They're not even atomic orbitals at this point. The drawing of p-orbitals on the carbon skeleton represents the relative contribution of the atomic orbital on each respective carbon center to the (globally delocalized) molecular orbital for a particular energy eigenvalue. In this case only the sign/phase but not the magnitude (with the exception of the nodes) of the respective p-orbital is represented. This is somewhat misleading, but it's important to realize that the p-orbital drawings are just for bookkeeping: again, the electronic π structure does not involve p
z-orbitals any longer - each state has a single molecular orbital that is constructed from linear combinations of atomic p-orbitals.
It is true that in general the number of nodes scales with the energy of the molecular orbital, as this also correlates to the amount of "antibonding" character. It becomes a little complicated here because of the degeneracy of the high level energy states; the nodes (dashed lines) here are somewhat arbitrarily places. Note that because of the symmetry of the molecule you can effectively rotate the nodes anywhere you want. When a node passes through a carbon center, there is no p-orbital drawn because the p-atomic orbital on this carbon does not contribute to the molecular orbital (it's contribution is zero). This isn't a binary proposition, though - it's not zero or one. A better way to draw it would be to scale the size of the drawn p-orbital with the relative magnitude of the contribution, but this becomes even more confusing to people who don't really know what they're looking at.
The plus-minus just refers to the phase of the atomic-orbital contributions with respect to each other. If you consider a simpler molecule like ethene, there are two carbon atomic p orbitals that combine to form two molecular orbitals. Each p orbital has two lobes of opposite phase (which we call arbitrarily + and -). When the two carbons are brought together the respective p orbitals can match phases (+ lobes interacting with + lobes and - lobes interacting with - lobes) or match opposite phases. There is some mathematical formulation to this but it's basically the equivalence of constructive and destructive interference in wave interaction. Anyway, in the constructive combination you get a bonding orbital with no nodes and with the destructive combination you get an antibonding (higher energy) orbital with one node between the two carbon centers where there is no electron density. The node also marks a point where the phases change (the + and - of the molecular orbital switch positions).
See here for an example figure:
http://www.chem.ucalgary.ca/courses/350/Carey5th/Ch10/ch10-6-1.html What happens in larger molecules like the one you are asking about is basically the same thing, except you have more possible combinations (and usually fractional contributions) because you have more p-atomic orbitals involved.