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davidbenari said:thanks I think I've got it now. But this got me thinking: how can wavepackets produce electron diffraction? The only way I see electron diffraction occurring is if the wave is smeared out across a big space. It seems awkward to apply path difference formulas in a double slit experiment to a localised wave packet.
Is it correct if I say that electron diffraction only occurs when the momentum is really really well defined and the wave is non-localised? This makes sense I think.
The electron and the baseball are both wave packets, so both have some distribution in real space as well as some distribution in momentum or wavelength space. In some cases we model an object as having an exact location in real space (eg. the baseball), in other cases we model an object as having an exact location in wavelength space (eg. the electron for diffraction), but both are approximations because the wave packet is not exactly localized in either position or momentum space. That is the uncertainty principle. Which approximation you use depends on your application, and again you can estimate how good your approximation is via jtbell's exercise.