Computational Chemistry
What a computed number means, and when to disbelieve it
About this course
Computing chemistry on the potential energy surface — geometry optimisation, force fields and molecular dynamics, free energy, Hartree-Fock, correlated methods and DFT, solvation, docking and machine-learned potentials, judged against benchmarks.
What you will be able to do
- Locate minima and transition states on a potential energy surface and verify them
- Explain why only energy differences are meaningful, and use error cancellation deliberately
- Run and interpret force-field molecular dynamics and free-energy calculations
- Choose a wavefunction method, basis set and functional, and state the errors each introduces
- Assess solvation models, docking scores and machine-learned potentials against benchmarks
What this course covers
- The central thesis: model's question vs. yours
- The potential energy surface as a construct
- The Born-Oppenheimer bargain and its expiry
- The dimensionality problem: surfaces that cannot be mapped
- Why the field is tractable: soft coordinates and error cancellation
- Precision vs. accuracy in computed numbers; method spread is not an error bar
- Restraints as part of the surface, not a view of it
- Practical checklist for evaluating a computed number
- Force field parameter space and the rules-vs-data reality
- Force field functional form and its deliberate absences
- Coverage signalling: MMFF refusal vs UFF generation
- The silent MMFF-to-UFF fallback and its logging fix
- Conformer disagreement and hydrogen-bonding molecules
- Fitted methods have no self-uncertainty term — the central result
- The continuum solvation trade-off
- Born's formula and the continuum model structure
- Dielectric saturation of the continuum model
- Cavity radius sensitivity and the 13-to-1 ratio
- Circularity of fitting radii to hydration energies
- Hydrogen bonds and the cost of isotropy
- Applying continuum solvation critically: worked case and checklist
- Exponential scaling of the exact wave function
- Hartree-Fock approximation and the self-consistent field
- Correlation energy as the name of Hartree-Fock's error
- Bond dissociation failure of restricted Hartree-Fock
- Unrestricted Hartree-Fock and spin contamination
- Error cancellation and the limits of agreement with experiment
- The Hohenberg-Kohn Theorem and the DFT Prize
- The Unknown Exact Functional and What Must Hide Inside It
- Thomas-Fermi Kinetic Energy Failure and the Kohn-Sham Fix
- Self-Interaction Error in Approximate Exchange Functionals
- Error Cancellation and the Absence of a Variational Bound
- Practical Use of DFT Without a Bound: Diagnosis and External Validation
- Local optimization and the stationary-point problem
- Conformational census: minima count and global-minimum probability
- Restart arithmetic and its circular requirement
- Two-stage conformational search and its hidden ordering assumption
- Hessian eigenvalues and stationary-point classification
- Finite-difference Hessian bug and external validation
- The timescale gap in molecular dynamics
- Velocity Verlet and the shadow Hamiltonian
- Stability edge and thermostat masking
- Exponential barrier crossing and sampling collapse
- Confident numbers from unsampled trajectories
- Practical diagnostics for sampling adequacy
- Ranking vs. accuracy as independent axes
- Error-to-spread ratio governs ranking power
- AUC interpretation and base-rate dependence
- Decoy set composition controls the metric
- What docking is and why it remains useful
- Recurring structure: fitted metrics certify themselves
- Basis set incompleteness error and its scale
- Why Gaussian basis functions are used
- Basis set convergence and the angular-momentum wall
- Basis set superposition error (BSSE) and counterpoise correction
- Better basis sets have larger superposition error
- Two independent axes of error and the rule against single-axis improvement
- Critical appraisal checklist for reported binding energies
- Jacob's Ladder hierarchy: structure and claim
- Code validation via the uniform-gas limit
- The first rung is real: gradient corrections vs. local density
- Ordering inside a rung inverts with system
- Absence of a variational guarantee on the DFT ladder
- Benchmark errors scale with system, not just functional
- Cancellation as a sharp, structural effect
- Absolute computed energies and moving zeros
- The isodesmic criterion and why it fails
- The homodesmotic criterion: counting environments
- Mechanism of cancellation: local error terms
- Consistency vs accuracy: limits of benchmarking
- Reference-scheme strategy for unbalanced reactions
- Semi-local functional structure and its two blindnesses
- Debugging by checking explanations against data
- Dispersion as an exact zero, not a small number
- Decay-ratio test distinguishing overlap from power-law
- Self-interaction as delocalization error (directional bias)
- Why the self-interaction correction is rarely used
- Two failures as one: non-locality as the common cause
- Dispersion correction as a force field bolted on
- Practical checklist and 'first principles' reassessment
- The Zwanzig Relation and Exponential Averaging
- Insertion–Deletion Asymmetry in Sampling Direction
- Staging and the Overlap as the Sizing Quantity
- Umbrella Sampling, WHAM Reconstruction, and Window Overlap
- Orthogonal Slow Coordinates and Conditional Free Energies
- Practical Validation Checklist for Free Energy Calculations
- The correlation ladder and its computational costs
- Local correlation and density-fitting approximations
- What a systematic hierarchy actually buys
- Performance of the ladder on a known exact system
- Size consistency and why CISD was abandoned
- Single-reference breakdown and the reference-weight diagnostic
- Practical reading of correlated calculations: a capstone checklist
- The repulsive wall failure case
- Interior accuracy and the learning curve
- Label quality ceiling: random vs. systematic error
- Extrapolation failure: silent settling outside training data
- The novelty warning term and its practical use
- Speed crossover and when to build a machine-learned potential
- Four diagnostic questions for evaluating ML potential results
- The scale problem: why cancellation is compulsory
- Error cancellation: mechanism and magnitude
- Partial cancellation and derivable error sign
- Complete cancellation failure at bond dissociation
- Checks that cannot fail and method disagreement as diagnostic
- The four-question procedure for evaluating a computed number
Syllabus
The Surface and Its Energies
- L1 · What a Computed Number Is: the Surface and the Bargain
- L2 · Geometry Optimisation: Minima, Saddles, and the Ones You Did Not Find
- L3 · Energies Are Differences: Cancellation and Reference States
Force Fields and Sampling
- L4 · Force Fields: Fitting a Function to Chemistry
- L5 · Molecular Dynamics: Sampling and the Timescale You Cannot Reach
- L6 · Free Energy: You Only Get Back What You Pushed Along
Wavefunction Methods
- L7 · Hartree-Fock: the Approximation That Defines the Error
- L8 · Basis Sets: the Other Error, and an Attraction That Is Not Chemistry
- L9 · The Correlation Hierarchy, and the Wall at the Fifth Power
Density Functional Theory
- L10 · DFT: an Exact Theory with an Unknown Ingredient
- L11 · Choosing a Functional: the Ladder That Is Not a Ladder
- L12 · Dispersion and Self-Interaction: Failures to Know By Name
Environments, Scale and Trust
- L13 · Solvation: Replacing an Ocean with a Constant
- L14 · Docking and Scoring: Ranking Without Computing
- L15 · Machine-Learned Potentials: Interpolation at Scale
- L16 · Benchmarks, Error Cancellation, and When to Disbelieve a Number