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Obtaining the Rayleigh-Jeans formula - what am I doing wrong?? |
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| Jan26-10, 09:41 PM | #1 |
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Obtaining the Rayleigh-Jeans formula - what am I doing wrong??
1. The problem statement, all variables and given/known data
Spectral energy density = [tex] u(\nu, T) = {\[\displaystyle \,8\,\pi \,h{\nu}^{3}{c}^{-3} \left( {{\rm e}^{{\frac {h\nu}{kT}}}}-1 \right) ^{-1}\]} [/tex] where h is Planck's constant and k is Bolzmann's constant. Using the relation [tex] \lambda = \frac{c}{\nu} [/tex] express the spectral energy density as a function of the wavelength and determine the energy du of a blackbody radiation per unit volume, in a narrow range of wavelength [tex] \lambda + d\lambda [/tex]. Using an expansion of the exponential factor obtain the Rayleigh-Jeans formula, [tex] du = \frac{8 \pi k T}{\lambda^4} d\lambda [/tex] 2. Relevant equations Given some function [tex] f(x_1, x_2, ..., x_n) [/tex], [tex] df = \left(\frac{\partial{f}}{\partial{x_1}}\right) dx_1 + ... + \left(\frac{\partial{f}}{\partial{x_n}}\right) dx_n [/tex]. Also, [tex] e^{x} \approx 1+x+\frac{x^2}{2!} + ... [/tex] 3. The attempt at a solution It seems like it should be easy, but I can't get the equation to come out right. Substituting in lambda, I get [tex]{\[\displaystyle {\it u}\, = \,8\,\pi \,h{\lambda}^{-3} \left( {{\rm e}^{{\frac {hc}{\lambda\,kT}}}}-1 \right) ^{-1}\]} [/tex] Then from my equation in part b, we should have that [tex] du = \frac{\partial{u}}{\partial{\lambda}} d\lambda [/tex] But I get [tex] \frac{\partial{u}}{\partial{\lambda}} = {\[\displaystyle \,-8\,\pi \,h \left( 3\,\lambda\,kT{{\rm e}^{{\frac {hc}{\lambda\,kT}}}}-3\,\lambda\,kT-hc{{\rm e}^{{\frac {hc}{\lambda\,kT}}}} \right) {\lambda}^{-5} \left( {{\rm e}^{{\frac {hc}{\lambda\,kT}}}}-1 \right) ^{-2}{k}^{-1}{T}^{-1}\]} [/tex] Upon using my expansion for the exp. term (expanding around nu = 0, then substituting in nu = c/lambda) the most I can simplify this is to: [tex] du ={\[\displaystyle \,8\,\pi \, \left( -2\,ckT+{\frac {h{c}^{2}}{\lambda}} \right) {\lambda}^{-3}{c}^{-2}\]}d\lambda [/tex] so... what am I doing wrong?? It could have something to do with the [tex] \lambda + d\lambda [/tex] (though I just thought that meant I could neglect higher than 2nd order terms in my expansion)... |
| Jan26-10, 10:46 PM | #2 |
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Recognitions:
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A quick check of the units of your original equation, [tex]u(\nu,T)=8h\pi\nu^3 c^{-3} \left(e^{\frac{h\nu}{kT} }-1\right)^{-1}[/tex] suggests that the problem lies there, not with your method.
If you are having doubts about whether or not using [itex]du=\frac{\partial u}{\partial\lambda}d\lambda[/itex] makes sense, another way to look at it is to realize that the spread in energy over the interval [itex]\lambda[/itex] to [itex]\lambda+ d\lambda[/itex] is defined as [itex]du=u(\lambda+d\lambda)-u(\lambda)[/itex]. And for infinitesimal [itex]d\lambda[/itex], a quick Taylor expansion gives [itex]u(\lambda+d\lambda)=u(\lambda)+\frac{\partial u}{\partial \lambda}d\lambda[/itex], from which the result follows. |
| Jan26-10, 10:50 PM | #3 |
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Interesting. This is an exam problem (from a previous year) at my school, so maybe the question has a typo. I can't see what else one would do to solve for this equation.
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| Jan26-10, 11:09 PM | #4 |
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Recognitions:
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Obtaining the Rayleigh-Jeans formula - what am I doing wrong??
I must apologize, I was thinking [itex]u[/itex] was just an energy density (units of Joules/m3), not a spectral energy density. Your original equation is just fine. However, you can't simply substitute [itex]\nu=\frac{c}{\lambda}[/itex] into your frequency spectral energy density equation and get a wavelength spectral energy density out of it.
In terms of frequency, the spectral energy density has units of Joule-seconds/m3. While in terms of wavelength, the spectral energy density has units of Joules/m4. The first is defined as an energy density per unit frequency, while the latter is defined as an energy density per unit wavelength. For this reason, [itex]u(\lambda,T)d\lambda=u(\nu,T)d\nu[/itex]. Or, [itex]u(\lambda,T)=u(\nu,T)\frac{d\nu}{d\lambda}=u(\nu,T)\times\frac{-c}{\lambda^2}[/itex] |
| Jul2-11, 12:47 AM | #5 |
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When we substitute d[itex]\nu[/itex]/d[itex]\lambda[/itex] = - c / [itex]\lambda[/itex]^2 in Plancks law of Black body radiation (in frequency), we would get an equation that is same as Plancks law of black body radiation (in wavelength) EXCEPT for a negative sign.
Because it is an ENERGY equation, the negative sign would be omitted. Is this correct |
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