Lindsayyyy said:
ok, thank you very much. I'm very uncertain about this subject. I just try different values. You asked beforehand how much higher the potential must be. I have a question about that. Why does tunneling happen in the first place? I haven't found anything about that. My wild guess would be that it's connected to the uncertainty principle but my imagination about it is very vague.
Yes, one could argue that the uncertainty principle plays a role. In tunneling problems, we are not typically dealing with localized particles. Rather, the wave-function of the particle is distributed in space - the uncertainty principle basically puts limits on how much the particle's wave function (or 'wave packet' for a more physical sounding description) can be spread out in space compared to the packet's momentum.
Slight digression - have you studied Fourier series and Fourier transforms? I ask because the uncertainty principle pops up in Fourier transforms. Basically, if you have a function of space, f(x), then the more concenrated the function is in space (i.e., the narrower the region for which f(x) is non-zero), the more spread out the Fourier transform of the function is in frequency space (where the spatial frequency is basically the momentum). Or, the narrower your function of space, the more wave packets of different frequencies (momenta) it is composed of. Similarly, a wide spread of a wave packet in space is composed of only a few waves of different momenta. We can also view this the other way around: if a wave packet has a very narrow spread in momentum, then it can be decomposed into wave packets that have large spatial distributions.
What does this mean in physical terms? Well, it means that if we have a wave-packet of an electron, for example, that we are firing at the wall, it has a fairly well defined momentum (there is a slight spread in the possible momentum values). This means that the spatial distribution of the wave packet is quite wide - wide enough, even, to extend beyond the barrier in front of the electron wave packet. This means that there is a chance that we can find an electron on the other side of a barrier, even though classically we would never expect to see it there.
Now, why is the universe like this? Well, no one really knows that for sure. We've just figured out the rules and compared our guesses to experiments, and the experiments agree.