# Canal surfaces in 4-dimensional euclidean space

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Vol.7, No.1, pp.83-89 (2017)

http://doi.org/10.11121/ijocta.01.2017.00338

RESEARCH ARTICLE

### Canal surfaces in 4-dimensional Euclidean space

Bet¨ul Bulcaa, Kadri Arslana, Beng¨u Bayramb and G¨unay ¨Ozt¨urkc*, aDepartment of Mathematics, Uluda˘g University, 16059 Bursa, Turkey bDepartment of Mathematics, Balikesir University, 10145 Balikesir, Turkey cDepartment of Mathematics, Kocaeli University, 41380 Kocaeli, Turkey

bbulca@uludag.edu.tr,arslan@uludag.edu.tr, benguk@balikesir.edu.tr, ogunay@kocaeli.edu.tr

ARTICLE INFO ABSTRACT

Article History: Received 26 April 2016 Accepted 22 November 2016 Available 13 December 2016

In this paper, we study canal surfaces imbedded in 4-dimensional Euclidean space E4

. We investigate these surface curvature properties with respect to the variation of the normal vectors and ellipse of curvature. Some special canal surface examples are constructed in E4

. Furthermore, we obtain necessary and sufficient condition for canal surfaces to become superconformal in E4

. At the end, we present the graphs of projections of canal surfaces in E3

. Keywords: Canal surface Curvature ellipse Superconformal surface AMS Classification 2010: 53C40, 53C42

Given a space curve γ (u) called spine curve, a canal surface associated to this curve is defined as a surface swept by a family of spheres of vary-ing radius r(u). If r(u) is constant, the canal surface is called a tube or a pipe surface. Apart from being used in pure mathematics, canal sur-faces are widely used in many areas especially in CAGD, e.g. construction of blending surfaces, i.e. canal surface with a rational radius, shape recon-struction or robotic path planning (see, [5], [11], [12]). Greater part of the studies on canal sur-faces within the CAGD context is related to the search of canal surfaces with rational spine curve and rational radius function. Canal surfaces are also useful in visualising long thin objects such as poles, 3D fonts, brass instruments or internal organs of the body in solid/surface modeling and CG/CAD. A national question is when the canal surface is developable. It is well known that, at regular points, the Gaussian curvature of a devel-opable surface is identically zero. In [14] it has been proved that developable canal surface is ei-ther a cylinder or a cone.

This study consists of 5 sections: In section 2, we explain some well-known properties of the sur-faces in E4. In section 3, we give the canal surfaces in E4 and some examples are presented. Section 4

investigates the ellipse of curvature of canal sur-faces in E4. Additionally we prove necessary and sufficient condition of canal surfaces to become superconformal in E4. In Section 5, the visualiza-tion of canal surfaces are given with using Maple programme.

1. Basic concepts

Let M be a regular surface in E4 given with the parametrization X(u, v) : (u, v) ∈ D ⊂ E2. The tangent space of M at an arbitrary point p = X(u, v) is spanned by the vectors Xu and

Xv. The first fundamental form coefficients of M

are computed by

E= hXu, Xui, F = hXu, Xvi , G = hXv, Xvi , (1)

where h, i is the scalar product of the Euclidean space. We consider the surface patch X(u, v) is regular, which implies that W2= EG − F2 6= 0. For the point p ∈ M, we can take the decompo-sition TpE4 = TpM ⊕ Tp⊥M, where Tp⊥M is the

*Corresponding Author

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orthogonal component of TpM in E4 with the

Rie-mannian connection∇.

The induced Riemannian connection ∇ on M for any given local vector fields X1, X2 tangent to M ,

is given by

∇X1X2= ( e∇X1X2)

T, (2)

where T expresses the tangential part.

Let us consider the spaces of the smooth vector fields χ(M ) and χ⊥(M ) which are tangent and

normal to M , respectively. The second funda-mental map is defined as follows:

h : χ(M ) × χ(M ) → χ⊥(M )

h(Xi, Xj) = ∇eXiXj − ∇XiXj 1 ≤ i, j ≤ 2. (3)

This map is well-defined, symmetric and bilinear. If we take the orthonormal frame field {N1, N2} of

M, then the shape operator which is self-adjoint and bilinear can be given by

A : χ⊥(M ) × χ(M) → χ(M) ANiXi = −( e∇XiNi)

T, X

i ∈ χ(M) (4)

which satisfies the equation:

hANkXj, Xii = hh(Xi, Xj), Nki = c

k

ij, 1 ≤ i, j, k ≤ 2

(5)

for any X1, X2∈ TpM.

The equality (3) is known as the Gaussian equa-tion, where ∇XiXj = 2 X k=1 ΓkijXk , 1 ≤ i, j ≤ 2 (6) and h(Xi, Xj) = 2 X k=1 ckijNk 1 ≤ i, j ≤ 2. (7) Here Γk

ij are Christoffel symbols and ckij are the

coefficients of the second fundamental form. The Gaussian curvature are given by

K=hh(X1, X1), h(X2, X2)i − kh(X1, X2)k

2

g (8)

and the mean curvature are given by

kHk = 1

4g2hh(X1, X1)+h(X2, X2), h(X1, X1)+h(X2, X2)i (9) where

g= kX1k2kX2k2− hX1, X2i2.

If the mean curvature of M vanishes identically in En, then M is said to be minimal [3]. See also

[1].

2. Canal surfaces in E4

Let γ(u) = (f1(u), f2(u), f3(u), 0) be a curve given

with arclength parameter. Then the Frenet for-mulae have the following form:

γ′(u) = e1(u),

e1′(u) = κ(u)e2(u),

e2′(u) = −κ(u)e1(u) + τ (u)e3(u), (10)

e3(u) = −τ(u)e2(u), e4′(u) = 0,

where {e1(u), e2(u), e3(u), e4(u)} is the Frenet

or-thonormal basis of γ. The canal surface in E4 has the following parametrization (see [6]):

M : X(u, v) = γ(u) + r(u) (e3(u) cos v + e4(u) sin v) .

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Example 1. Consider the helix γ(u) = (a cosu

c, asin u c,

bu

c) in E3. Then the canal

sur-face of γ in E4 has the following parametrization

X(u, v) = (a cosu c + b cr(u) sin u c cos v, asinu c − b cr(u) cos u c cos v, (12) bu c + a

cr(u) cos v, r(u) sin v).

Example 2. Consider the generalized helix γ(u) = ((1+u) 3 2 3 ,(1−u) 3 2 3 , u √ 2) in E

3. Then the canal

surface of γ in E4 has the following

parametriza-tion X(u, v) = ((1 + u) 3 2 3 − r(u) (1 + u)12 2 cos v, (1 − u)32 3 + r(u) (1 − u)12 2 cos v, (13) u √ 2 + 1 √

(3)

The space which is tangent to M is spanned by Xu = e1(u) − rτ cos ve2

+r′cos ve

3+r′sin ve4, (14)

Xv = −r sin ve3+r cos ve4.

The first fundamental form coefficients become E = 1 + (r′)2+ r2τ2cos2v,

F = 0, (15)

G = r2. The Christoffel symbols Γk

ij are given by Γ111 = 1 2E∂u(E) = 1 E hXuu, Xui , Γ211 = − 1 2G∂v(E) = − 1 GhXvu, Xui , Γ112 = 1 2E∂v(E) = 1 E hXvu, Xui , (16) Γ212 = 1 2G∂u(G) = 1 GhXvu, Xvi , Γ122 = − 1 2E∂u(G) = − 1 E hXvu, Xvi , Γ222 = 1 2G∂v(G) = 1 GhXvv, Xvi = 0. and they are symmetric according to the covari-ant indices ([7], p.398).

If we take the second partial derivatives of X(u, v), we find:

Xuu = κrτcos ve1+ (κ − (rτ)′cos v − r′τcos v)e2

+ cos v(r′′− rτ2)e3+ r′′sin ve4,

Xuv = rτsin ve2− r′sin ve3+ r′cos ve4, (17)

Xvv = −r cos ve3− r sin ve4,

Hence, by using (3), we find the Gaussian equa-tions; e ∇XuXu = Xuu= ∇XuXu+ h(Xu, Xu), e ∇XuXv = Xuv= ∇XuXv+ h(Xu, Xv),(18) e ∇XvXv = Xvv= ∇XvXv+ h(Xv, Xv), where ∇XuXu = Γ 1 11Xu+ Γ211Xv, ∇XuXv = Γ 1 12Xu+ Γ212Xv, (19) ∇XvXv = Γ 1 22Xu+ Γ222Xv.

Substituting (16) and (18) in (19), we obtain

h(Xu, Xu) = Xuu− 1 Eh Xuu, Xui Xu +1 GhXuv, Xui Xv, h(Xu, Xv) = Xuv− 1 EhXuv, Xui Xu (20) −1 GhXuv, Xvi Xv, h(Xv, Xv) = Xvv+ 1 EhXuv, Xvi Xu. Further using (20) hh(Xu, Xu), h(Xv, Xv)i = hXuu, Xvvi −1 EhXuu, Xui hXvv, Xui , hh(Xu, Xv), h(Xu, Xv)i = hXuv, Xuvi −1 EhXuv, Xui 2 −1 GhXvu, Xvi 2 , hh(Xu, Xv), h(Xv, Xv)i = hXuv, Xvvi −1 EhXuv, Xui hXvv, Xui , (21) hh(Xu, Xu), h(Xu, Xu)i = hXuu, Xuui −1 EhXuu, Xui 2 +hXuv, Xui G (2 hXuu, Xvi + hXuv, Xui) , hh(Xv, Xv), h(Xv, Xv)i = hXvv, Xvvi +1 EhXuv, Xvi (1 + 2 hXvv, Xui), hh(Xu, Xu), h(Xu, Xv)i = hXuu, Xuvi − 1 EhXuv, Xui −1 GhXuu, Xvi hXuv, Xvi

Thus, using (14) with (17) we get

hXuu, Xvvi = r2τ2cos2v− rr′′, hXuv, Xuvi = r2τ2sin2v+ (r′)2, hXuu, Xuui = (κrτ cos v)2 +(κ − (rτ)′cos v − r′τcos v)2+ + cos2v(r′′− rτ2)2+ (r′′)2sin2v, hXvv, Xvvi = r2, (22) hXuu, Xui = rτ(rτ)′cos2v+ r′r′′, hXuu, Xvi = r2τ2cos v sin v, hXvv, Xui = −rr′, hXuv, Xui = −r2τ2cos v sin v, hXuv, Xvi = rr′, hXuv, Xvvi = 0 hXuu, Xuvi = rτ sin v(κ − (rτ)′cos v)

Proposition 1. The Gaussian curvature of the canal surface M with the parametrization (11) in E4 is given by K = 1 g(hXuu, Xvvi − 1 EhXuu, Xui hXvv, Xui (23) −hXuv, Xuvi + 1 EhXuv, Xui 2 + 1 GhXuv, Xvi 2 ) where g = EG − F2.

Proof. By using the equation (8), we find

K= 1

g(hh(Xu, Xu), h(Xv, Xv)i − hh(Xu, Xv), h(Xu, Xv)i) , (24)

which is the Gaussian curvature of the canal sur-face M . Taking into account (21) and (24) we

obtain (23). 

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Corollary 1. The Gaussian curvature of the canal surface M with the parametrization (11) in E4 is given by K = r gE{r cos 2 v(2τ2+ 2(r′)2τ2− rr′′τ2+ r′τ(rτ )′) +r3 τ4cos4 v− r′′− rτ2 (1 + (r′)2 )}, (25) where E = 1 + (r′)2+ r2τ2cos2v, g = r2(1 + (r′)2+ r2τ2cos2v).

Proposition 2. The mean curvature of the canal surface M with the parametrization (11) in E4 is given by 4 kHk2 = hXuu, Xuui E2 + 2 hXuu, Xvvi EG + hXvv, Xvvi G2 +hXuv, Xvi EG2 (2 hXvv, Xui + hXuv, Xvi) (26) +hXuv, Xui E2G (2hXuu, Xvi + hXuv, Xui) − 2 E2GhXuu, XuihXvv, Xui − hXuu, Xui2 E3 .

Proof. By considering (9) the mean curvature of the canal surface M becomes

kHk = 1

4g2(hh(Xu, Xu) + h(Xv, Xv), h(Xu, Xu) + h(Xv, Xv)i) ,

(27)

Taking into account (21) and (27) we get the

result. 

By the use of (22) and Proposition 2, we have the following results:

Corollary 2. The mean curvature of the canal surface M with the parametrization (11) in E4 is given by kHk2 = 1 4E2r2[− r2 E(rτ (rτ ) ′cos2 v+ r′r′′)2 +r2cos2v((τ kr)2+ ((rτ )′+ rτ)2 − r2τ4+ 4τ2+ +3(r′)2 τ2− 2rτ2r′′+ 2rτ(rτ )) +4r4τ4cos4v− 2kr2cos v((rτ )′+ rτ) + +k2r2− 2rr′′+ 1 + (r)2 ].

Corollary 3. If the base curve γ of the canal sur-face M is a straight line, then the Gaussian and mean curvatures of M are

K = −r′′ r(1 + (r′)2)2, and kHk2 = −1 4r2(1 + (r)2)3  (rr′r′′)2 +(2rr′′− 1)(1 + (r′)2) , respectively.

3. Ellipse of curvature of the canal surfaces in E4

Let M be a regular surface given with the parametrization X (u, v) : (u, v) ∈ D ⊆ E2.

Con-sider a circle given with the angle θ ∈ [0, 2π]

in the tangent space TpM. The intersection of

the direct sum of the tangent direction of X = cos θX1+sin θX2and the normal space Tp⊥Mwith

the surface M forms a curve. Such a curve is called as a normal section curve in the direction θ. Denote this curve by γθ. Normal curvature

vec-tor ηθ of γθ lies in Tp⊥M. When θ changes from 0

to 2π, the normal curvature vector constitutes an ellipse called as a ellipse of curvature of M at p in T⊥

p M. Thus, the curvature ellipse of M at point

pis given as follows with the second fundamental form h:

E(p) = {h(X, X) | X ∈ TpM, kXk = 1} .

To see that this shows an ellipse, it is enough to have a look at the formulas

X= cos θX1+ sin θX2 and h(X, X) =−→H+ cos 2θ−→B + sin 2θ−→C . (28) Here, − → B = 1 2(h(X1, X1) − h(X2, X2)), − → C = h(X1, X2), (29)

are normal vectors and −→H = 1

2(h(X1, X1) +

h(X2, X2)) is the mean curvature vector. This

im-plies that, the vector h(X, X) goes twice around the ellipse of curvature centered at −→H, while X goes once around the unit tangent circle [9]. From the equation (28), one can get that E(p) is a circle if and only if for some orthonormal basis of Tp(M ) it holds that

hh(X1, X2), h(X1, X1) − h(X2, X2)i = 0, (30)

and

kh(X1, X1) − h(X2, X2)k = 2 kh(X1, X2)k .

(31) General aspects of the ellipse of curvature for sur-faces in E4 studied by Wong [13]. (See also [2],

[8], [9] and [10])

Definition 1. The surface M with the parametrization X (u, v) in E4 is superconformal if and only if its ellipse of curvature is a circle, i.e. D−→B ,−→CE= 0 and −→B = −→C holds [4]. If the equality D−→B ,−→CE= 0, the surface M is called weak superconformal.

Theorem 1. The canal surface M with the parametrization (11) in E4 is superconformal if

and only if the equalities

h1 Eh(Xu, Xu) − 1 Gh(Xv, Xv), 1 √ EGh(Xu, Xv)i = 0 (32)

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and 2 1 √ EGh(Xu, Xv) = 1 Eh(Xu, Xu) − 1 Gh(Xv, Xv) (33) hold.

Proof. If we use the orthonormal frame X1= Xu kXuk = √Xu E, X2 = Xv kXvk = √Xv G, (34) we get h(X1, X1) = 1 Eh(Xu, Xu), h(X1, X2) = √1 EGh(Xu, Xv), (35) h(X2, X2) = 1 Gh(Xv, Xv) .

Therefore, from (29) the normal vectors −→B and − →C become − →B = 1 2( 1 Eh(Xu, Xu) − 1 Gh(Xv, Xv)) (36) and − →C = √1 EGh(Xu, Xv). (37) Suppose M is superconformal then by Definition 1 h−→B ,−→Ci = 0 and −→B = −→C hold. Thus by the use of the equalities (36) and (37) we get the result.

Conversely, if the equations (32) and (33) hold then by the use of the equalities (36) and (37)

we obtain h−→B ,−→Ci = 0 and −→B = −→C , which shows that M is superconformal.  Substituting (21) and (22) into (32) we obtain the following results.

Corollary 4. Let M be a canal surface in E4

given with the parametrization (11). Then M is weak superconformal if and only if the equality

0 = r3τsin v((k − (rτ)′cos v)(1 + (r)2)

+rτ cos v(r′r′′+ krτ cos v))

holds.

Corollary 5. Every canal surface whose spine curve is a straight line of the form γ(u) = (a1u+

b1, a2u+ b2, a3u+ b3,0) is weak superconformal,

where a1, a2, a3, b1, b2, b3 are real constants. 4. Visualization

The 3D-surfaces geometric modeling are very im-portant in the surface modeling systems such as; CAD/CAM systems and NC-processing. We give the visualization of the surfaces with the parametrization

X(u, v) = (x(u, v), y(u, v), z(u, v), w(u, v)) in E4 by use of Maple Software Program. We plot the graph of the surface with plotting command

plot3d([x, y, z + w], u = a..b, v = c..d). (38) We construct the geometric model of the canal surfaces defined in Example 1 for the following values (see, Figure 1);

(a) (b)

(c)

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(a) (b)

(c)

Figure 2. The projections of canal surfaces of general helix in E3

(a) (b)

Figure 3. The projections of canal surfaces of straight line in E3

a) r(u) = eu/3, b) r(u) = u2, c) r(u) = 3u + 5.

Further, we construct the geometric model of the canal surfaces defined in Example 2 for the following values (see, Figure 2); a) r(u) = eu 2 , b) r(u) = 5u2, c) r(u) = 3u + 5.

Additionally, we construct the geometric model of the canal surfaces defined in Corollary 3 for the following values (see, Figure 3);

a) r(u) = eu, b) r(u) = sinh u.

5. Conclusion

In this manuscript, we considered canal surfaces in the 4-dimensional Euclidean space E4

. Most of the literature on canal surfaces within the CAGD context has been moti-vated by the observation that canal surfaces with rational spine curve. We have proved this property mathematically and also illustrated with some nice examples.

References

[1] Arslan, K., Bayram, K. B., Bulca, B. and ¨Ozt¨urk, G., Generalized rotation surfaces in E4

. Results in Math-ematics, 61, 315-327 (2012).

[2] Bayram, K. B., Bulca, B., Arslan, K. and ¨Ozt¨urk, G., Superconformal ruled surfaces in E4

. Mathemati-cal Communications, 14(2), 235-244 (2009).

[3] Chen, B. Y., Geometry of submanifolds. Dekker, New York, (1973).

[4] Dajczer, M. and Tojeiro, R., All superconformal sur-faces in R4

in terms of minimal surfaces. Mathematis-che Zeitschrift, 261, 869-890 (2009).

[5] Farouki, R.T. and Sverrissor, R., Approximation of rolling-ball blends for free-form parametric surfaces. Computer-Aided Design, 28, 871-878 (1996).

[6] Gal, R.O. and Pal, L., Some notes on drawing twofolds in 4-dimensional Euclidean space. Acta Univ. Sapien-tiae, Informatica, 1-2, 125-134 (2009).

[7] Gray, A., Modern differential geometry of curves and surfaces. CRC Press, Boca Raton Ann Arbor London Tokyo, (1993).

[8] Mello, L. F., Orthogonal asymptotic lines on surfaces immersed in R4

. Rocky Mountain J. Math., 39(5), 1597-1612 (2009).

[9] Mochida, D. K. H., Fuster, M.D.C.R and Ruas, M.A.S., The geometry of surfaces in 4-Space from a

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contact viewpoint. Geometriae Dedicata., 54, 323-332 (1995).

[10] Rouxel, B., Ruled A-submanifolds in Euclidean space E4

. Soochow J. Math., 6, 117-121 (1980).

[11] Shani, U. and Ballard, D.H., Splines as embeddings for generalized cylinders. Computer Vision,Graphics and Image Processing, 27, 129-156 (1984).

[12] Wang, L., Ming, C.L., and Blackmore, D., Generat-ing sweep solids for NC verification usGenerat-ing the SEDE method. Proceedings of the Fourth Symposium on Solid Modeling and Applications, Atlanta, Georgian, May 14-16, 364-375 (1995).

[13] Wong, Y.C., Contributions to the theory of surfaces in 4-space of constant curvature. Trans. Amer. Math. Soc., 59, 467-507 (1946).

[14] Xu, Z., Feng, R. and Sun, JG., Analytic and algebraic properties of canal surfaces. Journal of Computational and Applied Mathematics, 195(1-2), 220-228 (2006).

Bet¨ul Bulca is currently an asistant professor at Uludag University in Turkey. Her research interests include curves and surfaces.

Kadri Arslanis currently a professor at Uludag Uni-versity in Turkey. His research interests include curves and surfaces.

Beng¨u Bayramis currently an associate professor at Balikesir University in Turkey. Her research interests include curves and surfaces.

G¨unay ¨Ozt¨urkis currently an associate professor at Kocaeli University in Turkey. His research interests include curves and surfaces.

An International Journal of Optimization and Control: Theories & Applications (http://ijocta.balikesir.edu.tr)

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