What we usually do here at the The Virtuosi is take an interesting problem, and work out the physical principles behind what we're seeing. Or pose a question and try to answer it. Now, I'm a big fan of this kind of thing, which is why I've done so much of it. But I worry that it might give a slightly skewed view of physics. Sure, physics explains things. That's why we do it. But not everything in physics is laser guns and solar sails. There are a lot of interesting physics phenomena that the general public will never hear about, because they're just too, well, esoteric. What I'm going to do is occasionally talk about such effects, and, for some of them, give you applications for these strange effects you might see on a day-to-day basis. Today I'm going to examine the Hall effect.
The Hall effect is simple, as these things go, once we understand the pieces. The first piece is that magnetic fields deflect moving electrically charged particles. I don't think I can give you a good simple reason for this, you're just going to have to trust me (for those interested, I'd argue that the relativistic transformation of a magnetic field is an electric field, and that will certainly deflect an electrically charged particle). This is a piece of the Lorentz force. The next piece that we need to know is that opposite electrically charged particles attract. So a positively charged particle attracts a negatively charged particle. Knowing those two things we can detail the Hall effect.
The Hall effect has some nifty consequences physically. I mentioned that conventionally we take current to be positive particles moving. A microscopic picture of our conductors will tell us that, in general, electrons are what we consider to be flowing in an electric current. Now, it turns out that our magnetic field will deflect electrons moving opposite our current direction (negative current moving backwards is the same as positive current moving forwards) to the same side as our hypothetical positive particles got deflected to. This generates a charge differential with negative and positive charges on the opposite sides of the slab (shown below), which means the voltage is negative what we would have measured above! This means we expect to get a certain sign of the measured Hall voltage, which we can predict. This sign would correspond to negative particles (electrons) being the moving charge carriers in substances. It turns out that there are some substances (some semiconductors) where the sign of the Hall voltage is opposite what we expect from electrons. This means that in those substances the current is being carried by positive particles! I won't explain what that means here (I may address that in a later post), but I hope you can see why that would be fascinating. We expected to have electrons moving, and it turns out that something else is really doing the moving. The Hall effect is an experimental result that helped suggest a whole new way of thinking about conduction in materials.