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A new approach to Leonardo number sequences with the dual vector and dual angle representation

  • In this paper, we introduce dual numbers with components including Leonardo number sequences. This novel approach facilitates our understanding of dual numbers and properties of Leonardo sequences. We also investigate fundamental properties and identities associated with Leonardo number sequences, such as Binet's formula and Catalan's, Cassini's and D'ocagne's identities. Furthermore, we also introduce a dual vector with components including Leonardo number sequences and dual angles. This extension not only deepens our understanding of dual numbers, it also highlights the interconnectedness between numerical sequences and geometric concepts. In the future it would be valuable to replicate a similar exploration and development of our findings on dual numbers with Leonardo number sequences.

    Citation: Faik Babadağ, Ali Atasoy. A new approach to Leonardo number sequences with the dual vector and dual angle representation[J]. AIMS Mathematics, 2024, 9(6): 14062-14074. doi: 10.3934/math.2024684

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  • In this paper, we introduce dual numbers with components including Leonardo number sequences. This novel approach facilitates our understanding of dual numbers and properties of Leonardo sequences. We also investigate fundamental properties and identities associated with Leonardo number sequences, such as Binet's formula and Catalan's, Cassini's and D'ocagne's identities. Furthermore, we also introduce a dual vector with components including Leonardo number sequences and dual angles. This extension not only deepens our understanding of dual numbers, it also highlights the interconnectedness between numerical sequences and geometric concepts. In the future it would be valuable to replicate a similar exploration and development of our findings on dual numbers with Leonardo number sequences.



    The concept of dual numbers [1], which is an extension of real numbers, was initially introduced by Clifford in 1873. It is defined as follows:

    D={A=γ1+εγ2|γ1,γ2R,ε0,ε2=0}.

    These numbers form a commutative and associative algebra over the real numbers. Kotelnikov was the first to explore the practical applications of dual numbers, laying the groundwork for their utilization in various fields [2]. Notably, Study incorporated dual numbers and associated vectors into line geometry and kinematics, pioneering their use in these domains [3]. In the context of vectors, the set of dual vectors can be represented as D3, indicating all possible combinations of dual number pairs. Additionally, the collection of all unit dual vectors forms what is known as the unit dual sphere, denoted by

    S2={AD3|A=1},

    which plays a significant role in geometric interpretations and calculations involving dual vectors. This rich framework of dual numbers and vectors offers a versatile toolset for mathematical and geometric analyses, with applications ranging from kinematics to computer graphics and beyond.

    Study proved that there exists an isomorphism between the points of the dual unit sphere in D3 and the directed lines of Euclidean 3-space, which is known as Study mapping[3]. Dual numbers have been applied in most fields including research on rigid body motion, displacement analysis of spatial mechanisms, surface shape analysis and computer graphics, kinematic synthesis, human body motion analysis, and others [4,5,6,7,8,9,10].

    The algebra of dual numbers is represented by a ring with the following addition and multiplication operations:

    (γ1+εγ2)+(δ1+εδ2)=(γ1+δ1)+ε(γ2+δ2),
    (γ1+εγ2)(δ1+εδ2)=γ1δ1+ε(γ1δ2+γ2δ1).

    The multiplicative inverse of A=γ1+εγ2 is given by

    A1=1γ1εγ2γ21,γ10

    and there is no inverse for pure dual numbers; hence, this algebra of numbers is not a field over real numbers. By using the inverse of dual numbers we can define the division operation of two dual numbers A and B as AB1 where B is not a pure dual number and B0. The set given by

    D3={A=γ1+εγ2|γ1,γ2R3}

    is amodule over the ring of dual numbers D, the elements of this module are called dual vectors.

    Proposition 1. Let A and B be dual vectors; then, their scalar and cross products are respectively given by

    A,B=γ1,δ1+ε(γ1,δ2+γ2,δ1),A×B=γ1×δ1+ε(γ1×δ2+γ2×δ1).

    If A and B are unit dual vectors then

    A,B=cosΦ=cosϕεϕsinϕ,

    where Φ=ϕ+εϕ is a dual angle between them[1].

    Proposition 2. The norm of the dual vector A is given by

    A=γ1+εγ1,γ2γ1. (1.1)

    If A is a unit dual vector, then γ1=1 and γ1,γ2=0 [1].

    Sequences of integers hold an important place in mathematical literature with many famous sequences playing crucial roles across various branches of mathematics. These sequences often arise naturally in mathematical investigations and have been extensively studied due to their properties and profound connections to different areas of mathematics.

    The Fibonacci and Lucas number sequences [11,12,13,14,15,16] are defined by

    Fn=Fn1+Fn2;F0=0,F1=1,
    Ln=Ln1+Ln2;L0=2,L1=1.

    The characteristic equation of recurrences Fn and Ln is given by x2x1=0. The Binet formulas for the Fn and Ln sequences are respectively given by

    Fn=φnψnφψandLn=φn+ψn,

    where φ=1+52 and ψ=152 are the roots of the characteristic equation. The following identities are hold for Fibonacci and Lucas number sequences

    Ln=Fn1+Fn+1andLn1+Ln+1=5Fn. (1.2)

    The Leonardo number sequence [17,18,19,20,21,22,23,24] is defined as follows

    Len=Len1+Len2+1

    with the initial condition the Le0=Le1=1. The Leonardo numbers are related to the Fibonacci numbers through the below relation:

    Len=2Fn+11.

    This Binet's formula for the Leonardo number sequence is given by

    Len=2φn+12ψn+1φψ1, (1.3)

    where φ=1+52 and ψ=152 are roots of the characteristic equation x32x2+1=0 and the other root of this equation is λ=1.

    Here, our goal was to study this a new number system that can by generated by using dual numbers and well known Leonardo numbers as dual Leonardo number sequences and we describe dual Leonardo vectors and angles to apply these dual vectors and angles in the geometry of dual space.

    In this section, we demonstrate dual Leonardo number sequences, presenting their fundamental identities and properties. Some fundamental properties and identities of these number sequences are discussed, such as Binet's formula, Catalan's, Cassini's and D'ocagne's identities. These identities play crucial roles in obtaining on understanding of the properties of dual Leonardo number sequences, and we aim to establish and prove them by using Binet's formulas.

    The dual Leonardo number is defined by the following relation:

    Ln=Len+εLen+1, (2.1)

    where Len is the Leonardo number, ε2=0 and ε0. The following recurrence relation can be obtained directly by using the definition of dual Leonardo numbers

    Ln=Ln1+Ln2+L0,n2,

    where L0=1+ε,L1=1+3ε.

    Theorem 1. The Binet formula for dual Leonardo numbers is given by

    Ln=2φ_φn+12ψ_ψn+1φψL0, (2.2)

    where φ_=1+εφ, ψ_=1+εψ and φ_ψ_=1+ε=L0.

    Proof. From (1.3) and (2.1), we find that

    Ln=Len+εLen+1=2φn+12ψn+1φψ1+ε(2φn+22ψn+2φψ1)=2φ_φn+12ψ_ψn+1φψ(1+ε)=2φ_φn+12ψ_ψn+1φψL0.

    For the next proof we have taken into account the following equalities:

    φψ=1,φ+ψ=1and(φrψr+φrψr2)(φψ)2=(1)r(φrψrφψ)2. (2.3)

    Theorem 2. (Catalan's identity) For any integers n and r such that nr, we have

    Ln+rLnrL2n=(1)nr(Ler1+1)2L0(Ln+r+Lnr2Ln)L0.

    Proof. Using (1.2), (1.3), (2.3) and the Binet formula for dual Leonardo numbers in (2.2), we get

    Ln+rLnrL2n=(2φ_φn+r+12ψ_ψn+r+1φψL0)(2φ_φnr+12ψ_ψnr+1φψL0)(2φ_φn+12ψ_ψn+1φψL0)2=4(φψ)2φ_ψ_(1)n(φrψr+φrψr2)2φ_φn+r+12ψ_ψn+r+1φψL02φ_φnr+12ψ_ψnr+1φψL0+4ψ_ψn+14φ_φn+1φψL0=L0(1)nr(2φr2ψrφψ)2(Ln+r+Lnr2Ln)L0=(1)nr(Ler1+1)2L0(Ln+r+Lnr2Ln)L0.

    Corollary 1. (Cassini's identity) For any integer n and n1, the following identity holds:

    Ln+1Ln1L2n=4(1)n1L0(Ln+1+Ln12Ln)L0.

    Proof. This identity can be obtained from Catalan's identity by taking r=1.

    Theorem 3. (D'ocagne's identity) For any integers m and n, we have

    Lm+1LnLmLn+1=L0(Ln1Lm1)+2(1)mL0(Lenm1+1).

    Proof. Using (2.2) and (2.3), we will have

    Lm+1LnLmLn+1=(2φ_φm+22ψ_ψm+2φψL0)(2φ_φn+12ψ_ψn+1φψL0)(2φ_φm+12ψ_ψm+1φψL0)(2φ_φn+22ψ_ψn+2φψL0)=4(φψ)2φ_ψ_(φm+1ψn+2φm+2ψn+1+φn+2ψm+1φn+1ψm+2)+2L0(φψ)(φ_φn+2ψ_ψn+2+φ_φm+1ψ_ψm+1φ_φm+2+ψ_ψm+2φ_φn+1+ψ_ψn+1).

    By taking (1.3), we get

    Lm+1LnLmLn+1=L0(Ln1Lm1)+2(1)mL0(Lenm1+1).

    The proof is completed.

    In this section we introduce the dual Leonardo vector Ln and dual angle Φ, respectively. Moreover, we will give the main identities for this vector.

    Definition 1. The dual Leonardo vector Ln in D3 is defined by

    Ln=Len+εLen+1, (3.1)

    where Len=(Len,Len+1,Len+2) and Len+1=(Len+1,Len+2,Len+3) are real vectors.

    Theorem 4. If Ln is a unit dual vector, then

    2Len+1=2Le2n+2+Le2n+1+1,

    and

    2Le2n+3+1=(Len+21)(1Len+3).

    Proof. From (1.1), (1.3) and (3.1), we get

    Len2=Le2n+Le2n+1+Le2n+2=(2φn+1ψn+1φψ1)2+(2φn+2ψn+2φψ1)2+(2φn+3ψn+3φψ1)2=4(φψ)2(φ2n+2+ψ2n+2+φ2n+4+ψ2n+4+φ2n+6+ψn+6+2(1)n)2(2φn+12ψn+1φψ1+2φn+22ψn+2φψ1+2φn+32ψn+3φψ1+3)+3=45(L2n+2+L2n+4+L2n+6+2(1)n)2(Len+Len+1+Len+2)3.

    Using (1.2) and (1.3), we have

    Len=45(5F2n+3+5F2n+3)2(2Len+21)3=2(Le2n+2+1)+(Len+2+1)24Fn+21=2Le2n+2+Le2n+22Len+2+2.

    On the other hand

    Len,Len+1=LenLen+1+Len+1Len+2+Len+2Len+3=4(φψ)2(φ2n+3+ψ2n+3φn+1ψn+2φn+2ψn+1)2φψ(φn+1ψn+1+φn+2ψn+2)+1+4(φψ)2(φ2n+3+ψ2n+3φn+1ψn+2φn+2ψn+1)2φψ(φn+1ψn+1+φn+2ψn+2)+1+4(φψ)2(φ2n+3+ψ2n+3φn+1ψn+2φn+2ψn+1)2φψ(φn+1ψn+1+φn+2ψn+2)+1.

    Using (2.3) and performing necessary calculations, we obtain

    Len,Len+1=2Le2n+3+(Len+21)(Len+31)+1.

    Then, by using (1.1), the proof is completed.

    Theorem 5. For dual Leonardo vectors Ln and Lm, we have

    Ln,Lm=2Lm+n+2+(Ln+2L0)(Lm+2L0)+2ε(Ln+m+3+L0)+1,Ln×Lm=2(1)m(Lenm1(1+ε)+1)(e1e2e3)+(LnLm+ε(LenLem))e1+(Ln+1Lm+1)e2+(Ln1Lm1+ε(Len1Lem1))e3.

    Proof. Using (1.3), (2.2) and (2.3), we obtain

    Len,Lem=LenLem+Len+1Lem+1+Len+2Lem+2=(2φn+12ψn+1φψ1)(2φm+12ψm+1φψ1)+(2φn+22ψn+2φψ1)(2φm+22ψm+2φψ1)+(2φn+32ψn+3φψ1)(2φm+32ψm+3φψ1)=2(Len+m+2Len+2Lem+2)+(Len+2+1)(Lem+2)+1=2Len+m+2+(Len+21)(Lem+21)+1,

    and by using the properties of determinants, we get

    Len×Lem=|e1e2e3LenLen+1Len+2LemLem+1Lem+2|=(Len+1Lem+2Len+2Lem+1)e1(LenLem+2Len+2Lem)e2+(LenLem+1Len+1Lem)e3=2(1)m(Lenm1+1)(e1e2e3)+(LenLem)e1+(Len+1Lem+1)e2+(Len1Lem1)e3,

    where e1,e2,e3 are unit direction vectors. By Proposition (1) and the above calculations we have

    Ln,Lm=Len,Lem+ε(Len,Lem+1+Len+1,Lem)=2Len+m+2+(Lem+21)(Len+21)+1+ε(Len+4Lem+4+4Len+m+3+Len+2Lem+3+Len+3Lem+2+6)=2Len+m+2+(Lem+21)(Len+21)+1+ε(4Len+m+3+(Lem+31)(Len+21)+(Lem+21)(Len+31)+2)=2Lm+n+2+(Lem+21)(Ln+2L0)+ε(2Lem+n+3+Lem+3Len+2Lem+3Len+2+3)+1=2Lem+n+2+(Ln+2L0)(Lem+21+εLen+3ε)+2ε(Len+m+3+1)+1=2Lm+n+2+(Ln+2L0)(Lm+2L0)+2ε(Ln+m+3+L0)+1,

    and

    Ln×Lm=Len×Lem+ε(Len×Lem+1+Len+1×Lem)=2(1)m(Lenm1(1+ε)+1)(e1e2e3)+(LnLm+ε(LenLem))e1+(Ln+1Lm+1)e2+(Ln1Lm1+ε(Len1Lem1))e3.

    Proposition 3. Let A=γ1+εγ2 be a unit dual vector in D3; then the directed line that corresponds to A has an equation of the form

    x=γ1×γ2+μγ1,

    where 0μ1.

    Proof. Let A=γ1+εγ2 be the unit dual vector and if T and X are points on the corresponding line d and O is the origin (see Figure 1), then

    OX=OT+TX,x=t+λγ1,

    where λ is a real parameter. A point X is on the line of vectors γ1 and γ2 if and only if

    γ1×γ2=γ1×(t×γ1).

    Then,

    t=γ1×γ2+γ1,tγ1,

    and

    x=γ1×γ2+γ1,tγ1+λγ1.

    By taking μ=γ1,t +λ, we get the result as follows

    x=γ1×γ2+μγ1.
    Figure 1.  E. Study mapping.

    Theorem 6. Suppose that L0n is a dual Leonardo vector and let Ln=Len+εLen+1 be its unitized vector, that is LnS2; then, the equation for the corresponding line is given by

    xn=(2(1)n+1(Len2+1)+μLenLen11)e1+(2(1)n(Len2+1)+μLen+1Len1)e2+(2(1)n(Len2+1)+μLen+2+Len3+1)e3.

    Proof. By using (1.3) and Proposition (3), we obtain

    xn=Len×Len+1+μLen,=[e1e2e3LenLen+1Len+2Len+1Len+2Len+3]+μ(Lene1+Len+1e2+Len+2e3)=(2(1)n+1(Len2+1)+μLenLen11)e1+(2(1)n(Len2+1)+μLen+1Len1)e2+(2(1)n(Len2+1)+μLen+2+Len3+1)e3.

    The dual number Φ=ϕ+εϕ was defined by E. Study in 1903 as a dual angle, where ϕ is the angle between oriented lines l1 and l2 in R3 and ϕ is the vertical distance between these lines [3].

    Corollary 2. For unit vectors Ln and Lm, we have

    Ln,Lm=2Len+m+2+(Lem+21)(Len+21)+1+ε[Len+4Lem+4+4Len+m+3+Len+2Lem+3+Len+3Lem+2+6]=cosϕεϕsinϕ.

    The following cases can be given for a dual angle Φ satisfying that cosΦ=cosϕεϕsinϕ, as wellas the conditions for the corresponding lines l1 and l2.

    Case 1. Assume that ϕ=π2 and ϕ0; then,

    (1Len+2)(Lem+21)=1+2Len+m+2

    and

    ϕ=Len+4+Lem+44Len+m+3Len+2Lem+3Len+3Lem+26.

    Additionally the corresponding lines l1 and l2 are perpendicular such that not intersect each other (see Figure 2).

    Figure 2.  Geometric representation of a dual angle between the directed lines l1 and l2.

    Case 2. Assume that ϕ=0 and ϕ0; then, we obtain

    ϕ=arccos(2Len+m+2+(Len+21)(Lem+21)+1)

    and

    4Len+m+3+Len+2Lem+3+Len+3Lem+2+6=Len+4+Lem+4,

    in this case lines l1 and l2 intersect each other (see Figure 3).

    Figure 3.  Intersection of lines.

    Case 3. Assume that ϕ=π2 and ϕ=0; then,

    (1Len+2)(Lem+21)=1+2Len+m+2

    and

    4Len+m+3+Len+2Lem+3+Len+3Lem+2+6=Len+4+Lem+4,

    in this case lines l1 and l2 intersect each other at a right angle (see Figure 4).

    Figure 4.  Perpendicular intersection of lines.

    Case 4. Assume that ϕ=0 and ϕ0; then,

    2Len+m+2=(1Len+2)(Lem+21)

    and

    4Len+m+3+Len+2Lem+3+Len+3Lem+2+6=Len+4+Lem+4,

    in this case corresponding lines l1 and l2 are parallel (see Figure 5).

    Figure 5.  The lines are parallel.

    In this paper, we have introduced the concept of dual Leonardo number sequences and derived the fundamental identities associated with them. Then, we introduced the notion of dual Leonardo vectors and investigated their scalar and cross products. Additionally, we have provided the properties of dual Leonardo vectors, including Study mapping and relationship with dual angles. These findings provide valuable insights into the interference between dual Leonardo number sequences, vectors and geometric concepts within the framework of dual space. Moreover, our explanation of the fundamental identities and properties opens the door further research on the geometry of dual space.

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

    The authors declare no conflicts of interest.



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