admits at least three solutions
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(2) 82. DIEGO AVERNA - GABRIELE BONANNO. A weak solution to problem (P) is a function u ∈ W 1, p() such that |∇u(x )| p−2∇u(x )∇v(x ) dx + a(x )|u(x )| p−2u(x )v(x ) dx . . −λ. . f (x , u(x ))v(x ) dx = 0, ∀ v ∈ W 1, p ().. Problems of the above type were widely studied in these latest years and we refer to [1], [2], [5], [7], [8], (see also [6] and [9], for the case n = 1 and p = 2) and the references therein for more details. In particular, in [7] the authors obtained the existence of an open interval ⊆ [0, ∞[ such that for each λ ∈ problem (P) admits at least three weak solutions which are uniformly bounded with respect to λ, without, however, establishing where is located; while in [8], under a different set of assumptions, the existence of three weak solutions to (P) for λ = 1 was proved. The aim of this note is to establish the existence of a precise open interval ]λ , λ [, 0 < λ < λ ≤ +∞, for each λ of which problem (P) admits at least three weak solutions. Our main result is Theorem 1 and, as a way of example, we present, here, a particular case. Theorem A. Let h : R → R be a bounded continuous function such that δ h(u) = 0 and h(u) du > 0 for some δ > 0. lim u→0+ u 0 Then, for every non-negative function g ∈ C 0 ([0, 1]) such that g 1 >. 2. δ 0. δ2 h(u) du. the problem (P1). −u + u = g(t)h(u) u (0) = u (1) = 0,. admits at least two non-negative and non-trivial classical solutions. Example 2 at the end of the paper shows a Neumann problem that, owing to our results, admits three solutions, but to which Theorem 2.1 of [8] cannot be applied. Our results are based on the following recent three critical points theorem obtained in [3]..
(3) THREE SOLUTIONS FOR A NEUMANN BOUNDARY. . .. 83. Theorem B. (Theorem B of [3]) Let X be a real reflexive Banach space, : X → R a continuously Gˆateaux differentiable and sequentially weakly lower semicontinuous functional whose Gˆateaux derivative admits a continuous inverse on X ∗ , : X → R a continuously Gˆateaux differentiable functional whose Gˆateaux derivative is compact. Assume that: lim ( (u) + λ (u)) = +∞ for all λ ∈ [0, +∞[;. (i). u →+∞. there is r ∈ R such that:. (ii). inf < r, X. and ϕ1 (r) < ϕ2 (r), where ϕ1(r) := ϕ2(r) :=. inf. u∈ −1 (]−∞,r[). inf. u∈ −1 (]−∞,r[). (u) −. inf w. −1 (]−∞,r[). , r − (u). (u) − (v) sup , v∈ −1 ([r,+∞[) (v) − (u). w. and −1 (] − ∞, r[) is the closure of −1 (] − ∞, r[) in the weak topology. Then, for each λ ∈ ] ϕ21(r) , ϕ11(r) [ the functional + λ has at least three critical points in X . Other applications of Theorem B can be found in [3] and [4]. In order to apply Theorem B to our problem, let X be the space W 1, p () equipped with the norm 1p |∇u(x )| p dx + a(x )|u(x )| p dx , u := . . which is equivalent to the usual one, while on the space C 0 () we consider the norm u ∞ := sup |u(x )|. u∈. If p > n, X is compactly embedded in C 0 (), so that (1). c := sup. u∈X \{0}. u ∞ < +∞. u. Clearly, c p a 1 ≥ 1, where a 1 := |a(x )| dx . For other basic notations and definitions we refer to [11]..
(4) 84. DIEGO AVERNA - GABRIELE BONANNO. 2. Results. Our main result is the following Theorem 1. Let p > n and let f : × R → R be a Carath´eodory function such that, for every ρ > 0, sup | f (., u)| ∈ L 1 (). Put |u|≤ρ. . ξ. F(x , ξ ) :=. f (x , u) du. for every. (x , ξ ) ∈ × R ,. 0. and assume that there exist three positive constants γ , δ, and s, with γ < δ and s < p, and a function μ ∈ L 1() such that: sup F(x , ξ ) dx F(x , δ) dx 1 |ξ |≤γ < ; (j) γp 1 + c p a 1 δp (jj). F(x , ξ ) ≤ μ(x )(1 + |ξ |s ) for all (x , ξ ) ∈ × R. Then, setting λ :=. p. . a 1δ p F(x , δ) dx − sup F(x , ξ ) dx |ξ |≤γ. and λ := . cp p. . γp , sup F(x , ξ ) dx. |ξ |≤γ. . for each λ ∈ ]λ , λ [ problem (P) admits at least three weak solutions. Proof. For each u ∈ X , put (u) :=. 1 u p p. . and. (u) := −. . F(x , u(x )) dx .. Since p > n, X is compactly embedded in C 0 () and it is well known that and are (well defined and) continuously Gˆateaux differentiable functionals with . |∇u(x )| p−2 ∇u(x )∇v(x ) + a(x )|u(x )| p−2u(x )v(x ) dx (u)(v) = .
(5) 85. THREE SOLUTIONS FOR A NEUMANN BOUNDARY. . .. and. (u)(v) = −. . f (x , u(x ))v(x ) dt. for every u, v ∈ X , as well as is compact. Furthermore, by Proposition 25.20 (i) of [11], is sequentially weakly lower semicontinuous, while Proposition 1 of [7] ensures that admits a continuous inverse on X ∗ . Hypothesis (i) of Theorem B follows in a simple way thanks to (jj).. . sup F(x , ξ ) dx. |ξ |≤γ. c p a 1γ p. =. .. . 1 < p c a 1(1 + c p a 1) . p. γ c. 1 p. In order to prove (ii) of Theorem B, put r := From hypothesis (j), we get. . F(x , δ) dx δp. 1 1 − c p a 1 1 + c p a 1. . F(x , δ) dx , δp. then 1 1 + c p a 1. . . . F(x , δ) dx + δp. . sup F(x , ξ ) dx. |ξ |≤γ. c p a. 1γ. p. 1 < p c a 1. . F(x , δ) dx , δp. thus, being γ < δ, we have 1 1 + c p a 1. . . . F(x , δ) dx < δp. F(x , δ) dx −. . sup F(x , ξ ) dx. . |ξ |≤γ. ,. c p a 1 δ p. hence, using again (j), we get . . sup F(x , ξ ) dx. |ξ |≤γ. γp. <. . F(x , δ) dx −. . sup F(x , ξ ) dx. |ξ |≤γ. ,. c p a 1δ p. from which, multiplying by c p p, we obtain cp p (2). . . sup F(x , ξ ) dx. |ξ |≤γ. γp. <p. . F(x , δ) dx −. . sup F(x , ξ ) dx. |ξ |≤γ. a 1δ p. ..
(6) 86. DIEGO AVERNA - GABRIELE BONANNO. We claim that: cp p ϕ1 (r) ≤. (C1) and (C2). . ϕ2 (r) ≥ p. . sup F(x , ξ ) dx. |ξ |≤γ. γp. F(x , δ) dx −. . sup F(x , ξ ) dx. |ξ |≤γ. ,. a 1δ p. from which (ii) of Theorem B follows. In fact, taking into account that the function identically 0 obviously belongs to −1 (] − ∞, r[), and that (0) = 0, we get sup F(x , u(x )) dx w. ϕ1 (r) ≤. −1 (]−∞,r[). ,. r. w. and, since −1 (] − ∞, r[) = −1 (] − ∞, r]), we have F(x , u(x ))dx sup sup F(x , u(x )) dx w. −1 (]−∞,r[). =. r. −1 (]−∞,r]). . ,. r 1. thus, taking into account that |u(x )| ≤ c( pr) p = γ , for every u ∈ X such that (u) ≤ r and for each x ∈ , we obtain sup sup F(x , ξ ) dx F(x , u(x )) dx −1 (]−∞,r]). r. ≤. |ξ |≤γ. r. .. So, (C1) follows at once by the definition of r . Moreover, for each v ∈ X such that (v) ≥ r , we have F(x , v(x )) dx − F(x , u(x )) dx , inf ϕ2 (r) ≥ u∈ −1 (]−∞,r[) (v) − (u) 1. thus, from |u(x )| ≤ c( pr) p = γ , for every u ∈ X such that (u) < r and for each x ∈ , we obtain F(x , v(x )) dx − F(x , u(x )) dx inf (v) − (u) u∈ −1 (]−∞,r[).
(7) 87. THREE SOLUTIONS FOR A NEUMANN BOUNDARY. . .. ≥. . inf. . F(x , v(x )) dx −. . sup F(x , ξ ) dx. |ξ |≤γ. ,. (v) − (u). u∈ −1 (]−∞,r[). from which, being 0 < (v) − (u) ≤ (v) for every u ∈ −1(] − ∞, r[), and under further condition (3) F(x , v(x )) dx ≥ sup F(x , ξ ) dx , |ξ |≤γ. . we can write . inf. u∈ −1 (]−∞,r[). ≥p. . F(x , v(x )) dx −. . sup F(x , ξ ) dx. |ξ |≤γ. (v) − (u). F(x , v(x )) dx −. . sup F(x , ξ ) dx. |ξ |≤γ. .. v p 1. If we put v(x ) := δ, for each x ∈ , we have v = a 1p δ, hence, by (1) and γ < δ, we get (v) > r . Moreover, with this choice of v, (2) ensures (3), thus (C2) is also proved. Hence the conclusion follows by Theorem B, by observing that a 1δ p 1 ≤ ϕ2(r) p F(x , δ) dx − sup F(x , ξ ) dx |ξ |≤γ. and. γp 1 . ≥ p ϕ1 (r) c p sup F(x , ξ ) dx. . |ξ |≤γ. Remark 1. In applying Theorem 1, it is enough to know an explicit upper bound for the constant c defined in (1). In this connection, when is a convex set, we have the following estimate (see [1] for more details): (4). c≤2. p−1 p. . p−1 1 1p diam() p − 1 a ∞ p meas() max , . 1 a 1 p−n a 1 np.
(8) 88. DIEGO AVERNA - GABRIELE BONANNO. Example 1. The problem . −3 u + ∂u ∂ν. 2+x |u|u π.
(9) 2 = λ(x 2 + y 2) 2e−u u 17 (9 − u 2 ) + 1 in . = 0. on ∂,. where is the open unit ball in R2 , admits at least three weak solutions for each λ ∈ ]15 · 10−4, 15 · 10−2 [. In fact, choosing γ := 1, δ := 2, s := 2, and a(x , y) :=.
(10) 2+x 2 , f (x , y, u) := (x 2 + y 2 ) 2e−u u 17 (9 − u 2 ) + 1 π. for every (x , y) ∈ and every u ∈ R, and taking into account (4), it is simple to verify all the hypotheses of Theorem 1, and that ]15 · 10−4 , 15 · 10−2 [⊂]λ , λ [. Remark 2. In the ordinary case, whenever :=]α, β[ is a bounded open interval in R, a function u : [α, β] → R is said a generalized solution to problem (PO). − |u | p−2u + a(t)|u| p−2 u = λ f (t, u) in ]α, β[ u (α) = u (β) = 0,. if u ∈ C 1 ([α, β]), |u | p−2 u ∈ AC([α, β]), u (α) = u (β) = 0 and − |u (t)| p−2 u (t) + a(t)|u(t)| p−2u(t) = λ f (t, u(t)) for almost every t ∈ [α, β]. Using standard arguments, and taking into account that the correspondence u → |u| p−2 u is an homeomorphism in R, one can show that weak solutions coincides with generalized ones, provided a ∈ L ∞ (]α, β[) and f is as in Theorem 1. We point out the following simple consequence of Theorem 1, then we give the proof of Theorem A and finally we present an easy example of application. Theorem 2. Let p ≥ 2, and let g ∈ L 1 (]α, β[), h ∈ C 0 (R) be two non-negative functions, with g 1 > 0. Assume that there exists four positive constants γ , δ, η and s, with γ < δ and s < p, such that:.
(11) 89. THREE SOLUTIONS FOR A NEUMANN BOUNDARY. . .. γ (k). 0. γp . ξ. (kk). δ. h(u) du <. 1. h(u) du. 0 p. 1− p. 1 + 2 p−1max{1, (β − α)2 p−1 a ∞ a 1. }. δp. ;. h(u) du ≤ η(1 + |ξ |s ) for all ξ ∈ R.. 0. Then, for each λ in
(12). γ p a 1 δ p a 1 , δ γ p 1− p p g 1 γ h(u) du 2 p−1max{1, (β − α)2 p−1 a ∞ a 1 } p g 1 0 h(u) du. the problem − |u | p−2 u + a(t)|u| p−2u = λg(t)h(u) in ]α, β[ u (α) = u (β) = 0, admits at least three generalized solutions. Proof. Taking into account Remarks 1 and 2, the conclusion follows immediately from Theorem 1, by using f := gh and μ := ηg. Proof of Theorem A. Put h(u) :=. 0 h(u). if if. u<0 u ≥ 0.. Clearly, h is a continuous function on R. Moreover, taking into account that lim. max|ξ |≤γ. γ →0+. ξ. h(u) du. 0 2 γ. = 0,. it is enough to pick γ > 0 such that max|ξ |≤γ. ξ 0 2 γ. h(u) du γ2. 4 g 1 max|ξ |≤γ and. max. |ξ |≤γ. 0. ξ. 1 < 3. ξ 0. h(u) du < 0. δ. δ 0. h(u) du , δ2. h(u) du. >1. h(u) du −. δ2 2 g 1.
(13) 90. DIEGO AVERNA - GABRIELE BONANNO. so that, taking into account Remark 1, using f := gh, and observing that 1 ∈ ]λ, λ [, Theorem 1 ensures that the problem −u + u = g(t)h(u) (P2) u (0) = u (1) = 0, admits at least two non-null classical solutions. We claim that these solutions are non-negative. In fact, arguing by a contradiction, if one of them, say u 1 , is negative at one point of [0, 1], there exists an interval ]a, b[⊆ [0, 1] such that −u 1 (t) + u 1 (t) = 0 for every t ∈ ]a, b[ and, further, it must be true one of the following conditions: u 1 (a) = u 1 (b) = 0 (if 0 < a < b < 1), u 1 (0) = u 1 (b) = 0 (if 0 = a < b < 1), u 1 (a) = u 1 (1) = 0 (if 0 < a < b = 1), u 1 (0) = u 1 (1) = 0 (if 0 = a < b = 1). Therefore, u 1 (t) = 0 for every t ∈ [a, b] and this is a contradiction, so our claim is proved. Finally, the conclusion follows taking into account that the nonnegative solutions of (P2) are also solutions of (P1). Remark 3. If in Theorem A we also assume that 0 h(u) = 0 and h(u) du < 0 lim u→0− u −δ . for some δ > 0. then, for every non-negative function g ∈ C 0 ([0, 1]) such that . δ 2 δ2 , −δ g 1 > max δ 2 0 h(u) du 2 0 h(u) du problem (P1) admits also two non-positive solutions. It is enough to apply the same Theorem A to the function h ∗ (u) := −h(−u). Example 2. Let h : R → R the function defined as follows 0 if u≤0 h(u) := 3u 2 if 0<u<1 3 if u ≥ 1. Therefore, owing to Theorem A, for every non-negative function g ∈ C 0 ([0, 1]) such that g 1 > 12 , the problem −u + u = g(t)h(u) u (0) = u (1) = 0, admits at least two non-negative and non-trivial classical solutions. ξ On the other hand, the function H (ξ ) := 0 h(u) du does not satisfy the assumption 1. of Theorem 2.1 of [8]..
(14) THREE SOLUTIONS FOR A NEUMANN BOUNDARY. . .. 91. REFERENCES [1] [2]. [3]. [4]. [5]. [6] [7]. [8] [9]. [10] [11]. G. Anello - G. Cordaro, An existence theorem for the Neumann problem involving the p-Laplacian, J. Convex Anal., 10 (2003), pp. 185–198. G. Anello - G. Cordaro, Existence of solutions of the Neumann problem for a class of equations involving the p-Laplacian via a variational principle of Ricceri, Arch. Math. (Basel), 79 (2002), pp. 274–287. D. Averna - G. Bonanno, A three critical points theorem and its applications to the ordinary Dirichlet problem, Topol. Methods Nonlinear Anal., 22 (2003), pp. 93–104. D. Averna - G. Bonanno, Three solutions for a quasilinear two point boundary value problem involving the one-dimensional p-Laplacian, Proc. Edinb. Math. Soc., 47 (2004), pp. 257–270. P.A. Binding - P. Dr´abek - Y.X. Huang, On Neumann boundary value problems for some quasilinear elliptic equations, Electron. J. Differential Equations, 1997 n. 5 (1997), pp. 1–11. G. Bonanno, Multiple solutions for a Neumann boundary value problem, J. Nonlinear Convex Anal., 4 (2003), pp. 287–290. G. Bonanno - P. Candito, Three solutions to a Neumann problem for elliptic equations involving the p-Laplacian, Arch. Math. (Basel), 80 (2003), pp. 424– 429. F. Faraci, Multiplicity results for a Neumann problem involving the p-Laplacian, J. Math. Anal. Appl., 277 (2003), pp. 180–189. A.R. Miciano - R. Shivaji, Multiple positive solutions for a class of semipositone Neumann two point boundary value problems, J. Math. Anal. Appl., 178 (1993), pp. 102–115. B. Ricceri, A general variational principle and some of its applications, J. Comput. Appl. Math., 113 (2000), pp. 401–410. E. Zeidler, Nonlinear functional analysis and its applications, Vol. II/B. BerlinHeidelberg-New York, 1990.. Diego Averna, Dipartimento di Matematica ed Applicazioni Universit`a di Palermo Via Archirafi, 34, 90123 Palermo (ITALY) e-mail: [email protected] Gabriele Bonanno, D. I. M. E. T. Facolt`a di Ingegneria, Universit`a di Reggio Calabria Via Graziella (Feo di Vito), 89100 Reggio Calabria (ITALY) e-mail: [email protected].
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