Microworld: Calculus in Action: Chapter 3, Section 2: Logarithmic Spirals and Planetary Orbits
Click the Hyperlink above to visit the Microworld.
Author:James E. White

Nature presents us with many excellent examples of mathematical concepts. We should say that mathematics is the art that strives (in its finest moments) to reflect upon and illuminate our characteristic and human perception of Nature. The planets are (essentially) spheres, and they move in curves that have an exceedingly simple description. Flowers, plants and animals grow according to principles that can sometimes disclose simple mathematical relationships also. As an example, consider the contour of Oliver Wendell Holmes' "Chambered Nautilus" shell. This is an example of a construction of Jacob Bernoulli that he called the "equiangular spiral."

We can imagine, following an idea of D'Arcy Wentworth Thompson in his wonderful book, On Growth and Form, that it acquired its shape in the following way. As the shell grew from the center, the angle that the growing point made with the radius to the center, O, is always the same angle. This just means that the principle of growth is the same, and does not differ from time to time. The figure is then "self-similar." It has the same shape at any point. Such figures were sometimes called "gnomons" and are nowadays called "fractals."

We will see that we can approximate such growth with similar triangles.

The picture at the top of the page is at the heart of a method for representing curves by means of differential approximation. That method is called a "differential equation" model and it does more than represent the curves. It often offers explanatory principles that can help us understand how complex shapes can evolve from simple local laws.

In fact, the picture above, which is built from a growing sequence of similar triangles, contains the germ of the Euler sequence that we studied in the previous part and will, by means of that sequence provide a very simple description of the shape of a Nautilus shell in terms of exponential growth. In that model we will also find a standard method for solving differential equations in general. That method is called, unsurprisingly, Euler's method.

Now the real reason for studying the equiangular spiral is as heuristic preparation for Newton's deduction of Kepler's laws from universal gravitation. As we mentioned, Newton set up and solved the basic differential equation that provides the key to those laws. But his equation took into account the fact that gravity acts on velocities, and not directly on positions, as Galileo observed. Momentum, therefore, plays a key role in his equations, and makes them for that reason somewhat subtler than the spiral equations. In the picture below, we see that the red acceleration vector (which is determined by the position of the satellite) directly modifies the green velocity vector in each instant of time. The satellite moves along the modified velocity vector. Such a differential equation is called a "second-order ordinary differential equation." We will examine that process also in the exploration in order to understand Newton's deduction when we come to it in Harmony of the Spheres.

The following is the Table of Contents for this 6 page Microworld

  1. Exponential Functions and Euler's Number
  2. Natural Exponentials and Infinite Series
  3. Natural Logarithms and Area Integrals
  4. Of Nautilus Shells and Planets
  5. Symbolic Calculator

            Each page of the Microworld, including the Calculator page has the story for that page under the   icon.  Just click on this icon to read the story for the page.  The Calculator is quite versatile, and so we recommend you read through the instructions there to become familiar with it.

Return to the listing of MathwrightWeb Microworlds


    - James E. White, Ph.D. , Library Director,
    author of this website, Mathwright 2000, MindScapes,
    MathwrightWeb, and Mathwright32

 

Microworld Title Page

Calculus in Action: Chapter 3, Section 2
Logarithmic Spirals and Planetary Orbits


Individual and Institutional Members may sign in. Click here to join the Library

 

Requires the MathwrightWeb or MathwrightNET ActiveX Control to read in your Browser.
For proper viewing, be sure to use Version 2.15 or later, dated Dec 8, 2003


Library members, download the free Mathwright32 Reader, then press

or

All visitors may preview our

 

Once you download our free Mathwright32 Reader above, then simply click Get This Microworld, and it will be downloaded to your machine and installed in a directory there. You may find it whenever you want to view it, by going to the Start, Programs, Mathwright32 Reader menu.

To visit our Microworlds in your browser, it must be able to read ActiveX controls. Microsoft Internet Explorer 4.0 Browser (or later) is so equipped. You should check that the Security Settings under Tools, Internet Options, Security for the Internet, Custom Level has: