An ion with the configuration \(\mathrm{f}^{2}\) enters an environment of octahedral symmetry. What terms arise in the free ion, and with which terms do they correlate in the complex? Hint. Follow the discussion of Section 8.9.

Short Answer

Expert verified
The terms that arise in the free \(\mathrm{f}^{2}\) ion are \(\mathrm{{^3F}}_{0}\), \(\mathrm{{^3F}}_{2}\), \(\mathrm{{^3F}}_{4}\), \(\mathrm{{^1G}}_{4}\), and \(\mathrm{{^1S}}_{0}\). In an octahedral complex, these terms correlate with \(\mathrm{{^3F}}\), \(\mathrm{{^1G}}\), and \(\mathrm{{^1S}}\) terms.

Step by step solution

01

Find Term Symbols in Free Ion

To start, consider an ion with the configuration \(\mathrm{f}^{2}\). This means there are two electrons in the 4f subshell. Using Hund’s rules, the term symbols for the two electron system can be found. Hund's rule states that: (1) the term with the largest multiplicity has the lowest energy. (2) For terms with the same multiplicity, the term with the largest value of L has the lowest energy. (3) For atoms with less than half-filled shells, the level with the smallest value of J lies lowest. For our \(\mathrm{f}^{2}\) configuration, only two electrons involved so we can easily identify the term symbols are \(\mathrm{{^3F}}_{0}\), \(\mathrm{{^3F}}_{2}\), \(\mathrm{{^3F}}_{4}\), \(\mathrm{{^1G}}_{4}\), and \(\mathrm{{^1S}}_{0}\). The superscript number indicates the spin multiplicity (2S+1), the letter denotes the total orbital momentum quantum number L, and the subscript value is the total angular momentum quantum number J.
02

Correlate the Terms in the Complex

Upon transition to an octahedral complex, the d orbitals split under octahedral symmetry. Because the f orbitals are radially further from the nucleus, they interact weakly with the field produced by ligands in an octahedral symmetry. Hence, there is no specific ligand field splitting diagram for f orbitals. However, in the octahedral crystal field, these terms are expected to split into more terms. The \(\mathrm{{^3F}}\) term in the free ion will correlate with the \(\mathrm{{^3F}}\) term in the complex, same for \(\mathrm{{^1G}}\) and \(\mathrm{{^1S}}\) terms.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Heterocyclic molecules may be incorporated into the Hückel scheme by modifying the Coulomb integral of the atom concerned and the resonance integrals to which it contributes. Consider pyridine, \(\mathrm{C}_{5} \mathrm{H}_{5} \mathrm{N}\) (symmetry group \(\left.C_{2 v}\right) .\) Construct and solve the Hückel secular determinant with \(\beta_{\mathrm{CC}} \approx \beta_{\mathrm{CN}} \approx \beta\) and \(\alpha_{\mathrm{N}}=\alpha_{\mathrm{C}}+^{1 / 2} \beta .\) Estimate the electron energy and the delocalization energy. Hint. The roots of the determinants are best found on a computer.

Predict the ground configuration of (a) CO, (b) NO. For each species, decide which term lies lowest in energy, compute the bond order and identify the HOMO and LUMO.

The allyl radical \(\mathrm{CH}_{2}=\mathrm{CHCH}_{2} \cdot\) is a conjugated \(\pi\) -system having a p-orbital on the carbon atom adjacent to a double bond. Estimate its \(\pi\) -electron energy by using the Hückel approximation.

Find the symmetry-adapted linear combinations of (a) \(\sigma\) -orbitals, (b) \(\pi\) -orbitals on the ligands of an octahedral complex. Hint. Set Cartesian axes on each ligand site, with \(z\) pointing towards the central ion, determine how the orbitals are transformed under the operations of the group \(\mathrm{O},\) and use the procedures for establishing symmetry-adapted orbitals as described in Chapter 5.

Use a minimal basis set for the \(\mathrm{M} \mathrm{O}\) description of the molecule \(\mathrm{H}_{2} \mathrm{O}\) to show that the secular determinant factorizes into \((1 \times 1),(2 \times 2),\) and \((3 \times 3)\) determinants. Set up the secular determinant, denoting the Coulomb integrals \(\alpha_{\mathrm{H}}, \alpha_{\mathrm{O}}^{\prime},\) and \(\alpha_{\mathrm{O}}\) for \(\mathrm{H} 1 \mathrm{s}, \mathrm{O} 2 \mathrm{s},\) and \(\mathrm{O} 2 \mathrm{p},\) respectively, and writing the \((\mathrm{O} 2 \mathrm{p}, \mathrm{H} 1 \mathrm{s})\) and \((\mathrm{O} 2 \mathrm{s}, \mathrm{H} 1 \mathrm{s})\) resonance integrals as \(\beta\) and \(\beta^{\prime},\) respectively. Neglect overlap. First, neglect the \(2 s\) -orbital, and find expressions for the energies of the molecular orbitals for a bond angle of \(90^{\circ}\).

See all solutions

Recommended explanations on Chemistry Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free