On pages 1 and 2 we briefly review the physical basis of chemical bonding. This discussion will not be on an exam because it is not in McMurry. Its purpose here is to introduce the principle that the energy of a molecule can be lower if the molecule adopts a geometry with a delocalized (spread-out) electron distribution. McMurry discusses this at several places in the text, especially in molecules with pi bonds.
In 1916, G. N. Lewis proposed that bonds are formed by electron pairs shared between two atoms, such that both atoms obey the Octet Rule. Bonds were represented either by two dots or a line. Today, bonds are shown as lines, and Lewis dots are used for lone pairs (nonbonding pairs).
Lewis structures for H_(2)\mathrm{H}_{2} and water:
Covalent bonding is a quantum phenomenon - it has no classical analog. Consider the H-H\mathrm{H}-\mathrm{H} bond in H_(2)\mathrm{H}_{2}. When two H atoms approach each other and their 1s orbitals overlap, a bond is formed. This means that the energy is lower when the nuclei are close together (but not too close), as shown in the graph. This energy lowering is the bond. The H-H bond is not a separate physical entity connecting the H atoms but is simply the low energy region of the energy-vs-distance curve at right.
But what makes the energy lower?
Classical and quantum effects combine to lower the energy in the bonding region. Coulomb's Law gives the classical electrostatic force between charged particles (like charges repel, opposite charges attract). Two quantum effects are needed to make a covalent bond. One is the Heisenberg uncertainty principle, Delta q Delta p >= ℏ//2\Delta q \Delta p \geq \hbar / 2, where Delta q\Delta q is the spatial extent of the electron density (uncertainty in electron position), Delta p\Delta p is the range of electron momenta, and ℏ\hbar is
Planck's constant divided by 2pi2 \pi. The size of the space in which electrons move ( Delta q\Delta q, orange regions) is larger in H_(2)\mathrm{H}_{2} than in an H atom. This implies that Delta p\Delta p is smaller in H_(2)\mathrm{H}_{2} than in an H atom. Bond formation creates a space in which the average electron momentum pp is lower. This reduces the electronic kinetic energy ( =p^(2)//2m=p^{2} / 2 m ). As a result, molecules prefer to adopt geometries in which the electron density is delocalized (spread out), because a low energy molecule is formed with higher probability than an isomeric high energy molecule.
Another quantum effect important for bonding is the Pauli exclusion principle, which states that no two electrons in an atom or molecule can have the same set of quantum numbers. For example, if two electrons occupy the same spatial orbital, they must have opposite spin. Because of this constraint on the electronic wavefunction, electrons can occupy all bonding molecular orbitals, not just the lowest energy orbital. As a result, molecules can adopt specific shapes, and bulk matter can occupy volume in space.
Octet Rule: A molecule is stable only if each atom shares 8 valence electrons.
Given the molecular formula, one can use the octet rule to deduce the bond connectivities in the molecule.
In arranging bonds and lone pairs to satisfy the octet rule, follow these electron-counting guidelines:
For a bond, each atom shares the electron pair. Both electrons are part of the octets of each atom.
Both electrons of a lone pair are assigned to a single atom.
Atomic orbitals
s p_(x)\mathbf{p}_{\mathbf{x}} p_(y)\mathbf{p}_{\mathbf{y}} p_(z)\mathrm{p}_{\mathrm{z}}
Hybridization addresses the following question:
If we know the geometry of a molecule, how can we understand the bonding?
Bonding requires overlap of adjacent atomic orbitals (AOs).
Hybridization creates unidirectional AOs for more efficient bonding.
To create acetylene on the xx axis with 180^(@)180^{\circ} bond angles, each carbon needs one p_(xx)AOp_{\times} A O mixed with an s AO (sp hybridization) as shown below. The ss and p_(xx)AOsp_{\times} A O s mix to give two sps p hybrid AOsA O s pointing in opposite directions ( 180^(@)180^{\circ} bond angle) along the xx axis.
On each carbon atom, s and p AOs mix to form a pair of sp hybrid AOs:
Carbon-carbon triple bond
Carbon s,p_(x)\mathrm{s}, \mathrm{p}_{\mathrm{x}} and p_(y)AOs\mathrm{p}_{\mathrm{y}} \mathrm{AOs} combine to form 3sp^(2)AOs3 \mathrm{sp}^{2} \mathrm{AOs} in the x-y\mathrm{x}-\mathrm{y} plane.
Side view
Top view
The pi\pi orbital is perpendicular to the sp^(2)sigma\mathrm{sp}^{2} \sigma framework
Carbon s,p_(x)p_(y),p_(z)\mathrm{s}, \mathrm{p}_{\mathrm{x}} \mathrm{p}_{\mathrm{y}}, \mathrm{p}_{\mathrm{z}} combine to form four sp^(3)\mathrm{sp}^{3} hybrid AOs with tetrahedral symmetry.
Predicting hybridization, given the bond connectivity
Count the number of atoms + lone pairs bound to an atom sp^(3)\mathrm{sp}^{3} atoms + lone pairs = 4
sp2 atoms + lone pairs = 3
sp 2 atoms
Every hybridized atom is associated with a bond angle, which is a measurable quantity. Hybridization is uniquely defined only for atoms bound to >= 2\geq 2 other atoms, which defines a bond angle. NH_(3)\mathrm{NH}_{3}
[NH]
N 3 atoms +1 lone pair sp^(3)\mathbf{s p}^{\mathbf{3}}