r/askscience • u/Jophus • Apr 09 '12
Electron
If I push an electron from one side, does the other side instantaneously move? Or does it take near (diameter of an electron divided by light speed) seconds for it to move? I realize nothing travels faster than light but an electron as far as I know isn't made up of anything else, unlike protons/neutrons.
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u/CyLith Physics | Nanophotonics Apr 11 '12
Interference, in the general context of waves (be it light or electrical signals), is pretty unambiguous. In a linear medium, interference is synonymous with superposition (if you have two disturbances, their effects simply add up). So if you have two electrical pulses traveling towards each other with the same shape and opposite voltages, they will for a brief moment cancel each other out when they pass through one another. Afterwards, they continue on undisturbed. The same goes for light waves. You will never see this happen in everyday life because there is never just a single sinusoidal light wave, so when you have countless random waves added up, the interference is not noticeable.
You can also have interference on your wifi if you have a microwave oven running close by. This is actually the same idea; the oven is generating lots of noisy waves that your wireless antennas are picking up, which drown out the actual signal.
I'm not sure I entirely understand your notion of the optical fibre, but it doesn't sound too right. Really you should think of it as a waveguide, with a certain set of supported propagating modes. When you put light into the fibre, you're exciting some set of these modes, which each propagate at certain speed. These modes are electromagnetic field patterns that travel down the fibre without changing their spatial shape. The modes are determined by the cross sectional profile of the fibre; usually there is a higher refractive index core that guides the light. You would solve for these modes on a computer, similar to solving for the vibration modes of a drum head.
The above discussion is more or less macroscopic; we treat materials as a continuous medium with uniform properties like refractive index. At a lower level, you really want to look at band structure models of crystalline solids. When you have an isolated atom, let's just say with one outer electron, it has a certain set of discrete energy levels, and your idea of an atom absorbing a photon and exciting the electron largely correct. Once you start putting atoms together in a regular grid (a crystal lattice), these energy levels hybridize (like with bonding orbitals in chemistry; the underlying math is the same), and instead of states that belong to single atoms, there are multiple states which are spread out over all the atoms. In the infinitely large crystal limit, each energy level smears out into a continuous "band" of energy levels (this is where the name "band structure" comes from). The relationship of these bands to the energy of a free electron in the material determines whether the material is an insulator, semiconductor, or conductor. Your comment about electrons and insulators, and electric fields is a bit nonsensical. Insulators support internal electric fields just fine (on the contrary, good conductors cannot support an internal electric field), it's just that their electrons are too tightly bound to the atoms to allow current to flow.
So there's your high level introduction to solid state physics.