How to calculate the time taken for the sun to cool down?

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Discussion Overview

The discussion revolves around calculating the time it would take for the sun to cool down if nuclear energy production were to suddenly stop. Participants explore various theoretical approaches and assumptions related to the sun's energy, temperature, and cooling mechanisms.

Discussion Character

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

Main Points Raised

  • One participant suggests calculating the total energy of the sun using the formula (3/2)NkT and then determining the time using luminosity.
  • Another participant proposes that the sun loses energy primarily through radiation and mentions using Wien's law to estimate the frequency of radiation at a given temperature.
  • A later reply indicates uncertainty about the application of Wien's law, as it has not been covered in their course yet.
  • One participant critiques the hypothetical scenario posed by the lecturer, noting the complexities involved in the sun's cooling process and the changes that would occur if nuclear fusion ceased.
  • Another participant mentions the Pauli exclusion principle and the eventual fate of the sun as a white dwarf, acknowledging the unrealistic nature of the scenario.
  • A participant introduces the Stefan-Boltzmann law to describe the power radiated by a blackbody and suggests setting up a differential equation to calculate cooling time, while also noting the complications in the sun's structure.
  • One participant expresses confusion regarding the temperature gradient within the sun.
  • Another participant advises that a 'reasonable' temperature can be chosen for calculations, emphasizing that the main focus is on the cooling process rather than the exact average temperature of the sun.

Areas of Agreement / Disagreement

Participants express various viewpoints and approaches to the problem, with no consensus reached on a specific method or solution. There are competing ideas regarding the assumptions and calculations necessary to estimate the cooling time of the sun.

Contextual Notes

Participants acknowledge limitations in their understanding of the sun's temperature distribution and the complexities of its internal processes, which may affect the accuracy of their calculations.

Baggio
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We're asked how long would it take for the sun to cool down if nuclear energy production suddenly came to a hault

This is the question asked in one of my lecture courses given that the radius of the sun is ~ 10^9m, mass ~ 10^30 kg, luminosity ~ 10^26, and G = 6.7x10^-11

Am i correct in assuming we just calculate the total energy of the sun using (3/2)NkT then using the luminosity calc the time?
 
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In that example, the only way for the sun to lose energy is to radiate it. Given the starting energy, you could approximate the frequency of the radiation at a given absolute temperature using Wien's law (qg) and from the frequency estimate the energy lost at that temperature. And then...
 
Oh i see,

I've learned Wien law before but in this particular course we haven't covered it yet, so i guess there must be another way of doing it.
 
Hmm, somewhat tricky, since your lecturer seems to be wanting you to follow a path that is quite unreal*, so you have to choose (guess?) the method she is fishing for! Perhaps it's 'just' "what is the instantaneous rate of cooling of a blackbody, of mass x, radius y, and temperature z?"

*a real Sun will undergo a very complicated set of changes if its internal fire were extinguished ... for a start, without that fire, the internal pressure which stabilised it against gravitational contraction would diminish rather quickly ... next, energy is transported from the core to the surface of stars principally by two mechanisms - radiative and convective; the balance between the two in real stars composed of varying mixtures of real matter isn't something to be solved with pencil and paper; ...
 
While it is impossible for fusion to cease in the core of the sun [given the amount of hydrogen and gravitational forces], I will suspend disbelief for a moment. The pauli exclusion limit would kick in and the sun still ends up as a white dwarf.
 
The Stefan-Boltzmann law gives the power radiated by a blackbody of temperature T:

[tex]P = \frac{dE}{dt} = \sigma A T^4[/tex]

If you knew how much thermal energy was in the Sun at a specific temperature, you could setup a differential equation to calculute the time it would take. The Sun's structure is quite complicated, and this relationship would be very difficult to find.

Perhaps you could get a reasonable approximation by just assuming a sphere of gas at uniform temperature (despite the fact that such a sphere is not in hydrostatic equilibrium), but I'm not even sure how you'd find the average temperature of the Sun!

- Warren
 
I know that's what was puzzeling me :-/ I didn't know what to do about the temp gradient
 
If you think the approach outlined by chroot is what your lecturer is looking for, then you are free to choose any 'reasonable' temperature (if you get it wrong, you may lose some points, but since the main thrust is how the Sun cools, not what it's 'average temperature' is, that shouldn't hurt too much). Clearly, the Sun's 'average temperature' is greater than that of its photosphere and less than that of its core ... how to pick something in between?

Of course, the Sun is *currently* radiating as if it were a spherical blackbody (radius x, temperature y) - well, 'sorta' - if you replaced it with a spherical blackbody of the same radius but a temperature of 10y (say), it would 'cool' an awful lot more quickly than it is now! :-p :rolleyes:
 

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