Calculating the Temperature in Space

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Discussion Overview

The discussion revolves around calculating the distance from a star at which a black body would reach a specific temperature, particularly in relation to the frost line in the context of the solar system. Participants explore the implications of the Stefan-Boltzmann Law and its application to determining habitable zones around stars.

Discussion Character

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

Main Points Raised

  • One participant proposes using the Stefan-Boltzmann Law to calculate the distance at which a black body reaches a temperature of 160°K, citing a discrepancy with existing literature that suggests a frost line of ~5 AU.
  • Another participant confirms the goal of determining the distance for a black body to achieve a specific temperature and notes the challenges posed by the lack of perfect black bodies.
  • A participant mentions that the frost line is historically related to the conditions during the solar system's formation and suggests that current calculations may yield different results due to changing conditions.
  • It is noted that factors such as a planet's albedo and greenhouse effects could influence the distance at which a planet can support liquid water, complicating the calculations.
  • A later reply references the formation of a comet's coma and its relation to temperature calculations, suggesting that the observed phenomena align with the initial calculations presented.

Areas of Agreement / Disagreement

Participants express differing views on the accuracy of the initial calculations and the implications of historical versus current conditions on the frost line. There is no consensus on the correct distance for the frost line or the impact of various factors on temperature calculations.

Contextual Notes

Participants acknowledge limitations in their calculations due to assumptions about black body behavior, the influence of planetary atmospheres, and the historical context of the frost line. These factors contribute to the uncertainty in determining the exact distances involved.

Who May Find This Useful

This discussion may be of interest to those studying astrophysics, planetary science, or anyone exploring the conditions necessary for habitability around stars.

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I am trying to determine if I am on the right track by using the Stefan-Boltzmann Law to calculate the distance a point in space must be to have a given temperature. For example, the snow line (a.k.a. frost line, ice line) of a star is when the temperature reaches 160°K ± 10°K. Using the Stefan-Boltzmann Law :

313pt03.jpg

Where:
TE = The temperature of the black body object, in Kelvins (160°K in this case)
TS = The surface temperature of the star, in Kelvins
rS = The radius of the star, in meters
a0 = The distance the black body object is from the star, in meters​

Using Sol's data as an example, a black body object would have a temperature of 160°K at 3.04 AU. Yet, according to a paper published on May 9, 2003, the frost line for the Sol system should be ~5 AU.

Remote Infrared Observations of Parent Volatiles in Comets: A Window on the Early Solar System

Which leads me to believe that my approach is incorrect since it does not match our observations. If someone can set me right, it would be greatly appreciated.
 
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You are trying to work out the distance a test black-body is from a star for it to have a particular temperature?
 
Simon Bridge said:
You are trying to work out the distance a test black-body is from a star for it to have a particular temperature?
Yes. I realize that, except for perhaps a black hole, there is no such thing as a perfect black body. That may be where my problem lies. What I am actually trying to determine is the point in space where a particular temperature can be found. The snow line is one example, but if you used 273.15°K and 373.15°K you could, in theory, determine the inner and outer range of "habitable zones" for any given star. If you know the star's effective surface temperature and radius.
 
The " frost line" refers to the distance for certain molecules to coalese into the solid phase during the formation of the solar system billions of years ago. Your PDF does actually refer to it as the nebular frost line can be easily missed while reading. With the different conditions at present, you will of course calculate a different distance.

Take in mind that a planet will reflect some of the radiation which will decrease the distance, and greenhouse effects with an atmosphere will increase the distance .
 
256bits said:
The " frost line" refers to the distance for certain molecules to coalese into the solid phase during the formation of the solar system billions of years ago. Your PDF does actually refer to it as the nebular frost line can be easily missed while reading. With the different conditions at present, you will of course calculate a different distance.

Take in mind that a planet will reflect some of the radiation which will decrease the distance, and greenhouse effects with an atmosphere will increase the distance .
So you are saying that the frost line of ~5 AU was when the Sol system was still in its nebular state. Now, 4.5 billion years later, the frost line should be 3.04 AU, assuming 160°K is the temperature that must be achieved?

Yes, I understand that the albedo, radiative forcing, and atmospheric pressure of a planet will have an effect on whether or not it can support liquid water on its surface. However, absent any planetary information other than its radius and approximate orbit, it should provide a ballpark idea whether or not the planet is anywhere near that range.
 
The coma is generally made of ice and dust.[1] Water dominates up to 90% of the volatiles that outflow from the nucleus when the comet is within 3-4 AU of the Sun.[1] The H2O parent molecule is destroyed primarily through photodissociation and to a much smaller extent photoionization.[1] The solar wind plays a minor role in the destruction of water compared to photochemistry.[1] Larger dust particles are left along the comet's orbital path while smaller particles are pushed away from the Sun into the comet's tail by light pressure
http://en.wikipedia.org/wiki/Coma_(cometary )

If I interpret wiki correctly, the coma (atmosphere) for a comet begins to form roughly corresponding to your calculation.
 
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Yes. I realize that, except for perhaps a black hole, there is no such thing as a perfect black body.
It's all right, I was just making sure I understood you before replying.
The others have done the answering since so...
 

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