How to Estimate Energy Density Using Planck's Law?

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To estimate the energy density emitted by a blackbody at 2000 K between 499.5 and 499.6 nm using Planck's Law, one must integrate the law with the appropriate substitutions. The substitution x = hc/(KλT) is necessary, and the limits of integration should be adjusted accordingly for the given wavelengths. Given the close proximity of the wavelengths, an approximation using the integral formula is suggested. This approach allows for a simplified calculation of the energy density in that narrow range. The discussion emphasizes the need for numerical methods to solve the integral effectively.
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Homework Statement



Estimate the energy density between 499.5 and 499.6 nm emitted by a blackbody at a temperature of 2000 K. Compare to the classical value predicted by the Rayleigh-Jeans law.

Homework Equations



http://en.wikipedia.org/wiki/Planck's_law

The Attempt at a Solution



now I know how to integrate the indefinite integral of the law by setting x = \frac{hc}{KλT} (K = Boltzmann constant)

T = 2000K is substituted in and we use the same substitution for λ^5 of the equation.

However I do not understand how to numerically solve this with λ = 499.5 to 499.6, would we then substitute it to x = \frac{hc}{KλT} and make x the new limits of integration?
 
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The fact that the wavelengths you are given are so close together suggests to me you just need to approximate the integral using

$$\int_{\lambda}^{\lambda+\Delta \lambda} d\lambda'~f(\lambda') \approx \Delta \lambda f(\lambda).$$
 

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