
In this study, we introduce partner ruled surfaces according to the Flc frame that is defined on a polynomial curve. First, the conditions of each couple of two partner ruled surfaces to be simultaneously developable and minimal are investigated. Then, the asymptotic, geodesic and curvature lines of the parameter curves of the partner ruled surfaces are simultaneously characterized. Finally, the examples of the partner ruled surfaces are given, and their graphs are drawn.
Citation: Yanlin Li, Kemal Eren, Kebire Hilal Ayvacı, Soley Ersoy. Simultaneous characterizations of partner ruled surfaces using Flc frame[J]. AIMS Mathematics, 2022, 7(11): 20213-20229. doi: 10.3934/math.20221106
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In this study, we introduce partner ruled surfaces according to the Flc frame that is defined on a polynomial curve. First, the conditions of each couple of two partner ruled surfaces to be simultaneously developable and minimal are investigated. Then, the asymptotic, geodesic and curvature lines of the parameter curves of the partner ruled surfaces are simultaneously characterized. Finally, the examples of the partner ruled surfaces are given, and their graphs are drawn.
Surface theory is an attractive research field, as it has applications in many disciplines. Among the surfaces, the ruled surfaces are the most interesting and were first introduced by G. Monge. The ruled surfaces are formed by moving a line along a curve, where this curve is called the base curve, and the straight line is called the generator line. Since it consists of an infinite number of straight lines, it is known as a surface of lines. That is, the ruled surfaces are surfaces created by families of straight lines. The importance of the theory of ruled surfaces in some engineering fields is evident. Especially, in kinematics and computer-aided design problems, these surfaces have widespread use. Cylinder and cone surfaces are the most well-known ruled surfaces. The ruled surfaces also arise in admirable architectural works. For example, the ruled surfaces are seen in many famous structures, such as Ciechanow Water Tower, Kobe Port Tower and Shuckhov Tower. In addition to the visibility of ruled surfaces in real-world applications, theoretical developments for these surfaces continue in depth. After its localization in the scientific literature, researchers started to question the characterizations of these surfaces as well as the isoparametric curves lying on them. For example, the relations between the cylindrical helix and Gaussian curvature and between the Bertrand curve and the mean curvature of a ruled surface were given in [1]. The invariants and kinematic/ geometric properties of non-developable ruled surfaces were examined by considering the structural functions of ruled surfaces in [2]. The ruled surfaces with directrix of a focal curve of a given curve were studied and characterized in [3]. Developable ruled surfaces on Bezier curves were constructed in [4]. Normal and binormal ruled surfaces based on W-direction curves were discussed in [5].
Motivated by these, in this study, we have introduced partner ruled surfaces based on a polynomial curve and ruled by the vector elements of a Frenet-like frame known as the Flc frame [6]. Then, we have simultaneously provided the conditions for each partner ruled surface to be developable or minimal by considering the main curvatures with the Flc frame invariants. Such conditions have also been linked to the characterizations of isoparametric curves such as asymptotic, geodesic or curvature lines. An example has been given at the end of the paper with the corresponding figures of the generated partner ruled surfaces.
In this section, we present some basic concepts that will be used throughout the paper. Let α=α(s) be a regular space curve satisfying non-degenerate condition α′(s)∧α″(s)≠0. Then, the orthonormal vector system called the Frenet frame is defined by
T(s)=α′(s)‖α′(s)‖,B(s)=α′(s)∧α″(s)‖α′(s)∧α″(s)‖,N(s)=B(s)∧T(s), | (2.1) |
where T is tangent, N is principal normal and B is binormal vector field. The Frenet formulas are given by
T′=κηN,N′=−κηT+τηB,B′=−τηN,‖α′‖=η, | (2.2) |
where the curvature κ and torsion τ of the curve are[7],
κ=‖α′(s)∧α″(s)‖‖α′(s)‖3,τ=⟨α′(s)∧α″(s),α‴(s)⟩‖α′(s)∧α″(s)‖2. | (2.3) |
The nth degree polynomial with parameter s is defined as
P(s)=ansn+an−1sn−1+...+a1s1+a0,an≠0, |
where n∈N0, ai∈R, (0≤i≤n) [8].
Now, let us define a curve such that α:[a,b]→En,α(s)=(α1(s),α2(s),...,αn(s)). If each αis are polynomials for 1≤i≤n, then as∈R[s] is defined to be an n−dimensional polynomial curve [9]. The degree of such a polynomial curve as α(s) is given by
degα(s)=max{deg(α1(s)),deg(α2(s)),...,deg(αn(s))}[8]. |
The definition of the Flc frame of a polynomial space curve α=α(s) given by Dede in [6] is as follows:
T(s)=α′(s)‖α′(s)‖,D1(s)=α′(s)∧α(n)(s)‖α′(s)∧α(n)(s)‖,D2(s)=D1(s)∧T(s), | (2.4) |
where the prime ′ indicates the differentiation with respect to s and (n) stands for the nth derivative. The new vectors D1 and D2 are called the binormal-like vector and normal-like vector, respectively. The curvatures of the Flc-frame d1,d2and d3 are given by
d1=⟨T′,D2⟩η,d2=⟨T′,D1⟩η,d3=⟨D2′,D1⟩η, | (2.5) |
where ‖α′‖=η. The local rate of change of the Flc-frame called as the Frenet-like formulas can be expressed in the following form:
[T′D2′D1′]=η[0−d1−d2d10−d3d2d30][TD2D1]. | (2.6) |
On the other hand, a ruled surface as a family of straight lines is defined as
φ(s,u)=α(s)+ur(s), | (2.7) |
where α(s) is the base curve, and the r(s) is the generator. The Gaussian and mean curvatures of the ruled surface φ with the normal vector field Nφ are given as
K=eg−f2EG−F2,H=12Eg−2Ef+GeEG−F2. | (2.8) |
Here, the coefficients of first and second fundamental forms are defined as
E=⟨φs,φs⟩,F=⟨φs,φu⟩,G=⟨φu,φu⟩, | (2.9) |
e=⟨φss,Nφ⟩,f=⟨φsu,Nφ⟩,g=⟨φuu,Nφ⟩=0, | (2.10) |
respectively [7].
In this section, we study simultaneously partner ruled surfaces constructed by the tangent, normal-like and binormal-like vectors of the Flc frame along a polynomial space curve.
Definition 3.1. Let α be a differentiable polynomial space curve and {T,D2,D1} be the Flc frame of the polynomial space curve. The two ruled surfaces defined by
{φTD2(s,u)=T(s)+uD2(s),φD2T(s,u)=D2(s)+uT(s), | (3.1) |
are called TD2-partner ruled surfaces with the Flc frame of the polynomial curve.
Theorem 3.1. Let φTD2 and φD2T be TD2-partner ruled surfaces, and then TD2-partner ruled surfaces are simultaneously
(i) developable surfaces if and only if d1=0, d2≠0 or d3≠0,
(ii) minimal surfaces if and only if d2=d3=0 and d1≠0.
Proof. By differentiating the first equation of (3.1) with respect to s and u, respectively and using Flc frame derivative formulas, one can obtain
(φTD2)s=−ηud1T(s)+ηd1D2(s)+η(d2+ud3)D1(s),(φTD2)u=D2(s). | (3.2) |
Then, by considering the partial derivatives of the surface φTD2 given by Eq (3.2) and the cross product of both vectors (φTD2)s and (φTD2)u, the normal vector field of the surface φTD2 is found as
UTD2=(φTD2)s×(φTD2)u‖(φTD2)s×(φTD2)u‖=−(d2+ud1)T(s)−ud1D1(s)√u2d12+(d2+ud3)2. | (3.3) |
By applying the scalar product for both vectors in (3.2), we find the components of the first fundamental form of the ruled surface φTD2 as follows:
ETD2=η2((1+u2)d12+(d2+ud3)2),FTD2=ηd1,GTD2=1. | (3.4) |
By differentiating Eq (3.2) with respect to s and u and making the scalar product with the normal vector field (3.3), we have the component of the second fundamental form of the ruled surface φTD2 as follows:
eTD2=η((1+u2)d12d2η+(d2+ud3)(d2(d2+ud3)η+ud1′)−ud1(d2′+ud3′))√u2d12+(d2+ud3)2,fTD2=ηd1d2√u2d12+(d2+ud3)2,gTD2=0. | (3.5) |
Thus, by substituting Eqs (3.4) and (3.5) into Eq (2.8), the Gaussian curvature and the mean curvature of the ruled surface φTD2 are calculated by
KTD2=−(d1d2u2d12+(d2+ud3)2)2,HTD2=((−1+u2)d12d2η+(d2+ud3)(d2(d2+ud3)η+ud1′)−ud1(d2′+ud3′))2η(u2d12+(d2+ud3))32. | (3.6) |
On the other hand, by differentiating the second equation of (3.1) with respect to s and u, respectively and using the Flc frame derivative formulae, one can obtain
(φD2T)s=−ηd1T(s)+ηud1D2(s)+η(d3+ud2)D1(s),(φD2T)u=T(s). | (3.7) |
Then, by considering the partial derivatives of the surface φD2T given by Eq (3.7) and the cross product of both vectors, the normal vector field of the surface φD2T is found as
UD2T=(φD2T)s×(φD2T)u‖(φD2T)s×(φD2T)u‖=(d3+ud2)D2(s)−ud1D1(s)√u2d12+(d3+ud2)2. | (3.8) |
By applying the scalar product for both vectors in (3.8), we have the components of the first fundamental form of the ruled surface φD2T as follows:
ED2T=η2((1+u2)d12+(d3+ud2)2),FD2T=−ηd1,GD2T=1. | (3.9) |
By differentiating Eq (3.7) with respect to s and u and making the scalar product with the normal vector field (3.8), we have the component of the second fundamental form of the ruled surface φD2T as follows:
eD2T=−η((1+u2)d12d3η+(d3+ud2)(d3(d3+ud2)η−ud1′)+ud1(d3′+ud2′))√u2d12+(d3+ud2)2,fD2T=ηd1d3√u2d12+(d3+ud2)2,gD2T=0. | (3.10) |
Thus, by substituting Eqs (3.9) and (3.10) into Eq (2.8), the Gaussian curvature KD2T and the mean curvature HD2T of the ruled surface φD2T are calculated by
KD2T=−(d1d3u2d12+(d3+ud2)2)2,HD2T=((1−u2)d12d3η+(d3+ud2)(−d3(d3+ud2)η+ud1′)−ud1(d3′+ud2′))2η(u2d12+(d3+ud2))32. | (3.11) |
Consequently, from Eqs (3.6) and (3.11), it can easily be said TD2-partner ruled surfaces are simultaneously developable and minimal surfaces under the conditions stated in the hypothesis.
Theorem 3.2. Let φTD2 and φD2T be TD2-partner ruled surfaces, and then s-parameter curves of TD2-partner ruled surfaces are simultaneously
(i) not geodesic,
(ii) asymptotic if and only if d2=d3=0 and d1≠0.
Proof. Let φTD2 and φD2T be TD2-partner ruled surfaces and the cross products of second partial derivates with the normal vector fields of the TD2-partner ruled surfaces being found as
(φTD2)ss×UTD2=(ud1(ud12η2+η(d2d3η+ud32η−d′1)−d1η′)√u2d12+(d2+ud3)2,−ud13η2−d1η(d2d3+uη(d32η+ud′1))−u2d12η′−(d2+ud3)(η(d′2+ud′3)+(d2+ud3)η′)√u2d12+(d2+ud3)2,−(d2+ud3)(ud12η2+η(d2d3η+ud32η−d′1)−d1η′)√u2d12+(d2+ud3)2,) |
(φD2T)ss×UD2T=(ud13η2+d1η(ud22η+d2d3η−u2d′1)−u2d12η′−(ud2+d3)(η(ud′2+d′3)+(ud2+d3)η′)√u2d12+(ud2+d3)2,−ud1(ud12η2+η(ud22η+d2d3η+d′1)+d1η′)√u2d12+(ud2+d3)2,−(ud2+d3)(ud12η2+η(ud22η+d2d3η+d′1)+d1d′1)√u2d12+(ud2+d3)2.) |
Since (φTD2)ss×UTD2≠0 and (φD2T)ss×UD2T≠0, s-parameter curves of the TD2-partner ruled surfaces simultaneously are not geodesic. On the other hand, the scalar products of second partial derivates with the normal vector fields of the TD2-partner ruled surfaces are calculated as
⟨(φTD2)ss,UTD2⟩=η((1+u2)d12d2η+(d2+ud3)(d2(d2+ud3)η+ud′1)−ud1(d′2+ud′3))√u2d12+(d2+ud3)2, |
⟨(φD2T)ss,UD2T⟩=−η((1+u2)d12d3η+(ud2+d3)(d3η(ud2+d3)−ud′1)+ud1(ud′2+d′3))√u2d12+(ud2+d3)2. |
From here, if d2=d3=0 and d1≠0, then ⟨(φTD2)ss,UTD2⟩=0 and ⟨(φD2T)ss,UD2T⟩=0. So, we can say that s-parameter curves of the TD2-partner ruled surfaces simultaneously are asymptotic if and only if d2=d3=0 and d1≠0.
Theorem 3.3. Let φTD2 and φD2T be TD2-partner ruled surfaces, and then u-parameter curves of TD2-partner ruled surfaces are simultaneously
(i) geodesic,
(ii) asymptotic.
Proof. Let φTD2 and φD2T be TD2- partner ruled surfaces. Since (φTD2)uu×UTD2=0 and (φD2T)uu×UD2T=0, u-parameter curves of the TD2-partner ruled surfaces simultaneously are geodesic. On the other hand, since ⟨(φTD2)uu,UTD2⟩=0 and ⟨(φD2T)uu,UD2T⟩=0, u-parameter curves of the TD2-partner ruled surfaces are simultaneously asymptotic.
Theorem 3.4. Let φTD2 and φD2T be TD2-partner ruled surfaces, and then s and u-parameter curves of TD2-partner ruled surfaces are simultaneously lines of curvature if and only if d1=0.
Proof. Let φTD2 and φD2T be TD2-partner ruled surfaces. For d1=0,
FTD2=ηd1=0,fTD2=ηd1d2√u2d12+(d2+ud3)2=0, |
and
FD2T=−ηd1=0,fD2T=ηd1d3√u2d12+(d3+ud2)2=0. |
Thus, we can easily say that s and u-parameter curves of TD2-partner ruled surfaces are simultaneously lines of curvature if and only if d1=0.
Definition 3.2. Let α be a differentiable polynomial space curve and {T,D2,D1} be the Flc frame of the polynomial space curve. The two ruled surfaces defined by
{φTD1(s,u)=T(s)+uD1(s),φD1T(s,u)=D1(s)+uT(s), | (3.12) |
are called TD1-partner ruled surfaces with the Flc frame of the polynomial curve.
Theorem 3.5. Let φTD1 and φD1T be TD1-partner ruled surfaces, and then TD1-partner ruled surfaces are simultaneously
(i) developable surfaces if and only if d2=0 and d1≠0 or d3≠0,
(ii) minimal surfaces if and only if d1=d3=0 and d2≠0.
Proof. By differentiating the first equation of (3.12) with respect to s and u, respectively and using Flc frame derivative formulae, one can obtain
(φTD1)s=−ηud2T(s)+η(d1−ud3)D2(s)+ηd2D1(s),(φTD1)u=D1(s). | (3.13) |
Then, by considering the partial derivatives of the surface φTD1 given by Eq (3.13) and the cross product of both vectors, the normal vector field of the surface φTD1 is found as
UTD1=(φTD1)s×(φTD1)u‖(φTD1)s×(φTD1)u‖=(d1−ud3)T(s)+ud2D2(s)√u2d22+(d1−ud3)2. | (3.14) |
By applying the scalar product for both vectors in (3.13), we have the components of the first fundamental form of the ruled surface φTD1 as follows:
ETD1=η2((1+u2)d22+(d1−ud3)2),FTD1=ηd2,GTD1=1. | (3.15) |
By differentiating Eq (3.13) with respect to s and u and making the scalar product with the normal vector field (3.14), we have the component of the second fundamental form of the ruled surface φTD1 as follows:
eTD1=−η(η(d13−2ud12d3)+d1d22η((1+u2)+u(ud32η+d2′))−u(ud3d2′+d2(d1′−ud3′)))√u2d22+(d1−ud3)2,fTD1=−ηd1d2√u2d22+(d1−ud3)2,gTD1=0. | (3.16) |
Thus, by substituting Eqs (3.15) and (3.16) into Eq (2.8), the Gaussian curvature and the mean curvature of the ruled surface φTD1 are found by
KTD1=−(d1d2u2d22+(d1−ud3)2)2,HTD1=(η(−d13+2ud12d3)+d1((1−u2)d23η−u(ud32η+d2′))+u(ud3d2′+d2(d1′−ud3′)))2η(u2d22+(d1−ud3))32. | (3.17) |
On the other hand, by differentiating the second equation of (3.12) with respect to s and u, respectively and using Flc frame derivative formulae, one can obtain
(φD1T)s=−ηd2T(s)+η(ud1−d3)D2(s)+uηd2D1(s),(φD1T)u=T(s). | (3.18) |
Then, by considering the partial derivatives of the surface φD1T given by Eq (3.18) and the cross product of both vectors, the normal vector field of the surface φD1T is found as
UD1T=(φD1T)s×(φD1T)u‖(φD1T)s×(φD1T)u‖=ud2D2(s)−(ud1−d3)D1(s)√u2d22+(ud1−d3)2. | (3.19) |
By applying the scalar product for both vectors in (3.19), we have the components of the first fundamental form of the ruled surface φD1T as follows:
ED1T=η2((1+u2)d22+(d3−ud1)2),FD1T(s,u,t)=−ηd2,GD1T=1. | (3.20) |
The scalar products of differentiation of Eq (3.18) with respect to s and u with the normal vector field (3.19) gives us the component of the second fundamental form of the ruled surface φD1T as follows:
eD1T=−η(u2d12d3η+(1+u2)d22d3η+d33η−ud3d2′+ud1(−2d32η+ud2′)+ud2(−ud1′+d3′))√u2d22+(d3−ud1)2,fD1T=ηd2d3√u2d22+(d3−ud1)2,gD1T=0. | (3.21) |
Thus, by substituting Eqs (3.20) and (3.21) into Eq (2.8), the Gaussian curvature KD1T and the mean curvature HD1T of the ruled surface φD1T are calculated by
KD1T=−(d2d3u2d22+(d3−ud1)2)2,HD1T=((1−u2)d22d3η−u2d12d3η−d32η+ud3d2′+ud1(2ηd32−ud2′)+ud2(ud1′−d3′))2η(u2d22+(d3−ud1))32. | (3.22) |
Consequently, from Eqs (3.17) and (3.22), it can easily be said TD1-partner ruled surfaces are simultaneously developable and minimal surfaces under the conditions stated in the hypothesis.
Theorem 3.6. Let φTD1 and φD1T be TD1-partner ruled surfaces, and then s-parameter curves of TD1-partner ruled surfaces are simultaneously
(i) not geodesic,
(ii) asymptotic if and only if d1=d3=0 and d2≠0.
Proof. The proof is done in a similar way to the proof of the theorem given for TD2-partner ruled surfaces.
Theorem 3.7. Let φTD1 and φD1T be TD1-partner ruled surfaces, and then u-parameter curves of TD1-partner ruled surfaces are simultaneously
(i) geodesic,
(ii) asymptotic.
Proof. The proof is done in a similar way to the proof of the theorem given for TD2-partner ruled surfaces.
Theorem 3.8. Let φTD1 and φD1T be TD1-partner ruled surfaces, and then s and u-parameter curves of TD1-partner ruled surfaces are simultaneously lines of curvature if and only if d2=0.
Proof. The proof is done in a similar way to the proof of the theorem given for TD2-partner ruled surfaces.
Definition 3.3. Let α be a differentiable polynomial space curve and {T,D2,D1} be the Flc frame of the polynomial space curve. The two ruled surfaces defined by
{φD2D1(s,u)=D2(s)+uD1(s),φD1D2(s,u)=D1(s)+uD2(s), | (3.23) |
are called D2D1-partner ruled surfaces with the Flc frame of the polynomial curve.
Theorem 3.9. Let φD2D1 and φD1D2 be a D2D1-partner ruled surfaces, and then D2D1-partner ruled surfaces are simultaneously
(i) developable surfaces if and only if d3=0 and d1≠0 or d2≠0,
(ii) minimal surfaces if and only if d1=d2=0 and d3≠0.
Proof. By differentiating the first equation of (3.23) with respect to s and u, respectively and using Flc frame derivative formulae, one can obtain
(φD2D1)s=−η(d1+ud2)T(s)−ηd3D2(s)+ηd3D1(s),(φD2D1)u=D1(s). | (3.24) |
Then, by considering the partial derivatives of the surface φD2D1 given by Eq (3.24) and the cross product of both vectors, the normal vector field of the surface φD2D1 is found as
UD2D1=(φD2D1)s×(φD2D1)u‖(φD2D1)s×(φD2D1)u‖=−ud3D2(s)+(d1+ud2)D1(s)√u2d32+(d1+ud2)2. | (3.25) |
By applying the scalar product for both vectors in (3.24), we have the components of the first fundamental form of the ruled surface φD2D1 as follows:
ED2D1=η2((1+u2)d32+(d1+ud2)2),FD2D1=ηd3,GD2D1=1. | (3.26) |
By differentiating Eq (3.24) with respect to s and u and making the scalar product with the normal vector field (3.25), we have the component of the second fundamental form of the ruled surface φD2D1 as follows:
eD2D1=−η(d13η+2ud12d2η+d1(d32+u2η(d22+d32)+ud3′)+u(−d3(d1′+ud2′)+ud2d3′))√u2d32+(d1+ud2)2,fD2D1=ηd1d3√u2d32+(d1+ud2)2,gD2D1=0. | (3.27) |
Thus, by substituting Eqs (3.26) and (3.27) into Eq (2.8), the Gaussian curvature KD2D1 and the mean curvature HD2D1 of the ruled surface φD2D1 are calculated by
KD2D1=−(d1d3u2d32+(d1+ud2)2)2,HD2D1=(−d13η−2ud12d2η−d1(u2d22η+(−1+u2)d32η+ud3′+u(d3(d1′+ud2′)−ud2d3′)))2η(u2d32+(d1+ud2))32. | (3.28) |
On the other hand, by differentiating the second equation of (3.23) with respect to s and u, respectively and using Flc frame derivative formulae, one can obtain
(φD1D2)s=−η(d2+ud1)T(s)−ηd3D2(s)+uηd3D1(s),(φD1D2)u=D2(s). | (3.29) |
Then, by considering the partial derivatives of the surface φD1D2 given by Eq (3.29) and the cross product of both vectors, the normal vector field of the surface φD1D2 is found as
UD1D2=(φD1D2)s×(φD1D2)u‖(φD1D2)s×(φD1D2)u‖=−ud3T(s)−(d2+ud1)D1(s)√u2d32+(d2+ud1)2. | (3.30) |
By applying the scalar product for both vectors in (3.30), we have the components of the first fundamental form of the ruled surface φD1D2 as follows:
ED1D2=η2((1+u2)d32+(d2+ud1)2),FD1D2=−ηd3,GD1D2=1. | (3.31) |
By differentiating Eq (3.29) with respect to s and u and making the scalar product with the normal vector field (3.30), we have the component of the second fundamental form of the ruled surface φD1D2 as follows:
eD1D2=η(ud12d2η+d23η+ud3(d2′+ud1′)+ud1(2d22η−ud3′)+d2((1+u2)d32η−ud3′))√u2d32+(d2+ud1)2,fD1D2=−ηd2d3√u2d32+(d2+ud1)2,gD1D2=0. | (3.32) |
Thus, by substituting Eqs (3.31) and (3.32) into Eq (2.8), the Gaussian curvature KD1D2 and the mean curvature HD1D2 of the ruled surface φD1D2 are calculated by
KD1D2=−(d2d3u2d32+(d2+ud1)2)2,HD1D2=(u2d12d2η+d23η+ud3(d2′+ud1′)+ud1(2d22η−ud3′)+d2((−1+u2)d32η−ud3′))2η(u2d32+(d2+ud1))32. | (3.33) |
Consequently, from Eqs (3.28) and (3.33), it can easily be said D2D1-partner ruled surfaces are simultaneously developable and minimal surfaces under the conditions stated in the hypothesis.
Theorem 3.10. Let φD2D1 and φD1D2 be D2D1-partner ruled surfaces, and then s-parameter curves of D2D1-partner ruled surfaces are simultaneously
(i) not geodesic,
(ii) asymptotic if and only if d1=d2=0 and d3≠0.
Proof. The proof is done in a similar way to the proof of the theorem given for TD2-partner ruled surfaces.
Theorem 3.11. Let φD2D1 and φD1D2 be D2D1-partner ruled surfaces, and then s and u-parameter curves of D2D1-partner ruled surfaces are simultaneously line of curvatures if and only if d3=0.
Proof. The proof is done in a similar way to the proof of the theorem given for TD2-partner ruled surfaces.
Example 3.1. Let us consider a helical polynomial curve parameterized as α(s)=(6s,3s2,s3). Then, the Flc frame elements of α are given by
T(s)=(22+s2,2s2+s2,s22+s2),D1(s)=(s√1+s2,−1√1+s2,0),D2(s)=(−s2√1+s2(2+s2),−s3√1+s2(2+s2),2√1+s22+s2) |
and the corresponding curvatures according to the Flc frame are the following:
d1(s)=s√s2+1,d2(s)=−1√s2+1,d3(s)=s22(s2+1). |
(1) Thus, we have the parametric forms for TD2-partner ruled surfaces as follows:
φTD2=(2√s2+1−s2u(s2+2)√s2+1,s(2√s2+1−s2u)(s2+2)√s2+1,s2+2√1+s2u(s2+2)),φD2T=(−s2+2u√s2+1(s2+2)√s2+1,s(−s2+2u√s2+1)(s2+2)√s2+1,2√1+s2+s2u(s2+2)). |
See Figure 1.
(2) Thus, we have the parametric forms for TD1-partner ruled surfaces as follows:
φTD1=(22+s2+su√1+s2,2s2+s2−u√1+s2,s22+s2),φD1T=(s√1+s2+2u2+s2,−1√1+s2+2su2+s2,s2u2+s2). |
See Figure 2.
(3) Thus, we have the parametric forms for D2D1-partner ruled surfaces as the following:
φD2D1=(−s2+su(2+s2)√1+s2(2+s2),−2u−s2(s+u)√1+s2(2+s2),2√1+s22+s2),φD1D2=(s(2+s2−su)√1+s2(2+s2),−2−s2(1+su)√1+s2(2+s2),2√1+s2u2+s2). |
See Figure 3.
Example 3.2. Let us consider a helical polynomial curve parameterized as β(s)=(s3,s4,s5).Then the Flc frame elements of β are given by
T(s)=(3√25s4+16s2+9,,4s√25s4+16s2+9,5s2√25s4+16s2+9),D1(s)=(4s√16s2+9,−3√16s2+9,0),D2(s)=(−15s2√16s2+9√25s4+16s2+9,−20s3√16s2+9√25s4+16s2+9,√16s2+9√25s4+16s2+9), |
and the corresponding curvatures according to Flc frame are as the following:
d1(s)=10(8s2+9)s(25s4+16s2+9)32√16s2+9,d2(s)=−12s2(25s4+16s2+9)√16s2+9,d3(s)=60(25s4+16s2+9)(16s2+9). |
(1) Thus, we have the parametric forms for TD2-partner ruled surfaces as follows:
χTD2=(3√25s4+16s2+9−15us2√16s2+9√25s4+16s2+9,4s√25s4+16s2+9−20us3√16s2+9√25s4+16s2+9,5s2√25s4+16s2+9+u√16s2+9√25s4+16s2+9,)χD2T=(−15s2√16s2+9√25s4+16s2+9+3u√25s4+16s2+9,−20s3√16s2+9√25s4+16s2+9+4us√25s4+16s2+9,√16s2+9√25s4+16s2+9+5us2√25s4+16s2+9.) |
See Figure 4.
(2) Thus, we have the parametric forms for TD1-partner ruled surfaces as follows:
χTD1=(3√25s4+16s2+9+4us√16s2+9,4s√25s4+16s2+9−3u√16s2+9,5s2√25s4+16s2+9,)χD1T=(4s√16s2+9+3u√25s4+16s2+9,−3√16s2+9+4us√25s4+16s2+95us2√25s4+16s2+9.) |
See Figure 5.
(3) Thus, we have the parametric forms for D2D1-partner ruled surfaces as the following:
χD2D1=(−15s2√16s2+9√25s4+16s2+9+4us√16s2+9,−20s3√16s2+9√25s4+16s2+9−3u√16s2+9,√16s2+9√25s4+16s2+9,)χD1D2=(4s√16s2+9−15us2√16s2+9√25s4+16s2+9,−3√16s2+9−20us3√16s2+9√25s4+16s2+9,u√16s2+9√25s4+16s2+9.) |
See Figure 6.
In this paper, the invariants of partner ruled surfaces formed by tangent, normal-like and binormal-like vector fields of a polynomial space curve simultaneously are presented. Also, some characterizations of the parameter curves are examined. Examples of these surfaces are given and their graphics are drawn using the MATLAB R2021b program.
We gratefully acknowledge the constructive comments from the editor and the anonymous referees. This work was funded by the National Natural Science Foundation of China (Grant No. 12101168), Zhejiang Provincial Natural Science Foundation of China (Grant No. LQ22A010014).
The authors declare no conflict of interest.
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