Understanding the Derivation of E=hf and its Significance in Quantum Physics

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Discussion Overview

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.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants note that E=hf was not derived in the strict sense, suggesting that energy could be related to electromagnetic field strength rather than frequency.
  • It is mentioned that assuming energy is not frequency-dependent leads to infinite energy output from a black body, which is deemed nonsensical.
  • Planck's introduction of quantization in the emission process is highlighted as a pivotal moment in resolving the issue of infinite energy output.
  • Einstein's later interpretation of the photoelectric effect is discussed, where he posits that photons of frequency f carry energy E=hf, independent of the emission process.
  • Participants inquire about the concept of "state counting" and its implications for energy calculations in black body radiation.
  • Mathematical details regarding the density of states and the equipartition theorem are presented as part of the classical treatment of black body radiation.
  • Clarifications are sought regarding the notation used in equations, specifically the meaning of proportionality indicated by the tilde (~).

Areas of Agreement / Disagreement

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.

Contextual Notes

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.

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?
 
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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. So Planck introduced the idea that the memission process of radiation from the atoms of a black body is quantized as E=hf, i.e. that a photon of frequency f must always carry a fixed amount of energy E=hf (he did not say that these photons must always come in these quanta, he only assumed this for the emission). In that way Planck was able to guess an energy density (per frequency) which interpolated between two known formulas, one for low and one for high frequency, and to obtain a finite result for the total energy emitted by the black body.

http://en.wikipedia.org/wiki/Black-body_radiation
http://en.wikipedia.org/wiki/Planck's_law

It was Einstein who assumed (a few years later) for the interpretation of the photoelectric effect that photons of frequency f always carry energy E=hf (and that this is not only due to a specific emission process). He was then able to explain the observed energy spectrum of the photo electrons which only depends on the frequency (not on the intensity of light, what would have been guess based on classical elecromagnetism).

http://en.wikipedia.org/wiki/Photoelectric_effect
 
I was about to ask exactly this questions..
I found derivatoin of E =mc^2, and de Broigle eq p = h/lambda, but not E = hf
 
the de broglie formula comes from E=pc=hf
 
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.

I was just reading through the forum.

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?
 
Do a Google search for "Rayleigh-Jeans law".
 
Jay_ 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?
You have to use two inputs
- density of states
- equipartion theorem

Suppose you black body is an empty cube; you have to calculate the number of electromagnetic waves fitting into the cube i.e. satisfying the boundary conditions. In three dimensions the density of states for a given freqency interval reads

N(\nu)\,d\nu \sim v^2\,d\nu

The classical treatment goes as follows
- calculate the average energy contained in each mode with a given frequency
- classical statistical physics says that for a system in thermal equilibrium the equipartition theorem applies
- therefore the average kinetic energy per d.o.f. is constant, i.e. ~ kT

So

\bar\epsilon_T(\nu) = kT

Together the average energy density for a given freqency interval reads

u_T(\nu)\,d\nu \sim \bar\epsilon_T(\nu)\, N(\nu)\,d\nu \sim kT\,v^2\,d\nu

The total power (= radiation energy per time) is calculated by integrating

P(T) = \int_0^\infty u_T(\nu)\,d\nu = \infty

Therefore the above mentioned assumpttions are wrong b/c a black body of finite temperature T and finite internal energy cannot produce infinite radiation power.

It was Planck who corrected the assumptions and "guessed" a different energy density. And it was Einstein how derived this energy density using the assumption of equilibrium of absorption + spontaneous emission + induced emission.
 
I don't understand the equations completely. What is the tilde '~' stand for? But thanks for your explanation :)
 
~ means proportionality i.e. neglecting irrelevant constants b/c in the end the difference between ∞ and const. times ∞ doesn't matter ;-)
 

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