Why Do Astrophysicists Use νLν in Accretion Disk Emission Studies?

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Discussion Overview

The discussion centers on the use of the product νLν in the emission spectrum of accretion disks, particularly in the context of Active Galactic Nuclei (AGNs). Participants explore the reasons for this choice in plotting luminosity against frequency, touching on both theoretical and practical aspects of astrophysical graphing techniques.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants suggest that frequency is used to identify nuclei, while luminosity indicates the amount of energy emitted.
  • There is a question about why the product νLν is often plotted instead of just Lν, with some proposing that it helps reduce graph size and makes variations across the electromagnetic spectrum more visible.
  • One participant notes that logarithmic or power-of-10 scales are sometimes used to accommodate the wide range of values in the spectrum.
  • Another perspective is that the product νLν is conventional in the field, as AGNs typically exhibit a double hump structure in their emission spectra.
  • Concerns are raised about the theoretical basis for using νLν, with a participant arguing that the variations in luminosity are the primary concern, regardless of whether νLν or Lν is plotted.
  • Some participants clarify that Lν represents spectral luminosity measured in units of (W/Hz), and that multiplying by frequency gives total luminosity over a specific interval.
  • References to literature, such as Dan Maoz's "Astrophysics in a Nutshell" and Carroll & Ostlies' "An Introduction to Modern Astrophysics," are provided to support claims about the interpretation of the graphs.

Areas of Agreement / Disagreement

Participants express various viewpoints on the reasons for using νLν in plots, with no clear consensus reached. Some agree on the utility of the product for graphing purposes, while others question its theoretical justification.

Contextual Notes

Some limitations in the discussion include assumptions about the audience's familiarity with astrophysical concepts and the potential for different interpretations of the graphs based on plotting choices.

Astroiaco
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Why in Astrophysics it is used νLν (where ν is the frequency and Lν is the luminosity at that frequency) in the emission spectrum of an accretion disk?
 
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Frequency is used to identify nuclei, while luminosity will tell you how much.
 
Ok, but why often in the plot of luminosity (where there are ν in abscissa and ν*Lν in ordinate) there is the product between ν and Lν and not only Lν? I don't know if i explained myself better.
 
Accretion disk are of different scales, depending on the mass of the black hole. But guessing from your profile pic and the similarity of the field I assume you are talking about the supermassive black hole accreting galactic matter; more precisely Active Galactic Nuclei(AGNs).

Astroiaco said:
but why often in the plot of luminosity (where there are ν in abscissa and ν*Lν in ordinate) there is the product between ν and Lν and not only Lν?
Here's why I think it is so: to reduce the graph size!

There's something you missed, sometimes the graph is plotted logarithmically, otherwise in powers of 10. This is because the Spectrum is expected to account for the variations across the whole electromagnetic range, and hence the graph would be too big if plotted in normal units.
Spectral-energy-distributions-SED-of-the-blazar-PKS-2155-304-during-its-2006-highly.png


A similar reasoning goes for plotting the product νLν. In log units this is easier to see. Notice that log(νLν)=logν+logLν. Now look at the above graph, a simple subtraction will tell you that the y-axis of the graph scales from -24 to -35 if only logLν is plotted.

Another reason might be by convention. Usually AGNs have a typical double hump(the shapes vary for different sources) structure when plotted as a product. In field they usually fit the different emission mechanics to this double hump structure; not that you can't do this for just luminosity, it's just what they do.

PS: Why I think this can't be from concrete theoretical calculation? Well, it doesn't matter if you plot luminosity or the product of luminosity and frequency, since the only quantity with nontrivial variations is the luminosity. Besides there are options in plotting program to plot ν2Lν.
 

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Astroiaco said:
Why in Astrophysics it is used νLν (where ν is the frequency and Lν is the luminosity at that frequency) in the emission spectrum of an accretion disk?

Could you pls provide a reference source? I suspect that ##L_{\nu}## would be a spectral luminosity, i.e. luminosity per an unit frequency interval, measured in units ##(W/Hz)##. By multiplying this value and a specific frequency interval ##\nu##, you should get the total luminosity in Watts over this specific interval.
 
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lomidrevo said:
Could you pls provide a reference source? I suspect that ##L_{\nu}## would be a spectral luminosity, i.e. luminosity per an unit frequency interval, measured in units ##(W/Hz)##. By multiplying this value and a specific frequency interval ##\nu##, you should get the total luminosity in Watts over this specific interval.
I'm studying the AGNs for my undergraduate thesis, so i have many reference sources, but for example you can find this type of writing on: Dan Maoz "Astrophysics in a Nutshell".

Yes, ##L_{\nu}## is measured in units ##(W/Hz)##.
 
phoenix95 said:
Accretion disk are of different scales, depending on the mass of the black hole. But guessing from your profile pic and the similarity of the field I assume you are talking about the supermassive black hole accreting galactic matter; more precisely Active Galactic Nuclei(AGNs).Here's why I think it is so: to reduce the graph size!

There's something you missed, sometimes the graph is plotted logarithmically, otherwise in powers of 10. This is because the Spectrum is expected to account for the variations across the whole electromagnetic range, and hence the graph would be too big if plotted in normal units.
View attachment 230147

A similar reasoning goes for plotting the product νLν. In log units this is easier to see. Notice that log(νLν)=logν+logLν. Now look at the above graph, a simple subtraction will tell you that the y-axis of the graph scales from -24 to -35 if only logLν is plotted.

Another reason might be by convention. Usually AGNs have a typical double hump(the shapes vary for different sources) structure when plotted as a product. In field they usually fit the different emission mechanics to this double hump structure; not that you can't do this for just luminosity, it's just what they do.

PS: Why I think this can't be from concrete theoretical calculation? Well, it doesn't matter if you plot luminosity or the product of luminosity and frequency, since the only quantity with nontrivial variations is the luminosity. Besides there are options in plotting program to plot ν2Lν.
Thank you very much!
 
Astroiaco said:
I'm studying the AGNs for my undergraduate thesis, so i have many reference sources, but for example you can find this type of writing on: Dan Maoz "Astrophysics in a Nutshell".

Yes, ##L_{\nu}## is measured in units ##(W/Hz)##.

Ah good, I think I found quite a nice explanation in Carroll&Ostlies: "An Introduction to Modern Astrophysics", two snapshots below. If I got it right, when you construct graph like this, the area under the curve of an interval will be proportional to the amount of energy received in that interval (i.e. "equal areas under the graph correspond to equal amounts of energy").

upload_2018-9-10_8-10-58.png


upload_2018-9-10_8-9-47.png
 

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