Stable Orbits Kepler’s Laws Newton’s Gravity. I. Stable Orbits A. A satellite with no horizontal velocity will __________________. B. A satellite with.

Slides:



Advertisements
Similar presentations
What is Circular Motion?
Advertisements

Newton’s Law of Universal Gravitation
Newton’s Law of Universal Gravitation.  Any two objects exert a gravitational force of attraction on each other. The magnitude of the force is proportional.
18-1 Physics I Class 18 Newton’s Theory of Gravitation.
D. Roberts PHYS 121 University of Maryland Physic² 121: Phundament°ls of Phy²ics I November 6, 2006.
Gravitation Newton’s Law of Gravitation; Kepler’s Laws of Planetary Motion. Lecture 14 Monday: 1 March 2004.
Kepler’s Laws of Planetary Motion Newton’s Laws of Gravity
Chapter 13: Gravitation. Newton’s Law of Gravitation A uniform spherical shell shell of matter attracts a particles that is outside the shell as if all.
Satellite Motion. Low Orbit  A container falls off the space station while in low earth orbit. It will move A) straight down toward Earth. A) straight.
Physics 111: Mechanics Lecture 13 Dale Gary NJIT Physics Department.
Chapter 7 Review.
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.
Chapter-5: Circular Motion, the Planets, and Gravity Circular Motion: Centripetal acceleration Centripetal force Newton’s law of universal gravitation.
Introduction to Gravity and Orbits. Isaac Newton Born in England in 1642 Invented calculus in early twenties Finally published work in gravity in 1687.
Planets of the Solar System Section 2 Section 2: Models of the Solar System Preview Key Ideas Early Models Kepler’s Laws Newton’s Explanation of Kepler’s.
Physics 111: Mechanics Lecture 13
Ch. 8 Universal Gravitation
Circular Motion; Gravitation
Newton’s Law of Universal Gravitation
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.
Chapter 5 Dynamics of Uniform Circular Motion. Circular Motion If the acceleration is in the same direction as the velocity i.e., parallel to the velocity,
Planetary Dynamics § 13.4–13.8. Closed Orbits U g + K tr = constant < 0 The closer the satellite is to the main body, the faster it moves Objects do not.
Newton’s Law of Universal Gravitation
Chapter Planetary Motion & Gravitation Nicholas Copernicus (Polish) Pulished Earth-centered model in 1543 Tycho Brahe (Danish) Vowed to be an astronomer.
Kepler’s three laws Kepler’s three laws explain how planets orbit around the sun. These laws are common to any body orbiting around a massive body.
In this chapter you will:  Learn the nature of gravitational force.  Relate Kepler’s laws of planetary motion to Newton's laws of motion.  Describe.
Review Question What are Kepler’s laws?. Review Question What are Newton’s laws?
Gravitation. Gravitational Force and Field Newton proposed that a force of attraction exists between any two masses. This force law applies to point masses.
Chapter 12 Universal Law of Gravity
Kepler’s laws, Gravitational attraction, and projectile motion.
Newton’s Law of Universal Gravitation
Universal Gravitation. Paths of Satellites around Earth
17-1 Physics I Class 17 Newton’s Theory of Gravitation.
UNIVERSAL GRAVITATIONAL LAW of
Gravity and Orbits   Newton’s Law of Gravitation   The attractive force of gravity between two particles   G = 6.67 x Nm 2 /kg 2 Why is this.
SUMMARY Kepler’s 3 laws (pages 3-4-5) Illustration of Kepler’s laws (page 6) Newton’s law of universal gravitation (pages 7-8)Newton’s law of universal.
Chapter 6 - Gravitation Newton’s Law of Gravitation (1687)
Board Work 1.A satellite revolves around its planet in a perfectly circular orbit at a constant speed. a.At each of the four positions, draw a vector representing.
Daily Science Pg.30 Write a formula for finding eccentricity. Assign each measurement a variable letter. If two focus points are 450 km away from one another.
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.
Newton’s Law of Universal Gravitation
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
Gravitation and the Waltz of the Planets Chapter 4.
What is gravity? GalileoGalileo and Newton gave the name Newton GalileoNewton gravity to the force that exists between the Earth and objects. Newton showed.
Section Orbital Motion of Satellites and Kepler’s Laws
Universal Gravitation Newton’s 4 th law. Universal Gravitation Kepler’s Laws Newton’s Law of Universal Gravity Applying Newton’s Law of Universal Gravity.
Unit 3 Lesson 2 Kepler’s Laws of Planetary Motion.
Laws of Planetary Motion KEPLER & NEWTON. Kepler’s 3 Laws  1 st Law- Law of Ellipses  2 nd Law- Law of Equal Areas  3 rd Law- Law of Periods.
Satellite Motion Satellite – a projectile moving fast enough to fall continually around the Earth rather than into it - the Earth surface drops a vertical.
 Compare the models of the universe developed by Ptolemy and Copernicus.  Summarize Kepler’s three laws of planetary motion.  Describe how Newton explained.
Aristotle suggested an Earth-centered, or geocentric, model of the solar system. In this model, the sun, the stars, an the planets revolved around Earth.
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.
Chapter 9: Gravity Gravity is the force most familiar to us, and yet, is the least understood of all the fundamental forces of nature.
Newton’s Law of Universal Gravitation
Newton’s Law of Gravity
Newton’s Laws of Motion
What is gravity? Galileo and Newton gave the name
Section 2: Models of the Solar System
Models of the Solar System
Kepler’s Laws.
Chapter-5: Circular Motion, the Planets, and Gravity
Section 2: Models of the Solar System
Gravitational Fields, Circular Orbits and Kepler
Kepler’s Laws Ms. Jeffrey- Physics.
Gravitation See video on extreme sports --- defying gravity
Newton’s Law of Universal Gravitation
Kepler’s Three Laws of Planetary Motion
Kepler’s Laws.
Newton’s Law of Universal Gravitation
Presentation transcript:

Stable Orbits Kepler’s Laws Newton’s Gravity

I. Stable Orbits A. A satellite with no horizontal velocity will __________________. B. A satellite with some horizontal velocity will follow a ___________. C. A satellite with sufficient horizontal velocity will fall at the same rate that the Earth is curving away from it, maintaining a constant height above the ground. This satellite will be in a _______________ orbit. D. Essentially all satellites, moons and planets move in __________ orbits. Stable Orbits, Kepler’s Laws and Newton’s Law of Gravity

I. Stable Orbits no horizontal velocity fall straight down A. A satellite with no horizontal velocity will __fall straight down__. B. A satellite with some horizontal velocity will follow a ___________. C. A satellite with sufficient horizontal velocity will fall at the same rate that the Earth is curving away from it, maintaining a constant height above the ground. This satellite will be in a _______________ orbit. D. Essentially all satellites, moons and planets move in __________ orbits.

I. Stable Orbits fall straight down A. A satellite with no horizontal velocity will __fall straight down__. some horizontal velocitycurved path B. A satellite with some horizontal velocity will follow a _curved path_. C. A satellite with sufficient horizontal velocity will fall at the same rate that the Earth is curving away from it, maintaining a constant height above the ground. This satellite will be in a _______________ orbit. D. Essentially all satellites, moons and planets move in __________ orbits.

I. Stable Orbits fall straight down A. A satellite with no horizontal velocity will __fall straight down__. curved path B. A satellite with some horizontal velocity will follow a _curved path_. stable circular C. A satellite with sufficient horizontal velocity will fall at the same rate that the Earth is curving away from it, maintaining a constant height above the ground. This satellite will be in a __stable circular__ orbit. D. Essentially all satellites, moons and planets move in __________ orbits.

I. Stable Orbits fall straight down A. A satellite with no horizontal velocity will __fall straight down__. curved path B. A satellite with some horizontal velocity will follow a _curved path_. stable circular C. A satellite with sufficient horizontal velocity will fall at the same rate that the Earth is curving away from it, maintaining a constant height above the ground. This satellite will be in a __stable circular__ orbit. elliptical D. Essentially all satellites, moons and planets move in _elliptical__ orbits.

F. Speeds vary for a planet as it moves around the Sun in an elliptical orbit. E. Planets near the Sun will orbit with a _______ speed. Planets far from the Sun will orbit with a _________ speed. Distance From Sun Speed

F. Speeds vary for a planet as it moves around the Sun in an elliptical orbit. E. Planets near the Sun will orbit with a _______ speed. Planets far from the Sun will orbit with a _________ speed. Distance From Sun Speed faster slower

F. Speeds vary for a planet as it moves around the Sun in an elliptical orbit. faster E. Planets near the Sun will orbit with a _faster_ speed. Planets far from the Sun will orbit with a _________ speed. Distance From Sun Speed faster slower Sun

F. Speeds vary for a planet as it moves around the Sun in an elliptical orbit. faster slower E. Planets near the Sun will orbit with a _faster_ speed. Planets far from the Sun will orbit with a __slower__ speed. Distance From Sun Speed faster slower Sun

F. Speeds vary for a planet as it moves around the Sun in an elliptical orbit. faster slower E. Planets near the Sun will orbit with a _faster_ speed. Planets far from the Sun will orbit with a __slower__ speed. Distance From Sun Speed faster slower faster slower

II. Kepler’s 3 Laws 1. The orbit of a planet around the Sun is an _______ with the Sun at one _______. 2. A line joining the Sun and the planet sweep out equal ______ in equal _______. 3. The square of the planet’s orbital _______ is directly proportional to the cube of the ______________ of the planet’s orbit. Sun

II. Kepler’s 3 Laws ellipsefocus 1. The orbit of a planet around the Sun is an _ellipse_ with the Sun at one _focus_. 2. A line joining the Sun and the planet sweep out equal ______ in equal _______. 3. The square of the planet’s orbital _______ is directly proportional to the cube of the ______________ of the planet’s orbit. Sun

II. Kepler’s 3 Laws ellipsefocus 1. The orbit of a planet around the Sun is an _ellipse_ with the Sun at one _focus_. 2. A line joining the Sun and the planet sweep out equal ______ in equal _______. 3. The square of the planet’s orbital _______ is directly proportional to the cube of the ______________ of the planet’s orbit. elliptical orbit focusfocus Sun

II. Kepler’s 3 Laws ellipsefocus 1. The orbit of a planet around the Sun is an _ellipse_ with the Sun at one _focus_. areastimes 2. A line joining the Sun and the planet sweep out equal _areas_ in equal _times_. 3. The square of the planet’s orbital _______ is directly proportional to the cube of the ______________ of the planet’s orbit. elliptical orbit focusfocus Sun

A3 A2 A1 II. Kepler’s 3 Laws ellipsefocus 1. The orbit of a planet around the Sun is an _ellipse_ with the Sun at one _focus_. areastimes 2. A line joining the Sun and the planet sweep out equal _areas_ in equal _times_. 3. The square of the planet’s orbital _______ is directly proportional to the cube of the ______________ of the planet’s orbit. elliptical orbit focusfocus 1 month Sun A1 = A2 = A3

A3 A2 A1 II. Kepler’s 3 Laws ellipsefocus 1. The orbit of a planet around the Sun is an _ellipse_ with the Sun at one _focus_. areastimes 2. A line joining the Sun and the planet sweep out equal _areas_ in equal _times_. period semimajor axis 3. The square of the planet’s orbital _period_ is directly proportional to the cube of the _semimajor axis_ of the planet’s orbit. elliptical orbit focusfocus 1 month Sun A1 = A2 = A3

A3 A2 A1 II. Kepler’s 3 Laws ellipsefocus 1. The orbit of a planet around the Sun is an _ellipse_ with the Sun at one _focus_. areastimes 2. A line joining the Sun and the planet sweep out equal _areas_ in equal _times_. period semimajor axis 3. The square of the planet’s orbital _period_ is directly proportional to the cube of the _semimajor axis_ of the planet’s orbit. elliptical orbit focusfocus 1 month T (period) = time it takes for the planet to make one orbit a (semimajor axis) = average distance between the planet and the Sun Sun A1 = A2 = A3 T 2 ~ a 3

III. Newton’s Law of Gravity 1. All masses ________ one another and never ______. 2. The gravitational force between two masses, m 1 and m 2, is proportional to the ________ of the two masses. 3. The gravitational force between two masses is also _____________________ to the distance between to the two masses squared. m1m1m1m1 m2m2m2m2 r

III. Newton’s Law of Gravity attractrepel 1. All masses _attract_ one another and never _repel_. 2. The gravitational force between two masses, m 1 and m 2, is proportional to the ________ of the two masses. 3. The gravitational force between two masses is also _____________________ to the distance between to the two masses squared. m1m1m1m1 m2m2m2m2 r

III. Newton’s Law of Gravity attractrepel 1. All masses _attract_ one another and never _repel_. product 2.The gravitational force between two masses, m 1 and m 2, is proportional to the _product_ of the two masses. 3. The gravitational force between two masses is also _____________________ to the distance between to the two masses squared. m1m1m1m1 m2m2m2m2 r

III. Newton’s Law of Gravity attractrepel 1. All masses _attract_ one another and never _repel_. product 2.The gravitational force between two masses, m 1 and m 2, is proportional to the _product_ of the two masses. inverselyproportional 3. The gravitational force between two masses is also _inversely_proportional_ to the distance between to the two masses squared. m1m1m1m1 m2m2m2m2 r

III. Newton’s Law of Gravity attractrepel 1. All masses _attract_ one another and never _repel_. product 2. The gravitational force between two masses, m 1 and m 2, is proportional to the _product_ of the two masses. inverselyproportional 3. The gravitational force between two masses is also _inversely_proportional_ to the distance between to the two masses squared. Newton’s gravitational constant m1m1m1m1 m2m2m2m2 r