How big is the Milky Way? Introduction. by Toby O'Neil. How big is the Milky Way? about Plus support Plus subscribe to Plus terms of use

Similar documents
Making the grade: Part II

Making the grade. by Chris Sangwin. Making the grade

Assignment #9 Star Colors & the B-V Index

Please bring the task to your first physics lesson and hand it to the teacher.

MITOCW ocw f99-lec01_300k

MITOCW ocw f99-lec05_300k

Extracting beauty from chaos

Measure for measure. by Andrew Davies. Measure for Measure, or, How to make a carpet out of nothing. Measure for measure

Solving with Absolute Value

Outer space: A matter of gravity

Homework on Properties of Galaxies in the Hubble Deep Field Name: Due: Friday, April 8 30 points Prof. Rieke & TA Melissa Halford

0. Introduction 1 0. INTRODUCTION

Primary KS1 1 VotesForSchools2018

PHY323:Lecture 7 Dark Matter with Gravitational Lensing

MITOCW 6. Standing Waves Part I

Catching waves with Kip Thorne

It is a very human trait to wonder where we are in this universe. Usually, the only hint of the vastness of the universe comes at night.

Homework #7: Properties of Galaxies in the Hubble Deep Field Name: Due: Friday, October points Profs. Rieke

MITOCW ocw f99-lec30_300k

What is Crater Number Density?

Preparing Your Magical Equipment

Note: Please use the actual date you accessed this material in your citation.

Instructor (Brad Osgood)

Remote Sensing/Reflectance Spectrometer

PHYSICS 107. Lecture 27 What s Next?

Electromagnetic Theory Prof. D. K. Ghosh Department of Physics Indian Institute of Technology, Bombay

An Intuitive Introduction to Motivic Homotopy Theory Vladimir Voevodsky

The Hubble Deep Field

Water tank. Fortunately there are a couple of objectors. Why is it straight? Shouldn t it be a curve?

4.3 The accelerating universe and the distant future

Chapter 23 Lecture. The Cosmic Perspective Seventh Edition. Dark Matter, Dark Energy, and the Fate of the Universe Pearson Education, Inc.

Physics Lab #2: Spectroscopy

Lecture Tutorial: Using Astronomy Picture of the Day to learn about the life cycle of stars

MITOCW MITRES18_005S10_DiffEqnsGrowth_300k_512kb-mp4

If you have completed your extra credit opportunity, please place it on your inbox.

Physics 10 Spring Final Exam: You are a Turtle. Name:

GAP CLOSING. Algebraic Expressions. Intermediate / Senior Facilitator s Guide

Group Member Names: You may work in groups of two, or you may work alone. Due November 20 in Class!

MITOCW ocw f99-lec17_300k

Assignment #12 The Milky Way

Physics Lab #4: Citizen Science - The Milky Way Project

Understanding the Universe S TA R T ING WITH EARTH A ND B E YO ND

MITOCW watch?v=pqkyqu11eta

UNIT 1 MECHANICS PHYS:1200 LECTURE 2 MECHANICS (1)

A Brief Guide to Our Cosmic Context

A supernova is the explosion of a star. It is the largest explosion that takes place in space.

Finding the Median. 1 The problem of finding the median. 2 A good strategy? lecture notes September 2, Lecturer: Michel Goemans

The importance of beings fractal

Properties of Sequences

Chapter 23 Lecture. The Cosmic Perspective Seventh Edition. Dark Matter, Dark Energy, and the Fate of the Universe Pearson Education, Inc.

Note: Please use the actual date you accessed this material in your citation.

MITOCW ocw-18_02-f07-lec02_220k

Star Systems and Galaxies

MI 4 Mathematical Induction Name. Mathematical Induction

Galaxies and The Milky Way

MITOCW ocw f99-lec09_300k

Module 8: The Cosmos in Motion. UNC-TFA H.S. Astronomy Collaboration, Copyright 2011

Chapter 16 Dark Matter, Dark Energy, & The Fate of the Universe

Physics 10 Summer Midterm #1: You Are a Dog. Name:

Review of Lecture 15 3/17/10. Lecture 15: Dark Matter and the Cosmic Web (plus Gamma Ray Bursts) Prof. Tom Megeath

Volume vs. Diameter. Teacher Lab Discussion. Overview. Picture, Data Table, and Graph

Galaxy Classification and the Hubble Deep Field

Plasma Physics Prof. V. K. Tripathi Department of Physics Indian Institute of Technology, Delhi

Isaac Newton & Gravity

1.20 Formulas, Equations, Expressions and Identities

Mathematics-I Prof. S.K. Ray Department of Mathematics and Statistics Indian Institute of Technology, Kanpur. Lecture 1 Real Numbers

ENZYME KINETICS AND INHIBITION

Fractals and Dimension

Modern Algebra Prof. Manindra Agrawal Department of Computer Science and Engineering Indian Institute of Technology, Kanpur

What is Quantum Mechanics?

MITOCW free_body_diagrams

Sundaram's Sieve. by Julian Havil. Sundaram's Sieve

Graphical Analysis; and Vectors

Study skills for mathematicians

Black Holes, or the Monster at the Center of the Galaxy

Slope Fields: Graphing Solutions Without the Solutions

2 Systems of Linear Equations

Basics of Proofs. 1 The Basics. 2 Proof Strategies. 2.1 Understand What s Going On

Functions and graphs - Grade 10 *

ASTRO 114 Lecture Okay. We re now gonna continue discussing and conclude discussing the entire

ABE Math Review Package

Experiment 1: The Same or Not The Same?

MITOCW MITRES18_005S10_DerivOfSinXCosX_300k_512kb-mp4

What is proof? Lesson 1

Surveying Prof. Bharat Lohani Department of Civil Engineering Indian Institute of Technology, Kanpur. Module - 11 Lecture No. # 01 Project surveys

Sections 8.1 & 8.2 Systems of Linear Equations in Two Variables

5th Grade. Slide 1 / 67. Slide 2 / 67. Slide 3 / 67. Matter and Its Interactions. Table of Contents: Matter and Its Interactions

Electro Magnetic Field Dr. Harishankar Ramachandran Department of Electrical Engineering Indian Institute of Technology Madras

ASTRO 114 Lecture Okay. What we re going to discuss today are what we call radiation laws. We ve

Lab 1: Measurement Errors Adapted from Holtzman's Intro Lab for Astr110

Slope Fields and Differential Equations. Copyright Cengage Learning. All rights reserved.

But, there is always a certain amount of mystery that hangs around it. People scratch their heads and can't figure

ASTRO 1050 LAB #10: The Structure of the Milky Way Galaxy

Cosmology: the History of the Universe

MATH 320, WEEK 2: Slope Fields, Uniqueness of Solutions, Initial Value Problems, Separable Equations

2 Exercises 1. The following represent graphs of functions from the real numbers R to R. Decide which are one-to-one, which are onto, which are neithe

Nuclear Physics Fundamental and Application Prof. H. C. Verma Department of Physics Indian Institute of Technology, Kanpur

Calculus 140, section 4.7 Concavity and Inflection Points notes by Tim Pilachowski

Isaac Newton was a British scientist whose accomplishments

Astronomy 1. 10/17/17 - NASA JPL field trip 10/17/17 - LA Griffith Observatory field trip

Transcription:

about Plus support Plus subscribe to Plus terms of use search plus with google home latest issue explore the archive careers library news 1997 2004, Millennium Mathematics Project, University of Cambridge. Permission is granted to print and copy this page on paper for non commercial use. For other uses, including electronic redistribution, please contact us. May 2001 Features How big is the Milky Way? by Toby O'Neil Introduction How big is the Milky Way? 1

A photograph of part of the Milky Way, courtesy of NASA All objects attract each other and when we look up at a (clear) night sky we see many massive stars all exerting forces on each other. A question which has been vexing astronomers for a long time is whether these forces of attraction between stars and galaxies will eventually result in the universe collapsing back into a single point, or whether it will expand forever with the distances between stars and galaxies growing ever larger. The answer to this question turns out to depend on how much matter the universe contains: the more matter, the more attraction and the more likely the "collapse" theory. So how can we find how much matter there is in the universe? In this article, I'm going to describe how the mathematical theory of dimension gives us one way of approaching this question, and helps us to estimate how much visible matter there is in the universe. What is dimension? We all think of a line segment as being one dimensional, a square two dimensional and a cube three dimensional, but what does this really mean? Intuitively, the dimension of an object should measure how well it fills space, how "wriggly" it is: the problem is to turn this intuitive idea into a mathematical definition. In order to reduce problems with visualising what is happening, we consider objects sitting in the plane. We begin by looking at a line and a square more closely. The line Consider a line segment sitting in the plane we expect this to be one dimensional. If we split the plane up into squares of the same side lengths r and count how many hit the line segment, what do we find? In the figure below we have divided the plane up into boxes of side lengths, 1, 1/2, 1/4 and 1/8, and counted how many of the boxes hit (or intersect) a particular line segment. What is dimension? 2

Finding the box dimension of a line segment If we tabulate the results we find the following: Side length 1 1/2 1/4 1/8... 2 k Number of boxes 2 8 16 28... approx 2 k Thus, if N r denotes the number of boxes of side length r required to cover the line segment, then The square N r r 1 =(1/r) 1. Now consider a square. This is something which we would expect to be two dimensional. Again, if we split the plane up into squares of the same side lengths r and count how many hit our square, what do we find? In the figure below we have divided the plane up into boxes of side lengths, 1, 1/2, 1/4 and 1/8, and counted how many of the boxes hit (or intersect) a particular line segment. The square 3

Finding the box dimension of a square Side length 1 1/2 1/4 1/8... 2 k Number of boxes 4 4 16 64... approx 2 2k Thus, if N r denotes the number of boxes of side length r required to cover the square, then N r r 2 =(1/r) 2. Thus for these examples we find that when r is very small, then the number of boxes of side length r required to cover the set is roughly (1/r) to the power of the dimension. This suggests that we make the following definition: The (box) dimension of a set E is the number d such that the number of boxes of side length r required to cover E is proportional to r d. A strange set Now let us consider something a little more complicated, a set which is somewhere between being a line and a square in that its dimension will turn out to be between one and two. We construct it as follows: We start with a square of side length 1, and we split it into 9 smaller subsquares of side lengths 1/3. We then keep the four corner subsquares and throw the rest away. For each of these four squares we then repeat the process: we divide each up into 9 smaller squares of side lengths 1/9 and keep only the four corner squares of these new squares. We repeat this process forever..., and in the end obtain the object illustrated below. This A strange set 4

sort of set is known as a Cantor Dust and is named after the German mathematician Georg Cantor, who was one of the pioneers of modern mathematical analysis. A Cantor Dust Let's now try to find the box dimension of this set. If, instead of boxes of side lengths 1,1/2, 1/4, 1/8,..., we use boxes of side lengths (1/3) k, k=1,2,3,, then we need exactly (4 k ) boxes to cover the set. Hence and we can calculate that log(n (3 k)) log(3 k ) = log(4 k ) klog(3) N (3 k ) = 4 k = klog(4) klog(3) = log(4) log(3) 1.26. We deduce that the box dimension of this set is 1.26. This is an example of what is known as a fractal set since its dimension is not a whole number. Comparing this object to our picture of the Milky Way, we see that the Milky Way appears to have a far denser distribution of matter, and so we expect that our calculation of the dimension of the Milky Way will give an answer which is larger than 1.26. The box dimension of our photo of the Milky Way Now we'll look at the photo at the beginning of this article, and use it to try to estimate the box dimension of the Milky Way. We begin by modifying the photo to create an image which is amenable to analysis: calculations of box dimension require a completely black and white image no greyscale is allowed. We do this by first inverting the greyscale so that the stars are black and the empty space is white. We then convert the picture to a black and white image, by making anything above a certain level of grey, black, and colouring the remainder, white, as above. There is a certain amount of freedom as to the choices we make here and we shall need to consider how this affects the accuracy of our results later on. The box dimension of our photo of the Milky Way 5

Inverting the greyscale Changing greyscale to black and white We now divide the picture up into a grid of squares (of side length r, say) and count how many contain any black parts of the image. We do this for grids if various sizes and record the results. There are many computer programs which can do this rather tedious work for us and I used the Fractal Dimension Calculator to find the counts for boxes of various sizes. The table below shows the number of boxes of various sizes required to cover the stars in our photo. The size of a box is given as a fraction of the image's height. Size of box, s 1 6 0.5 18 0.4375 28 0.375 40 0.3125 45 0.25 84 0.1875 120 0.125 252 0.07083 760 0.01667 12066 0.00833 31701 0.00417 47364 Number of boxes, N s If, as we expect, for (small) boxes of side length r, N r cr dim (Milky Way), then taking the log of both sides, we find that The box dimension of our photo of the Milky Way 6

log(n r ) dim (Milky Way)log(1/r) +log(c). Hence, if we plot log(n r ) against log(1/r), then provided the resulting graph is a straight line, then the box dimension of our picture of the Milky Way will be given by the line's slope. In the figure below, we show the resulting graph. A plot of log N(r) against log (1/r). The line of best fit has gradient approximately 1.82 As you can see, the result is a rather convincing straight line with slope about 1.82 and we conclude that the box dimension of our photo of the Milky Way is about 1.82. There is a problem, however we haven't examined the relationship between the dimension of the image in the photo and the dimension of the Milky Way itself! This is our final task. Projections In a photograph, the distances between various stars are distorted and it is also very likely that some stars which are in the Milky Way are not visible on the photo. Thus we expect the photo to show us less than is actually there. Hence any estimate we make of the dimension is likely to be too small. The question is whether we can say anything sensible about what the error is likely to be. Projections 7

Our photo of the Milky Way is a projection, not an accurate representation Our photo of the Milky Way can be viewed as a projection of the Milky Way onto a sheet of paper, see the figure above. Thus it would be useful if, given an object E in space, and a projection P(E) of it, we could find a relationship between their dimensions. If we draw a grid of boxes over E of size r and then look at the corresponding grid on the projection of E, then the number of boxes we need to cover the projection is always less than or equal to the number of boxes we needed to cover E, see the figure below. (We are ignoring the fact that the projected boxes may be distorted when the argument is done more carefully, it turns out that this doesn't matter.) Projecting cannot increase the number of boxes needed Thus N r (P(E)) N r (E) and so log[n r (P(E)]) log[n r (E)] Projections 8

and hence log[n r (P(E))] log( r) log[ N r (E)] log( r) if 0 < r < 1. (We are using the fact that for 0 < r < 1, log(r) > 0.) Thus as we expected. How big is the Milky Way? dim (P(E)) dim (E), It is always possible that the photo we have of the Milky Way is taken from a very special direction where there is a lot of overlapping, see the figure below. In the projection to the right, there is an exceptional amount of overlapping. The projection downwards has less. However, we would expect that if our photograph of the Milky Way is taken from a typical position, then we would not get an exceptional amount of overlap. Our problem is how to measure how much overlap we typically get. Fortunately for us, a very recent result by John Howroyd (a mathematician at Goldsmiths College in London) tells us what to expect. He showed that for the projection from space onto a typical plane of an object, E with dim(e) > 0, then the box dimension of the projection, dim (P(E)), satisfies 1 dim(p(e)) 1 2 1 dim(e) 1 3. If we rearrange this in order to estimate dim(e) in terms of dim (P(E)), then we find that and so, if dim(e) > 0, then which simplifies to give 1 1 1 dim (P(E)) 6 dim(e) 1 dim(e) [1/dim(P(E))] [1/6] dim(e) dim (P(E))., Projections 9

1 [dim(p(e))/6] Hence, on the assumption that the image in our photo of the Milky Way is essentially just a projection of the Milky Way onto a plane in a typical position, we estimate that dim (Milky Way) 1.82 1 [1.82/6] 2.61. That is, the dimension of the Milky Way is no larger than about 2.6. Since we know that its dimension must be at least as large as that estimated from the photo, we conclude that the dimension of the Milky Way lies somewhere between 1.82 and 2.6. Conclusions Our analysis suggests that the dimension of the Milky Way is between 1.82 and 2.6. However there are many potential problems with our approach which may mean these estimates are meaningless! Here are a few of them (you may be able to find others): 1. There was an arbitrary judgement involved in converting our photo into a pure black and white image we had to decide which shades of grey were to be black and which were to be white; 2. The definition of box dimension involves looking at how many boxes cover a set for arbitrarily small boxes. Since our image of the Milky Way was just a computer graphic, it had a scale below which we would learn nothing useful. This is a problem for calculating box dimension of many things in science. 3. We haven't take any account of the fact that astronomers believe that much of the universe is made up of "dark matter" which is not visible to us on Earth this could increase the dimension of the universe substantially. Despite these problems, though, the method does give us some insight into the distribution of matter in the Milky Way. Many of these problems can be overcome and the only one which will always be present, no matter the problem under investigation, is the fact that the calculation of box dimension requires us to look at what happens as the boxes used become arbitrarily small. In practice, this is impossible, and it is a matter of judgement as to whether one has enough data to make a sensible calculation. For many stars, we also know how far away from us they are, and you may wonder whether it is possible to use this information to get better estimates on the dimension. Of course from our viewpoint on Earth, there will be many stars we can't see, and it is unknown if this extra information does enable better estimates to be made. About the author Conclusions 10

Toby O'Neil is a Lecturer in Analysis at the Department of Pure Mathematics of the Open University, and when he's not busy counting boxes, he likes to spend his time staring vacantly into space. Download PDF version Printer friendly version Return to article contact copyright info sponsors privacy info Plus is part of the family of activities in the Millennium Mathematics Project, which also includes the NRICH and MOTIVATE sites. Download PDF version Printer friendly version 11