Say what it encloses.

An orbital picture is not a picture of a cloud. It is a contour — the surface on which the wavefunction takes one chosen value — and the value was chosen by whoever drew it. "The ninety per cent surface" is the stock phrase and very often not what has been plotted, because nobody did the integral. These are essays about molecular shape and bonding with the integrals done: every orbital here is drawn at a level found by integrating the density, and says what fraction it encloses.

The 2pz orbital. The 2pz orbital at the contour enclosing 90 per cent of its density — a level solved for by integration rather than chosen. The two colours are the two signs of the wavefunction, which is what distinguishes a bonding interaction from an antibonding one. Contours drawn: 2pz at 90% of its density, |ψ| = 9.48e-3.
Fig. 1 A 2p orbital at the contour enclosing ninety per cent of its density — a level solved for rather than picked. The two lobes are drawn in different colours because they differ in the sign of the wavefunction, which is the whole of what makes one interaction bonding and another antibonding, and a picture of the magnitude alone has thrown it away.

430 essays · 9 fields · 31 series · 366 named objects · every figure computed from its model

The parts of the subject

9 fields — what each one is for

Orbitals

A one-electron wavefunction, drawn as a contour surface at a level somebody chose. Nodes, signs, and what the picture is a picture of.

48 essays · begins at What an orbital is

Where the atoms go

VSEPR as a repulsion minimisation rather than a table, the angles that fall out of it, and the case where five sites are not all alike.

47 essays · begins at VSEPR, computed

Bonding models

Valence bond, molecular orbital, and hybrids — three descriptions of one thing, related by transformations that change no observable.

48 essays · begins at Overlap decides

What symmetry decides

A molecule's point group follows from its coordinates, and it settles whether the molecule can be polar or chiral with no reference to bonding.

47 essays · begins at Point groups from coordinates

Beyond the octet

Hypervalency without d orbitals, delocalisation, aromaticity, and the structures the first-year rules quietly cannot describe.

48 essays · begins at Hypervalency without d orbitals

What a spectrum settles

A spectrum is a list of positions, and how many there can be is decided by the shape before any of them is measured. Counting them, and reading a structure back out.

48 essays · begins at Normal modes are not bond stretches

When the molecule does not stop

A chain of two hundred atoms is a molecule and behaves like a solid. Bands, gaps, metals, defects and surfaces, every one of them out of a finite matrix — and a clear account of what that route cannot reach.

48 essays · begins at A solid is a molecule that did not stop

What the shape is for

Coordination compounds, where the shape decides a colour, a magnetic moment and a bond length — and where the one-electron picture used everywhere else in the collection stops being enough.

48 essays · begins at The splitting is a symmetry statement

What is taught wrongly

The explanations that are confident, memorable and false — stated fairly and then tested against a calculation rather than an opinion.

48 essays · begins at Hybridisation does not explain

How far each idea goes

31 series — every one of them

Representation

A molecule's point group is a list of matrices, not a label. Generating them, sorting them into classes, and dividing by the group order turns any set...

21 essays, in order of depth

Contour

An orbital picture is a contour at a level somebody chose, and almost no source says which. Two textbooks can draw the same orbital at visibly...

19 essays, in order of depth

Basis

Sixty years of molecular calculation are built on functions that get the two ends of an orbital wrong. A Gaussian has no cusp at the nucleus and dies...

16 essays, in order of depth

Hypervalency

Sulfur hexafluoride is not d²sp³ hybridised. The d orbitals are far too high in energy to contribute meaningfully, the bonding is three-centre...

16 essays, in order of depth

Magnetism

A magnetic moment is one of the few chemical measurements that returns an integer. Feed the count of unpaired electrons into √(n(n+2)) and nine...

16 essays, in order of depth

Multicentre

A bond between two atoms is a special case, not the general one. Rings, clusters and metals are held together by orbitals spread over many centres,...

16 essays, in order of depth

Point group

A molecule's symmetry is not a label to be looked up. It is decidable from the atom positions by searching for the operations that permute them, and...

16 essays, in order of depth

Delocalisation

Benzene does not alternate between two structures. It has one structure, and the two Kekulé forms are basis functions in a description of it — which...

15 essays, in order of depth

Threads running through

themes, not chapters

Say what it encloses

An orbital picture is a contour at a level somebody chose, and almost no source says which. Every one here is drawn at a level found by integrating the density, and states the fraction it encloses.

19 essays

Exactly zero

Where symmetry forbids an interaction the overlap is not small, it is zero. Computing it and finding arithmetic noise is a different kind of statement from computing it and finding a small number.

78 essays

A basis is not a thing

Hybrid orbitals, localised bonds and canonical molecular orbitals are related by transformations that leave every observable unchanged. Arguing about which is real is arguing about a coordinate system.

101 essays

Symmetry settles it

Whether a molecule can have a dipole, or be chiral, or show a particular spectral line, follows from its point group alone — with no reference to what the bonds are made of.

139 essays

One electron only

Every orbital drawn here is a hydrogen-like solution. A many-electron atom has no exact orbitals at all, and keeping that in view is the difference between a model and a picture of reality.

156 essays

Taught confidently, and wrong

This subject has an unusual number of explanations that are memorable, widespread and false. Each is stated fairly here and then tested against a computation rather than an opinion.

246 essays

Measured from somewhere

A great many numbers in this subject are differences, fits or projections: a resonance energy against a reference state, a mode's percentage composition in a set of coordinates, a structure's weight under a convention, a moment from a fitted law. Each is quoted as though it were measured, and each changes when the choice behind it changes.

140 essays

What the measurement does not fix

A spectrum with two lines in it constrains two numbers, and a model with three parameters fitted to it has a curve of answers rather than an answer. These essays are about measurements that leave a family of possibilities standing — and about what it takes to tell the members of the family apart.

155 essays

Counted, not quoted

Node counts, bond angles, overlap integrals and point groups are all computed from the geometry and the wavefunctions themselves. None of them is a number recalled from a table.

419 essays

Just written

the most recent — what arrived when

The consecutive triples fail for a uniform chain at every length. The share of three decades of accuracy line over which some basis size is usable, against the number of fragments from three to eight, for three arrangements and three ways of assembling the correction. On the uniform chain the consecutive-triple assembly covers less than pairs alone at every length from four, and the shortfall grows. On the heavy-inside chain it covers exactly what every triple covers. On the heavy-outside chain it covers more than every triple from five fragments on. Orbitals

Length did not rescue the consecutive triples

On four fragments, keeping only the consecutive triples of a counterpoise assembly worked for two arrangements and did worse than pairs for the uniform chain, and a short chain was the obvious excuse. Carried to eight fragments the excuse fails: the uniform chain's consecutive assembly settles at 48 per cent of the line against 68 for pairs. And the heavy-outside chain turns the lesson over — from five fragments every triple together covers less than the consecutive ones alone.

6 figures
The zero at π/R follows parity, not bonding. The bonding and antibonding combinations of three atomic functions on nitrogen, each along the bond and each normalised to its own largest value, against momentum in units of π/R. For 2s the bonding combination is zero at π/R and the antibonding one is not. For 2p along the bond it is the other way round: the σ bond carries a sine, is zero at the origin and near its largest at π/R, and the antibonding combination carries the cosine. For 2p across the bond the π bond carries the cosine again. The factor is a cosine exactly when the orbital's inversion parity matches the atomic function's. Orbitals

The zero is a parity, not a bond

A hydrogen-like σ bond has a momentum profile along its axis that vanishes at π/R, and it is natural to read that zero as a bond's signature. Built from 2p functions pointing along the axis, the σ bond carries a sine instead and sits at 83 per cent of its peak there. Which factor an orbital carries is decided by whether its inversion parity matches its atom's, and bonding has nothing to do with it.

6 figures
Folding the ring off its plane never gives the orbital back. For rings of four to eight ligands round a centre with no lone pair, the orphan count minus the formula n + L − 4, at polar angles from 60° to 120°. The upper dot in each row is the bare ring and the lower the same ring with a ligand on the axis. The bare ring is one over the formula at every angle, including 90°, where the ring is flat and its group is D₄ₕ, D₅ₕ or D₆ₕ; there is no table here for D₇ₕ or D₈ₕ. The capped ring agrees with the formula at every angle, 90° included, where the ring is exactly flat and the apex alone keeps its group C₄ᵥ to C₈ᵥ. Beyond the octet

Folding the ring does not give the orbital back

Three arrangements break the orphan count n + L − 4, all flat, and the reason given was flatness: the p orbital perpendicular to the ring has no ligand combination of its species. Fold the ring into an umbrella at any angle and that orbital becomes totally symmetric — and the count stays wrong by exactly one, for rings of four to eight. The ring offers one symmetric combination to a centre with two symmetric orbitals. Writing C₅ᵥ to see it also counts the pentagonal pyramid at last, and the formula holds there.

6 figures
An antibonding occupation fills the zero and moves the minimum. The profile along the bond near π/R, per electron, on a logarithmic scale, for five antibonding occupations of the same two orbitals. With nothing in the antibonding orbital the profile is exactly zero at π/R = 1.573. Two hundredths of an electron leave a minimum at 1.608, which reads the separation as 1.954 bohr instead of 1.997. At 0.104 the minimum becomes a flat shoulder, and the Heitler–London bond, at 0.236, has none. Orbitals

The zero belongs to one determinant

A bonding orbital's momentum profile along the bond is exactly zero at π/R, and that zero reads a bond length with nothing fitted. It is a property of putting every electron into that one orbital. Any antibonding occupation fills it in linearly and drags the minimum outward, a tenth of an electron erases it, and the valence-bond wavefunction built from the same two functions never has one at any separation.

7 figures
A long bond goes axial at five and equatorial at seven. The energy of the odd site placed axially minus placed equatorially, against the odd bond's length relative to the others, for the trigonal bipyramid and the pentagonal bipyramid. Above zero the equatorial site is preferred. At five a longer bond goes axial and a shorter one equatorial; at seven, from 0.7 to 1.3, every sign is reversed — a shorter bond axial, a longer one equatorial. An open marker is a placement that is not a minimum: at seven the site each bond avoids is one it would slide out of. Where the atoms go

The long bond goes to the crowded site

Given one bond longer than the others, the repulsion model puts it axial in a trigonal bipyramid — against the rule it is usually cited for. The reason is a crowding count, and at seven sites the count reverses: the pentagonal bipyramid's crowded site is equatorial, so a long bond goes equatorial and a short one axial. PF₅'s long bonds are axial and IF₇'s are equatorial. And at seven the site a bond avoids is not even a minimum.

6 figures
Angular rings leave the heteroatom's own ring alone and scale the rest. Each ring's response as a fraction of the straight chain's, with the heteroatom on ring 0 and the first one, two, four or ten interior rings angularly fused, on a logarithmic axis. The heteroatom's ring stays within one and a half per cent in every case. The rings beyond the angular fusions fall, to under half by the third ring once two are angular, and to between an eighth and a third along the fully angular chain, alternating from ring to ring. Beyond the octet

An angular ring rescales what lies beyond it

A heteroatom's influence along a chain of fused rings decays with a length near 0.7 rings, and one bend was found to change almost nothing. Counted properly, that bend was two angular rings, and counting angular rings one at a time shows what they do: the heteroatom's own ring never moves by more than one and a half per cent, the rings beyond angular fusions fall to between an eighth and a half of their response — or rise by up to two fifths — and the decay length changes by a tenth.

6 figures