Brander, David

Gravesen, Jens

Surfaces foliated by planar geodesics are a natural model for surfaces made from wood strips. We outline how to construct all solutions, and produce non-trivial examples, such as a wood-strip Klein bottl

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Downloaded from orbit.dtu.dk on: Apr 10, 2018Surfaces foliated by planar geodesics: a model forcurved wood designBrander, David; Gravesen, JensPublished in:Proceedings of Bridges 2017Publication date:2017Document VersionPeer reviewed versionLink back to DTU OrbitCitation (APA):Brander, D., & Gravesen, J. (2017). Surfaces foliated by planar geodesics: a model forcurved wood design. In D.Swart, C. Séquin, & K. Fenyvesi (Eds.), Proceedings of Bridges 2017 (pp. 487–490 ). Tessellations Publishing.Surfaces Foliated by Planar Geodesics:A Model for Curved Wood DesignDavid BranderDept. of Applied Math. & Comp. Sci,Technical University of DenmarkJens GravesenDept. of Applied Math. & Comp. Sci,Technical University of DenmarkAbstractSurfaces foliated by planar geodesics are a natural model for surfaces made from wood strips. We outline how toconstruct all solutions, and produce non-trivial examples, such as a wood-strip Klein bottle.IntroductionThe construction of curved surfaces by bending flat strips of wood and placing them side by side has a longhistory. In some settings, such as in the design of furniture or art-works, a curved surface is wanted foraesthetic reasons. In other applications, such as ship-building or air-craft design (Figure 1, left), the need fora curved surface is dictated by practical considerations, e.g., aerodynamic efficiency.Mathematically, any regular surface can be approximated by such a wood-strip construction, simply bychoosing some 1-parameter family of geodesics (Figure 1) that covers the surface (several patches might beneeded). A geodesic is a curve that only bends in the direction perpendicular to the surface. Thus, laying awooden strip along a geodesic means that the normal vector to the strip is parallel to the normal vector to thesurface being modeled. In other words, the strips are tangent to the surface – at least along their centerlines.Figure 1 : Left: curved wooden boats. Middle: geodesics on a cylinder. Right: non-geodesic curves.For practical assembly, the bending of the strips must be achieved by fixing the positions of variouspoints with, for example cross-beams. If the curve that the strip follows is planar, then the shape of the curvebetween these fixed points is predictable, independent of the material or thickness of the strip, provided noplastic deformation occurs. Moreover, a wood strip can follow the curve with no twisting. It is desirable,therefore, to find a 1-parameter family of planar geodesics. Such a family cannot be expected to exist onan arbitrary surface. Therefore, the problem of mathematically designing a surface for wood strip assemblyinvolves first understanding how to generate the right kind of surface, and this is the main purpose of thisarticle. Note that the considerations above apply equally well if we replace wood with paper or cardboard,both popular media for artistic expression.Surfaces Foliated by Planar GeodesicsA family of smoothly varying curves that sweeps out a surface (such as one of the families of coordinate linesin a parameterization) is called a foliation. We are interested in the case that each curve is a planar geodesic.Figure 2 : Hyperboloid. Left, Middle: as a ruled surface. Right: as a surface of revolution.The most obvious example is a ruled surface, i.e., a surface swept out by a family of straight lines, such asthe hyperboloid in Figure 2. However, ruled surfaces are an exceptional case because a given line lies ininfinitely many planes, unlike a typical plane curve. Moreover, a line does not have a unique normal vector,so there are many different ways to lay a wood strip along it: two choices are shown in Figure 2. Finally,and most importantly, the surface normal is not usually constant along a ruling: thus, it is not possible to laya wood strip along the ruling in such a way that the normal of the wood strip is the same as the normal tothe underlying surface without twisting the wood. The exception to this is a developable surface defined tobe a ruled surface in which the surface normal is constant along each of the rulings. These are the only ruledsurfaces that satisfy the followingDefinition. A planar geodesic foliation (PGF) is a surface foliated by planar geodesic curves such that,along each of these planar curves, the normal to the surface is parallel to the plane containing the curve.Πvq1q2γv1Figure 3 : A subset (striped) of a ro-tational surface is also foliated byplanar geodesics.Rotational Surfaces: Although not developable, the hyper-boloid nevertheless qualifies as a PGF, because it happens tobe an instance of a second well known type of surface foli-ated by planar geodesics: a surface of revolution. Take a pro-file curve γ0(u) = (f(u), 0, g(u)) in the xz-plane, and thenrotate this plane about the z-axis by angle v to get a newplane Πv. As v varies, the curve sweeps out a surface of rev-olution x(u, v) = (cos(v)f(u), sin(v)f(u), g(u)) (Figure 3).As is well-known, the plane Πv is orthogonal to the surfaceof revolution, and this implies that each iso-curve γv0(u) =(cos(v0)f(u), sin(v0)f(u), g(u)) is a geodesic.Monge Surfaces: A surface of revolution is obtained from a planecurve by a perpendicular sweep of the plane along a circle. If wereplace the circle with an arbitrary space curve, the spine curve,that is always perpendicular to the moving plane, we have a Mongesurface ([4], §XXV). Again, each iso-curve γv(u) = x(u, v) isa planar geodesic. (See Figure 4). Note that both developablesurfaces and surfaces of revolution are also Monge surfaces.Constructing a Monge surface: Given a plane Π (which contains the profile curve γ0), and a candidatedifferentiable space curve r(v) for the spine curve, with r′(v0) perpendicular to Π, one can take advan-tage of the so-called minimal rotating frame (MRF) defined by R. Bishop [1]. Take an orthonormal basisQ1, Q2 for Π: then there is a unique orthonormal frame field (t(v),q1(v),q2(v)) that evaluates at v0 to(r′(v0)/|r′(v0)|, Q1, Q2), and such that the derivatives of the frame vectors have components only in thedirection r′(v). The plane Πv = span(q1(v),q2(v)) remains perpendicular to the spine curve for all v, and aMonge surface is swept out by γ0 as the plane moves. The frame is calculated by solving an ODE (see [2]).Figure 4 : Monge surfaces: the middle and right surface have the same spine curve (red) butdifferent profile curves.It follows from the above that a Monge surface can be parameterized as:x(u, v) = r(v) + x(u)q1(v) + y(u)q2(v) , (1)with r a space curve with MRF (t = r′/|r′|,q1,q2), and each iso-curve γv(u) = x(u, v) is then a geodesic.How to Produce All Planar Geodesic FoliationsFrom the point of view of designing with wood strips, it’s obvious to ask now whether there are any otherPGF’s, besides Monge surfaces. To better understand this question, let’s consider one more application ofPGF’s. In architecture, a new method for production of formwork for curved surfaces is robotic hot-bladecutting [3]. A heated blade or rod sweeps out a surface by melting through polystyrene foam, to create amould for concrete casting. The shape of the blade can change dynamically during the motion, to createcomplex geometry; for stability and control, the blade is constrained always to form a plane curve. If a flatblade is used then it’s not hard to see that, in order to progress smoothly, the sweeping direction needs to beorthogonal to the plane that the blade is curving in, so the blade is sweeping out planar geodesics, and thesurface is a PGF. If the surface is a Monge surface, then the shape of the blade (the profile curve) remainsfixed during the sweeping, and this is clearly a severe restriction. Therefore, it’s interesting to ask: can theshape of the “profile curve” change dynamically during the sweeping? The answer to this is “no”:Theorem. Every planar geodesic foliation can be locally parameterized as a Monge surface.Proof. (Outline). Given a PGF, we can assume the surface is locally parameterized as (u, v) 7→ x(u, v),where the iso-curve γv0(u) := x(u, v0) is a planar unit-speed geodesic for each fixed v0. Now, varying vgives us a 1-parameter family Π(v) of planes in R3. Let N(v) be the family of normals to these planes. Byintegrating r′(v) = N(v), with r(v0) = x(u0, v0), we obtain a curve r(v), the spine curve, that intersectsthe planes orthogonally. Let (t,q1,q2) be a minimal rotating frame along r. Since each curve γv lies in theplane through r(v) spanned by qi(v), we can writex(u, v) = r(v) + x(u, v)q1(v) + y(u, v)q2(v) . (2)A short argument (see [2]) then shows that each iso-curve αv(u) = (x(u, v), y(u, v)) is a just a reparame-terization of a single curve αv0(u). We can then reparameterize the surface so that x(u, v) and y(u, v) areindependent of v, which is the claim of the theorem.Closed Spine CurvesFigure 5 : A non-closingPGF surface with closedspine curve.The theorem above generates essentially all PGF’s from the ingredientsof a planar profile curve γ0(u), a space curve r(v), and a choice of initialvectors Qi in the plane perpendicular to r(v0). If the spine curve r(v) is aclosed curve, i.e., if r(v + P ) = r(v) for some P , it does not follow thatthe profile curve returns to its original position after passing around theloop, to form a closed surface (see Figure 5): the other tangent direction,or equivalently the minimal rotating frame, of the surface needs to closeup as well. This is a property of the spine curve alone.In [2] we give a method to produce closed spine curves with suchclosed MRF’s. A brief outline: assume that r(v) has a well-defined nor-mal n and binormal b. The Frenet frame (t,n,b) is closed (as r isclosed) but is not an MRF. In fact, the torsion τ of the curve, given byb′(v) = τ(v)n(v), is the rate of rotation of the normal plane Πv in thebasis (n,b) compared with the zero rotation of the MRF. Hence, the MRF also closes up if and only if2mpi =∫τds =∫b′ds = length of b, for some m ∈ Z.We first find a candidate periodic binormal function b. A result of Fenchel states that a necessary andsufficient condition for a closed curve b in the 2-sphere to be the binormal for a closed space curve is thatthe tangent geodesic curves of the trace of b cover the whole sphere. It is not difficult to find such curves,and scale them so that the above closing conditions are satisfied. From there, one can solve a linear systemon (for example) a space of polynomial splines to find the curvature and torsion for the desired curve r.If we instead take b with length an odd multiple of pi, we can obtain a PGF Mo¨bius strip, provided thatthe profile curve is invariant under a rotation of pi. A figure-8 profile curve gives a Klein bottle, (Figure 6).Figure 6 : Two PGF Mo¨bius strips (the first developable), and an immersed Klein bottle.Using the Methods in this ArticleMore details can be found in [2], and some code is available at http://geometry.compute.dtu.dk/software. Forour images, we used the solutions to create wood-strip models by taking a subset of the planar geodesics andlaying ruled strips along these curves. At each point on a curve, the width of the strip is proportional to thedistance to the adjacent curves. Code to produce these wood-strip models is also available at the above link.References[1] R Bishop. There is more than one way to frame a curve. Amer. Math. Monthly, 82:246–251, 1975.[2] D Brander and J Gravesen. Monge surfaces and planar geodesic foliations. In preparation.[3] D Brander et al. Designing for hot-blade cutting: geometric approaches for high-speed manufacturingof doubly-curved architectural surfaces. In Advances in Architectural Geometry, pages 306–327. 2016.[4] G Monge. Application de l’analyse a la ge´ome´trie. Bachelier, Paris, fifth edition, 1850.

Surfaces foliated by planar geodesics: a model forcurved wood design

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Surfaces foliated by planar geodesics: a model forcurved wood design

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