• Nenhum resultado encontrado

Oscillatory generalized Lucas sequences

N/A
N/A
Protected

Academic year: 2021

Share "Oscillatory generalized Lucas sequences"

Copied!
16
0
0

Texto

(1)

doi:10.1155/2010/596350

Research Article

Oscillatory Nonautonomous Lucas Sequences

Jos ´e M. Ferreira

1

and Sandra Pinelas

2

1Department of Mathematics, Instituto Superior T´ecnico, Avenue Rovisco Pais, 1049-001 Lisboa, Portugal 2Department of Mathematics, Universidade dos Ac¸ores, R. M˜ae de Deus, 9500-321 Ponta Delgada, Portugal

Correspondence should be addressed to Sandra Pinelas,spinelas@uac.pt

Received 18 September 2009; Accepted 3 December 2009 Academic Editor: Elena Braverman

Copyrightq 2010 J. M. Ferreira and S. Pinelas. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

The oscillatory behavior of the solutions of the second-order linear nonautonomous equation

xn  1  anxn − bnxn − 1, n ∈ N0, where a, b : N0 → R, is studied. Under the assumption that the sequencebn dominates somehow an, the amplitude of the oscillations and the asymptotic behavior of its solutions are also analized.

1. Introduction

The aim of this note is to study the oscillatory behavior of the equation

xn  1  anxn − bnxn − 1, n ∈ N0, 1.1

where a, b : N0 → R. Equation 1.1 is the nonautonomous case of the so-called Lucas

sequences, which are obtained through the recursive law:

xn  1  axn − bxn − 1, n ∈ N0, 1.2

which corresponds to have in 1.1 both sequences an and bn constant and equal,

respectively, to real numbers a and b. Lucas sequences are well known in number theory

as an extension of the Fibonacci sequencesee 1, Chapter 2, Section IV.

Several particular cases of1.1 are considered in literature. This is the case of equation

see 2, Chapter 6

(2)

withqn being arbitrary and pn being positive, corresponding to have in 1.1

an  qnpn, bn  pn − 1pn . 1.4

The equationsee 3,4 and references therein

Δ2xn − 1  Pnxn  0, n ∈ N0 1.5

is also a particular case of1.1. In fact, 1.5 can be written as

xn  1  2 − Pnxn − xn − 1, n ∈ N0, 1.6

corresponding to have in 1.1, an  2 − Pn and bn constant and equal to 1. Other

particular cases of1.1 will be referred along the text.

As usual, we will say that a solution xn of 1.1 is nonoscillatory if it is either

eventually positive or eventually negative. Otherwise xn is called oscillatory. When all

solutions of1.1 are oscillatory, 1.1 is said oscillatory.

It is well known that1.2 is oscillatory if and only if the polynomial z2− az  b has no

positive real roots. This is equivalent to have one of the following two cases:

i a ≤ 0, b ≥ 0; ii a > 0, b > a2

4 . 1.7

In order to obtain1.1 oscillatory, this specific case seems to justify that the sequence bn

be assumed positive. However, forbn > 0 for every n, notice that if one has either an ≤ 0

eventually oran oscillatory, then xn cannot be neither eventually positive nor eventually

negative. That is, in such circumstances the equation is oscillatory. So hereafter we will

assume thatan and bn are both positive sequences.

Through a direct manipulation of the terms of the solutions of1.1, we show in the

following sections a few results which seem, as far as we know, uncommon in literature. We

state that ifbn dominates somehow the sequence an, then all solutions of the equation

exhibit a specific oscillatory and asymptotic behavior. Oscillations through the existence of periodic solutions will be studied in a sequel, but they cannot then happen under a similar

relationship betweenan and bn.

2. Oscillatory Behavior

The oscillatory behavior of1.1 can be stated through the application of some results already

existent in literature. This is the case of the following theorem based upon a result in5.

Theorem 2.1. If

bn

an − 1an>

1

(3)

holds eventually and lim sup n → ∞ bn an − 1an > 1 4, 2.2 then1.1 is oscillatory.

Proof. By making the change of variable

yn  2n−1nxn

k1ak

, 2.3

one can see that1.1 is equivalent to

Δ2yn − 1   1− 4bn an − 1an  yn − 1, n ∈ N0, 2.4

where byΔ we mean the usual difference operator.

Therefore applying5, Theorem 1.3.1, one can conclude under 2.1 and 2.2 that

every solution of2.4 is oscillatory. Then, as all terms of the sequence an are positive, also

xn is oscillatory.

Remark 2.2. In6 the equation

xt p

j1

αjtxt − j, 2.5

where, forj  1, . . . , p, αjt are real continuous functions on 0, ∞, is studied. Through 6,

Theorem 10, this equation is oscillatory if

βj αjt  γj 2.6 forj  1, . . . , p, and 1 p  j1 γjexp−λj 2.7

has no real roots. Since 1.1 is the discrete case of 2.5 with p  2, if an and bn are

both bounded sequences, one can apply6, Theorem 10. As a matter of fact, if an ≤ α

and−bn ≤ −β, for every n, then through 1.7 one can conclude that 1.1 is oscillatory if

β > α2/4. This condition implies 2.1 and 2.2.

Remark 2.3. In literature is largely considered the equation

(4)

see 7 and references therein. For τ  1 one obtains the case of 1.1 where an is constant

and equal to 1. In8, Theorems 7.5.2 and 7.5.3 is stated that 1.1 in such case is oscillatory

provided that one of the following two conditions is satisfied: lim inf n → ∞ bn > 1 4, lim sup n → ∞ bn  bn  1 > 1. 2.9

Both these conditions imply the correspondent conditions2.1 and 2.2.

Remark 2.4. In2, Theorem 6.5.3 is stated that the particular case of 1.1 given by 1.3, with

qn also positive, is oscilattory if there exists ε > 0 such that

qnqn  1 ≤ 4 − p2n 2.10

holds eventually. On the other hand, one easily sees that 2.1 and 2.2 are, respectively,

equivalent to have eventually

qn − 1qn < 4p2n − 1, lim sup n → ∞ p2n − 1 qn − 1qn > 1 4. 2.11

Notice that2.10 implies 2.11.

Remark 2.5. ThroughTheorem 2.1one can state that1.5 is oscillatory, if Pn < 2, for every

n, Pn − 1Pn 2 < Pn − 1  Pn, 2.12 eventually, and lim inf n → ∞  Pn − 1Pn 2 − Pn − 1 − Pn  < 0. 2.13

These conditions, with respect to those obtained in3,4, seem to be of different kind.

3. Oscillations

The results of the preceding section state that all solutions of1.1 oscillate. In this section we

will characterize the oscillations of such solutions.

We first notice that if two of three consecutive termsxk − 1, xk, and xk  1 are

zero, then necessarilyxn  0 for every n > k  1. This means that if the sequence xn has

two consecutive or alternate zeros, then it is eventually null. In the following we will exclude this trivial situation.

(5)

Lemma 3.1. a For every n one has

i xn > 0 ∧ xn  2 > 0 ⇒ xn  1 > 0, ii xn < 0 ∧ xn  2 < 0 ⇒ xn  1 < 0. b If there exists a positive integer N such that

bn > anan − 1 for every n ≥ N, 3.1

then

iii xn > 0 ∧ xn  2 > 0 ⇒ xn  3 < 0, iv xn < 0 ∧ xn  3 < 0 ⇒ xn  2 > 0

for everyn ≥ N.

Proof. a From 1.1 one obtains

xn  2  an  1xn  1 − bn  1xn. 3.2 So xn > 0, xn  2 > 0 3.3 impliesxn  1 > 0, and if xn < 0, xn  2 < 0, 3.4 thenxn  1 < 0.

b Notice that xn can be written as

xn  an  1bn  1xn  1 − bn  11 xn  2. 3.5 Therefore by recurrence xn  an  1 bn  1  an  2 bn  2xn  2 − 1 bn  2xn  3  − 1 bn  1xn  2, 3.6

and through a rearrangement

xn  bn  11  an  1an  2 bn  2 − 1  xn  2 −bn  1bn  2an  1 xn  3. 3.7

(6)

Thus ifxn > 0, one has xn  3 <  an  2 −bn  2an  1  xn  2, 3.8

and lettingn ≥ N and xn  2 > 0 one concludes that xn  3 < 0, which shows iii.

Analogously,xn < 0 and n ≥ N imply

1 bn  1  1−an  1an  2 bn  2  xn  2 > − an  1 bn  1bn  2xn  3, 3.9

and consequently one hasxn  2 > 0 if xn  3 < 0.

We notice that assumption3.1 implies obviously 2.1 and 2.2, which means that

under3.1, equation 1.1 is oscillatory. However, under 3.1 one can further state some

interesting characteristics regarding the oscillations of the solutions of1.1.

For that purpose, letk ∈ N. Denote by mk the smallest number of consecutive terms

ofxn, which, for n > k, are positive; by Mk we mean the largest number of consecutive

terms ofxn, which, for n > k, are positive. Analogously, let mkandMk−be, respectively, the

smallest and largest numbers of consecutive terms ofxn, which, for n > k, are negative.

Theorem 3.2. Under 3.1, for every k > N one has m

k, mk ≥ 2 and Mk, Mk ≤ 3.

Proof. Assuming that there exists an > k such that

xn > 0, xn  1 < 0, xn  2 > 0, 3.10

one contradictsi ofLemma 3.1. In the same way,

xn < 0, xn  1 > 0, xn  2 < 0 3.11

is in contradiction withLemma 3.1ii.

Moreover if for somen > k one has xn  0, then both xn  1 and xn  2 are

nonzero real numbers with equal sign and contrary to the sign ofxn − 1 and xn − 2.

Thusmk, mk≥ 2.

Suppose now that

xn > 0, xn  1 > 0, xn  2 > 0, xn  3 > 0. 3.12

(7)

Analogously if

xn < 0, xn  1 < 0, xn  2 < 0, xn  3 < 0, 3.13

we contradictLemma 3.1iv.

HenceMk, Mk≤ 3.

From this theorem one can conclude immediately the following statement.

Theorem 3.3. Under 3.1 all solutions of 1.1 are oscillatory with at least two and no more than three consecutive terms of the same sign.

Example 3.4. The particular case of1.1, where bn is constant and equal to b > 0, gives the

equation

xn  1  anxn − bxn − 1, n ∈ N0. 3.14

Notice that byTheorem 2.1this equation is oscillatory ifanan − 1 < 4b eventually and

lim infn → ∞anan − 1 < 4b. But if anan − 1 < b eventually, then 3.14 is oscillatory

having at least two and no more than three consecutive terms of the same sign. This is the

case whenb ≥ 4 and

an 

n  1 n − 1

n , 3.15

sincean → 2, as n → ∞, in manner that an < 2, for every n.

Example 3.5. Let now1.1 with an constant and equal to a > 0:

xn  1  axn − bnxn − 1, n ∈ N0. 3.16

Ifbn > a2 eventually, then all solutions of3.16 oscillate with at least two and no more

than three consecutive terms of the same sign. This is the case whenbn  n and a is any

positive real number. However, the equation is oscillatory more generally ifbn > a2/4 and

lim supn → ∞bn > a2/4.

Example 3.6. All solutions of1.5 have this same type of oscillation, whenever Pn < 2 for

everyn and eventually

2 − Pn − 12 − Pn < 1. 3.17

This occurs, for example, if 1< Pn < 2, for every n.

These examples show that the gain ofTheorem 3.3is not in concluding the oscillatory

(8)

4. Oscillation Amplitude

In this section we complement the oscillatory properties of xn with the study of the

amplitude with respect to the real line of its oscillations.

By a semicycle ofxn we will mean any maximal set of nonzero consecutive terms

with the same sign. If

S  {xn, . . . , xn  k} 4.1

is a semicycle ofxn, to the value

|S|  max{|xn|, . . . , |xn  k|} 4.2

we call the amplitude ofS.

Under 3.1 we have shown that xn is constituted by a sequence of semicycles

alternately composed by positive and negative terms, each one having at least two and no

more than three elements. Between semicycles is possible that might exist a null term ofxn,

but byLemma 3.1iii, a semicycle of three elements cannot precede a zero of xn.

If one denotes that sequence of semicycles is bySkk  1, 2, . . . in the following, we

will analize the properties of the sequence|Sk| of its amplitudes. For that purpose we will

assume that for some integer positiveN, one has

an  1an  1 < bn  1 4.3

for everyn > N. This condition implies obviously 3.1.

Lemma 4.1. Assume that 4.3 holds and that for every n > N

bn > an. 4.4

If

xn − 1 > 0, xn > 0, xn  1 > 0 4.5

forn > N, then xn  2 < 0 and xn  3 < 0 such that

max{|xn  2|, |xn  3|} > max{xn − 1, xn, xn  1}. 4.6

Proof. Asxn  1 > 0 we have

anxn − bnxn − 1 > 0, 4.7

and so, by4.4,

(9)

Now we will prove that−xn  2 > xn and −xn  3 > xn  1. In fact, we have xn  2  an  1xn  1 − bn  1xn

 an  1anxn − bnxn − 1 − bn  1xn  an  1an − bn  1xn − an  1bnxn − 1 < an  1an − bn  1xn

4.9

and by4.3 we obtain

xn  2 < −xn, 4.10

for everyn > N.

In the same way one can conclude that

xn  3 < an  2an  1 − bn  2xn  1 < −xn  1. 4.11

This proves the lemma.

Lemma 4.2. Assume that 4.3 holds and that for every n > N

an  1bn > 1. 4.12

If

xn − 1 > 0, xn > 0, xn  1 < 0, xn  2 < 0 4.13

forn > N, then

max{|xn  1|, |xn  2|} > max{xn − 1, xn}. 4.14

Proof. Noticing that

xn  2  an  1anxn − bnxn − 1 − bn  1xn

 an  1an − bn  1xn − an  1bnxn − 1, 4.15

by4.3 one has

xn  2 < an  1an − bn  1xn < −xn,

xn  2 < −an  1bnxn − 1 < −xn − 1, 4.16

(10)

Lemma 4.3. Assume that 4.3, 4.4, and 4.12 hold. If

xn − 1 > 0, xn > 0, xn  1  0, xn  2 < 0, xn  3 < 0 4.17

forn > N, then

max{|xn  2|, |xn  3|} > max{xn − 1, xn}. 4.18

Proof. First take into account thatxn  1  0 implies

anxn  bnxn − 1 ⇐⇒ xn  bn

anxn − 1 > xn − 1. 4.19

Notice now that

xn  2  −bn  1xn < −xn 4.20

since4.3 implies bn > 1 for every n > N. On the other hand

xn  3  an  2xn  2  −an  2bn  1xn < −xn.

4.21

This achieves the proof.

Remark 4.4. Observe thatun  −xn is also a solution of 1.1 which of course has the same

oscillatory characteristics as xn. This fact enables to conclude similar lemmas by simple

change of sign.

Theorem 4.5. Assuming that 4.3, 4.4, and 4.12 hold, then |Sk| is eventually increasing.

Proof. LetSkandSk1be two consecutive semicycles. Several cases can be performed.

1 Assume that

Sk {xn − 1 > 0, xn > 0, xn  1 > 0},

Sk1 {xn  2 < 0, xn  3 < 0}. 4.22

Then byLemma 4.1one has|Sk1| > |Sk|.

ByRemark 4.4the same holds if

Sk {xn − 1 < 0, xn < 0, xn  1 < 0},

(11)

2 If

Sk {xn − 1 > 0, xn > 0, xn  1 > 0},

Sk1 {xn  2 < 0, xn  3 < 0, xn  4 < 0}, 4.24

then still by4.6 ofLemma 4.1one obtains

|Sk1| ≥ max{|xn  3|, |xn  2|} > |Sk|. 4.25

AgainRemark 4.4provides the same conclusion if

Sk {xn − 1 < 0, xn < 0, xn  1 < 0}, Sk1 {xn  2 > 0, xn  3 > 0, xn  4 > 0}. 4.26 3 Let now Sk {xn − 1 > 0, xn > 0}, Sk1 {xn  1 < 0, xn  2 < 0}. 4.27

The inequality4.14 ofLemma 4.2expresses directly that|Sk1| > |Sk|. The use ofRemark 4.4

enables to conclude that the same is verified when

Sk {xn − 1 < 0, xn < 0}, Sk1 {xn  1 > 0, xn  2 > 0}. 4.28 4 If Sk {xn − 1 > 0, xn > 0}, Sk1 {xn  1 < 0, xn  2 < 0, xn  3 < 0}, 4.29

then by4.14 one can obtain

|Sk1| ≥ max{|xn  1|, |xn  2|} > |Sk|. 4.30

ByRemark 4.4one obtains the same for

Sk {xn − 1 < 0, xn < 0},

(12)

5 In the case where

Sk {xn − 1 > 0, xn > 0},

Sk1 {xn  2 < 0, xn  3 < 0}

4.32

withxn  1  0, one obtains |Sk1| > |Sk| directly from the inequality 4.18. The case where

Sk {xn − 1 < 0, xn < 0},

Sk1 {xn  2 > 0, xn  3 > 0}

4.33

can be obtained by the use ofRemark 4.4.

6 Finally when xn  1  0 and

Sk {xn − 1 > 0, xn > 0},

Sk1 {xn  2 < 0, xn  3 < 0, xn  4 < 0},

4.34

still through the inequality4.18 ofLemma 4.3we conclude that

|Sk1| ≥ max{|xn  3|, |xn  2|} > |Sk|. 4.35

AgainRemark 4.4enables us to conclude the same for the case

Sk {xn − 1 < 0, xn < 0},

Sk1 {xn  2 > 0, xn  3 > 0, xn  4 > 0}.

4.36

This completes the proof of the theorem.

ThroughTheorem 4.5one can state the following asymptotic behavior ofxn.

Theorem 4.6. Assume 4.3 and 4.12. If lim sup

n → ∞

1 an

bn < 1, 4.37

then

(13)

Proof. Notice first that since an bn < 1 an bn , 4.39 equation4.37 implies 4.4.

Assuming thatxn is bounded, let

K  sup{|xn| : n ∈ N}. 4.40 From1.1 we have bn|xn − 1| ≤ |xn  1|  an|xn|, 4.41 and so |xn − 1| ≤1 an bn K 4.42 for everyn.

On the other hand, taking arbitrarily 0< δ < 1, there exists an integer N > 0 such that,

for everyn > N,

1 an

bn < δ. 4.43

Thus by consequence

|xn − 1| ≤ δK < K 4.44

for everyn > N. This means that K  max{|xn| : n  1, . . . , N − 1} which is in contradiction

withTheorem 4.5.

Thusxn is not a bounded sequence and again byTheorem 4.5one can conclude the

existence of two increasing sequencesn, nk∈ N such that

xn −→ ∞, xnk −→ −∞ 4.45

ask, → ∞, which achieves the proof.

Example 4.7. Regarding1.2, if a > 0 and

b > max  a  1, a2 1,1 a , 4.46

(14)

then all its solutions exhibit the properties stated in Theorems3.3and4.6. For2.8 the same holds whenever

lim inf

n → ∞ bn > 2. 4.47

With respect to1.3 the same behavior is verified for all its solutions provided that one has,

eventually, qnqn  1  pnpn  1 < pn − 1pn  1, pnpn  1 < qn  1pn − 1, lim sup n → ∞ pnqn pn − 1 < 1. 4.48

Example 4.8. Let us consider the Hermite polynomial equation

Hn1x  xHnx − nHn−1x 4.49

with

H−1x  1, H0x  x. 4.50

For every x > 0, all the assumptions 4.3, 4.12, and 4.37 are satisfied. Then we can

complement the oscillatory result stated in 5, Theorem 1.3.5, by saying that Hnx is an

oscillatory sequence with at least two and no more than three consecutive terms of the same

sign, admitting one subsequence going to ∞ and another tending to −∞. In a different

framework the same situation can be seen for other kinds of orthogonal polynomials in

9,10.

Remark 4.9. Finally we observe that for having the asymptotic behavior stated inTheorem 4.6,

we are implicitly asking that the sequencebn dominates in some manner an. That kind of

domination is not verified in1.5. As a matter of fact, the required assumption that Pn < 2,

for everyn, does not allow that the corresponding conditions 4.3 and 4.37 be verified.

Acknowledgment

This research was partially supported by FCT.

References

1 P. Ribenboim, The book of Prime Number Records, Springer, New York, NY, USA, 2nd edition, 1989. 2 R. P. Agarwal, Difference Equations and Inequalities, vol. 155 of Monographs and Textbooks in Pure and

Applied Mathematics, Marcel Dekker, New York, NY, USA, 1992.

3 Y. G. Sun, “Oscillation and non-oscillation for second-order linear difference equations,” Applied

(15)

4 Y. Zhou, B. G. Zhang, and C. F. Li, “Remarks on oscillation and nonoscillation for second-order linear difference equations,” Applied Mathematics Letters, vol. 21, no. 6, pp. 578–580, 2008.

5 R. P. Agarwal, S. Grace, and D. O’Regan, Oscillation Theory for Difference and Functional Differential

Equations, Kluwer Academic Publishers, Dordrecht, The Netherlands, 2000.

6 J. M. Ferreira and A. M. Pedro, “Oscillations of delay difference systems,” Journal of Mathematical

Analysis and Applications, vol. 221, no. 1, pp. 364–383, 1998.

7 G. E. Chatzarakis and I. P. Stavroulakis, “Oscillations of first order linear delay difference equations,”

The Australian Journal of Mathematical Analysis and Applications, vol. 3, no. 1, article 14, pp. 1–11, 2006.

8 I. Gy¨ori and G. Ladas, Oscillation Theory of Delay Differential Equations, Oxford Mathematical Monographs, Oxford University Press, New York, NY, USA, 1991.

9 J. M. Ferreira, S. Pinelas, and A. Ruffing, “Nonautonomous oscillators and coefficient evaluation for orthogonal function systems,” Journal of Difference Equations and Applications, vol. 15, no. 11-12, pp. 1117–1133, 2009.

10 J. M. Ferreira, S. Pinelas, and A. Ruffing, “Oscillatory difference equations and moment problems,” to appear in International Journal of Difference Equations.

(16)

Submit your manuscripts at

http://www.hindawi.com

Hindawi Publishing Corporation

http://www.hindawi.com Volume 2014

Mathematics

Journal of

Hindawi Publishing Corporation

http://www.hindawi.com Volume 2014

Mathematical Problems in Engineering

Hindawi Publishing Corporation http://www.hindawi.com

Differential Equations

International Journal of Volume 2014

Hindawi Publishing Corporation

http://www.hindawi.com Volume 2014 Mathematical PhysicsAdvances in

Complex Analysis

Journal of

Hindawi Publishing Corporation

http://www.hindawi.com Volume 2014

Optimization

Journal of

Hindawi Publishing Corporation

http://www.hindawi.com Volume 2014

Combinatorics

Hindawi Publishing Corporation

http://www.hindawi.com Volume 2014

International Journal of

Journal of

Hindawi Publishing Corporation

http://www.hindawi.com Volume 2014

Function Spaces

Abstract and Applied Analysis

Hindawi Publishing Corporation

http://www.hindawi.com Volume 2014 International Journal of Mathematics and Mathematical Sciences

Hindawi Publishing Corporation http://www.hindawi.com Volume 2014

The Scientific

World Journal

Hindawi Publishing Corporation

http://www.hindawi.com Volume 2014

Discrete Dynamics in Nature and Society Hindawi Publishing Corporation

http://www.hindawi.com Volume 2014

Discrete Mathematics

Journal of

Hindawi Publishing Corporation

http://www.hindawi.com Volume 2014 Hindawi Publishing Corporationhttp://www.hindawi.com Volume 2014

Stochastic Analysis

International Journal of

Referências

Documentos relacionados

do 8oacica (APIB) Dezenbro/87 Mista e de Colonizacao do Caiurupia (COOPERCAM) Dezeibro/87. dos Colonos dos Nudeos VI, IX e XI Dezeibro/87

O presente estudo visou mapear o impacto ambiental no vale do submédio do Rio São Francisco, causado pelos resíduos líquidos provenientes do esgoto e águas servidas de dois

Os indicadores bibliométricos recentemente divulgados pela Thomson Reuters Científica indicaram que a Revista Ciência e Tecnologia de Alimentos, indexada há quatro anos, está

na temática pelo documetário, a partir da narração dos temores de viver numa grande       cidade performatizada por atores, mas cujas falas se baseiam em relatos apurados nas    

Also, the project described in the paper &#34;Recognizing clothes patterns and colors for blind people using neural network&#34; allows to classify the type of pattern of

1987, que dividem o Grupo Tubarão em Subgrupo Itararé e Formação Tatuí, e que subdividem o Subgrupo Itararé em: Formação Itu, para a seqüência de depósitos glaciais e de

A Matriz de Insumo-Produto (MIP) apresenta, em determinado período, o fluxo de bens e serviços realizado entre diferentes ramos que compõe a economia de uma cidade,

Assim, este estudo evidenciou que não há uma correlação significativa entre o estresse oxidativo celular, as reações adversas apresentadas durante o