ASYMPTOTIC BEHAVIOR FOR DISCRETIZATIONS OF A SEMILINEAR PARABOLIC EQUATION WITH A NONLINEAR BOUNDARY CONDITION NABONGO DIABATE THÉODORE K. BONI Université d’Abobo-Adjamé UFR-SFA, Dépt. de Math. et Informatiques 16 BP 372 Abidjan 16, (Côte d’Ivoire). EMail: nabongo_diabate@yahoo.fr Inst. Nat. Polytech. Houphouët-Boigny de Yamoussoukro BP 1093 Yamoussoukro, (Côte d’Ivoire). Received: 16 October, 2007 Accepted: 17 March, 2008 Communicated by: C. Bandle 2000 AMS Sub. Class.: 35B40, 35B50, 35K60, 65M06. Key words: Semidiscretizations, Semilinear parabolic equation, Asymptotic behavior, Convergence. Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Title Page Contents JJ II J I Page 1 of 26 Abstract: This paper concerns the study of the numerical approximation for the following initialboundary value problem: p−1 u, 0 < x < 1, t > 0, ut = uxx − a|u| ux (0, t) = 0 ux (1, t) + b|u(1, t)|q−1 u(1, t) = 0, t > 0, (P) u(x, 0) = u0 (x) > 0, 0 ≤ x ≤ 1, where a > 0, b > 0 and q > p > 1. We show that the solution of a semidiscrete form of (P ) goes to zero as t goes to infinity and give its asymptotic behavior. Using some nonstandard schemes, we also prove some estimates of solutions for discrete forms of (P ). Finally, we give some numerical experiments to illustrate our analysis. Go Back Full Screen Close Contents 1 Introduction 3 2 Semidiscretizations Scheme 5 3 Asymptotic Behavior 8 4 Convergence 14 5 Full Discretizations 17 6 Numerical Results 24 Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Title Page Contents JJ II J I Page 2 of 26 Go Back Full Screen Close 1. Introduction Consider the following initial-boundary value problem: (1.1) (1.2) ut = uxx − a|u|p−1 u, 0 < x < 1, t > 0, q−1 ux (0, t) = 0 ux (1, t) + b|u(1, t)| u(1, t) = 0, t > 0, Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 (1.3) u(x, 0) = u0 (x) > 0, 0 ≤ x ≤ 1, where a > 0, b > 0, q > p > 1, u0 ∈ C 1 ([0, 1]), u00 (0) = 0 and u00 (1) + b|u0 (1)|q−1 u0 (1) = 0. The theoretical study of the asymptotic behavior of solutions for semilinear parabolic equations has been the subject of investigation for many authors (see [2], [4] and the references cited therein). In particular, in [4], when b = 0, the authors have shown that the solution u of (1.1) – (1.3) goes to zero as t tends to infinity and satisfies the following : (1.4) 0 ≤ ku(x, t)k∞ ≤ Title Page Contents JJ II J I Page 3 of 26 Go Back 1 1 (ku0 (x)k∞ + a(p − 1)t) p−1 for t ∈ [0, +∞), Full Screen Close (1.5) lim t t→∞ 1 p−1 ku(x, t)k∞ = C0 , 1 p−1 1 where C0 = a(p−1) . The same results have been obtained in [2] in the case where b > 0 and q > p > 1. In this paper we are interested in the numerical study of (1.1) – (1.3). At first, using a semidiscrete form of (1.1) – (1.3), we prove similar results for the semidiscrete solution. We also construct two nonstandard schemes and show that these schemes allow the discrete solutions to obey an estimation as in (1.4). Previously, authors have used numerical methods to study the phenomenon of blow-up and the one of extinction (see [1] and [3]). This paper is organized as follows. In the next section, we prove some results about the discrete maximum principle. In the third section, we take a semidiscrete form of (1.1) – (1.3), and show that the semidiscrete solution goes to zero as t tends to infinity and give its asymptotic behavior. In the fourth section, we show that the semidiscrete scheme of the third section converges. In Section 5, we construct two nonstandard schemes and obtain some estimates as in (1.4). Finally, in the last section, we give some numerical results. Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Title Page Contents JJ II J I Page 4 of 26 Go Back Full Screen Close 2. Semidiscretizations Scheme In this section, we give some lemmas which will be used later. Let I be a positive integer, and define the grid xi = ih, 0 ≤ i ≤ I, where h = 1/I. We approximate the solution u of the problem (1.1) – (1.3) by the solution Uh (t) = (U0 (t), U1 (t), . . . , UI (t))T of the semidiscrete equations (2.1) d Ui (t) = δ 2 Ui (t) − a|Ui (t)|p−1 Ui (t), dt Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and 0 ≤ i ≤ I − 1, t > 0, Théodore K. Boni (2.2) d 2b UI (t) = δ 2 UI (t) − a|UI (t)|p−1 UI (t) − |UI (t)|q−1 UI (t), dt h vol. 9, iss. 2, art. 33, 2008 t > 0, Title Page Ui (0) = (2.3) Ui0 > 0, 0 ≤ i ≤ I, Contents where Ui+1 (t) − 2Ui (t) + Ui−1 (t) , 1 ≤ i ≤ I − 1, h2 2U1 (t) − 2U0 (t) 2UI−1 (t) − 2UI (t) δ 2 U0 (t) = , δ 2 UI (t) = . 2 h h2 The following lemma is a semidiscrete form of the maximum principle. δ 2 Ui (t) = 0 I+1 1 Lemma 2.1. Let ah (t) ∈ C ([0, T ], R ) and let Vh (t) ∈ C ([0, T ], R that d (2.4) Vi (t) − δ 2 Vi (t) + ai (t)Vi (t) ≥ 0, 0 ≤ i ≤ I, t ∈ (0, T ), dt (2.5) Vi (0) ≥ 0, 0 ≤ i ≤ I. Then we have Vi (t) ≥ 0 for 0 ≤ i ≤ I, t ∈ (0, T ). JJ II J I Page 5 of 26 Go Back I+1 ) such Full Screen Close Proof. Let T0 < T and let m = min0≤i≤I,0≤t≤T0 Vi (t). Since for i ∈ {0, . . . , I}, Vi (t) is a continuous function, there exists t0 ∈ [0, T0 ] such that m = Vi0 (t0 ) for a certain i0 ∈ {0, . . . , I}. It is not hard to see that dVi0 (t0 ) Vi (t0 ) − Vi0 (t0 − k) = lim 0 ≤ 0, k→0 dt k (2.6) (2.7) (2.8) δ 2 Vi0 (t0 ) = δ 2 Vi0 (t0 ) = V1 (t0 ) − V0 (t0 ) ≥ 0 if h2 Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and i0 = 0, Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Vi0 +1 (t0 ) − 2Vi0 (t0 ) + Vi0 −1 (t0 ) ≥ 0 if h2 1 ≤ i0 ≤ I − 1, Title Page Contents (2.9) δ 2 Vi0 (t0 ) = VI−1 (t0 ) − VI (t0 ) ≥ 0 if h2 i0 = I. λt Define the vector Zh (t) = e Vh (t) where λ is large enough such that ai0 (t0 )−λ > 0. A straightforward computation reveals: (2.10) dZi0 (t0 ) − δ 2 Zi0 (t0 ) + (ai0 (t0 ) − λ)Zi0 (t0 ) ≥ 0. dt dZi0 (t0 ) dt JJ II J I Page 6 of 26 Go Back Full Screen Close 2 We observe from (2.6) – (2.9) that ≤ 0 and δ Zi0 (t0 ) ≥ 0. Using (2.10), we arrive at (ai0 (t) − λ)Zi0 (t0 ) ≥ 0, which implies that Zi0 (t0 ) ≥ 0. Therefore, Vi0 (t0 ) = m ≥ 0 and we have the desired result. Another form of the maximum principle is the following comparison lemma. Lemma 2.2. Let Vh (t), Uh (t) ∈ C 1 ([0, ∞), RI+1 ) and f ∈ C 0 (R × R, R) such that for t ∈ (0, ∞), (2.11) dVi (t) 2 dUi (t) 2 −δ Vi (t)+f (Vi (t), t) < −δ Ui (t)+f (Ui (t), t), dt dt Vi (0) < Ui (0), (2.12) 0 ≤ i ≤ I, Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and 0 ≤ i ≤ I. Théodore K. Boni Then we have Vi (t) < Ui (t), 0 ≤ i ≤ I, t ∈ (0, ∞). vol. 9, iss. 2, art. 33, 2008 Proof. Define the vector Zh (t) = Uh (t) − Vh (t). Let t0 be the first t > 0 such that Zi (t) > 0 for t ∈ [0, t0 ), i = 0, . . . , I, but Zi0 (t0 ) = 0 for a certain i0 ∈ {0, . . . , I}. We observe that dZi0 (t0 ) Zi (t0 ) − Zi0 (t0 − k) = lim 0 k→0 dt k Z (t )−2Z (t )+Z (t ) i0 +1 0 i0 0 i0 −1 0 ≥ 0 if h2 2Z1 (t0 )−2Z0 (t0 ) δ 2 Zi0 (t0 ) = ≥0 if h2 2ZI−1 (t0 )−2ZI (t0 ) ≥0 if h2 Contents ≤ 0. 1 ≤ i0 ≤ I − 1, i0 = 0, JJ II J I Page 7 of 26 Go Back i0 = I, which implies: dZi0 (t0 ) − δ 2 Zi0 (t0 ) + f (Ui0 (t0 ), t0 ) − f (Vi0 (t0 ), t0 ) ≤ 0. dt But this inequality contradicts (2.11). Title Page Full Screen Close 3. Asymptotic Behavior In this section, we show that the solution Uh of (2.1) – (2.3) goes to zero as t → +∞ and give its asymptotic behavior. Firstly, we prove that the solution tends to zero as t → +∞ by the following: Theorem 3.1. The solution Uh (t) of (2.1) – (2.3) goes to zero as t → ∞ and we have the following estimate 0 ≤ kUh (t)k∞ ≤ 1 (kUh (0)k1−p ∞ + a(p − 1)t) 1 p−1 for t ∈ [0, +∞). Proof. We introduce the function α(t) which is defined as α(t) = Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Title Page 1 Contents 1 (kUh (0)k1−p ∞ + a(p − 1)t) p−1 and let Wh be the vector such that Wi (t) = α(t). It is not hard to see that dWi (t) − δ 2 Wi (t) + a|Wi (t)|p−1 Wi (t) = 0, dt 0 ≤ i ≤ I − 1, t ∈ (0, T ), JJ II J I Page 8 of 26 Go Back 2b dWI (t) − δ 2 WI (t) + a|WI (t)|p−1 WI (t) + |WI (t)|q−1 WI (t) ≥ 0, dt h Wi (0) ≥ Ui (0), 0 ≤ i ≤ I, t ∈ (0, T ), where (0, T ) is the maximal time interval on which kUh (t)k∞ < ∞. Setting Zh (t) = Wh (t) − Uh (t) and using the mean value theorem, we see that dZi (t) − δ 2 Zi (t) + ap|θi (t)|p−1 Zi (t) = 0, dt 0 ≤ i ≤ I − 1, t ∈ (0, T ) Full Screen Close dZI (t) 2b 2 p−1 q−1 − δ ZI (t) + ap|θI (t)| + |θI (t)| ZI (t) ≥ 0, dt h Zi (0) ≥ 0, t ∈ (0, T ), 0 ≤ i ≤ I, where θi is an intermediate value between Ui (t) and Wi (t). From Lemma 2.1, we have 0 ≤ Ui (t) ≤ Wi (t) for t ∈ (0, T ). If T < ∞, we have kUh (T )k∞ ≤ 1 1 (kUh (0)k1−p ∞ + a(p − 1)T ) p−1 < ∞, which leads to a contradiction. Hence T = ∞ and we have the desired result. Remark 1. The estimate of Theorem 3.1 is a semidiscrete version of the result established in (1.4) for the continuous problem. Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Title Page Contents Let us give the statement of the main theorem of this section. Theorem 3.2. Let Uh be the solution of (2.1) – (2.2). Then we have 1 lim t p−1 kUh (t)k∞ = C0 , t→∞ where C0 = 1 a(p−1) 1 p−1 . The proof of Theorem 3.2 is based on the following lemmas. We introduce the function µ(x) = −λ(C0 + x) + (C0 + x)p , 1 p−1 1 where C0 = a(p−1) . Firstly, we establish an upper bound of the solution for the semidiscrete problem. JJ II J I Page 9 of 26 Go Back Full Screen Close Lemma 3.3. Let Uh be the solution of (2.1) – (2.3). For any ε > 0, there exist positive times T and τ such that Ui (t + τ ) ≤ (C0 + ε)(t + T )−λ + (t + T )−λ−1 , 0 ≤ i ≤ I. Proof. Define the vector Wh such that Wi (t) = (C0 + ε)t−λ + t−λ−1 . A straightforward computation reveals that dWi − δ 2 Wi + a|Wi |p−1 Wi dt = −λ(C0 + ε)t−λ−1 − (λ + 1)t−λ−2 + a((C0 + ε)t−λ + t−λ−1 )p Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Title Page = t−λ−1 (−λ(C0 + ε) − (λ + 1)t−1 + a(C0 + ε + t−1 )p ), because λp = λ + 1. Using the mean value theorem, we get (C0 + ε + t−1 )p = (C0 + ε)p + ξi t−1 , where ξi (t) is a bounded function. We deduce that dWi − δ 2 Wi + a|Wi |p−1 Wi = t−λ−1 (µ(ε) − (λ + 1)t−1 + ξi t−1 ), dt Contents JJ II J I Page 10 of 26 Go Back Full Screen Close dWI 2b − δ 2 WI + a|WI |p−1 WI + |WI |q−1 WI dt h 2b −qλ+λ+1 −λ−1 −1 −1 −1 q =t µ(ε) − (λ + 1)t + ξi t + t (C0 + ε + t ) . h p−q Obviously −qλ + λ + 1 = p−1 < 0. We also observe that µ(0) = 0 and µ0 (0) = 1, which implies that µ(ε) > 0. Therefore there exists a positive time T such that dWi − δ 2 Wi + a|Wi |p−1 Wi > 0, dt 0 ≤ i ≤ I − 1, t ∈ [T, +∞), dWI 2b − δ 2 WI + a|WI |p−1 WI + |WI (t)|q−1 WI (t) > 0, t ∈ [T, +∞), dt h T −λ C0 . Wi (T ) > 2 Since from Theorem 3.1 limt→∞ Ui (t) = 0, there exists τ > T such that Ui (τ ) < T −λ C0 < Wi (T ). We introduce the vector Zh (t) such that Zi (t) = Ui (t + τ − T ), 2 0 ≤ i ≤ I. We obtain dZi − δ 2 Zi + a|Zi |p−1 Zi > 0, dt Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Title Page Contents 0 ≤ i ≤ I − 1, t ≥ T, dZI 2b − δ 2 ZI + a|ZI |p−1 ZI + |ZI (t)|q−1 ZI (t) > 0, dt h Zi (T ) = Ui (τ ) < Wi (T ). t ≥ T, We deduce from Lemma 2.2 that Zi (t) ≤ Wi (t), that is to say (3.1) Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Ui (t + τ − T ) ≤ Wi (t) for t ≥ T, which leads us to the result. The lemma below gives a lower bound of the solution for the semidiscrete problem. JJ II J I Page 11 of 26 Go Back Full Screen Close Lemma 3.4. Let Uh be the solution of (2.1) – (2.3). For any ε > 0, there exists a positive time τ such that Ui (t + 1) ≥ (C0 − ε)(t + τ )−λ + (t + τ )−λ−1 , 0 ≤ i ≤ I. Proof. Introduce the vector Vh such that Vi (t) = (C0 − ε)t−λ + t−λ−1 . A direct calculation yields dVi − δ 2 Vi + a|Vi |p−1 Vi = −λ(C0 − ε)t−λ−1 − (λ + 1)t−λ−2 + a((C0 − ε)t−λ + t−λ−1 )p dt = t−λ−1 (−λ(C0 − ε) − (λ + 1)t−1 + a(C0 − ε + t−1 )p ) because λp = λ + 1. From the mean value theorem, we have Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Title Page Contents (C0 − ε + t−1 )p = (C0 − ε)p + χi (t)t−1 , where χi (t) is a bounded function. We deduce that dVi − δ 2 Vi + a|Vi |p−1 Vi = t−λ−1 (µ(−ε) − (λ + 1)t−1 + χi t−1 ), dt J I Page 12 of 26 Full Screen 2b −qλ+λ+1 −1 q −1 −1 µ(ε) − (λ + 1)t + χi t + t (C0 − ε + t ) . h Obviously −qλ + λ + 1 < 0. Also, since µ(0) = 0 and µ0 (0) = 1, it is easy to see that µ(−ε) < 0. Hence there exists T > 0 such that dVi − δ 2 Vi + a|Vi |p−1 Vi < 0, dt II Go Back dVI 2b − δ 2 VI + a|VI |p−1 VI + |VI |q−1 VI dt h = t−λ−1 JJ 0 ≤ i ≤ I − 1, t ∈ [T, +∞), Close dVI 2b − δ 2 VI + a|VI |p−1 VI + |VI |q−1 VI < 0, t ∈ [T, +∞). dt h Since Vi (t) goes to zero as t → +∞, there exists τ > max(T, 1) such that Vi (τ ) < Ui (1). Setting Xi (t) = Vi (t + τ − 1), we observe that dXi − δ 2 Xi + a|Xi |p−1 Xi < 0, dt 0 ≤ i ≤ I − 1, t ≥ 1, 2b dXI − δ 2 XI + a|XI |p−1 XI + |XI |q−1 XI < 0, dt h Xi (1) = Vi (τ ) < Ui (1). t ≥ 1, We deduce from Lemma 2.2 that (3.2) Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Title Page Ui (t) ≥ Vi (t + τ − 1) for t ≥ 1, which leads us to the result. Now, we are in a position to give the proof of the main result of this section. Proof of Theorem 3.2. From Lemma 3.3 and Lemma 3.4, we deduce Ui (t) Ui (t) (C0 − ε) ≤ lim inf ≤ lim sup ≤ (C0 + ε), t→∞ t→∞ tλ tλ and we have the desired result. Contents JJ II J I Page 13 of 26 Go Back Full Screen Close 4. Convergence In this section, we will show that for each fixed time interval [0, T ], where u is defined, the solution Uh (t) of (2.1) – (2.3) approximates u, when the mesh parameter h goes to zero. Theorem 4.1. Assume that (1.1) – (1.3) has a solution u ∈ C 4,1 ([0, 1] × [0, T ]) and the initial condition at (2.3) satisfies kUh0 − uh (0)k∞ = o(1) (4.1) as h → 0, Théodore K. Boni where uh (t) = (u(x0 , t), . . . , u(xI , t))T . Then, for h sufficiently small, the problem (2.1) – (2.3) has a unique solution Uh ∈ C 1 ([0, T ], RI+1 ) such that (4.2) max kUh (t) − uh (t)k∞ = O(kUh0 − uh (0)k∞ + h2 ) as 0≤t≤T h → 0. vol. 9, iss. 2, art. 33, 2008 Title Page Contents Proof. Let K > 0 and L be such that 2kuxxx k∞ K ≤ , 3 2 Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and kuxxxx k∞ K ≤ , 12 2 kuk∞ ≤ K, ap(K + 1)p−1 ≤ L, JJ II J I Page 14 of 26 (4.3) 2q(K + 1)q−1 ≤ L. Go Back The problem (2.1) – (2.3) has for each h, a unique solution Uh ∈ C 1 ([0, Tqh ), RI+1 ). Let t(h) the greatest value of t > 0 such that (4.4) kUh (t) − uh (t)k∞ < 1f ort ∈ (0, t(h)). The relation (4.1) implies that t(h) > 0 for h sufficiently small. Let t∗ (h) = min{t(h), T }. By the triangular inequality, we obtain kUh (t)k∞ ≤ ku(x, t)k∞ + kUh (t) − uh (t)k∞ f or t ∈ (0, t∗ (h)), Full Screen Close which implies that (4.5) kUh (t)k∞ ≤ 1 + K, f or t ∈ (0, t∗ (h)). Let eh (t) = Uh (t)−uh (x, t) be the error of discretization. Using Taylor’s expansion, we have for t ∈ (0, t∗ (h)), h2 d ei (t) − δ 2 ei (t) = uxxxx (e xi , t) − apξip−1 ei (t), dt 12 d 2 2h2 h2 eI (t) − δ 2 eI (t) = qθIq−1 eI + uxxx (e xI , t) + uxxxx (e xI , t) − apξIp−1 eI (t), dt h 3 12 where θI ∈ (UI (t), u(xI , t) and ξi ∈ (Ui (t), u(xi , t). Using (4.3) and (4.5), we arrive at (4.6) (4.7) d ei (t) − δ 2 ei (t) ≤ L|ei (t)| + Kh2 , 0 ≤ i ≤ I − 1, dt L|eI (t)| deI (t) (2eI−1 (t) − 2eI (t)) − ≤ + L|eI (t)| + Kh2 . 2 dt h h Consider the function Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Title Page Contents JJ II J I Page 15 of 26 Go Back 2 z(x, t) = e((M +1)t+Cx ) (kUh0 − uh (0)k∞ + Qh2 ) where M , C, Q are constants which will be determined later. We get zt (x, t) − zxx (x, t) = (M + 1 − 2C − 4C 2 x2 )z(x, t), zx (0, t) = 0, zx (1, t) = 2Cz(1, t), 2 z(x, 0) = eCx (Uh0 − uh (0)∞ + Qh). Full Screen Close By a semidiscretization of the above problem, we may choose M, C, Q large enough that (4.8) d z(xi , t) > δ 2 z(xi , t) + L|z(xi , t)| + Kh2 , 0 ≤ i ≤ I − 1, dt (4.9) L d z(xI , t) > δ 2 z(xI , t) + |z(xI , t)| + L|z(xI , t)| + Kh2 , dt h Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 z(xi , 0) > ei (0), 0 ≤ i ≤ I. (4.10) It follows from Lemma 3.4 that z(xi , t) > ei (t) f or t ∈ (0, t∗ (h)), Title Page 0 ≤ i ≤ I. By the same way, we also prove that z(xi , t) > −ei (t) f or t ∈ (0, t∗ (h)), 0 ≤ i ≤ I, which implies that kUh (t) − uh (t)k∞ ≤ e(M t+C) (Uh0 − uh (0)∞ + Qh2 ), t ∈ (0, t∗ (h)). Let us show that t∗ (h) = T . Suppose that T > t(h). From (4.4), we obtain (4.11) 1 = kUh (t(h)) − uh (t(h))k∞ ≤ e(M T +C) (Uh0 − uh (0)∞ + Qh2 ). Since the term in the right hand side of the inequality goes to zero as h goes to zero, we deduce from (4.11) that 1 ≤ 0, which is impossible. Consequently t∗ (h) = T , and we obtain the desired result. Contents JJ II J I Page 16 of 26 Go Back Full Screen Close 5. Full Discretizations In this section, we study the asymptotic behavior, using full discrete schemes (explicit and implicit) of (1.1) – (1.3). Firstly, we approximate the solution u(x, t) of (n) (1.1) – (1.3) by the solution Uh = (U0n , U1n , . . . , UIn )T of the following explicit scheme (n+1) (n) Ui − Ui (n) p−1 (n+1) (n) (5.1) = δ 2 Ui − a Ui Ui , 0 ≤ i ≤ I − 1, ∆t Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 (n+1) (5.2) UI (n) − UI ∆t =δ 2 (n) UI (n) p−1 (n+1) 2b (n) q−1 (n+1) − a UI UI − UI UI , h Title Page Contents (0) Ui (5.3) = φi > 0, 0 ≤ i ≤ I, 2 JJ II J I where n ≥ 0, ∆t ≤ h2 . We need the following lemma which is a discrete form of the maximum principle for ordinary differential equations. Page 17 of 26 Lemma 5.1. Let f ∈ C 1 (R) and let an and bn be two bounded sequences such that Go Back (5.4) (5.5) an+1 − an bn+1 − bn + f (an ) ≥ + f (bn ), ∆t ∆t a0 ≥ b 0 . Then we have an ≥ bn , n ≥ 0 for h small enough. n ≥ 0, Full Screen Close Proof. Let Zn = an − bn . We get Zn+1 − Zn + f 0 (ξn )Zn ≥ 0, ∆t (5.6) where ξn is an intermediate value between an and bn . Obviously Zn+1 ≥ Zn (1 − ∆tf 0 (ξn )). (5.7) Since an and bn are bounded and f ∈ C 1 (R), there exists a positive M such that |f 0 (ξn )| ≤ M . Let j be the first integer such that Zj < 0. From (5.5), j ≥ 0. We have Zj ≥ Zj−1 (1 − ∆tM ). Since ∆tM goes to zero as h → 0 and Zj−1 ≥ 0, we deduce that Zj ≥ 0 as h → 0 which is a contradiction. Therefore, Zn ≥ 0 for any n and we have proved the lemma. Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Title Page Now, we may state the following. Contents (n) Theorem 5.2. Let Uh be the solution of (5.1) – (5.3). We have Uh ≥ 0 and 1 (n) Uh ≤ 1 , p−1 ∞ (0) 1−p + A(p − 1)n∆t Uh ∞ where A = a p−1 . (0) 1+a∆tUh II J I Page 18 of 26 Go Back Full Screen ∞ Proof. A straightforward calculation yields (n) (n) ∆t (n) 2∆t U + 1 − Ui + Ui−1 2 2 (n+1) i+1 h h , (5.8) Ui = (n) p−1 1 + a∆t Ui JJ Close 1 ≤ i ≤ I − 1, (n+1) U0 (5.9) (n+1) UI (5.10) = 2∆t (n) U1 h2 (n) + 1 − 2∆t U0 h2 , p−1 (n) 1 + a∆t U0 2∆t (n) UI−1 h2 (n) + 1 − 2∆t UI 2 h = p−1 . (n) q−1 (n) 1 + a∆t UI + 2 hb ∆t UI Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Since 1 − (n) Uh 2 ∆t h2 is nonnegative, using a recursive argument, it is easy to see that (n) (n) ≥ 0. Let i0 be such that Ui0 = Uh . From (5.8), we get ∞ (n+1) Uh ∞ ≤ ∆t (n) U h2 i0 +1 (n) (n) + 1− Uh + Ui0 −1 ∞ (n) p−1 1 + a∆t Uh 2∆t h2 Contents if 1 ≤ i0 ≤ I − 1. ∞ Applying the triangle inequality and the fact that 1 − 2∆t is nonnegative, we arrive h2 at (n) Uh (n+1) (5.11) Uh ≤ ∞ p−1 . (n) ∞ 1 + a∆t Uh ∞ We obtain if i0 = 0 or i0 = I. Theinequality (5.11) that the same estimation implies (n+1) (n) (n) (0) Uh ≤ Uh and by iterating, we obtain Uh ≤ Uh . From ∞ ∞ Title Page ∞ ∞ JJ II J I Page 19 of 26 Go Back Full Screen Close (5.11), we also observe that (n+1) Uh − kU (n) k∞ ∞ ∆t (n) p a Uh ≤− ∞p−1 . (n) 1 + a∆t Uh ∞ (n) (0) Using the fact that Uh ≤ Uh , we have ∞ ∞ (n+1) (n) Uh − Uh (n) p ∞ ∞ ≤ −A Uh . ∆t ∞ We introduce the function α(t) which is defined as follows Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Title Page 1 α(t) = 1 . p−1 (0) 1−p + A(p − 1)t Uh ∞ We remark that α(t) obeys the following differential equation (0) α0 (t) = −Aαp (t), α(0) = Uh . ∞ Using a Taylor’s expansion, we have (∆t)2 00 ˜ α (tn ), α(tn+1 ) = α(tn ) + ∆tα0 (tn ) + 2 where t˜n is an intermediate value between tn and tn+1 . It is not hard to see that α(t) is a convex function. Therefore, we obtain α(tn+1 ) − α(tn ) ≥ −Aαp (tn ). ∆t Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Contents JJ II J I Page 20 of 26 Go Back Full Screen Close (n) From Lemma 5.1, we get Uh ∞ (n) Uh ∞ ≤ α(tn ), which ensures that 1 ≤ 1 , p−1 1−p (0) + A(p − 1)n∆t Uh ∞ and we have the desired result. Remark 2. The estimate of Theorem 5.2 is the discrete form of the one given in (1.4) for the continuous problem. Now, we approximate the solution u(x, t) of problem (1.1) – (1.3) by the solution (n) Uh of the following implicit scheme (n+1) (n+1) (5.13) UI (n) − Ui ∆t Ui (5.12) (n+1) = δ 2 Ui (n) − UI ∆t = (n+1) δ 2 UI (n) p−1 (n+1) − Ui Ui , Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Title Page Contents 0 ≤ i ≤ I − 1, (n) p−1 (n+1) 2b (n) p−1 (n+1) − a UI UI − UI UI , h JJ II J I Page 21 of 26 Go Back (5.14) (0) Ui = φi > 0, 0 ≤ i ≤ I, where n ≥ 0. Let us note that in the above construction, we do not need a restriction on the step time. The above equations may be rewritten in the following form: 2∆t (n+1) ∆t (n) p−1 (n) (n+1) U0 = − 2 U1 + 1 + 2 2 + a∆t U0 U0 , h h Full Screen Close ∆t ∆t (n+1) (n) p−1 (n+1) ∆t (n+1) = − 2 Ui−1 + 1 + 2 2 + a∆t Ui Ui − 2 Ui+1 , 1 ≤ i ≤ I−1, h h h 2∆t (n+1) ∆t (n) p−1 2b (n) q−1 (n) (n+1) UI = − 2 UI−1 + 1 + 2 2 + a∆t UI + ∆t UI UI , h h h (n) Ui which gives the following linear system (n+1) A(n) Uh Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and (n) = Uh where A(n) is the tridiagonal matrix defined as follows d0 −2∆t 0 0 ··· 0 h2 −∆t −∆t h2 d1 0 ··· 0 h2 −∆t −∆t 0 d 0 · ·· 2 h2 h2 . . .. (n) .. .. .. .. A = . . . . .. 0 −∆t −∆t 0 ··· dI−2 h2 h2 0 0 0 · · · −∆t dI−1 h2 −2∆t 0 0 0 ··· 0 h2 with di = 1 + 2 ∆t (n) + a∆t|Ui |p−1 h2 for Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 0 0 0 .. . , 0 −∆t h2 dI 0≤i≤I −1 Title Page Contents JJ II J I Page 22 of 26 Go Back Full Screen and ∆t (n) p−1 2b (n) q−1 + a∆t U ∆t U + I I . h2 h Let us remark that the tridiagonal matrix A(n) satisfies the following properties dI = 1 + 2 (n) (n) Aii > 0 and Aij < 0 i 6= j, Close (n) X (n) Aij . Aii > i6=j (n) Uhn These properties imply that exists for any n and Uh ≥ 0 (see for instance [2]). As we know that the solution of the discrete implicit scheme exists, we may state the following. (n) (n) Theorem 5.3. Let Uh be the solution of (5.12) – (5.14). We have Uh ≥ 0 and 1 (n) Uh ≤ 1 , p−1 1−p ∞ (0) + A(p − 1)n∆t Uh Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 ∞ where A = a p−1 . (0) 1+a∆tUh Title Page ∞ (n) ≥ 0 as we have seen above. Now, let us obtain the above (n) (n) estimate to complete the proof. Let i0 be such that Ui0 = Uh . Using the ∞ equality (5.12), we have ∆t ∆t (n) ∆t (n) (n) (n+1) (n) 1 + 2 2 + a∆t Uh Uh ≤ Uh + 2 Ui0 −1 + 2 Ui0 +1 h h h ∞ ∞ ∞ if 1 ≤ i0 ≤ I − 1. Proof. We know that Uh Applying the triangle inequality, we derive the following estimate (n) Uh (n+1) Uh ≤ ∞ p−1 . (n) ∞ 1 + a∆t Uh ∞ We obtain the same estimation if we take i0 = 0 or i0 = I. Reasoning as in the proof of Theorem 5.3, we obtain the desired result. Contents JJ II J I Page 23 of 26 Go Back Full Screen Close 6. Numerical Results In this section, we consider the explicit scheme in (5.1) – (5.3) and the implicit scheme in (5.12) – (5.14). We suppose that p = 2, q = 3, a = 1, b = 1, Ui0 = 2 0.8 + 0.8 ∗ cos(πhi) and ∆t = h2 . In the following tables, in the rows, we give the first n when (n) n∆tUh − 1 < ε, ∞ the corresponding time T n = n∆t, the CPU time and the order(s) of method computed from log((T4h − T2h )/(T2h − Th )) s= . log(2) Table 1: (ε = 10−2 ) Numerical times, numbers of iterations, CPU times (seconds), and orders of the approximations obtained with the implicit Euler method I 16 32 64 128 256 Tn 674.0820 674.2632 674.3085 674.3278 674.4807 n 345129 1.380890. 5.523.934 22095735 87383041 CPU time 103 660 6020 58290 574823 s 2.01 1.24 2.99 Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Title Page Contents JJ II J I Page 24 of 26 Go Back Full Screen Close Table 2: (ε = 10−2 ) Numerical times, numbers of iterations, CPU times (seconds) and orders of the approximations obtained with the explicit Euler method I 16 32 64 128 256 Tn 674.3281 674.3452 674.3290 674.3187 674.3098 n 345.255 1.381.058 5.524.102 22845950 88237375 CPU time 90 720 10820 323528 19457811 s 0.08 0.65 0.21 Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni vol. 9, iss. 2, art. 33, 2008 Title Page Contents JJ II J I Page 25 of 26 Go Back Full Screen Close References [1] L. ABIA, J.C. LÓPEZ-MARCOS AND J. MARTINEZ, On the blow-up time convergence of semidiscretizations of reaction-diffusion equations, Appl. Numer. Math., 26 (1998), 399–414. [2] T.K. BONI, On the asymptotic behavior of solutions for some semilinear parabolic and elliptic equation of second order with nonlinear boundary conditions, Nonl. Anal. TMA, 45 (2001), 895–908. Discretizations of a Semilinear Parabolic Equation Nabongo Diabate and Théodore K. Boni [3] T.K. BONI, Extinction for discretizations of some semilinear parabolic equations, C.R.A.S, Serie I, 333 (2001), 795–800. vol. 9, iss. 2, art. 33, 2008 [4] V.A. KONDRATIEV AND L. VÉRON, Asymptotic behaviour of solutions of some nonlinear parabolic or elliptic equation, Asymptotic Analysis, 14 (1997), 117–156. Title Page [5] R.E. MICKENS, Relation between the time and space step-sizes in nonstandard finite difference schemes for the fisher equation, Num. Methods. Part. Diff. Equat., 13 (1997), 51–55. Contents JJ II J I Page 26 of 26 Go Back Full Screen Close