De Broglie wavelengths and electron diffraction

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Discussion Overview

The discussion revolves around the requirements for electron acceleration in diffraction experiments, specifically questioning why higher voltages (around 5kV) are necessary to observe distinct electron diffraction patterns, particularly in relation to de Broglie wavelengths and lattice spacings in materials like graphite.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants note that a de Broglie wavelength of approximately 1.2 x 10^-11m is achieved at 5kV, while the lattice spacing in graphite is about 2 x 10^-10m, raising questions about the necessity of such high voltage.
  • One participant calculates the electron momentum and kinetic energy required to achieve a de Broglie wavelength comparable to the lattice spacing, suggesting that 37.8eV electrons would be needed, thus questioning the sufficiency of a 50V supply.
  • Another participant references external resources indicating that the first interference peak for electrons striking nickel occurs at 54 volts, implying that lower voltages may not be effective for certain targets.
  • It is suggested that while diffraction may occur at lower speeds, the visibility of the diffraction pattern depends on the ratio of the de Broglie wavelength to the lattice spacing, with a preference for this ratio to be significantly less than one for observable patterns.
  • One participant mentions historical experiments by G. P. Thomson, noting that at lower electron speeds, the circular wave patterns were larger but suffered from decreased intensity and resolution, making them less usable.

Areas of Agreement / Disagreement

Participants express differing views on the necessity of high voltage for observing diffraction patterns, with some suggesting that lower voltages may suffice under certain conditions, while others emphasize the importance of achieving a suitable wavelength-to-spacing ratio for visibility.

Contextual Notes

There are unresolved assumptions regarding the relationship between electron energy, de Broglie wavelength, and observable diffraction patterns, as well as the specific conditions under which these phenomena can be effectively demonstrated.

DGriffiths
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I am interested to know why in any description of electron diffraction apparatus they seem to suggest that the electrons need accelerating up to 5kV (or at least several kV) to show the electron diffraction rings, this seems to give a de Broglie wavelength of around 1.2 x 10^-11m whereas the lattice spacing in a graphite target is of the order of 2 x 10^-10m

Now working back from this to get de Broglie wavelength similar to this lattice spacing gives electron momentum of 3.32 x 10^-24kgm/s, ke of 6.03 x 10^-18J and so we are talking 37.8eV electrons?

Why isn't a 50V supply enough then why the need for 5kV?
 
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DGriffiths said:
I am interested to know why in any description of electron diffraction apparatus they seem to suggest that the electrons need accelerating up to 5kV (or at least several kV) to show the electron diffraction rings, this seems to give a de Broglie wavelength of around 1.2 x 10^-11m whereas the lattice spacing in a graphite target is of the order of 2 x 10^-10m

Now working back from this to get de Broglie wavelength similar to this lattice spacing gives electron momentum of 3.32 x 10^-24kgm/s, ke of 6.03 x 10^-18J and so we are talking 37.8eV electrons?

Why isn't a 50V supply enough then why the need for 5kV?

Hello DGriffiths.
De Broglie wavelength=h/mv and eV=0.5mv^2.
From the above, wavelength=h/(2eVm)^0.5
I am wondering if you used an incorrect equation or made a mistake in your calculations somewhere.
 
Last edited by a moderator:
I don't think you can run a CRT at 50 V.

I suspect the 5kV isn't required for the diffraction itself, but to literally show the pattern.
 
Perhaps diffraction will take place at those speeds, but this is hardly observable. To actually generate a nice diffraction pattern you need the ratio \lambda / d to be small (and not of order 1). Here \lambda is the de Broglie wavelength and d the lattice spacing.

The reason is that the peaks with minimum intensity are positioned at angles \theta_n (as measured from the normal vector of the lattice)

\sin(\theta_n) = n\lambda / d

So if \lambda / d is of order 1, i.e. the two are of equal size, then the first minimum peak is at 90 degrees -- so you won't see a diffraction pattern at all. You will need the wavelength to be, preferably, a factor of 10 smaller. That way you can at least spot a couple of peaks of the diffraction pattern.
 
Yes, and from what I've read about the G. P. Thomson experiments, at slower electron speeds the circular wave pattern was larger but at a certain point the intensity and subsequent resolution dropped too low to be usable.
 
Thanks for all the replies folks, I didn't think about the ability to see a nice diffraction pattern being dependent on the correct lambda/d but that makes sense to me so cheers
 

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