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Determination of the 3D Navier-Stokes equations with damping


  • 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)={ayfn1(t)+fn2(t)n0(mod2),byfn1(t)+fn2(t)n1(mod2),n2,

    and

    l0(t)=2,l1(t)=at,ln(t)={byln1(t)+ln2(t)n0(mod2),ayln1(t)+ln2(t)n1(mod2),n2,

    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)={0n0(mod2),1n1(mod2),n2.

    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 n0, σ(t), and τ(t) are zeros of λ2abtλab. This is σ(t)=abt+a2b2t2+4ab2 and τ(t)=abta2b2t2+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 m1 be an integer, then the sum

    L1L3L5L2m+1nk=1F2m+12k

    can be represented as (F2n+11)2R2m1(F2n+1), including R2m1(t) as a polynomial with integer coefficients of degree 2m1.

    Conjecture 2. Let m1 be an integer, then the sum

    L1L3L5L2m+1nk=1L2m+12k

    can be represented as (L2n+11)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

    nk=1f2m+12k(t)=a2m+1b(a2b2t2+4ab)mmj=0(1)mj(2m+1mj)(f(2n+1)(2j+1)(t)f2j+1(t)l2j+1(t)), (1.3)
    nk=1f2m+12k+1(t)=(ab)m(a2b2t2+4ab)mmj=0(2m+1mj)(f(2n+2)(2j+1)(t)f2(2j+1)(t)l2j+1(t)), (1.4)
    nk=1l2m+12k(t)=mj=0(2m+1mj)(l(2n+1)(2j+1)(t)l2j+1(t)l2j+1(t)), (1.5)
    nk=1l2m+12k+1(t)=am+1bm+1mj=0(1)mj(2m+1mj)(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

    nk=1f2m2k(t)=a2m(a2b2t2+4ab)mmj=0(1)mj(2mmj)f2j(2n+1)(t)f2j(t)a2m(a2b2t2+4ab)m(2mm)(1)m(n+12), (1.7)
    nk=1f2m2k+1(t)=(ab)m(a2b2t2+4ab)mmj=0(2mmj)(f2j(2n+2)(t)f4j(t)f2j(t))(ab)m(a2b2t2+4ab)m(2mm)n, (1.8)
    nk=1l2m2k(t)=mj=0(2mmj)f2j(2n+1)(t)l2j+1(t)22m1(2mm)(n+12), (1.9)
    nk=1l2m2k+1(t)=ambmmj=0(1)mj(2mmj)(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)nk=1f2m+12k(t)0(modf2n+1(t)1), (1.11)

    and

    al1(t)l3(t)l2m+1(t)nk=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:

    bl1l3l2m+1nk=1f2m+12k0(modf2n+11), (1.13)

    and

    al1l3l2m+1nk=1l2m+12k0(modl2n+1a), (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:

    L1L3L2m+1nk=1F2m+12k0(modF2n+11), (1.15)

    and

    L1L3L2m+1nk=1L2m+12k0(modL2n+11), (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 j0. 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+12, we have

    l2(2n+1)(t)f(2n+1)(2j+1)(t)=f(2n+1)(2j+3)(t)+abf(2n+1)(2j1)(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)(2k1)(t)l2(t)f2k+1(t)+abf2k1(t)((abt2+4)f21(t)2)f(2n+1)(2k+1)(t)abf(2n+1)(2k1)(t)((abt2+4)f21(t)2)f2k+1(t)+abf2k1(t)((abt2+4)f21(t)2)(f(2n+1)(2k+1)(t)f2k+1(t))ab(f(2n+1)(2k1)(t)f2k1(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 j0. 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+12, we have

    l2(2n+1)(t)l(2n+1)(2j+1)(t)=l(2n+1)(2j+3)(t)+l(2n+1)(2j1)(t),

    and

    al2(2n+1)(t)=bl22n+1(t)+2abl21(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)(2k1)(t))a(l2(t)l2k+1(t)l2k1(t))(bl21(t)+2a)l(2n+1)(2k+1)(t)al(2n+1)(2k1)(t)(bl21(t)+2a)l2k+1(t)+al2k1(t)(abt2+2)(al(2n+1)(2k+1)(t)al2k+1(t))(al(2n+1)(2k1)(t)al2k1(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.

    nk=1f2m+12k(t)=nk=1(aς(2k+1)(ab)2k2(σ2k(t)τ2k(t)σ(t)τ(t)))2m+1=a2m+1(σ(t)τ(t))2m+1nk=1(σ2k(t)τ2k(t))2m+1(ab)(2m+1)k=a2m+1(σ(t)τ(t))2m+1nk=12m+1j=0(1)j(2m+1j)σ2k(2m+1j)(t)τ2kj(t)(ab)(2m+1)k=a2m+1(σ(t)τ(t))2m+12m+1j=0(1)j(2m+1j)(1σ2n(2m+12j)(t)(ab)(2m+12j)n(ab)2m+12jσ2(2m+12j)(t)1)=a2m+1(σ(t)τ(t))2m+1mj=0(1)j(2m+1j)(1σ2n(2m+12j)(t)(ab)(2m+12j)n(ab)2m+12jσ2(2m+12j)(t)11σ2n(2j12m)(t)(ab)(2j12m)n(ab)2j12mσ2(2j12m)(t)1)=a2m+1(σ(t)τ(t))2m+1mj=0(1)j(2m+1j)(σ2(2m+12j)(t)(ab)2m+12jσ(2n+2)(2m+12j)(t)(ab)(n+1)(2m+12j)+1σ2n(2j12m)(t)(ab)(2j12m)n1σ2(2m+12j)(t)(ab)(2m+12j))=a2m+1(σ(t)τ(t))2m+1mj=0(1)j(2m+1j)×(σ2m+12j(t)τ2m+12j(t)σ(2n+1)(2m+12j)(t)(ab)(2m+12j)n+τ(2n+1)(2m+12j)(t)(ab)(2m+12j)nσ2m+12j(t)τ2m+12j(t))=a2m+1b(a2b2t2+4ab)mmj=0(1)mj(2m+1mj)(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.

    nk=1f2m2k(t)=nk=1(aς(2k+1)(ab)2k2(σ2k(t)τ2k(t)σ(t)τ(t)))2m=a2m(σ(t)τ(t))2mnk=1(σ2k(t)τ2k(t))2m(ab)2mk=a2m(σ(t)τ(t))2mnk=12mj=0(1)j(2mj)σ2k(2mj)(t)τ2kj(t)(ab)2mk=a2m(σ(t)τ(t))2m2mj=0(1)j(2mj)(1σ2n(2m2j)(t)(ab)(2m2j)n(ab)2m2jσ2(2m2j)(t)1)
    =a2m(σ(t)τ(t))2mmj=0(1)j(2mj)(1σ2n(2m2j)(t)(ab)(2m2j)n(ab)2m2jσ2(2m2j)(t)1+1σ2n(2j2m)(t)(ab)(2j2m)n(ab)2j2mσ2(2j2m)(t)1)+a2m(σ(t)τ(t))2m(1)m+1(2mm)n=a2m(σ(t)τ(t))2mmj=0(1)j(2mj)(σ2(2m2j)(t)(ab)2m2jσ(2n+2)(2m2j)(t)(ab)(n+1)(2m2j)1+σ2n(2j2m)(t)(ab)(2j2m)n1σ2(2m2j)(t)(ab)2m2j)+a2m(σ(t)τ(t))2m(1)m+1(2mm)n=a2m(σ(t)τ(t))2mmj=0(1)j(2mj)(σ2m2j(t)τ2m2j(t)σ(2n+1)(2m2j)(t)(ab)n(2m2j)+τ(2n+1)(2m2j)(t)(ab)n(2m2j)τ2m2j(t)σ2m2j(t))+a2m(σ(t)τ(t))2m(1)m+1(2mm)n=a2m(a2b2t2+4ab)mmj=0(1)mj(2mmj)(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)nk=1f2m+12k(t)=l1(t)l3(t)l2m+1(t)(a2m+1(σ(t)τ(t))2mmj=0(1)mj(2m+1mj)(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)nk=1l2m+12k(t)=l1(t)l3(t)l2m+1(t)(mj=0(2m+1mj)(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.



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