holtto
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What is the derivation for E=hf and why did experimental observation of black bodies show that quantization of light was necessary?
The discussion revolves around the derivation of the equation E=hf and its significance in quantum physics, particularly in the context of black body radiation and the photoelectric effect. Participants explore theoretical aspects, historical context, and mathematical reasoning related to these concepts.
Participants express differing views on the derivation of E=hf and the implications of classical assumptions in black body radiation. There is no consensus on a singular derivation or interpretation, and the discussion remains unresolved regarding the foundational aspects of these concepts.
The discussion includes limitations related to assumptions made in classical physics, the dependence on definitions of energy, and the unresolved nature of certain mathematical steps in the derivation of energy density.
tom.stoer said:E=hf was not 'derived' in the strict sense. In back body radiation one could assume that energy of a certain mode with frequency f is not related to its frequency but to the electromagnetic field strength (squared). That would mean that a 'photon' of frequency f could carry an arbitrary energy E (like a classical electromagnetic wave where the energy has nothing to do with the frequency). Doing state counting that way one finds that the total energy emitted by a black body (of temeperature T) is infinite - which is nonsense.
You have to use two inputsJay_ said:Can you explain "state counting" in simple words? Let's say a photon does have energy proportional to its EMfield squared. How does that make its energy infinite?