Newton's Method and Fractals 1
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Mathematics Is a Gentleman's Art: Analysis and Synthesis in American College Geometry Teaching, 1790-1840 Amy K
Iowa State University Capstones, Theses and Retrospective Theses and Dissertations Dissertations 2000 Mathematics is a gentleman's art: Analysis and synthesis in American college geometry teaching, 1790-1840 Amy K. Ackerberg-Hastings Iowa State University Follow this and additional works at: https://lib.dr.iastate.edu/rtd Part of the Higher Education and Teaching Commons, History of Science, Technology, and Medicine Commons, and the Science and Mathematics Education Commons Recommended Citation Ackerberg-Hastings, Amy K., "Mathematics is a gentleman's art: Analysis and synthesis in American college geometry teaching, 1790-1840 " (2000). Retrospective Theses and Dissertations. 12669. https://lib.dr.iastate.edu/rtd/12669 This Dissertation is brought to you for free and open access by the Iowa State University Capstones, Theses and Dissertations at Iowa State University Digital Repository. It has been accepted for inclusion in Retrospective Theses and Dissertations by an authorized administrator of Iowa State University Digital Repository. For more information, please contact [email protected]. INFORMATION TO USERS This manuscript has been reproduced from the microfilm master. UMI films the text directly from the original or copy submitted. Thus, some thesis and dissertation copies are in typewriter face, while others may be from any type of computer printer. The quality of this reproduction is dependent upon the quality of the copy submitted. Broken or indistinct print, colored or poor quality illustrations and photographs, print bleedthrough, substandard margwis, and improper alignment can adversely affect reproduction. in the unlikely event that the author did not send UMI a complete manuscript and there are missing pages, these will be noted. -
Linear Approximation of the Derivative
Section 3.9 - Linear Approximation and the Derivative Idea: When we zoom in on a smooth function and its tangent line, they are very close to- gether. So for a function that is hard to evaluate, we can use the tangent line to approximate values of the derivative. p 3 Example Usep a tangent line to approximatep 8:1 without a calculator. Let f(x) = 3 x = x1=3. We know f(8) = 3 8 = 2. We'll use the tangent line at x = 8. 1 1 1 1 f 0(x) = x−2=3 so f 0(8) = (8)−2=3 = · 3 3 3 4 Our tangent line passes through (8; 2) and has slope 1=12: 1 y = (x − 8) + 2: 12 To approximate f(8:1) we'll find the value of the tangent line at x = 8:1. 1 y = (8:1 − 8) + 2 12 1 = (:1) + 2 12 1 = + 2 120 241 = 120 p 3 241 So 8:1 ≈ 120 : p How accurate was this approximation? We'll use a calculator now: 3 8:1 ≈ 2:00829885. 241 −5 Taking the difference, 2:00829885 − 120 ≈ −3:4483 × 10 , a pretty good approximation! General Formulas for Linear Approximation The tangent line to f(x) at x = a passes through the point (a; f(a)) and has slope f 0(a) so its equation is y = f 0(a)(x − a) + f(a) The tangent line is the best linear approximation to f(x) near x = a so f(x) ≈ f(a) + f 0(a)(x − a) this is called the local linear approximation of f(x) near x = a. -
Generalized Finite-Difference Schemes
Generalized Finite-Difference Schemes By Blair Swartz* and Burton Wendroff** Abstract. Finite-difference schemes for initial boundary-value problems for partial differential equations lead to systems of equations which must be solved at each time step. Other methods also lead to systems of equations. We call a method a generalized finite-difference scheme if the matrix of coefficients of the system is sparse. Galerkin's method, using a local basis, provides unconditionally stable, implicit generalized finite-difference schemes for a large class of linear and nonlinear problems. The equations can be generated by computer program. The schemes will, in general, be not more efficient than standard finite-difference schemes when such standard stable schemes exist. We exhibit a generalized finite-difference scheme for Burgers' equation and solve it with a step function for initial data. | 1. Well-Posed Problems and Semibounded Operators. We consider a system of partial differential equations of the following form: (1.1) du/dt = Au + f, where u = (iti(a;, t), ■ ■ -, umix, t)),f = ifxix, t), ■ • -,fmix, t)), and A is a matrix of partial differential operators in x — ixx, • • -, xn), A = Aix,t,D) = JjüiD', D<= id/dXx)h--Yd/dxn)in, aiix, t) = a,-,...i„(a;, t) = matrix . Equation (1.1) is assumed to hold in some n-dimensional region Í2 with boundary An initial condition is imposed in ti, (1.2) uix, 0) = uoix) , xEV. The boundary conditions are that there is a collection (B of operators Bix, D) such that (1.3) Bix,D)u = 0, xEdti,B<E(2>. We assume the operator A satisfies the following condition : There exists a scalar product {,) such that for all sufficiently smooth functions <¡>ix)which satisfy (1.3), (1.4) 2 Re {A4,,<t>) ^ C(<b,<p), 0 < t ^ T , where C is a constant independent of <p.An operator A satisfying (1.4) is called semi- bounded. -
Introduction to Ultra Fractal
Introduction to Ultra Fractal Text and images © 2001 Kerry Mitchell Table of Contents Introduction ..................................................................................................................................... 2 Assumptions ........................................................................................................................ 2 Conventions ........................................................................................................................ 2 What Are Fractals? ......................................................................................................................... 3 Shapes with Infinite Detail .................................................................................................. 3 Defined By Iteration ........................................................................................................... 4 Approximating Infinity ....................................................................................................... 4 Using Ultra Fractal .......................................................................................................................... 6 Starting Ultra Fractal ........................................................................................................... 6 Formula ............................................................................................................................... 6 Size ..................................................................................................................................... -
Rendering Hypercomplex Fractals Anthony Atella [email protected]
Rhode Island College Digital Commons @ RIC Honors Projects Overview Honors Projects 2018 Rendering Hypercomplex Fractals Anthony Atella [email protected] Follow this and additional works at: https://digitalcommons.ric.edu/honors_projects Part of the Computer Sciences Commons, and the Other Mathematics Commons Recommended Citation Atella, Anthony, "Rendering Hypercomplex Fractals" (2018). Honors Projects Overview. 136. https://digitalcommons.ric.edu/honors_projects/136 This Honors is brought to you for free and open access by the Honors Projects at Digital Commons @ RIC. It has been accepted for inclusion in Honors Projects Overview by an authorized administrator of Digital Commons @ RIC. For more information, please contact [email protected]. Rendering Hypercomplex Fractals by Anthony Atella An Honors Project Submitted in Partial Fulfillment of the Requirements for Honors in The Department of Mathematics and Computer Science The School of Arts and Sciences Rhode Island College 2018 Abstract Fractal mathematics and geometry are useful for applications in science, engineering, and art, but acquiring the tools to explore and graph fractals can be frustrating. Tools available online have limited fractals, rendering methods, and shaders. They often fail to abstract these concepts in a reusable way. This means that multiple programs and interfaces must be learned and used to fully explore the topic. Chaos is an abstract fractal geometry rendering program created to solve this problem. This application builds off previous work done by myself and others [1] to create an extensible, abstract solution to rendering fractals. This paper covers what fractals are, how they are rendered and colored, implementation, issues that were encountered, and finally planned future improvements. -
Lecture 9: Newton Method 9.1 Motivation 9.2 History
10-725: Convex Optimization Fall 2013 Lecture 9: Newton Method Lecturer: Barnabas Poczos/Ryan Tibshirani Scribes: Wen-Sheng Chu, Shu-Hao Yu Note: LaTeX template courtesy of UC Berkeley EECS dept. 9.1 Motivation Newton method is originally developed for finding a root of a function. It is also known as Newton- Raphson method. The problem can be formulated as, given a function f : R ! R, finding the point x? such that f(x?) = 0. Figure 9.1 illustrates another motivation of Newton method. Given a function f, we want to approximate it at point x with a quadratic function fb(x). We move our the next step determined by the optimum of fb. Figure 9.1: Motivation for quadratic approximation of a function. 9.2 History Babylonian people first applied the Newton method to find the square root of a positive number S 2 R+. The problem can be posed as solving the equation f(x) = x2 − S = 0. They realized the solution can be achieved by applying the iterative update rule: 2 1 S f(xk) xk − S xn+1 = (xk + ) = xk − 0 = xk − : (9.1) 2 xk f (xk) 2xk This update rule converges to the square root of S, which turns out to be a special case of Newton method. This could be the first application of Newton method. The starting point affects the convergence of the Babylonian's method for finding the square root. Figure 9.2 shows an example of solving the square root for S = 100. x- and y-axes represent the number of iterations and the variable, respectively. -
Newton.Indd | Sander Pinkse Boekproductie | 16-11-12 / 14:45 | Pag
omslag Newton.indd | Sander Pinkse Boekproductie | 16-11-12 / 14:45 | Pag. 1 e Dutch Republic proved ‘A new light on several to be extremely receptive to major gures involved in the groundbreaking ideas of Newton Isaac Newton (–). the reception of Newton’s Dutch scholars such as Willem work.’ and the Netherlands Jacob ’s Gravesande and Petrus Prof. Bert Theunissen, Newton the Netherlands and van Musschenbroek played a Utrecht University crucial role in the adaption and How Isaac Newton was Fashioned dissemination of Newton’s work, ‘is book provides an in the Dutch Republic not only in the Netherlands important contribution to but also in the rest of Europe. EDITED BY ERIC JORINK In the course of the eighteenth the study of the European AND AD MAAS century, Newton’s ideas (in Enlightenment with new dierent guises and interpre- insights in the circulation tations) became a veritable hype in Dutch society. In Newton of knowledge.’ and the Netherlands Newton’s Prof. Frans van Lunteren, sudden success is analyzed in Leiden University great depth and put into a new perspective. Ad Maas is curator at the Museum Boerhaave, Leiden, the Netherlands. Eric Jorink is researcher at the Huygens Institute for Netherlands History (Royal Dutch Academy of Arts and Sciences). / www.lup.nl LUP Newton and the Netherlands.indd | Sander Pinkse Boekproductie | 16-11-12 / 16:47 | Pag. 1 Newton and the Netherlands Newton and the Netherlands.indd | Sander Pinkse Boekproductie | 16-11-12 / 16:47 | Pag. 2 Newton and the Netherlands.indd | Sander Pinkse Boekproductie | 16-11-12 / 16:47 | Pag. -
Calculus I - Lecture 15 Linear Approximation & Differentials
Calculus I - Lecture 15 Linear Approximation & Differentials Lecture Notes: http://www.math.ksu.edu/˜gerald/math220d/ Course Syllabus: http://www.math.ksu.edu/math220/spring-2014/indexs14.html Gerald Hoehn (based on notes by T. Cochran) March 11, 2014 Equation of Tangent Line Recall the equation of the tangent line of a curve y = f (x) at the point x = a. The general equation of the tangent line is y = L (x) := f (a) + f 0(a)(x a). a − That is the point-slope form of a line through the point (a, f (a)) with slope f 0(a). Linear Approximation It follows from the geometric picture as well as the equation f (x) f (a) lim − = f 0(a) x a x a → − f (x) f (a) which means that x−a f 0(a) or − ≈ f (x) f (a) + f 0(a)(x a) = L (x) ≈ − a for x close to a. Thus La(x) is a good approximation of f (x) for x near a. If we write x = a + ∆x and let ∆x be sufficiently small this becomes f (a + ∆x) f (a) f (a)∆x. Writing also − ≈ 0 ∆y = ∆f := f (a + ∆x) f (a) this becomes − ∆y = ∆f f 0(a)∆x ≈ In words: for small ∆x the change ∆y in y if one goes from x to x + ∆x is approximately equal to f 0(a)∆x. Visualization of Linear Approximation Example: a) Find the linear approximation of f (x) = √x at x = 16. b) Use it to approximate √15.9. Solution: a) We have to compute the equation of the tangent line at x = 16. -
Generating Fractals Using Complex Functions
Generating Fractals Using Complex Functions Avery Wengler and Eric Wasser What is a Fractal? ● Fractals are infinitely complex patterns that are self-similar across different scales. ● Created by repeating simple processes over and over in a feedback loop. ● Often represented on the complex plane as 2-dimensional images Where do we find fractals? Fractals in Nature Lungs Neurons from the Oak Tree human cortex Regardless of scale, these patterns are all formed by repeating a simple branching process. Geometric Fractals “A rough or fragmented geometric shape that can be split into parts, each of which is (at least approximately) a reduced-size copy of the whole.” Mandelbrot (1983) The Sierpinski Triangle Algebraic Fractals ● Fractals created by repeatedly calculating a simple equation over and over. ● Were discovered later because computers were needed to explore them ● Examples: ○ Mandelbrot Set ○ Julia Set ○ Burning Ship Fractal Mandelbrot Set ● Benoit Mandelbrot discovered this set in 1980, shortly after the invention of the personal computer 2 ● zn+1=zn + c ● That is, a complex number c is part of the Mandelbrot set if, when starting with z0 = 0 and applying the iteration repeatedly, the absolute value of zn remains bounded however large n gets. Animation based on a static number of iterations per pixel. The Mandelbrot set is the complex numbers c for which the sequence ( c, c² + c, (c²+c)² + c, ((c²+c)²+c)² + c, (((c²+c)²+c)²+c)² + c, ...) does not approach infinity. Julia Set ● Closely related to the Mandelbrot fractal ● Complementary to the Fatou Set Featherino Fractal Newton’s method for the roots of a real valued function Burning Ship Fractal z2 Mandelbrot Render Generic Mandelbrot set. -
Chapter 3, Lecture 1: Newton's Method 1 Approximate
Math 484: Nonlinear Programming1 Mikhail Lavrov Chapter 3, Lecture 1: Newton's Method April 15, 2019 University of Illinois at Urbana-Champaign 1 Approximate methods and asumptions The final topic covered in this class is iterative methods for optimization. These are meant to help us find approximate solutions to problems in cases where finding exact solutions would be too hard. There are two things we've taken for granted before which might actually be too hard to do exactly: 1. Evaluating derivatives of a function f (e.g., rf or Hf) at a given point. 2. Solving an equation or system of equations. Before, we've assumed (1) and (2) are both easy. Now we're going to figure out what to do when (2) and possibly (1) is hard. For example: • For a polynomial function of high degree, derivatives are straightforward to compute, but it's impossible to solve equations exactly (even in one variable). • For a function we have no formula for (such as the value function MP(z) from Chapter 5, for instance) we don't have a good way of computing derivatives, and they might not even exist. 2 The classical Newton's method Eventually we'll get to optimization problems. But we'll begin with Newton's method in its basic form: an algorithm for approximately finding zeroes of a function f : R ! R. This is an iterative algorithm: starting with an initial guess x0, it makes a better guess x1, then uses it to make an even better guess x2, and so on. We hope that eventually these approach a solution. -
Newton's Mathematical Physics
Isaac Newton A new era in science Waseda University, SILS, Introduction to History and Philosophy of Science LE201, History and Philosophy of Science Newton . Newton’s Legacy Newton brought to a close the astronomical revolution begun by Copernicus. He combined the dynamic research of Galileo with the astronomical work of Kepler. He produced an entirely new cosmology and a new way of thinking about the world, based on the interaction between matter and mathematically determinate forces. He joined the mathematical and experimental methods: the hypothetico-deductive method. His work became the model for rational mechanics as it was later practiced by mathematicians, particularly during the Enlightenment. LE201, History and Philosophy of Science Newton . William Blake’s Newton (1795) LE201, History and Philosophy of Science Newton LE201, History and Philosophy of Science Newton . Newton’s De Motu coporum in gyrum Edmond Halley (of the comet) visited Cambridge in 1684 and 1 talked with Newton about inverse-square forces (F 9 d2 ). Newton stated that he has already shown that inverse-square force implied an ellipse, but could not find the documents. Later he rewrote this into a short document called De Motu coporum in gyrum, and sent it to Halley. Halley was excited and asked for a full treatment of the subject. Two years later Newton sent Book I of The Mathematical Principals of Natural Philosophy (Principia). Key Point The goal of this project was to derive the orbits of bodies from a simpler set of assumptions about motion. That is, it sought to explain Kepler’s Laws with a simpler set of laws. -
The Newton Fractal's Leonardo Sequence Study with the Google
INTERNATIONAL ELECTRONIC JOURNAL OF MATHEMATICS EDUCATION e-ISSN: 1306-3030. 2020, Vol. 15, No. 2, em0575 OPEN ACCESS https://doi.org/10.29333/iejme/6440 The Newton Fractal’s Leonardo Sequence Study with the Google Colab Francisco Regis Vieira Alves 1*, Renata Passos Machado Vieira 1 1 Federal Institute of Science and Technology of Ceara - IFCE, BRAZIL * CORRESPONDENCE: [email protected] ABSTRACT The work deals with the study of the roots of the characteristic polynomial derived from the Leonardo sequence, using the Newton fractal to perform a root search. Thus, Google Colab is used as a computational tool to facilitate this process. Initially, we conducted a study of the Leonardo sequence, addressing it fundamental recurrence, characteristic polynomial, and its relationship to the Fibonacci sequence. Following this study, the concept of fractal and Newton’s method is approached, so that it can then use the computational tool as a way of visualizing this technique. Finally, a code is developed in the Phyton programming language to generate Newton’s fractal, ending the research with the discussion and visual analysis of this figure. The study of this subject has been developed in the context of teacher education in Brazil. Keywords: Newton’s fractal, Google Colab, Leonardo sequence, visualization INTRODUCTION Interest in the study of homogeneous, linear and recurrent sequences is becoming more and more widespread in the scientific literature. Therefore, the Fibonacci sequence is the best known and studied in works found in the literature, such as Oliveira and Alves (2019), Alves and Catarino (2019). In these works, we can see an investigation and exploration of the Fibonacci sequence and the complexification of its mathematical model and the generalizations that result from it.