Linearizing Stefan-Boltzmann equation

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SUMMARY

The discussion focuses on linearizing the Stefan-Boltzmann equation, represented as L=4πσ(R^2)(T^4), and the adiabatic relation TV^(γ-1) = constant. The goal is to derive the relationship δL/L(0) = (2δR/R(0)) + (4δT/T(0)). The solution involves applying a Taylor Expansion to approximate the terms involving small changes in radius and temperature, specifically using the expansion (a+x)^4 ≈ a^4(1 + 4x/a) for small x. Participants emphasize the importance of ensuring that the ratios remain small for the approximations to hold true.

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J_I_F
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Homework Statement


I want to linearize both the Stefan-Boltzmann equation and the adiabatic relation to draw a relationship between δL/L(0) and δR/R(0).


Homework Equations


Stefan-Boltzmann equation in the form of L=4πσ(R^2)(T^4)
Adiabatic relation TV^(γ-1) = constant


The Attempt at a Solution


I have L(0) + δL = 4πσ((R(0) + δR)^2)*((T(0) + δT)^4) for the S-B part, but don't know how to get it into this desired form:

δL/L(0) = (2δR/R(0)) + (4δT/T(0))
 
Last edited:
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J_I_F said:
I have L(0) + δL = 4πσ((R(0) + δR)^2)*((T(0) + δT)^4)

δL/L(0) = (2δR/R(0)) + (4δT/T(0))

So you have:

L_0+\delta L=4\pi\sigma(R_0+\delta R)^2(T_0+\delta T)^4

You will have to use a Taylor Expansion to expand the terms that can be considered very small. For example:

(a+x)^4=a^4(1+\frac{x}{a})^4 \approx a^4(1+\frac{4x}{a})

This only works when \frac{x}{a} is very small compared to 1, as is the case in your example. If you're still having trouble, show your work and we can go from there.
 
Last edited:
That helped a bunch, thanks.
 

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