corso di Laurea in Ingegneria Aerospaziale Alterazioni del sistema cardiovascolare nel volo spaziale Relatore Ing. Stefania Scarsoglio Studente Marco Enea Anno accademico 2015 2016
Déformation et quantification par groupoïde des variétés toriques
Défomation et uantification pa goupoïde de vaiété toiue Fédéic Cadet To cite thi veion: Fédéic Cadet. Défomation et uantification pa goupoïde de vaiété toiue. Mathématiue [math]. Univeité d Oléan, 200.
Bandwidth mismatch calibration in time-interleaved analog-to-digital converters
Bandwidth mismatch calibration in time-interleaved analog-to-digital converters Fatima Ghanem To cite this version: Fatima Ghanem. Bandwidth mismatch calibration in time-interleaved analog-to-digital converters.
Spectres de diffusion Raman induits par les intéractions pour les bandes v2 et v3 de la molécule CO2 en gaz pur et en mélange avec de l argon
Spectres de diffusion Raman induits par les intéractions pour les bandes v2 et v3 de la molécule CO2 en gaz pur et en mélange avec de l argon Natalia Egorova To cite this version: Natalia Egorova. Spectres
P P Ô. ss rt çã r s t à rs r ç s rt s 1 ê s Pr r Pós r çã ís r t çã tít st r t
P P Ô P ss rt çã r s t à rs r ç s rt s 1 ê s Pr r Pós r çã ís r t çã tít st r t FELIPE ANDRADE APOLÔNIO UM MODELO PARA DEFEITOS ESTRUTURAIS EM NANOMAGNETOS Dissertação apresentada à Universidade Federal
Chromodynamique quantique sur réseau et propriétés du nucléon
Chromodynamique quantique sur réseau et propriétés du nucléon Rémi Baron To cite this version: Rémi Baron. Chromodynamique quantique sur réseau et propriétés du nucléon. Physique [physics]. Université
Łs t r t rs tø r P r s tø PrØ rø rs tø P r s r t t r s t Ø t q s P r s tr. 2stŁ s q t q s t rt r s t s t ss s Ø r s t r t. Łs t r t t Ø t q s
Łs t r t rs tø r P r s tø PrØ rø rs tø P r s r t t r s t Ø t q s P r s tr st t t t Ø t q s ss P r s P 2stŁ s q t q s t rt r s t s t ss s Ø r s t r t P r røs r Łs t r t t Ø t q s r Ø r t t r t q t rs tø
Assessment of otoacoustic emission probe fit at the workfloor
Assessment of otoacoustic emission probe fit at the workfloor t s st tt r st s s r r t rs t2 t P t rs str t t r 1 t s ér r tr st tr r2 t r r t s t t t r t s r ss r rr t 2 s r r 1 s r r t s s s r t s t
A Comparison of numerical simulation models for predicting temperature in solidification analysis with reference to air gap formation
A Comparison of numerical simulation models for predicting temperature in solidification analysis with reference to air gap formation J. Kron, Michel Bellet, Andreas Ludwig, Bjorn Pustal, Joachim Wendt,
AVERTISSEMENT. D'autre part, toute contrefaçon, plagiat, reproduction encourt une poursuite pénale. LIENS
AVERTISSEMENT Ce document est le fruit d'un long travail approuvé par le jury de soutenance et mis à disposition de l'ensemble de la communauté universitaire élargie. Il est soumis à la propriété intellectuelle
Raréfaction dans les suites b-multiplicatives
Raréfaction dans les suites b-multiplicatives Alexandre Aksenov To cite this version: Alexandre Aksenov. Raréfaction dans les suites b-multiplicatives. Mathématiques générales [math.gm]. Université Grenoble
Discouraging abusive behavior in privacy-preserving decentralized online social networks
Discouraging abusive behavior in privacy-preserving decentralized online social networks Álvaro García-Recuero To cite this version: Álvaro García-Recuero. Discouraging abusive behavior in privacy-preserving
Démembrement génétique des déficiences intellectuelles et compréhension des bases physiopathologiques associées, à l ère du séquençage à haut débit
Démembrement génétique des déficiences intellectuelles et compréhension des bases physiopathologiques associées, à l ère du séquençage à haut débit Maéva Langouët To cite this version: Maéva Langouët.
A Probabilistic Numerical Method for Fully Non-linear Parabolic Partial Differential Equations
A Probabilistic Numerical Metod for Fully Non-linear Parabolic Partial Differential Equations Aras Faim To cite tis version: Aras Faim. A Probabilistic Numerical Metod for Fully Non-linear Parabolic Partial
ss rt çã r s t à rs r ç s rt s 1 ê s Pr r Pós r çã ís r t çã tít st r t
ss rt çã r s t à rs r ç s rt s 1 ê s Pr r Pós r çã ís r t çã tít st r t FichaCatalografica :: Fichacatalografica https://www3.dti.ufv.br/bbt/ficha/cadastrarficha/visua... Ficha catalográfica preparada
m 1, m 2 F 12, F 21 F12 = F 21
m 1, m 2 F 12, F 21 F12 = F 21 r 1, r 2 r = r 1 r 2 = r 1 r 2 ê r = rê r F 12 = f(r)ê r F 21 = f(r)ê r f(r) f(r) < 0 f(r) > 0 m 1 r1 = f(r)ê r m 2 r2 = f(r)ê r r = r 1 r 2 r 1 = 1 m 1 f(r)ê r r 2 = 1 m
ss rt t r s t t t rs r ç s s rt t r t Pr r r q r ts P 2s s r r t t t t t st r t
Ô P ss rt t r s t t t rs r ç s s rt t r t Pr r r q r ts P 2s s r r t t t t t st r t FichaCatalografica :: Fichacatalografica https://www3.dti.ufv.br/bbt/ficha/cadastrarficha/visua... Ficha catalográfica
Raisonnement équationnel et méthodes de combinaison: de la programmation à la preuve
Raisonnement équationnel et méthodes de combinaison: de la programmation à la preuve Christophe Ringeissen To cite this version: Christophe Ringeissen. Raisonnement équationnel et méthodes de combinaison:
LEM. Non-linear externalities in firm localization. Giulio Bottazzi Ugo Gragnolati * Fabio Vanni
LEM WORKING PAPER SERIES Non-linear externalities in firm localization Giulio Bottazzi Ugo Gragnolati * Fabio Vanni Institute of Economics, Scuola Superiore Sant'Anna, Pisa, Italy * University of Paris
Multi-scale method for modeling thin sheet buckling under residual stress : In the context of cold strip rolling
Multi-scale method for modeling thin sheet buckling under residual stress : In the context of cold strip rolling Rebecca Nakhoul To cite this version: Rebecca Nakhoul. Multi-scale method for modeling thin
(ii) x[y (x)] 4 + 2y(x) = 2x. (vi) y (x) = x 2 sin x
ΕΥΓΕΝΙΑ Ν. ΠΕΤΡΟΠΟΥΛΟΥ ΕΠΙΚ. ΚΑΘΗΓΗΤΡΙΑ ΤΜΗΜΑ ΠΟΛΙΤΙΚΩΝ ΜΗΧΑΝΙΚΩΝ ΠΑΝΕΠΙΣΤΗΜΙΟ ΠΑΤΡΩΝ ΑΣΚΗΣΕΙΣ ΓΙΑ ΤΟ ΜΑΘΗΜΑ «ΕΦΑΡΜΟΣΜΕΝΑ ΜΑΘΗΜΑΤΙΚΑ ΙΙΙ» ΠΑΤΡΑ 2015 1 Ασκήσεις 1η ομάδα ασκήσεων 1. Να χαρακτηρισθούν πλήρως
ON THE MEASUREMENT OF
ON THE MEASUREMENT OF INVESTMENT TYPES: HETEROGENEITY IN CORPORATE TAX ELASTICITIES HENDRIK JUNGMANN, SIMON LORETZ WORKING PAPER NO. 2016-01 t s r t st t t2 s t r t2 r r t t 1 st t s r r t3 str t s r ts
Prés té r t r P Ô P P é té r t q r t t r2 t r t r t q s t r s t s t t s à t té rt rs r r ss r s rs tés r r ss r s rs tés 1 1 t rs r st r ss r s rs tés P r s 13 è îtr ér s r P rr îtr ér s rt r îtr ér s
γ 1 6 M = 0.05 F M = 0.05 F M = 0.2 F M = 0.2 F M = 0.05 F M = 0.05 F M = 0.05 F M = 0.2 F M = 0.05 F 2 2 λ τ M = 6000 M = 10000 M = 15000 M = 6000 M = 10000 M = 15000 1 6 τ = 36 1 6 τ = 102 1 6 M = 5000
Σηµειώσεις Μιγαδικής Ανάλυσης Θέµης Μήτσης
Σηµειώσεις Μιαδικής Ανάλυσης Θέµης Μήτσης Τµηµα Μαθηµατικων Πανεπιστηµιο Κρητης Ηρακλειο Περιεχόµενα Κεφάλαιο 1. Εισαωικά 5 Η αλεβρική δοµή 5 Η τοπολοική δοµή τού 6 Το εκτεταµένο µιαδικό επίπεδο 7 Συνεκτικότητα
VISCOUS FLUID FLOWS Mechanical Engineering
NEER ENGI STRUCTURE PRESERVING FORMULATION OF HIGH VISCOUS FLUID FLOWS Mechanical Engineering Technical Report ME-TR-9 grad curl div constitutive div curl grad DATA SHEET Titel: Structure preserving formulation
1. (a) (5 points) Find the unit tangent and unit normal vectors T and N to the curve. r(t) = 3cost, 4t, 3sint
1. a) 5 points) Find the unit tangent and unit normal vectors T and N to the curve at the point P, π, rt) cost, t, sint ). b) 5 points) Find curvature of the curve at the point P. Solution: a) r t) sint,,
m i N 1 F i = j i F ij + F x
N m i i = 1,..., N m i Fi x N 1 F ij, j = 1, 2,... i 1, i + 1,..., N m i F i = j i F ij + F x i mi Fi j Fj i mj O P i = F i = j i F ij + F x i, i = 1,..., N P = i F i = N F ij + i j i N i F x i, i = 1,...,