PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL 2014-2015 DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 15 1 How much.

Slides:



Advertisements
Similar presentations
ConcepTest 12.1a Earth and Moon I
Advertisements

The Beginning of Modern Astronomy
PHYS-1700/2100PHYS-1700/2100 I6 CapacitanceNEBRASKA WESLEYAN UNIVERSITYSPRING DEAN SIEGLAFF NATHANIEL CUNNINGHAM BOB FAIRCHILD of 9 1 [Insert.
PHYS-1700/2100PHYS-1700/2100 II5 Analyzing Resistor NetworksNEBRASKA WESLEYAN UNIVERSITYSPRING DEAN SIEGLAFF NATHANIEL CUNNINGHAM BOB FAIRCHILD.
PHYS-1600/2000PHYS-1600/2000 I5 Position VectorNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 14 1 Today’s Physics Puzzler:
PHYS-1600/2000PHYS-1600/2000 I2 Graphing Constant Velocity MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 14 1.
PHYS-1600/2000PHYS-1600/2000 IV6 Angular Energy and MomentumNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 18 1 Puzzler:
PHYS-1600/2000PHYS-1600/2000 III1 Work and EnergyNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 18 1 Puzzler: A monkey.
PHYS-1600/2000PHYS-1600/2000 II2 Free Body AnalysisNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 12 1 Today’s Puzzler:
PHYS-1600/2000PHYS-1600/2000 I3 AccelerationNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 14 1 Today’s Puzzler: Two.
ConcepTest Clicker Questions
Physics: Principles with Applications, 6th edition
“ If I have seen farther than others, it is because I have stood on the shoulders of giants.” Sir Isaac Newton (1642 – 1727) Physicist.
PHYS-1700/2100PHYS-1700/2100 II1 EMF and Electrical CurrentNEBRASKA WESLEYAN UNIVERSITYSPRING DEAN SIEGLAFF NATHANIEL CUNNINGHAM BOB FAIRCHILD.
Circular motion and Gravitation Chapter 6 1Physics Chapter 6.
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
Chapter 13 Gravitation.
Chapter 12.
Chapter 7 Tangential Speed
Satellites What keeps them in orbit?. Satellites A satellite is any projectile given a large enough velocity so its path follows the curvature of the.
PHYS-1600/2000PHYS-1600/2000 I7 Motion of a ProjectileNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 14 1 Today’s Puzzler:
PHYS-1600/2000PHYS-1600/2000 II5 Internal ForcesNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 11 1 [Insert Puzzler Here]
Earth and Moon I 1) the Earth pulls harder on the Moon
PHYS-1600/2000PHYS-1600/2000 I6 Curved Path MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 14 1 Today’s Puzzler:
Newton’s Law of Gravitation. Newton concluded that gravity was a force that acts through even great distances Newton did calculations on the a r of the.
Gravity. Newton’s Law of Universal Gravitation Newton’s insight: The force accelerating an apple downward is the same force that keeps the Moon in its.
What keeps them in orbit?
Kepler’s first law of planetary motion says that the paths of the planets are A. Parabolas B. Hyperbolas C. Ellipses D. Circles Ans: C.
Circular Motion.
Physics Unit Four Forces that Affect Motion. Force A push or a pull. Measured in newtons with a spring scale. 1 newton (N) = 1 kg m/s 2 An apple weighs.
Bellringer/11.2 Notes Recall that weight is defined as a measure of the gravitational force exerted on an object. Use knowledge you have about gravity.
A Brief History of Classical Physics (Natural Philosophy) Ms. DiVincenzo December, 2006.
Chapter 7 Rotational Motion and the Law of Gravity
PHYS-1600/2000PHYS-1600/2000 IV2 Angular and Linear VariablesNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 11 1 [Insert.
Chapter 5 Circular Motion; Gravitation. 1. Use Newton's second law of motion, the universal law of gravitation, and the concept of centripetal acceleration.
PHYS-1700/2100PHYS-1700/2100 II8 The RC Series CircuitNEBRASKA WESLEYAN UNIVERSITYSPRING DEAN SIEGLAFF NATHANIEL CUNNINGHAM BOB FAIRCHILD of.
PHYS-1600/2000PHYS-1600/2000 IV1 Angular Velocity and AccelerationNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 11 1.
PHYS-1600/2000PHYS-1600/2000 I1 Velocity and SpeedNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 14 1 Today’s physics.
Law of universal Gravitation Section The force of gravity: All objects accelerate towards the earth. Thus the earth exerts a force on these.
PHYS-1700/2100PHYS-1700/2100 II3 Resistivity and ResistanceNEBRASKA WESLEYAN UNIVERSITYSPRING DEAN SIEGLAFF NATHANIEL CUNNINGHAM BOB FAIRCHILD.
PHYS-1700/2100PHYS-1700/2100 III5 Ampere’s LawNEBRASKA WESLEYAN UNIVERSITYSPRING DEAN SIEGLAFF NATHANIEL CUNNINGHAM BOB FAIRCHILD of 9 1 [Insert.
Proportionality between the velocity V and radius r
 This version has no answers.. Which is stronger, Earth’s pull on the Moon, or the Moon’s pull on Earth? 1) the Earth pulls harder on the Moon 2) the.
Unit 1 Lesson 4 Gravity and Motion. Down to Earth Copyright © Houghton Mifflin Harcourt Publishing Company What is gravity? Gravity is a noncontact force.
The First Two Laws of Motion
Sir Isaac Newton (1642 – 1727) Physicist
Q12.1 The mass of the Moon is 1/81 of the mass of the Earth.
C H A P T E R 5 Dynamics of Uniform Circular Motion.
Circular Orbits and Weightlessness © 2015 Pearson Education, Inc.
Lecture 4 Force and Motion Gravitation Chapter 2.7  2.15 Outline Laws of Motion Mass and Weight Gravitation The law of gravity – 1666, 3 laws of motion.
Newton’s Second Law Pages Describe your acceleration if you are in a circular motion. What is the net force of your motion? You are constantly.
Gravity Chapter Gravity Law of Universal Gravitation- all objects in the universe attract each other through gravitational force Law of Universal.
PHYSICS 103: Lecture 11 Circular Motion (continued) Gravity and orbital motion Example Problems Agenda for Today:
Law of Gravitation. Law of Gravity  Gravitational Force  All objects have mass and therefore will attract all other objects.  The size of the gravitational.
Section 2Forces Section 2: Gravity Preview Key Ideas Bellringer Weight and Mass Law of Universal Gravitation Free Fall Projectile Motion.
A satellite orbits the earth with constant speed at height above the surface equal to the earth’s radius. The magnitude of the satellite’s acceleration.
FgFg agag mg g W Do you know the difference?? Newton’s Law of Universal Gravitation Every body in the universe attracts every other body with a force.
Circular Motion and the Law of Universal Gravitation.
SACE Stage 2 Physics Circular Motion.
Section 2Forces EQ: 〉 What is the relationship between free-fall acceleration and mass?
Satellites and “Weightlessness”
Clicker Questions ConcepTests Chapter 12 Physics, 3rd Edition
Newton’s Second Law Force equals mass times acceleration. F = ma.
A New Vision of the Cosmos
Unit 1 Lesson 4 Gravity and Motion
ConcepTest Clicker Questions Chapter 6
Solution... Click for answers.
Section 2: Gravity Preview Key Ideas Bellringer Weight and Mass
Section 2: Gravity Preview Key Ideas Bellringer Weight and Mass
Section 2: Gravity Preview Key Ideas Bellringer Weight and Mass
Presentation transcript:

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 15 1 How much less do you weigh at the earth's equator than if you were standing at the north or south pole? Assume a spherical earth with radius R = 6400 km, and one rotation per day. Enter your answer as a decimal, a fraction of your weight at the north pole, to 3 places after the decimal. For example, if your weight would be 150 lbs at the pole but 135 lbs at the equator, your answer would be 135/150 = 0.900

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 15 2 ANNOUNCEMENTS

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of of 3 Satellite A moves in a circular orbit of radius R. Satellite B moves in a circular orbit of radius 2R. The magnitude of the gravity force acting upon B is 1.Four times that acting upon A. 2.Twice that acting upon A. 3.Equal to that acting upon A. 4.Half that acting upon A. 5.One-quarter that acting upon A. Earth A B

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of of 3 Satellite A moves in a circular orbit of radius R. Satellite B moves in a circular orbit of radius 2R. The speed of B is 1.Twice that of A. 2.Less than twice that of A, but greater than that of A. 3.Equal to that of A. 4.Less than that of A, but more than half that of A. 5.Half that of A. Earth A B

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of of 3 Consider an astronaut aboard the International Space Station. The astronaut weighs: 1.The same as on Earth. 2.Somewhat greater than on Earth. 3.Somewhat less than on Earth (but greater than zero Newtons). 4.Zero Newtons. Name:Anousheh Ansari Nationality:Iranian Born:1966 Mission:Soyuz TMA-9/ISS, 20 Sep 2006 Notes:1 st Iranian in space 4 th self-funded space participant B.S. Engineering, George Mason U. M.S. Engineering, George Wash. U. Created, sold telecom company for $550 million US.

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 15 6 ANNOUNCEMENTS Track ISS at Track satellites at

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 15 M m R R is the distance between centers of gravity 7

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 15 FgFg Newton’s Universal Law of Gravity obeys Newton’s Third Law of Motion 8

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 15 FgFg Newton’s Universal Law of Gravity obeys Newton’s Third Law of Motion 9

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of 15 FgFg path of motion Circular Orbit Equation v 10

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of II7 Exit Homework Problem #1

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of II7 Exit Homework Problem #2

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of of 3 Satellite A moves in a circular orbit of radius R. Satellite B moves in a circular orbit of radius 2R. The magnitude of the gravity force acting upon B is 1.Four times that acting upon A. 2.Twice that acting upon A. 3.Equal to that acting upon A. 4.Half that acting upon A. 5.One-quarter that acting upon A. Earth A B

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of of 3 Satellite A moves in a circular orbit of radius R. Satellite B moves in a circular orbit of radius 2R. The speed of B is 1.Twice that of A. 2.Less than twice that of A, but greater than that of A. 3.Equal to that of A. 4.Less than that of A, but more than half that of A. 5.Half that of A. Earth A B

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of of 3 Consider an astronaut aboard the International Space Station. The astronaut weighs: 1.The same as on Earth. 2.Somewhat greater than on Earth. 3.Somewhat less than on Earth (but greater than zero Newtons). 4.Zero Newtons. Name:Anousheh Ansari Nationality:Iranian Born:1966 Mission:Soyuz TMA-9/ISS, 20 Sep 2006 Notes:1 st Iranian in space 4 th self-funded space participant B.S. Engineering, George Mason U. M.S. Engineering, George Wash. U. Created, sold telecom company for $550 million US.

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of PROJECTION SCREEN II7: HAND IN TODAY’S ACTIVITIES SHEETS 6666

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of rotating space station FNFN t y 0 FNFN Path through space-time Albert Einstein taught us that this… …is equivalent to (physically indistinguishable from) this Einstein’s Principle of Equivalence Adapted from Lewis Carroll Epstein’s Relativity Visualized, Insight Press

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of Two Ideas About Gravitation Isaac NewtonAlbert Einstein I am stationary in three dimensions of space and I am not accelerating. mg FNFN t y 0 FNFN I am stationary in three dimensions of space but moving through time (the fourth dimension). Gravitation is a curvature of space-time. Therefore I am following a curved path in four dimensional space, and I am accelerating. Path through space-time Adapted from Lewis Carroll Epstein’s Relativity Visualized, Insight Press

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of Freefall Isaac NewtonAlbert Einstein My position coordinate is changing non-uniformly. I am not obeying my First Law of Motion. I am accelerating. mg t y 0 I am moving uniformly in a straight line through space-time. I am obeying Newton’s First Law of Motion. No force is acting upon me. I am not accelerating. Path through space-time a = g Adapted from Lewis Carroll Epstein’s Relativity Visualized, Insight Press

PHYS-1600/2000PHYS-1600/2000 II7 Gravity and Orbital MotionNEBRASKA WESLEYAN UNIVERSITYFALL DEAN SIEGLAFF NATHANIEL CUNNINGHAM of Tossing a Clock Up in the Air and the Speeding Up of Time t y 0 Clock A’s path Clock B’s path Clock B ends up advanced in time! Adapted from Lewis Carroll Epstein’s Relativity Visualized, Insight Press