Optical depth from radiative transfer equation

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SUMMARY

The discussion centers on deriving optical depth using the radiative transfer equation, specifically the equation $$\frac{I}{\tau}= I_0 e^{-\tau}$$. The proposed solution involves taking the natural logarithm of both sides to express optical depth as $$\tau= -\ln(\frac{I}{I_0})$$. The main concern raised is whether it is valid to exclude the source term S from the equation in this context. This indicates a need for clarity on the assumptions made when simplifying the equation.

PREREQUISITES
  • Understanding of the radiative transfer equation
  • Familiarity with optical depth concepts
  • Knowledge of logarithmic functions and their properties
  • Basic principles of light interaction with matter
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  • Study the complete form of the radiative transfer equation
  • Research the role of the source term S in radiative transfer
  • Explore applications of optical depth in astrophysics
  • Learn about numerical methods for solving radiative transfer problems
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Students and researchers in physics, particularly those focused on astrophysics and atmospheric sciences, as well as professionals working with radiative transfer modeling.

Kayla Martin
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Homework Statement
Hi, I can't figure out how to find the optical depth for the following situation:
A supernova remnant has a brightness of I=1.5x10^{-19} Wm^{-2}Hz^{-1}sr^{-1} at frequencies around 1.6-1.7 GHz, but OH molecules in a homogenous foreground cloud produce an absorption line at 1667MHz. The observed intensity at the center of the line is 3.0x10^{-20} Wm^{-2}Hz^{-1}sr^{-1} and the width is 16kHz (corresponding to a velocity width of about 3km/s).
Assuming T_{ex}=12K throughout the cloud for this transition I need to use the radiative transfer equation to calculate the optical depth at the center of the line, tau_0.
Can someone please help me figure this out? I know we have been given all the equations for this in our lecture notes, but I am stumped at how to put it all together?
Relevant Equations
$$\frac{dI}{dS} = - \alpha I + j$$ where $$\alpha$$ is absorption coefficient...
$$\frac{dI}{\tau} = - I + S$$ where S is the source function $$S = \frac{j}{\alpha}$$ and $$\tau$$ is the optical depth.
q.png
 
Last edited:
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The only solution (for part a) I can think of is if we use the radiative transfer equation without S... i.e. $$\frac{I}{\tau}= I_0 e^{-\tau}$$ and then take the natural log of each side to get $$\tau= -\ln(\frac{I}{I_0})$$ but I don't know if I can just get rid of S like that?
 
Last edited:

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