In this work, we study the canal surfaces foliated by pseudo hyperbolic spheres H20 along a Frenet curve in terms of their Gauss maps in Minkowski 3-space. Such kind of surfaces with pointwise 1-type Gauss maps are classified completely. For example, an oriented canal surface that has proper pointwise 1-type Gauss map of the first kind satisfies ΔG=−2KG, where K and G is the Gaussian curvature and the Gauss map of the canal surface, respectively.
Citation: Jinhua Qian, Jie Liu, Xueshan Fu, Seoung Dal Jung. Geometric characterizations of canal surfaces with Frenet center curves[J]. AIMS Mathematics, 2021, 6(9): 9476-9490. doi: 10.3934/math.2021551
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In this work, we study the canal surfaces foliated by pseudo hyperbolic spheres H20 along a Frenet curve in terms of their Gauss maps in Minkowski 3-space. Such kind of surfaces with pointwise 1-type Gauss maps are classified completely. For example, an oriented canal surface that has proper pointwise 1-type Gauss map of the first kind satisfies ΔG=−2KG, where K and G is the Gaussian curvature and the Gauss map of the canal surface, respectively.
The idea of finite type immersion of Riemannian manifolds into Euclidean space (resp. pseudo Euclidean space) was introduced by B.Y. Chen in the late 1970's, which was extended to the differential maps on the submanifolds such as the Gauss maps. A submanifold M in Euclidean space (resp. pseudo Euclidean space) whose Gauss map G satisfies ΔG=f(G+C) is said to have a proper pointwise 1-type Gauss map for a non-zero smooth function f and a constant vector C, where Δ is the Laplacian defined on M and in local coordinates given by
Δ=−1√|det(gij)|∑i,j∂∂xi(√|det(gij)|gij∂∂xj), | (1.1) |
where gij are the components of the inverse matrix of the first fundamental form of M. Specially, it is said to be of the first kind or the second kind when the vector C is zero or non-zero, respectively. Furthermore, G is said to be of proper pointwise 1-type if the function f is not constant, otherwise a non-proper pointwise 1-type Gauss map is just of ordinary 1-type. When the smooth function f vanishes, G is said to be harmonic [1,2,5].
In the theory of surfaces, a canal surface is formed by moving a family of spheres whose centers lie on a space curve in Euclidean 3-space. The geometric characteristics of such surfaces have been studied by many experts and geometers [4,8,13]. For example, the authors of [4] investigated the geometric properties of such surfaces, including the Gaussian curvature, the mean curvature and their relationships. In recent years, the construction idea of canal surfaces in Euclidean 3-space is extended to Lorentz-Minkowski space. In Minkowski 3-space, a canal surface can be formed as the envelope of a family of pseudo-Riemannian space forms, i.e., pseudo spheres S21, pseudo hyperbolic spheres H20 and lightlike cones Q2 [3,9,12]. Let p be a fixed point, r>0 be a constant in E31. The pseudo-Riemannian space forms, i.e., the de-Sitter space S21(p,r), the hyperbolic space H20(p,r) and the lightlike cone Q21(p) are defined by
M2(ϵ)={x∈E31:⟨x−p,x−p⟩=ϵr2}={S21(p,r) | ϵ=1;H20(p,r) | ϵ=−1;Q21(p)| ϵ=0. |
When r=1 and the center p is the origin, we write them by S21, H20 and Q2, simply. According to the classification of curves in Minkowski space, there are nine types of canal surfaces in Minkowski 3-space whose fundamental geometric properties have been achieved by discussing the linear Weingarten canal surfaces in [3,9].
Based on the conclusions obtained in [4], a canal surface with pointwise 1-type Gauss map is discussed in [8]. In order to do further geometric investigation for canal surfaces in Minkowski 3-space, in this work we study surfaces foliated by pseudo hyperbolic spheres H20 along Frenet curves. In section 2, the Frenet formulas of Frenet curves, the parameterized equations and the relationships between the Gaussian curvatures and the mean curvatures of three types of canal surfaces are recalled. In section 3, three types of canal surfaces with pointwise 1-type Gauss maps are classified completely.
The surfaces which are discussed here are smooth, regular and topologically connected unless otherwise stated.
Let E31 be a Minkowski 3-space with natural Lorentzian metric
⟨⋅,⋅⟩=dx21+dx22−dx23 |
in terms of the natural coordinate system (x1,x2,x3). It is well known that a vector υ∈E31 is called to be spacelike if ⟨υ,υ⟩>0 or υ=0; timelike if ⟨υ,υ⟩<0; null (lightlike) if ⟨υ,υ⟩=0, respectively. The norm of a vector υ is given by ‖υ‖=√|⟨υ,υ⟩|. The timelike or lightlike vector is said to be causal [6]. Due to the causal character of the tangent vectors, the curves are classified into spacelike curves, timelike curves or lightlike (null) curves. What's more, the spacelike curves are classified into the first and the second kind of spacelike curves or the null type spacelike curves (pseudo null curves) according to their normal vectors are spacelike, timelike or lightlike, respectively.
Remark 2.1. [7] Timelike curves and spacelike curves with spacelike or timelike normal vectors are called Frenet curves in Minkowski space.
Proposition 2.2. [4] Let c(s):I→E31 be a Frenet curve parameterized by arclength s with Frenet frame {T(s),N(s),B(s)}. Then the following Frenet equations are satisfied
{T′(s)=κ(s)N(s),N′(s)=−ϵ1κ(s)T(s)+ϵ2τ(s)B(s),B′(s)=τ(s)N(s), |
where T is the tangent vector, N and B is the normal vector and the binormal vector of c(s), respectively. When c(s) is a timelike curve, ϵ1=ϵ2=−1; when c(s) is a spacelike curve of the first kind, ϵ1=ϵ2=1; when c(s) is a spacelike curve of the second kind, ϵ1=−ϵ2=−1. The function κ(s), τ(s) is called the curvature, the torsion of c(s), respectively.
Definition 1. [3] A surface M in E31 is called a canal surface which is formed as the envelope of a family of pseudo hyperbolic spheres H20 (resp. pseudo spheres S21 or lightlike cones Q2) whose centers lie on a space curve c(s) framed by {T,N,B}. Then M can be parameterized by
x(s,θ)=c(s)+λ(s,θ)T(s)+μ(s,θ)N(s)+ω(s,θ)B(s), |
where λ, μ and ω are differential functions of s and θ, ‖x(s,θ)−c(s)‖2=ϵr2(s), (ϵ=±1 or 0). The curve c(s) is called the center curve and r(s) is called the radial function of M.
Precisely, if M is foliated by pseudo hyperbolic spheres H20 (resp. pseudo spheres S21 or lightlike cones Q2), then ϵ=−1(resp. 1 or 0) and M is said to be of type M− (resp. M+ or M0). As well, the canal surfaces of type M− can be classified into M1− (resp. M2− or M3−) when c(s) is spacelike (resp. timelike or null). Moreover, when c(s) is the first kind spacelike curve, the second kind spacelike curve and the pseudo null curve, M1− is denoted by M11−, M12− and M13−, respectively. Similarly, the canal surfaces M+ (resp. M0) can be classified into M1+, M2+ and M3+ (resp. M10, M20 or M30). Naturally, M1+ (resp. M10) can be divided into M11+, M12+ and M13+ (resp. M110, M120 or M130) [9].
Remark 2.3. In the present work, we consider the canal surfaces foliated by pseudo hyperbolic spheres H20 which have Frenet curves as center curves, i.e., the canal surfaces of type M11−, M12− and M2−.
The canal surfaces M11−, M12− and M2− are expressed as [9]
M11−:x(s,θ)=c(s)+r(s)(r′(s)T+√1+r′2(s)sinhθN+√1+r′2(s)coshθB); |
M12−:x(s,θ)=c(s)+r(s)(r′(s)T+√1+r′2(s)coshθN+√1+r′2(s)sinhθB); |
M2−:x(s,θ)=c(s)+r(s)(−r′(s)T+√r′2(s)−1cosθN+√r′2(s)−1sinθB). |
Without loss of generality, the authors assumed r′(s)=sinhφ for M11− and M12−, −r′(s)=coshφ for M2−, where φ=φ(s) is a smooth function, then the canal surfaces M11−, M12− and M2− can be rewritten by
M11−:x(s,θ)=c(s)+r(s)(sinhφ(s)T+coshφ(s)sinhθN+coshφ(s)coshθB); | (2.1) |
M12−:x(s,θ)=c(s)+r(s)(sinhφ(s)T+coshφ(s)coshθN+coshφ(s)sinhθB); | (2.2) |
M2−:x(s,θ)=c(s)+r(s)(coshφ(s)T+sinhφ(s)cosθN+sinhφ(s)sinθB). | (2.3) |
Proposition 2.4. [9] For the canal surface M11− \ (resp. M12−,M2−), the Gaussian curvature K and the mean curvature H satisfy
H=−12(Kr−1r). |
Remark 2.5. By Proposition 2.4, the principal curvatures κ1,κ2 of the canal surface M11−\ (resp. M12−,M2−) are given by
κ1=Kr, κ2=−1r. |
From now on, we concern on the classifications of three kinds of canal surfaces in terms of their Gauss maps. We only prove the results for M11− and omit the proofs for M12− and M2− since they can be similarly done to those of M11−.
From Eq (2.1), the canal surface M11− is parameterized by
x(s,θ)=c(s)+r(s)(sinhφ(s)T+coshφ(s)sinhθN+coshφ(s)coshθB), |
where sinhφ(s)=r′(s).
Through direct calculations, we have
xs=x1sT+x2sN+x3sB, xθ=x1θN+x2θB, |
where
x1s=rr″−rκcoshφsinhθ+cosh2φ,x2s=r′coshφsinhθ+rr′κ+rr′φ′sinhθ+rτcoshφcoshθ,x3s=r′coshφcoshθ+rτcoshφsinhθ+rr′φ′coshθ,x1θ=rcoshφcoshθ,x2θ=rcoshφsinhθ. | (3.1) |
Thus, the Gauss map G of M11− is
G=sinhφT+coshφsinhθN+coshφcoshθB, | (3.2) |
which point outwards M11− and ⟨G,G⟩=−1.
Meanwhile, the component functions of the first fundamental form are obtained as
g11=P21+r2R21cosh2φ, g12=r2R1, g22=r2cosh2φ, | (3.3) |
the component functions of the second fundamental form are written by
h11=−rR21+P1Q1cosh2φ, h12=−rR1, h22=−rcosh2φ, | (3.4) |
where
P1=rr″+cosh2φ−rκcoshφsinhθ=rQ1+cosh2φ,Q1=r″−κcoshφsinhθ,R1=r′κcoshφcoshθ+τcosh2φ. | (3.5) |
From Eqs (3.3) and (3.4), the Gaussian curvature K and the mean curvature H of M11− are
K=−Q1rP1, H=2P1−cosh2φ2rP1. | (3.6) |
Remark 3.1. From g11g22−g212=r2P21, due to regularity, we see that P1≠0 everywhere.
Serving the following discussion, the Laplacian of the Gauss map G of M11− need to be calculated. First, from the first fundamental form of M11−, we have
g11=cosh2φP21, g12=−R1P21, g22=P21+r2R21r2P21cosh2φ. | (3.7) |
Substituting (3.2), (3.3) and (3.7) into (1.1), and by putting
U1=g22Hs−g12Hθ, V1=−g12Hs+g11Hθ, | (3.8) |
where
Hs=5r2r′r″κcoshφsinhθ−2r2r′κ2cosh2φsinh2θ+r2r‴cosh2φ−2rr′r″cosh2φ−4r2r′r″22r2P21+(2rr′κ−r2κ′)cosh3φsinhθ−r′cosh4φ2r2P21,Hθ=−κcosh3φcoshθ2P21, | (3.9) |
after tedious tidying up, we get
ΔG=−1r2P21{[(r2Q21+P21)sinhφ−2x1sU1]T+[(r2Q21+P21)coshφsinhθ−2(x2sU1+x1θV1)]N+[(r2Q21+P21)coshφcoshθ−2(x3sU1+x2θV1)]B}. | (3.10) |
Assume a canal surface M11− satisfies ΔG=f(G+C). Without loss of generality, we may suppose
C=C1T+C2N+C3B, | (3.11) |
where C1=⟨C,T⟩,C2=⟨C,N⟩,C3=−⟨C,B⟩.
Substituting (3.2), (3.10) and (3.11) into ΔG=f(G+C), we obtain the following equation system
{(r2Q21+P21)sinhφ−2x1sU1=−r2P21(sinhφ+C1)f,(r2Q21+P21)coshφsinhθ−2(x2sU1+x1θV1)=−r2P21(coshφsinhθ+C2)f,(r2Q21+P21)coshφcoshθ−2(x3sU1+x2θV1)=−r2P21(coshφcoshθ+C3)f. | (3.12) |
From the last two equations of (3.12), we have
2U1(rτcosh2φ+rr′κcoshφcoshθ−x3sC2+x2sC3)+2V1(rcosh2φ−x2θC2+x1θC3)=coshφ(2P21−2P1cosh2φ+cosh4φ)(C3sinhθ−C2coshθ). | (3.13) |
Rearranging (3.13) with the help of (3.1), (3.5) and (3.8), we get
2(g22Hs−g12Hθ)(rτcosh2φ+rr′κcoshφcoshθ−x3sC2+x2sC3)+2(−g12Hs+g11Hθ)(rcosh2φ−rcoshφsinhθC2+rcoshφcoshθC3)=coshφ[(rr″−rκcoshφsinhθ)2+(rr″+cosh2φ−rκcoshφsinhθ)2](C3sinhθ−C2coshθ). | (3.14) |
Since {cosh(mθ),sinh(mθ)|m∈N} constructs a set of linearly independent functions, in view of the coefficients of sinh5θ and cosh5θ in (3.14) by the aid of (3.1), (3.3) and (3.9), we have
{r6κ4cosh5φC3=0,r6κ4cosh5φC2=0. | (3.15) |
From (3.15), we consider a non-empty open subset O={p∈M11−∣κ(p)≠0} of M11−. Since r≠0, coshφ≠0, then we have C2=C3=0 on O. However, if C2=C3=0, (3.14) gives
−r2R21+g11cosh2φ=P21=0 |
which contradicts to the regularity of M11−. Therefore, κ≡0, M11− is a surface of revolution.
Let c(s)=(s,0,0) and T=(1,0,0),N=(0,1,0),B=(0,0,1), then M11− can be represented as
x(s,θ)=(s+r(s)sinhφ,r(s)coshφsinhθ,r(s)coshφcoshθ). |
Furthermore, when κ=0, the first equation of (3.12) gives
f=2r2cosh2φP1Hs−(2P21−2P1cosh2φ+cosh4φ)sinhφr2P21(sinhφ+C1). | (3.16) |
Because P1,Hs are all functions of s when κ=0, Equation (3.16) yields f=f(s). Then, by the last two equations of (3.12), we have
{(r2Q21+P21)coshφsinhθ−2r2r′cosh2φHs(coshφ+rφ′)sinhθ=−r2P21(coshφsinhθ+C2)f,(r2Q21+P21)coshφcoshθ−2r2r′cosh2φHs(coshφ+rφ′)coshθ=−r2P21(coshφcoshθ+C3)f. | (3.17) |
Because r≠0, P1≠0 and f=f(s), Equation system (3.17) implies C2=C3=0. And
f(s)=2r2HsP1sinhφ−(2P21−2P1cosh2φ+cosh4φ)r2P21. | (3.18) |
Combining (3.16) and (3.18), we get
C1(2P21−2P1cosh2φ+cosh4φ)+2r2HsP1(1−C1r′)=0, | (3.19) |
substituting (3.19) into (3.18), we have
f(s)=2HsC1P1=4H2+2KC1r′−1. | (3.20) |
Considering the principal curvatures are given by
κ1=−r″rr″+r′2+1, κ2=−1r | (3.21) |
when κ=0, thus the Gaussian curvature K and the mean curvature H are
K=−r″r(rr″+r′2+1), H=2rr″+r′2+12r(rr″+r′2+1). | (3.22) |
Due to f≠0, the mean curvature cannot be constant. With the help of (3.6), Equation (3.19) can be rewritten as
2r2Hs(1−rH)(C1r′−1)=C1(2r2H2−2rH+1)(r′2+1). | (3.23) |
Simplifying Eq (3.23) with the help of (3.22), the radial function r(s) satisfies
κ1(κ1−1r)′=(ln|C1r′−1|)′(κ21+1r2), | (3.24) |
where κ1 is stated as (3.21).
Conversely, if M11− is a surface of revolution satisfying (3.24), ΔG=f(G+C) can be satisfied for a non-zero function f as stated by (3.20) and a constant vector C=(C1,0,0) in which C1 is a non-zero constant.
Theorem 3.2. A canal surface M11− has proper pointwise 1-type Gauss map of the second kind if and only if it is a surface of revolution with the following form
x(s,θ)=(s+r(s)sinhφ,r(s)coshφsinhθ,r(s)coshφcoshθ), |
where r(s) satisfies (3.24).
Corollary 3.3. A canal surface M11− with proper pointwise 1-type Gauss map of the second kind satisfies ΔG=f(G+C) for a constant vector C=(C1,0,0) and non-zero smooth function
f(s)=4H2+2KC1r′−1, |
where H and K are given by (3.22), C1 is a non-zero constant.
Corollary 3.4. A canal surface M11− has 1-type Gauss map of the second kind if and only if it is a surface of revolution represented as
x(s,θ)=(s+r(s)sinhφ,r(s)coshφsinhθ,r(s)coshφcoshθ), |
where r(s) satisfies (3.26).
Proof of Corollary 3.4. When a canal surface M11− satisfies ΔG=λ(G+C), (λ∈R−{0},C≠0), by Theorem 3.2, M11− is a surface of revolution satisfying (3.24). By Corollary 3.3, we get
κ1(κ1−1r)′=λC1r″. | (3.25) |
From (3.24) and (3.25), we have
κ21+1r2=λ(C1r′−1), | (3.26) |
where λ and C1 are non-zero constants, κ1 is stated as (3.21). The converse is straightforward.
Theorem 3.5. A canal surface M11− has proper pointwise 1-type Gauss map of the first kind if and only if it is minimal. Precisely, it is a part of a surface of revolution as
x(s,θ)=(s+r(s)sinhφ,r(s)coshφsinhθ,r(s)coshφcoshθ), |
where r(s) satisfies (3.29).
Proof of Theorem 3.5. A canal surface M11− has proper pointwise 1-type Gauss map of the first kind, i.e., ΔG=fG for a smooth function f. From Equation (3.10), we have
{(r2Q21+P21)sinhφ−2x1sU1=−r2P21sinhφf,(r2Q21+P21)coshφsinhθ−2(x2sU1+x1θV1)=−r2P21coshφsinhθf,(r2Q21+P21)coshφcoshθ−2(x3sU1+x2θV1)=−r2P21coshφcoshθf. | (3.27) |
From the last two equations of (3.27), we get
(g22Hs−g12Hθ)(τcosh2φ+r′κcoshφcoshθ)+(−g12Hs+g11Hθ)cosh2φ=0. | (3.28) |
With the help of Eq (3.3), we obtain P21Hθ=0. Therefore, Hθ=0 due to P1≠0. Furthermore, from the first two equations of (3.27), we get 2r2P1Hs=0. It is obvious that Hs=0. Then, the mean curvature of M11− is constant. By the Corollary 2 of [9], i.e., the canal surface M11− with non-zero constant mean curvature does not exist, thus the canal surface M11− is minimal. From the Theorem 4 of [9], it is a part of a surface of revolution with the following form
x(s,θ)=(s+r(s)sinhφ,r(s)coshφsinhθ,r(s)coshφcoshθ), |
where r(s) satisfies
s=c2±∫√rc1−rdr,(c1>r,c2∈R). | (3.29) |
Looking back the Eq (3.27) with the conclusions obtained above, we have
f(s)=−2K=−2r2. | (3.30) |
Conversely, suppose that M11− is a surface of revolution satisfying (3.29), M11− is minimal from the Theorem 4 of [9] and ΔG=fG is satisfied for a non-zero function f given by (3.30).
Corollary 3.6. A canal surface M11− with proper pointwise 1-type Gauss map of the first kind satisfies
ΔG=−2KG=−2r2G. |
Assume that a canal surface M11− satisfies ΔG=λG, (λ∈R−{0}). By Corollary 3.6, we have λ=−2r2 is a constant, i.e., r is a constant. Thus, we have the following result.
Corollary 3.7. A canal surface M11− has 1-type Gauss map of the first kind if and only if it is a circular cylinder.
From Corollary 3.6, the following conclusion is straightforward since −2r2≠0.
Corollary 3.8. The canal surface M11− with harmonic Gauss map does not exist.
From Eq (2.2), the canal surface M12− is parameterized by
x(s,θ)=c(s)+r(s)(sinhφ(s)T+coshφ(s)coshθN+coshφ(s)sinhθB), |
where sinhφ(s)=r′(s).
Through direct calculations, we have
xs=x1sT+x2sN+x3sB, xθ=x1θN+x2θB, |
where
x1s=rr″+cosh2φ+rκcoshφcoshθ;x2s=r′coshφcoshθ+rr′κ+rr′φ′coshθ+rτcoshφsinhθ;x3s=r′coshφsinhθ+rτcoshφcoshθ+rr′φ′sinhθ;x1θ=rcoshφsinhθ;x2θ=rcoshφcoshθ. |
Then, the Gauss map G of M12− is
G=−sinhφT−coshφcoshθN−coshφsinhθB, | (4.1) |
which point outwards M12− and ⟨G,G⟩=−1.
Meanwhile, the component functions of the first fundamental form are given by
g11=P22+r2R22cosh2φ, g12=r2R2, g22=r2cosh2φ, | (4.2) |
the component functions of the second fundamental form are written by
h11=−rR22+P2Q2cosh2φ, h12=−rR2, h22=−rcosh2φ, | (4.3) |
where
P2=rr″+cosh2φ+rκcoshφcoshθ=rQ2+cosh2φ,Q2=r″+κcoshφcoshθ,R2=τcosh2φ−r′κcoshφsinhθ. |
From Eqs (4.2) and (4.3), the Gaussian curvature K and the mean curvature H of M12− are
K=−Q2rP2, H=2P2−cosh2φ2rP2. |
Remark 4.1. From g11g22−g212=r2P22, due to regularity, we see that P2≠0 everywhere.
Next, we compute the Laplacian of the Gauss map G of M12−. First, from the first fundamental form of M12−, we have
g11=cosh2φP22, g12=−R2P22, g22=r2R22+P22r2P22cosh2φ. | (4.4) |
Substituting (4.1), (4.2) and (4.4) into (1.1), and by putting
U2=g22Hs−g12Hθ, V2=−g12Hs+g11Hθ, |
where
Hs=2rr′r″cosh2φ+r2r‴cosh2φ−4r2r′r″2−2r2r′κ2cosh2φcosh2θ−5r2r′r″κcoshφcoshθ2r2P22−(2rr′κ−r2κ′)cosh3φcoshθ+r′cosh4φ2r2P22,Hθ=κcosh3φsinhθ2P22, |
after tedious tidying up, we get
ΔG=1r2P22{[(r2Q22+P22)sinhφ+2x1sU2]T+[(r2Q22+P22)coshφcoshθ+2(x2sU2+x1θV2)]N+[(r2Q22+P22)coshφsinhθ+2(x3sU2+x2θV2)]B}. |
Do discussions similar to those of M11−, we have the following conclusions directly.
Theorem 4.2. A canal surface M12− has proper pointwise 1-type Gauss map of the second kind if and only if it is a surface of revolution with the following form
x(s,θ)=(r(s)sinhφ+s,r(s)coshφsinhθ,r(s)coshφcoshθ), |
in which r(s) satisfies
κ1(κ1−1r)′=−(ln|1+C1r′|)′(κ21+1r2), |
where C1 is a non-zero constant and κ1 is the principal curvature as
κ1=−r″rr″+r′2+1. |
Corollary 4.3. A canal surface M12− with proper pointwise 1-type Gauss map of the second kind satisfies ΔG=f(G+C) for a constant vector C=(C1,0,0) and non-zero smooth function
f(s)=−4H2+2K1+C1r′, |
where C1 is a non-zero constant, H and K are given by
K=−r″r(rr″+r′2+1), H=2rr″+r′2+12r(rr″+r′2+1). |
Corollary 4.4. A canal surface M12− has 1-type Gauss map of the second kind if and only if it is a surface of revolution represented as
x(s,θ)=(s+r(s)sinhφ,r(s)coshφsinhθ,r(s)coshφcoshθ), |
in which r(s) satisfies
κ21+1r2=−λ(1+C1r′), |
where λ and C1 are non-zero constants and
κ1=−r″rr″+r′2+1. |
Theorem 4.5. A canal surface M12− has proper pointwise 1-type Gauss map of the first kind if and only if it is minimal. Precisely, it is a part of a surface of revolution as
x(s,θ)=(s+r(s)sinhφ(s),r(s)coshφ(s)sinhθ,r(s)coshφ(s)coshθ), |
in which r(s) satisfies
s=c2±∫√rc1−rdr,(c1>r,c2∈R). |
Corollary 4.6. A canal surface M12− with proper pointwise 1-type Gauss map of the first kind satisfies
ΔG=−2KG=−2r2G. |
Corollary 4.7. A canal surface M12− has 1-type Gauss map of the first kind if and only if it is a circular cylinder.
Corollary 4.8. The canal surface M12− with harmonic Gauss map does not exist.
From Eq (2.3), the canal surface M2− is parameterized by
x(s,θ)=c(s)+r(s)(coshφ(s)T+sinhφ(s)cosθN+sinhφ(s)sinθB), |
where −coshφ(s)=r′(s).
Through direct calculations, we have
xs=x1sT+x2sN+x3sB, xθ=x1θN+x2θB, |
where
x1s=−rr″+rκsinhφcosθ−sinh2φ;x2s=r′sinhφcosθ−rr′κ−rr′φ′cosθ+rτsinhφsinθ;x3s=r′sinhφsinθ−rτsinhφcosθ−rr′φ′sinθ;x1θ=−rsinhφsinθ;x2θ=rsinhφcosθ. |
Then, the Gauss map G of M2− is
G=−coshφT−sinhφcosθN−sinhφsinθB, | (5.1) |
which point outwards M2− and ⟨G,G⟩=−1.
Meanwhile, the component functions of the first fundamental form are obtained as
g11=P23+r2R23sinh2φ, g12=r2R3, g22=r2sinh2φ, | (5.2) |
the component functions of the second fundamental form are written by
h11=−rR23+P3Q3sinh2φ, h12=−rR3, h22=−rsinh2φ, | (5.3) |
where
P3=rr″−rκsinhφcosθ+sinh2φ=rQ3+sinh2φ,Q3=r″−κsinhφcosθ,R3=τsinh2φ+r′κsinhφsinθ. |
From Eqs (5.2) and (5.3), the Gaussian curvature K and the mean curvature H of M2− are
K=−Q3rP3, H=2P3−sinh2φ2rP3. | (5.4) |
Remark 5.1. From g11g22−g212=r2P23, due to regularity, we see that P3≠0 everywhere.
In the following, the Laplacian of the Gauss map G of M2− is to be calculated. First, from the first fundamental form of M2−, we have
g11=sinh2φP23, g12=−R3P23, g22=P23+r2R23r2P23sinh2φ. | (5.5) |
Substituting (5.1), (5.2) and (5.5) into (1.1), and by putting
U3=g22Hs−g12Hθ, V3=−g12Hs+g11Hθ, |
where
Hs=−2r2r′κ2sinh2φcos2θ+r2r′r″κsinhφcosθ−2rr′r″sinh2φ+r2r‴sinh2φ−4r2r′r″22r2P23+(2rr′κ−r2κ′)sinh3φcosθ−r′sinh4φ2r2P23,Hθ=κsinh3φsinθ2P23, |
after complicated arrangements, we get
ΔG=1r2P23{[(r2Q23+P23)coshφ+2x1sU3]T+[(r2Q23+P23)sinhφcosθ+2(x2sU3+x1θV3)]N+[(r2Q23+P23)sinhφsinθ+2(x3sU3+x2θV3)]B}. |
Do discussions similar to those of M11− and M12−, the following results for M2− can be given directly.
Theorem 5.2. A canal surface M2− has proper pointwise 1-type Gauss map of the second kind if and only if it is a surface of revolution with the following form
x(s,θ)=(r(s)sinhφsinθ,r(s)sinhφcosθ,s+r(s)coshφ), |
in which r(s) satisfies
κ1(κ1−1r)′=−(ln|1+C1r′|)′(κ21+1r2), |
where C1 is a non-zero constant and κ1 is the principal curvature as
κ1=−r″rr″+r′2−1. |
Corollary 5.3. A canal surface M2− with proper pointwise 1-type Gauss map of the second kind satisfies ΔG=f(G+C) for a constant vector C=(C1,0,0) and non-zero smooth function
f(s)=−4H2+2K1+C1r′, |
where C1 is a non-zero constant, H and K are given by
K=−r″r(rr″+r′2−1), H=2rr″+r′2−12r(rr″+r′2−1). |
Corollary 5.4. A canal surface M2− has 1-type Gauss map of the second kind if and only if it is a surface of revolution represented as
x(s,θ)=(r(s)sinhφsinθ,r(s)sinhφcosθ,s+r(s)coshφ), |
in which r(s) satisfies
κ21+1r2=−λ(1+C1r′), |
where λ and C1 are non-zero constants and
κ1=−r″rr″+r′2−1. |
Theorem 5.5. A canal surface M2− has proper pointwise 1-type Gauss map of the first kind if and only if it is minimal. Precisely, it is a part of a surface of revolution as
x(s,θ)=(r(s)sinhφsinθ,r(s)sinhφcosθ,s+r(s)coshφ), |
in which r(s) satisfies
s=c2±∫√rc1+rdr,(c1>−r,c2∈R). |
Corollary 5.6. A canal surface M2− with proper pointwise 1-type Gauss map of the first kind satisfies
ΔG=−2KG=−2r2G. |
Corollary 5.7. The canal surface M2− with 1-type Gauss map of the first kind does not exist.
Proof. Assume that a canal surface M2− satisfies ΔG=λG, (λ∈R−{0}). By Corollary 5.6, we have λ=−2r2 is a constant, i.e., r is a constant. Notice that the radial function r(s) can't be constant for M2−, therefore, we get contradiction.
Corollary 5.8. The canal surface M2− with harmonic Gauss map does not exist.
Until now, the canal surfaces M11−, M12− and M2− foliated by pseudo hyperbolic spheres H20 along the first kind spacelike curve, the second kind spacelike curve and a timelike curve, respectively have been classified in terms of their Gauss maps. The similar works for the canal surfaces M11+, M12+ and M2+ have been done in another recent work. The canal surfaces M13−, M3− (M13+, M3+) foliated by pseudo hyperbolic spheres H20 (resp. pseudo spheres S21) along a null type spacelike curve or a null curve are to be investigated in the continued works.
We thank the referee for the careful review and the valuable comments to improve the paper. The authors are supported by NSFC (11801065) and the Fundamental Research Funds for the Central Universities (N2005012 and N2005016) and the National Research Foundation of Korea (NRF) grant funded by the Korea government (MSIP) (NRF-2018R1A2B2002046) and the 2021 scientific promotion program funded by Jeju National University.
The authors declare that there is no conflict of interest.
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