Parametric Equations and Polar Coordinates 605 7 | PARAMETRIC EQUATIONS and POLAR COORDINATES
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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. -
Polar Coordinates and Complex Numbers Infinite Series Vectors and Matrices Motion Along a Curve Partial Derivatives
Contents CHAPTER 9 Polar Coordinates and Complex Numbers 9.1 Polar Coordinates 348 9.2 Polar Equations and Graphs 351 9.3 Slope, Length, and Area for Polar Curves 356 9.4 Complex Numbers 360 CHAPTER 10 Infinite Series 10.1 The Geometric Series 10.2 Convergence Tests: Positive Series 10.3 Convergence Tests: All Series 10.4 The Taylor Series for ex, sin x, and cos x 10.5 Power Series CHAPTER 11 Vectors and Matrices 11.1 Vectors and Dot Products 11.2 Planes and Projections 11.3 Cross Products and Determinants 11.4 Matrices and Linear Equations 11.5 Linear Algebra in Three Dimensions CHAPTER 12 Motion along a Curve 12.1 The Position Vector 446 12.2 Plane Motion: Projectiles and Cycloids 453 12.3 Tangent Vector and Normal Vector 459 12.4 Polar Coordinates and Planetary Motion 464 CHAPTER 13 Partial Derivatives 13.1 Surfaces and Level Curves 472 13.2 Partial Derivatives 475 13.3 Tangent Planes and Linear Approximations 480 13.4 Directional Derivatives and Gradients 490 13.5 The Chain Rule 497 13.6 Maxima, Minima, and Saddle Points 504 13.7 Constraints and Lagrange Multipliers 514 CHAPTER 12 Motion Along a Curve I [ 12.1 The Position Vector I-, This chapter is about "vector functions." The vector 2i +4j + 8k is constant. The vector R(t) = ti + t2j+ t3k is moving. It is a function of the parameter t, which often represents time. At each time t, the position vector R(t) locates the moving body: position vector =R(t) =x(t)i + y(t)j + z(t)k. -
Arts Revealed in Calculus and Its Extension
See discussions, stats, and author profiles for this publication at: https://www.researchgate.net/publication/265557431 Arts revealed in calculus and its extension Article · August 2014 CITATIONS READS 9 455 1 author: Hanna Arini Parhusip Universitas Kristen Satya Wacana 95 PUBLICATIONS 89 CITATIONS SEE PROFILE Some of the authors of this publication are also working on these related projects: Pusnas 2015/2016 View project All content following this page was uploaded by Hanna Arini Parhusip on 16 September 2014. The user has requested enhancement of the downloaded file. [Type[Type aa quotequote fromfrom thethe documentdocument oror thethe International Journal of Statistics and Mathematics summarysummary ofof anan interestinginteresting point.point. YouYou cancan Vol. 1(3), pp. 016-023, August, 2014. © www.premierpublishers.org, ISSN: xxxx-xxxx x positionposition thethe texttext boxbox anywhereanywhere inin thethe IJSM document. Use the Text Box Tools tab to document. Use the Text Box Tools tab to changechange thethe formattingformatting ofof thethe pullpull quotequote texttext box.]box.] Review Arts revealed in calculus and its extension Hanna Arini Parhusip Mathematics Department, Science and Mathematics Faculty, Satya Wacana Christian University (SWCU)-Jl. Diponegoro 52-60 Salatiga, Indonesia Email: [email protected], Tel.:0062-298-321212, Fax: 0062-298-321433 Motivated by presenting mathematics visually and interestingly to common people based on calculus and its extension, parametric curves are explored here to have two and three dimensional objects such that these objects can be used for demonstrating mathematics. Epicycloid, hypocycloid are particular curves that are implemented in MATLAB programs and the motifs are presented here. The obtained curves are considered to be domains for complex mappings to have new variation of Figures and objects. -
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 -
Around and Around ______
Andrew Glassner’s Notebook http://www.glassner.com Around and around ________________________________ Andrew verybody loves making pictures with a Spirograph. The result is a pretty, swirly design, like the pictures Glassner EThis wonderful toy was introduced in 1966 by Kenner in Figure 1. Products and is now manufactured and sold by Hasbro. I got to thinking about this toy recently, and wondered The basic idea is simplicity itself. The box contains what might happen if we used other shapes for the a collection of plastic gears of different sizes. Every pieces, rather than circles. I wrote a program that pro- gear has several holes drilled into it, each big enough duces Spirograph-like patterns using shapes built out of to accommodate a pen tip. The box also contains some Bezier curves. I’ll describe that later on, but let’s start by rings that have gear teeth on both their inner and looking at traditional Spirograph patterns. outer edges. To make a picture, you select a gear and set it snugly against one of the rings (either inside or Roulettes outside) so that the teeth are engaged. Put a pen into Spirograph produces planar curves that are known as one of the holes, and start going around and around. roulettes. A roulette is defined by Lawrence this way: “If a curve C1 rolls, without slipping, along another fixed curve C2, any fixed point P attached to C1 describes a roulette” (see the “Further Reading” sidebar for this and other references). The word trochoid is a synonym for roulette. From here on, I’ll refer to C1 as the wheel and C2 as 1 Several the frame, even when the shapes Spirograph- aren’t circular. -
Art and Engineering Inspired by Swarm Robotics
RICE UNIVERSITY Art and Engineering Inspired by Swarm Robotics by Yu Zhou A Thesis Submitted in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy Approved, Thesis Committee: Ronald Goldman, Chair Professor of Computer Science Joe Warren Professor of Computer Science Marcia O'Malley Professor of Mechanical Engineering Houston, Texas April, 2017 ABSTRACT Art and Engineering Inspired by Swarm Robotics by Yu Zhou Swarm robotics has the potential to combine the power of the hive with the sen- sibility of the individual to solve non-traditional problems in mechanical, industrial, and architectural engineering and to develop exquisite art beyond the ken of most contemporary painters, sculptors, and architects. The goal of this thesis is to apply swarm robotics to the sublime and the quotidian to achieve this synergy between art and engineering. The potential applications of collective behaviors, manipulation, and self-assembly are quite extensive. We will concentrate our research on three topics: fractals, stabil- ity analysis, and building an enhanced multi-robot simulator. Self-assembly of swarm robots into fractal shapes can be used both for artistic purposes (fractal sculptures) and in engineering applications (fractal antennas). Stability analysis studies whether distributed swarm algorithms are stable and robust either to sensing or to numerical errors, and tries to provide solutions to avoid unstable robot configurations. Our enhanced multi-robot simulator supports this research by providing real-time simula- tions with customized parameters, and can become as well a platform for educating a new generation of artists and engineers. The goal of this thesis is to use techniques inspired by swarm robotics to develop a computational framework accessible to and suitable for both artists and engineers. -
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). -
Transformation of Axes
19 Chapter 2 Transformation of Axes 2.1 Transformation of Coordinates It sometimes happens that the choice of axes at the beginning of the solution of a problem does not lead to the simplest form of the equation. By a proper transformation of axes an equation may be simplified. This may be accom- plished in two steps, one called translation of axes, the other rotation of axes. 2.1.1 Translation of axes Let ox and oy be the original axes and let o0x0 and o0y0 be the new axes, parallel respectively to the old ones. Also, let o0(h, k) referred to the origin of new axes. Let P be any point in the plane, and let its coordinates referred to the old axes be (x, y) and referred to the new axes be (x0y0) . To determine x and y in terms of x0, y0, h and x = h + x0 y = k + y0 20 Chapter 2. Transformation of Axes these equations represent the equations of translation and hence, the coeffi- cients of the first degree terms are vanish. 2.1.2 Rotation of axes Let ox and oy be the original axes and ox0 and oy0 the new axes. 0 is the origin for each set of axes. Let the angle x0 ox through which the axes have been rotated be represented by q. Let P be any point in the plane, and let its coordinates referred to the old axes be (x, y) and referred to the new axes be (x0, y0), To determine x and y in terms of x0, y0 and q : x = OM = ON − MN = x0 cos q − y0 sin q and y = MP = MM0 + M0P = NN0 + M0P = x0 sin q + y0 cos q 2.1. -
A Dynamic Rod Model to Simulate Mechanics of Cables and Dna
A DYNAMIC ROD MODEL TO SIMULATE MECHANICS OF CABLES AND DNA by Sachin Goyal A dissertation submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy (Mechanical Engineering and Scientific Computing) in The University of Michigan 2006 Doctoral Committee: Professor Noel Perkins, Chair Associate Professor Edgar Meyhofer, Co-Chair Assistant Professor Ioan Andricioaei Assistant Professor Krishnakumar Garikipati Assistant Professor Jens-Christian Meiners Dedication To my parents ii Acknowledgements I am extremely grateful to my advisor Prof. Noel Perkins for his highly conducive and motivating research guidance and overall mentoring. I sincerely appreciate many engaging discussions of DNA mechanics and supercoiling with Prof. E. Meyhofer and Prof. K. Garikipati in Mechanical Engineering Program, Prof. C. Meiners in the Biophysics Program, Prof. I. Andricioaei in the Biochemistry/ Biophysics Program and and Dr. S. Blumberg in Medical school at the University of Michigan and Dr. C. L. Lee at the Lawrence Livermore National Laboratory, California. I also appreciate Professor Jason D. Kahn (Department of Chemistry and Biochemistry, University of Maryland) for providing the sequences used in his experiments, and Professor Wilma K. Olson (Department of Chemistry and Chemical Biology, Rutgers University) for suggesting alternative binding topologies in DNA-protein complexes. I also acknowledge recent graduate students T. Lillian in Mechanical Engineering Program, D. Wilson in Physics Program and J. Wereszczynski in Chemistry Program to extend my work and collaborate on ongoing studies beyond the scope of dissertation. I also gratefully acknowledge the research support provided by the U. S. Office of Naval Research, Lawrence Livermore National Laboratories, and the National Science Foundation. -
Analysis of a Hyperbolic Paraboloid Surface with Curved Edges
ANALYSIS,, OF A HYPERBOLIC PARABOLOID by Carlos Alberto Asturias Theai1 submitted to the Graduate Faculty of the Virginia Polytechnic Institute in candidacy for the degree of MASTER OF SCIENCE in Structural Engineering December 17, 1965 Blacksburg, Virginia · -2- TABLE OF CONTENTS Page I. INTRODUCTION ••••••••••••••••••••••••••••••••••• 5 11. OBJECTIVE •••••••••••••••••••••••••••••••••••••• 8 Ill. HISTORICAL BACKGROUND • ••••••••••••••••••••••••• 9 IV. NOTATION ••••••••••••••••••••••••••••••••••••••• 10 v. METHOD OF ANALYSIS • •••••••••••••••••••••••••••• 12 VI. FORMULATION OF THE METHOD • ••••••••••••••••••••• 15 VII. THEORETICAL INVESTIGATION • ••••••••••••••••••••• 24 A. DEVELOPMENT OF EQUATIONS • •••••••••••••• 24 B. ILLUSTRATIVE EXAMPLE • •••••••••••••••••• 37 VIII. EXPERIMENTAL WORK • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • 50 A. DESCRIPTION OF THE MODEL ••••••••••••••• 50 B. TEST SET UP •••••••••••••••••••••••••••• 53 IX. TEST RESULTS AND CONCLUSIONS • •••••••••••••••••• 61 X. BIBLIOGRAPHY ••••••••••••••••••••••••••••••••••• 65 XI. ACKNOWLEDGMENT • •••••••••••••••••••••••••••••••• 67 XII. VITA • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • 68 -3- LIST OF FIGURES Page FIGURE I. HYPERBOLIC PARABOLOID TYPES ••••••••••••• 7 FIGURE II. DIFFERENTIAL ELEMENT .................... 13 FIGURE III. AXES .................................... 36 FIGURE IV. DIMENSIONS •••••••••••••••••••••••••••••• 36 FIGURE v. STRESSES ., • 0 ••••••••••••••••••••••••••••• 44 FIGURE VI. STRESSES ••••••••••••••••••••••••••• -
Differential Geometry of Curves and Surfaces 1
DIFFERENTIAL GEOMETRY OF CURVES AND SURFACES 1. Curves in the Plane 1.1. Points, Vectors, and Their Coordinates. Points and vectors are fundamental objects in Geometry. The notion of point is intuitive and clear to everyone. The notion of vector is a bit more delicate. In fact, rather than saying what a vector is, we prefer to say what a vector has, namely: direction, sense, and length (or magnitude). It can be represented by an arrow, and the main idea is that two arrows represent the same vector if they have the same direction, sense, and length. An arrow representing a vector has a tail and a tip. From the (rough) definition above, we deduce that in order to represent (if you want, to draw) a given vector as an arrow, it is necessary and sufficient to prescribe its tail. a c b b a c a a b P Figure 1. We see four copies of the vector a, three of the vector b, and two of the vector c. We also see a point P . An important instrument in handling points, vectors, and (consequently) many other geometric objects is the Cartesian coordinate system in the plane. This consists of a point O, called the origin, and two perpendicular lines going through O, called coordinate axes. Each line has a positive direction, indicated by an arrow (see Figure 2). We denote by R the a P y a y x O O x Figure 2. The point P has coordinates x, y. The vector a has also coordinates x, y.