A Characterization of Helical Polynomial Curves of Any Degree

Total Page:16

File Type:pdf, Size:1020Kb

A Characterization of Helical Polynomial Curves of Any Degree A CHARACTERIZATION OF HELICAL POLYNOMIAL CURVES OF ANY DEGREE J. MONTERDE Abstract. We give a full characterization of helical polynomial curves of any degree and a simple way to construct them. Existing results about Hermite interpolation are revisited. A simple method to select the best quintic interpolant among all possible solutions is suggested. 1. Introduction The notion of helical polynomial curves, i.e, polynomial curves which made a constant angle with a ¯xed line in space, have been studied by di®erent authors. Let us cite the papers [5, 6, 7] where the main results about the cubical and quintic cases are stablished. In [5] the authors gives a necessary condition a polynomial curve must satisfy in order to be a helix. The condition is expressed in terms of its hodograph, i.e., its derivative. If a polynomial curve, ®, is a helix then its hodograph, ®0, must be Pythagorean, i.e., jj®0jj2 is a perfect square of a polynomial. Moreover, this condition is su±cient in the cubical case: all PH cubical curves are helices. In the same paper it is also stated that not only ®0 must be Pythagorean, but also ®0^®00. Following the same ideas, in [1] it is proved that both conditions are su±cient in the quintic case. Unfortunately, this characterization is no longer true for higher degrees. It is possible to construct examples of polynomial curves of degree 7 verifying both conditions but being not a helix. The aim of this paper is just to show how a simple geometric trick can clarify the proofs of some previous results and to simplify the needed compu- tations to solve some related problems as for instance, the Hermite problem using helical polynomial curves. The Dietz-Hoschek-JÄuttlertheorem (see [2] or [3]) relates the Pythagorean condition to the Hopf map H : C2 ! R3. A polynomial curve ® is Pythagorean 0 if and only if there exist z1; z2 such that ® = H(z1; z2) where z1; z2 are two polynomial complex functions. The geometric trick is based on the following facts: ¯rst, the normalized Hopf map is related to the stereographic projection (the usual stereographic projection from the two dimensional unit sphere, S2, into the complex plane, Date: October 6, 2006. 2000 Mathematics Subject Classi¯cation. Primary 53A04; Secondary 53C40. Key words and phrases. generalized polynomial helices, Pythagorean hodograph curves. 1 2 J. MONTERDE not the generalized stereographic projection from the three-dimensional pro- jective space, using homogeneous coordinates, to S2, as it appears in Remark 1 of [5], or in Remark 2 of [6]); second, the tangent indicatrix of a helical curve describes a circle on the unit sphere and, ¯nally, the image by the stereographic projection of a circle on the unit sphere is a line-or-circle in the complex plane. Joining up these arguments, we obtain a full characterization of polyno- mial helices of any degree in terms of the quotient z1 . The condition is of z2 geometric nature: ® is an helix if and only if z1 is a rational parametriza- z2 tion of a piece of a line or a circle in C depending whether or not the vector (0; 0; 1) belongs to the hodograph, respectively. According to this approach, the already known results ([6, 7]) about Her- mite interpolation using helical curves are revisited and their proofs sim- pli¯ed. Moreover, the classi¯cation into two classes of helical PH quintics introduced in [5] is also clari¯ed, and a result concerning a su±cient condi- tion on the quaternions generating a PH helical curve stated and proved for quintics in the cited reference is here generalized to any dimension (see Cor. 2). Finally, a simple method to choose the best among all possible general PH quintic helices solving the ¯rst order Hermite problem is suggested. In the cited references, the choice among all the possible solutions involves the computation of some integral, the energy associated with the rotation- minimizing frame. Here we simply control the values of two parameters involved in our method (see Prop. 1). 2. Spatial Pythagorean hodograph curves Initially, we will use the quaternion representation of spatial PH curves. Given a quaternion polynomial A(t) = u(t) + iv(t) + jp(t) + kq(t); the product ®0(t) = A(t)iA¤(t) de¯nes (the asterisk means quaternionic conjugate) a spatial Pythagorean hodograph, ®0, whose components are x0 = u2 + v2 ¡ p2 ¡ q2; (2.1) y0 = 2(up + vq); z0 = 2(vp ¡ uq); and such that jj®0jj2 = (x0)2 + (y0)2 + (z0)2 = (u2 + v2 + p2 + q2)2. In terms of the Hopf map (see [3], theorem 4.2) H : C2 ! R3 2 2 de¯ned by H(z1; z2) = (2z1z¹2; jz1j ¡ jz2j ), and taking (2.2) z1(t) = u(t) + iv(t); z2(t) = p(t) + iq(t); CHARACTERIZATION OF HELICAL CURVES OF ANY DEGREE 3 the derivative of the curve can be written as 0 ® (t) = H(z1(t); z2(t)): 0 Theorem 1. A Pythagorean polynomial curve ® with ® (t) = H(z1(t); z2(t)) is a helix if and only the curve in the complex plane t ! z1(t) traces a line- z2(t) or-circle. Proof. A curve ® is a general helix if and only if its tangent indicatrix is a subset of a circle on the unit sphere S2. Let us de¯ne the normalized Hopf map Hn : C2 ! S2 by n 1 2 2 H (z1; z2) = 2 2 (2z1z¹2; jz1j ¡ jz2j ): jz1j + jz2j 0 If ® (t) = H(z1(t); z2(t)), then its tangent indicatrix is ®0(t) = Hn(z (t); z (t)): jj®0(t)jj 1 2 Notice that Hn(z ; z ) = Hn( z1 ; 1), and that for any z 2 C, Hn(z; 1) = 1 2 z2 ¡1 2 pst (z) where pst : S ! C[f1g denotes the extended stereographic projec- tion from the north pole of the whole unit sphere to the extended complex plane with the assumption pst(0; 0; 1) = 1. Therefore, ® is a general helix if and only if p¡1( z1(t) ) 2 S2 belongs to a st z2(t) circle in the unit sphere. But the image by the stereographic projection of a circle in the unit sphere is a line-or-circle in the extended complex plane (see Proposition 7.23 in [8]). ¤ 0 Corollary 1. A Pythagorean polynomial curve ® with ® (t) = H(z1(t); z2(t)) with (0; 0; 1) in the trace of tangent indicatrix is a helix if and only the curve in the complex plane t ! z1(t) traces a piece of a straight line. z2(t) Proof. Recall that a circle on the unit sphere passes trough the north pole if and only if its image by the extended stereographic projection is a straight line of the complex plane. ¤ Figure I. Representation of the tangent indicatrix of an helical curve and of its stereographic projection. 4 J. MONTERDE The next result was proved for the quadratic case in [5]. We shall prove it in its full generality. n Corollary 2. Let us suppose that fAigi=0 are a set of n + 1 quaternionic control points of a B¶eziercurve such that the interior control points are linear combinations of the exterior ones, then the associated quaternionic B¶eziercurve is the hodograph of a helical curve. Proof. If all the interior quaternionic control points are linear combinations Pn n of fA0; Ang, then A(t) = i=0 Bi (t)Ai is a parametrization of a piece of the quaternionic straight line B(t) = (1 ¡ t)A0 + tAn. What we need to prove is that B(t)iB(t)¤ is the hodograph of an helical curve, or equivalently that if z1(t) = a + tb; z2(t) = c + td; a; b; c; d 2 C then z1(t) belongs to a line-or-circle. z2(t) An straightforward computation shows that if Im(c ¢ d) 6= 0 then z1(t) z2(t) ¹ belongs to a circle with center p = i b¢c¹¡a¢d and radius r = j a ¡ pj. 2Im(c¢d) c If Im(c ¢ d) = 0, then we can write z2(t), after an a±ne change of the parameter t, as z2(t) = t¹ where ¹ 2 C ¡ f0g. Again a simple computa- ¹ tion shows that z1(t) belongs to a line passing through the point a¹+b with z2(t) ¹ a direction ¡ 2¹ . ¤ 2.1. Examples. It is just a matter of computation to check that the two examples of quintic helices in [5] verify the condition written in the statement of Th. 1. As it is said in the cited reference, they are, respectively, examples of the two classes of helical PH quintics. 2.1.1. Monotone-helical PH quintic example. The ¯rst example is de¯ned by the four quadratic polynomials u(t) = t2¡3t; v(t) = t2¡5t+10; p(t) = t2¡9t+10; q(t) = ¡2t2+3t+5: Let us recall that for this case the polynomials z1 and z2 share a common factor corresponding to the root 1 + 2i. So, we can simplify the quotient z1(t) and to check that it belongs to the circumference with center ( 3 ; 1 ) z2(t) p 10 10 2 and radius r = 2 . Moreover, let us see for this example which kind of rational parametriza- tion of a straight line is z1(t) when the hodograph is rotated in the space in z2(t) such a way that the tangent vector at t = 0 is (0; 0; 1). After a rotation with y-axis and angle arccos( p1 ) and a rotation with p 17 17 x-axis and angle arccos( 9 ) the hodograph curve is transformed into µ ¶ 2t(7t ¡ 15) 2t(71t ¡ 225) 1 ®0(t) = (5 ¡ 2t + t2) p ; p ; (405 ¡ 288t + 43t2) : 17 9 17 9 CHARACTERIZATION OF HELICAL CURVES OF ANY DEGREE 5 ¡! ®0(0) Now, it veri¯es t (0) = jj®0(0)jj = (0; 0; 1).
Recommended publications
  • Engineering Curves – I
    Engineering Curves – I 1. Classification 2. Conic sections - explanation 3. Common Definition 4. Ellipse – ( six methods of construction) 5. Parabola – ( Three methods of construction) 6. Hyperbola – ( Three methods of construction ) 7. Methods of drawing Tangents & Normals ( four cases) Engineering Curves – II 1. Classification 2. Definitions 3. Involutes - (five cases) 4. Cycloid 5. Trochoids – (Superior and Inferior) 6. Epic cycloid and Hypo - cycloid 7. Spiral (Two cases) 8. Helix – on cylinder & on cone 9. Methods of drawing Tangents and Normals (Three cases) ENGINEERING CURVES Part- I {Conic Sections} ELLIPSE PARABOLA HYPERBOLA 1.Concentric Circle Method 1.Rectangle Method 1.Rectangular Hyperbola (coordinates given) 2.Rectangle Method 2 Method of Tangents ( Triangle Method) 2 Rectangular Hyperbola 3.Oblong Method (P-V diagram - Equation given) 3.Basic Locus Method 4.Arcs of Circle Method (Directrix – focus) 3.Basic Locus Method (Directrix – focus) 5.Rhombus Metho 6.Basic Locus Method Methods of Drawing (Directrix – focus) Tangents & Normals To These Curves. CONIC SECTIONS ELLIPSE, PARABOLA AND HYPERBOLA ARE CALLED CONIC SECTIONS BECAUSE THESE CURVES APPEAR ON THE SURFACE OF A CONE WHEN IT IS CUT BY SOME TYPICAL CUTTING PLANES. OBSERVE ILLUSTRATIONS GIVEN BELOW.. Ellipse Section Plane Section Plane Hyperbola Through Generators Parallel to Axis. Section Plane Parallel to end generator. COMMON DEFINATION OF ELLIPSE, PARABOLA & HYPERBOLA: These are the loci of points moving in a plane such that the ratio of it’s distances from a fixed point And a fixed line always remains constant. The Ratio is called ECCENTRICITY. (E) A) For Ellipse E<1 B) For Parabola E=1 C) For Hyperbola E>1 Refer Problem nos.
    [Show full text]
  • Linguistic Presentation of Objects
    Zygmunt Ryznar dr emeritus Cracow Poland [email protected] Linguistic presentation of objects (types,structures,relations) Abstract Paper presents phrases for object specification in terms of structure, relations and dynamics. An applied notation provides a very concise (less words more contents) description of object. Keywords object relations, role, object type, object dynamics, geometric presentation Introduction This paper is based on OSL (Object Specification Language) [3] dedicated to present the various structures of objects, their relations and dynamics (events, actions and processes). Jay W.Forrester author of fundamental work "Industrial Dynamics”[4] considers the importance of relations: “the structure of interconnections and the interactions are often far more important than the parts of system”. Notation <!...> comment < > container of (phrase,name...) ≡> link to something external (outside of definition)) <def > </def> start-end of definition <spec> </spec> start-end of specification <beg> <end> start-end of section [..] or {..} 1 list of assigned keywords :[ or :{ structure ^<name> optional item (..) list of items xxxx(..) name of list = value assignment @ mark of special attribute,feature,property @dark unknown, to obtain, to discover :: belongs to : equivalent name (e.g.shortname) # number of |name| executive/operational object ppppXxxx name of item Xxxx with prefix ‘pppp ‘ XXXX basic object UUUU.xxxx xxxx object belonged to UUUU object class & / conjunctions ‘and’ ‘or’ 1 If using Latex editor we suggest [..] brackets
    [Show full text]
  • Helical Curves and Double Pythagorean Hodographs
    Helical polynomial curves and “double” Pythagorean-hodograph curves Rida T. Farouki Department of Mechanical & Aeronautical Engineering, University of California, Davis — synopsis — • introduction: properties of Pythagorean-hodograph curves • computing rotation-minimizing frames on spatial PH curves • helical polynomial space curves — are always PH curves • standard quaternion representation for spatial PH curves • “double” Pythagorean hodograph structure — requires both |r0(t)| and |r0(t) × r00(t)| to be polynomials in t • Hermite interpolation problem: selection of free parameters Pythagorean-hodograph (PH) curves r(ξ) = PH curve ⇐⇒ coordinate components of r0(ξ) comprise a “Pythagorean n-tuple of polynomials” in Rn PH curves incorporate special algebraic structures in their hodographs (complex number & quaternion models for planar & spatial PH curves) • rational offset curves rd(ξ) = r(ξ) + d n(ξ) Z ξ • polynomial arc-length function s(ξ) = |r0(ξ)| dξ 0 Z 1 • closed-form evaluation of energy integral E = κ2 ds 0 • real-time CNC interpolators, rotation-minimizing frames, etc. helical polynomial space curves several equivalent characterizations of helical curves • tangent t maintains constant inclination ψ with fixed vector a • a · t = cos ψ, where ψ = pitch angle and a = axis vector of helix • fixed curvature/torsion ratio, κ/τ = tan ψ (Theorem of Lancret) • curve has a circular tangent indicatrix on the unit sphere (small circle for space curve, great circle for planar curve) • (r(2) × r(3)) · r(4) ≡ 0 — where r(k) = kth arc–length derivative
    [Show full text]
  • Chapter 2. Parameterized Curves in R3
    Chapter 2. Parameterized Curves in R3 Def. A smooth curve in R3 is a smooth map σ :(a, b) → R3. For each t ∈ (a, b), σ(t) ∈ R3. As t increases from a to b, σ(t) traces out a curve in R3. In terms of components, σ(t) = (x(t), y(t), z(t)) , (1) or x = x(t) σ : y = y(t) a < t < b , z = z(t) dσ velocity at time t: (t) = σ0(t) = (x0(t), y0(t), z0(t)) . dt dσ speed at time t: (t) = |σ0(t)| dt Ex. σ : R → R3, σ(t) = (r cos t, r sin t, 0) - the standard parameterization of the unit circle, x = r cos t σ : y = r sin t z = 0 σ0(t) = (−r sin t, r cos t, 0) |σ0(t)| = r (constant speed) 1 Ex. σ : R → R3, σ(t) = (r cos t, r sin t, ht), r, h > 0 constants (helix). σ0(t) = (−r sin t, r cos t, h) √ |σ0(t)| = r2 + h2 (constant) Def A regular curve in R3 is a smooth curve σ :(a, b) → R3 such that σ0(t) 6= 0 for all t ∈ (a, b). That is, a regular curve is a smooth curve with everywhere nonzero velocity. Ex. Examples above are regular. Ex. σ : R → R3, σ(t) = (t3, t2, 0). σ is smooth, but not regular: σ0(t) = (3t2, 2t, 0) , σ0(0) = (0, 0, 0) Graph: x = t3 y = t2 = (x1/3)2 σ : y = t2 ⇒ y = x2/3 z = 0 There is a cusp, not because the curve isn’t smooth, but because the velocity = 0 at the origin.
    [Show full text]
  • On Helices and Bertrand Curves in Euclidean 3-Space
    ON HELİCES AND BERTRAND CURVES IN EUCLİDEAN 3-SPACE Murat Babaarslan Department of Mathematics, Faculty of Science and Arts Bozok University, Yozgat, Turkey [email protected] Yusuf Yaylı Department of Mathematics, Faculty of Science Ankara University, Tandoğan, Ankara, Turkey [email protected] Abstract- In this article, we investigate Bertrand curves corresponding to spherical images of the tangent indicatrix, binormal indicatrix, principal normal indicatrix and Darboux indicatrix of a space curve in Euclidean 3-space. As a result, in case of a space curve is general helix, we show that curve corresponding to spherical images of its tangent indicatrix and binormal indicatrix are circular helices and Bertrand curves. Similarly, in case of a space curve is slant helix, we demonstrate that the curve corresponding to spherical image of its principal normal indicatrix is circular helix and Bertrand curve. Key Words- Helix, Bertrand curve, Spherical Images 1. INTRODUCTION In the differential geometry of a regular curve in Euclidean 3-space E3 , it is well known that, one of the important problems is characterization of a regular curve. The curvature and the torsion of a regular curve play an important role to determine the shape and size of the curve 1,2. Natural scientists have long held a fascination, sometimes bordering on mystical obsession for helical structures in nature. Helices arise in nanosprings, carbon nonotubes, helices, DNA double and collagen triple helix, the double helix shape is commonly associated with DNA, since the double helix is structure of DNA 3 . This fact was published for the first time by Watson and Crick in 1953 4.
    [Show full text]
  • Effect of Superhelical Structure on the Secondary Structure of DNA Rings
    VOL. 5, PP. 691-696 (1967) Effect of Superhelical Structure on the Secondary Structure of DNA Rings DANIEL GLAUBIGER and JOHN E. HEARST, Departnient of Chemistry, University of California, Berkeley, California Synopsis A quantity, called the linking number, is defined, which specifies the total number of t,wists in a circular helix. The linking number is invariant under continuous deforma- tions of the ring and therefore enables one to calculate the influence of superhelical structures on the secondary helix of a circular molecule. The linking number can be determined by projecting the helix into a plane and counting strand crosses in the projection as described. For example, it has been shown that for each 180" twist in a left-handed superhelix, a right-handed 360" twist is removed from the secondary helix, thus allowing local unwinding. Introduction It is of interest to relate superhelical structure of helical molecules to their secondary structure.' By defining a quantity characteristic of two- stranded circular helical niolecules, related to the helical structure, and in- variant under continuous deformations of the molecule, we are able to evaluate the changes in helical structure brought about by the imposition of superhelical configurations on such molecules. The quantity of interest, called the linking number, is related to the number of turns/cycle for a circular helical molecule.* It will be shown that superhelical structures which are made from helical polymers con- tribute to this number and alter the contribution made by the secondary structure of the molecule to this number. This is made manifest as a change in the number of turns/cycle or as a change in the number of turns/ unit length.
    [Show full text]
  • The Helix and the Heart
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector The Journal of BSR Thoracic and Cardiovascular Surgery Vol 124, No. 5, November 2002 Basic science review: The helix and the heart Gerald D. Buckberg, MD t is an enormous privilege and honor to be asked to give the basic science See related editorials on pages lecture. Please join me on an adventure that I have taken over the past three 884 and 886. years. I described this type of voyage to my daughters many years ago as “discovery,” in which you walk down certain common pathways but always see something different on that journey. I will tell you about my concept of how the helix and the heart affect nature, the heart, and the human. ITo pursue this new route, I select a comment from my hero, Albert Einstein, who said, “All our science, measured against reality, is primitive and childlike, and yet www.mosby.com/jtcvs is the most precious thing we have.” We all have to be students, who are often wrong and always in doubt, while a professor is sometimes wrong and never in doubt. Please join me on my student pathway to see something I discovered recently and will now share with you. The object of our affection is the heart, which is, in reality, a helix that contains an apex. The cardiac helix form, in Figure 1, was described in the 1660s by Lower as having an apical vortex, in which the muscle fibers go from outside in, in a clockwise way, and from inside out, in a counterclockwise direction.
    [Show full text]
  • X-Ray Scattering from the Superhelix in Circular DNA (Supercoiling/Diffraction from Solutions/Specific Linking Difference/Writhe Vs
    Proc. Nati Acad. Sci. USA Vol. 80, pp. 741-744, February 1983 Biophysics X-ray scattering from the superhelix in circular DNA (supercoiling/diffraction from solutions/specific linking difference/writhe vs. twist) G. W. BRADY*, D. B. FEIN*, H. LAMBERTSONt, V. GRASSIANt, D. Foost, AND C. J. BENHAMt Institute, Troy, New York 12181; *Center for Laboratories and Research, New York State Department of Health, Albany, New York 12222; tRensselaer Polytechnic and tDepartment of Mathematics, University of Kentucky, Lexington, Kentucky 40506 Communicated by Bruno H. Zimm, October 25, 1982 ABSTRACT This communication presents measurements, creased the lower angle limit of resolution of the instrument made with a newly constructed position-sensitive detector, of the because the inner portion of the scattering curve was super- small-angle x-ray scattering from the first-order superhelix ofna- imposed on a risingbackground resultingfrom parasitic slit scat- tive COP608 plasmid DNA. This instrument measures intensities tering. In consequence, the resulting data could not be de- free of slit effects and provides good resolution in the region of smeared, so a direct comparison with theory was precluded. interest. The reported observations, made both in the presence This paper presents measurements of SAS from the first-or- and in the absence of intercalator, closely fit the scattering pat- der ccc DNA superhelix made with a new position-sensitive terns calculated for noninterwound helical first-order superhel- detector (PSD). The resulting profiles are free of slit effects, ices. These results are consistent with a toroidal helical structure permitting direct and unambiguous comparisons with theory. but not with interwound conformations.
    [Show full text]
  • Cyclic GMP–AMP Signalling Protects Bacteria Against Viral Infection
    Article Cyclic GMP–AMP signalling protects bacteria against viral infection https://doi.org/10.1038/s41586-019-1605-5 Daniel Cohen1,3, Sarah Melamed1,3, Adi Millman1, Gabriela Shulman1, Yaara Oppenheimer-Shaanan1, Assaf Kacen2, Shany Doron1, Gil Amitai1* & Rotem Sorek1* Received: 25 June 2019 Accepted: 11 September 2019 The cyclic GMP–AMP synthase (cGAS)–STING pathway is a central component of the Published online: xx xx xxxx cell-autonomous innate immune system in animals1,2. The cGAS protein is a sensor of cytosolic viral DNA and, upon sensing DNA, it produces a cyclic GMP–AMP (cGAMP) signalling molecule that binds to the STING protein and activates the immune response3–5. The production of cGAMP has also been detected in bacteria6, and has been shown, in Vibrio cholerae, to activate a phospholipase that degrades the inner bacterial membrane7. However, the biological role of cGAMP signalling in bacteria remains unknown. Here we show that cGAMP signalling is part of an antiphage defence system that is common in bacteria. This system is composed of a four-gene operon that encodes the bacterial cGAS and the associated phospholipase, as well as two enzymes with the eukaryotic-like domains E1, E2 and JAB. We show that this operon confers resistance against a wide variety of phages. Phage infection triggers the production of cGAMP, which—in turn—activates the phospholipase, leading to a loss of membrane integrity and to cell death before completion of phage reproduction. Diverged versions of this system appear in more than 10% of prokaryotic genomes, and we show that variants with efectors other than phospholipase also protect against phage infection.
    [Show full text]
  • A Conformal Approach to Bour's Theorem
    Mathematica Aeterna, Vol. 2, 2012, no. 8, 701 - 713 A Conformal Approach to Bour's Theorem ZEHRA BOZKURT Department of Mathematics, Faculty of Science, Ankara University Tando˘gan, Ankara, TURKEY ISMA_ IL_ GOK¨ Department of Mathematics, Faculty of Science, Ankara University Tando˘gan, Ankara, TURKEY F. NEJAT EKMEKCI_ Department of Mathematics, Faculty of Science, Ankara University Tando˘gan, Ankara, TURKEY YUSUF YAYLI Department of Mathematics, Faculty of Science, Ankara University Tando˘gan, Ankara, TURKEY Abstract In this paper, we give relation between Bour's theorem and confor- mal map in Euclidean 3−space. We prove that a spiral surface and a helicoidal surface have a conformal relation. So, a helix on the helicoid correspond to a spiral on the spiral surface. Moreover we obtain that a spiral surface and a rotation surface have a conformal relation. So, spirals on the spiral surface correspond to parallel circles on the rotation surface. When the conformal map is an isometry we obtain the Bour's theorem ,i.e, we obtain an isometric relation between the helisoidal sur- face and the rotation surface, which was given by Bour in [1]. Thus this paper is a generalization of Bour's theorem. Mathematics Subject Classification: 53A05, 53C10S Keywords: Bour's theorem, spiral surface, rotation surface, helicoid 702 Z.BOZKURT, I_ GO¨K, F. N. EKMEKCI_ and Y. YAYLI 1 Introduction Surface theory in Euclidean 3−space has been studied for a long time. In classical differential geometry, rotation surfaces with constant curvature and the right helicoid (resp catenoid) which is the only ruled minimal surface have been known.
    [Show full text]
  • OSL - Object Specification Language
    Zygmunt Ryznar dr emeritus Cracow Poland [email protected] OSL - Object Specification Language (includes BSL,SSL,HSL,geometric structures & brain definition) Abstract OSL© is a markup descriptive language for a simple formal description of any object in terms of structure and behavior. In this paper we present a geometric approach, the kernel and subsets for IT system, business and human-being as a proof of universality. This language was invented as a tool for a free structured modeling and design. Keywords free structured modeling and design, OSL, object specification language, human descriptive language, factual markup, geometric view, object specification, GSO -geometrically structured objects. I. INTRODUCTION Generally, a free structured modeling is a collection of methods, techniques and tools for modeling the variable structure as an opposite to the widely used “well-structured” approach focused on top-down hierarchical decomposition. It is assumed that system boundaries are not finally defined, because the system is never to be completed and components are are ready to be modified at any time. OSL is dedicated to present the various structures of objects, their relations and dynamics (events, actions and processes). This language may be counted among markup languages. The fundamentals of markup languages were created in SGML (Standard Generalized Markup Language) [6] descended from GML (name comes from first letters of surnames of authors: Goldfarb, Mosher, Lorie, later renamed as Generalized Markup Language) developed at IBM [15]. Markups are usually focused on: - documents (tags: title, abstract, keywords, menu, footnote etc.) e.g. latex [14], - objects (e.g. OSL), - internet pages (tags used in html, xml – based on SGML [8] rules), - data (e.g.
    [Show full text]
  • The Anatomy of Conical Helices, Consciousness, and Universal Constants
    The Anatomy of Conical Helices, Consciousness, and Universal Constants Author: Jeffrey S. Keen BSc Hons ARCS MInstP CPhys MBCS MIMS CEng © 2006 by Jeffrey S Keen All rights reserved. No part of this article may be reproduced, stored in a retrieval system, or transmitted or translated in machine language in any form or by any means, electronic, mechanical, photocopying, recording or otherwise, without the prior written permission of the author. Page 1 of 27 The Anatomy of Conical Helixes, Consciousness, and Universal Constants Abstract As rotation is an important feature of the universe, preliminary evidence suggests that its study could help in understanding consciousness. Research detailed in this paper further develops the author’s work in Reference 1, with particular emphasis on fields perceived to be displaying a spiral nature. Numerous quantitative properties of these fields are detailed, and as often found in scientific research, the results spring several surprises. The study of spirals and vortices results in relationships with high correlation coefficients, together with universal constants that occur in other disciplines in science. These facts not only reinforce the validity of the research techniques being adopted, but also further the quest in understanding consciousness and the structure of the universe. The conclusions suggest that vortices are not only involved in consciousness, but also have wider implications in understanding our universe, and therefore the subject warrants further research. Objectives Rotation of objects in orbit, or the spin of objects around their axes seem to be an important property of the universe at whatever scale one chooses – be it rotating galaxies, planets revolving in solar systems, planets spinning on their own axes, electrons spinning around nuclei of atoms, or the spin associated with fundamental particles.
    [Show full text]