The shape of the orbital depends on many factors. The most important
are the quantum numbers associated with the particular energy state. These
are n, the principal quantum number, l, the oribital quantum
number, and m, the angular momentum quantum number. The following
table shows some of these shapes.
| n=1,l=0 | n=2,l=0 | n=2,l=1 | n=3,l=0 | n=3,l=1 | n=3,l=2 | n=4,l=0 | n=4,l=1 | n=4,l=2 | n=4,l=3 | |
| m=0 | ![]() |
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| m=1 | ![]() |
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| m=2 | ![]() |
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| m=3 | ![]() |
These shapes
continue on infinitely, getting ever more lobes or rings on them. Although
the l=0, m=0 orbitals look like simple spheres, regardless
of n value, this is not actually the case. To the right is a cutaway
of a 4s0 (n=4, l=0, m=0) oribital, showing that it
is really concentric spheres.
A note about the drawings: The blue color indicates a positive phase, while the orange color indicates a negative phase, with the phase taken as defined by Condon and Shortley. The colors become important when molecular orbitals are computed.
So far, all
of the pictures have been of electron orbitals associated with a single
atom. Molecules can become much more complicated. When two atoms are within
a certain proximity of each other, the orbital probabilities can either
reinforce each other or cancel each other out. If the phase is the same
sign (the same color), the probabilities are reinforced. To the right is
a picture of the bonding orbit for H2O (water).