Research article

Physical significance and periodic solutions of the high-order good Jaulent-Miodek model in fluid dynamics

  • Received: 03 September 2024 Revised: 27 October 2024 Accepted: 04 November 2024 Published: 08 November 2024
  • MSC : 35Q31, 35Q51

  • Using Whitham modulation theory, this paper examined periodic solutions and the problem of discontinuous initial values for the higher-order good Jaulent-Miodek (JM) equation. The physical significance of the JM equations was discussed by considering the reduction of Euler's equation. Next, the zero- and one-phase periodic solutions of the JM equation, along with the associated Whitham equations, were derived. The analysis included the degeneration of the one-phase periodic solution and the genus-one Whitham equation by examining the limits of the modulus m of the Jacobi elliptic functions. Additionally, analytical and graphical representations of rarefaction wave solutions and periodic wave patterns were provided, and a solution for discontinuous initial values in the JM equation was presented. The results of this study offer a theoretical foundation for analyzing discontinuous initial values in nonlinear dispersion equations.

    Citation: Wenzhen Xiong, Yaqing Liu. Physical significance and periodic solutions of the high-order good Jaulent-Miodek model in fluid dynamics[J]. AIMS Mathematics, 2024, 9(11): 31848-31867. doi: 10.3934/math.20241530

    Related Papers:

    [1] Kamaraj Dhurai, Nak Eun Cho, Srikandan Sivasubramanian . On a class of analytic functions closely related to starlike functions with respect to a boundary point. AIMS Mathematics, 2023, 8(10): 23146-23163. doi: 10.3934/math.20231177
    [2] Lina Ma, Shuhai Li, Huo Tang . Geometric properties of harmonic functions associated with the symmetric conjecture points and exponential function. AIMS Mathematics, 2020, 5(6): 6800-6816. doi: 10.3934/math.2020437
    [3] Georgia Irina Oros, Gheorghe Oros, Daniela Andrada Bardac-Vlada . Certain geometric properties of the fractional integral of the Bessel function of the first kind. AIMS Mathematics, 2024, 9(3): 7095-7110. doi: 10.3934/math.2024346
    [4] Bo Wang, Rekha Srivastava, Jin-Lin Liu . Certain properties of multivalent analytic functions defined by q-difference operator involving the Janowski function. AIMS Mathematics, 2021, 6(8): 8497-8508. doi: 10.3934/math.2021493
    [5] Pinhong Long, Huo Tang, Wenshuai Wang . Functional inequalities for several classes of q-starlike and q-convex type analytic and multivalent functions using a generalized Bernardi integral operator. AIMS Mathematics, 2021, 6(2): 1191-1208. doi: 10.3934/math.2021073
    [6] K. Saritha, K. Thilagavathi . Differential subordination, superordination results associated with Pascal distribution. AIMS Mathematics, 2023, 8(4): 7856-7864. doi: 10.3934/math.2023395
    [7] Muajebah Hidan, Abbas Kareem Wanas, Faiz Chaseb Khudher, Gangadharan Murugusundaramoorthy, Mohamed Abdalla . Coefficient bounds for certain families of bi-Bazilevič and bi-Ozaki-close-to-convex functions. AIMS Mathematics, 2024, 9(4): 8134-8147. doi: 10.3934/math.2024395
    [8] Kholood M. Alsager, Sheza M. El-Deeb, Ala Amourah, Jongsuk Ro . Some results for the family of holomorphic functions associated with the Babalola operator and combination binomial series. AIMS Mathematics, 2024, 9(10): 29370-29385. doi: 10.3934/math.20241423
    [9] Zhi-Gang Wang, M. Naeem, S. Hussain, T. Mahmood, A. Rasheed . A class of analytic functions related to convexity and functions with bounded turning. AIMS Mathematics, 2020, 5(3): 1926-1935. doi: 10.3934/math.2020128
    [10] İbrahim Aktaş . On some geometric properties and Hardy class of q-Bessel functions. AIMS Mathematics, 2020, 5(4): 3156-3168. doi: 10.3934/math.2020203
  • Using Whitham modulation theory, this paper examined periodic solutions and the problem of discontinuous initial values for the higher-order good Jaulent-Miodek (JM) equation. The physical significance of the JM equations was discussed by considering the reduction of Euler's equation. Next, the zero- and one-phase periodic solutions of the JM equation, along with the associated Whitham equations, were derived. The analysis included the degeneration of the one-phase periodic solution and the genus-one Whitham equation by examining the limits of the modulus m of the Jacobi elliptic functions. Additionally, analytical and graphical representations of rarefaction wave solutions and periodic wave patterns were provided, and a solution for discontinuous initial values in the JM equation was presented. The results of this study offer a theoretical foundation for analyzing discontinuous initial values in nonlinear dispersion equations.



    In the literature, special functions have a great importance in a variety of fields of mathematics, such as mathematical physics, mathematical biology, fluid mechanics, geometry, combinatory and statistics. Due of the essential position of special functions in mathematics, they continue to play an essential role in the subject as well as in the geometric function theory. For geometric behavior of some other special functions, one can refer to [1,2,3,4,5,6,7,8,9,10,11,12]. An interesting way to discuss the geometric properties of special functions is by the means of some criteria due to Ozaki, Fejér and MacGregor. One of the important special functions is the Mathieu series that appeared in the nineteenth century in the monograph [13] defined on R by

    S(r)=n12n(n2+r2)2. (1.1)

    Surprisingly, the Mathieu series is considered in a variety of fields of mathematical physics, namely, in the elasticity of solid bodies [13]. For more applications regarding the Mathieu series, we refer the interested reader to [14, p. 258, Eq (54)]. The functions bear the name of the mathematician Émile Leonard Mathieu (1835–1890). Recently, a more general family of the Mathieu series was studied by Diananda [15] in the following form:

    Sμ(r)=n12n(n2+r2)μ+1(μ>0,rR). (1.2)

    In 2020, Gerhold et al. [16], considered a new Mathieu type power series, defined by

    Sα,β,μ(r;z)=k=0(k!)αzk((k!)β+r2)μ+1, (1.3)

    where α,μ0,β,r>0 and |z|1, such that α<β(μ+1).

    In [17], Bansal and Sokól have determined sufficient conditions imposed on the parameters such that the normalized form of the function S(r,z) belong to a certain class of univalent functions, such as starlike and close-to-convex. In [18], the authors presented some generalizations of the results of Bansal and Sokól by using the same technique. In addition, Gerhold et al. [18, Theorems 5 and 6] has established some sufficient conditions imposed on the parameter of the normalized form of the function S1,2,μ(r;z) defined by

    Qμ(r;z):=z+n=2n!(r2+1)μ+1((n!)2+r2)μ+1zn, (1.4)

    to be starlike and close-to-convex in the open unit disk. The main focus of the present paper is to extend and improve some results from [18] by using a completely different method. More precisely, in this paper we present some sufficient conditions, such as the normalized form of the function S1,β,μ(r;z) defined by

    Qμ,β(r;z)=z+n=2n!(r2+1)μ+1zn((n!)β+r2)μ+1, (1.5)

    satisfying several geometric properties such as starlikeness, convexity and close-to-convexity.

    We denoted by H the class of all analytic functions inside the unit disk

    D={z:zCand|z|<1}.

    Assume that A denoted the collection of all functions fH, satisfying the normalization f(0)=f(0)1=0 such that

    f(z)=z+k=2akzk,(zD).

    A function fA is said to be a starlike function (with respect to the origin zero) in D, if f is univalent in D and f(D) is a starlike domain with respect to zero in C. This class of starlike functions is denoted by S. The analytic characterization of S is given [19] below:

    (zf(z)f(z))>0(zD).

    If f(z) is a univalent function in D and f(D) is a convex domain in C, then fA is said to be a convex function in D. We denote this class of convex functions by K, which can also be described as follows:

    (1+zf(z)f(z))>0(zD).

    An analytic function f in A is called close-to-convex in the open unit disk D if there exists a function g(z), which is starlike in D such that

    (zf(z)g(z))>0,zD.

    It can be noted that every close-to-convex function in D is also univalent in D (see, for details, [19,20]).

    In order to show the main results, the following preliminary lemmas will be helpful. The first result is due to Ozaki (see also [21, Lemma 2.1]).

    Lemma 1.1. [22] Let

    f(z)=z+n=2anzn,

    be analytic in D. If

    12a2(n+1)an+10,

    or if

    12a2(n+1)an+12,

    then f is close-to-convex with respect to the function log(1z).

    Remark 1.2. We note that, as Ponnusamy and Vuorinen pointed out in [21], proceeding exactly as in the proof of Lemma 1.1, one can verify directly that if a function f:DC satisfies the hypothesis of the above lemma, then it is close-to-convex with respect to the convex function

    z1z.

    The next two lemmas are due to Fejér [23].

    Lemma 1.3. Suppose that a function f(z)=1+k=2akzk1, with ak0(k2) as analytic in D. If (ak)k1 is a convex decreasing sequence, i.e., ak2ak+1+ak+20 and akak+10 for all k1, then

    (f(z))>12(zD).

    Lemma 1.4. Suppose that a f(z)=z+k=2akzk, with ak0(k2) as analytic in D. If (kak)k1 and (kak(k+1)ak+1)k1 both are decreasing, then f is starlike in D.

    Lemma 1.5 ([24]). Assume that fA. If the following inequality

    |f(z)z1|<1,

    holds for all zD, then f is starlike in

    D12:={zCand|z|<12}.

    Lemma 1.6 ([25]). Assume that fA and satisfies

    |f(z)1|<1,

    for each zD, then f is convex in D12.

    Theorem 2.1. Let μ,β>0 and 0<r1 such that β1+2μ+1. In addition, if the following condition holds:

    H:(2β+12)μ+14,

    then the function Qμ,β(r;z) is close-to-convex in D with respect to the function log(1z).

    Proof. For the function Qμ,β(r;z), we have

    a1=1andak=k!(r2+1)μ+1((k!)β+r2)μ+1(k2).

    To prove the result, we need to show that the sequence {kak}k1 is decreasing under the given conditions. For k2 we have

    kak(k+1)ak+1=(r2+1)μ+1[kk!((k!)β+r2)μ+1(k+1)(k+1)!(((k+1)!)β+r2)μ+1]=k!(r2+1)μ+1[k((k!)β+r2)μ+1(k+1)2(((k+1)!)β+r2)μ+1]=k!(r2+1)μ+1Ak(β,μ,r)[((k!)β+r2)(((k+1)!)β+r2)]μ+1, (2.1)

    where

    Ak(β,μ,r)=k(((k+1)!)β+r2)μ+1(k+1)2((k!)β+r2)μ+1,k2.

    However, we have

    Ak(β,μ,r)=(k1μ+1((k+1)!)β+k1μ+1r2)μ+1((k+1)2μ+1(k!)β+(k+1)2μ+1r2)μ+1=exp((μ+1)log[k1μ+1((k+1)!)β+k1μ+1r2])exp((μ+1)log[(k+1)2μ+1(k!)β+(k+1)2μ+1r2])=j=0[logj(k1μ+1((k+1)!)β+k1μ+1r2)logj((k+1)2μ+1(k!)β+(k+1)2μ+1r2)](μ+1)jj!. (2.2)

    In addition, for all k2, we have

    k1μ+1((k+1)!)β+k1μ+1r2(k+1)2μ+1(k!)β+(k+1)2μ+1r2=r2(k1μ+1(k+1)2μ+1)+k1μ+1((k+1)!)β(k+1)2μ+1(k!)β[k1μ+1(k+1)2μ+1+k1μ+1((k+1)!)β2]+[k1μ+1((k+1)!)β2(k+1)2μ+1(k!)β]=k1μ+1(1+((k+1)!)β2((k+1)2k)1μ+1)+(k!)β(k1μ+1(k+1)β2(k+1)2μ+1)k1μ+1(k+1)2μ+1(1+(k!)β(k+1)21k1μ+1)+(k!)β(k+1)2μ+1(k1μ+1(k+1)21)k1μ+1(k+1)2μ+1(1+(k!)βk1μ+11k1μ+1)+(k!)β(k+1)2μ+1(k1μ+11), (2.3)

    which is positive by our assumption. Having (2.1)–(2.3), we conclude that the sequence (kak)k2 is decreasing. Finally, we see that the condition (H) implies that a12a2, then the function Qμ,β(r;z) is close-to-convex in D with respect to the function log(1z) by Lemma 1.1.

    If we set β=32 in Theorem 2.1, we derive the following result as follows:

    Corollary 2.2. Let 0<r1. If μ3, then the function Qμ,32(r;z) is close-to-convex in D with respect to the function log(1z).

    Upon setting μ=2 in Theorem 2.1, we get the following result:

    Corollary 2.3. Let 0<r1. If β53, then the function Q2,β(r;z) is close-to-convex in D with respect to the function log(1z).

    Remark 2.4. In [18], it is established that the function Qμ,2(r;z)=:Qμ(r;z) is close-to-convex in D with respect to the function z1z for all 0<rμ. Moreover, in view of Remark 1.2, we conclude that the function Qμ,2(r;z) is close-to-convex in D with respect to the function log(1z) for all 0<rμ. However, in view of Corollaries 2.2 and 2.3, we deduce that Theorem 2.1 improves the corresponding result available in [18, Theorem 5] for 0<r1.

    Theorem 2.5. Assume that μ,β>0,0<r1 such that β1+1μ+1. In addition, if the condition (H) holds, then

    (Qμ,β(r;z)z)>12,

    for all zD.

    Proof. For k1, we get

    ((k!)β+r2)μ+1(((k+1)!)β+r2)μ+1(akak+1)(r2+1)μ+1=k!(((k+1)!)β+r2)μ+1(k+1)!((k!)β+r2)μ+1=[(k!)1μ+1((k+1)!)β+r2)]μ+1[((k+1)!)1μ+1((k!)β+r2)]μ+1. (2.4)

    Further, for all k1, we have

    (k!)1μ+1((k+1)!)β+r2)((k+1)!)1μ+1((k!)β+r2)=r2[(k!)1μ+1((k+1)!)1μ+1]+(k!)1μ+1((k+1)!)β((k+1)!)1μ+1(k!)β(k!)1μ+1((k+1)!)1μ+1+(k!)1μ+1((k+1)!)β((k+1)!)1μ+1(k!)β=(k!)1μ+1[1+(k!)β(k+1)β2(k+1)1μ+1]+(k!)β+1μ+1[(k+1)β2(k+1)1μ+1](k!)1μ+1[1+(k+1)1+1μ+12(k+1)1μ+1]+(k!)β+1μ+1[(k+1)1+1μ+12(k+1)1μ+1]=(k!)1μ+1[1+(k+1)1μ+1((k+1)21)]+(k!)β+1μ+1(k+1)1μ+1((k+1)21)>0. (2.5)

    Hence, in view of (2.4) and (2.5), we deduce that the sequence (ak)k1 is decreasing. Next, we prove that (ak)k1 is a convex decreasing sequence, then, for k2 we obtain

    ((k!)β+r2)μ+1(((k+1)!)β+r2)μ+1(ak2ak+1)(r2+1)μ+1=k!(((k+1)!)β+r2)μ+12(k+1)!((k!)β+r2)μ+1=[(k!)1μ+1((k+1)!)β+r2)]μ+1[(2(k+1)!)1μ+1((k!)β+r2)]μ+1. (2.6)

    Moreover, we get

    (k!)1μ+1(((k+1)!)β+r2)(2(k+1)!)1μ+1((k!)β+r2)=r2[(k!)1μ+1(2(k+1)!)1μ+1]+(k!)1μ+1((k+1)!)β(2(k+1)!)1μ+1(k!)β>[(k!)1μ+1(2(k+1)!)1μ+1]+(k!)1μ+1((k+1)!)β3+2(k!)β+1μ+13[(k+1)β3.2μμ+1(k+1)1μ+1](k!)1μ+1[1+((k+1)!)1+1μ+13(2(k+1))1μ+1]+2(k!)β+1μ+13[(k+1)1+1μ+13.2μμ+1(k+1)1μ+1]=(k!)1μ+1[1+(k+1)1μ+1{(k+1)(k!)1+1μ+1321μ+1}]+2(k!)β+1μ+1(k+1)1μ+13[(k+1)3.2μμ+1]>2[12μμ+1](k!)β+1μ+1(k+1)1μ+1>0. (2.7)

    Keeping (2.6) and (2.7) in mind, we have ak2ak+1>0 for all k2. In addition, the condition (H) implies a12a20. This in turn implies that the sequence (ak)k1 is convex. Finally, by Lemma 1.3, we obtain the desired result.

    Taking β=32 in Theorem 2.5, we derive the following result:

    Corollary 2.6. Assume that r(0,1]. If μlog(4)log(232+1)log(2)11.14, then

    (Qμ,32(r;z)z)>12(zD).

    Setting μ=1 in Theorem 2.5, we established the following result which reads as follows:

    Corollary 2.7. Let 0<r1. If βlog(3)log(2), then

    (Q1,β(r;z)z)>12(zD).

    Remark 2.8. The result obtained in the above theorem has been derived from [18, Theorem 6] for β=2,μ>0 and 0<r<μ. Hence, in view of Corollaries 2.2 and 2.6, we deduce that Theorem 2.5 improves the corresponding result given in [18, Theorem 6] for 0<r1.

    Theorem 2.9. Assume that min(μ,β)>0,0<r1 such that β1+3μ+1, then the function Qμ,β(r;z) is starlike in D.

    Proof. We see in the proof of Theorem 2.1 that the sequence (kak)k1 is decreasing. Hence, with the aid of Lemma 1.4 to show that the function Qμ,β(r;z) is starlike in D, it suffices to prove that the sequence (kak(k+1)ak+1)k1 is decreasing. We have

    kak2(k+1)ak+1=k!(r2+1)μ+1Bk(β,μ,r)[((k!)β+r2)((k+1)!)β+r2)]μ+1, (2.8)

    where

    Bk(β,μ,r)=k(((k+1)!)β+r2)μ+12(k+1)2((k!)β+r2)μ+1,k1.

    For k2, we have

    k1μ+1(((k+1)!)β+r2)(2(k+1)2)1μ+1((k!)β+r2)k1μ+1(2(k+1)2)1μ+1+k1μ+1((k+1)!)β2+[k1μ+1((k+1)!)β2(2(k+1)2)1μ+1(k!)β]=k1μ+1+k1μ+1((k+1)!)β2(2(k+1)2)1μ+1+(k!)β(k1μ+1(k+1)β2(2(k+1)2)1μ+1)k1μ+1+(k+1)2μ+1(k1μ+1(k!)β(k+1)221μ+1)+(k!)β(k+1)2μ+1(k1μ+1(k+1)221μ+1)k1μ+1+(k+1)2μ+1(k1μ+1(k!)β21μ+1)+(k!)β(k+1)2μ+1(k1μ+121μ+1)>0, (2.9)

    which in turn implies that

    Bk(β,μ,r)>0,

    for all k2, and consequently, the sequence (kak(k+1)ak+1)k2 is decreasing. Further, a simple computation gives

    a14a2+3a3(1+r2)μ+1=1(1+r2)μ+18(2β+r2)μ+1+18(6β+r2)μ+112μ+182β(μ+1)+18(6β+r2)μ+1=2β(μ+1)2μ+42(β+1)(μ+1)+18(6β+r2)μ+12μ+42μ+42(β+1)(μ+1)+18(6β+r2)μ+1>0.

    Therefore, (kak(k+1)ak+1)k1 is decreasing, which leads us to the asserted result.

    In the next Theorem we present another set of sufficient conditions to be imposed on the parameters so that the function Qμ,β(r;z) is starlike in D.

    Theorem 2.10. Let the parameters be the same as in Theorem 2.1. In addition, if the following conditions

    H:(2β+12)μ+18(e2),

    hold true, then the function Qμ,β(r;z) is starlike in D.

    Proof. First of all, we need to prove that the sequences (uk)k2 and (vk)k2 defined by

    uk=(k!)2(r2+1)μ+1((k!)β+r2)μ+1andvk=(k1)(k!)2(r2+1)μ+1((k!)β+r2)μ+1,

    are decreasing. Indeed, we have

    ((k!)β+r2)μ+1(((k+1)!)β+r2)μ+1(ukuk+1)(k!)2(r2+1)μ+1=(((k+1)!)β+r2)μ+1(k+1)2((k!)β+r2)μ+1. (2.10)

    In addition, for any k2, we have

    ((k+1)!)β+r2(k+1)2μ+1((k!)β+r2)=r2(1(k+1)2μ+1)+((k+1)!)β(k+1)2μ+1(k!)β1(k+1)2μ+1+((k+1)!)β(k+1)2μ+1(k!)β=1+(((k+1)!)β2(k+1)2μ+1)+(((k+1)!)β2(k+1)2μ+1(k!)β)1+((k!)β(k+1)1+2μ+12(k+1)2μ+1)+(k!)β((k+1)1+2μ+12(k+1)2μ+1)=1+(k+1)2μ+1((k!)β(k+1)21)+(k!)β(k+1)2μ+1(k+121)>0. (2.11)

    According to (2.10) and (2.11) we conclude that the sequence (uk)k2 is decreasing. Also, for k2, we have

    ((k!)β+r2)μ+1(((k+1)!)β+r2)μ+1(vkvk+1)(k!)2(r2+1)μ+1=(k1)(((k+1)!)β+r2)μ+1k(k+1)2((k!)β+r2)μ+1. (2.12)

    Moreover, for all k2, we find

    (k1)1μ+1(((k+1)!)β+r2)(k(k+1)2)1μ+1((k!)β+r2)=r2((k1)1μ+1(k(k+1)2)1μ+1)+(k1)1μ+1((k+1)!)β(k(k+1)2)1μ+1(k!)β(k1)1μ+1(k(k+1)2)1μ+1+(k1)1μ+1((k+1)!)β3+2(k1)1μ+1((k+1)!)β3(k(k+1)2)1μ+1(k!)β(k1)1μ+1+(k+1)2μ+1((k1)1μ+1(k!)1+2μ+1(k+1)3k1μ+1)+(k!)β(k+1)2μ+1(2(k1)1μ+1(k+1)3k1μ+1)(k1)1μ+1+(k+1)2μ+1((k1)1μ+1(k!)1+2μ+1k1μ+1)+(k!)β(k+1)2μ+1(2(k1)1μ+1k1μ+1). (2.13)

    Since the sequence (k/(k1))n2 is decreasing, we deduce that kk12 for all k2 and consequently,

    (kk1)1μ+121μ+12(k2,μ>0).

    Hence, in view of the above inequality combined with (2.13) and (2.12), we conclude that the sequence (vk)k2 is decreasing. Now, we set

    ˜Qμ,β(r;z):=z[Qμ,β(r;z)]Qμ,β(r;z),zD.

    We see that the function ˜Qμ,β(r;z) is analytic in D and satisfies ˜Qμ,β(r;0)=1. Hence, to derive the desired result, it suffices to prove that, for any zD, we have

    (˜Qμ,β(r;z))>0.

    For this goal in view, it suffices to show that

    |˜Qμ,β(r;z)1|<1(zD).

    For all zD, we get

    |[Qμ,β(r;z)]Qμ,β(r;z)z|<k=2(k1)k!(r2+1)μ+1((k!)β+r2)μ+1=k=2vkk!v2(e2). (2.14)

    In addition, in view of the inequality:

    |a+b|||a||b||,

    we obtain

    |Qμ,β(r;z)z|>1k=2(k!)(r2+1)μ+1((k!)β+r2)μ+1=1k=2ukk!1u2(e2). (2.15)

    By using (2.14) and (2.15), for zD, we get

    |˜Qμ,β(r;z)1|=|[Qμ,β(r;z)]Qμ,β(r;z)z||Qμ,β(r;z)z|<v2(e2)1u2(e2). (2.16)

    Furthermore, by using the fact that the function rχμ,β(r)=(r2+1r2+2β)μ+1 is strictly increasing on (0,1], and with the aid of condition (H), we obtain

    (v2+u2)(e2)=8(e2)(r2+1)μ+1(2β+r2)μ+1<8(e2)(22β+1)μ+11. (2.17)

    Finally, by combining (2.16) and (2.17), we derived the desired results.

    By setting β=2 in Theorem 2.10, we obtain the following corollary:

    Corollary 2.11. If 0<r1 and μ1, then the function Qμ(r;z) defined in (1.4) is starlike in D.

    Taking β=32 in Theorem 2.10, we obtain:

    Corollary 2.12. Under the assumptions of Corollary 2.2, the function Qμ,32(r;z) is starlike in D.

    Setting in Theorem 2.10 the values μ=2, we compute the following corollary:

    Corollary 2.13. Suppose that all hypotheses of Corollary 2.3 hold, then the function Q2,β(r;z) is starlike in D.

    Example 2.14. The functions Q3,32(1/2;z) and Q2,53(1/2;z) are starlike in D.

    Figure 1 illustrates the mappings of the above examples in D.

    Figure 1.  Mappings of Qμ,β(r;z) over D.

    Theorem 2.15. Let μ,β>0 and 0<r1 such that β1+3μ+1. If the following condition

    H:(2β+12)μ+116(e2),

    holds true, then the function Qμ,β(r;z) is convex in D.

    Proof. We define the sequences (xk)k2 and (yk)k2 by

    xk=k(k!)2(r2+1)μ+1((k!)β+r2)μ+1andyk=k(k1)(k!)2(r2+1)μ+1((k!)β+r2)μ+1.

    Let k2, then

    ((k!)β+r2)μ+1(((k+1)!)β+r2)μ+1(xkxk+1)(k!)2(r2+1)μ+1=k(((k+1)!)β+r2)μ+1(k+1)3((k!)β+r2)μ+1. (2.18)

    However, we have

    k1μ+1(((k+1)!)β+r2)(k+1)3μ+1((k!)β+r2)k1μ+1(k+1)3μ+1+k1μ+1((k+1)!)β(k+1)3μ+1(k!)β=k1μ+1+(k1μ+1(k!)β(k+1)β2(k+1)3μ+1)+(k1μ+1(k!)β(k+1)β2(k+1)3μ+1(k!)β)k1μ+1+(k+1)3μ+1(k1μ+1(k!)β(k+1)21)+(k!)β(k+1)3μ+1(k1μ+1(k+1)21)>0. (2.19)

    Hence, in view of (2.18) and (2.19), we get that (xk)k2 is decreasing. Also, we have

    ((k!)β+r2)μ+1(((k+1)!)β+r2)μ+1(ykyk+1)k(k!)2(r2+1)μ+1=(k1)(((k+1)!)β+r2)μ+1(k+1)3((k!)β+r2)μ+1. (2.20)

    Moreover, for k2, we find that

    (k1)1μ+1(((k+1)!)β+r2)(k+1)3μ+1((k!)β+r2)(k1)1μ+1+((k1)1μ+1(k!)β(k+1)β2(k+1)3μ+1)+(k!)β((k1)1μ+1(n+1)β2(n+1)3μ+1)(k1)1μ+1+(k+1)3μ+1((k1)1μ+1(k!)β(k+1)21)+(k!)β(k+1)3μ+1((k1)1μ+1(k+1)21)>0. (2.21)

    Having (2.20) and (2.21) in mind, we deduce that the sequence (yk)k2 is decreasing. To show that the function Qμ,β(r;z) is convex in D, it suffices to establish that the function

    ˆQμ,β(r;z):=z[Qμ,β(r;z)],

    is starlike in D. For this objective in view, it suffices to find that

    |z[ˆQμ,β(r;z)]ˆQμ,β(r;z)1|<1(zD).

    For all zD and since (yk)k2 is decreasing, we get

    |[ˆQμ,β(r;z)]ˆQμ,β(r;z)z|<k=2k(k1)k!(r2+1)μ+1((k!)β+r2)μ+1=k=2ykk!y2(e2). (2.22)

    Further, for any zD, we obtain

    |ˆQμ,β(r;z)z|>1k=2k(k!)(r2+1)μ+1((k!)β+r2)μ+1=1k=2xkk!1x2(e2). (2.23)

    Keeping (2.22) and (2.23) in mind, for zD, we get

    |z[ˆQμ,β(r;z)]ˆQμ,β(r;z)1|=|[ˆQμ,β(r;z)]ˆQμ,β(r;z)z||ˆQμ,β(r;z)z|<y2(e2)1x2(e2)=8(e2)(r2+1)μ+1(2β+r2)μ+18(e2)(r2+1)μ+1. (2.24)

    Again, by using the fact that the function rχμ,β(r) is increasing on (0,1] and with the aid of hypothesis (H) we obtain that

    8(e2)(r2+1)μ+1(2β+r2)μ+18(e2)(r2+1)μ+1<1. (2.25)

    Finally, by combining the above inequality and (2.24), we obtain the desired result asserted by Theorem 2.15.

    Taking β=2 in Theorem 2.15, in view of (1.4), the following result holds true:

    Corollary 2.16. Let 0<r1. If μ2, then the function Qμ(r;z) is convex in D.

    If we set μ=1 in Theorem 2.15, in view of (1.5), we derive the following result:

    Corollary 2.17. Let 0<r1. If βlog(8e21)log(2), then the function Q1,β(r;z) is convex in D.

    Example 2.18. The functions Q2(r;z) and Q1,83(r;z) are convex in D.

    Figure 2 gives the mappings of the above presented examples in D.

    Figure 2.  Mappings of Qμ,β(r;z) over D.

    Theorem 2.19. Let the parameters be the same as in Theorem 2.1, then the function Qμ,β(r;z) is starlike in D12.

    Proof. For any zD we get

    |Qμ,β(r;z)z1|<k=2k!(r2+1)μ+1(k!)β+r2)μ+1=k=2ckk!, (2.26)

    where

    ck:=(k!)2(r2+1)μ+1((k!)β+r2)μ+1,k2.

    Straightforward calculation gives

    [((k!)β+r2)(((k+1)!)β+r2)]μ+1(ckck+1)(k!)2(r2+1)μ+1=(((k+1)!)β+r2)μ+1((k+1)2μ+1((k!)β+r2))μ+1. (2.27)

    Furthermore, for k2, we get

    ((k+1)!)β+r2(n+1)2μ+1((k!)β+r2)=r2(1(k+1)2μ+1)+((k+1)!)β(k!)β(k+1)2μ+1(1+((k+1)!)β2(k+1)2μ+1)+(k!)β((k+1)β2(k+1)2μ+1)(1+(k!)β(k+1)1+2μ+12(k+1)2μ+1)+(k!)β(k+1)2μ+1(k1)2(1+(k+1)2μ+1((k!)β(k+1)2)2)+(k!)β(k+1)2μ+1(k1)2>0. (2.28)

    Thus, the sequence (ck)k2 is decreasing. However, in view of (2.26), for zD we obtain

    |Qμ,β(r;z)z1|<k=2k!(r2+1)μ+1((k!)β+r2)μ+1=k=2c2k!=c2(e2)=4(e2)(r2+1)μ+1(2β+r2)μ+1. (2.29)

    According to the monotony property of the function rχβ,μ(r) on (0,1) we get

    χβ,μ(r)<14. (2.30)

    Hence, in view (2.29) and (2.30) we find for all zD that

    |Qμ,β(r;z)z1|<(e2)<1.

    With the help of Lemma 1.5, we deduce that the function Qμ,β(r;z) is starlike in D12.

    Corollary 2.20. Assume that all conditions of Corollary 2.2 are satisfied, then the function Qμ,32(r;z) is starlike in D12.

    Corollary 2.21. Suppose that all hypotheses of Corollary 2.3 hold, then the function Q2,β(r;z) is starlike in D12.

    If we set β=2 in the above Theorem, in view of (1.4), the following result is true:

    Corollary 2.22. Let 0<r1 If μ1, then the function Qμ(r;z) is starlike in D12.

    Example 2.23. The functions Q3,32(1/2;z),Q1(1;z) and Q2,53(1/2;z) are starlike in D12.

    In Figure 3, we give the mappings of the above presented examples in D.

    Figure 3.  Mappings of Qμ,β(r;z) over D12.

    Theorem 2.24. Let β,μ>0 and 0<r<1. If β1+3μ+1, then the function Qμ,β(r;z) is convex in D12.

    Proof. For all zD, it follows that

    |Qμ,β(r;z)1|<k=2kk!(r2+1)μ+1((k!)β+r2)μ+1=k=2dkk(k1), (2.31)

    where

    dk:=k2(k1)k!(r2+1)μ+1(k!)β+r2)μ+1,k2.

    For all k2, we get

    ((k!)β+r2)μ+1(((k+1)!)β+r2)μ+1(dkdk+1)kk!(1+r2)μ+1=((k(k1))1μ+1[((k+1)!)β+r2])μ+1(((k+1))3μ+1[(k!)β+r2])μ+1. (2.32)

    However, for all k2 and under the conditions imposed on the parameters, we have

    (k(k1))1μ+1[((k+1)!)β+r2]((k+1))3μ+1[(k!)β+r2](k(k1))1μ+1((k+1))3μ+1+(k(k1))1μ+1((k+1)!)β(k+1)3μ+1(k!)β=(k(k1))1μ+1+((k(k1))1μ+1(k!)β(k+1)β2(k+1)3μ+1)+(k!)β((k(k1))1μ+1(k+1)β2(k+1)3μ+1)(k(k1))1μ+1+(n+1)3μ+1((k(k1))1μ+1(k!)β(k+1)21)+(k!)β(k+1)3μ+1((k(k1))1μ+1(k+1)21)(k(k1))1μ+1+(k+1)3μ+1((k(k1))1μ+1(k!)β1)+(k!)β(k+1)3μ+1((k(k1))1μ+11)>0. (2.33)

    Hence, in view of (2.32) and (2.33) we conclude that the sequence (dk)k2 is decreasing. Therefore, by (2.31), we conclude

    |Qμ,β(r;z)1|<k2d2k(k1)=d2. (2.34)

    Moreover, since β1+3μ+1 and r(0,1], we get

    (r2+1r2+2β)μ+118,

    and consequently, for all zD, we obtain

    |Qμ,β(r;z)1|<1. (2.35)

    Finally, with the means of Lemma 1.6, we conclude that the function Qμ,β(r;z) is convex in D12.

    If we take β=2 in Theorem 2.15, in view of (1.4), the following result holds true:

    Corollary 2.25. Let 0<r1. If μ2, then the function Qμ(r;z) is convex in D12.

    If we let μ=1 in Theorem 2.15, in view of (1.5), we derive the following result:

    Corollary 2.26. Let 0<r1. If β52, then the function Q1,β(r;z) is convex in D12.

    Example 2.27. The functions Q2(r;z) and Q1,52(r;z) are convex in D12.

    In Figure 4, we present the mappings of these examples in D.

    Figure 4.  Mappings of Qμ,β(r;z) over D12.

    Remark 2.28. The geometric properties of the function Qμ(r;z) derived in Corollaries 2.16, 2.22 and 2.25 are new.

    In our present paper, we have derived sufficient conditions such that a class of functions associated to the generalized Mathieu type power series are to be starlike, close-to-convex and convex in the unit disk D. The various results, which we have established in this paper, are believed to be new, and their importance is illustrated by several interesting corollaries and examples. Furthermore, we are confident that our paper will inspire further investigation in this field and pave the way for some developments in the study of geometric functions theory involving certain classes of functions related to the Mathieu type powers series.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    The authors extend their appreciation to the Deanship of Scientific Research at Northern Border University, Arar, KSA for funding this research work through the project number "NBU-FFR-2023-0093".

    The authors declare that they have no conflicts of interest.



    [1] S. Kumar, H. Almusawa, I. Hamild, M. A. Abdou, Abundant closed-form solutions and solitonic structures to an integrable fifth-order generalized nonlinear evolution equation in plasma physics, Results Phys., 26 (2021), 104453. https://doi.org/10.1016/j.rinp.2021.104453 doi: 10.1016/j.rinp.2021.104453
    [2] X. Y. Gao, In plasma physics and fluid dynamics: Symbolic computation on a (2+1)-dimensional variable-coefficient Sawada-Kotera system, Appl. Math. Lett., 159 (2025), 109262. https://doi.org/10.1016/j.aml.2024.109262 doi: 10.1016/j.aml.2024.109262
    [3] G. X. Zhang, P. Huang, B. F. Feng, C. F. Wu, Rogue waves and their patterns in the vector nonlinear Schrödinger equation, J. Nonlinear Sci., 33 (2023), 116. https://doi.org/10.1007/s00332-023-09971-5 doi: 10.1007/s00332-023-09971-5
    [4] B. F. Feng, C. Y. Shi, G. X. Wu, C. F. Wu, Higher-order rogue wave solutions of the Sasa-Satsuma equation, J. Phys. A, 55 (2022), 235701. https://doi.org/10.1088/1751-8121/ac6917 doi: 10.1088/1751-8121/ac6917
    [5] M. A. Helal, Soliton solution of some nonlinear partial differential equations and its applications in fluid mechanics, Chaos Soliton. Fract., 13 (2002), 1917–1929. https://doi.org/10.1016/S0960-0779(01)00189-8 doi: 10.1016/S0960-0779(01)00189-8
    [6] X. Y. Gao, Auto-Bäcklund transformation with the solitons and similarity reductions for a generalized nonlinear shallow water wave equation, Qual. Theor. Dyn. Syst., 23 (2024), 181. https://doi.org/10.1007/s12346-024-01034-8 doi: 10.1007/s12346-024-01034-8
    [7] X. Y. Gao, Oceanic shallow-water investigations on a generalized Whitham-Broer-Kaup-Boussinesq-Kupershmidt system, Phys. Fluids, 35 (2023), 127106. https://doi.org/10.1063/5.0170506 doi: 10.1063/5.0170506
    [8] L. C. Zhao, C. Liu, Z. Y. Yang, The rogue waves with quintic nonlinearity and nonlineardispersion effects in nonlinear optical fibers, Commun. Nonlinear Sci., 20 (2015), 9–14. https://doi.org/10.1016/j.cnsns.2014.04.002 doi: 10.1016/j.cnsns.2014.04.002
    [9] M. Tlidi, K. Panajotov, Two-dimensional dissipative rogue waves due to time-delayed feedback in cavity nonlinear optics, Chaos, 27 (2017), 013119. https://doi.org/10.1063/1.4974852 doi: 10.1063/1.4974852
    [10] X. Y. Gao, Symbolic computation on a (2+1)-dimensional generalized nonlinear evolution system in fluid dynamics, plasma physics, nonlinear optics and quantum mechanics, Qual. Theor. Dyn. Syst., 23 (2024), 202. https://doi.org/10.1007/s12346-024-01045-5 doi: 10.1007/s12346-024-01045-5
    [11] Y. Shen, B. Tian, T. Y. Zhou, C. D. Cheng, Multi-pole solitons in an inhomogeneous multi-component nonlinear optical medium, Chaos Soliton. Fract., 171 (2023), 113497. https://doi.org/10.1016/j.chaos.2023.113497 doi: 10.1016/j.chaos.2023.113497
    [12] S. Burger, K. Bongs, S. Dettmer, W. Ertmer, K. Sengstock, Dark solitons in Bose-Einstein codensates, Phys. Rev. Lett., 83 (1999), 5198–5201. https://doi.org/10.1103/PhysRevLett.83.5198 doi: 10.1103/PhysRevLett.83.5198
    [13] V. E. Zakharov, S. V. Nazarenko, Dynamics of the Bose-Einstein condensation, Physica D, 201 (2005), 203–211. https://doi.org/10.1016/j.physd.2004.11.017 doi: 10.1016/j.physd.2004.11.017
    [14] M. Jaulent, I. Miodek, Nonlinear evolution equations associated with energy-dependent schrödinger potentials, Lett. Math. Phys., 1 (1976), 243–250. https://doi.org/10.1007/BF00417611 doi: 10.1007/BF00417611
    [15] G. A. El, R. H. J. Grimshaw, M. V. Pavlov, Integrable shallow-water equations and undular bores, Stud. Appl. Math., 106 (2001), 157–186. https://doi.org/10.1111/1467-9590.00163 doi: 10.1111/1467-9590.00163
    [16] G. B. Whitham, Linear and nonlinear waves, New York: John Wiley and Sons, 1974.
    [17] A. M. Kamchatnov, Whitham equation in the AKNS scheme, Phys. Lett. A, 186 (1994), 387–390. https://doi.org/10.1016/0375-9601(94)90699-8 doi: 10.1016/0375-9601(94)90699-8
    [18] G. A. El, V. V. Geogjaev, A. V. Gurevich, A. L. Krylov, Decay of an initial discontinuity in the defocusing NLS hydrodynamics, Physica D, 87 (1995), 186–192. https://doi.org/10.1016/0167-2789(95)00147-V doi: 10.1016/0167-2789(95)00147-V
    [19] Y. J. Kodama, V. U. Pierce, F. R. Tian, On the Whitham equations for the defocusing complex modified KdV equation, SIAM J. Math. Anal., 40 (2008), 1750–1782. https://doi.org/10.1137/070705131 doi: 10.1137/070705131
    [20] S. K. Ivanov, Riemann problem for the light pulses in optical fibers for the generalized Chen-Lee-Liu equation, Phys. Rev. A, 101 (2020), 053827. https://doi.org/10.1103/PhysRevA.101.053827 doi: 10.1103/PhysRevA.101.053827
    [21] T. J. Bridges, D. J. Ratliff, Nonlinear theory for coalescing characteristics in multiphase Whitham modulation theory, J. Nonlinear Sci., 31 (2021), 7. https://doi.org/10.1007/s00332-020-09669-y doi: 10.1007/s00332-020-09669-y
    [22] Y. Q. Liu, D. S. Wang, Exotic wave patterns in Riemann problem of the high-order Jaulent-Miodek equation: Whitham modulation theory, Stud. Appl. Math., 149 (2022), 588–630. https://doi.org/10.1111/sapm.12513 doi: 10.1111/sapm.12513
    [23] A. Abeya, G. Biondini, M. A Hoefer, Whitham modulation theory for the defocusing nonlinear Schrödinger equation in two and three spatial dimensions, J. Phys. A, 56 (2023), 025701. https://doi.org/10.1088/1751-8121/acb117 doi: 10.1088/1751-8121/acb117
    [24] Y. Q. Liu, S. J. Zeng, Discontinuous initial value and Whitham modulation for the generalized Gerdjikov-Ivanov equation, Wave Motion, 127 (2024), 103276. https://doi.org/10.1016/j.wavemoti.2024.103276 doi: 10.1016/j.wavemoti.2024.103276
    [25] J. B. Chen, Quasi-periodic solutions of the negative-order Jaulent-Miodek hierarchy, Rev. Math. Phys., 32 (2020), 2050007. https://doi.org/10.1142/S0129055X20500075 doi: 10.1142/S0129055X20500075
    [26] Y. Matsuno, Reduction of dispersionless coupled Korteweg-de Vries equations to the Euler-Darboux equation, J. Math. Phys., 42 (2001), 1744–1760. https://doi.org/10.1063/1.1345500 doi: 10.1063/1.1345500
    [27] R. G. Zhou, The finite-band solution of the Jaulent-Miodek equation, J. Math. Phys., 38 (1997), 2535–2546. https://doi.org/10.1063/1.531993 doi: 10.1063/1.531993
    [28] E. G. Fan, Uniformly constructing a series of explicit exact solutions to nonlinear equations in mathematical physics, Chaos Soliton. Fract., 13 (2003), 819–839. https://doi.org/10.1016/S0960-0779(02)00472-1 doi: 10.1016/S0960-0779(02)00472-1
    [29] A. M. Wazwaz, The tanh-coth and the sech methods for exact solutions of the Jaulent-Miodek equation, Phys. Lett. A, 366 (2007), 85–90. https://doi.org/10.1016/j.physleta.2007.02.011 doi: 10.1016/j.physleta.2007.02.011
    [30] M. S. Iqbal, A. R. Seadawy, M. Z. Baber, M. Qasim, Application of modified exponential rational method to Jaulent-Miodek system leading to exact classical solutions, Chaos Soliton. Fract., 164 (2022), 112600. https://doi.org/10.1016/j.chaos.2022.112600 doi: 10.1016/j.chaos.2022.112600
    [31] H. Wang, T. C. Xia, Super Jaulent-Miodek hierarchy and its super Hamiltonian structure, conservation laws and its self-consistent sources, Front. Math. China, 9 (2014), 1367–1379. https://doi.org/10.1007/s11464-014-0419-x doi: 10.1007/s11464-014-0419-x
    [32] S. Alshammari, M. M. Al-Sawalha, R. Shah, Approximate analytical methods for a fractional-order nonlinear system of Jaulent-Miodek equation with energy-dependent Schrödinger potential, Fractal Fract., 7 (2023), 140. https://doi.org/10.3390/fractalfract7020140 doi: 10.3390/fractalfract7020140
    [33] R. Ivanov, Two-component integrable systems modelling shallow water waves: The constant vorticity case, Wave Motion, 46 (2009), 389–396. https://doi.org/10.1016/j.wavemoti.2009.06.012 doi: 10.1016/j.wavemoti.2009.06.012
    [34] D. Duthkh, Effects of vorticity on the travelling waves of some shallow water two-component systems, Discrete Contin. Dyn. Syst., 39 (2019), 5521–5541. https://doi.org/10.3934/dcds.2019225 doi: 10.3934/dcds.2019225
    [35] H. Flaschka, M. G. Forest, D. W. McLaughlin, Multiphase averaging and the inverse spectral solution of the Korteweg-de Vries equation, Pure Appl. Math., 33 (1980), 739–784. https://doi.org/10.1002/cpa.3160330605 doi: 10.1002/cpa.3160330605
    [36] A. B. Monnel, I. Egorova, The Toda lattice with step-like initial data. Soliton asymptotics, Inverse Probl., 16 (2000), 955–977. https://doi.org/10.1088/0266-5611/16/4/306 doi: 10.1088/0266-5611/16/4/306
    [37] Z. Y. Wang, K. Xu, E. G. Fan, The complex MKDV equation with step-like initial data: Large time asymptotic analysis, J. Math. Phys., 64 (2023), 103504. https://doi.org/10.1063/5.0131306 doi: 10.1063/5.0131306
    [38] L. Lei, S. F. Tian, Y. Q. Wu, Multi-soliton solutions for the nonlocal Kundu-nonlinear Schrödinger equation with step-like initial data, J. Nonlinear Math. Phys., 30 (2023), 1661–1679. https://doi.org/10.1007/s44198-023-00149-x doi: 10.1007/s44198-023-00149-x
    [39] A. S. Alshehry, H. Yasmin, R. Shah, A. Ali, I. Khan, Fractional-order view analysis of Fisher's and foam drainage equations within Aboodh transform, Eng. Computation., 41 (2024), 489–515. https://doi.org/10.1108/EC-08-2023-0475 doi: 10.1108/EC-08-2023-0475
    [40] H. Yasmin, A. S. Alshehry, A. H. Ganie, A. M. Mahnashi, Perturbed Gerdjikov-Ivanov equation: Soliton solutions via Bäcklund transformation, Optik, 298 (2024), 171576. https://doi.org/10.1016/j.ijleo.2023.171576 doi: 10.1016/j.ijleo.2023.171576
    [41] A. S. Alshehry, H. Yasmin, M. A. Shah, R. Shah, Analyzing fuzzy fractional Degasperis-Procesi and Camassa-Holm equations with the Atangana-Baleanu operator, Open Phys., 22 (2024), 20230191. https://doi.org/10.1515/phys-2023-0191 doi: 10.1515/phys-2023-0191
  • Reader Comments
  • © 2024 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(492) PDF downloads(32) Cited by(1)

Figures and Tables

Figures(9)

Other Articles By Authors

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog