Guide to the Cosmos

 Making the Wonders of our Universe Accessible to Everyone.

 

 

Historic First Black Hole Image

 

In April, news outlets across the world announced the first successful attempt to capture the image of a black hole, accomplished by the Event Horizon Telescope (EHT) consortium, which comprises over 207 scientists from 36 universities and scientific institutes (by my count).

 

Recently, EHT published six research papers describing this feat. This newsletter explores the highlights of those papers.

 

EHT confirmed Einstein’s theory of general relativity in several exceptional regards. They achieved the most precise measurement ever made of the size of a black hole, and validated general relativity in a record-high gravitational field — about one billion g (1 g = Earth’s surface gravity).

 

To accomplish this feat, EHT built an array of 8 radio telescopes spanning half Earth’s surface, as shown here. Two telescopes are in Hawaii, two in Chile, one in Arizona, one in Mexico, one in Spain, and one near the South Pole. Using interferometry, this array achieves sufficient resolution — about 10 micro-arcseconds — to read 10-point type from 50,000 miles away.

 

 

On four nights in April 2017, EHT targeted M87*, the black hole at the center of galaxy M87, 55 million light-years away. They spent two years processing 15 million gigabytes of data to get this image.

 

The black hole, hidden within its event horizon, is in the dark center of the yellow/orange donut. In this image, color denotes temperature — the brightest yellow corresponds to 11 billion ºF.

 

The “donut” is actually a photon ring — light captured by the black hole’s gravity that spirals in quasi-stable, nearly circular orbits. From their analysis, EHT determined the photons at the donut’s bottom are moving toward us as they orbit the black hole and therefore appear brighter than the photons at the donut’s top, which are moving away from us.

 

EHT analyzed radio waves of frequency 320 GHz (1.3 mm wavelength), because light of that frequency easily penetrates the material surrounding a black hole — a plasma of electrons and ionized gas.

 

Astronomers typically minimize atmospheric interference by placing their telescopes atop high mountains. EHT telescopes are at elevations ranging from 9,400 to 17,000 feet (2816 to 5105 m). EHT went further and collected data only on clear, cold winter’s nights (as cold as –300ºF). In air that thin, normal computer hard drives fail quickly, so EHT puts their drives in pressurized, helium-filled containers.

 

If EHT had one 7000-mile-wide radio telescope, obtaining this image would be almost as easy as point-and-shoot. However, getting that resolution from 8 telescopes spread across 7000 miles is much more complex — that’s why it took two years.

 

Interferometry relies on comparing the phases of radio waves arriving at each of the 8 telescopes. All the data from each telescope must be recorded and precisely time-stamped. Computer hard drives full of data must be flown from the telescope sites to two analysis centers that independently process them (double checking one another). More about image processing later.

 

From their analysis, EHT measured the mass of black hole M87* to be 6.5 billion times the mass of our Sun, its gravitational radius Rg to be 10 billion km, and the photon ring radius to be 5.5Rg — all measured with 10% precision, and all consistent with general relativity.

 

With this image, general relativity has been validated over a range of masses spanning 15 orders of magnitude.

 

A jet of charged particles shoots out along the rotational axis of M87*, as seen in this Hubble Space Telescope image. When measured at radio frequencies, this jet is 200,000 light-years along, about twice the diameter of our Milky Way galaxy.

 

EHT will soon target Sag A*, the black hole at the center of our galaxy. Sag A* is 27,000 light-years from us, and its mass is 4.1 million times our Sun’s mass. Sag A* is 2000 times closer and 1600 times less massive than M87*. Objects in the inner most stable orbit take days to orbit M87* but only minutes to orbit Sag A*, which makes imaging Sag A*’s rings more challenging. With some upgrades, EHT has a good shot at making high precision measurements of Sag A*.

 

For those interested in more technical details, interferometry produces a frequency map (2D Fourier transform) of the target rather than a conventional image. Here is EHT’s frequency map of M87A*. The data lie in arcs due to Earth’s rotation during each night’s exposure.

 

If the colored frequency data filled the entire outer circle, EHT could easily reconstruct a perfect image. The art here is filling in the blanks. Incidentally, this is the same problem I once faced doing CT-scans on beating human hearts.

 

 

 

 

Best Regards,

Robert


October, 2019

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To learn more about the mechancs of Black Holes, their expansion, their size, and where & how many exist in the cosmos, click here.

 

 

 

 

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