Recognition of Feature Curves on 3D Shapes Using an Algebraic Approach to Hough Transforms ∗
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The Ordered Distribution of Natural Numbers on the Square Root Spiral
The Ordered Distribution of Natural Numbers on the Square Root Spiral - Harry K. Hahn - Ludwig-Erhard-Str. 10 D-76275 Et Germanytlingen, Germany ------------------------------ mathematical analysis by - Kay Schoenberger - Humboldt-University Berlin ----------------------------- 20. June 2007 Abstract : Natural numbers divisible by the same prime factor lie on defined spiral graphs which are running through the “Square Root Spiral“ ( also named as “Spiral of Theodorus” or “Wurzel Spirale“ or “Einstein Spiral” ). Prime Numbers also clearly accumulate on such spiral graphs. And the square numbers 4, 9, 16, 25, 36 … form a highly three-symmetrical system of three spiral graphs, which divide the square-root-spiral into three equal areas. A mathematical analysis shows that these spiral graphs are defined by quadratic polynomials. The Square Root Spiral is a geometrical structure which is based on the three basic constants: 1, sqrt2 and π (pi) , and the continuous application of the Pythagorean Theorem of the right angled triangle. Fibonacci number sequences also play a part in the structure of the Square Root Spiral. Fibonacci Numbers divide the Square Root Spiral into areas and angle sectors with constant proportions. These proportions are linked to the “golden mean” ( golden section ), which behaves as a self-avoiding-walk- constant in the lattice-like structure of the square root spiral. Contents of the general section Page 1 Introduction to the Square Root Spiral 2 2 Mathematical description of the Square Root Spiral 4 3 The distribution -
Curvature Theorems on Polar Curves
PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES Volume 33 March 15, 1947 Number 3 CURVATURE THEOREMS ON POLAR CUR VES* By EDWARD KASNER AND JOHN DE CICCO DEPARTMENT OF MATHEMATICS, COLUMBIA UNIVERSITY, NEW YoRK Communicated February 4, 1947 1. The principle of duality in projective geometry is based on the theory of poles and polars with respect to a conic. For a conic, a point has only one kind of polar, the first polar, or polar straight line. However, for a general algebraic curve of higher degree n, a point has not only the first polar of degree n - 1, but also the second polar of degree n - 2, the rth polar of degree n - r, :. ., the (n - 1) polar of degree 1. This last polar is a straight line. The general polar theory' goes back to Newton, and was developed by Bobillier, Cayley, Salmon, Clebsch, Aronhold, Clifford and Mayer. For a given curve Cn of degree n, the first polar of any point 0 of the plane is a curve C.-1 of degree n - 1. If 0 is a point of C, it is well known that the polar curve C,,- passes through 0 and touches the given curve Cn at 0. However, the two curves do not have the same curvature. We find that the ratio pi of the curvature of C,- i to that of Cn is Pi = (n -. 2)/(n - 1). For example, if the given curve is a cubic curve C3, the first polar is a conic C2, and at an ordinary point 0 of C3, the ratio of the curvatures is 1/2. -
Coverrailway Curves Book.Cdr
RAILWAY CURVES March 2010 (Corrected & Reprinted : November 2018) INDIAN RAILWAYS INSTITUTE OF CIVIL ENGINEERING PUNE - 411 001 i ii Foreword to the corrected and updated version The book on Railway Curves was originally published in March 2010 by Shri V B Sood, the then professor, IRICEN and reprinted in September 2013. The book has been again now corrected and updated as per latest correction slips on various provisions of IRPWM and IRTMM by Shri V B Sood, Chief General Manager (Civil) IRSDC, Delhi, Shri R K Bajpai, Sr Professor, Track-2, and Shri Anil Choudhary, Sr Professor, Track, IRICEN. I hope that the book will be found useful by the field engineers involved in laying and maintenance of curves. Pune Ajay Goyal November 2018 Director IRICEN, Pune iii PREFACE In an attempt to reach out to all the railway engineers including supervisors, IRICEN has been endeavouring to bring out technical books and monograms. This book “Railway Curves” is an attempt in that direction. The earlier two books on this subject, viz. “Speed on Curves” and “Improving Running on Curves” were very well received and several editions of the same have been published. The “Railway Curves” compiles updated material of the above two publications and additional new topics on Setting out of Curves, Computer Program for Realignment of Curves, Curves with Obligatory Points and Turnouts on Curves, with several solved examples to make the book much more useful to the field and design engineer. It is hoped that all the P.way men will find this book a useful source of design, laying out, maintenance, upgradation of the railway curves and tackling various problems of general and specific nature. -
Some Curves and the Lengths of Their Arcs Amelia Carolina Sparavigna
Some Curves and the Lengths of their Arcs Amelia Carolina Sparavigna To cite this version: Amelia Carolina Sparavigna. Some Curves and the Lengths of their Arcs. 2021. hal-03236909 HAL Id: hal-03236909 https://hal.archives-ouvertes.fr/hal-03236909 Preprint submitted on 26 May 2021 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Some Curves and the Lengths of their Arcs Amelia Carolina Sparavigna Department of Applied Science and Technology Politecnico di Torino Here we consider some problems from the Finkel's solution book, concerning the length of curves. The curves are Cissoid of Diocles, Conchoid of Nicomedes, Lemniscate of Bernoulli, Versiera of Agnesi, Limaçon, Quadratrix, Spiral of Archimedes, Reciprocal or Hyperbolic spiral, the Lituus, Logarithmic spiral, Curve of Pursuit, a curve on the cone and the Loxodrome. The Versiera will be discussed in detail and the link of its name to the Versine function. Torino, 2 May 2021, DOI: 10.5281/zenodo.4732881 Here we consider some of the problems propose in the Finkel's solution book, having the full title: A mathematical solution book containing systematic solutions of many of the most difficult problems, Taken from the Leading Authors on Arithmetic and Algebra, Many Problems and Solutions from Geometry, Trigonometry and Calculus, Many Problems and Solutions from the Leading Mathematical Journals of the United States, and Many Original Problems and Solutions. -
Archimedean Spirals ∗
Archimedean Spirals ∗ An Archimedean Spiral is a curve defined by a polar equation of the form r = θa, with special names being given for certain values of a. For example if a = 1, so r = θ, then it is called Archimedes’ Spiral. Archimede’s Spiral For a = −1, so r = 1/θ, we get the reciprocal (or hyperbolic) spiral. Reciprocal Spiral ∗This file is from the 3D-XploreMath project. You can find it on the web by searching the name. 1 √ The case a = 1/2, so r = θ, is called the Fermat (or hyperbolic) spiral. Fermat’s Spiral √ While a = −1/2, or r = 1/ θ, it is called the Lituus. Lituus In 3D-XplorMath, you can change the parameter a by going to the menu Settings → Set Parameters, and change the value of aa. You can see an animation of Archimedean spirals where the exponent a varies gradually, from the menu Animate → Morph. 2 The reason that the parabolic spiral and the hyperbolic spiral are so named is that their equations in polar coordinates, rθ = 1 and r2 = θ, respectively resembles the equations for a hyperbola (xy = 1) and parabola (x2 = y) in rectangular coordinates. The hyperbolic spiral is also called reciprocal spiral because it is the inverse curve of Archimedes’ spiral, with inversion center at the origin. The inversion curve of any Archimedean spirals with respect to a circle as center is another Archimedean spiral, scaled by the square of the radius of the circle. This is easily seen as follows. If a point P in the plane has polar coordinates (r, θ), then under inversion in the circle of radius b centered at the origin, it gets mapped to the point P 0 with polar coordinates (b2/r, θ), so that points having polar coordinates (ta, θ) are mapped to points having polar coordinates (b2t−a, θ). -
Limits of Pgl(3)-Translates of Plane Curves, I
LIMITS OF PGL(3)-TRANSLATES OF PLANE CURVES, I PAOLO ALUFFI, CAREL FABER Abstract. We classify all possible limits of families of translates of a fixed, arbitrary complex plane curve. We do this by giving a set-theoretic description of the projective normal cone (PNC) of the base scheme of a natural rational map, determined by the curve, 8 N from the P of 3 × 3 matrices to the P of plane curves of degree d. In a sequel to this paper we determine the multiplicities of the components of the PNC. The knowledge of the PNC as a cycle is essential in our computation of the degree of the PGL(3)-orbit closure of an arbitrary plane curve, performed in [5]. 1. Introduction In this paper we determine the possible limits of a fixed, arbitrary complex plane curve C , obtained by applying to it a family of translations α(t) centered at a singular transformation of the plane. In other words, we describe the curves in the boundary of the PGL(3)-orbit closure of a given curve C . Our main motivation for this work comes from enumerative geometry. In [5] we have determined the degree of the PGL(3)-orbit closure of an arbitrary (possibly singular, re- ducible, non-reduced) plane curve; this includes as special cases the determination of several characteristic numbers of families of plane curves, the degrees of certain maps to moduli spaces of plane curves, and isotrivial versions of the Gromov-Witten invariants of the plane. A description of the limits of a curve, and in fact a more refined type of information is an essential ingredient of our approach. -
Geometry of Algebraic Curves
Geometry of Algebraic Curves Fall 2011 Course taught by Joe Harris Notes by Atanas Atanasov One Oxford Street, Cambridge, MA 02138 E-mail address: [email protected] Contents Lecture 1. September 2, 2011 6 Lecture 2. September 7, 2011 10 2.1. Riemann surfaces associated to a polynomial 10 2.2. The degree of KX and Riemann-Hurwitz 13 2.3. Maps into projective space 15 2.4. An amusing fact 16 Lecture 3. September 9, 2011 17 3.1. Embedding Riemann surfaces in projective space 17 3.2. Geometric Riemann-Roch 17 3.3. Adjunction 18 Lecture 4. September 12, 2011 21 4.1. A change of viewpoint 21 4.2. The Brill-Noether problem 21 Lecture 5. September 16, 2011 25 5.1. Remark on a homework problem 25 5.2. Abel's Theorem 25 5.3. Examples and applications 27 Lecture 6. September 21, 2011 30 6.1. The canonical divisor on a smooth plane curve 30 6.2. More general divisors on smooth plane curves 31 6.3. The canonical divisor on a nodal plane curve 32 6.4. More general divisors on nodal plane curves 33 Lecture 7. September 23, 2011 35 7.1. More on divisors 35 7.2. Riemann-Roch, finally 36 7.3. Fun applications 37 7.4. Sheaf cohomology 37 Lecture 8. September 28, 2011 40 8.1. Examples of low genus 40 8.2. Hyperelliptic curves 40 8.3. Low genus examples 42 Lecture 9. September 30, 2011 44 9.1. Automorphisms of genus 0 an 1 curves 44 9.2. -
Analysis of Spiral Curves in Traditional Cultures
Forum _______________________________________________________________ Forma, 22, 133–139, 2007 Analysis of Spiral Curves in Traditional Cultures Ryuji TAKAKI1 and Nobutaka UEDA2 1Kobe Design University, Nishi-ku, Kobe, Hyogo 651-2196, Japan 2Hiroshima-Gakuin, Nishi-ku, Hiroshima, Hiroshima 733-0875, Japan *E-mail address: [email protected] *E-mail address: [email protected] (Received November 3, 2006; Accepted August 10, 2007) Keywords: Spiral, Curvature, Logarithmic Spiral, Archimedean Spiral, Vortex Abstract. A method is proposed to characterize and classify shapes of plane spirals, and it is applied to some spiral patterns from historical monuments and vortices observed in an experiment. The method is based on a relation between the length variable along a curve and the radius of its local curvature. Examples treated in this paper seem to be classified into four types, i.e. those of the Archimedean spiral, the logarithmic spiral, the elliptic vortex and the hyperbolic spiral. 1. Introduction Spiral patterns are seen in many cultures in the world from ancient ages. They give us a strong impression and remind us of energy of the nature. Human beings have been familiar to natural phenomena and natural objects with spiral motions or spiral shapes, such as swirling water flows, swirling winds, winding stems of vines and winding snakes. It is easy to imagine that powerfulness of these phenomena and objects gave people a motivation to design spiral shapes in monuments, patterns of cloths and crafts after spiral shapes observed in their daily lives. Therefore, it would be reasonable to expect that spiral patterns in different cultures have the same geometrical properties, or at least are classified into a small number of common types. -
Unsupervised Smooth Contour Detection
Published in Image Processing On Line on 2016–11–18. Submitted on 2016–04–21, accepted on 2016–10–03. ISSN 2105–1232 c 2016 IPOL & the authors CC–BY–NC–SA This article is available online with supplementary materials, software, datasets and online demo at https://doi.org/10.5201/ipol.2016.175 2015/06/16 v0.5.1 IPOL article class Unsupervised Smooth Contour Detection Rafael Grompone von Gioi1, Gregory Randall2 1 CMLA, ENS Cachan, France ([email protected]) 2 IIE, Universidad de la Rep´ublica, Uruguay ([email protected]) Abstract An unsupervised method for detecting smooth contours in digital images is proposed. Following the a contrario approach, the starting point is defining the conditions where contours should not be detected: soft gradient regions contaminated by noise. To achieve this, low frequencies are removed from the input image. Then, contours are validated as the frontiers separating two adjacent regions, one with significantly larger values than the other. Significance is evalu- ated using the Mann-Whitney U test to determine whether the samples were drawn from the same distribution or not. This test makes no assumption on the distributions. The resulting algorithm is similar to the classic Marr-Hildreth edge detector, with the addition of the statis- tical validation step. Combined with heuristics based on the Canny and Devernay methods, an efficient algorithm is derived producing sub-pixel contours. Source Code The ANSI C source code for this algorithm, which is part of this publication, and an online demo are available from the web page of this article1. -
ALL ABOUT SPIRALS a Spiral Can Be Described As Any 2D Continuous Curve Where the Radial Distance R from the Origin Equals a Specified Function of the Angle Θ
, ALL ABOUT SPIRALS A spiral can be described as any 2D continuous curve where the radial distance r from the origin equals a specified function of the angle θ. Mathematically it has the unique derivative given by- dr=(df/dθ)dθ with r=0 at θ=0 On integrating one finds- () ∫ 푑푡 r= This solution yields two simple forms. The first occurs when df/dt=α. We get- r=α(θ) This simplest of continuous spiral figures is just the Archimedes Spiral discovered by him over two thousand years ago. Setting the constant to α=3/π , we have the plot- Note that the distance between turns of the spiral remain the same. A second simple spiral is found when df/dθ=βf, where f=exp(훽휃). If we take r=1 at θ=0, it produces- r=exp(βθ) or the equivalent ln(r)=βθ It is known as the Logarithmic Spiral or Bernoulli’s Spiral. Here is its graph when β=1/10- A property of the Bernouli Spiral is that the angle between any radial line and the tangent to the spiral remains a constant. J. Bernoulli was so intrigued by this spiral that he had a copy placed on his tombstone in Basel Switzerland. Here I am pointing to it back in 2000 - One can construct numerous other spirals by simply changing the form of df(θ)/dθ and picking a starting point r(θ0)=r0. So if df/dθ=α/[2sqrt(θ)] and r=0 when θ=0, we get the spiral– r=αsqrt(θ) It looks as follows- This figure is known as the Fermat Spiral. -
1 Riemann Surfaces - Sachi Hashimoto
1 Riemann Surfaces - Sachi Hashimoto 1.1 Riemann Hurwitz Formula We need the following fact about the genus: Exercise 1 (Unimportant). The genus is an invariant which is independent of the triangu- lation. Thus we can speak of it as an invariant of the surface, or of the Euler characteristic χ(X) = 2 − 2g. This can be proven by showing that the genus is the dimension of holomorphic one forms on a Riemann surface. Motivation: Suppose we have some hyperelliptic curve C : y2 = (x+1)(x−1)(x+2)(x−2) and we want to determine the topology of the solution set. For almost every x0 2 C we can find two values of y 2 C such that (x0; y) is a solution. However, when x = ±1; ±2 there is only one y-value, y = 0, which satisfies this equation. There is a nice way to do this with branch cuts{the square root function is well defined everywhere as a two valued functioned except at these points where we have a portal between the \positive" and the \negative" world. Here it is best to draw some pictures, so I will omit this part from the typed notes. But this is not very systematic, so let me say a few words about our eventual goal. What we seem to be doing is projecting our curve to the x-coordinate and then considering what this generically degree 2 map does on special values. The hope is that we can extract from this some topological data: because the sphere is a known quantity, with genus 0, and the hyperelliptic curve is our unknown, quantity, our goal is to leverage the knowns and unknowns. -
Calculus-Free Derivatives of Sine and Cosine
Calculus-free Derivatives of Sine and Cosine B.D.S. McConnell [email protected] Wrap a square smoothly around a cylinder, and the curved images of the square’s diagonals will trace out helices, with the (original, uncurved) diag- onals tangent to those curves. Projecting these elements into appropriate planes reveals an intuitive, geometric development of the formulas for the derivatives of sine and cosine, with no quotient of vanishing differences re- quired. Indeed, a single —almost-“Behold!”-worthy— diagram and a short notational summary (see the last page of this note) give everything away. The setup. Consider a cylinder (“C”) of radius 1 and a unit square (“S”), with a pair of S’s edges parallel to C’s axis, and with S’s center (“P ”) a point of tangency with C’s surface. We may assume that the cylinder’s axis coincides with the z axis; we may also assume that, measuring along the surface of the cylinder, the (straight-line) distance from P to the xy-plane is equal to the (arc-of-circle) distance from P to the zx-plane. That is, we take P to have coordinates (cos θ0, sin θ0, θ0) for some θ0, where cos() and sin() take radian arguments. Wrapping S around C causes the image of an extended diagonal of S to trace out the helix (“H”) containing all (and only) points of the form (cos θ, sin θ, θ). Moreover, the original, uncurved diagonal segment of S de- termines a vector, v :=< vx, vy, vz >, tangent to H at P ; taking vz = 1, we assure that the vector conveniently points “forward” (that is, in the direction of increasing θ) along the helix.