Gravitational Potential Energy When we are close to the surface of the Earth we use the constant value of g. If we are at some altitude above the surface.

Slides:



Advertisements
Similar presentations
P5a(i) Satellites, Gravity and Circular Motion
Advertisements

Special Stars Neutron Stars Black Holes. Massive Star Evolution 4 Massive stars burn hot and bright while on the main sequence, usually as a blue or whitish-blue.
Universal Gravitation
9A Black Holes and Neutron Stars Dead Stars Copyright – A. Hobart.
Neutron Stars and Black Holes Please press “1” to test your transmitter.
Copyright © 2010 Pearson Education, Inc. Chapter 13 Black Holes.
Black Holes. Outline Escape velocity Definition of a black hole Sizes of black holes Effects on space and time Tidal forces Making black holes Evaporation.
Solar System. What is the Solar System? Consists of a star, (like the sun) and all of the planets, moons and other bodies that travel around it. Planets.
Neutron Stars and Black Holes
10 Black Holes and Neutron Stars Dead Stars Copyright – A. Hobart.
PHYS16 – Lecture 27 Gravitation November 10, 2010.
13 Black Holes and Neutron Stars Dead Stars Copyright – A. Hobart.
13 Black Holes and Neutron Stars Dead Stars Copyright – A. Hobart.
SMDEP Physics Gravity: Orbits, energy. Ch 6, #27 (b) only: mass of stars? 1.9x10 28 kg 2.9x10 26 kg 3.5x10 26 kg 4.5x10 24 kg 5.Other 6.Didn’t finish.
Chapter 12 Gravitation. Theories of Gravity Newton’s Einstein’s.
Two satellites A and B of the same mass are going around Earth in concentric orbits. The distance of satellite B from Earth’s center is twice that of satellite.
Black Holes By Irina Plaks. What is a black hole? A black hole is a region in spacetime where the gravitational field is so strong that nothing, not even.
Gravitational Potential Energy When we are close to the surface of the Earth we use the constant value of g. If we are at some altitude above the surface.
Black Holes.
Unit 06 “Circular Motion, Gravitation and Black Holes” “Gravitation and Black Holes”
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.
-Energy Considerations in Satellite and Planetary Motion -Escape Velocity -Black Holes AP Physics C Mrs. Coyle.
What keeps them in orbit?
Gravity Review.
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.
Black Holes. Gravity is not a force – it is the curvature of space-time - Objects try and move in a straight line. When space is curved, they appear to.
Gravitational Interactions
Unit 06 “ Circular Motion, Gravitation and Black Holes” Gravity in our Solar System.
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 Universal Gravitation. Intro Prior to – Vast amounts of data collected on planetary motion. – Little understanding of the forces involved.
Chapter 12 Universal Law of Gravity
Copyright © 2012 Pearson Education Inc. Orbital motion, final review Physics 7C lecture 18 Thursday December 5, 8:00 AM – 9:20 AM Engineering Hall 1200.
Black Holes This one’s green. I like green.. What happens after a SN? Material remaining after a supernova is 3 times more massive than the sun or more.
Death of Stars III Physics 113 Goderya Chapter(s): 14 Learning Outcomes:
Newton’s Law of Universal Gravitation
Unit 06 “ Circular Motion, Gravitation and Black Holes” Gravitation Problem Solving.
Life Cycle of a Star. Nebula(e) A Star Nursery! –Stars are born in nebulae. –Nebulae are huge clouds of dust and gas –Protostars (young stars) are formed.
Black Holes Chapter 14. Review What is the life cycle of a low mass star (
Black Holes Astrophysics Lesson 14. Learning Objectives To know:-  How to define the event horizon for a black hole.  How to calculate the Schwarzschild.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 12 Physics, 4 th Edition James S. Walker.
It was discovered in the early 1990’s that the pulse period of a millisecond pulsar 500 parsecs from earth varies in a regular way.
Q12.1 The mass of the Moon is 1/81 of the mass of the Earth.
Gravitation Using the law of universal gravitation to gain perspective on planets, moons, stars and black holes.
T072: Q19: A spaceship is going from the Earth (mass = M e ) to the Moon (mass = M m ) along the line joining their centers. At what distance from the.
Neutron Stars & Black Holes. Neutron Stars and Black Holes I. Neutron Stars A. Remnant from the collapse of a _________. B. During the core collapse of.
Black Holes. Escape Velocity The minimum velocity needed to leave the vicinity of a body without ever being pulled back by the body’s gravity is the escape.
Physics. Gravitation - 2 Session Session Opener How much velocity do you need to impart a stone such that it escapes the gravitational field of the earth?
Black Holes and Gravity 1)Type II Supernova 2)Neutron Stars 3)Black Holes 4)More Gravity April 7, 2003
Astronomy 1020 Stellar Astronomy Spring_2016 Day-34.
PHY 151: Lecture Newton’s Law of Universal Gravitation 11.2 Structural Models 11.3 Kepler’s Laws 11.4 Energy Considerations in Planetary and Satellite.
1 The law of gravitation can be written in a vector notation (9.1) Although this law applies strictly to particles, it can be also used to real bodies.
Black Hole. Special Relativity Einstein’s special theory of relativity has two parts. –All objects moving at constant velocity have the same laws of physics.
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.
Newton Anything with mass attracts anything else with mass. The size of that attraction is given by my Law of Gravitation: Fg = Gm 1 m 2 r 2.
Variation of g with Height
This one’s green. I like green.
Chapter 12 Gravity.
Lecture Outline Chapter 12 Physics, 4th Edition James S. Walker
The Sun The sun is made up of no solids or liquids
Black Holes and Neutron Stars
Chapter 13 Universal Gravitation
Universal Gravitation
Universal Gravitation & Satellites
The Death of a Star.
THE LIFE CYCLE OF STARS Chapter 15-2 Part 3.
THE LIFE CYCLE OF STARS Chapter 15-2 Part 3.
Black Holes Chapter 14.
The Death of a Star.
THE LIFE CYCLE OF STARS Chapter 15-2 Part 3.
Learning Goals: 4. Complex Knowledge: demonstrations of learning that go aboveand above and beyond what was explicitly taught. 3. Knowledge: meeting.
Presentation transcript:

Gravitational Potential Energy When we are close to the surface of the Earth we use the constant value of g. If we are at some altitude above the surface of the Earth we must use the radially dependent form of the gravitational acceleration. Assumes constant g! 0 0 We will define U i = 0 when r i = For more than two masses: Only valid for r > R E !

Energy Considerations for Planetary Motion This is the total energy of an object orbiting a larger stationary mass. This is a reasonable assumption if m << M. For circular orbits, the speed of the small mass is constant. For elliptical orbits the speed of the small mass is not constant! For a circular orbit we can determine v in the following way: 1 2 What happens as the planet moves from 1 to 2? What happens as the planet moves from 2 to 1? The distance from the sun decreases and hence the potential energy decreases, therefore the kinetic energy and hence the speed must increase. The distance from the sun increases and hence the potential energy increases, therefore the kinetic energy and hence the speed must decrease. We can now rewrite the energy:

Escape Speed The term escape speed or escape velocity if often used when discussing the launching of a rocket into space. What is escape speed? Escape speed is the minimum initial speed required for an object to approach an infinite separation from the Earth. There is no propulsion system on this object. 0

Black Holes What is a black hole? Gravitational well with extremely high gravitational forces. Singularity Event Horizon (Point of no return) RsRs Creation of a black hole: 1.Massive star explodes – Supernova 2.Mass that does not travel far enough gets pulled back and the mass collapses under gravitational forces to form one of the following: a)White Dwarf – M < 1.4 M sun b)Neutron Star – M > 1.4 M sun c)Black Hole – M > 3 M sun For a black hole the mass is compacted into a single point called a singularity. Ideally this point would have zero volume and therefore infinite density. Everything that enters a black hole (passes the event horizon) is pulled into the singularity, including light! R s – Schwartzchild radius Extremely dense star (R ~ 10 km) 1 teaspoon weighs 5 billion tons!

The black hole can emits high energy electromagnetic radiation, as shown in the illustration below. This electromagnetic radiation is not in the visible spectrum. A star loses mass to a black hole. This is the result of a single star of a binary pair collapsing into a black hole, or possibly a single star exploding and creating a black hole and another star. An astronaut entering a black hole. The gravitational forces are so strong that the gravitational force at the astronauts head is stronger than the gravitational force at his feet. This causes the stretching and eventually the astronaut would be torn apart.