Exercise: Estimating the Mass of Jupiter Difficulty: Medium



Similar documents
From Aristotle to Newton

Lecture 13. Gravity in the Solar System

PTYS/ASTR 206 Section 2 Spring 2007 Homework #2 (Page 1/5) NAME: KEY

Newton s Law of Gravity

Name: Earth 110 Exploration of the Solar System Assignment 1: Celestial Motions and Forces Due in class Tuesday, Jan. 20, 2015

Unit 8 Lesson 2 Gravity and the Solar System

This paper is also taken for the relevant Examination for the Associateship. For Second Year Physics Students Wednesday, 4th June 2008: 14:00 to 16:00

1.1 A Modern View of the Universe" Our goals for learning: What is our place in the universe?"

Lab 7: Gravity and Jupiter's Moons

Gravitation and Newton s Synthesis

Newton s Law of Universal Gravitation

2. Orbits. FER-Zagreb, Satellite communication systems 2011/12

Astronomy 1140 Quiz 1 Review

AE554 Applied Orbital Mechanics. Hafta 1 Egemen Đmre

A = 6561 times greater. B. 81 times greater. C. equally strong. D. 1/81 as great. E. (1/81) 2 = 1/6561 as great.

Chapter 25.1: Models of our Solar System

GRAVITATIONAL FIELDS PHYSICS 20 GRAVITATIONAL FORCES. Gravitational Fields (or Acceleration Due to Gravity) Symbol: Definition: Units:

An Introduction to Astronomy and Cosmology. 1) Astronomy - an Observational Science

The University of Texas at Austin. Gravity and Orbits

Use the following information to deduce that the gravitational field strength at the surface of the Earth is approximately 10 N kg 1.

Lab 6: Kepler's Laws. Introduction. Section 1: First Law

Name Class Period. F = G m 1 m 2 d 2. G =6.67 x Nm 2 /kg 2

Halliday, Resnick & Walker Chapter 13. Gravitation. Physics 1A PHYS1121 Professor Michael Burton

Newton s Law of Universal Gravitation

NASA Explorer Schools Pre-Algebra Unit Lesson 2 Student Workbook. Solar System Math. Comparing Mass, Gravity, Composition, & Density

Notes: Most of the material in this chapter is taken from Young and Freedman, Chap. 13.

AP Environmental Science Graph Prep

USING MS EXCEL FOR DATA ANALYSIS AND SIMULATION

Planetary Orbit Simulator Student Guide

x Distance of the Sun to planet

Periods of Western Astronomy. Chapter 1. Prehistoric Astronomy. Prehistoric Astronomy. The Celestial Sphere. Stonehenge. History of Astronomy

The orbit of Halley s Comet

Astronomy 110 Homework #04 Assigned: 02/06/2007 Due: 02/13/2007. Name:

Halliday, Resnick & Walker Chapter 13. Gravitation. Physics 1A PHYS1121 Professor Michael Burton

Q3.2.a The gravitational force exerted by a planet on one of its moons is 3e23 newtons when the moon is at a particular location.

Chapter 3 The Science of Astronomy

Study Guide: Solar System

1. Title: Relative Sizes and Distance in the Solar System: Introducing Powers of Ten

Solar System. 1. The diagram below represents a simple geocentric model. Which object is represented by the letter X?

RETURN TO THE MOON. Lesson Plan

GRAVITY CONCEPTS. Gravity is the universal force of attraction between all matter

SOLVING EQUATIONS WITH RADICALS AND EXPONENTS 9.5. section ( )( ). The Odd-Root Property

How To Understand The Theory Of Gravity

Chapter 7 Our Planetary System. Agenda. Intro Astronomy. Intro Astronomy. What does the solar system look like? A. General Basics

Solar System Formation

Orbital Dynamics with Maple (sll --- v1.0, February 2012)

Planets beyond the solar system

Name: Date: Period: Gravity Study Guide

DIRECT ORBITAL DYNAMICS: USING INDEPENDENT ORBITAL TERMS TO TREAT BODIES AS ORBITING EACH OTHER DIRECTLY WHILE IN MOTION

ax 2 by 2 cxy dx ey f 0 The Distance Formula The distance d between two points (x 1, y 1 ) and (x 2, y 2 ) is given by d (x 2 x 1 )

Barycenter of Solar System Earth-Moon barycenter? Moon orbits what?

The Solar System. Unit 4 covers the following framework standards: ES 10 and PS 11. Content was adapted the following:

EDMONDS COMMUNITY COLLEGE ASTRONOMY 100 Winter Quarter 2007 Sample Test # 1

astronomy A planet was viewed from Earth for several hours. The diagrams below represent the appearance of the planet at four different times.

Douglas Adams The Hitchhikers Guide to the Galaxy

Scales of the Universe

Grade 6 Standard 3 Unit Test A Astronomy. 1. The four inner planets are rocky and small. Which description best fits the next four outer planets?

Calculating Astronomical Unit from Venus Transit

Math 1302, Week 3 Polar coordinates and orbital motion

FIRST GRADE 1 WEEK LESSON PLANS AND ACTIVITIES

Binary Stars. Kepler s Laws of Orbital Motion

Physics 53. Gravity. Nature and Nature's law lay hid in night: God said, "Let Newton be!" and all was light. Alexander Pope

In this project, you will be observing at least three objects with a telescope or binoculars, and drawing what you see.

Physics Midterm Review Packet January 2010

Vocabulary - Understanding Revolution in. our Solar System

Solar System Fundamentals. What is a Planet? Planetary orbits Planetary temperatures Planetary Atmospheres Origin of the Solar System

Data Provided: A formula sheet and table of physical constants is attached to this paper. DARK MATTER AND THE UNIVERSE

Name Class Date. true

Orbital Mechanics. Angular Momentum

The Hidden Lives of Galaxies. Jim Lochner, USRA & NASA/GSFC

Beginning of the Universe Classwork 6 th Grade PSI Science

Penn State University Physics 211 ORBITAL MECHANICS 1

Unit One Organizer: The Stars and Our Solar System (Approximate Time: 7 Weeks)

Please be sure to save a copy of this activity to your computer!

NOTES: GEORGIA HIGH SCHOOL SCIENCE TEST THE SOLAR SYSTEM

Forces between masses

Newton s Laws of Motion

The Distance Formula and the Circle

Motions of Earth, Moon, and Sun

Class 2 Solar System Characteristics Formation Exosolar Planets

DESCRIPTION ACADEMIC STANDARDS INSTRUCTIONAL GOALS VOCABULARY BEFORE SHOWING. Subject Area: Science

5- Minute Refresher: Daily Observable Patterns in the Sky

Unit 11: Gravity & the Solar System

UNIT V. Earth and Space. Earth and the Solar System

Solar System Fact Sheet

GETTING STARTED IN STAR GAZING. The fact you are here in this introductory session says you have an interest in the hobby of

SPEED, VELOCITY, AND ACCELERATION

Forces. When an object is pushed or pulled, we say that a force is exerted on it.

Exam # 1 Thu 10/06/2010 Astronomy 100/190Y Exploring the Universe Fall 11 Instructor: Daniela Calzetti

Introduction to Netlogo: A Newton s Law of Gravity Simulation

HONEY, I SHRUNK THE SOLAR SYSTEM

The Solar System. Olivia Paquette

CELESTIAL CLOCK - THE SUN, THE MOON, AND THE STARS

Chapter 5: Circular Motion, the Planets, and Gravity

Chapter 1: Our Place in the Universe Pearson Education Inc., publishing as Addison-Wesley

Phases of the Moon. Preliminaries:

Satellites and Space Stations

The sun and planets. On this picture, the sizes of the sun and 8 planets are to scale. Their positions relative to each other are not to scale.

Transcription:

Exercise: Estimating the Mass of Jupiter Difficulty: Medium OBJECTIVE The July / August observing notes for 010 state that Jupiter rises at dusk. The great planet is now starting its grand showing for the late Summer and Autumn. Jupiter s ideal position in the sky also presents a great opportunity for amateur astronomers to discover for themselves how scientists have been able to determine some of the important characteristics of our solar system. In this simple practical experiment you will use observational data acquired over a number of evenings using your own telescope and just a little basic mathematics - to estimate the mass of the planet Jupiter, the largest planet in our solar system. EQUIPMENT All you need to perform this experiment are: A telescope with enough magnification to show Jupiter as a small disk A pen and paper to record your observations An up to date star map to give you the location of Jupiter in the sky SOME BACKGROUND HOW DO YOU WEIGH A PLANET? Kepler discovered the laws of planetary motion in 1609 by analyzing Tycho Brahe s observations of planetary motion. Kepler s three laws of planetary motion describe the orbits of planets about the Sun. Isaac Newton later generalised these laws to describe the motion of any two bodies orbiting their common centre of mass. First Second Third The relative orbit of two bodies is a conic section with one of the objects at a focus. The line connecting the two bodies sweeps out equal areas in equal times. The product of the square of the period and the total mass of the system is proportional to the cube of the mean separation of the bodies You can use Newton s version of Kepler s third law to determine the total mass within any system of orbiting bodies by using measurements just so long as you can determine the orbital period and the separation. Farnham Astronomical Society

METHOD This very simple method can be used to estimate the mass of Jupiter from your own observations of its moons orbits: 1. Using your telescope, measure the positions of the four moons of Jupiter (Io, Europa, Ganymede and Callisto) at regular intervals.. Plot your observations for each moon on a graph (when the clouds permit). Determine the period (T) and semi-major axis (a) for the orbit of each moon from your graphs. 4. Calculate the mass of Jupiter as the average of the four values for Jupiter's mass calculated from your individual observations. Note that the principles behind this method are used by Astronomers to calculate the masses of the other planets in our solar system, the mass of the Sun, the masses of binary stars and even galaxies. Step 1: Measuring the positions of Jupiter s four moons To measure the positions, use the highest magnification that still allows all four moons to occupy the field of view with Jupiter centred in the field of view. Estimate the distance as the number of Jupiter diameters from the centre of the planet to the moon (or better still, use a reticule eyepiece if you have one). Herein lays your first challenge how do you tell which moon is which? You might be able to work this out by looking at your data knowing that Io completes an orbit in about two days, Europa takes three and a half days Ganymede takes a little over seven days and Callisto has a period of over two weeks. Remember also that the radius of Io s orbit is much smaller than that of Callisto. Alternatively you can use ephemeris data published in an astronomy magazine to help you. Record the date, time and distances. You can use the observation record sheet at the end of this document to record observations print off as many copies of this sheet as you need to record your nightly observations. When you record the distances make the distance a positive value if the moon is to the West of Jupiter and a negative value if the moon is to the East of Jupiter (alternatively mark your measurements with an E or W as appropriate. You will also find that moons are not visible when their orbit takes them behind the planet (simply record these distances as zero). Observations every 4 hours (if the clouds permit) should allow you to create a rough curve for Callisto but more frequent measurements will be required for the other moons. The more measurements you make the more smooth your curve will be. Step : Plot your data Plot a graph of distance (Y axis) against time in days (X Axis). Remember to plot fractions of days correctly (i.e. 1800hrs is 0.75 of a day). The graph below shows a data plot for an imaginary moon. With gaps in your data don t expect to see anything quite this perfect. If you have too much uncertainty then take more frequent observations until you have collected enough good quality data. Farnham Astronomical Society Page of 4

5 Distance (Jupiter Diameters) 4 1 0-1 - - -4 Period (T) 1 5 7 9 11 1 15 17 19 1 5 7 9 1 5 7 9 41 Radius (a) -5 Time (days) Step : Determine the period and semi-major axis Sketch a smooth curve which best represents the data and taking in as many points on your graph as possible. The curve should be a sine curve. Consider rechecking points which look very different from their expected position. Don t worry about the zero values when the moon disappeared behind Jupiter, just plot the zeros on the graph as shown above. The period T and the radius a can be read from your graph directly. In this made-up example: Period (T) = 10 days (8.64 x 10 5 seconds). Radius (a) = 4 Jupiter diameters (approx 5.7x10 8 metres). Step 4: Calculate the mass of Jupiter This is where the maths comes in, but thankfully it is all basic stuff. To calculate the mass of Jupiter you simply use Newton s version of Kepler s Third Law. T 4π = G a. M + m Where M is the mass of Jupiter and m is the mass of the moon and G is the universal gravitational constant (6.67 x 10-11 m / kg-sec ). Because the mass of the moon (m) is so small compared to the mass of Jupiter (M) we are able to remove m from the equation. Rearranging we get: 4π M = G a. T Farnham Astronomical Society Page of 4

Simply plug in your values for a and T into this formula to calculate the mass of Jupiter using your data for the four moons (remembering to convert the radius a into metres and the period T into seconds) then take the average value. ANALYSIS OF YOUR RESULTS Look up the mass of Jupiter (look it up on the web, try using the Wolfram Alpha search engine). Are your results consistent with the currently accepted value? If not, why do you think this is? Lookup details of the period and radius of the Moon s orbit and try calculate the mass of the Earth. Is the margin of error any more or less than your calculation for Jupiter. Why do you think this is? If you try this experiment for yourself let us know how you got on and how well your result compared with the accepted figure. You can use the comment form at the bottom of this post to leave your answer. If you are feeling adventurous try this approach to calculate the mass of Saturn; this is a little harder because the moons are fainter and unlike Jupiter the moons of Saturn are not conveniently in a line. You will need to take a little more care calculating the radius of the orbits. Farnham Astronomical Society Page 4 of 4

Observing Log Sheet #: Observation details Distance from Centre of Jupiter (in Jupiter Diameters) Date Time Io Europa Ganymede Callisto Farnham Astronomical Society