The physical basis of splitting is a bit beyond the scope of the MCAT but it does help explain the n+1 rule. For all MCAT purposes, use the n+1 rule to determine the multiplicity. So how this arises is as follows. Each proton in the vicinity of the proton in question also has a magnetic field. That field is what splits the signal of the relevant proton. So to see a concrete example, let's start with a simple system: F2HC-CH2F. I'm going to call the proton on the left Ha and the proton on the right Hb for simplicity's sake. Let's focus on Ha. Ha will "feel" the magnetic field of the instrument. That's the basis of NMR. But it will also feel the magnetic fields of the vicinal protons. Those fields will be randomly oriented - it's a statistical system. So the magnetic fields of the Hb protons (there are two of them) can be either both aligned with the field of the instrument, both opposed to the field of the instrument, or one aligned with the field and one not. So in other words, let's say that the field of the instrument points up. The fields associated with the two Hb protons can be either: up-up, up-down, down-up, or down-down. That's a statistical distribution. Up-down and down-up of course give you the same observable effect. When both fields are aligned with the instrument's magnetic field, you get either shielding or deshielding. Again, the physical basis of this is more advanced and I don't want to get into it but you can see the end result. You get a three separate peaks, corresponding to the up-up, up-down/down-up, and down-down fields, in a 1:2:1 ratio. This is a triplet and this is why two vicinal protons will split a proton like Ha into a triplet. Now you can extend this to six protons as you see in this case and see that the same statistical argument applies - it's just a larger statistical distribution now.