Derive two additional mutually orthogonal hybrid orbitals for the lone pairs
on oxygen in \(\mathrm{H}_{2} \mathrm{O}\), each of which is orthogonal to
\(\psi_{a}\) and \(\psi_{b},\) by following these steps:
a. Starting with the following formulas for the lone pair orbitals
$$\begin{array}{l}\psi_{c}=d_{1} \phi_{2 p_{z}}+d_{2} \phi_{2 p_{y}}+d_{3}
\phi_{2 s}+d_{4} \phi_{2 p_{x}} \\
\psi_{d}=d_{5} \phi_{2 p_{z}}+d_{6} \phi_{2 p_{y}}+d_{7} \phi_{2 s}+d_{8}
\phi_{2 p_{x}}
\end{array}$$
use symmetry conditions to determine \(d_{2}\) and \(d_{4}\) and to determine the
ratio of \(d_{3}\) to \(d_{7}\) and of \(d_{4}\) to \(d_{8}\)
b. Use the condition that the sum of the square of the coefficients over all
the hybrid orbitals and lone pair orbitals is 1 to determine the unknown
coefficients.