• No results found

Monotone iterative technique for weakly coupled system of finite difference equations of time degenerate parabolic problems

N/A
N/A
Protected

Academic year: 2020

Share "Monotone iterative technique for weakly coupled system of finite difference equations of time degenerate parabolic problems"

Copied!
6
0
0

Loading.... (view fulltext now)

Full text

(1)

Monotone iterative technique for weakly coupled

system of finite difference equations of time

degenerate parabolic problems

Kailas S. Ahire

1

* and Dnyanoba B. Dhaigude

2

Abstract

The purpose of this paper is to develop monotone iterative technique for finite difference system, which correspond to a class of semilinear weakly coupled system of time degenerate parabolic initial boundary value problems and prove existence-comparison result.

Keywords

Monotone iterative technique, Finite difference equations,Dirichlet initial boundary value problem, Existence-comparison result.

AMS Subject Classification 26A33, 33E12 34A08, 35R11.

1Department of Mathematics, M. S. G.College, Malegaon Camp. Dist Nashik-423105, India (M.S.)

2Department of Mathematics, Dr. Babasaheb Ambedkar, Marathwada University, Aurangabad-431004, India (M.S.)

*Corresponding author:1[email protected]

Article History: Received21October2018; Accepted26March2019 c2019 MJM.

Contents

1 Introduction. . . 171

2 Upper Lower Solutions. . . .172

3 Monotone Iterative Technique. . . 173

4 Application. . . 175

References. . . 176

1. Introduction

The monotone iterative technique is one of the well known method employed successfully in the study of existence com-parison of solution of initial boundary value problem (IBVP) for nonlinear partial differential equations.In 1972,Sattinger [13] first developed monotone technique for nonlinear parabolic as well as elliptic boundary value problems. His work, later on refined and extended by many researchers and series of papers appeared in the literature. An excellent account of these results are given in the elegant books by Ladde, Laksh-mikantham and Vatsala [7], Pao [10] and Leung [8].

In 1985, Pao [9] introduced monotone technique for fi-nite difference equations of nonlinear parabolic and elliptic boundary value problems. A series of papers appeared in the literature for reaction diffusion problems under

differ-ent conditions (see [3],[11], [12])and references therein. Re-cently Dhaigude et.al[4]developed monotone technique for discrete weakly coupled system of finite difference equations of parabolic type. In this paper, the backward approximation for the spatial derivative terms are used and the monotone technique is developed, using the notion of upper-lower solu-tions for weakly coupled system of finite difference equasolu-tions which corresponds to weakly coupled system of semilinear time degenerate parabolic Dirichlet IBVP when the reaction functionsfi(1),n(ui,n,vi,n)and fi(2),n(ui,n,vi,n)are assumed to be

quasimonotone nonincreasing. Positivity lemma is the main ingredient used in the proof of these results.

(2)

2. Upper Lower Solutions

In this section,we obtain the discrete version of the Dirich-let Initial Boundary Value Problem (IBVP) for weakly coupled system of semilinear time degenerate parabolic equations.We consider the time degenerate Dirichlet IBVP for weakly cou-pled system of semilinear time degenerate parabolic equations.

d(1)(x,t)ut−D(1)(x,t)∇2u=f(1)(x,t,u,v);

d(2)(x,t)vt−D(2)(x,t)∇2v=f(2)(x,t,u,v);

in DT (2.1)

boundary conditions

u(x,t) =h(1)(x,t);

v(x,t) =h(2)(x,t);

on ST (2.2)

initial conditions

u(x,0) =ψ(1)(x);

v(x,0) =ψ(2)(x);

inΩ (2.3)

whereΩis a bounded domain inRn,(n=1,2, . . .)with

bound-ary ∂Ω. Suppose that the functions d(1)(x,t),d(2)(x,t)are nonnegative inDT. However we will not assume thatd(1)(x,t)

and d(2)(x,t)are bounded away from zero. Since the co-efficients d(1)(x,t) =0,d(2)(x,t) =0 for some (x,t)∈DT

and hence the system is time degenerate.The coefficients

D(1)(x,t),D(2)(x,t)are positive inDT. The functions

f(1)(x,t,u,v), f(2)(x,t,u,v)are in general nonlinear inu,v

and depend explicitly on(x,t).They are quasimonotone non-increasing. Now, we write the discrete version of the above continuous IBVP (2.1)- (2.3) by converting it into finite differ-ence equations as in [[1],[6]]. Let i=(i1,i2,...,ip) be a multiple

index withiν= 0,1,2,...,Mν+1 and letxi= (xi1,xi2,...,xip) be an

arbitrary mesh point inΩpwhereMνis the total number of

interior mesh points in thexiν co-ordinate direction.Denoted

byΩp, ¯Ωp,∂Ωp,ΛpandSpthe sets of mesh points inΩ, ¯Ω, ∂Ω,Ω×(0,T) and∂Ω×(0,T)respectively and ¯Λpdenote the

set of all mesh points in ¯Ω×[0,T] where ¯Ωis the closure of

Ω.Let (i,n) be used to represent the mesh point (xi,tn). Set

ui,n≡u(xi,tn),vi,n≡v(xi,tn),d (1) i,n ≡d

(1)(x i,tn),

di(2),n ≡d(2)(xi,tn);D (1) i,n ≡D

(1)(x i,tn),D

(2) i,n ≡D

(2)(x i,tn),

h(1)i,n ≡h(1)(xi,tn),h(2)i,n ≡h (2)(x

i,tn);u(1)i,0 ≡u(1)(xi,0),

u(2)i,0 ≡u(2)(xi,0),v(1)i,0 ≡v(1)(xi,0),v(2)i,0 ≡v(2)(xi,0);

ψi(1)≡ψ(1)(xi),ψi(2)≡ψ(2)(xi);

fi(1),n(ui,n,vi,n)≡ f(1)(xi,tn,ui,n,vi,n),

fi(2),n(ui,n,vi,n)≡ f(2)(xi,tn,ui,n,vi,n)

Letkn=tn−tn−1be thenthtime increment forn=1,2, ...N

andhνbe the spatial increment in thexiνco-ordinate direction.

Leteν= (0,...,1...,0) be the unit vector inRnwhere the constant

1 appears in theνthcomponent and zero elsewhere.The

stan-dard second order difference approximation is (see [1],[6])

4(ν)u(x

i,tn) =h(

−2)

ν [u(xi+hνeν,tn)−2u(xi,tn) +u(xi−hνeν,tn)]

and usual backward difference approximation forutisk−n1(ui,n−

ui,n−1).

Then the continuous Dirichlet IBVP (2.1)- (2.3) for time degenerate parabolic partial differential equations becomes

di(1),nk−n1(ui,n−ui,n−1)− p

ν=1

D(1)i,n4(ν)u i,n=f

(1)

i,n(ui,n,vi,n);

(i,n)∈Λp

di(2),nk−n1(vi,n−vi,n−1)− p

ν=1

D(2)i,n4(ν)v i,n=f

(2)

i,n(ui,n,vi,n);

(2.4)

boundary conditions

ui,n=h(1)i,n;

vi,n=h (2) i,n;

(i,n) ∈ Sp (2.5)

initial conditions

ui,0=Ψ(1)i ;

vi,0=Ψ (2) i ;

i ∈ Ωp (2.6)

In this way we have obtained the discrete Dirichlet IBVP (2.4)-(2.6) for time degenerate parabolic partial differential equations.The functions fi(1),nandfi(2),n are quasimonotone non-increasing.We define them as follows:

Definition 2.1. The C1-functions fi(1),nand fi(2),n are said to be quasimonotone nonincreasing if

fi(1),n(ui,n,vi,n)≥fi(1),n(ui,n,v0i,n)for v0i,n≥vi,n

and

fi(2),n(ui,n,vi,n)≥fi(2),n(u

0

i,n,vi,n)for u0i,n≥ui,n

respectively

Now we define upper and lower solutions of the discrete time degenerate Dirichlet IBVP (2.4)-(2.6).

Definition 2.2. The functions(u˜i,n,v˜i,n)and(uˆi,n,vˆi,n)with (u˜i,n,v˜i,n)≥(uˆi,n,vˆi,n)are called ordered upper and lower

solutions of discrete time degenerate Dirichlet IBVP(2.4)

(3)

(2.6)if they satisfy differential inequalities

di(1),nk−n1(u˜i,n−u˜i,n−1)− p

υ=1

D(1)i,n4(υ)u˜ i,n

≥fi(1),n(u˜i,n,v˜i,n);

di(1),nk−n1(uˆi,n−uˆi,n−1)− p

υ=1

D(1)i,n4(υ)uˆ i,n

≤fi(1),n(uˆi,n,vˆi,n);

(i,n)∈Λp

di(2),nk−n1(v˜i,n−v˜i,n−1)− p

υ=1

D(2)i,n4(υ)v˜ i,n

≥fi(2),n(u˜i,n,v˜i,n);

di(2),nk−n1(vˆi,n−vˆi,n−1)− p

υ=1

D(2)i,n4(υ)vˆ i,n

≤fi(2),n(uˆi,n,vˆi,n);

boundary conditions

˜

ui,n≥h (1) i,n ≥uˆi,n

(i,n)∈Sp

˜

vi,n≥h(2)i,n ≥vˆi,n

initial conditions

˜

ui,0≥Ψ(1)i ≥uˆi,0

i∈Ωp

˜

vi,0≥Ψ(2)i ≥vˆi,0

Definition 2.3. For any ordered upper and lower solutions

(u˜i,n,u˜i,n)and(vˆi,n,vˆi,n)the sector is denoted by Si,nand is

defined as

Si,n={(ui,n,vi,n)∈Λ¯p:(uˆi,n,vˆi,n)≤(ui,n,vi,n)≤(u˜i,n,v˜i,n)}

(2.7)

Suppose there exist nonnegative constants c(1)i,n andc(2)i,n

such that the function(fi(1),n and fi(2),n)satisfies the following one sided Lipschitz condition forui,n≥u0i,nandvi,n≥v0i,n

fi(1),n(ui,n,vi,n)−fi(1),n(u

0

i,n,vi,n)≥ −c(1)i,n(ui,n−u

0

i,n)

fi(2),n(ui,n,vi,n)−fi(2),n(ui,n,v0i,n)≥ −c (2)

i,n(vi,n−v0i,n)

(2.8)

Addingc(1)i,nui,nandc (2)

i,nvi,non both sides of equation in (2.4)

respectively, we get

d(1)i,nk−n1(ui,n−ui,n−1)− p

ν=1

D(1)i,n4(ν)u i,n+c

(1) i,nui,n

=c(1)i,nui,n+fi(1),n(ui,n,vi,n)

di(2),nk−n1(vi,n−vi,n−1)− p

ν=1

D(2)i,n4(ν)v i,n+c

(2) i,nvi,n

=c(2)i,nvi,n+fi(2),n(ui,n,vi,n)

Suppose

L[ui,n]≡di(1),nk

−1

n (ui,n−ui,n−1)− p

ν=1

D(1)i,n4(ν)u i,n

+c(1)i,nui,n

L[vi,n]≡di(2),nk

−1

n (vi,n−vi,n−1)− p

ν=1

D(2)i,n4(ν)v i,n

+c(2)i,nvi,n

Now we develop monotone scheme for the discrete time de-generate Dirichlet IBVP (2.4)-(2.6). The discrete version of the positivity lemma in [2] for the continuous problem play an important role in the construction of monotone and convergent sequences.We state it as follows:

Lemma 2.4. (Positivity Lemma) Suppose wi,nsatisfies the

following inequalities

di,nk−n1(wi,n−wi,n−1)− p

ν=1

Di,n∆(ν)wi,n+ci,nwi,n

≥0;(i,n)∈Λp

Bwi,n≥0;(i,n)∈Sp

wi,0≥0;i∈Ωp

where Bwi,n=α(xi,tn)|xi−xˆi|−1[w(xi,tn)−w(xˆi,tn)] +β(xi,tn)w(xi,tn),ci,n≥0,di,n≥0,xˆiis a suitable point in

Ωpand|xi−xˆi|is the distance between xiandxˆithen

wi,n≥0 in Λ¯p.

3. Monotone Iterative Technique

We choose suitable initial iterations(u(0)i,n,v(0)i,n)as either(u˜i,n,v˜i,n)

or(uˆi,n,vˆi,n)and construct a sequence of iterations{u (m) i,n,v

(m) i,n }

from the following iterative scheme.

L[u(m)i,n] =ci(1),nu(mi,n−1)+fi(1),n(ui(m,n−1),v(mi,n−1)),

L[v(m)i,n] =ci(2),nv(mi,n−1)+fi(2),n(u(m)i,n,v(mi,n−1)),

(i,n)∈Λp

(3.1)

¯

u(m)i,n =h(1)i,n

v(m)i,n =h(2)i,n,

(4)

¯

u(m)i,0i(1)

v(m)i,0i(2),

i ∈ Ωp (3.3)

It is a system of linear algebraic equations. Here m =1 and with suitable choice of initial iterations (u¯(0)i,n,v(0)i,n) =

(u˜i,n,vˆi,n). we get(u¯(1)i,n)from first equation.Put this value in

second equation,we get first iteration(u¯(1)i,n,v(1)i,n).Repeat the

process form=2,3, ...We construct a sequence{u¯(m)i,n,v(m)i,n}.

Further,suppose m =1 and with suitable choice of initial iter-ations(u(0)i,n,v¯(0)i,n) = (uˆi,n,v˜i,n). we get(u(1)i,n)from first

equa-tion.Put this value in second equation,we get first iteration

(u(1)i,n,v¯(1)i,n).Repeat the process for m=2,3,.... .We construct a

sequence{u(m)i,n,v¯(m)i,n}.An interesting point about the above

it-erative scheme is that the component(u¯(1)i,n)from first equation

is used immediately in second equation,to obtain(v¯(1)i,n). We note the above kind of iteration is similar to the Gauss-Seidal iterative method for algebraic systems.It has the advantage of obtaining faster convergent sequences.In the following,we obtain the monotone property of the sequences when initial iteration is either an upper solution or a lower solution.

Lemma 3.1(Monotone Property). Suppose that

(i)(u˜i,n,v˜i,n)and(uˆi,n,vˆi,n)are ordered upper and lower

solu-tions of discrete time degenerate Dirichlet IBVP(2.4)-(2.6)

(ii)the function(fi(1),n,fi(2),n)is quasimonotone nonincreasing in Si,n,

(iii)the function(fi(1),n,fi(2),n)satisfies the one sided Lipschitz condition(2.8)

Then the sequences{u¯(m)i,n,v(m)i,n }and{u(m)i,n,v¯(m)i,n}obtained

from iteration process(3.1)-(3.3)with(u¯(0)i,n,v(0)i,n) = (u˜i,n,vˆi,n)

and(u(0)i,n,v¯(0)i,n) = (uˆi,n,v˜i,n)possess the mixed monotone

prop-erty in the sense that their componentsu¯(m)i,n,v¯(m)i,n and u(m)i,n ,v(m)i,n, satisfy the following relation inΛ¯p

ˆ

ui,n≤u (1)

i,n ≤ · · · ≤u (m+1) i,n ≤u¯

(m+1)

i,n ≤ · · · ≤u¯ (1) i,n ≤u˜i,n

(3.4)

ˆ

vi,n≤v(1)i,n ≤ · · · ≤v (m+1) i,n ≤v¯

(m+1)

i,n ≤ · · · ≤v¯ (1) i,n ≤v˜i,n

(3.5)

for all m

Proof.Definewi,n=u¯ (0) i,n−u¯

(1)

i,n=u˜i,n−u¯ (1) i,nwhere ¯u

(0) i,n=u˜i,n.

ConsiderL[wi,n] =L[u˜i,n]−L[u¯(1)i,n]

L[wi,n] =di(1),nk

−1

n (u˜i,n−u˜i,n−1)− p

ν=1

D(1)i,n4(ν)u˜ i,n

+c(1)i,nu˜i,n−[d(1)i,nk

−1 n (u¯

(1) i,n−u¯

(1) i,n−1)

p

ν=1

D(1)i,n4(ν)u¯(1) i,n+c

(1) i,nu¯

(1) i,n]

=di(1),nk−n1(u˜i,n−u˜i,n−1)− p

ν=1

D(1)i,n4(ν)u˜ i,n

+c(1)i,nu˜i,n−[c (1) i,nu˜i,n+f

(1)

i,n(u˜i,n,vˆi,n)]

(By iteration scheme)

=di(1),nk−n1(u˜i,n−u˜i,n−1)− p

ν=1

D(1)i,n4(ν)u˜ i,n

−fi(1),n(u˜i,n,vˆi,n)≥0

Since ˜ui,nis an upper solution.

Thus we have

d(1)i,nk−n1(wi,n−wi,n−1)− p

ν=1

D(1)i,n4(ν)w

i,n+c(1)i,nwi,n

≥0;(i,n)∈Λp

wi,n=u˜i,n−hi(1),n ≥0;(i,n)∈Sp

wi,0=u˜i,0−Ψ(1)i ≥0;i∈Ωp

By Positivity lemma2.4,we getwi,n≥0 implies that

¯

u(1)i,n ≤u˜i,n.

Define z(1)i,n =v¯i(1),n−v(1)i,n.Consider

L[z(1)i,n] =L[v¯i(1),n]−L[v(1)i,n]

L[z(1)i,n] =di(2),nk−n1(v¯(1)i,n−v¯(1)i,n1)−

p

ν=1

D(2)i,n4(ν)v¯(1) i,n

+c(2)i,ni(1),n−[di(2),nk−n1(v(1)i,n−v(1)i,n1)

p

ν=1

D(2)i,n4(ν)v(1) i,n+c

(2) i,nv

(1) i,n]

=c(2)i,nv¯(0)i,n+fi(2),n(ui(1),n,v¯(0)i,n)−c(2)i,nv(0)i,n

−fi(2),n(u¯i(1),n,v(0)i,n)(By iteration scheme)

=[c(2)i,n(v¯(0)i,n−v(0)i,n) +fi(2),n(u(1)i,n,v¯(0)i,n)

−fi(2),n(ui(1),n,v(0)i,n)] + [fi(2),n(u(1)i,n,v(0)i,n)

−fi(2),n(u¯(1)i,n,v(0)i,n)]≥0

fi(2),n is Lipchitzian and quasimonotone nonincreasing

d(2)i,nk−n1(zi(1),n−z(1)i,n1)−

p

ν=1

D(2)i,n4(ν)z(1) i,n+c

(2) i,nz

(1) i,n ≥0;

z(1)i,n =v¯(1)i,n−vi(1),n ≥h(2)i,n−v(1)i,n

(5)

For(i,n)∈Λp,≥0;(i,n)∈Spandi∈ΩpIn view of positivity

lemma2.4,we getz(1)i,n≥0 implies thatv(1)i,n ≤v¯(1)i,nWe conclude that

ˆ

ui,n≤u (1) i,n ≤u¯

(1)

i,n ≤u˜i,nin ¯Λp

ˆ

vi,n≤v(1)i,n ≤v¯ (1)

i,n ≤v˜i,nin ¯Λp

Thus result is true form=1. Assume that it is true form=l

u(li,n−1)≤u(l)i,n≤u¯(l)i,n≤u¯(li,n−1)in ¯Λp

v(li,n−1)≤v(l)i,n≤v¯(l)i,n≤v¯(li,n−1)in ¯Λp

Now we prove that it is true form=l+1.

Define w(l)i,n=u¯(l)i,n−u¯(l+1)i,n .Consider

L[w(l)i,n] =L[u¯i(l),n]−L[u¯(l+1)i,n ]

L[w(l)i,n] =di(1),nk−n1(u¯(l)i,n−u¯(l)i,n1)

p

ν=1

D(1)i,n4(ν)u¯(l) i,n+c

(1) i,nu¯

(l) i,n−

[d(1)i,nk−n1(u¯(l+1)i,n −u¯(l+1)i,n1)

p

ν=1

D(1)i,n4(ν)u¯(l+1) i,n +c

(1) i,nu¯

(l+1) i,n ]

=c(1)i,nu¯(li,n−1)+fi(1),n(u¯(li,n−1),v(li,n−1))

−[c(1)i,nu(l)i,n+fi(1),n(u(l)i,n,v¯(l)i,n)]

(By iteration scheme)

=c(1)i,n(u¯(li,n−1)−u(l)i,n) +fi(1),n(u¯i(l,n−1),v(li,n−1))

−fi(1),n(u(l)i,n,v¯(l)i,n)

=[c(1)i,n(u¯(li,n−1)−u(l)i,n) +fi(1),n(u¯i(k,n−1),v(li,n−1))

−fi(1),n(u(l)i,n,v(li,n−1))]+

[fi(1),n(u(l)i,n,v(li,n−1))

−fi(1),n(u(l)i,n,v¯(l)i,n)]

≥0

fi(1),n is Lipchitzian and quasimonotone nonincreasing. We have

di(1),nk−n1(wi(l),n−w(l)i,n1)−

p

ν=1

D(1)i,n4(ν)w(l) i,n

+c(1)i,nw(l)i,n≥0;

w(l)i,n=u¯(l)i,n−u(l)i,n≥h(1)i,n−u(l)i,n≥0;

w(l)i,0=u¯(l)i,0−ui(l),0≥Ψ(1)i −u(l)i,0≥0;

For(i,n)∈Λp,(i,n)∈Spandi∈ΩpBy lemma2.4,we get

w(l)i,n≥0 implies that ¯u(l+1)i,n ≤u¯(l)i,n.On similar lines we can

prove thatu(l)i,n≤u(l+1)i,n andu(l+1)i,n ≤u¯(l+1)i,n .

Define z(l)i,n=v¯(l)i,n−v¯(l+1)i,n .Consider

L[z(l)i,n] =L[v¯i(l),n]−L[v¯(l+1)i,n ]

L[z(l)i,n] =di(2),nk−n1(v¯(l)i,n−v¯(l)i,n1)−

p

ν=1

D(2)i,n4(ν)v¯(l) i,n

+c(2)i,nv¯(l)i,n−[d(2)i,nkn−1(v¯(l+1)i,n −v¯(l+1)i,n1)

p

ν=1

D(2)i,n4(ν)v¯(l+1) i,n +c

(2) i,nv¯

(l+1) i,n ]≥0

it follows from iteration scheme,Lipchitzian and quasimono-tone nonincreasing property of fi(2),n.We have

d(2)i,nk−n1(zi(l),n−z(l)i,n1)−

p

ν=1

D(2)i,n4(ν)z(l) i,n+c

(2) i,nz

(l) i,n≥0;

z(l)i,n=v¯(l)i,n−v¯(l+1)i,n ≥h(2)i,n−v¯(l+1)i,n ≥0;

z(l)i,0=v¯(1)i,0−v¯i(l+1),0 ≥Ψ(2)i −v¯(l+1)i,0 ≥0;

For(i,n)∈Λp,(i,n)∈Spandi∈Ωp. In view of positivity

lemma2.4,we getw(l)i,n≥0 implies that ¯vi(l+1),n ≤v¯(l)i,n.Note that

using similar arguments we can provev(l)i,n≤v(l+1)i,n as well as

v(l+1)i,n ≤v¯(l+1)i,n .Thus from principle of mathematical induction result is true for all m

4. Application

In this section, we show that the monotone iterative tech-nique is successfully applied to prove existence - comparison result for the solution of the discrete time degenerate Dirichlet IBVP (2.4)-(2.6)

Theorem 4.1. (Existence -Comparison Theorem)Suppose that (i)(u˜i,n,v˜i,n)and(uˆi,n,vˆi,n)are ordered upper and lower

solu-tions of discrete time degenerate Dirichlet IBVP(2.4)-(2.6)

(ii)the function(fi(1),n,fi(2),n)is quasimonotone nonincreasing in Si,n,

(iii)the function(fi(1),n,fi(2),n)satisfies the one sided Lipschitz condition(2.8)

Then the sequence{u¯(m)i,n,v¯(m)i,n}converges monotonically from above to maximal solution{u¯i,n,v¯i,n}and the sequence

{u(m)i,n,v(m)i,n} converges monotonically from below to mini-mal solution{ui,n,vi,n}of discrete Dirichlet IBVP(2.4)-(2.6). More over maximal solution{u¯i,n,v¯i,n}and minimal solution

{ui,n,vi,n}satisfy the relation,

(uˆi,n,vˆi,n)≤(ui,n,vi,n)≤(u¯i,n,v¯i,n)≤(u˜i,n,v˜i,n)inΛ¯p (4.1)

(6)

bounded from above hence it is convergent to some limit function.So,

lim

m→∞

¯

u(m)i,n =u¯i,n; lim m→∞

¯

v(m)i,n =v¯i,n

and

lim

m→∞u

(m)

i,n =ui,n; lim m→∞v

(m) i,n =vi,n

exist and called maximal and minimal solutions respectively of the discrete Dirichlet IBVP (2.4)-(2.6) and they satisfy the relation

(uˆi,n,vˆi,n)≤(ui,n,vi,n)≤(u¯i,n,v¯i,n)≤(u˜i,n,v˜i,n)inΛp (4.2)

This completes the proof.

References

[1] Ames,W.F.: Numerical methods for partial differential

equations(3rd edition).Academic Press, San Diego, 1992.

[2] Dhaigude, D.B., Dhaigude, R.M.,Dhaigude,C.D.:

Mono-tone technique for nonlinear time degenerate reaction-diffusion problems,Recent Advances in Mathematical Sciences and Applications, (2009), 112–120.

[3] Dhaigude,D.B., Kiwne, S.B.,Dhaigude, R.M.: Method

of upper lower solutions for finite difference coupled reaction diffusion systems,Bull. Marathwada Math. Soc., 8(2007), 21-31.

[4] Dhaigude, D.B., Kiwne ,S.B.,Dhaigude, R. M.:

Mono-tone iterative scheme for weakly coupled system of fi-nite difference reaction-diffusion equations,Comm. Appl. Anal.,12(2)(2008), 161–172.

[5] Dhaigude, D.B., Sontakke, B.R.,Dhaigude, C.D.:

Mono-tone technique for nonlinear degenerate weakley cou-pled system of parabolic problems,Comm. Appl. Anal.,

15(1)(2011), 13–24.

[6] Forsythe, G.E.,Wasow, W.R.: Finite difference methods

for partial differential equations, Wiley, New York, 1964.

[7] Ladde,G.S., Lakshmikantham,V., Vatsala,A.S.:

Mono-tone iterative techniques for nonlinear differential equa-tions. Pitman, New York, 1985.

[8] Leung, A.W.: Systems of nonlinear partial differential

equations. Kluwer, Dordrecht-Boston, 1989.

[9] Pao, C.V.: Monotone iterative method for finite difference

system of reaction diffusion equations, Numer. Math.,

46(1985), 571–586.

[10] Pao, C.V.: Nonlinear parabolic and elliptic equations,

Plenum Press, New York, 1992.

[11] Pao, C.V.: Numerical methods for coupled systems of

nonlinear parabolic boundary value problems,J. Math. Anal. Appl.151(1990), 581–608.

[12] Pao, C.V.: Numerical methods for coupled systems of

nonlinear parabolic boundary value problems,J. Math. Anal. Appl.,171(2002), 681–708.

[13] Sattinger, D.H.: Monotone methods in nonlinear elliptic

and parabolic boundary value problems, Indiana Uni. Math.J.,21(1972), 979–1000.

[14] Sontakke, B.R.,Dhaigude,C.D.: Monotone method for

nonlinear weakley coupled degenerate parabolic system,

Recent Advances in Mathematical Sciences and Applica-tions, (2009), 258–268.

? ? ? ? ? ? ? ? ? ISSN(P):2319−3786 Malaya Journal of Matematik

References

Related documents

In order words, in the light of the above conceptual exposition of work life balance, it is quite glaring that to sustain a balance between work and personal

AD: Alzheimer ’ s disease; BMI: body mass index; CABG: coronary artery bypass surgery; CPSP: chronic postsurgical pain; ICU: intensive care unit; MCI: mild cognitive impairment;

Fasting blood and urine and non-fasting blood following oral glucose intake were analysed in 90 Caucasians, South Asians and South East/East

he District University in partnership with the District Department of Transportation developed the project "Technical, legal, financial and social withdrawal

To understand the major changes in Islamic political thought and Koranic religion, one must go to the three men who reinterpreted Islam along radical

DART and CUTE are the two techniques in dynamic test generation DART short for “Directed Automated Random Testing”, blends dynamic test generation with random testing and

An evaporator is used in an air-conditioning system or refrigeration system to allow a compressed cooling chemical, such as Freon or R-22, to evaporate from

Radenovic, Coupled coincidence point theorems for generalized nonlinear contraction in partially ordered metric spaces, Fixed Point Theory Appl. Kim, Common …xed point theorems for (