This paper is concerned the determination of trajectories for the three-dimensional Navier-Stokes equations with nonlinear damping subject to periodic boundary condition. By using the energy estimate of Galerkin approximated equation, the finite number of determining modes and asymptotic determined functionals have been shown via the Grashof numbers for the non-autonomous and autonomous damped Navier-Stokes fluid flow respectively.
Citation: Wei Shi, Xinguang Yang, Xingjie Yan. Determination of the 3D Navier-Stokes equations with damping[J]. Electronic Research Archive, 2022, 30(10): 3872-3886. doi: 10.3934/era.2022197
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This paper is concerned the determination of trajectories for the three-dimensional Navier-Stokes equations with nonlinear damping subject to periodic boundary condition. By using the energy estimate of Galerkin approximated equation, the finite number of determining modes and asymptotic determined functionals have been shown via the Grashof numbers for the non-autonomous and autonomous damped Navier-Stokes fluid flow respectively.
Fibonacci polynomials and Lucas polynomials are important in various fields such as number theory, probability theory, numerical analysis, and physics. In addition, many well-known polynomials, such as Pell polynomials, Pell Lucas polynomials, Tribonacci polynomials, etc., are generalizations of Fibonacci polynomials and Lucas polynomials. In this paper, we extend the linear recursive polynomials to nonlinearity, that is, we discuss some basic properties of the bi-periodic Fibonacci and Lucas polynomials.
The bi-periodic Fibonacci {fn(t)} and Lucas {ln(t)} polynomials are defined recursively by
f0(t)=0,f1(t)=1,fn(t)={ayfn−1(t)+fn−2(t)n≡0(mod2),byfn−1(t)+fn−2(t)n≡1(mod2),n≥2, |
and
l0(t)=2,l1(t)=at,ln(t)={byln−1(t)+ln−2(t)n≡0(mod2),ayln−1(t)+ln−2(t)n≡1(mod2),n≥2, |
where a and b are nonzero real numbers. For t=1, the bi-periodic Fibonacci and Lucas polynomials are, respectively, well-known bi-periodic Fibonacci {fn} and Lucas {ln} sequences. We let
ς(n)={0n≡0(mod2),1n≡1(mod2),n≥2. |
In [1], the scholars give the Binet formulas of the bi-periodic Fibonacci and Lucas polynomials as follows:
fn(t)=aς(n+1)(ab)⌊n2⌋(σn(t)−τn(t)σ(t)−τ(t)), | (1.1) |
and
ln(t)=aς(n)(ab)⌊n+12⌋(σn(t)+τn(t)), | (1.2) |
where n≥0, σ(t), and τ(t) are zeros of λ2−abtλ−ab. This is σ(t)=abt+√a2b2t2+4ab2 and τ(t)=abt−√a2b2t2+4ab2. We note the following algebraic properties of σ(t) and τ(t):
σ(t)+τ(t)=abt,σ(t)−τ(t)=√a2b2t2+4ab,σ(t)τ(t)=−ab. |
Many scholars studied the properties of bi-periodic Fibonacci and Lucas polynomials; see [2,3,4,5,6]. In addition, many scholars studied the power sums problem of second-order linear recurrences and its divisible properties; see [7,8,9,10].
Taking a=b=1 and t=1, we obtain the Fibonacci {Fn} or Lucas {Ln} sequence. Melham [11] proposed the following conjectures:
Conjecture 1. Let m≥1 be an integer, then the sum
L1L3L5⋯L2m+1n∑k=1F2m+12k |
can be represented as (F2n+1−1)2R2m−1(F2n+1), including R2m−1(t) as a polynomial with integer coefficients of degree 2m−1.
Conjecture 2. Let m≥1 be an integer, then the sum
L1L3L5⋯L2m+1n∑k=1L2m+12k |
can be represented as (L2n+1−1)Q2m(L2n+1), where Q2m(t) is a polynomial with integer coefficients of degree 2m.
In [12], the authors completely solved the Conjecture 2 and discussed the Conjecture 1. Using the definition and properties of bi-periodic Fibonacci and Lucas polynomials, the power sums problem and their divisible properties are studied in this paper. The results are as follows:
Theorem 1. We get the identities
n∑k=1f2m+12k(t)=a2m+1b(a2b2t2+4ab)mm∑j=0(−1)m−j(2m+1m−j)(f(2n+1)(2j+1)(t)−f2j+1(t)l2j+1(t)), | (1.3) |
n∑k=1f2m+12k+1(t)=(ab)m(a2b2t2+4ab)mm∑j=0(2m+1m−j)(f(2n+2)(2j+1)(t)−f2(2j+1)(t)l2j+1(t)), | (1.4) |
n∑k=1l2m+12k(t)=m∑j=0(2m+1m−j)(l(2n+1)(2j+1)(t)−l2j+1(t)l2j+1(t)), | (1.5) |
n∑k=1l2m+12k+1(t)=am+1bm+1m∑j=0(−1)m−j(2m+1m−j)(l(2n+2)(2j+1)(t)−l2(2j+1)(t)l2j+1(t)), | (1.6) |
where n and m are positive integers.
Theorem 2. We get the identities
n∑k=1f2m2k(t)=a2m(a2b2t2+4ab)mm∑j=0(−1)m−j(2mm−j)f2j(2n+1)(t)f2j(t)−a2m(a2b2t2+4ab)m(2mm)(−1)m(n+12), | (1.7) |
n∑k=1f2m2k+1(t)=(ab)m(a2b2t2+4ab)mm∑j=0(2mm−j)(f2j(2n+2)(t)−f4j(t)f2j(t))−(ab)m(a2b2t2+4ab)m(2mm)n, | (1.8) |
n∑k=1l2m2k(t)=m∑j=0(2mm−j)f2j(2n+1)(t)l2j+1(t)−22m−1−(2mm)(n+12), | (1.9) |
n∑k=1l2m2k+1(t)=ambmm∑j=0(−1)m−j(2mm−j)(f2j(2n+2)(t)−f4j(t)f2j(t))−ambm(2mm)(−1)mn, | (1.10) |
where n and m are positive integers.
As for application of Theorem 1, we get the following:
Corollary 1. We get the congruences:
bl1(t)l3(t)⋯l2m+1(t)n∑k=1f2m+12k(t)≡0(modf2n+1(t)−1), | (1.11) |
and
al1(t)l3(t)⋯l2m+1(t)n∑k=1l2m+12k(t)≡0(modl2n+1(t)−at), | (1.12) |
where n and m are positive integers.
Taking t=1 in Corollary 1, we have the following conclusions for bi-periodic Fibonacci {fn} and Lucas {ln} sequences.
Corollary 2. We get the congruences:
bl1l3⋯l2m+1n∑k=1f2m+12k≡0(modf2n+1−1), | (1.13) |
and
al1l3⋯l2m+1n∑k=1l2m+12k≡0(modl2n+1−a), | (1.14) |
where n and m are nonzero real numbers.
Taking a=b=1 and t=1 in Corollary 1, we have the following conclusions for bi-periodic Fibonacci {Fn} and Lucas {Ln} sequences.
Corollary 3. We get the congruences:
L1L3⋯L2m+1n∑k=1F2m+12k≡0(modF2n+1−1), | (1.15) |
and
L1L3⋯L2m+1n∑k=1L2m+12k≡0(modL2n+1−1), | (1.16) |
where n and m are nonzero real numbers.
To begin, we will give several lemmas that are necessary in proving theorems.
Lemma 1. We get the congruence
f(2n+1)(2j+1)(t)−f2j+1(t)≡0(modf2n+1(t)−1), |
where n and m are nonzero real numbers.
Proof. We prove it by complete induction for j≥0. This clearly holds when j=0. If j=1, we note that abf3(2n+1)(t)=(a2b2t2+4ab)f32n+1(t)−3abf2n+1(t) and we obtain
f3(2n+1)(t)−f3(t)=(abt2+4)f32n+1(t)−3f2n+1(t)−(abt2+4)f31(t)+3f1(t)=(abt2+4)(f2n+1(t)−f1(t))(f22n+1(t)+f2n+1(t)f1(t)+f21(t))−3(f2n+1(t)−f1(t))=(abt2+4)(f2n+1(t)−1)(f22n+1(t)+f2n+1(t)f1(t)+f21(t))−3(f2n+1(t)−1)≡0(modf2n+1(t)−1). |
This is obviously true when j=1. Assuming that Lemma 1 holds if j=1,2,…,k, that is,
f(2n+1)(2j+1)(t)−f2j+1(t)≡0(modf2n+1(t)−1). |
If j=k+1≥2, we have
l2(2n+1)(t)f(2n+1)(2j+1)(t)=f(2n+1)(2j+3)(t)+abf(2n+1)(2j−1)(t), |
and
abl2(2n+1)(t)=(a2b2t2+4ab)f22n+1(t)−2ab≡(a2b2t2+4ab)f21(t)−2ab(modf2n+1(t)−1). |
We have
f(2n+1)(2k+3)(t)−f2k+3(t)=l2(2n+1)(t)f(2n+1)(2k+1)(t)−abf(2n+1)(2k−1)(t)−l2(t)f2k+1(t)+abf2k−1(t)≡((abt2+4)f21(t)−2)f(2n+1)(2k+1)(t)−abf(2n+1)(2k−1)(t)−((abt2+4)f21(t)−2)f2k+1(t)+abf2k−1(t)≡((abt2+4)f21(t)−2)(f(2n+1)(2k+1)(t)−f2k+1(t))−ab(f(2n+1)(2k−1)(t)−f2k−1(t))≡0(modf2n+1(t)−1). |
This completely proves Lemma 1.
Lemma 2. We get the congruence
al(2n+1)(2j+1)(t)−al2j+1(t)≡0(modl2n+1(t)−at), |
where n and m are nonzero real numbers.
Proof. We prove it by complete induction for j≥0. This clearly holds when j=0. If j=1, we note that al3(2n+1)(t)=bl32n+1(t)+3al2n+1(t) and we obtain
al3(2n+1)(t)−al3(t)=bl32n+1(t)+3al2n+1(t)−bl31(t)−3al1(t)=(l2n+1(t)−l1(t))(bl22n+1(t)+bl2n+1(t)l1(t)+bl21(t))−3a(l2n+1(t)−l1(t))=(l2n+1(t)−at)(bl22n+1(t)+bayl2n+1(t)+ba2t2)−3a(l2n+1(t)−at)≡0(modl2n+1(t)−at). |
This is obviously true when j=1. Assuming that Lemma 2 holds if j=1,2,…,k, that is,
al(2n+1)(2j+1)(t)−al2j+1(t)≡0(modl2n+1(t)−at). |
If j=k+1≥2, we have
l2(2n+1)(t)l(2n+1)(2j+1)(t)=l(2n+1)(2j+3)(t)+l(2n+1)(2j−1)(t), |
and
al2(2n+1)(t)=bl22n+1(t)+2a≡bl21(t)+2a(modl2n+1(t)−at). |
We have
al(2n+1)(2k+3)(t)−al(2k+3)(t)=a(l2(2n+1)(t)l(2n+1)(2k+1)(t)−l(2n+1)(2k−1)(t))−a(l2(t)l2k+1(t)−l2k−1(t))≡(bl21(t)+2a)l(2n+1)(2k+1)(t)−al(2n+1)(2k−1)(t)−(bl21(t)+2a)l2k+1(t)+al2k−1(t)≡(abt2+2)(al(2n+1)(2k+1)(t)−al2k+1(t))−(al(2n+1)(2k−1)(t)−al2k−1(t))≡0(modl2n+1(t)−at). |
This completely proves Lemma 2.
Proof of Theorem 1. We only prove (1.3), and the proofs for other identities are similar.
n∑k=1f2m+12k(t)=n∑k=1(aς(2k+1)(ab)⌊2k2⌋⋅(σ2k(t)−τ2k(t)σ(t)−τ(t)))2m+1=a2m+1(σ(t)−τ(t))2m+1n∑k=1(σ2k(t)−τ2k(t))2m+1(ab)(2m+1)k=a2m+1(σ(t)−τ(t))2m+1n∑k=12m+1∑j=0(−1)j(2m+1j)σ2k(2m+1−j)(t)τ2kj(t)(ab)(2m+1)k=a2m+1(σ(t)−τ(t))2m+12m+1∑j=0(−1)j(2m+1j)(1−σ2n(2m+1−2j)(t)(ab)(2m+1−2j)n(ab)2m+1−2jσ2(2m+1−2j)(t)−1)=a2m+1(σ(t)−τ(t))2m+1m∑j=0(−1)j(2m+1j)(1−σ2n(2m+1−2j)(t)(ab)(2m+1−2j)n(ab)2m+1−2jσ2(2m+1−2j)(t)−1−1−σ2n(2j−1−2m)(t)(ab)(2j−1−2m)n(ab)2j−1−2mσ2(2j−1−2m)(t)−1)=a2m+1(σ(t)−τ(t))2m+1m∑j=0(−1)j(2m+1j)(σ2(2m+1−2j)(t)(ab)2m+1−2j−σ(2n+2)(2m+1−2j)(t)(ab)(n+1)(2m+1−2j)+1−σ2n(2j−1−2m)(t)(ab)(2j−1−2m)n1−σ2(2m+1−2j)(t)(ab)(2m+1−2j))=a2m+1(σ(t)−τ(t))2m+1m∑j=0(−1)j(2m+1j)×(σ2m+1−2j(t)−τ2m+1−2j(t)−σ(2n+1)(2m+1−2j)(t)(ab)(2m+1−2j)n+τ(2n+1)(2m+1−2j)(t)(ab)(2m+1−2j)n−σ2m+1−2j(t)−τ2m+1−2j(t))=a2m+1b(a2b2t2+4ab)mm∑j=0(−1)m−j(2m+1m−j)(f(2n+1)(2j+1)(t)−f2j+1(t)l2j+1(t)). |
Proof of Theorem 2. We only prove (1.7), and the proofs for other identities are similar.
n∑k=1f2m2k(t)=n∑k=1(aς(2k+1)(ab)⌊2k2⌋⋅(σ2k(t)−τ2k(t)σ(t)−τ(t)))2m=a2m(σ(t)−τ(t))2mn∑k=1(σ2k(t)−τ2k(t))2m(ab)2mk=a2m(σ(t)−τ(t))2mn∑k=12m∑j=0(−1)j(2mj)σ2k(2m−j)(t)τ2kj(t)(ab)2mk=a2m(σ(t)−τ(t))2m2m∑j=0(−1)j(2mj)(1−σ2n(2m−2j)(t)(ab)(2m−2j)n(ab)2m−2jσ2(2m−2j)(t)−1) |
=a2m(σ(t)−τ(t))2mm∑j=0(−1)j(2mj)(1−σ2n(2m−2j)(t)(ab)(2m−2j)n(ab)2m−2jσ2(2m−2j)(t)−1+1−σ2n(2j−2m)(t)(ab)(2j−2m)n(ab)2j−2mσ2(2j−2m)(t)−1)+a2m(σ(t)−τ(t))2m(−1)m+1(2mm)n=a2m(σ(t)−τ(t))2mm∑j=0(−1)j(2mj)(σ2(2m−2j)(t)(ab)2m−2j−σ(2n+2)(2m−2j)(t)(ab)(n+1)(2m−2j)−1+σ2n(2j−2m)(t)(ab)(2j−2m)n1−σ2(2m−2j)(t)(ab)2m−2j)+a2m(σ(t)−τ(t))2m(−1)m+1(2mm)n=a2m(σ(t)−τ(t))2mm∑j=0(−1)j(2mj)(σ2m−2j(t)−τ2m−2j(t)−σ(2n+1)(2m−2j)(t)(ab)n(2m−2j)+τ(2n+1)(2m−2j)(t)(ab)n(2m−2j)τ2m−2j(t)−σ2m−2j(t))+a2m(σ(t)−τ(t))2m(−1)m+1(2mm)n=a2m(a2b2t2+4ab)mm∑j=0(−1)m−j(2mm−j)(f2j(2n+1)(t)−f2j(t)f2j(t))+a2m(a2b2t2+4ab)m(−1)m+1(2mm)n. |
Proof of Corollary 1. First, from the definition of fn(t) and binomial expansion, we easily prove (f2n+1(t)−1,a2b2t2+4ab)=1. Therefore, (f2n+1(t)−1,(a2b2t2+4ab)m)=1. Now, we prove (1.11) by Lemma 1 and (1.3):
bl1(t)l3(t)⋯l2m+1(t)n∑k=1f2m+12k(t)=l1(t)l3(t)⋯l2m+1(t)(a2m+1(σ(t)−τ(t))2mm∑j=0(−1)m−j(2m+1m−j)(f(2n+1)(2j+1)(t)−f2j+1(t)l2j+1(t)))≡0(modf2n+1(t)−1). |
Now, we use Lemma 2 and (1.5) to prove (1.12):
al1(t)l3(t)⋯l2m+1(t)n∑k=1l2m+12k(t)=l1(t)l3(t)⋯l2m+1(t)(m∑j=0(2m+1m−j)(al(2n+1)(2j+1)(t)−al2j+1(t)l2j+1(t)))≡0(modl2n+1(t)−at). |
In this paper, we discuss the power sums of bi-periodic Fibonacci and Lucas polynomials by Binet formulas. As corollaries of the theorems, we extend the divisible properties of the sum of power of linear Fibonacci and Lucas sequences to nonlinear Fibonacci and Lucas polynomials. An open problem is whether we extend the Melham conjecture to nonlinear Fibonacci and Lucas polynomials.
The authors declare that they did not use Artificial Intelligence (AI) tools in the creation of this paper.
The authors would like to thank the editor and referees for their helpful suggestions and comments, which greatly improved the presentation of this work. All authors contributed equally to the work, and they have read and approved this final manuscript. This work is supported by Natural Science Foundation of China (12126357).
The authors declare that there are no conflicts of interest regarding the publication of this paper.
[1] |
A. M. Alghamdi, S. Gala, M. A. Ragusa, Regularity criterion for weak solutions to the Navier-Stokes involving one velocity and one vorticity components, Siberian Electron. Math. Rep., 19 (2022), 309–315. https://doi.org/10.33048/semi.2022.19.025 doi: 10.33048/semi.2022.19.025
![]() |
[2] |
A. Choucha, S. Boulaaras, D. Ouchenane, Exponential decay and global existence of solutions of a singular nonlocal viscoelastic system with distributed delay and damping terms, Filomat, 35 (2021), 795–826. https://doi.org/10.2298/FIL2103795C doi: 10.2298/FIL2103795C
![]() |
[3] |
C. S. Dou, Z. S. Zhao, Analytical solution to 1D compressible Navier-Stokes equations, J. Funct. Spaces, 2021 (2021), 6339203. https://doi.org/10.1155/2021/6339203 doi: 10.1155/2021/6339203
![]() |
[4] | C. Foias, O. Manley, R. Rosa, R. Temam, Navier-Stokes Equations and Turbulence, Cambridge University Press, Cambridge, 2001. |
[5] | J. L. Lions, Quelques Méthodes de Résolution des Problémes aux Limites Non Linéaires, Dunod, Gauthier-Villars, Paris, 1969. |
[6] | J. C. Robinson, J. L. Rodrigo, W. Sadowski, The Three-Dimensional Navier-Stokes Equations, Cambridge University Press, Cambridge, 2016. |
[7] | R. Temam, Navier-Stokes Equations and Nonlinear Functional Analysis, Philadelphia, PA, 1995. |
[8] |
J. M. Ball, Continuity properties and global attractors of generalized semiflows and the Navier-Stokes equations, J. Nonlinear Sci., 7 (1997), 475–502. https://doi.org/10.1007/s003329900037 doi: 10.1007/s003329900037
![]() |
[9] |
A. Cheskidov, C. Foias, On global attractors of the 3D Navier-Stokes equations, J. Differ. Equations, 231 (2006), 714–754. https://doi.org/10.1016/j.jde.2006.08.021 doi: 10.1016/j.jde.2006.08.021
![]() |
[10] |
X. Cai, Q. Jiu, Weak and strong solutions for the incompressible Navier-Stokes equations with damping, J. Math. Anal. Appl., 343 (2008), 799–809. https://doi.org/10.1016/j.jmaa.2008.01.041 doi: 10.1016/j.jmaa.2008.01.041
![]() |
[11] |
F. Li, B. You, Pullback exponential attractors for the three dimensional non-autonomous Navier-Stokes equations with nonlinear damping, Discrete Contin. Dyn. Syst. Ser. B, 25 (2020), 55–80. https://doi.org/10.3934/dcdsb.2019172 doi: 10.3934/dcdsb.2019172
![]() |
[12] |
F. Li, B. You, Y. Xu, Dynamics of weak solutions for the three dimensional Navier-Stokes equations with nonlinear damping, Discrete Contin. Dyn. Syst. Ser. B, 23 (2018), 4267–4284. https://doi.org/10.3934/dcdsb.2018137 doi: 10.3934/dcdsb.2018137
![]() |
[13] |
D. Pardo, J. Valero, Á. Giménez, Global attractors for weak solutions of the three-dimensional Navier-Stokes equations with damping, Discrete Contin. Dyn. Syst. Ser. B, 24 (2019), 3569–3590. https://doi.org/10.3934/dcdsb.2018279 doi: 10.3934/dcdsb.2018279
![]() |
[14] |
X. L. Song, Y. R. Hou, Attractors for the three-dimensional incompressible Navier-Stokes equations with damping, Discrete Contin. Dyn. Syst., 31 (2011), 239–252. https://doi.org/10.3934/dcds.2011.31.239 doi: 10.3934/dcds.2011.31.239
![]() |
[15] |
C. Foias, O. P. Manley, R. Temam, Y. M. Trève, Asymptotic analysis of the Navier-Stokes equations, Physica D, 9 (1983), 157–188. https://doi.org/10.1016/0167-2789(83)90297-X doi: 10.1016/0167-2789(83)90297-X
![]() |
[16] |
D. A. Jones, E. S. Titi, Upper bounds on the number of determining modes, nodes, and volume elements for the Navier-Stokes equations, Indiana Univ. Math. J., 42 (1993), 875–887. https://doi.org/10.1512/iumj.1993.42.42039 doi: 10.1512/iumj.1993.42.42039
![]() |
[17] |
P. Constantin, P. Foias, R. Temam, On the dimension of the attractors in two-dimensional turbulence, Physica D, 30 (1988), 284–296. https://doi.org/10.1016/0167-2789(88)90022-X doi: 10.1016/0167-2789(88)90022-X
![]() |
[18] |
R. Selmi, A. Châabani, Well-posedness, stability and determining modes to 3D Burgers equation in Gevrey class, Z. Angew. Math. Phys., 71 (2020), 162. https://doi.org/10.1007/s00033-020-01389-3 doi: 10.1007/s00033-020-01389-3
![]() |
[19] | J. C. Kuang, Applied Inequalities (Changyong Budengshi), 2nd edition, Hunan Education Publishing House, 1993. |
[20] |
B. L. Guo, P. C. Zhu, Partial regularity of suitable weak solutions to the system of the incompressible Non-Newtonian fluids, J. Differ. Equations, 178 (2002), 281–297. https://doi.org/10.1006/jdeq.2000.3958 doi: 10.1006/jdeq.2000.3958
![]() |
[21] | V. Kalantarov, A. Kostianko, S. Zelik, Determining functionals and finite-dimensional reduction for dissipative PDEs revisited, preprint, arXiv: 2111.04125. |