Estimate the dipole moment of the LiH molecule from the orbitals of Eq. (20.4-8):
ψ_{1σ}=ψ_{1sLi} (20.4-8a)
ψ_{2σ}=c_{2sp(1)Li}ψ_{2sp(1)Li} + c_{1sH}ψ_{1sH} =−0.47ψ_{2sp(1)Li }− 0.88ψ_{1sH} (20.4-8b)
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Estimate the dipole moment of the LiH molecule from the orbitals of Eq. (20.4-8):
ψ_{1σ}=ψ_{1sLi} (20.4-8a)
ψ_{2σ}=c_{2sp(1)Li}ψ_{2sp(1)Li} + c_{1sH}ψ_{1sH} =−0.47ψ_{2sp(1)Li }− 0.88ψ_{1sH} (20.4-8b)
The lithium nucleus has charge 3e . The two nonbonding electrons in the 1σ orbital contribute as though they were at the lithium nucleus. The probability density of an electron in the 2σ orbital is
\left|ψ_{2σ}\right|^{2} = (0.47)^{2}ψ^{2}_{2sp(1)Li}+(0.47)(0.88)ψ_{2sp(1)Li}ψ_{1sH} + (0.88)^{2}ψ^{2}_{1sH}We neglect the second term in this expression because it is appreciably nonzero only in the overlap region. The third term will make its contribution to the integral in Eq. (20.4-13):\left\langleμ\right\rangle =μ_{nuc} − e\sum\limits^{n_{e}}_{i=1}{\int{ψ_{i}(i)^{∗}r_{i}ψ_{i}(i)d^{3}r_{i} } } =μ_{nuc} − e\sum\limits^{n_{e}}_{i=1}{\int{r_{i}\left|ψ_{i}(i)\right|^{2}d^{3}r_{i}}} as though the electron were centered at the hydrogen nucleus. The 2sp(1) hybrid orbital does not have its center of charge exactly at the lithium nucleus, but we approximate the contribution of the first term as though it did. The net charge at the lithium nucleus is
Q_{Li} = 3e − 2e − 2(0.47)^{2}e = 0.56e = 8.9 × 10^{−20} CThe net charge at the hydrogen nucleus is
Q_{H}= e − 2(0.88)^{2}e = −0.56e= −8.9 × 10^{−20} Cwith a bond length of 1.595 × 10^{−10} m,
μ ≈ (8.9 × 10^{−20} C)(1.595 × 10^{−10} m) = 1.42 × 10^{−29}Cm = 4.3 Debye
This estimate of the dipole moment is about 60% as large as the value for a purely ionic bond, indicating a bond that is roughly 60% ionic in character. It agrees only roughly with the experimental value, 5.88 Debye.