| |
| |
where s is an s orbital on a particular nucleus and pi and pj are two p orbitals on the same nucleus pointing in arbitrary directions. |
where rho is the distance from electron to nucleus, and x is the coordinate in the direction of the p orbital. This can be any direction, not just the x, y, or z direction of some arbitrary cartesian coordinate system. The spwhatever hybrid orbital will point in the direction of this axis, the direction of its p orbital component.
Here's the constraint: the hybrids in use on any given center must be orthogonal to one another. Otherwise if both were occupied by two electrons, there would be too much electron density in one of their component orbitals (violating the Pauli Principle, which is an empirical statement of the way things always seem to be).
The hybrids are are said to be "orthogonal" when the integral of their product over all space is zero. Of course the integral of the product of sums is the sum of the integrals of products:
| |