
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,γ2∈R,ε≠0,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={→A∈D3|‖→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
A−1=1γ1−εγ2γ21,γ1≠0 |
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 AB−1 where B is not a pure dual number and B≠0. The set given by
D3={→A=→γ1+ε→γ2|→γ1,→γ2∈R3} |
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=cosϕ−εϕ∗sinϕ, |
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‖+ε⟨→γ1,→γ2⟩‖→γ1‖. | (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=Fn−1+Fn−2;F0=0,F1=1, |
Ln=Ln−1+Ln−2;L0=2,L1=1. |
The characteristic equation of recurrences Fn and Ln is given by x2−x−1=0. The Binet formulas for the Fn and Ln sequences are respectively given by
Fn=φn−ψnφ−ψandLn=φn+ψn, |
where φ=1+√52 and ψ=1−√52 are the roots of the characteristic equation. The following identities are hold for Fibonacci and Lucas number sequences
Ln=Fn−1+Fn+1andLn−1+Ln+1=5Fn. | (1.2) |
The Leonardo number sequence [17,18,19,20,21,22,23,24] is defined as follows
Len=Len−1+Len−2+1 |
with the initial condition the Le0=Le1=1. The Leonardo numbers are related to the Fibonacci numbers through the below relation:
Len=2Fn+1−1. |
This Binet's formula for the Leonardo number sequence is given by
Len=2φn+1−2ψn+1φ−ψ−1, | (1.3) |
where φ=1+√52 and ψ=1−√52 are roots of the characteristic equation x3−2x2+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 ε≠0. The following recurrence relation can be obtained directly by using the definition of dual Leonardo numbers
Ln=Ln−1+Ln−2+L0,n≥2, |
where L0=1+ε,L1=1+3ε.
Theorem 1. The Binet formula for dual Leonardo numbers is given by
Ln=2φ_φn+1−2ψ_ψn+1φ−ψ−L0, | (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+1−2ψn+1φ−ψ−1+ε(2φn+2−2ψn+2φ−ψ−1)=2φ_φn+1−2ψ_ψn+1φ−ψ−(1+ε)=2φ_φn+1−2ψ_ψn+1φ−ψ−L0. |
For the next proof we have taken into account the following equalities:
φψ=−1,φ+ψ=1and(φrψ−r+φ−rψr−2)(φ−ψ)2=(−1)−r(φr−ψrφ−ψ)2. | (2.3) |
Theorem 2. (Catalan's identity) For any integers n and r such that n≥r, we have
Ln+rLn−r−L2n=(−1)n−r(Ler−1+1)2L0−(Ln+r+Ln−r−2Ln)L0. |
Proof. Using (1.2), (1.3), (2.3) and the Binet formula for dual Leonardo numbers in (2.2), we get
Ln+rLn−r−L2n=(2φ_φn+r+1−2ψ_ψn+r+1φ−ψ−L0)(2φ_φn−r+1−2ψ_ψn−r+1φ−ψ−L0)−(2φ_φn+1−2ψ_ψn+1φ−ψ−L0)2=4(φ−ψ)2φ_ψ_(−1)n(φrψ−r+φ−rψr−2)−2φ_φn+r+1−2ψ_ψn+r+1φ−ψL0−2φ_φn−r+1−2ψ_ψn−r+1φ−ψL0+4ψ_ψn+1−4φ_φn+1φ−ψL0=L0(−1)n−r(2φr−2ψrφ−ψ)2−(Ln+r+Ln−r−2Ln)L0=(−1)n−r(Ler−1+1)2L0−(Ln+r+Ln−r−2Ln)L0. |
Corollary 1. (Cassini's identity) For any integer n and n≥1, the following identity holds:
Ln+1Ln−1−L2n=4(−1)n−1L0−(Ln+1+Ln−1−2Ln)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+1Ln−LmLn+1=L0(Ln−1−Lm−1)+2(−1)mL0(Len−m−1+1). |
Proof. Using (2.2) and (2.3), we will have
Lm+1Ln−LmLn+1=(2φ_φm+2−2ψ_ψm+2φ−ψ−L0)(2φ_φn+1−2ψ_ψn+1φ−ψ−L0)−(2φ_φm+1−2ψ_ψm+1φ−ψ−L0)(2φ_φn+2−2ψ_ψn+2φ−ψ−L0)=4(φ−ψ)2φ_ψ_(φm+1ψn+2−φm+2ψn+1+φn+2ψm+1−φn+1ψm+2)+2L0(φ−ψ)(φ_φn+2−ψ_ψn+2+φ_φm+1−ψ_ψm+1−φ_φm+2+ψ_ψm+2−φ_φn+1+ψ_ψn+1). |
By taking (1.3), we get
Lm+1Ln−LmLn+1=L0(Ln−1−Lm−1)+2(−1)mL0(Len−m−1+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+ε→Len+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+2−1)(1−Len+3). |
Proof. From (1.1), (1.3) and (3.1), we get
‖→Len‖2=Le2n+Le2n+1+Le2n+2=(2φn+1−ψn+1φ−ψ−1)2+(2φn+2−ψn+2φ−ψ−1)2+(2φn+3−ψn+3φ−ψ−1)2=4(φ−ψ)2(φ2n+2+ψ2n+2+φ2n+4+ψ2n+4+φ2n+6+ψn+6+2(−1)n)−2(2φn+1−2ψn+1φ−ψ−1+2φn+2−2ψn+2φ−ψ−1+2φn+3−2ψn+3φ−ψ−1+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+2−1)−3=√2(Le2n+2+1)+(Len+2+1)2−4Fn+2−1=√2Le2n+2+Le2n+2−2Len+2+2. |
On the other hand
⟨→Len,→Len+1⟩=LenLen+1+Len+1Len+2+Len+2Len+3=4(φ−ψ)2(φ2n+3+ψ2n+3−φn+1ψn+2−φn+2ψn+1)−2φ−ψ(φn+1−ψn+1+φn+2−ψn+2)+1+4(φ−ψ)2(φ2n+3+ψ2n+3−φn+1ψn+2−φn+2ψn+1)−2φ−ψ(φn+1−ψn+1+φn+2−ψn+2)+1+4(φ−ψ)2(φ2n+3+ψ2n+3−φn+1ψn+2−φn+2ψn+1)−2φ−ψ(φn+1−ψn+1+φn+2−ψn+2)+1. |
Using (2.3) and performing necessary calculations, we obtain
⟨→Len,→Len+1⟩=2Le2n+3+(Len+2−1)(Len+3−1)+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+2−L0)(Lm+2−L0)+2ε(Ln+m+3+L0)+1,→Ln×→Lm=2(−1)m(Len−m−1(1+ε)+1)(→e1−→e2−→e3)+(Ln−Lm+ε(Len−Lem))→e1+(Ln+1−Lm+1)→e2+(Ln−1−Lm−1+ε(Len−1−Lem−1))→e3. |
Proof. Using (1.3), (2.2) and (2.3), we obtain
⟨→Len,→Lem⟩=LenLem+Len+1Lem+1+Len+2Lem+2=(2φn+1−2ψn+1φ−ψ−1)(2φm+1−2ψm+1φ−ψ−1)+(2φn+2−2ψn+2φ−ψ−1)(2φm+2−2ψm+2φ−ψ−1)+(2φn+3−2ψn+3φ−ψ−1)(2φm+3−2ψm+3φ−ψ−1)=2(Len+m+2−Len+2−Lem+2)+(Len+2+1)(Lem+2)+1=2Len+m+2+(Len+2−1)(Lem+2−1)+1, |
and by using the properties of determinants, we get
→Len×→Lem=|→e1→e2→e3LenLen+1Len+2LemLem+1Lem+2|=(Len+1Lem+2−Len+2Lem+1)→e1−(LenLem+2−Len+2Lem)→e2+(LenLem+1−Len+1Lem)→e3=2(−1)m(Len−m−1+1)(→e1−→e2−→e3)+(Len−Lem)→e1+(Len+1−Lem+1)→e2+(Len−1−Lem−1)→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+2−1)(Len+2−1)+1+ε(−Len+4−Lem+4+4Len+m+3+Len+2Lem+3+Len+3Lem+2+6)=2Len+m+2+(Lem+2−1)(Len+2−1)+1+ε(4Len+m+3+(Lem+3−1)(Len+2−1)+(Lem+2−1)(Len+3−1)+2)=2Lm+n+2+(Lem+2−1)(Ln+2−L0)+ε(2Lem+n+3+Lem+3Len+2−Lem+3−Len+2+3)+1=2Lem+n+2+(Ln+2−L0)(Lem+2−1+εLen+3−ε)+2ε(Len+m+3+1)+1=2Lm+n+2+(Ln+2−L0)(Lm+2−L0)+2ε(Ln+m+3+L0)+1, |
and
→Ln×→Lm=→Len×→Lem+ε(→Len×→Lem+1+→Len+1×→Lem)=2(−1)m(Len−m−1(1+ε)+1)(→e1−→e2−→e3)+(Ln−Lm+ε(Len−Lem))→e1+(Ln+1−Lm+1)→e2+(Ln−1−Lm−1+ε(Len−1−Lem−1))→e3. |
Proposition 3. Let →A=→γ1+ε→γ2 be a unit dual vector in D3; then the directed line that corresponds to →A has an equation of the form
→x=→γ1×→γ2+μ→γ1, |
where 0≤μ≤1.
Proof. Let →A=→γ1+ε→γ2 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+λ→γ1, |
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,→t⟩→γ1, |
and
→x=→γ1×→γ2+⟨→γ1,→t⟩→γ1+λ→γ1. |
By taking μ=⟨→γ1,→t⟩ +λ, we get the result as follows
→x=→γ1×→γ2+μ→γ1. |
Theorem 6. Suppose that →L0n is a dual Leonardo vector and let →Ln=→Len+ε→Len+1 be its unitized vector, that is →Ln∈S2; then, the equation for the corresponding line is given by
→xn=(2(−1)n+1(Len−2+1)+μLen−Len−1−1)→e1+(2(−1)n(Len−2+1)+μLen+1−Len−1)→e2+(2(−1)n(Len−2+1)+μLen+2+Len−3+1)→e3. |
Proof. By using (1.3) and Proposition (3), we obtain
→xn=→Len×→Len+1+μ→Len,=[→e1→e2→e3LenLen+1Len+2Len+1Len+2Len+3]+μ(Len→e1+Len+1→e2+Len+2→e3)=(2(−1)n+1(Len−2+1)+μLen−Len−1−1)→e1+(2(−1)n(Len−2+1)+μLen+1−Len−1)→e2+(2(−1)n(Len−2+1)+μLen+2+Len−3+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+2−1)(Len+2−1)+1+ε[−Len+4−Lem+4+4Len+m+3+Len+2Lem+3+Len+3Lem+2+6]=cosϕ−εϕ∗sinϕ. |
The following cases can be given for a dual angle Φ satisfying that cosΦ=cosϕ−εϕ∗sinϕ, as wellas the conditions for the corresponding lines l1 and l2.
Case 1. Assume that ϕ=π2 and ϕ∗≠0; then,
(1−Len+2)(Lem+2−1)=1+2Len+m+2 |
and
ϕ∗=Len+4+Lem+4−4Len+m+3−Len+2Lem+3−Len+3Lem+2−6. |
Additionally the corresponding lines l1 and l2 are perpendicular such that not intersect each other (see Figure 2).
Case 2. Assume that ϕ∗=0 and ϕ≠0; then, we obtain
ϕ=arccos(2Len+m+2+(Len+2−1)(Lem+2−1)+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).
Case 3. Assume that ϕ=π2 and ϕ∗=0; then,
(1−Len+2)(Lem+2−1)=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).
Case 4. Assume that ϕ=0 and ϕ∗≠0; then,
2Len+m+2=(1−Len+2)(Lem+2−1) |
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).
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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1. | Ali Atasoy, A New Polar Representation and Identities for Split Leonardo Quaternions, 2025, 0170-4214, 10.1002/mma.10830 |