Radio Galaxy Zoo Talk

The Perfect Example?

  • Rosco.medows by Rosco.medows

    Can someone please explain what this image contains. It looks to me like a good example of the symmetry of jets. I have little knowledge of astronomy and joined to learn a little more as i'm fascinated with it.

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  • JeanTate by JeanTate

    Welcome to RGZ, Rosco.medows.

    This is an almost classic example of a #triple, a central radio source (called the "core") and two, almost perfectly symmetrical lobes, connected by back-to-back jets. Each lobe has a "hotspot", which is where the radio intensity reaches its maximum.

    Physically, there's a supermassive black hole in the center of the galaxy (called the "host") - the white (IR) blob - which, through its interactions with the surrounding plasma, produces two highly relativistic jets, shooting in opposite directions. There's a lot which is yet to be understood about exactly how this works, but comparing either jet to what's in the Large Hadron Collider is like comparing a supernova to a candle. The jets plow through the diffuse, hot plasma that surrounds the host (called the intergalactic medium, IGM, or intra-cluster medium), eventually being stopped by it; that's where the hotspots are. The lobes are kinda like bubbles resulting from the energy the jets dump into the IGM.

    The host in this case is SDSS J103748.94+154123.3, which has a redshift of 0.196. Interestingly, its spectrum gives little hint of the stupendous particle accelerator at its center; here's an image of it:

    enter image description here

    Hope this helps, and happy hunting! 😃

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  • Rosco.medows by Rosco.medows

    That's amazing such an epic picture to imagine. Thanks for the explanation

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  • ivywong by ivywong scientist, admin

    Wow, this is a picture perfect #doublelobe. great spotting @Rosco.medows and great explanation as always @JeanTate!

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  • JeanTate by JeanTate in response to Rosco.medows's comment.

    You're welcome @Rosco.medows, and thanks @ivywong !

    which has a redshift of 0.196

    I should have added some words about how far away this is ... as the universe is ruled by General Relativity, "distance" is not so simple! 😮

    The time it took light to get from there to us is ~2.4 billion years; however, the "comoving radial distance" is ~2.6 billion light-years (a light-year is a measure of distance), the "angular size distance" is ~2.2 billion light-years, and the "luminosity distance" is ~3.2 billion light-years.

    However, you measure it, a very long way away!

    If you're interested in doing your own conversions from redshift to distance, I recommend Ned Wright's CosmoCalc. It also includes links to his excellent Cosmology Tutorial, which covers things like why there isn't a single "distance" measure, in cosmology.

    Happy hunting! 😃

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