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ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp)

LARGE TIME BEHAVIOR OF SOLUTIONS TO SECOND-ORDER DIFFERENTIAL EQUATIONS WITH p-LAPLACIAN

MILAN MEDVE ˇD, EVA PEK ´ARKOV ´A

Abstract. We study asymptotic properties of solutions for certain second- order differential equation withp-Laplacian. The main purpose is to investi- gate when all global solutions behave at infinity like nontrivial linear functions.

Making use of Bihari’s inequality and its Dannan’s version, we obtain results for differential equations withp-Laplacian analogous which extend those known in the literature concerning ordinary second order differential equations.

1. Introduction

In this paper, we study asymptotic properties of the second-order differential equation withp-Laplacian

(|u0|p−1u0)0+f(t, u, u0) = 0, p≥1. (1.1) In the sequel, it is assumed that all solutions of (1.1) are continuously extendable throughout the entire real axis. We refer to such solutions as to global solutions.

We shall prove sufficient conditions under which all global solutions are asymptotic to at+b, as t → +∞, where a, b are real numbers. The problem for ordinary second order differential equations without p-Laplacian has been studied by many authors, e. g. by Cohen [6], Constantin [7], Dannan [8], Kusano and Trench [9, 10], Rogovchenko [13], Rogovchenko [14], Tong [15] and Trench [16]. Our results are more close to those obtained in the papers [13, 14]. The main tool of the proofs are the Bihari’s and Dannan’s integral inequalities. We remark that sufficient conditions on the existence of global solutions for second order differential equations and second order functional-differential equations with p-Laplacian are proved in the papers [1, 2, 3, 4, 11]. Many references concerning differential equations with p-Laplacian can be found in the paper by Rachunkov´a, Stanˇek and Tvrd´y [12], where boundary value problems for such equations are treated.

Let

u(t0) =u0, u0(t0) =u1, (1.2) whereu0, u1∈Rbe initial condition for solutions of (1.1).

We say that a solutionu(t) of (1.1) possesses the property (L) ifu(t) =at+b+o(t) ast→ ∞, wherea,b are real constants.

2000Mathematics Subject Classification. 34C11.

Key words and phrases. Second order differential equation;p-Laplacian; Bihari’s inequality;

asymptotic properties; Dannan’s inequality.

c

2008 Texas State University - San Marcos.

Submitted June 9, 2008. Published August 11, 2008.

1

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2. Main results

Theorem 2.1. Let p≥1,r >0 andt0>0. Suppose that the following conditions are satisfied:

(1) f(t, u, v)is a continuous function inD={(t, u, v) :t∈< t0,∞), u, v∈R}, wheret0>0

(2) There exist continuous functionsh, g:R+=<0,∞)→R+ such that

|f(t, u, v)| ≤h(t)g |u|

t r

|v|r,(t, u, v)∈D,

where fors >0 the functiong(s)is positive and nondecreasing, Z

t0

h(s)ds <∞,

and if we denote

G(x) = Z x

t0

ds sr/pg(sr/p), then

G(∞) = Z

t0

ds

sr/pg(sr/p) =p r

Z

a

τpr−1dτ τ g(τ) =∞, wherea= (t0)r/p.

Then any global solutionu(t)of the equation (1) possesses the property (L).

Proof. Without loss of generality we may assumet0= 1. Let u(t) be a solution of (1.1), (1.2). Then

(u0(t))p≤ |u0(t)|p−1u0(t)≤c2+ Z t

1

|f(s, u(s), u0(s))|ds, (2.1) wherec2=|u1|p. Letw(t) be the right-hand side of inequality (2.1). Then

u0(t)≤w(t)1/p and

u(t)≤c1+ Z t

1

w(s)1/pds≤c1+ (t−1)w(t)1/p≤t[c1+w(t)1/p], (2.2) wherec1=|u0|, i.e.

u(t)≤t[c1+w(t)1/p], t≥1.

Applying the inequality (A+B)p ≤2p−1(Ap+Bp), A, B≥0 and the assumption (2) of Theorem 2.1 we obtain from (2.2):

|u(t)|

t p

≤2p−1cp1+ 2p−1w(t)

≤2p−1cp1+ 2p−1 c2+

Z t

0

h(s)g |u(s)|

s r

|u0(s)|r ds.

(2.3)

Let

d= 2p−1(cp1+c2), H(t) = 2p−1h(t). (2.4) Then

|u(t)|

t p

≤d+ Z t

1

H(s)g|u(s)|

s r

|u0(s)|rds:=z(t); (2.5)

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i.e.,

|u(t)|

t r

≤z(t)r/p.

From the assumption (2) of Theorem 2.1 and the inequality (2.1) it follows

|u0(t)|p≤up1+ Z t

1

h(s)g |u(s)|

s r

|u0(s)|rds≤z(t);

i.e. we have

|u0(t)|p≤z(t).

Sinceg(s) is nondecreasing, the inequality (2.3) yields g|u(t)|

t r

≤g(z(t)r/p) and so we conclude fort≥1,

z(t)≤d+ Z t

1

H(s)g(z(t)r/p)z(t)r/pds.

From the assumption (2) of Theorem 2.1 it follows that the inverse G−1 of G is defined on the interval (G(+0),∞). Applying the Bihari theorem (see [5]) we obtain

z(t)≤G−1

G(d) + 2p−1 Z

1

h(s)ds

:=K <∞.

Therefore the inequality (2.4) yields

|u0(t)| ≤L:=K1/p and from (2.3) we have

|u(t)|

t ≤L.

Since Z t

1

|f(s, u(s), u0(s))|ds≤ Z t

1

h(s)g(|u(s)|

s r

)|u0(s)|rds≤z(t)≤K for t ≥ 1, the integral R

1 |f(s, u(s), u0(s))|ds exists. From (2.5) it follows that there existsa∈Rsuch that

t→∞lim u0(t) =a.

By the l’Hospital rule, we can conclude that

t→∞lim u(t)

t = u1+Rt

1u0(τ)dτ

t = lim

t→∞u0(t) =a.

Therefore there existb∈Rsuch thatu(t) =at+b+o(t).

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Example 1. Lett0= 1, p≥r >0, f(t, u, u0) =η(t)t1−αe−tu

t p−r

lnh

2 +|u|

t ri

(u0)r, t≥1, (2.6) where 0 < α < 1, η(t) is a continuous function on interval h1,∞) with K = supt≥1|η(t)|<∞.

The functionf(t, u, u0) can be written in the form f(t, u, u0) =h(t)g

[u t]r

(u0)r, (2.7)

where h(t) = η(t)t1−αe−t, g(u) = upr−1ln(2 +|u|). Obviously g(u) is positive, continuous and nondecreasing function, R

1 |h(s)|ds < KΓ(α) = KR

0 s1−αe−sds and

Z

1

τpr−1dτ τ g(τ) =

Z

1

dτ τln(2 +τ) >

Z

1

(2 +τ) ln(2 +τ)=∞. (2.8) Thus we have proved that all conditions of Theorem 1 are satisfied. This means that for every solutionu(t) of the initial value problem (1.1), (1.2) there exist numbers a, bsuch thatu(t) =at+b+o(t) ast→ ∞.

Theorem 2.2. Let p≥1, r >0 andt0>0. Suppose the following conditions are satisfied:

(1) The functionf(t, u, v) is continuous in D ={(t, u, v) :t∈< t0,∞), u, v ∈ R},

(2) There exist continuous functionsh1, h2, h3, g1, g2:R+→R+ such that

|f(t, u, v)| ≤h1(t)g1

|u|

t r

+h2(t)g2(|v|r) +h3(t),(t, u, v)∈D, where Hi := R

t0 hi(s)ds < ∞, i = 1,2,3, for s > 0 the functions g1(s), g2(s)are nondecreasing and if

G(x) = Z x

t0

ds

g1(sr/p) +g2(sr/p) then

G(∞) = Z

t0

ds

g1(sr/p) +g2(sr/p) =p r

Z

a

τpr−1

g1(τ) +g2(τ) =∞, wherea= (t0)r/p.

Then any global solutionu(t)of the equation (1) possesses the property (L).

Proof. Without loss of generality we may assumet0= 1. By the standard existence results, it follows from the continuity of the function f that equation (1.1) has solutionu(t) corresponding to the initial datau(1) =u0,u0(1) =u1. Two times of integration (1.1) from 1 tot, yields fort≥1

(u0(t))p≤ |u0(t)|p−1u0(t) =up1− Z t

1

f(s, u(s), u0(s))ds, (2.9) u(t)≤u0+ (t−1)h

up1− Z t

1

f(s, u(s), u0(s))dsi1/p

. (2.10)

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It follows from (2.9) and (2.10) that fort≥1,

|u0(t)| ≤w(t)1/p,

|u(t)| ≤t c1+w(t)1/p ,

wherec1=|u0|,c2=|u1|p, w(t) =c2+Rt

1|f(s, u(s), u0(s))|ds. Using the assump- tion (2) we obtain fort≥1

|u0(t)| ≤h c2+

Z t

1

h1(s)g1

|u(s)|

s r

ds +

Z t

1

h2(s)g2(|u0(s)|r)ds+ Z t

1

h3(s)dsi1/p ,

|u(t)|

t ≤c1+h c2+

Z t

1

h1(s)g1

|u(s)|

s r

ds +

Z t

1

h2(s)g2(|u0(s)|r)ds+ Z t

1

h3(s)dsi1/p

.

Applying the inequality (A+B)p≤2p−1(Ap+Bp), whereA, B≥0, we obtain

|u(t)|

t p

≤d+ Z t

1

H1(s)g1

|u(s)|

s r

ds +

Z t

1

H2(s)g2(|u0(s)|r)ds+ Z t

1

H3(s)ds.

(2.11)

where d= 2p−1(cp1+c2),Hi(t) = 2p−1hi(t), i= 1,2,3. Denote byz(t) the right- hand side inequality (2.11)

|u0(t)|r≤z(t)r/p, |u(t)|

t r

≤z(t)r/p. (2.12)

Since the functiong1(s) andg2(s) are nondecreasing fors >0, we obtain g1

|u0(t)|r

≤g1

z(t)r/p

, g1h|u(t)|

t ir

≤g2

z(t)r/p .

Thus, fort≥1, z(t)≤d+

Z t

1

H1(s)g1(z(s)r/p)ds+ Z t

1

H2(s)g2(z(s)r/p)ds+ Z t

1

H3(s)ds. (2.13) Furthermore, due to evident inequality

H1(s)g1(z(s)r/p) +H2(s)g2(z(s)r/p)≤(H1(s) +H2(s))(g1(z(s)r/p) +g2(z(s)r/p)) (2.14) By (2.14), we have

z(t)≤d+ ¯H3+ Z t

1

(H1(s) +H2(s))(g1(z(s)r/p) +g2(z(s)r/p))ds;

i.e.,

z(t)≤d+ 2p−1¯h3+ 2p−1 Z t

1

(h1(s) +h2(s))(g1(z(s)r/p) +g2(z(s)r/p))ds. (2.15) Applying Bihari’s inequality (see [5]) to (2.15), we obtain, fort≥1,

z(t)≤G−1

G(d+ 2p−1¯h3) + 2p−1 Z t

1

(h1(s) +h2(s))ds ,

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where

G(x) = Z x

1

ds

g1(sr/p) +g2(sr/p),

andG−1(x) is the inverse function forG(x) defined forx∈(G(+0),∞). Note that G(+0)<0, andG−1(x) is increasing.

Now, let

K=G(d+ 2p−1¯h3) + 2p−1(¯h1+ ¯h2)<∞.

SinceG−1(x) is increasing, we have

z(t)≤G−1(K)<∞;

so it yields

|u(t)|

t ≤G−1(K), |u0(t)| ≤G−1(K).

Using assumption (2) of the Theorem 2.2, we have Z t

1

|f(s, u(s), u0(s))|ds≤h1(t)g1|u|

t r

+h2(t)g2(|u0(s)|r) +h3(t)

≤z(t)≤G−1(K), wheret≥1, the integralRt

1|f(s, u(s), u0(s))|dsconverges, and there exists ana∈R such that

t→∞lim u0(t) =a.

Example 2. Lett0= 1, p≥r >0,

f(t, u, v) =η1(t)t1−α1e−t u t

p−r

ln 2 + u

t r

2(t)t1−α2e−tvp−rln(3 +vr) +η3(t)t1−α3e−t

where 0< αi<1,ηi(t) are continuous functions on [1,∞),Ki= supt≥1i(t)|<∞, i= 1,2,3. Then f(t, u, u0) can be written as

f(t, u, v) =h1(t)g1 [u t]r

+h2(t)g2(vr) +h3(t),

wherehi(t) =ηi(t)t1−αie−t,i= 1,2,3,g1(u) =upr ln(2 +u),g2(u) =uprln(2 +u).

Then

|f(t, u, v)| ≤ |h1(t)|g1

[u

t]r

+|h2(t)|g2(|v|r) +|h3(t)|,

where (t, u, v)∈D={(t, u, v) :t∈ h1,∞), u, v∈R},|hi(t)| ≤KiΓ(αi),i= 1,2,3 and obviously we have

G(∞) = Z

1

τpr−1dτ g1(τ) +g2(τ)

= Z

1

τpr−1

τpr[ln(2 +τ) + ln(3 +τ)]

≥ 1 2

Z

1

(3 +τ) ln(3 +τ)=∞.

This means that all assumptions of Theorem 2.2 are satisfied and thus any global solutionu(t) of the equation (1) possesses the property (L).

Theorem 2.3. Let t0>0. Suppose that the following assumptions hold:

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(i) there exist nonnegative continuous function h1, h2, g1, g2 :R+ → R+ such that

|f(t, u, v)| ≤h1(t)g1

|u|

t r

+h2(t)g2(|v|r);

(ii) fors >0 the functiong1(s),g2(s)are nondecreasing, and g1(αu)≤ψ1(α)g1(u), g2(αu)≤ψ2(α)g2(u)

for α ≥ 1, u ≥ 0, where the functions ψ1(α), ψ2(α) are continuous for α≥1;

(iii) R

t0 hi(s)ds=Hi<∞,i= 1,2.

Assume that there exists a constantK≥1 such that K−11(K) +ψ2(K))2p−1(H1+H2)≤

Z +∞

t0

ds

g1(sr/p) +g2(sr/p)

=p r

Z +∞

a

τpr−1dτ g1(τ) +g2(τ),

where a= (t0)r/p. Then any global solutionu(t) of the equation (1.1) with initial data u(t0) = u0, u0(t0) = u1 such that (|u0|+|u1|)p ≤ K possesses the property (L).

Proof. Without loss of generality we may assumet0= 1. Arguing in the same way as in Theorem 2.1, we obtain by assumption (i) of Theorem 2.3

|u0(t)| ≤h

|u1|p+ Z t

1

h1(s)g1

[u(s)

s ]r ds+

Z t

1

h2(s)g2(|u0(s)|r)dsi1/p

(2.16)

|u(t)|

t ≤ |u0|+h

|u1|p+ Z t

1

h1(s)g1 [u(s)

s ]r ds+

Z t

1

h2(s)g2(|u0(s)|r)dsi1/p

(2.17) wheret≥1.

|u(t)|

t p

≤K+ 2p−1Z t 1

h1(s)g1 [u(s)

s ]r ds+

Z t

1

h2(s)g2(|u0(s)|r)ds

, (2.18) where K = 2p−1(|u0|p+|u1|p) ≥(|u0|+|u1|)p. Denoting by z(t) the right-hand side of inequality (2.18) we have by (2.16) and (2.18)

|u0(t)|r≤z(t)r/p, |u(t)|

t r

≤z(t)r/p. (2.19)

Since the functiong1(s),g2(s) are nondecreasing fors >0, fort≥1, (2.19) yields z(t)≤K+ 2p−1Z t

1

h1(s)g1 z(s)r/p ds+

Z t

1

h2(s)g2(z(s)r/p)

ds. (2.20) By assumption (ii) of Theorem 2.3, the functionsg1(u),g2(u) belong to the classH. Furthermore, ifg1(u) andg2(u) belong to the classHwith corresponding multiplier functionψ1(α),ψ2(α) respectively, then the sumg1(u) +g2(u). Applying Bihari’s Theorem (see [5]) to (2.20), we have fort≥1

z(t)≤KW−1(K−11(K) +ψ2(K)))2p−1 Z t

1

(h1(s) +h2(s))ds, (2.21) where

W(u) = Z u

1

ds g1 sr/p

+g2 sr/p,

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and W−1(u) is inverse function for W(u). Inequality (2.21) holds for all t ≥ 1 because

(K−11(K) +ψ2(K))2p−1(H1+H2) =L <∞.

SinceW−1(u) is increasing, we get

z(t)≤KW−1(L)<∞, so it follows from (2.19), (2.20) that

|u(t)|

t ≤KW−1(L), |u0(t)| ≤KW−1(L).

The rest of the proof is similar to that of Theorem 2.2 and thus it is omitted.

Example 3. Lett0>0. Consider (1.1) withp≥1,pq = 2,

f(t, u, v) =h1(t)u2=h2(t)v2, (2.22) where h1(t) = η1t(t)2 t1−α1e−t, h2(t) = η2(t)t1−α2e−t, 0< αi ≤1, ηi(t), i= 1,2 are continuous functions on the interval h0,∞) withKi = supt≥t0i(t)| <∞. Then we can write

f(t, u, v) =η1(t)t1−α1e−t u t

2

2(t)t1−α2e−tv2 (2.23) and

|f(t, u, u0)| ≤K1Γ(α1)g1(u) +K2Γ(α2)g2(u0), (2.24) whereg1(u) =u2,g2(u0) = (u0)2 . The functionsg1, g2 satisfy the condition (ii) of Theorem 2.3 withψ1(α) =ψ2(α) =α2 and

Z

t0

τpr−1dτ g1(τ) +g2(τ) =

Z

t0

τ =∞. (2.25)

Thus all assumptions of Theorem 2.3 are satisfied and therefore any global solution u(t) of the equation (1.1) (independently on the initial valuesu0, u1) possesses the property (L).

Theorem 2.4. Let t0>0. Suppose that the assumptions (i) and (iii) of Theorem 2.3 hold, while (ii) is replaced by

(ii’) fors >0 the functions g1(s), g2(s) are nonnegative, continuous and non- decreasing, g1(0) =g2(0) = 0 and satisfy a Lipschitz condition

|g1(u+v)−g1(u)| ≤λ1v, |g2(u+v)−g2(u)| ≤λ2v, whereλ1, λ2 are positive constants.

Then any global solutionu(t)of (1.1)with initial datau(t0) =u0,u0(t0) =u1such that |u0|p+|u1|p≤K possesses property (L).

Proof. Applying [8, Corollary 2] to (2.20), we have fort≥1 z(t)≤K+ 2p−1

Z t

t0

(h1(s) +h2(s))(g1(K) +g2(K))

×exp 2p−1

Z t

t0

12)(h1(τ) +h2(τ))dτ ds

≤K+ 2p−1(H1+H2)(g1(K) +g2(K)) exp

2p−112)(H1+H2)

<+∞.

The proof can be completed with the same argument as in Theorem 2.2.

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Theorem 2.5. Let t0>0. Suppose that there exist continuous functionsh, g1, g2: R+→R+ such that

|f(t, u, v)| ≤h(t)g1 |u|

t r

g2(|v|r), where fors >0 the functions g1(s),g2(s)are nondecreasing;

Z

t0

h(s)ds <∞,

and if we denote

G(x) = Z x

t0

ds g1(sr/p)g2(sr/p) then G(+∞) = prR

a

τpr−1

g1(τ)g2(τ)dτ = +∞, where a= (t0)pr. Then any global solu- tionu(t)of the equation (1.1)possesses the property (L).

Proof. Without loss of generality we may assumet0= 1. Arguing as in the proof of Theorem 2.2, we obtain fort≥1

|u0(t)| ≤h

|u1|p+ Z t

1

h(s)g1

[u(s)

s ]r

g2(|u0(s)|r)dsi1/p ,

|u(t)|

t ≤ |u0|+h

|u1|p+ Z t

1

h(s)g1 [u(s)

s ]r

g2(|u0(s)|r)dsi1/p ,

|u(t)|

t p

≤C+ 2p−1 Z t

1

h(s)g1

[u(s)

s ]r

g2(|u0(s)|r)ds,

(2.26)

where C = 2p−1(|u0|p+|u1|p)≥ (|u0|+|u1|)p. Denoting by z(t) the right-hand side of inequality (2.26) and using the assumptions of the Theorem 2.5, we have for t≥1

z(t)≤1 +C+ 2p−1 Z t

1

h(s)g1(zr/p)g2(zr/p)ds. (2.27) Applying Bihari’s inequality (see [5]) to (2.27), fort≥1, we obtain

z(t)≤G−1

G(1 +C) + 2p−1 Z t

1

h(s)ds

≤G−1(K), where

G(w) = Z w

1

ds g1(sr/p)g2(sr/p),

and G−1(w) is the inverse function for G(w). The function G−1(w) is defined for w∈(G(+0),∞), whereG(+0)<0, it is increasing, and

K=G(1 +C) + 2p−1 Z

1

h(s)ds <∞.

The rest of proof is similar that of Theorem 2.2 and thus is omitted.

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Example 4. Lett0= 1,p≥r >0, f(t, u, v) =η(t)t1−αe−thu

t p−r

ln 2 +u

t r

i34

·h

vp−rln(2 +vr)i14 ,

whereη(t) is a continuous function on h1,∞) withK= supt∈h1,∞)η(t)<∞. Let g1(u) =h

upr−1ln(2 +u)i3/4

, g2(v) =h

vpr−1ln(2 +v)i1/4

, h(t) =η(t)t1−αe−t.

Then

f(t, u, v) =h(t)g1

[u

t]r g2(vr) and

G(+∞) =p r

Z

1

τpr−1

g1(τ)g2(τ)dτ =p r

Z

1

dτ τln(2 +τ)

>p r

Z

1

(2 +τ) ln(2 +τ) = +∞.

Obviously|f(t, u, v)|can be estimated as in Theorem 2.5. Thus all assumptions of Theorem 2.5 are satisfied and this means that any global solution of the equation (1.1) possesses the property (L).

Theorem 2.6. Let t0>0. Suppose that the following conditions hold:

(i) there exist nonnegative continuous functionsh, g1, g2:R+→R+ such that

|f(t, u, v)| ≤h(t)g1

h|u(t)|

t ir

g2(|v|r) (ii) fors >0 the functionsg1(s), g2(s)are nondecreasing; and

g1(αu)≤ψ1(α)g1(u), g2(αu)≤ψ2(α)g2(u)

forα≥1, u≥0, where the functionsψ1(α), ψ2(α)are continuous forα≥1;

(iii) R

t0 h(s)ds=H <+∞.

Assume also that there exists a constant K≥1 such that K−11(K)ψ2(K)≤

Z

1

ds

g1(sr/p)g2(sr/p)= p r

Z

a

τpr−1

g1(τ)g2(τ), (2.28) where a = (t0)rp. Then any global solution u(t) of the equation (1.1) with initial datau(t0) =u0, u0(t0) =u1such that2p−1(|u0|p+|u1|p)≤Kpossesses the property (L).

Proof. Without loss of generality we assume thatt0= 1. With the same argument as in Theorem 2.2, fort≥1, we have

|u0(t)| ≤h

|u1|p+ Z t

1

h(s)g1

|u(s)|

s r

g2(|u0(s)|r)dsi1/p

,

|u(t)|

t ≤ |u0|+h

|u1|p+ Z t

1

h(s)g1

|u(s)|

s r

g2(|u0(s)|r)dsi1/p .

Applying the inequality (A+B)p≤2p−1(Ap+Bp),A, B≥0 we obtain |u(t)|

t p

≤2p−1(|u0|p+|u1|p) + 2p−1hZ t 1

g1

|u(s)|

s r

g2(|u0(s)|r)dsi

. (2.29)

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Denoting byz(t) the right-hand side of inequality (2.29), fort≥1, we obtain z(t)≤K+

Z t

1

H(s)g1(z(s)r/p)g2(z(s)r/p)ds, (2.30) whereK = 2p−1(|u0|p+|u1|p) andH(t) = 2p−1h(t). Assumption (ii) implies that the functions g1(u), g2(u) belong to the class H. Furthermore, it follows from [6, Lemma 1] that if g1(u) and g2(u) belong to the class H with the corresponding multiplier functions ψ1(α) and ψ2(α) respectively, then the product g1(u)g2(u) also belongs to Hand the corresponding multiplier function isψ1(α)ψ2(α). Thus, applying [8, Theorem 1] to (2.30), fort≥1, we have

z(t)≤KW−1

K−1ψ1(K)ψ2(K) Z t

1

H(s)ds

, (2.31)

where

W(u) = Z u

1

ds

g1(sr/p)g2(sr/p), (2.32) andW−1(u) is the inverse function forW(u). Evidently, inequality (2.31) holds for allt≥1 since by (2.28)

K−1ψ1(K)ψ2(K) Z t

1

H(s)ds∈Dom(W−1) (2.33) for all t ≥ 1. The rest of the proof is analogous to that of Theorem 2.2 and is

omitted.

Theorem 2.7. Let t0>0. Suppose that assumptions (i) and (iii) of Theorem 2.6 hold, while (ii) is replaced by

(ii’) for s > 0 the functions g1(s), g2(s) are continuous and nondecreasing, g1(0) =g2(0) = 0, and satisfy a Lipschitz condition

|g1(u+v)−g1(u)| ≤λ1v, |g2(u+v)−g2(u)| ≤λ2v, whereλ1, λ2 are positive constants.

Then any global solution u(t) of the equation (1.1) with initial data u(t0) = u0, u0(t0) =u1 such that |u0|p+|u1|p≤K possesses the property (L).

Proof. Without loss of generality we may assumet0= 1. Applying [8, Corollary 2]

to (2.30), we have fort≥1

z(t)≤K+g1(K)g2(K) Z t

1

H(s) exp λ1λ2

Z t

1

H(τ)dτ ds

≤K+ ¯Hg1(K)g2(K) exp (λ1λ2H¯)<+∞.

The proof of the above theorem can be completed with the same argument as in

Theorem 2.2.

Acknowledgements. The first author was supported by Grant No. 1/0098/08 from the Slovak Grant Agency VEGA-SAV-M. The second author was supported by Grant No. 201/08/0469 from Grant Agency of the Czech Republic.

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References

[1] M. Bartuˇsek, Singular solutions for the differential equation with p-Laplacian, Archivum Math. (Brno),41(2005) 123–128.

[2] M. Bartuˇsek,On singular solutions of a second order differential equations, Electronic Jour- nal of Qualitaive Theory of Differential Equations,8(2006), 1–13.

[3] M. Bartuˇsek and M. Medveˇd, Existence of global solutions for systems of second-order functional-differential equations withp-Laplacian, Electronic Jornal of Differential Equations, 2008(40) (2008), 1–8.

[4] M. Bartuˇsek and E. Pek´arkov´a,On existence of proper solutions of quasilinear second order differential equations, Electronic Journal of Qualitative Theory of Differential Equations,1 (2007), 1–14.

[5] I. Bihari,A generalization of a lemma of Bellman and its applications to uniqueness problems of differential equations, Acta Math. Acad. Sci. Hungar.,7(1956), 81–94.

[6] D. S. Cohen The asymptotic behavior of a class of nonlinear differntial equations, Proc.

Amer. Math. Soc.18(1967),607–609.

[7] A. Constantin,On the asymptotic behavior of second order nonlinear differential equations, Rend. Math. Appl.,13(7) (1993), 627–634.

[8] F. M. Dannan,Integral inequalities of Gronwall-Bellman-Bihari type and asymptotic behavior of certain second order nonlinear differential equations, J.Math. Anal.Appl., 108 (1985), 151–164.

[9] T. Kusano and W. F. Trench, Global existence of scond order differential equations with integrable coefficientsJ. London Math. Soc.31(1985), 478–486.

[10] T. Kusano and W. F. Trench,Existence of global solutions with prescribed asymptotic behav- ior for nonlnear ordinary differential equations, Mat. Pura Appl.142(1985), 381–392.

[11] M. Medveˇd and E. Pek´arkov´a,Existence of global solutions of systems of second order dif- ferential equations withp-Laplacian, Electronic Jornal of Differential Equations,2007(136) (2007), 1–9.

[12] I. Rachunkov´a, S. Stanˇek and M. Tvrd´y,Singularities and Laplacians in Boundary Value Problems for Nonlinear Ordinary Differential Equations, Handbook of Differential Equations.

Ordinary Differential Equations3606–723, Ed. by A. Canada, P. Dr´abek, A. Fonde, Elsevier 2006.

[13] Y. V. Rogovchenko,On asymptotics behavior of solutions for a class of second order nonlinear differential equations, Collect. Math.,49(1) (1998), 113–120.

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[15] J. Tong, The asymptotic behavior of a class of nonlinear differential equations of second order, Proc. Amer. Math. Soc.,84(1982), 235–236.

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Milan Medveˇd

Department of Mathematical Analysis and Numerical Mathematics, Faculty of Mathe- matics, Physics and Informatics, Comenius University, Ml´ynsk´a dolina, 842 48 Bratislava, Slovakia

E-mail address:[email protected]

Eva Pek´arkov´a

Department of Mathematics and Statistics, Faculty of Science, Masaryk University, Jan´ckovo n´am. 2a, CZ-602 00 Brno, Czech Republic

E-mail address:[email protected]

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