I Are continous Spectra actually discrete?

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The discussion centers on the nature of continuous spectra in relation to emitted photons from a charged particle spiraling towards another. It highlights the confusion between the continuous spectrum, which suggests an infinite range of frequencies, and the discrete nature of individual photons that can only produce photoelectrons above a certain threshold frequency. While the emitted spectrum is continuous, the actual number of photons and their distinct frequencies lead to a finite number of photoelectrons. The conversation clarifies that a continuous spectrum does not imply the presence of all frequencies at once, but rather that emitted photons can span a range of frequencies. Ultimately, the conclusion is that the spectrum produced is more accurately described as a line spectrum with closely spaced lines rather than a truly continuous spectrum.
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If we assume that there is a fixed charged particle and another charged particle is spiraling down towards it, it emits electromagnetic waves as it is accelerated motion. We get a continuous spectrum. Now, if I allow the emitted photons to fall on a very photosensitive material, whose efficiency is known, then i can get photo electrons for those photons whose frequency is beyond threshold frequency. By knowing the current, i can know the number of electrons and from number of electrons, i can calculate the number of incident photons by dividing the number of electrons by efficiency. As photons have a unique frequency, i can determine the number of frequencies the photon can assume between the range in which it can make an electron come out. So this means that i am getting discrete values. But the spectrum is continuous everywhere. So, that's my question. Where am I making a mistake?
 
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The "continuous spectrum" statement relates to a vast number of photons taken together. If you plot enough of their energies, you will get a smooth curve. But as you say, each photon on its own is just a data point in that plot with a distinct frequency and energy.
 
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I meant that if the spectrum is continuous, then I can get an infinite number of photons in any range of frequency. Let the frequencies in this range be more that the threshold frequency. As photoelectric effect is one photon one electron phenomenon, i must get infinite number of photo electrons (we make sure that the photo sensitive material remains neutral.) Also efficiency cannot be zero. So zero x infinity thing doesn't work. So that is where the problem is.
 
Continuous spectrum does not mean that at any given time, all frequencies are present. That would indeed mean infinite number of photons, which obviously isn't true.
Continuous here means that the photons that *do* get emitted can have any frequency in that spectrum.
 
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So actually the spectrum that I get from a charge spiraling inward is a line spectrum with the lines very close to each other. Will this solution work out?
 
Rohan Patil said:
So actually the spectrum that I get from a charge spiraling inward is a line spectrum with the lines very close to each other. Will this solution work out?

You'll get a finite number of photons but I wouldn't call this a "line spectrum" with the lines very close to one another. To me that implies a line spectrum implies spectral lines at certain energies, such as the spectral emission lines of a gases. If you were to perform this experiment over and over you would get photons of all frequencies from some lower range to some upper range.
 
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