AST101: Our Corner of the Universe Lab 8: Measuring the Mass of Jupiter

Similar documents
The Law of Ellipses (Kepler s First Law): all planets orbit the sun in a

The Mass of Jupiter Student Guide

Prelab 4: Revolution of the Moons of Jupiter

The Revolution of the Moons of Jupiter

Introduction To Modern Astronomy I

Physics 1100: Uniform Circular Motion & Gravity

CESAR Science Case. Jupiter Mass. Calculating a planet s mass from the motion of its moons. Student s Guide

GEOL212 Due 9/24/18 Homework 4

Planetary Orbits: Kepler s Laws 1/18/07

Lecture 23: Jupiter. Solar System. Jupiter s Orbit. The semi-major axis of Jupiter s orbit is a = 5.2 AU

PHYS133 Lab 2 Scale Model of the Solar System

Astronomy 101 Exam 2 Form Akey

Astronomy 101 Exam 2 Form Bkey

Astronomy 101 Exam 2 Form Dkey

Most of the time during full and new phases, the Moon lies above or below the Sun in the sky.

9/12/2010. The Four Fundamental Forces of Nature. 1. Gravity 2. Electromagnetism 3. The Strong Nuclear Force 4. The Weak Nuclear Force

CIRCULAR MOTION AND UNIVERSAL GRAVITATION

Today. Events. Energy. Gravity. Homework Due Next time. Practice Exam posted

Label next 2 pages in ISN Gas Giants. Make sure the following assignments are turned in:

Chapter 13: universal gravitation

CESAR Science Case. Jupiter Mass. Calculating a planet s mass from the motion of its moons. Teacher

Gravitation and the Waltz of the Planets

Gravitation and the Waltz of the Planets. Chapter Four

Gravitation and the Motion of the Planets

Chapter 1 The Copernican Revolution

Lesson 2. NON OPTICAL ASTRONOMY: GRAVITATION SCIENTIFIC CASE: Gravitation. Spokesperson:

18. Kepler as a young man became the assistant to A) Nicolaus Copernicus. B) Ptolemy. C) Tycho Brahe. D) Sir Isaac Newton.

Chapter 14 Satellite Motion

Lecture 13. Gravity in the Solar System

ASTR 310 Tutorial 3: A Human Orrery

Johannes Kepler ( ) German Mathematician and Astronomer Passionately convinced of the rightness of the Copernican view. Set out to prove it!

Universal Gravitation

CESAR Science Case. The mass of Jupiter. Calculating the mass of a planet from the motion of its moons. Teacher Guide

Gravitation & Kepler s Laws

Key Points: Learn the relationship between gravitational attractive force, mass and distance. Understand that gravity can act as a centripetal force.

Today. Laws of Motion. Conservation Laws. Gravity. tides

STANDARD WHII.6a The student will demonstrate knowledge of scientific, political, economic, and religious changes during the sixteenth, seventeenth,

Assignment 1. Due Feb. 11, 2019

Unit 5 Gravitation. Newton s Law of Universal Gravitation Kepler s Laws of Planetary Motion

Gravitation Part I. Ptolemy, Copernicus, Galileo, and Kepler

Name Class Date. For each pair of terms, explain how the meanings of the terms differ.

(BASED ON SG 1609 JUPITER AT OPPOSITION AND SG 1713 ROYAL OPPOSITION! )

Lecture Outlines. Chapter 11. Astronomy Today 8th Edition Chaisson/McMillan Pearson Education, Inc.

End-of-Chapter Exercises

Celestial Objects. Background Questions. 1. What was invented in the 17 th century? How did this help the study of our universe? 2. What is a probe?

Circular/Gravity ~ Learning Guide Name:

Ch. 22 Origin of Modern Astronomy Pretest

Name. Satellite Motion Lab

ACCEL: PATTERNS OF MASS AND DENSITY IN THE SOLAR SYSTEM

Name and Student ID Section Day/Time:

Lecture 4: Kepler and Galileo. Astronomy 111 Wednesday September 6, 2017

PHYS133 Lab 4 The Revolution of the Moons of Jupiter

AP Physics C Textbook Problems

Copyright 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.

Apples and Planets. PTYS Feb 2008

Gravity and the Laws of Motion

Patterns in the Solar System (Chapter 18)

The escape speed for an object leaving the surface of any celestial body of mass M and radius d is

Gravity. Newton s Law of Gravitation Kepler s Laws of Planetary Motion Gravitational Fields

The Outer Planets (pages )

Radial Acceleration. recall, the direction of the instantaneous velocity vector is tangential to the trajectory

Lab 6: The Planets and Kepler

Satellites and Kepler's Laws: An Argument for Simplicity

Uniform Circular Motion

6 The Orbit of Mercury

Describe the lifecycle of a star in chronological order and explain the main stages, relating the stellar evolution to initial mass

Exploring The Planets: Jupiter

Circular Motion and Gravitation Auxilliary Items

How big is the Universe and where are we in it?

Gravity and the Orbits of Planets

PLANETARY SYSTEM: FROM GALILEO TO EXOPLANETS

Name: Lab Partner: Department of Physics Gettysburg College Gettysburg, PA 17325

PTYS/ASTR 206 Section 2 Spring 2007 Homework #1 (Page 1/4)

Pull out a ½ sheet or use the back of your old quiz

Physics 12. Unit 5 Circular Motion and Gravitation Part 2

Kepler, Newton, and laws of motion

Explain how it is possible for the gravitational force to cause the satellite to accelerate while its speed remains constant.

(d) State the effect on the magnitude of the centripetal force in the following cases:

Chapter 4. The Origin Of Modern Astronomy. Is okay to change your phone? From ios to Android From Android to ios

Astron 104 Laboratory #6 The Speed of Light and the Moons of Jupiter

Adios Cassini! Crashed into Saturn 9/15/17 after 20 years in space.

Chapter 02 The Rise of Astronomy

Monday, October 3, 2011

AY2 Winter 2017 Midterm Exam Prof. C. Rockosi February 14, Name and Student ID Section Day/Time

Overview of Astronautics and Space Missions

1. The bar graph below shows one planetary characteristic, identified as X, plotted for the planets of our solar system.

Name: Earth 110 Exploration of the Solar System Assignment 1: Celestial Motions and Forces Due on Tuesday, Jan. 19, 2016

The Acceleration of Gravity (g)

9.2 Worksheet #3 - Circular and Satellite Motion

ASTR-1010: Astronomy I Course Notes Section III

The Revolution of the Moons of Jupiter Student Manual

7.4 Universal Gravitation

Science Unit Test Grade: 8 Unit 6: Gravity

Astr 2320 Tues. Jan. 24, 2017 Today s Topics Review of Celestial Mechanics (Ch. 3)

Section 37 Kepler's Rules

Key Stage 3: Celestia Navigation Teacher s Notes

Planetary Rings (cont.) Rings / Galilean Satellites 4/10/07

Episode 403: Orbital motion

Name: Date: Hour: 179 degrees celsius. 5% of Earth A 70 pound person would weigh 27 pounds on Mercury.

Our Planetary System. Chapter 7

Transcription:

AST101: Our Corner of the Universe Lab 8: Measuring the Mass of Jupiter Name: Student number (SUID): Lab section number: 1 Introduction Objectives In a previous lab, we measured the mass of the Earth with a pendulum and found it to be 6 10 24 kg. In this lab we will use Kepler s and Newton s laws to measure the mass of Jupiter and see how it compares to the mass of the Earth. Materials A chart showing the motion of the moons of Jupiter, a ruler and a calculator. 2 The Galilean Moons The Galilean moons are the four largest moons of Jupiter and were discovered in 1610 by Galileo Galilei. They are named Io, Europa, Ganymede and Callisto after the lovers of Zeus, the Greek equivalent of the Roman god Jupiter. The Galilean Moons are among the most massive objects in the Solar system, comparable in size to the planet Mercury, with a radius larger than any of the dwarf planets. Figure 1 shows the Galilean moons as seen through a telescope. Galileo observed these moons orbiting Jupiter, providing evidence for the Copernican model of the solar system, rather than the prevailing Earth-centric model of the Solar system. Figure 1: The four Galilean moons of Jupiter seen through an optical telescope. 1

Io, which has a mass of 8.93 10 22 kg is the closest moon to Jupiter, with a semi-major axis of 421, 800 km. Table 1 shows the masses and semi-major axes of the Galilean moons relative to those of Io. Moon Mass Semi-major axis Io 1 M Io 1 a Io Europa 0.54 M Io 1.6 a Io Ganymede 1.7 M Io 2.5 a Io Callisto 1.2 M Io 4.5 a Io Table 1: The masses and semi-major axes of the Galilean moons, relative to M Io = 8.93 10 22 kg and a Io = 421, 800 km. Remember that Newton s law of gravitation tells us that the force of gravity scales as the mass of the moon, divided by the inverse square of the distance from Jupiter: F = G M JupiterM Moon r 2. (1) If we double the mass of the moon, the force goes up by a factor of 2, but if the moon is twice as far from Jupiter, then force goes down by a factor of 2 2 = 4. First we will rank the Galilean moons by the strength of the force of gravity between the moon and Jupiter. Let s consider Europa, which is 0.54 times as massive as Io and has a semi-major axis 1.6 times that of Io. (For this lab, we will assume that the orbits of the Galilean moons are circular so that r in Newton s law is given by the semi-major axis a.) This means that the force of gravity between Europa and Jupiter is reduced by a factor of 0.54 = 0.21 (2) 1.62 relative to that between Io and Jupiter. So the force between Jupiter and Europa is smaller than that between Jupiter and Io. Using the space below, calculate the strength of the gravitational force between Jupiter and the other two moons (Ganymede and Callisto), relative to the force between Jupiter and Io, and so rank the moons by the strength of the force between Jupiter and each moon from largest to smallest. You do not need to know G or the mass of Jupiter to do this. Largest Smallest 2

3 The Motion of the Galilean Moons Kepler s third law tells us that the square of the period of a planet s (or a moon s or a satellite s) orbit is proportional to the cube of the semi-major axis, or P 2 = Ka 3, (3) where P is the period in years, a is the semi-major axis in A.U. and K is a constant of proportionality. We have seen in a previous lab how this constant K depends on the mass of the object that the planet is orbiting. Newton later showed that all of Kepler s empirical laws could be derived from his own, more fundamental, laws of motion as set forth in his book PhilosophiæNaturalis Principia Mathematica. Newton also showed that the constant of proportionality in the above formula depends upon the masses of the bodies involved P 2 = a 3 /M, (4) where P is the period in years, a is the semi-major axis in A.U. and M is measured in solar masses. The mass of the Sun (written 1 M ) is 1.99 10 33 kg. Remember that a planet s mass does not affect the orbital period of a planet and so M in equation (4) is the mass of the body being orbited. In the above form, we can use Kepler s Third Law to determine the mass M, if we know P and a. In particular, the mass of a planet can be determined from the orbital motion of its moons. In order to apply Newton s revision of Kepler s Third Law, we must know the semi-major axis (in A.U.) as well as the period of one of Jupiter s moons. We will determine each of these from the chart provided on the last page of this lab. We must first make sure we understand what information is contained in the chart. If we observe Jupiter through the telescope at midnight, on October 10, what will we see? In the space below, draw and label a picture of the telescopic view. Be sure you have the correct relative distance of the moons from Jupiter. Draw and label the same situation as viewed from above Jupiter s North Pole. 3

Make another two sketches showing what you would see on October 19. First draw the telescope view Draw and label the same situation as viewed from above Jupiter s North Pole. 4 Measuring the Mass of Jupiter Follow the procedure below to measure the mass of Jupiter: 1. First, obtain the semi-major axes of Callisto and Ganymede. Measure the distance between the extreme points east and west of Jupiter in the motion of Callisto and Ganymede as shown on the chart. Divide by 2 to obtain the semi-major axes with respect to the scale of the chart. All measurements should be made to the nearest tenth of a millimeter. Callisto: a = mm, Ganymede: a = mm. 2. To convert your measurement of the semi-major axis to A.U., measure Jupiter s diameter in mm. Divide Jupiter s diameter at it s equator (9.5 10 4 A.U.) by this measurement to obtain the appropriate scale factor: Scale factor = 9.5 10 4 A.U. Diameter in mm = 3. Multiply the semi-major axis as measured in the scale of the chart by this scale factor to obtain the semi-major axis in A.U. Callisto: a = A.U., Ganymede: a = A.U. = 4

4. Next we will find the period of Callisto and Ganymede orbit s about Jupiter. Again, referring to the chart, measure the distance between the maxima of the greatest eastern or western elongation from Jupiter. Convert this number from days to years, to obtain the period P. Callisto: P = years, Ganymede: P = years. 5. Using your measurements and equation (4) find the mass Jupiter (in solar masses) from both Callisto s and Ganymede s motion. M Jupiter using Callisto s motion: = M, M Jupiter using Ganymede s motion: = M. 6. What is the average of your measurements for Jupiters mass? 7. How much more massive is Jupiter than the Earth, according to your measurements? 5