Why is E = hf applicable to electrons with quantized energy?

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budafeet57
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I came across a problem my teacher assigned. We are asked to calculate frequency of electron having certain energy. My teacher used E = hf to solve the problem. I thought that could only be applied to photon. Is it because electron has wave-like nature and has quantized energy?
 
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Okay . You need to clear your fundamentals from your teacher.
E=hf. does not give the energy of electron. It gives the energy required / released when electrons change their energy levels. And this energy may be radiated in the form of photons or by heat or any other form.

I recommend you to go through Bohr's postulates regarding Atomic model.
 
The question is given like this:
electron has 511keV and kinetic energy of 100 MeV and determines its frequency.
the answer is 2.43*10^22 Hz, which can be determined through f = E/h.

I just wonder how can my teacher use the equation like that for such straightforward question.
 
budafeet57 said:
The question is given like this:
electron has 511keV and kinetic energy of 100 MeV and determines its frequency.
the answer is 2.43*10^22 Hz, which can be determined through f = E/h.

I just wonder how can my teacher use the equation like that for such straightforward question.
It's the frequency corresponding to the electron's De Broglie wavelength. E = 100.511 MeV, f = E/h.
 
E=hf is fine for describing the energy associated with a photon but I am not familiar with assigning frequency to energy for a particle. There is a relationship between wavelength (de Broglie) and momentum for particles (P=h/λ) but where does a constant relationship between Energy and Frequency for particles come in? Where would that leave the equation for waves 'c=fλ' for instance?
What am I missing here?
 
We can connect E = hf for an electron to the Schrödinger equation for matter waves by examining the time dependency of a stationary state.

[itex]| \Psi (t)> = e^{-iE_{n}t/\hbar}| n>[/itex]

Where |n> represents a stationary (stable) state at time zero, and En represents the energy of that state. Now, if we substitute into the above equation the following:

[itex]E_{n} = hf = \hbar \omega = \hbar 2\pi f[/itex]

Then, we'd get

[itex]| \Psi (t)> = e^{-i2\pi ft}| n >[/itex]

Notice that the exponential multiplying the stationary state has a frequency of magnitude [itex]f[/itex]. So the phase of a stationary state of a matter wave (from Schrödinger's equation) cycles at a frequency given by the energy of the state and the equation E = hf.
 
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