Photoelectric effect and kinetic energy

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The discussion centers on the photoelectric effect and why emitted electrons do not all share the same kinetic energy, even when exposed to a single wavelength of radiation. The work function (φ) of the metal defines the maximum energy threshold for electrons, but many occupy lower energy states, resulting in varied kinetic energies. The formula Ephoton = Φ + KEmax indicates that KEmax applies only to electrons with maximum energy within the potential well of the metal. Additionally, not all electrons at this maximum energy will achieve the highest kinetic energy due to the complex structure of the potential well. A minimum frequency of electromagnetic radiation is necessary to free an electron from the metal.
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hi
i have a small question:

how come not all emitted electrons have the same kinetic energy despite the radiation of only a single wavelength (that does cause emission of electrons) ?

thanks
 
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The energy structure of the electrons in the metal gives a maximum energy of -φ (the "work function") w.r.t the free state, but the electrons can occupy energy states below this threshhold, as well.
 
thanks for your reply

i don't want to be a troublesome person, but does it mean that the maximum kinetic energy that is calculated by the formula refers to free electrons, while others can occupy different energy levels and therefore have smaller kinetic energy?

thanks again
 
What formula?
 
Ephoton = Φ + KEmax


Ephoton = hf is energy of the photon.

Φ is the work function of the metal.

KEmax is the maximum kinetic energy of the ejected electrons .
 
OK, no. It means that the maximum kinetic energy refers to only those electrons that have a maximum energy "in the potential well of the metal". Actually, not even all of these electrons will obtain the maximum kinetic energy in your formula, because the potential well has some nontrivial structure. For your purposes, it is probably sufficient to realize that there is a minimum required EM radiation frequency to free an electron.
 
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