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Oct 11 at 16:51 comment added Philip Wood Because if the emission is uniform across a band of wavelengths ($\lambda_2-\lambda_1$, say), the proportion of that power that will be emitted over a narrow band of width $\Delta \lambda$ somewhere between $\lambda_1$ and $\lambda_2$, will be $\frac {\Delta \lambda}{\lambda_2-\lambda_1}$, and if $\Delta \lambda$ is zero, that is for one discrete wavelength, the proportion of that power will be zero.
Oct 11 at 10:30 comment added Peter swift @PhilipWood "Because at that particular wavelength, no power will be emitted." But why is that, sir?
Mar 29, 2021 at 12:57 vote accept Harshit Rajput
Mar 29, 2021 at 12:53 comment added Philip Wood I've expanded the first bit of my answer.
Mar 29, 2021 at 12:52 history edited Philip Wood CC BY-SA 4.0
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Mar 29, 2021 at 12:45 comment added Harshit Rajput Actually I was looking for an answer to why we can't define power for a single wavelength.
Mar 29, 2021 at 12:43 comment added Philip Wood I don't think that any more detail is possible! I've looked through a few statistical mechanics textbooks, and they do seem to gloss over it. But it's implicit in the treatments of black body radiation given by Reif, Hill, Mandl, Huang...
Mar 29, 2021 at 12:21 comment added Harshit Rajput Found this really interesting. This wasn't mentioned in any of my graduation level books. Could you provide me any source in which this is discussed in detail?
Mar 29, 2021 at 12:02 history edited Philip Wood CC BY-SA 4.0
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Mar 29, 2021 at 11:54 history answered Philip Wood CC BY-SA 4.0