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Measuring the Black Hole July 9, 2009

Posted by jcconwell in Black Holes, General Relativity, IYA 2009, Podcast.
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Today’s podcast at 365 days of Astronomy is about measuring those mysterious objects, Black Holes. Usually you think about the tidal forces of a Black Hole ripping and compressing anything falling in until it’s so hot, about 10 million K, that it emits x-rays.

credit: NASA Chandra Space telescope

credit: NASA Chandra Space telescope

In today’s pod-cast sponsored by the EIU Physics Department learn how radio telescope aid our knowledge of these dark objects. Go to:

http://365daysofastronomy.org/2009/07/09/july-9th-measuring-the-black-hole/

Gravitational Waves and LISA January 11, 2009

Posted by jcconwell in Astronomy, Black Holes, General Relativity.
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The AAS meeting in Long Beach this week had many nifty displays. My favorite, since I’m biased toward  general relativity, is the LISA display. LISA stands for Laser Interferometer Space Antenna. Here I am in front of the full scale model of one of three proposed LISA satellites.

The author and a scale model of a LISA satelite

The author and a scale model of a LISA satellite

Now you may wonder why you want an orbiting gravitational wave satellite, especially since we have LIGO (Laser Interferometer Gravitational-Wave Observatory) already taking data. The answer is in the sensitivity diagram below

lisa-ligo_noise_spec1In order to make gravitational radiation you need to have an accelerated mass. The biggest masses with the largest accelerations are colliding black holes and neutron stars. Since most actual collisions are thought to be between orbiting bodies, the frequency of the radiation is related to the orbital frequency = orbits/second.

Now black holes seem to come in two classes. First, stellar mass black holes, created in massive core collapse supernovae. These black holes are around 10 solar masses and have a radius of 30 kilometers (18 miles). The greatest amount of radiation comes just as the two black holes are touching, or merging. The orbital velocities are about the speed of light. and the time to complete one orbit is

(orbital circumference) / velocity = .0006 second

or a frequency of 1600 orbits/second. This about the peak frequency for the radiation from this type of collision. In the diagram above, this frequency band is where LIGO was designed to be the most sensitive.

But there is a second class of black holes, the supermassive holes. These giants are from a million to several billion times the mass of the sun. They seem to form the core in most galaxies, and so when galaxies collide and merge, two orbiting monster black holes will release copious amount of energy. The good news is you can detect this from much further away than the merger of the smaller black holes. The bad news is the frequency.

A two million solar mass hole has a radius of 60 million kilometer and a circumference of about 380 million kilometers. In this case the period for the holes to orbit around each other is much longer

(orbital circumference) / velocity = 126 seconds

or a frequency of .008 orbits/second. A very low frequency, too low to detect on Earth, due earthquakes and seismic activities. This is where the frequency band where  LISA comes in and why you need it in space rather than on Earth.

Extreme Universe: Smallest Black Hole January 10, 2009

Posted by jcconwell in Astronomy, Black Holes, Extreme Universe.
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Not all records in astronomy are about the big stuff.  Good information comes in small packages. A classic case is XTE J1650-500, the smallest or lightest Black Hole measured.

Discovered in 2008 the lowest-mass known black hole belongs to a binary system.. The black hole has about 3.8 times the mass of our sun, and is orbited by a companion star, as depicted in this illustration.

smallbhjpg

Credit: NASA/CXC/A. Hobar

Using a new technique, two NASA scientists have identified the lightest known black hole. With a mass only about 3.8 times greater than our Sun and a radius of  11 kilometers, the black hole lies very close to the minimum size predicted for black holes, or the maximum mass neutron star that originate from dying stars.

The search for the smallest black holes is  important because of the information they tell us about neutron stars, which have a critical upper mass thought to no larger than 3 time the mass of the sun. This upper mass, very similar to the upper mass of white dwarf , which is about 1.4 Solar Masses called Chandrasekhar’s limit, is harder to calculate for the case of a neutron star.

Neutron stars have three extra complications, their rapid spin, the necessity of using general relativity to describe the gravitation, and most important, the nuclear forces at densities the exceed that of normal nuclei. Depending on the nature of the force you can get equations that relate the pressure and densities that very by a factor of 2 or more. resulting in different maximum mass neutron stars that depend on the nuclear force.

Thus the smallest black holes put constraints on the possible type of matter that make up neutron stars.

Inspirally Black Holes & Charleston January 6, 2009

Posted by jcconwell in Black Holes.
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On Monday one of the more interesting talks was the study of binary Black Holes using DEEP2 data. The second interesting part it was given by a Charleston native Julia Comerford, soon to be Dr. Julia Comerford, from UC Berkeley.

DEEP2 uses the DEIMOS spectroscopic data taken with the Keck telescopes on ~1000 galaxies to get rotation curves on galaxies with redshifts z> .7. Some of these galaxies show evidence of two cores or two supermassive holes due to mergers of galaxies over time. The purpose of the survey is to study the evolution of galaxies and their merger over time.

Julie Comerford

Julia Comerford

Extreme Universe: Biggest Black Hole! December 26, 2008

Posted by jcconwell in Astronomy, Black Holes, Extreme Universe.
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In keeping with the end of the year theme of the blog “Extremes in the Universe”. The day after Christmas, an irresistible pull… a point of no return… no we’re not talking about your holiday credit card bill or the after Christmas sales. We are talking black holes.

The heavyweight champion of the year, and at 18 billion solar masses, the largest known black hole in the universe was discovered in January of this year. The biggest black hole beats out its nearest competitor, the black hole in the heart of M87, by a factor of six.

black_hole_big_2_3

Located in the heart of a quasar called OJ287, it’s at a distance of 3.5 billion light years .

Just like other champions, it had some help. In order to measure the black hole’s mass you need an object orbiting it. A smaller black hole, which weighs about 100 million Solar masses, orbits the larger one on an eccentric path every 12 years. It comes close enough to fly through the disc of matter around the larger black hole twice each orbit, causing a pair of outbursts, coming and going, that make OJ287 suddenly brighten.

General relativity predicts that the smaller hole’s orbit itself should precess over time. This effect  is seen in Mercury’s orbit around the Sun, on a much smaller scale.

In the case of OJ287, the immense gravitational field of the larger black hole causes the smaller black hole’s orbit to precess at an  39° each orbit! The precession changes the timing of when the smaller hole punches through the disc surrounding its larger companion.

About a dozen of the resulting bright outbursts have been observed to date, and astronomers led by Mauri Valtonen of Tuorla Observatory in Finland have analysed them to measure the precession rate of the smaller hole’s orbit. That, along with the period of the orbit, suggests the larger black hole weighs a record 18 billion Suns.

The most recent outburst occurred on 13 September 2007, as predicted by general relativity. “If there was no orbital decay, the outburst would have been 20 days later than when it actually happened,” Valtonen told New Scientist, adding that the black holes are on track to merge within 10,000 years, due to orbital decay caused by gravitational radiation.

Craig Wheeler, of the U of Texas, says the observations of the outbursts fit closely with the expectations from general relativity. “The fact that you can fit Einstein’s theory [so well] … is telling you that that’s working,” he says.