Lab Title: The Moons of Jupiter (Distance Education Version)

Similar documents
Exercise: Estimating the Mass of Jupiter Difficulty: Medium

Chapter 3 The Science of Astronomy

Lecture 13. Gravity in the Solar System

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

Are Those Sunspots Really on the Sun?

Exploration of the Solar System

Newton s Law of Gravity

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

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

Imaging Systems Laboratory II. Laboratory 4: Basic Lens Design in OSLO April 2 & 4, 2002

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

Astronomy 1140 Quiz 1 Review

Exercise 5.0 LUNAR MOTION, ELONGATION, AND PHASES

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

Earth, Sun and Moon is a set of interactives designed to support the teaching of the QCA primary science scheme of work 5e - 'Earth, Sun and Moon'.

FIRST GRADE 1 WEEK LESSON PLANS AND ACTIVITIES

Beginning of the Universe Classwork 6 th Grade PSI Science

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

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

Lab 7: Gravity and Jupiter's Moons

Changes in Our Sky Grade Two

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

Planning Observations

Tutorial for Tracker and Supporting Software By David Chandler

SIERRA COLLEGE OBSERVATIONAL ASTRONOMY LABORATORY EXERCISE NUMBER III.F.a. TITLE: ASTEROID ASTROMETRY: BLINK IDENTIFICATION

Activity 10 - Universal Time

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

Newton s Law of Universal Gravitation

Newton s Law of Universal Gravitation

Scales of the Universe

Motions of Earth, Moon, and Sun

Lunar Phase Simulator Student Guide

Phases of the Moon. Preliminaries:

FREE FALL. Introduction. Reference Young and Freedman, University Physics, 12 th Edition: Chapter 2, section 2.5

Orientation to the Sky: Apparent Motions

Planetary Orbit Simulator Student Guide

Lesson 26: Reflection & Mirror Diagrams

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?

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

CELESTIAL MOTIONS. In Charlottesville we see Polaris 38 0 above the Northern horizon. Earth. Starry Vault

Class 2 Solar System Characteristics Formation Exosolar Planets

Chapter 7 Our Planetary System. What does the solar system look like? Thought Question How does the Earth-Sun distance compare with the Sun s radius

The University of Texas at Austin. Gravity and Orbits

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

Freehand Sketching. Sections

Our Planetary System. Earth, as viewed by the Voyager spacecraft Pearson Education, Inc.

From Aristotle to Newton

Updates to Graphing with Excel

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

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

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

ACTIVITY 6: Falling Objects

Basic Coordinates & Seasons Student Guide

A.4 The Solar System Scale Model

This activity will show you how to draw graphs of algebraic functions in Excel.

ACCELERATION DUE TO GRAVITY

Chapter 17: Light and Image Formation

Geometric Optics Converging Lenses and Mirrors Physics Lab IV

MARS STUDENT IMAGING PROJECT

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

SolidWorks Tutorial 3 MAGNETIC BLOCK

Experiment 5: Magnetic Fields of a Bar Magnet and of the Earth

E/M Experiment: Electrons in a Magnetic Field.

Coordinate Systems. Orbits and Rotation

Intermediate PowerPoint

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

A Determination of g, the Acceleration Due to Gravity, from Newton's Laws of Motion

HONEY, I SHRUNK THE SOLAR SYSTEM

Chapter 1. Creating Sketches in. the Sketch Mode-I. Evaluation chapter. Logon to for more details. Learning Objectives

Reflection and Refraction

Background Information

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

RAY OPTICS II 7.1 INTRODUCTION

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

1 One Dimensional Horizontal Motion Position vs. time Velocity vs. time

Cycles in the Sky. Teacher Guide: Cycles in the Sky Page 1 of Discovery Communications, LLC

The Solar System. Olivia Paquette

Magnetic Fields and Their Effects

ASTR 1030 Astronomy Lab 65 Celestial Motions CELESTIAL MOTIONS

Classroom Exercise ASTR 390 Selected Topics in Astronomy: Astrobiology A Hertzsprung-Russell Potpourri

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

SPEED, VELOCITY, AND ACCELERATION

Name Partners Date. Energy Diagrams I

The Force Table Vector Addition and Resolution

Science Standard 4 Earth in Space Grade Level Expectations

Vocabulary - Understanding Revolution in. our Solar System

Introduction to Netlogo: A Newton s Law of Gravity Simulation

Observing the Constellations of the Zodiac

Mirror, mirror - Teacher Guide

Introduction to the Solar System

1.2 Investigations and Experiments

Study Guide due Friday, 1/29

Science 9 Worksheet 13-1 The Solar System

Gravitation and Newton s Synthesis

Protocol for Microscope Calibration

Experiment 6: Magnetic Force on a Current Carrying Wire

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

Due Tuesday, January 27th IN CLASS. Grading Summary: Question 11: 12 points. Question 12: 26 points. Question 13: 12 Points.

Excel Basics By Tom Peters & Laura Spielman

Transcription:

Name: Lab Title: The Moons of Jupiter (Distance Education Version) Equipment: Scientific calculator, computer, and the Contemporary Laboratory Experiences in Astronomy (CLEA) computer program Moons of Jupiter. Purpose: In this lab, you shall measure the orbital properties of Jupiter's moons, and analyze their motions using Kepler's Third Law in order to obtain the mass of Jupiter. Introduction and Historical Background: We can deduce some properties of celestial bodies from their motions despite the fact that we cannot directly measure them. In 1543, Nicolas Copernicus hypothesized that the planets revolve in circular orbits around the Sun. Tycho Brahe (1546-1601) carefully observed the locations of the planets and 777 stars over a period of 20 years using a sextant and compass. These observations were used by Johannes Kepler, a student of Brahe's, to deduce three empirical mathematical laws governing the orbit of one object around another. In 1609, Galileo Galilei heard of the invention of a new optical instrument by a Dutch spectacle maker, Hans Lippershey. By using two lenses, one convex and one concave, Lippershey found that distant objects could be made to look nearer. This instrument was called a telescope. Without even having seen an assembled telescope, Galileo was able to construct his own telescope with a magnification of about three. He soon perfected the construction of the telescope, and became famous as the builder of the world's best telescopes. His best telescopes had a magnification of about thirty. Galileo immediately began observing celestial objects with his crude instrument. He was a careful observer, and published a small book in 1610 of his remarkable discoveries called the Sidereal Messenger. One can imagine the excitement these new discoveries caused in the scientific community. Suddenly, a whole new world was opened! Galileo found sunspots on the Sun, and craters on the Moon. He found that Venus had phases, much as the Moon has phases. He was able to tell that the Milky Way was a myriad of individual stars. He could see that there was something strange about Saturn, but his small telescope was not able to resolve its rings. One of the most important discoveries was that Jupiter had four moons revolving around it. Galileo made such exhaustive studies of these moons that they have come to be known as the Galilean satellites. This "miniature solar system" was clear evidence that the Copernican theory of a Sun-centered solar system was physically possible. Because he was developing a world view which was not easily reconciled with the religious dogma of his period, Galileo was compelled by the Inquisition to neither "hold nor defend" the Copernican hypothesis. Nevertheless, in 1632 he published his

Dialogue on the Great World Systems which was a thinly disguised defense of the Copernican system. This led to his trial, his forced denunciation of the theory, and confinement to his home for the rest of his life. In this lab, you are going to repeat Galileo's observations (without threat of government condemnation!). Today, however, we also know the size of Jupiter. Jupiter's diameter is 11 times Earth's diameter, or about 1.5 10 5 kilometers. The data collected in this experiment and this information allow us to determine the mass of Jupiter. Kepler s Third Law: When one body such as a moon orbits around a much more massive parent body, Kepler's Third Law is: m = a p 3 2 m is the mass of the parent body, in units of the mass of the Sun. a is the length of the semi-major axis of the elliptical orbit in units of the mean Earth-Sun distance, A.U. (Astronomical Unit). If the orbit is circular (as will be assumed in this lab), the semi-major axis is the same as the radius of the orbit. p is the period of the orbit in Earth years. The period is the amount of time required for a moon to orbit the parent body once. This law applies to planets orbiting about the Sun (check: for the Earth orbiting around the Sun: a = 1 A.U. and p = 1 year, and we obtain for the mass of the Sun: m = 1 solar mass) or to any moon orbiting around its planet. You will be determining a and p for the Galilean moons of Jupiter and then m J, the mass of Jupiter, in solar masses. In this computer simulation, you will first determine a in units of Jupiter's Diameter (J.D.) and the period p will be in Earth-days. You will convert these units to A.U. and years at the end of the lab. Jupiter's Moons This lab can in principle be done by anyone with a set of binoculars or a small telescope. The computer simulation Moons of Jupiter replaces actual observing sessions at the observatory using the telescope. The computer simulation is based on the real orbital data for each satellite. As a matter of fact, if you were to set the simulation for today's date and time, you could verify the position of the Jovian moons by direct observation through a telescope at an observatory. You will note that the computer also

provides you some of the pitfalls of actual live telescopic observations such as occasional cloudy nights! You will obtain data from 18 clear observing sessions making observations twice per evening, spaced 12 hours apart. We could do this lab for any one moon of Jupiter. If we did the experiment very accurately, the answer for Jupiter's mass should be the same whatever moon we used. But there will be errors, and we shall use data collected on all four Galilean moons of Jupiter. They are named Io, Europa, Ganymede and Callisto, in order of increasing actual distance from Jupiter. You can remember the order by the mnemonic "I Eat Green Carrots". We also refer to them in this exercise as moons I, II, III, and IV. If you looked through any small telescope, the picture might look like this: The moons appear to be lined up because we are looking edge-on to the orbital plane of the moons around Jupiter. As time goes by, the moons will move about Jupiter. Thus, while the moons move in roughly circular orbits, we generally see only the apparent distance of each moon from Jupiter's center as projected in the east-west direction which is perpendicular to the line-of-sight between Jupiter and Earth. On the computer screen, Jupiter and its moons will look much like Galileo's original sketches. Remember that west is to the right and east is to the left on the screen. This is the way the sky looks through a telescope. It will be necessary to record the apparent (east-west) distance of a moon from Jupiter's center in units of Jupiter diameters (J.D.). Lucky for you, the measurement mode of the computer equipment you will use provides a direct readout in J.D. The computer simulation will be presenting data on the moons as they would be seen every 12 hours. Such observations are possible only in the winter time when the nights are long. The observations are complete when you have obtained a total of at least 18 actual observations NOT counting cloudy days. For each moon and for each of the 18 observing sessions, you are to measure the apparent distance of the moon from Jupiter. The data you will collect will be placed on the Data Table or printed out as a comparable spreadsheet. Procedure: You will need to download the CLEA Moons of Jupiter simulation by clicking the link on your lab schedule website. After downloading it, run the program JupLab.EXE

and follow the installation instructions. When you have finished installing the program, click on the yellow Jupiter Moons icon to start the simulation program. The Moons of Jupiter program simulates the operation of an automatically controlled telescope with a Charge-Coupled Device (CCD) camera that provides a video image to a computer screen. It is a sophisticated computer program that allows convenient measurements to be made at the computer console, as well as adjusting the telescope's magnification. The computer simulation is realistic in all important ways, and using it will give you a good feel for how modern astronomers actually collect data and control their telescopes. Instead of using a telescope and actually observing the moons for many nights, the Moons of Jupiter computer simulation shows the moons to you as they would appear if you were to look through a telescope at the specified time. Initial Setup After the display of a couple of introductory graphics, a Student Accounting dialog box appears. If it does not appear, click File Log In. Enter your name. You may leave the laboratory table field blank. When you have finished logging in, click File Run. The Set Date/Time dialog box will appear. Startup values are needed by the computer to establish your initial observation session. The students at each computer will perform and analyze a different set of observing sessions. Enter today s date, leaving the Universal Time set to 0. When you have finished entering the date and time, click File Timing and change the Observation Interval to 12 hours. The Main Telescope Screen After you have entered all of this information into the computer, it will display a screen similar to that shown below. If you wish to make adjustments later you can do so by clicking on the File menu and choosing Observation Date or Timing. You control the observing session from this Main Telescope Screen. Notice that Jupiter is displayed in the center of your computer screen. To either side are the small point-like Galilean satellites. Sometimes a moon is behind Jupiter, so it cannot be seen. Even at high magnifications, the moons are very small compared to Jupiter. The current telescope magnification is shown in the upper left corner. The date, the UT (Universal Time -- the time in Greenwich, England), and the Julian Day are all displayed in the lower left-hand corner of the screen. You may select Help from the menu to receive on-line help at any time while you are in the Main Telescope Screen. You can display the screen at four scales of magnification by clicking on the 100X, 200X, 300X, and 400X buttons at the bottom of the screen. Try them now. To improve the accuracy of your measurement of a moon, you should always use the largest possible magnification which leaves the moon visible on the screen. Be careful NOT to click the button marked Next just yet!

Now, position the mouse cursor over the screen and hold down the button. The measurement system turns on and displays the apparent perpendicular distance R (in Jupiter Diameters) that the cursor is away from the center of Jupiter. Notice the edge of Jupiter is R = 0.5 J.D. In order to measure the perpendicular distance of each moon from Jupiter, move the cursor until the moon is centered in the cross hairs and then hold down the mouse button. As you move the mouse, the current position of the cursor appears on the control panel. When the satellite is carefully centered, release the mouse button and information about the moon will appear at the lower right corner of the screen. This information includes the name of the selected moon, the X and Y pixel location on the screen, and the perpendicular distance R (in units of Jupiter's Diameter) from the Earth-Jupiter line-ofsight for the selected moon as well as E or W to indicate whether it is east or west of Jupiter. If the moon's name does not appear, you did not center the moon in the cross hairs exactly and you should try again! If a moon is behind Jupiter, record the apparent distance for that moon as 0 since you don't know its location any better than this.

To measure a moon, always switch to the highest magnification that still leaves the moon on the screen. It is important to use the highest magnification possible for each moon for best accuracy. You have two options about how to record your data. You may print out the data table included in this document and fill it out by hand, or you may hit the Record button on the simulation each time you measure the position of a moon. This will save the data in the CLEA program. If you choose to record your data electronically, then before quitting the program you must click File Data Save.csv Format and then use Excel or another spreadsheet program to access and print your data. In either case, your data table should include the following information: Column 1: Julian Day Columns 2 5: Record each moon's position under the column for that moon. Count positions to the left (east) of Jupiter as negative and those to the right (west) as positive. If Europa were selected and had a R = 2.75 west of Jupiter, you would enter +2.75 in column 5. When you have recorded the Universal Time and perpendicular distance for each moon, click the Next button and the image will advance by the amount of time you specified in the Observation Interval. Note that a certain percentage of observing sessions will be "cloudy". If you encounter bad weather, just click Next. Do NOT remeasure any of the Cloudy Days you will just have to allow for any gaps in your data due to these days. The observations are complete when you have obtained a total of 18 actual observations. Stop collecting data after you have 18 non-cloudy observations and when you have completely finished filling out the Data Table, select File Exit. Remember, once you Exit the program altogether, you cannot continue where you left off! If you are recording your data electronically, be sure to click File Data Save.csv Format before quitting! Analysis Of The Data You will use the data to obtain a graph that looks like this (the data points shown in the graph below are for an imaginary moon named Clea and is different from the moons in the lab).

Time (days) p = 14 days p = 0.0383 years a = 3.0 J.D. a = 0.00286 A.U. Each dot in the figure is one observation of Moon Clea. Note the irregular spacing of dots, due to clouds or poor weather and other observing problems on some nights. The curve drawn through the points is the smooth curve that would be made by Clea if you had enough observations. The shape of the curve is called a sine curve. You will need to determine the sine curve that best fits your data in order to determine the orbital properties of each moon. Here are a few hints: (i) the orbits of the moons are regular, that is, they don't speed up or slow down from one period to the next, and (ii) the actual radius of each orbit does NOT change from one period to the next. The sine curve that you draw through your data points should therefore also be REGULAR and SMOOTH. It should go through all of the points, and NOT be higher at the maxima in some places than others. It should also NOT be wider in some places than others.

Using the data from Moon Clea shown in the above graph, it is possible to determine both the radius, a, and the period, p, of the orbit for each moon. The period is the time it takes to get back to the same point in the orbit. Thus: (i) the time between two consecutive maxima (or minima) is the period, (ii) the time between two consecutive crossings at 0 J.D. is equal to 1/2 the period because this is the time it takes to get from the front of Jupiter to the back of Jupiter (or vise versa) which is 1/2 way around in its orbit, (iii) the time between a crossing at 0 J.D and the nearest maximum or minimum is equal to 1/4 the period. For some moons, you may not get enough observations for a full period, so these points may be of use to you in determining the period, even though the moon has not gone through a complete orbit. On the other hand, if you have enough observations for several cycles, you can find a more accurate period by taking the time it takes for a moon to complete, say, 4 cycles, and then dividing it by 4. Your period must then be converted to units of years by dividing by 365.25 days. Remember, it is important to stay in the correct set of units if you are going to use Kepler's Third Law. You can determine the semi-major axis (the radius), a, for each moon by measuring the maxima and minima in your smooth sine curves. When a moon is at the maximum position eastward or westward, it is at the largest apparent distance from the planet. Remember that the orbits of the moons are nearly circular, but since we see the orbits edge on, we can only determine the actual radius of the orbit when the moon is at its maximum position eastward or westward from Jupiter. Repeat Steps 1 4 below for each of the four Jovian moons that you measured: Step 1. Enter the data for the four moons on the graphs provided for each one. Along the horizontal scale, write day numbers starting on the left with the number of the first day on which you have data. Calibrate the horizontal scale of each graph to make your data as stretched out as possible. (The graph for Io, in particular, will benefit from this stretching). The vertical scale is already marked. Each day's measurement of a moon's apparent separation from Jupiter should give you one dot on the graph for that moon. Since each observing day has two sessions, be sure that each point on the graph on the horizontal axis represents only one session. Remember NOT to plot any points for Cloudy Days since you don't know where any of the moons are on those days. Step 2. For each moon, draw a smooth sine curve through the points. Mark all maxima and minima on the curve by crosses. They need not fall on one of the grid lines. The curve should be symmetric about the horizontal line corresponding to zero apparent separation. The maxima and minima should have the SAME values, except for their sign. Step 3. Read off the period, p, and the semi-major axis, a, from your figure, in the manner shown in the earlier example for Moon Clea. These units will be days for p and J.D. for a.

Step 4. To obtain p in years, divide your result in days by 365.25 since there are 365.25 days in a year. To obtain a in A.U., divide your result in J.D. by 1050, since there are 1050 Jupiter diameters (J.D.) in one A.U. Enter your converted values in the spaces provided at the bottom of each graph. You now have all the information you need for each of the four moons to use Kepler's Third Law, to determine the mass of Jupiter, m J, as: where: m J = p has units of years, a has units of A.U.'s, and m J has units of solar masses. a p 3 2

Data Table Example: Julian Day Io Europa Ganymede Callisto 2454740.5 +2.95 +2.75 7.43 +13.15 2454741.0 0.86 +4.70 6.30 +13.15 Your Data: Julian Day Io Europa Ganymede Callisto Continue making measurements until you have 18 observations.

p = days p = years a = J.D. a = A.U. p = days p = years a = J.D. a = A.U.

p = days p = years a = J.D. a = A.U. p = days p = years a = J.D. a = A.U.

Use the space below to show your four separate calculations of Jupiter's mass based on your observations of each Galilean moon. Don't forget to include the appropriate units for the mass of Jupiter. Summarize your calculations for the mass for Jupiter in each of the four cases below: Io: m J = solar masses Europa: m J = solar masses Ganymede: m J = solar masses Callisto: m J = solar masses Hint: If one of the values is very different from the other three, look for a source of error. Perhaps the data are not adequate for a better result, in which case leave the value as you obtained it. Average mj = solar masses.

Additional Questions and Discussion: 1. Convert your average value for mj into kilograms by multiplying your previous result (in solar masses) times the mass of the Sun in kilograms (this can be found in your textbook). What is the percent difference between your average value for m J and the accepted value (can be looked up online) for the mass of Jupiter in kilograms? 2. To express the mass of Jupiter in units of the mass of the Earth, divide your result from Question 1 above by 5.97 1027 grams, which is the mass of the Earth. SHOW YOUR WORK BELOW. m J = Earth masses. 3. Which of the four Galilean moons was the most difficult to fit a smooth sine curve to? Why?

4. How would you change the time interval between observations for this "difficult" moon? (Remember that since you are observing from the surface of the Earth, you are still stuck with a certain amount of time each day when Jupiter is not visible!) 5. When a moon was not visible because it was behind Jupiter, you entered 0 J.D. for its apparent distance from Jupiter. However, all you really know from your measurement is that it's apparent distance was somewhere between the edges of Jupiter at +0.5 J.D. and at 0.5 J.D. How would you account for this uncertainty when drawing your smooth sine curve through all of your "0 J.D." points? 6. Suppose that you were only able to get telescope time to observe Jupiter's moons once every 4 days instead of once every 12 hours as in this lab. Which of Jupiter's four moons would you still be able to fit accurately to a sine curve and which ones would be very difficult to fit? Why?