Similar documents
Section 4. Newton s Law of Universal Gravitation: The Ups and Downs of a Roller Coaster. What Do You See?

Physics Unit 7: Circular Motion, Universal Gravitation, and Satellite Orbits. Planetary Motion

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

Observational Astronomy - Lecture 4 Orbits, Motions, Kepler s and Newton s Laws

PHYSICS. Chapter 13 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.

The Acceleration of Gravity (g)

6. Summarize Newton s Law of gravity and the inverse square concept. Write out the equation

October 19, NOTES Solar System Data Table.notebook. Which page in the ESRT???? million km million. average.

Physics 12. Unit 5 Circular Motion and Gravitation Part 2

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

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

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

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

Gravity and the Orbits of Planets

Chapter 12 Gravity. Copyright 2010 Pearson Education, Inc.

Lecture 13. Gravity in the Solar System

Early Theories. Early astronomers believed that the sun, planets and stars orbited Earth (geocentric model) Developed by Aristotle

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

7.4 Universal Gravitation

Learning Objectives. one night? Over the course of several nights? How do true motion and retrograde motion differ?

Pedagogical information

PHYS 155 Introductory Astronomy

CHAPTER 7 GRAVITATION

Yes, inner planets tend to be and outer planets tend to be.

Unit: Planetary Science

Physics Test 7: Circular Motion page 1

Planetary Mechanics:

KEPLER S LAWS OF PLANETARY MOTION

Chapter 12 Gravity. Copyright 2010 Pearson Education, Inc.

Physics Mechanics. Lecture 29 Gravitation

Chapter 14 Satellite Motion

Section 37 Kepler's Rules

7 Study Guide. Gravitation Vocabulary Review

Announcements 15 Oct 2013

Planetary Orbits: Kepler s Laws 1/18/07

By; Jarrick Serdar, Michael Broberg, Trevor Grey, Cameron Kearl, Claire DeCoste, and Kristian Fors

Occam s Razor: William of Occam, 1340(!)

AP Physics-B Universal Gravitation Introduction: Kepler s Laws of Planetary Motion: Newton s Law of Universal Gravitation: Performance Objectives:

Circular Motion and Gravitation. Centripetal Acceleration

CH 8. Universal Gravitation Planetary and Satellite Motion

VISUAL PHYSICS ONLINE

Gravitation. Luis Anchordoqui

Outline for Today: Newton s Law of Universal Gravitation The Gravitational Field Orbital Motion Gravitational Potential Energy. Hello!

January 19, notes.notebook. Claudius Ptolemaeus Second Century AD. Jan 5 7:37 AM

Unit 3 Lesson 2 Gravity and the Solar System. Copyright Houghton Mifflin Harcourt Publishing Company

Patterns in the Solar System (Chapter 18)

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

Practice Test DeAnza College Astronomy 04 Test 1 Spring Quarter 2009

Chapter 5 Centripetal Force and Gravity. Copyright 2010 Pearson Education, Inc.

Astronomy- The Original Science

Copyright 2010 Pearson Education, Inc. GRAVITY. Chapter 12

Kepler, Newton, and laws of motion

Patterns in the Solar System (Chapter 18)

Claudius Ptolemaeus Second Century AD. Jan 5 7:37 AM

AST 105. Introduction to Astronomy: The Solar System. Announcement: First Midterm this Thursday 02/25

Notes: The Solar System

Announcements. Topics To Be Covered in this Lecture

Circular Motion. Gravitation

In so many and such important. ways, then, do the planets bear witness to the earth's mobility. Nicholas Copernicus

21/11/ /11/2017 Space Physics AQA Physics topic 8

cosmogony geocentric heliocentric How the Greeks modeled the heavens

Chapter 8 - Gravity Tuesday, March 24 th

Question number Answer Notes Marks 1 correctly; (ii) Sun X should be left of the imaginary 5-7 line, reject X placed outside the orbit

Gravitation and Newton s Synthesis

towards the modern view

Gravitation and the Motion of the Planets

Satellites and Kepler's Laws: An Argument for Simplicity

Outline for Today: Newton s Law of Universal Gravitation The Gravitational Field Orbital Motion Gravitational Potential Energy

Evidence that the Earth does not move: Greek Astronomy. Aristotelian Cosmology: Motions of the Planets. Ptolemy s Geocentric Model 2-1

CIRCULAR MOTION AND UNIVERSAL GRAVITATION

Gravitation. Makes the World Go Round

Astronomy A BEGINNER S GUIDE TO THE UNIVERSE EIGHTH EDITION

5. How did Copernicus s model solve the problem of some planets moving backwards?

NAME: PERIOD: DATE: LAB PARTNERS: LAB #39 ECCENTRICITY OF PLANETARY ORBITS

Chapter 5 Review : Circular Motion; Gravitation

Astronomy 104: Stellar Astronomy

Name Class Date. Chapter 23 Touring Our Solar System Investigation 23

Gravitation and the Waltz of the Planets

Gravitation and the Waltz of the Planets. Chapter Four

Copernican Revolution. ~1500 to ~1700

Motion in the Heavens

Circular Motion and Gravitation. Centripetal Acceleration

4π 2 G(M1+M2 ) p2 = Newton s 3 Laws of Motion AST 105. Introduction to Astronomy: The Solar System. Newton's Version of Kepler's Third Law

Days of the week: - named after 7 Power (moving) objects in the sky (Sun, Moon, 5 planets) Models of the Universe:

Ast ch 4-5 practice Test Multiple Choice

Gravitation & Kepler s Laws

Lecture #5: Plan. The Beginnings of Modern Astronomy Kepler s Laws Galileo

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

Name Period Date Earth and Space Science. Solar System Review

Astronomy Lesson 8.1 Astronomy s Movers and Shakers

Kepler's Laws and Newton's Laws

Gravity and the Laws of Motion

Astronomy Notes Chapter 02.notebook April 11, 2014 Pythagoras Aristotle geocentric retrograde motion epicycles deferents Aristarchus, heliocentric

Tycho Brahe

Introduction to Astronomy

4 A(n) is a small, rocky object that orbits the sun; many of these objects are located in a band between the orbits of Mars and Jupiter.

Circular Motion and Gravitation Notes 1 Centripetal Acceleration and Force

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

Test Bank for Life in the Universe, Third Edition Chapter 2: The Science of Life in the Universe

ASTR 150. Planetarium Shows begin Sept 9th. Register your iclicker! Last time: The Night Sky Today: Motion and Gravity. Info on course website

Transcription:

Chapter 4 Thrills and Chills +Math +Depth Acceleration of the Moon +Concepts The Moon is 60 times further away from the center of Earth than objects on the surface of Earth, and moves about Earth in an approximately circular path. 1. If the acceleration due to gravity on the surface of Earth is 9.8 m/s 2, use the inverse square relationship and your calculator to determine the acceleration due to gravity at the Moon s distance. Since the Moon orbits Earth, you can calculate its acceleration. The equation for acceleration of any object moving in a circle at constant speed is a = 2 v r where v is the speed r is the distance (radius) of the object from the center The Moon s distance is 60 times the radius of Earth (60 6.4 10 6 m = 3.84 10 8 m). The Moon travels once about Earth in 28.25 days. 2. Find the speed of the Moon using the equation v = d/t where d is the circumference of the Moon s orbit (2π r). 3. Calculate the acceleration of the Moon. 4. Compare the acceleration of the Moon using these two different approaches. (When Newton made this comparison, he was confident that his inverse square law of gravity was correct.) +Exploration Kepler s Laws Newton once stated, If I have seen further than others, it is because I have stood on the shoulders of giants. Tycho Brahe and Johannes Kepler were two of those giants. Tycho Brahe observed and recorded the positions of the planets every night over many years. Kepler viewed the data and tried for years to form mathematical relationships that could explain all of Brahe s data. At first, it appeared that the planet s data could be adequately described by stating that the planets moved in circles about the Sun. This description was only approximately true. Kepler had to decide if Brahe s data was a bit imprecise or whether the circular path was incorrect. Kepler s confidence in Brahe s observations forced him to keep trying other descriptions of the paths. Kepler eventually did find three mathematical relationships that fit the data very well. These are now known as Kepler s laws. Kepler s first law: The planets travel in ellipses about the Sun. An ellipse is a mathematical shape that is defined by two foci. The Sun is at one focus. There is nothing at the other focus. Sun x Active Physics Plus planet foci x Active Physics 388

Section 4 The Ups and Downs of a Roller Coaster Kepler s second law: The planets sweep out equal areas in equal times. Imagine a pizza in the shape of an ellipse. Slices of pizza are cut from one of the foci. Each slice of pizza has the same area. The planets would travel along the edge of the ellipse. The time needed to travel along the edge of each slice of pizza would be identical. Since the edge of the pizza represents the path of the planet around the Sun, this means that the planet travels faster when it is near the Sun and slower when it is further from the Sun. Sun equal areas in equal times Kepler s third law: There is a mathematical relationship that defines the time it takes for a planet to complete an orbit about the Sun and the average distance of the planet from the Sun. 2 T 3 R = a constant where T is the time to complete one orbit and R is the average distance from the Sun. The quantity T 2 3 R is identical for all planets orbiting the Sun. Kepler found this equation from the experimental data of Brahe. Newton derived the same equation from his assertion that the Sun and each planet have an attractive gravitational force. Gm m F = 1 2 G 2 r 1. Earth travels about the Sun in 1 year. The average distance of Earth from the Sun is 1.50 10 11 m. Convert the 1 year to seconds and find the value of T 2 for Earth. 3 R Defining Earth s average distance from the Sun as 1 AU (astronomical unit), all other planets average distance and period can be defined in terms of Earth. 2. Show that Kepler s value T 3 is R identical for all planets, using the table below. A spreadsheet program will allow you to make these calculations in very little time. 2 Mean distance from the Sun (AU) Sidereal period of orbit (years) Mercury Venus Earth Mars Jupiter Saturn Uranus Neptune 0.3871 0.7233 1 1.524 5.203 9.539 19.19 30.06 0.24 0.62 1 1.88 11.86 29.46 84.01 164.79 What Do You Think Now? At the beginning of this section, you were asked the following: Does gravity have a direction? How can people in Australia be held on Earth when they are upside down? Now that you have completed this section, how would you revise your answers to these questions? 389 Active Physics

Chapter 4 Thrills and Chills Physics Essential Questions What does it mean? Newton s law of gravitation says that all massive objects attract each other with a force that decreases with the square of the distance between them. How does the Gm m equation F = 1 2 also communicate this relationship? G 2 r How do you know? You observe the force of gravity when a penny is dropped. Earth attracts the penny. How did Cavendish demonstrate that two objects attract each other? Why do you believe? Connects with Other Physics Content Fits with Big Ideas in Science Meets Physics Requirements Forces and motion Models Good, clear explanation, no more complex than necessary Newton s law of gravitation states that Earth attracts the Moon in the same way that Earth attracts an apple. Why do you believe that the physics laws on Earth work equally well for the objects outside of Earth? Why should you care? As you design your roller coaster on Earth, you may also wonder would the roller coaster behave identically on the Moon? What changes would you expect if your roller coaster was on the Moon where the acceleration due to gravity is only 1 6 that on Earth? Reflecting on the Section and the Challenge In this section, you mapped the gravitational field by using data of the acceleration of objects falling at specific locations. Patterns help you understand the world around you, such as Newton s law of universal gravitation, with its inverse square relationship. With this concept, you have a reason for the flights of projectiles and the elliptical orbits of satellites. You have both a field model Gm m and a mathematical model, F = 1 2 G. Both can be and have been tested 2 r experimentally, and they both are successful. Gravity is required for any roller-coaster ride. The acceleration due to gravity at Earth s surface is 9.8 m/s every second or 9.8 m/s 2. This will not only determine the speed at different parts of the coaster ride, but will also have an impact on your apparent weight during the roller-coaster ride. Physics to Go 1. The gravitational force between two asteroids is 500 N. What would the force be if the distance between them doubled? Active Physics 390