A neutron star over the Sandias?

Slides:



Advertisements
Similar presentations
Mr Green sees the shorter, straight, green path and Mr. Red sees the longer, curved, red path.
Advertisements

9A Black Holes and Neutron Stars Dead Stars Copyright – A. Hobart.
Black Holes. Dark stars a star that has an escape velocity greater than the speed of light.
Chapter 18: Relativity and Black Holes
Stellar Deaths II Neutron Stars and Black Holes 17.
Neutron Stars and Black Holes Please press “1” to test your transmitter.
Copyright © 2010 Pearson Education, Inc. Chapter 13 Black Holes.
Neutron Stars and Black Holes
The mass of a neutron star cannot exceed about 3 solar masses. If a core remnant is more massive than that, nothing will stop its collapse, and it will.
Black Holes - Chapter 22.
13 Black Holes and Neutron Stars Dead Stars Copyright – A. Hobart.
How do we transform between accelerated frames? Consider Newton’s first and second laws: m i is the measure of the inertia of an object – its resistance.
1. White Dwarf If initial star mass < 8 M Sun or so. (and remember: Maximum WD mass is 1.4 M Sun, radius is about that of the Earth) 2. Neutron Star If.
Review for Test #3 April 16 Topics: Measuring the Stars The Interstellar medium Stellar Evolution and Stellar Death Gamma Ray Bursts Neutron stars, pulsars.
Apparent Brightness α Luminosity/Distance^2
Review for Test #3 Sunday 3-5 PM Topics: The Sun Stars (including our Sun) The Interstellar medium Stellar Evolution and Stellar Death for Low mass, medium.
This set of slides This set of slides continues the late-in-life evolution and death of massive stars, stars > 8 solar masses. It starts with Special and.
Black Holes Astronomy 315 Professor Lee Carkner Lecture 16.
Escape Velocity Velocity needed to escape the gravitational pull of an object. 2GM R vesc = Escape velocity from Earth's surface is 11 km/sec. If Earth.
Question The pressure that prevents the gravitational collapse of white dwarfs is a result of ______.  A) Conservation of energy  B) Conservation of.
Spectral Classes Strange lettering scheme is a historical accident. Spectral Class Surface Temperature Examples OBAFGKMOBAFGKM 30,000 K 20,000 K 10,000.
Clicker Question: The age of a cluster can be found by: A: Looking at its velocity through the galaxy. B: Determining the turnoff point from the main sequence.
Black Holes.
Stationary Elevator with gravity: Ball is accelerated down.
Binary star motion demonstration What does the first demo represent? What will happen if I replace one ball with a smaller ball? What does the second model.
Copyright © 2010 Pearson Education, Inc. Neutron Stars and Black Holes Unit 9.
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.
A black hole is a region of space with such a strong gravitational field that not even light can escape.
Black Holes Formation Spacetime Curved spacetime Event horizon Seeing black holes Demo: 1L Gravity Well - Black Hole.
Lecture 27: Black Holes. Stellar Corpses: white dwarfs white dwarfs  collapsed cores of low-mass stars  supported by electron degeneracy  white dwarf.
Death of Stars III Physics 113 Goderya Chapter(s): 14 Learning Outcomes:
Historical SN and their properties Total energy released ~10 54 erg in a few hours.
Pulsars, Neutron Stars and Black Holes Model of a Neutron Star.
Copyright © 2010 Pearson Education, Inc. Chapter 13 Neutron Stars and Black Holes Lecture Outline.
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.
Announcements Grades for third exam are now available on WebCT Observing this week and next week counts on the third exam. Please print out the observing.
Chapter 13 Neutron Stars and Black Holes. Optical, Infrared and X-ray Image of Cassiopeia A.
ASTR 113 – 003 Spring 2006 Lecture 08 March 22, 2006 Review (Ch4-5): the Foundation Galaxy (Ch 25-27) Cosmology (Ch28-29) Introduction To Modern Astronomy.
A recap of the main points so far… Observers moving uniformly with respect to each other do not agree on time intervals or distance intervals do not agree.
Neutron Stars, Black Holes, Pulsars and More 1)Star Clusters 2)Type II Supernova 3)Neutron Stars 4)Black Holes 5)More Gravity October 30, 2002.
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.
Black Holes A stellar mass black hole accreting material from a companion star 1.
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.
Black Holes A stellar mass black hole accreting material from a companion star 1.
Neutron Stars & Black Holes (Chapter 11) APOD. Student Learning Objective Indentify properties of Neutron Stars & Black Holes NASA.
© 2017 Pearson Education, Inc.
General Relativity.
Chapter S3 Spacetime and Gravity
Supernovas Neutron Stars and Black Holes
Exam Monday Covers reading and related notes from chapters
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.
This one’s green. I like green.
© 2017 Pearson Education, Inc.
Neutron Stars and Black Holes
Incredible Shrinking Stars The End States of Stars.
Relativity H7: General relativity.
Black Holes The mass of a neutron star cannot exceed about 3 solar masses. If a core remnant is more massive than that, nothing will stop its collapse,
Black Holes - Chapter 21.
Black Holes and Neutron Stars
Special vs. General Relativity
Neutron Stars and Black Holes
Exam 3 average: 65%. You will have all of class time on Thursday to do the group review. The response “Exams” will be on Learning Suite by Wed noon. They.
Chapter 22 Black Holes Chapter 22 opener. Neutron stars and black holes are among the more exotic members of the vast population of stars throughout the.
Chapter 13 Neutron Stars and Black Holes
Parts, existence of, origin,
The Death of a Star.
Black Holes Chapter 14.
The Death of a Star.
Principle of Equivalence: Einstein 1907
Presentation transcript:

A neutron star over the Sandias? Neutron Stars If star has mass 12-25 MSun , remnant of supernova expected to be a tightly packed ball of neutrons. Diameter: 10 km only! Mass: 1.4 - 3(?) MSun Density: 1014 g / cm3 ! Rotation rate: few to many times per second!!! Magnetic field: 1010 x typical bar magnet! A neutron star over the Sandias? Please read about observable neutron stars: pulsars.

Black Holes and General Relativity General Relativity: Einstein's (1915) description of gravity (extension of Newton's). It begins with: The Equivalence Principle Demonstrated by either of two thought experiments. 1) Freefall and weightlessness are equivalent a) Imagine you are far from any source of gravity, in free space, weightless. If you shine a light or throw a ball, it will move in a straight line.

b) If you are in freefall (due to gravity), you are also weightless b) If you are in freefall (due to gravity), you are also weightless. Einstein says these are equivalent. So in freefall, light and ball also travel in straight lines. c) Now imagine two people in freefall on Earth, passing a ball back and forth. From their perspective, they pass it in a straight line. From a stationary perspective, it follows a curved path. So will a flashlight beam, but curvature of light path small because light is fast (but not infinitely so). The different perspectives are called frames of reference.

2) Gravity and acceleration are equivalent. An apple falling in Earth's gravity is the same as one falling in an elevator accelerating upwards, in free space. All effects you would observe by being in an accelerated frame of reference you would also observe when under the influence of gravity.

Bending of light in this case: Accelerating elevator in free space: straight path of light appears curved Therefore, same is true of stationary elevator in gravity link

Testable Consequences of General Relativity: 1. Bending of light (just discussed) Observed! In 1919 eclipse.

Gravitational lensing Gravitational lensing. The gravity of a foreground cluster of galaxies distorts the images of background galaxies into arc shapes.

Saturn-mass black hole

2. Gravitational Redshift light received when elevator receding at some speed. later, speed > 0 Consider accelerating elevator in free space (no gravity). Received light has longer wavelength because of Doppler Shift ("redshift"). Gravity must have same effect! Verified in Pound-Rebka experiment. time zero, speed=0 light emitted when elevator at rest. 3. Gravitational Time Dilation Direct consequence of the redshift. Observers disagree on rate of time passage, depending on strength of gravity they’re in.

Escape Velocity Velocity needed to escape an object’s gravitational pull. 2GM R vesc = Earth's surface: vesc = 11 km/sec. If Earth shrunk to R=1 cm, then vesc = c, the speed of light! Then nothing, including light, could escape Earth. This special radius, for a particular object, is called the Schwarzschild Radius, RS. RS  M.

Black Holes If core with about 3 MSun or more collapses, not even neutron pressure can stop it (total mass of star about 25 MSun ?). Core collapses to a point, a "singularity". Gravity is so strong that not even light can escape. RS for a 3 MSun object is 9 km. Event horizon: imaginary sphere around object, with radius RS . Event horizon RS Anything crossing the event horizon, including light, is trapped

Black hole achieves this by severely curving space Black hole achieves this by severely curving space. According to General Relativity, all masses curve space. Gravity and space curvature are equivalent. Like a rubber sheet, but in three dimensions, curvature dictates how all objects, including light, move when close to a mass.

Curvature at event horizon is so great that space “folds in on itself”.

Effects around Black Holes 1) Enormous tidal forces. 2) Gravitational redshift. Example, blue light emitted just outside event horizon may appear red to distant observer. 3) Time dilation. Clock just outside event horizon appears to run slow to a distant observer. At event horizon, clock appears to stop.

Do Black Holes Really Exist? Good Candidate: Cygnus X-1 - Binary system: 30 MSun star with unseen companion. - Binary orbit => companion > 7 MSun. - X-rays => million degree gas falling into black hole.

Final States of a Star 1. White Dwarf If initial star mass < 8-12 Msun . 2. Neutron Star If initial mass > 12 MSun and < 25 ? MSun . 3. Black Hole If initial mass > 25 ? MSun .