What Are Jupiter and Its Moons Like?
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Introduction to Astronomy from Darkness to Blazing Glory
Introduction to Astronomy From Darkness to Blazing Glory Published by JAS Educational Publications Copyright Pending 2010 JAS Educational Publications All rights reserved. Including the right of reproduction in whole or in part in any form. Second Edition Author: Jeffrey Wright Scott Photographs and Diagrams: Credit NASA, Jet Propulsion Laboratory, USGS, NOAA, Aames Research Center JAS Educational Publications 2601 Oakdale Road, H2 P.O. Box 197 Modesto California 95355 1-888-586-6252 Website: http://.Introastro.com Printing by Minuteman Press, Berkley, California ISBN 978-0-9827200-0-4 1 Introduction to Astronomy From Darkness to Blazing Glory The moon Titan is in the forefront with the moon Tethys behind it. These are two of many of Saturn’s moons Credit: Cassini Imaging Team, ISS, JPL, ESA, NASA 2 Introduction to Astronomy Contents in Brief Chapter 1: Astronomy Basics: Pages 1 – 6 Workbook Pages 1 - 2 Chapter 2: Time: Pages 7 - 10 Workbook Pages 3 - 4 Chapter 3: Solar System Overview: Pages 11 - 14 Workbook Pages 5 - 8 Chapter 4: Our Sun: Pages 15 - 20 Workbook Pages 9 - 16 Chapter 5: The Terrestrial Planets: Page 21 - 39 Workbook Pages 17 - 36 Mercury: Pages 22 - 23 Venus: Pages 24 - 25 Earth: Pages 25 - 34 Mars: Pages 34 - 39 Chapter 6: Outer, Dwarf and Exoplanets Pages: 41-54 Workbook Pages 37 - 48 Jupiter: Pages 41 - 42 Saturn: Pages 42 - 44 Uranus: Pages 44 - 45 Neptune: Pages 45 - 46 Dwarf Planets, Plutoids and Exoplanets: Pages 47 -54 3 Chapter 7: The Moons: Pages: 55 - 66 Workbook Pages 49 - 56 Chapter 8: Rocks and Ice: -
1. Two Objects Attract Each Other Gravitationally. If the Distance Between Their Centers Is Cut in Half, the Gravitational Force A) Is Cut to One Fourth
MULTIPLE CHOICE REVIEW – GRAVITATION (Dynamics Part 3) 1. Two objects attract each other gravitationally. If the distance between their centers is cut in half, the gravitational force A) is cut to one fourth. B) is cut in half. C) doubles. D) quadruples 2. Two objects, with masses m1 and m2, are originally a distance r apart. The magnitude of the gravitational force between them is F. The masses are changed to 2m1 and 2m2, and the distance is changed to 4r. What is the magnitude of the new gravitational force? A) F/16 B) F/4 C) 16F D) 4F 3. As a rocket moves away from the Earth's surface, the rocket's weight A) increases. B) decreases. C) remains the same. D) depends on how fast it is moving. 4. A hypothetical planet has a mass of half that of the Earth and a radius of twice that of the Earth. What is the acceleration due to gravity on the planet in terms of g, the acceleration due to gravity at the Earth? A) g B) g/2 C) g/4 D) g/8 5. Two planets have the same surface gravity, but planet B has twice the mass of planet A. If planet A has radius r, what is the radius of planet B? A) 0.707r B) r C) 1.41r D) 4r 6. A planet is discovered to orbit around a star in the galaxy Andromeda, with the same orbital diameter as the Earth around our Sun. If that star has 4 times the mass of our Sun, what will the period of revolution of that new planet be, compared to the Earth's orbital period? A) one-fourth as much B) one-half as much C) twice as much D) four times as much 7. -
Jupiter Mass
CESAR Science Case Jupiter Mass Calculating a planet’s mass from the motion of its moons Student’s Guide Mass of Jupiter 2 CESAR Science Case Table of Contents The Mass of Jupiter ........................................................................... ¡Error! Marcador no definido. Kepler’s Three Laws ...................................................................................................................................... 4 Activity 1: Properties of the Galilean Moons ................................................................................................. 6 Activity 2: Calculate the period of your favourite moon ................................................................................. 9 Activity 3: Calculate the orbital radius of your favourite moon .................................................................... 12 Activity 4: Calculate the Mass of Jupiter ..................................................................................................... 15 Additional Activity: Predict a Transit ............................................................................................................ 16 To know more… .......................................................................................................................... 19 Links ............................................................................................................................................ 19 Mass of Jupiter 3 CESAR Science Case Background Kepler’s Three Laws The three Kepler’s Laws, published between -
PHYS133 – Lab 4 the Revolution of the Moons of Jupiter
PHYS133 – Lab 4 The Revolution of the Moons of Jupiter Goals: Use a simulated remotely controlled telescope to observe Jupiter and the position of its four largest moons. Plot their positions relative to the planet vs. time and fit a curve to them to determine their orbit characteristics (i.e., period and semi‐major axis). Employ Newton’s form of Kepler’s third law to determine the mass of Jupiter. What You Turn In: Graphs of your orbital data for each moon. Calculations of the mass of Jupiter for each moon’s orbit. Calculate the time required to go to Mars from Earth using the lowest possible energy. Background Reading: Background reading for this lab can be found in your text book (specifically, Chapters 3 and 4 and especially section 4.4) and the notes for the course. Equipment provided by the lab: Computer with Internet Connection • Project CLEA program “The Revolutions of the Moons of Jupiter” Equipment provided by the student: Pen Calculator Background: Astronomers cannot directly measure many of the things they study, such as the masses and distances of the planets and their moons. Nevertheless, we can deduce some properties of celestial bodies from their motions despite the fact that we cannot directly measure them. In 1543, Nicolaus 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, to deduce three empirical mathematical laws governing the orbit of one object around another. -
Arxiv:1209.5996V1 [Astro-Ph.EP] 26 Sep 2012 1.1
, 1{28 Is the Solar System stable ? Jacques Laskar ASD, IMCCE-CNRS UMR8028, Observatoire de Paris, UPMC, 77 avenue Denfert-Rochereau, 75014 Paris, France [email protected] R´esum´e. Since the formulation of the problem by Newton, and during three centuries, astrono- mers and mathematicians have sought to demonstrate the stability of the Solar System. Thanks to the numerical experiments of the last two decades, we know now that the motion of the pla- nets in the Solar System is chaotic, which prohibits any accurate prediction of their trajectories beyond a few tens of millions of years. The recent simulations even show that planetary colli- sions or ejections are possible on a period of less than 5 billion years, before the end of the life of the Sun. 1. Historical introduction 1 Despite the fundamental results of Henri Poincar´eabout the non-integrability of the three-body problem in the late 19th century, the discovery of the non-regularity of the Solar System's motion is very recent. It indeed required the possibility of calculating the trajectories of the planets with a realistic model of the Solar System over very long periods of time, corresponding to the age of the Solar System. This was only made possible in the past few years. Until then, and this for three centuries, the efforts of astronomers and mathematicians were devoted to demonstrate the stability of the Solar System. arXiv:1209.5996v1 [astro-ph.EP] 26 Sep 2012 1.1. Solar System stability The problem of the Solar System stability dates back to Newton's statement concerning the law of gravitation. -
Tidal Tomography to Probe the Moon's Mantle Structure Using
Tidal Tomography to Probe the Moon’s Mantle Structure Using Lunar Surface Gravimetry Kieran A. Carroll1, Harriet Lau2, 1: Gedex Systems Inc., [email protected] 2: Department of Earth and Planetary Sciences, Harvard University, [email protected] Lunar Tides Gravimetry of the Lunar Interior VEGA Instrument through the Moon's PulSE • Gedex has developed a low cost compact space gravimeter instrument , VEGA (Vector (GLIMPSE) Investigation Gravimeter/Accelerometer) Moon • Currently this is the only available gravimeter that is suitable for use in space Earth GLIMPSE Investigation: • Proposed under NASA’s Lunar Surface Instrument and Technology Payloads • ca. 1972 MIT developed a space gravimeter (LSITP) program. instrument for use on the Moon, for Apollo 17. That instrument is long-ago out of • To fly a VEGA instrument to the Moon on a commercial lunar lander, via NASA’s production and obsolete. Commercial Lunar Payload Services (CLPS) program. VEGA under test in thermal- GLIMPSE Objectives: VEGA Space Gravimeter Information vacuum chamber at Gedex • Prove the principle of measuring time-varying lunar surface gravity to probe the lunar • Measures absolute gravity vector, with no • Just as the Moon and the Sun exert tidal forces on the Earth, the Earth exerts tidal deep interior using the Tidal Tomography technique. bias forces on the Moon. • Determine constraints on parameters defining the Lunar mantle structure using time- • Accuracy on the Moon: • Tidal stresses in the Moon are proportional to the gravity gradient tensor field at the varying gravity measurements at a location on the surface of the Moon, over the • Magnitude: Effective noise of 8 micro- Moon’s centre, multiplies by the distance from the Moon’s centre. -
Prelab 4: Revolution of the Moons of Jupiter
Name: Section: Date: Prelab 4: Revolution of the Moons of Jupiter Many of the parameters astronomers study cannot be directly measured; rather, they are inferred from properties or other observations of the bodies themselves. The mass of a celestial object is one such parameter|after all, how would one weigh something suspended in mid-air? In 1543, Nicolaus Copernicus hypothesized that the planets revolve in circular orbits around the sun. His contemporary Tycho Brahe, famous for his observations, carefully charted the locations of the planets and hundreds of stars over a period of twenty years, using a sextant and a compass. These observations were eventually used by Johannes Kepler, a student of Brahe's, to deduce three empirical mathematical laws governing the orbit of one object around another. Kepler's Third Law is the one that applies to this lab. In the early 17th century, with the recent invention of the telescope, Galileo was able to extend astronomical observations beyond what was available to the naked eye. He discovered four moons orbiting Jupiter and made exhaustive studies of this system. Galileo's work is of particular interest, not only for its pioneering observations, but because Jupiter and the four Galilean moons (as they came to be called) can be viewed as a miniature version of the larger Solar System in which they lie. Furthermore, Jupiter provided clear evidence that Copernicus's heliocentric model of the Solar System was physically possible; it is largely from these scientists' work that the modern study of Astronomy was born. The purpose of this lab is to determine the mass of Jupiter by observing the motion of the four Galilean moons: Io, Europa, Ganymede, and Callisto. -
The Jovian System: a Scale Model Middle Grades
The Jovian System: A Scale Model Middle grades Lesson Summary Teaching Time: One 45-minute period This exercise will give students an idea of the size and scale of the Jovian system, and also illustrate Materials the Galileo spacecraft's arrival day trajectory. To share with the whole class: • Materials for scale-model moons (optional, may Prior Knowledge & Skills include play-dough or cardboard) Characteristics of the Jupiter system • • Rope marked with distance units • Discovery of Jupiter’s Galilean satellites • Copy of arrival day geometry figure • The Galileo probe mission AAAS Science Benchmarks Advanced Planning Preparation Time: 30 minutes The Physical Setting 1. Decide whether to use inanimate objects or The Universe students to represent the moons Common Themes 2. If using objects, gather materials Scale 3. Mark off units on rope 4. Review lesson plan NSES Science Standards • Earth and space science: Earth in the Solar System • Science and technology: Understandings about science and technology NCTM Mathematics Standards • Number and Operations: Compute fluently and make reasonable estimates Source: Project Galileo, NASA/JPL The Jovian System: A Scale Model Objectives: This exercise will give students an idea of the size and scale of the Jovian system, and also illustrate the Galileo spacecraft's arrival day trajectory. 1) Set the Stage Before starting your students on this activity, give them at least some background on Jupiter and the Galileo mission: • Jupiter's mass is more than twice that of all the other planets, moons, comets, asteroids and dust in the solar system combined. • Jupiter is looked on as a "mini solar system" because it resembles the solar system in miniature-for example, it has many moons (resembling the Sun's array of planets), and it has a huge magnetosphere, or volume of space where Jupiter's magnetic field pushes away that of the Sun. -
Chapter 3 Projects Test Monday Gravity
Chapter 3 Celestial Sphere Movie Gravity and Motion Projects Test Monday Preview • I moved due-date for Part 1 to 10/21 Ch 1 Ch 2 • I added a descriptive webpage about the Galileo Movie projects. Essay 1: Backyard Astronomy Ch. 3 (just beginning) Northern Hemisphere sky: Big Dipper Little Dipper Cassiopeia Orion Polaris Gravity The Problem of Astronomical Motion • Gravity gives the Universe its structure • Astronomers of antiquity did – It is a universal force that not connect gravity and causes all objects to pull on astronomical motion all other objects • Galileo investigated this everywhere connection with experiments – It holds objects together using projectiles and balls – It is responsible for holding rolling down planks the Earth in its orbit around • He put science on a course to the Sun, the Sun in its orbit determine laws of motion and around the Milky Way, and to develop the scientific the Milky Way in its path method within the Local Group Inertia and Newton’s First Law Inertia • This concept was • Galileo established the idea of inertia incorporated in – A body at rest tends to remain at rest Newton’s First Law – A body in motion tends to remain in motion of Motion: – Through experiments with inclined planes, Galileo demonstrated the idea of inertia and the A body continues in a importance of forces (friction) state of rest or uniform motion in a straight line unless made to change that state by forces acting on it Newton’s First Law Astronomical Motion • As seen earlier, planets • Must there be a force at move along curved work? • Important ideas of (elliptical) paths, or Newton’s First Law – The law implies that if • Yes! an object is not moving orbits. -
The Mass of the Moon Is 1/81 of the Mass of the Earth. Q14.1 Compared to the Gravitational Force That the Earth Exerts on the Mo
Q14.1 The mass of the Moon is 1/81 of the mass of the Earth. Compared to the gravitational force that the Earth exerts on the Moon, the gravitational force that the Moon exerts on the Earth is A. 812 = 6561 times greater. B. 81 times greater . C. equally strong. D1/81D. 1/81 as great. E. (1/81)2 = 1/6561 as great. © 2012 Pearson Education, Inc. A14.1 The mass of the Moon is 1/81 of the mass of the Earth. Compared to the gravitational force that the Earth exerts on the Moon, the gravitational force that the Moon exerts on the Earth is A. 812 = 6561 times greater. B. 81 times greater . C. equally strong. D1/81D. 1/81 as great. E. (1/81)2 = 1/6561 as great. © 2012 Pearson Education, Inc. Q14.2 The planet Saturn has 100 times the mass of the Earth and is 10 times more distant from the Sun than the Earth is. Compared to the Earth’s acceleration as it orbits the Sun, the accelileration of fS Saturn as ibihSiit orbits the Sun is A. 100 times greater. B. 10 times greater . C. the same. D1/10D. 1/10 as great. E. 1/100 as great. © 2012 Pearson Education, Inc. A14.2 The planet Saturn has 100 times the mass of the Earth and is 10 times more distant from the Sun than the Earth is. Compared to the Earth’s acceleration as it orbits the Sun, the accelileration of fS Saturn as ibihSiit orbits the Sun is A. -
A Astronomical Terminology
A Astronomical Terminology A:1 Introduction When we discover a new type of astronomical entity on an optical image of the sky or in a radio-astronomical record, we refer to it as a new object. It need not be a star. It might be a galaxy, a planet, or perhaps a cloud of interstellar matter. The word “object” is convenient because it allows us to discuss the entity before its true character is established. Astronomy seeks to provide an accurate description of all natural objects beyond the Earth’s atmosphere. From time to time the brightness of an object may change, or its color might become altered, or else it might go through some other kind of transition. We then talk about the occurrence of an event. Astrophysics attempts to explain the sequence of events that mark the evolution of astronomical objects. A great variety of different objects populate the Universe. Three of these concern us most immediately in everyday life: the Sun that lights our atmosphere during the day and establishes the moderate temperatures needed for the existence of life, the Earth that forms our habitat, and the Moon that occasionally lights the night sky. Fainter, but far more numerous, are the stars that we can only see after the Sun has set. The objects nearest to us in space comprise the Solar System. They form a grav- itationally bound group orbiting a common center of mass. The Sun is the one star that we can study in great detail and at close range. Ultimately it may reveal pre- cisely what nuclear processes take place in its center and just how a star derives its energy. -
How High Can You Jump on Other Planets?
Student activity How high can you jump on other planets? Background Information Weight and mass are very different even though the words are used interchangeably in the English language. Mass is a measure of the total amount of material or matter that makes up a body and is measured in kg. Weight is a measure of how much force pulls on a body and is measured in Newtons (N). Weight is dependent on mass and acceleration or gravity ‘g’. The mathematical relationship can be described with the following equation: W = m x g (N) ‘g’ varies according to which planet you are standing on. In general, planets with more mass have stronger surface gravity. On the Earth’s surface g = 9.8kg/m/s2 (where m = metres and s = seconds). If your mass is 70kg, then your Weight = 70 x 9.8 = 686 N So your weight can vary according to which planet you are standing on, however your mass stays the same. Students are provided with relative scaling factors for the surface gravity of the Sun, the other planets in our Solar System, Pluto (a dwarf planet) and the Moon. With this information they can calculate and compare the heights of their jumps and the reading that bathroom scales (calibrated on Earth) would have if they were to stand on the different bodies in the Solar System. The stronger the surface gravity, the more they are pulled by the planet, moon or star so it would make it more difficult for them to jump. Object Surface Gravity (ms-2) Surface Gravity relative to Earth Earth 9.8 1 Sun 273.42 27.9 Mercury 3.72 0.38 Venus 8.92 0.91 Mars 3.72 0.38 Jupiter 23.13 2.36 Saturn 9.02 0.92 Uranus 8.72 0.89 Neptune 10.98 1.12 Pluto (dwarf planet) 0.59 0.06 The Moon 1.63 0.16 Worksheet http://museumvictoria.com.au/scienceworks/education/ 1 Student activity How high can you jump on other planets? Worksheet Introduction The larger the mass of the planet, moon or star, the more it would pull on you and the harder it would be to jump.