Estimate the central temperature of the Sun

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SUMMARY

The discussion focuses on estimating the central temperature of the Sun using the integral of temperature and luminosity functions. The participant successfully calculated the solar luminosity as 3.87E26 W but encountered difficulties with the integration process, particularly regarding the behavior of luminosity L(r) within the Sun's core. Key insights include the need to define L(r) as a function that varies within the core and remains constant outside it, leading to a more accurate model for temperature estimation. The final suggestion emphasizes estimating the core radius and integrating accordingly to derive the central temperature.

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  • Understanding of thermodynamics and stellar physics
  • Familiarity with integral calculus and differential equations
  • Knowledge of solar luminosity and its implications
  • Concept of radiative transfer and mean free path in astrophysics
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Homework Statement


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Homework Equations





The Attempt at a Solution



I'm only stuck on part b). I make a) to be 3.87E26 W, but it gives that anyway in part b). OK, so here's my attempt:

\int_{r=0}^{r=R}dT(r)T(r)^3 = -\frac{3L(r)}{16\pi acl_{mfp}}\int_{r=0}^{r=R}dr\frac{1}{r^{2}}

\frac{T(r)^4}{4}|^{r=R}_{r=0} \sim \frac{T(r)^4_{centre}}{4}

\frac{T(r)^4_{centre}}{4}\sim-\frac{3L(r)}{16\pi acl_{mfp}}[-\frac{1}{r}]^{r=R}_{r=0}

OK, so am I on the right lines? If so, this is where I get stuck. The last bit of the R.H.S ends up having a 1/0 once evaluated. Any help would be great :). Also I wasn't sure about the L(r). Isn't the luminosity constant at all r? I guess L being a function of r suggests the contrary. :S
 

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The luminosity can't be constant at all r, because in the core energy is being produced. L(r) is the total power radiated from inside r, so it has to go to zero at r=0. You need to estimate the size of the core and make a guess at the functional form of L(r) inside the core, then you can assume L(r) is constant outside the core.
 
Ok I was initially under the impression that was the solution, but then why would the question supply me with the solar luminosity if I integrate over the functional form?
 
You still need to know the total luminosity, since this normalizes the functional form of L(r). Try setting up the problem and you'll see.
 
ok so after saying L(r)=4\pi r^2F_\odot

\frac{-T^4_{centre}}{4}=-\frac{3}{16\pi acl_{mfp}}\int_{r=0}^{r=R_\odot}dr\frac{4\pi r^2F_\odot}{r^2}

\frac{-T^4_{centre}}{4}=-\frac{3(4\pi R_\odot F_\odot)}{16\pi acl_{mfp}}

\frac{-T^4_{centre}}{4}=-\frac{3(\frac{L_\odot}{R_\odot})}{16\pi acl_{mfp}}

Is this right, or?
 
No. This assumes that L(r) increases steadily from r=0 to r=Rsun. In fact, only a small region in the core of the sun is generating energy, so you should try something like:

L = K * r^2 r < Rcore
L = Lsun Rcore < r < Rsun

You'll need to estimate Rcore, then calculate K, then integrate.
 

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