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Chemistry · Lesson

Clusters, extended structures and unusual bonding

Extend ordinary pair-bond thinking to bridges, cages and periodic solids. Use restricted electron counts and a three-site orbital toy without treating a topological edge, close contact or model population as a measured localized bond.

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By the end, you can

  • Explain why diborane’s contacts cannot all be ordinary two-center pair bonds.
  • Count terminal and skeletal electrons in a selected closo borane.
  • Apply fractional unit-cell shares in conventional rock salt.
  • Read a restricted three-orbital four-electron model with its assumptions intact.
01

A three-center bridge is not two independent pair bonds

Diborane B₂H₆ has 2× 3+6× 1=12 valence electrons. Its selected bonding description uses four terminal ordinary B–H pair bonds, consuming eight electrons, and two bridging B–H–B three-center/two-electron units, consuming four. Each bridge shares one pair over three centers.

Counting all eight B–H contacts as independent two-center/two-electron bonds would demand 16 electrons, more than the available 12. A contact count is therefore not a localized pair-bond count. These bridges are not automatically ordinary intermolecular hydrogen bonds. The electron-allocation model itself gives no measured geometry, partial charges or individual bond-order value.

02

Terminal and skeletal electron pools are separate

For the simple closo borane B₆H₆²⁻, total valence electrons are 6× 3+6× 1+2=26. Six terminal B–H pairs use 12, leaving 14 skeletal electrons, or seven pairs. In this restricted borane class, the closo count is n+1 skeletal pairs for n vertices; n=6 gives seven, consistent with the selected octahedral closed cage.

An octahedral graph has six vertices, twelve edges and eight triangular faces. Its twelve drawn edges do not mean twelve independently localized two-center pair bonds. Nor does this cage have the same bridging-H arrangement as diborane: the selected B₆H₆²⁻ has terminal hydrogens. More general clusters require their own electron-count conventions, not automatic application of this restricted rule.

03

A conventional unit cell counts shares rather than molecules

For conventional cubic rock salt, represent chloride at eight corners and six faces, sodium at twelve edges and the body center. Periodic sharing gives chloride count 8×(1/8)+6×(1/2)=4, sodium count 12×(1/4)+1=4. The cell thus contains four NaCl formula units and net charge zero under Na⁺/Cl⁻ assignments.

Each ion has six opposite-ion neighbors in this stated phase, including neighbors across cell boundaries. The unit cell is not an isolated Na₄Cl₄ molecule, and coordination count differs from formula ratio. No lattice length, radius or rule that every one-to-one salt must adopt rock salt follows from this count.

04

Three sites can give bonding, nonbonding and antibonding combinations

For an original equal-site open-chain toy, use an orthonormal three-site basis and matrix rows (0,−1,0), (−1,0,−1) and (0,−1,0) in arbitrary energy units. Diagonal energies are all zero; adjacent couplings are equal and nonadjacent coupling is zero. Eigenvalues are −√2, 0 and +√2.

Normalized eigenvectors can be written (1/2,1/√2,1/2), (1/√2,0,−1/√2) and (1/2,−1/√2,1/2). Four independent electrons occupy the lower and middle levels with two each, leaving the upper level empty. The middle combination has zero coefficient at the central site. Summing occupied squared coefficients gives toy site populations 1.5, 1 and 1.5, conserving four electrons.

This is an illustrative three-center/four-electron orbital pool, not a complete real molecule. XeF₂ is heteronuclear and has other orbitals, overlap, correlation and ionic contributions. The equal-site toy does not predict its actual population charges, energies, distances or bond strengths. An expanded Lewis drawing is not evidence that literal d-orbital hybridization is required.

Restricted three-site orbital energy levels with four electrons

Toy eigenvalue / arbitrary energy units

Original equal-site open-chain matrix with zero diagonal entries, adjacent coupling −1 and an orthonormal basis. Four independent electrons occupy the lower and middle levels with two electrons each; the upper level is empty. Horizontal index labels the three ordered combinations, not time or geometry. Energies are arbitrary model units, not measured XeF₂ orbital levels or the energy of a complete molecule.123-1.6-0.800.81.6

Ordered orbital combination index

  • Occupied: two electrons each
  • Unoccupied
Underlying data
Ordered orbital combination indexToy eigenvalue / arbitrary energy units
1-1.4142135623730951 · Occupied: two electrons each
20 · Occupied: two electrons each
31.4142135623730951 · Unoccupied

Original equal-site open-chain matrix with zero diagonal entries, adjacent coupling −1 and an orthonormal basis. Four independent electrons occupy the lower and middle levels with two electrons each; the upper level is empty. Horizontal index labels the three ordered combinations, not time or geometry. Energies are arbitrary model units, not measured XeF₂ orbital levels or the energy of a complete molecule.

05

Choose a representation that answers the stated question

Ordinary pair ledgers, multicenter descriptions, skeletal counting, periodic composition and orbital models each expose different constraints. A graph can record connectivity; a cage edge records topology; an electron count records a chosen pool. None should be silently substituted for the others.

Assess the question, phase and evidence before extending a familiar model. Actual unusual bonding needs structural and electronic support. The examples here establish internally consistent constrained descriptions, with the real-system limits kept beside their calculations.

Worked examples

Count pair units rather than contacts

Use B₂H₆ with four terminal bonds and two selected three-center bridges.

  1. Total electrons = 2× 3 + 6 = 12.
  2. Terminal pairs use 4× 2=8; bridge pairs use 2× 2=4.
  3. Eight independent two-center contact pairs would instead demand 16.

The selected multicenter allocation uses the available 12 electrons; contact count alone overcounts pair bonds.

Subtract the terminal pair pool first

Use B₆H₆²⁻ with six terminal B–H pairs.

  1. Total valence electrons = 6× 3 + 6 + 2 = 26.
  2. Terminal pool = 6× 2 = 12.
  3. Skeletal pool = 26−12 = 14 electrons, or seven pairs.
  4. For this simple closo class, n+1 = 6+1 = 7 pairs.

Consistent with the selected six-vertex octahedral cage, without assigning one localized pair to every edge.

Count periodic shares in conventional rock salt

Use the stated corner/face chloride and edge/body sodium sites.

  1. Cl count = 8/8 + 6/2 = 4.
  2. Na count = 12/4 + 1 = 4.
  3. Assigned charge sum = 4×(+1)+4×(−1)=0.

Four NaCl formula units per stated conventional cell, rather than an isolated molecule.

Check the occupied coefficients against the electron total

Fill the lower and middle toy eigenvectors with two electrons each.

  1. End site population = 2×(1/2)² + 2×(1/√2)² = 1.5.
  2. Center population = 2×(1/√2)² + 2× 0² = 1.0.
  3. Other end is 1.5; total = 4.0.
  4. Occupied toy energy sum = 2×(−√2) + 2× 0 = −2√2.

Conserved four-electron pool and arbitrary occupied energy −2.82843 units; not actual atom charges or a complete molecular energy.

Try it yourself

  1. Does one B–H–B three-center/two-electron bridge contain two independent ordinary pair bonds?

    Show the answer and reasoning

    No.

    Its one pair is shared across three centers in the selected description.

  2. In the same simple B₆H₆²⁻ closo ledger, subtract six terminal B–H pairs from 26 total valence electrons. What remains?

    Show the answer and reasoning

    14 skeletal electrons, or seven pairs.

    26−6× 2=14, and 14/2=7=n+1 for n=6 in the restricted cluster class; cage edges do not count localized pairs.

  3. For the stated four-electron three-site toy, both occupied eigenvectors have central coefficients 1/√2 and 0. Find the central site population.

    Show the answer and reasoning

    1.0 electron in the stipulated basis-population model.

    Two electrons per occupied orbital give 2(1/√2)²+2× 0²=1. This is a toy basis population, not a real molecular atomic charge.

  4. Do equal-site toy populations 1.5,1,1.5 predict real XeF₂ atomic charges?

    Show the answer and reasoning

    No.

    The heteronuclear molecule and its full electronic structure are outside the equal-site model.

What to carry forward

  • Distinguish contacts from independent pair bonds.
  • Separate terminal and skeletal electrons in the stated cluster class.
  • Use fractional shares for periodic composition.
  • Keep orbital-pool assumptions visible.
  • Do not turn a representation into unmeasured real-system properties.

References

Teaching resources and reference material supporting this lesson’s explanations and examples.

  1. Andrew R. Barron; Rice University author content via CNX/LibreTexts2 sources
    1. Boron HydridesAndrew R. Barron; Rice University author content via CNX/LibreTextsSourcechem.libretexts.orgRead source
    2. Wade’s RulesAndrew R. Barron; Rice University author content via CNX/LibreTextsSourcechem.libretexts.orgRead source
  2. Main group elements of2nd and3rd periods and their compoundsTaro Saito; author content, attributed Kanagawa University, hosted via LibreTextsSourcechem.libretexts.orgRead source
  3. Lattice Structures in Crystalline SolidsPaul Flowers; Klaus Theopold; Richard Langley; William R. RobinsonSourceopenstax.orgRead source
  4. Identification of a Simplest Hypervalent Hydrogen Fluoride Anion in Solid ArgonMeng-Chen Liu; Hui-Fen Chen; Chih-Hao Chin; Tzu-Ping Huang; Yu-Jung Chen; Yu-Jong WuSourcenature.comRead source