PHYSICS 197 Section 1 Chapter N11 Kepler’s Laws

Slides:



Advertisements
Similar presentations
The Beginning of Modern Astronomy
Advertisements

Chapter 9 & 10 Gravity Pythagoras (550 BC) n Claimed that natural phenomena could be described by mathematics.
Gravitation Newton’s Law of Gravitation Superposition Gravitation Near the Surface of Earth Gravitation Inside the Earth Gravitational Potential Energy.
Taking cube roots on a simple “scientific” calculator y x or using shift x  y 27 y x = or 27 shift x  y 3 = 3.
Ch12-1 Newton’s Law of Universal Gravitation Chapter 12: Gravity F g = Gm 1 m 2 /r 2 G = 6.67 x Nm 2 /kg 2.
Kepler’s Laws of Planetary Motion Newton’s Laws of Gravity
Physics 218 Lecture 21 Dr. David Toback Physics 218, Lecture XXI.
NJIT Physics 320: Astronomy and Astrophysics – Lecture II Carsten Denker Physics Department Center for Solar–Terrestrial Research.
Physics 202: Introduction to Astronomy – Lecture 4 Carsten Denker Physics Department Center for Solar–Terrestrial Research.
Chapter 13 Gravitation.
CH 12: Gravitation. We have used the gravitational acceleration of an object to determine the weight of that object relative to the Earth. Where does.
Newton’s Laws of Motion and Planetary Orbits Gravity makes the solar system go round.
Chapter 8 Universal Gravitation
Physics 2113 Lecture 03: WED 17 JAN CH13: Gravitation III Physics 2113 Jonathan Dowling Michael Faraday (1791–1867) Version: 9/18/2015 Isaac Newton (1642–1727)
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.
Physics 201: Lecture 24, Pg 1 Chapter 13 The beautiful rings of Saturn consist of countless centimeter-sized ice crystals, all orbiting the planet under.
Essential Idea:  The Newtonian idea of gravitational force acting between two spherical bodies and the laws of mechanics create a model that can be.
Physics 215 – Fall 2014Lecture Welcome back to Physics 215 Today’s agenda: Newtonian gravity Planetary orbits Gravitational Potential Energy.
Announcements Exam 1 is next time. Will cover material in textbook up through Chapter 3 section 3.3 plus additional material on sidereal time and Julian.
Physics 221 Chapter 13 Is there gravity on Mars? Newton's Law of Universal Gravitation F = GmM/r 2 Compare with F = mg so g = GM/r 2 g depends inversely.
Chapter 13 Gravitation. Newton’s law of gravitation Any two (or more) massive bodies attract each other Gravitational force (Newton's law of gravitation)
Monday, Oct. 4, 2004PHYS , Fall 2004 Dr. Jaehoon Yu 1 1.Newton’s Law of Universal Gravitation 2.Kepler’s Laws 3.Motion in Accelerated Frames PHYS.
Gravitation. Gravitational Force and Field Newton proposed that a force of attraction exists between any two masses. This force law applies to point masses.
17-1 Physics I Class 17 Newton’s Theory of Gravitation.
Chapter 13 Outline Gravitation Newton’s law of gravitation Weight Gravitational potential energy Circular orbits Kepler’s laws Black holes.
Proportionality between the velocity V and radius r
Chapter 13 Gravitation Newton’s Law of Gravitation Here m 1 and m 2 are the masses of the particles, r is the distance between them, and G is the.
Chapter 13 Gravitation.
Developing the Science of Astronomy (Chapter 4). Student Learning Objectives Compare ancient and modern theories of the solar system Apply Kepler’s Laws.
Kepler’s Laws of planetary motion Newton’s law of universal gravitation Free fall acceleration on surface of a planet Satellite motion Lecture 13: Universal.
Spring 2002 Lecture #21 Dr. Jaehoon Yu 1.Kepler’s Laws 2.The Law of Gravity & The Motion of Planets 3.The Gravitational Field 4.Gravitational.
Gravitation. Flat Earth This is true for a flat earth assumption. Is the earth flat? What evidence is there that it is not? Up to now we have parameterized.
PHYS 2010 Nathalie Hoffmann University of Utah
Stable Orbits Kepler’s Laws Newton’s Gravity. I. Stable Orbits A. A satellite with no horizontal velocity will __________________. B. A satellite with.
Gravitation and the Waltz of the Planets Chapter 4.
Wednesday, Oct. 10, 2007 PHYS , Fall 2007 Dr. Jaehoon Yu 1 PHYS 1443 – Section 002 Lecture #11 Wednesday, Oct. 10, 2007 Dr. Jaehoon Yu Free Fall.
Section Orbital Motion of Satellites and Kepler’s Laws
Chapter 13 Gravitation & 13.3 Newton and the Law of Universal Gravitation Newton was an English Scientist He wanted to explain why Kepler’s Laws.
Satellite Physics & Planetary Motion Illustration from Isaac Newton, Philosophiae Naturalis Principia Mathematica, Book III Isaac Newton was the first.
Physics 141Mechanics Lecture 18 Kepler's Laws of Planetary Motion Yongli Gao The motion of stars and planets has drawn people's imagination since the.
Physics Section 7.3 Apply Kepler’s Laws of Planetary Motion The Polish astronomer Nicolas Copernicus was the first to correctly place the sun at the center.
Kepler’s Laws What are the shapes and important properties of the planetary orbits? How does the speed of a planet vary as it orbits the sun? How does.
Newton’s Law of Universal Gravitation by Daniel Silver AP Physics C
The Science of Orbits (Power Point 04) Image Credit: NASA.
College Physics, 7th Edition
Physics for Scientists and Engineers, 3rd edition
Kepler’s Laws of Orbital Motion
Chapter 12 Gravity.
Kepler’s 3 Laws of planetary motion
Kepler’s Laws of Motion
Origin of Modern Astronomy
3.2 Gravity and Kepler’s Solar System
Universal Law of Gravitation
Newton’s Law of Universal Gravitation
Newton’s Laws of Motion
Last Time: Centripetal Acceleration, Newtonian Gravitation
Physics I Class 18 Newton’s Theory of Gravitation.
Chapter 13 Universal Gravitation
Unit 2 Review Questions.
Kepler’s Laws.
PHYS 1443 – Section 003 Lecture #11
Universal Gravitation
Gravitational Fields, Circular Orbits and Kepler
Chapter 2 - Part 1 The two body problem
Gravitation.
PHYS 1443 – Section 001 Lecture #8
Gravitational Fields, Circular Orbits and Kepler’s Laws
Kepler’s Laws.
Kepler’s Laws and Universal Gravitation
Newton’s Laws: The New Physics
Presentation transcript:

PHYSICS 197 Section 1 Chapter N11 Kepler’s Laws November 3, 2017

Announcements Wednesday, November 8: Newton’s Law Problem Solving (please email me the problems you want to be discussed in class by 9pm Tuesday, November 7). Wednesday, November 15: Review of Unit N (more problem solving). Thursday, November 16: Exam #2 (6.30-11pm). Please (RE)DO the book examples, weekly HWs and practice problems by yourself (without looking at the solution or any other help) before exam.

Overview Orbital Motion: Use Newton’s gravitational force law to predict planetary orbits. Derive Kepler’s laws as a consequence of Newtonian laws of mechanics (planets are freely falling around the sun). Universal model (for terrestrial and celestial mechanics).

Kepler’s Laws (derived using Brahe’s data) 1st law: The orbits of planets are ellipses, with the sun at one focus. Sum of distances to the two focii is constant for each point on the curve.

Kepler’s Laws (derived using Brahe’s data) 2nd law: A line from the sun to the planet sweeps out equal areas in equal time.

Kepler’s Laws 3rd law: The square of a planet’s period T is proportional to the cube of its orbit’s semimajor axis a.

Clicker Question

Answer

Orbits Around a Massive Primary Consider a very massive object interacting with a much lighter object. Choose the origin of our reference frame to be the system’s center of mass.

Orbits Around a Massive Primary

Orbits Around a Massive Primary For M >> m,

Kepler’s 2nd Law Total angular momentum of the system: Conservation of angular momentum implies that the angular momentum of either object is conserved, along with that of the whole system. From the definition,

Kepler’s 2nd Law

Kepler’s 3rd Law Newton’s law of universal gravitation: If this is the only force acting on the satellite (separated by distance R from the primary), For a uniform circular motion, the centripetal acceleration is So we get Time period which gives

Escape Velocity For earth, ve = 11.2 km/s For moon, ve = 2.4 km/s (Smaller than the average molecular speed at room temperature. That’s why no atmosphere on moon!)

Black Hole An object for which the escape velocity is greater than the speed of light. So not even light can escape! Then how do we know they exist? Use Kepler’s 3rd law: (if we can measure the orbit of a visible companion) Supermassive black holes (up to a billion solar masses) found in the center of almost all known galaxies (including Milky Way).

Dark Matter The Large Magellanic Cloud is a satellite galaxy of our Milky Way, orbiting with a radius of about 170,000 light years (1.6x1021m) and orbital velocity of about 200 km/s. This implies the total mass of our galaxy Visible matter is only about 20%. The rest is dark matter.

Practice Problem