Astron 104 Laboratory #4 Gravity and Orbital Motion

Similar documents
Name. Satellite Motion Lab

General Physics 1 Lab - PHY 2048L Lab 2: Projectile Motion / Solar System Physics Motion PhET Lab Date. Part 1: Projectile Motion

Kepler, Newton, and laws of motion

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

Circular Orbits for m << M; a planet and Star

PHYS 106 Fall 2151 Homework 3 Due: Thursday, 8 Oct 2015

Gravity Investigation

1. Which of the following correctly lists our cosmic address from small to large?

Kepler's Laws and Newton's Laws

Gravity and Orbits Activity Page 1. Name: Grade: Gravity and Orbits. Pre-lab. 1. In the picture below, draw how you think Earth moves.

Gravity and Orbits. 1. Choose the picture you think shows the gravity forces on the Earth and the Sun.

Unit: Planetary Science

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

Where do objects get their energy?

LESSON 1. Solar System

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

What is the solar system?

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

Chapter 13: universal gravitation

MOTION IN THE SOLAR SYSTEM ENGAGE, EXPLORE, EXPLAIN

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

Newton s Law of Universal Gravitation

Homeroom: OBJECTIVES: By the end of today s lesson, you will be able to. SWBAT explain how the gravity of the moon causes tides in Earth s oceans.

Astro Lecture 12. Energy and Gravity (Cont d) 13/02/09 Habbal Astro Lecture 12 1

Gravity Well Demo - 1 of 9. Gravity Well Demo

Chapter 5 Newton s Universe

AST101: Our Corner of the Universe Lab 4: Planetary Orbits

December 04, Monday Gravitational force.notebook. Gravitational Force. Return to Table of Contents.

Thursday is last Planetarium observing. Nighttime observing starts next week.

End-of-Chapter Exercises

Chapter 13. Gravitation. PowerPoint Lectures for University Physics, 14th Edition Hugh D. Young and Roger A. Freedman Lectures by Jason Harlow

GraspIT Questions AQA GCSE Physics Space physics

Gravitation. Objectives. The apple and the Moon. Equations 6/2/14. Describe the historical development of the concepts of gravitational force.

Lab 6: The Planets and Kepler

GRAVITY IS AN ATTRACTIVE FORCE

Lecture 13. Gravity in the Solar System

u Today I will look for key ideas in the text to support the role gravity has on the formation of the planets.


Lab 4. Habitable Worlds: Where Should NASA Send a Probe to Look for Life?

The Doppler Effect is the change in frequency observed when a source of sound waves is moving relative to an observer.

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

Today. life the university & everything. Reminders: Review Wed & Fri Eyes to the web Final Exam Tues May 3 Check in on accomodations

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

Chapter 13. Universal Gravitation

Physics 12. Unit 5 Circular Motion and Gravitation Part 2

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

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

2010 Pearson Education, Inc. Chapter 4 Making Sense of the Universe: Understanding Motion, Energy, and Gravity

Please turn on your clickers

Inquiry 6.1 Gravity s effect on objects in motion

Gravitation and the Waltz of the Planets

Gravitation and the Waltz of the Planets. Chapter Four

Gravitation & Kepler s Laws

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

Gravity. Gravity and Newton. What really happened? The history of Gravity 3/9/15. Sir Isaac Newton theorized the Law of Gravitation in 1687

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

Gravitation and the Motion of the Planets

Astron 104 Laboratory #4 Orbital Motion of a Planet

ASTRO 1050 LAB #3: Planetary Orbits and Kepler s Laws

Chapter 4. Motion and gravity

Chapter 8 - Gravity Tuesday, March 24 th

Motion, Energy, and Gravity. Reminder to take out your clicker and turn it on!

Quest Chapter 12. What things did Newton bring together and what did he toss? Read the text or check your notes. How does the moon move?

UNIT 12B Continuous Time Simulations. Announcements

Astronomy A BEGINNER S GUIDE TO THE UNIVERSE EIGHTH EDITION

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

Physics 10 Summer Midterm #1: You Are a Dog. Name:

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

The Hertzprung-Russell Diagram. The Hertzprung-Russell Diagram. Question

ASTRO Fall 2012 LAB #6: Extrasolar Planets

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

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

Section 2: Friction, Gravity, and Elastic Forces

Describing Motion. Newton Newton s Laws of Motion. Position Velocity. Acceleration. Key Concepts: Lecture 9

Newton s Laws of Motion. Newton s Second Law

Chapter 13. Gravitation

Isaac Newton & Gravity

Making Sense of the Universe (Chapter 4) Why does the Earth go around the Sun? Part, but not all, of Chapter 4

More examples: Summary of previous lecture

4.3 Conservation Laws in Astronomy

Newton s Laws of Motion

= v = 2πr. = mv2 r. = v2 r. F g. a c. F c. Text: Chapter 12 Chapter 13. Chapter 13. Think and Explain: Think and Solve:

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

Lecture 16. Gravitation

Newton s Wagon. Materials. friends rocks wagon balloon fishing line tape stopwatch measuring tape. Lab Time Part 1

KNOWLEDGE TO GET FROM TODAY S CLASS MEETING

Answer Key for Exam C

Answer Key for Exam B

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

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

12/1/2014. Chapter 5 Circular Motion; Gravitation. Contents of Chapter 5. Contents of Chapter Kinematics of Uniform Circular Motion

Answer Key for Exam D

Chapter 16 Dark Matter, Dark Energy, & The Fate of the Universe

Is there life outside of Earth? Activity 2: Moving Stars and Their Planets

Astronomy- The Original Science

Unit 16: Astronomy and space science. Learning aim A Understand the fundamental aspects of the solar system

Chapter 5 Circular Motion; Gravitation

Newton s Laws of Motion

Our Place in the Universe

How does the solar system, the galaxy, and the universe fit into our understanding of the cosmos?

Transcription:

Name: Date: Section: Astron 104 Laboratory #4 Gravity and Orbital Motion Section 5.5, 5.6 Introduction No astronomical object can stand still gravity makes certain of this. Newton s Law of Universal Gravitation tells us that any two bodies attract each other by their mutual gravitational force. Every object in the Universe moves in response to the pull of gravity: moons orbit planets, planets and comets orbit stars, stars follow orbits through their galaxy, galaxies orbit each other in giant galaxy clusters. In this lab, you will use a gravity simulator to investigate orbital motion and Kepler s Laws. Learning Objectives At the completion of this lab, you should be able to: 1. Explain what we mean by down in terms of gravity 2. Describe the role of mass in gravitational acceleration 3. Describe the variations in orbital speed with position in the orbit 4. Describe the patter of orbital speed with semimajor axis length 5. Construct a plot comparing speed and semimajor axis for an orbit Gravity [30 pts total] Open the PhET My Solar System program 1 and verify that the following boxes are checked: System Centered 1 Available at http://phet.colorado.edu/sims/my-solar-system/my-solar-system_en.html. Astron 104 Fall 2015 1

Show Traces Show Grid Set the slider to the middle (between Accurate and Fast). Set the number of bodies to 2. Set the masses to for Body 1 and 1 for Body 2. Place Body 1 at (x, y) = (0, 0) and Body 2 at (, 0). Now we re ready to test it out! 1. What do you predict will happen if we just release Body 2 from rest (set all velocities to 0 in both x and y directions? [5 pts] 2. Test your prediction by setting the velocities to 0 for both Bodies and pressing Start. Briefly describe the motions of the Bodies. [5 pts] 3. Reset the mass of Body 1 to 20 and repeat the experiment. Try it again with the mass of Body 1 set to 2. Describe the motions of the two bodies in these tests. Do both objects move? Do they move the same amount? [5 pts] 4. Compare these three tests. As you change the mass of Body 1, what changes about the motion of the two bodies? Does the strength of the gravitational attraction between the bodies depend on their masses? [5 pts] 5. Predict what would happen if you repeat the experiment, but increase the mass of Body 2 while leaving Body 1 at. Test your prediction! [5 pts] Astron 104 Fall 2015 2

6. If you think about it, you have performed this experiment in real life: releasing a small object (a ball, for example) at rest near a large object (Earth!). Usually we call this dropping something. Set Body 1 at mass 0 (Earth), Body 2 at mass 0.01 (ball) and 0 velocity for both. You can use the mouse to drag the ball around the grid. Try a few experiments placing the ball at different locations and release it by pressing Start. Based on your experiments, what direction does a ball fall if we drop it? (In other words, how does gravity influence what we mean by down? ) [5 pts] Orbiting [30 pts total] We could imagine a scenario where the two bodies are a star and a planet. Typically, the mass of the star s much larger, so let s use for the star and 1 for the planet. Let s start with the star at (x, y) = (0, 0) and the planet at (, 0). 1. Clearly from your earlier experiments, a motionless planet will fall toward a star. What if the planet is in motion: will it still fall? Try adding a positive velocity in the x direction, say units, and press Start. Describe the resulting motion of the planet. [5 pts] 2. Will adding enough velocity in the x direction eventually make the planet simply leave? Try it, and describe what happens. [5 pts] 3. The other way to avoid falling into a star is orbiting the star. Set the planet s x velocity to 0 and the y velocity to 10. What happens? [5 pts] Astron 104 Fall 2015 3

4. Increase the y velocity, multiplying by two each time, until the planet misses the star. Now you have an orbit! What is the minimum y velocity you need? Describe the shape of the orbit. [5 pts] 5. Now, keep increasing the y velocity until the planet follows a circular orbit (you can tell from the grid: the planet should pass through the the point (, 0) on the other side of the star). What y velocity gives a circular orbit? [10 pts] Orbit Speed: Kepler s Third Law [60 pts total] 1. Set the (x, y) position back to (, 0) and set the y velocity for a circular orbit. Record the values you found in the table below. The period of the orbit is the time required to complete one lap. Measure the period of the orbit using the timer in the program. You can get good precision by counting out several orbits (5 10) and noting the total time required. Then divide the total time by the number of orbits to get the period of one orbit. Record the value in the table. Repeat these steps for the other x positions in the table. For the positions between the grid lines, use the Tape Measure feature in the program to make sure your orbits are circular. [20 pts] x position y velocity of circular orbit Period of circular orbit Astron 104 Fall 2015 4

2. Now, plot the velocity against hte distance from the star for your orbits: 300 Velocity 0 0 300 Distance Connect the points with a line and describe the relationship between distance from the star and the planet s speed in a circular orbit. [10 pts] 3. Use your plot to predict the velocity required for a circular orbit at x = 125. Test your prediction: did you get it right? [5 pts] 4. Kepler s Third Law tells us that for orbital motion, the period squared is proportional to the semimajor axis cubed: P 2 a 3. In other words, P 2 = Ka 3 where K is some constant. For a circular orbit, the semimajor axis a is equal to the distance to the star. Use the table below to record your values [10 pts]: Astron 104 Fall 2015 5

x position (Semimajor axis) 3 (Period) 2 5. The general equation for a straight line is y = Kx + b. Make substitutions to show that Kepler s Third Law has the form of the equation of a straight line. What is y? What is x? [5 pts] 6. Kepler s Third Law predicts that a plot of P 2 versus a 3 should lead to data points that all fall along a straight line. You can test this prediction using your data from My Solar System. Astron 104 Fall 2015 6

Plot your (period) 2 and (semimajor axis) 3 on the plot below: 400 3 300 Period Squared 0 0 5 10 15 20 25 30 Semimajor Axis Cubed (millions) Based on your plot, does Kepler s Third Law corectly predict the orbital motions in your data? How can you tell? [10 pts] Astron 104 Fall 2015 7