🔬 Lecture 8 · Structural Biology Part I Xiuyuan Li · 28 Oct 2026
Four ways to see a molecule you cannot see: crystals, electrons, magnetic nuclei, and scattered X-rays. Learn what each one buys, what each one costs, and which question each one answers.
101 · L8 Structural Biology Part I — Crystallography, Cryo-EM, NMR, SAXS
Lecture 8 · Structural Biology Part I (Xiuyuan Li, 28 Oct 2026)
Eighth lecture of ABCT5101, opening a two-part block on structural biology. Part I is the four techniques and their trade-offs; Part II (next week) is applications and case studies, and the practice brief points at 18 Nov. The stated aim is not to make you a crystallographer but to make you the person who can choose the right technique and run the project — “strategic decision-making”, in the lecturer's words.
| Item | Value | Why it matters |
|---|---|---|
| Optical microscopy limit | ~200 nm (0.2 µm) | Visible light is 400–750 nm; below this you need a different probe |
| X-ray: low resolution | > 3.0 Å | Overall shape only, no atomic detail |
| X-ray: medium / high | 2.5–3.0 Å / 2.0–2.5 Å | Side chains appear at 2.0–2.5; waters and metal ions may appear |
| X-ray: atomic | < 1.5 Å | Individual atoms, precise bond geometry |
| Cryo-EM resolution | 2–3 Å | Atomic resolution became routine only after ~2013 |
| Cryo-EM sweet spot | > 150 kDa | Smaller proteins need phase plates or special treatment |
| Protein needed | X-ray 1–10 mg · cryo-EM 0.1–1 mg · NMR > 5 mg at mM · SAXS 0.1–0.5 mg | The first filter on any project is how much protein you can make |
| NMR / SAXS size ceiling | NMR < 30 kDa · SAXS > 10 kDa | NMR and cryo-EM are almost complementary in size range |
| Cryo-EM throughput | ~300 movies / hr | Sets the real cost of a data-collection session |
| Nobel Prize | 2017 Chemistry | Cryo-EM; the technique's arrival as a mainstream method |
1 · What “structure” buys you
Structure is not a picture; it is the arrangement that explains behaviour.
The lecture opens deliberately outside biology. Structure is defined as the way the parts of a system are arranged or organised. Why it matters is the same in engineering, geology, science and social studies: once you know the arrangement, you can decode the system, predict outcomes, and carry knowledge across disciplines. The deck's own example is a tectonic framework over Cambrian salt basins.
Structural biology then applies that idea to living material — formed, composed, maintained and refined by living cells — at every organisational level. The reason it matters clinically is the oldest idea in the field: function follows form. A structure tells you which residues touch, which pocket a ligand occupies, and therefore what a mutation or a drug would do.
2 · “Seeing” is model-building, not photons
Below 200 nm you cannot see the thing itself; you see a model inferred from data.
Optical microscopy stops at roughly 0.2 µm — enough for mitochondria and bacteria, not for molecules. Two walls: the diffraction limit (visible light is 400–750 nm, so nothing smaller than ~200 nm resolves) and photon damage (higher resolution needs more intense light, which destroys the sample).
The lecture then redefines seeing. A model is what lets you understand and interpret a structure; a good model (i) captures all key elements and relationships, (ii) is verifiable and predictive, and (iii) stays simple enough to communicate. This is scientific constructivism: a scientist “sees” a protein through a model built from experimental data, not by looking at it.
3 · X-ray crystallography: the principle and the resolution ladder
Crystal gives order, X-rays give diffraction, maths gives electron density.
Three ideas, in order. Order: a crystal is a solid whose molecules sit in a long-range, orderly arrangement — that repeating lattice is what turns scattering into sharp spots. Diffraction: high-energy X-rays passing through the crystal are scattered, following Bragg's Law. Inversion: the diffraction pattern is mathematically transformed into an electron density map, and a molecular model is fitted into it.
Resolution is the only currency here, and the deck gives it as a ladder:
| Resolution | What you can conclude |
|---|---|
| > 3.0 Å | Low — overall shape, no atomic detail |
| 2.5–3.0 Å | Medium — general structure, some side-chain information |
| 2.0–2.5 Å | High — clear side chains and interactions; structural waters and metal ions may appear |
| < 1.5 Å | True atomic — individual atoms, precise bond geometry |
At high resolution the method answers the question industry actually pays for: how does a drug bind? The deck's two examples are databases rather than single papers — a collection of known enzyme mechanisms (M-CSA) and coordinate/ligand records in the PDB.
4 · The workflow, and where projects actually die
Seven steps; step 1 is where 90% of the schedule goes.
| Step | What happens | Failure mode |
|---|---|---|
| 0 · Sample prep | Purify the biomolecule; recombinant expression in E. coli or mammalian cells, with tags | Yield, purity, heterogeneity |
| 1 · Crystallization | Grow high-quality crystals under controlled conditions | The real bottleneck — some proteins never crystallise |
| 2 · Data collection | Expose the crystal to X-rays, record diffraction | Radiation damage, poor order |
| 3 · Data processing | Integrate patterns → electron density map | Bad statistics poison everything after |
| 4 · Model building | Fit a molecular model into the density | Over-fitting to noise |
| 5 · Refinement | Iteratively minimise difference between observed and calculated density (e.g. Phenix) | Refining into a wrong basin |
| 6 · Validation | R factors, Ramachandran plot, bond lengths | Skipping it — the model is publication-ready but wrong |
| 7 · Deposition | PDB / EMDB; validation report, conditions, software, source; unique accession code | Un-citable, unreproducible work |
Note how much of this is now automated: data processing and model building are largely software-driven, so the human decisions concentrate at step 0–1 (can I make the protein, can I crystallise it) and at step 6 (is the answer real).
5 · Crystallization: the part that decides the project
You are trying to make a molecule abandon its preferred state and pack into a lattice.
Small molecules crystallise easily — evaporation, cooling, organic solvents. Macromolecules do not: they need high purity, controlled conditions and specialised methods. The classic recipe is buffer (pH for stability) + salt (ammonium sulfate to lower solubility) + precipitant (PEG, to dehydrate gradually).
Four standard techniques: vapour diffusion (hanging drop over a reservoir, or sitting drop beside it — both rely on gradual evaporation), microbatch (mixed under oil, no evaporation), and microdialysis (dialyse against precipitant). Modern practice adds commercial screening kits, robotic dispensing (down to ~100 nL per condition), automated imaging, fine screening of pH/concentration/temperature, and seeding — introducing crushed microcrystals to nucleate better ones.
Complexes are the interesting cases. For protein–ligand work you either co-crystallise (ligand added before) or soak (ligand diffused into existing crystals); the constraints are binding affinity, the protein:ligand ratio, and stabilisation of the complex. For protein–protein or protein–nucleic-acid complexes the constraints shift to complex stability, flexibility of large assemblies, and stoichiometry — sometimes solved by fusing partners.
6 · Cryo-EM: why 2013 changed the field
Same physics as a light microscope, different illumination: electrons instead of photons.
Cryo-EM was developed in the 1980s but spent decades as “blobology” — low-resolution shapes. Three advances made atomic resolution routine after ~2013: direct electron detectors (better sensitivity and contrast), better image-processing algorithms (averaging thousands of images to beat noise and radiation damage), and cryo-stage stability (less movement, sharper images). The 2017 Nobel Prize in Chemistry marked the arrival.
The instrument: a beam of electrons as the “light”, magnetic coils as lenses, high vacuum throughout, and image formation from elastically scattered electrons — those that change direction but keep their energy, carrying the structural information.
| Component | Detail worth knowing |
|---|---|
| Grid | ~3 mm disc; copper, nickel or gold; mesh 200/300/400 squares per inch; carbon or holey-carbon film; glow discharge to make the surface hydrophilic |
| Vitrification | Plunge into liquid ethane; control humidity to avoid ice contamination; avoids fixatives and stains, so the native state survives; also limits radiation damage |
| Sample tolerance | Purity not very strict; 0.1–5 mg/mL; avoid high concentrations of additives — far kinder than crystallography |
| Thick samples | Electrons penetrate poorly — cells need FIB milling (e.g. Aquilos 2) to thin the region of interest |
| Imaging | Low dose to search (atlas → squares → holes), then high magnification; movie mode with motion correction; automatic collection up to ~300 movies/hr |
Why a single molecule is not enough: biological samples are weak scatterers (C, N, S, O, H against water) so contrast is intrinsically low, and even frozen samples suffer radiation damage. The answer is statistics — assume a homogeneous population, collect a large dataset, classify and align, then average. Fine detail emerges from the average, not from any one image.
The processing pipeline: micrographs → particle picking → 2D classification and averaging → CTF correction → initial 3D model → 3D classification and refinement → post-processing and validation. Published benchmarks in the deck: β-galactosidase at 3.2 Å (Bartesaghi 2014), GroEL at 3.5 Å (Roh 2017).
7 · NMR and SAXS: the two specialists
NMR gives dynamics in solution; SAXS gives shape in solution — neither gives you a crystal.
NMR works on the magnetic behaviour of nuclei (1H, 13C, 15N) in a strong field: they absorb and emit radiofrequency energy, and the signal is exquisitely sensitive to the local chemical environment, reporting distances up to ~5 Å and bond angles. Its niche is solution structure of small proteins (< 30 kDa), real-time dynamics and interactions, and being non-destructive under near-physiological conditions. Its costs are size, spectral complexity, mM concentrations of very pure protein, and expensive high-field instruments — which is why cryo-EM and crystallography took most of its territory.
SAXS measures X-ray scattering at small angles in solution to report size, shape and conformation. It is explicitly a low-resolution technique, needs very little protein (0.1–0.5 mg), and is extremely sensitive to aggregation — hence the standard practice of running it inline with SEC, so only the clean monomer reaches the beam.
Two case studies worth the detail: a de novo designed transmembrane protein where the NMR structure (PDB 9FDG) and the crystal structure (8UZL) both match the computational design (Berhanu et al., Science 2024) — two independent techniques validating a design; and a JACS 2018 study using SAXS to distinguish different conformations of the same molecule in solution.
8 · The decision table you will actually use
Four techniques, one table — this is the slide to photograph.
| Technique | Resolution | Protein needed | Size range | Strength | Weakness |
|---|---|---|---|---|---|
| X-ray | down to 1.0 Å | 1–10 mg | small molecules to large complexes | Atomic detail; drug binding and mechanism | Crystallisation is slow and may never work; static crystal snapshot |
| Cryo-EM | down to 2–3 Å | 0.1–1 mg | best >150 kDa | Native conformation without crystals; membrane proteins, large assemblies | Purity/homogeneity limits; heavy processing and expensive instruments |
| NMR | no fixed spatial resolution | > 5 mg at mM | < 30 kDa | Dynamics and interactions near physiological conditions | Isotope labelling; high concentration; complex spectra |
| SAXS | low, shape only | 0.1–0.5 mg | > 10 kDa | Solution conformation; flexible molecules; tiny material cost | No atomic detail; needs another technique alongside |
9 · Outsourcing: the decisions you will actually be making
Expression, purification and crystallisation are mature enough to buy — the judgement is not.
The lecture is explicit that this block is about technological leadership, not bench craft. Protein expression, purification and crystallisation are mature enough for CRO outsourcing; specialised companies can deliver high-purity, active protein in roughly two weeks, often at lower cost, which frees the research team to do the structural analysis.
| Decision | What you are choosing between |
|---|---|
| Expression system | E. coli / yeast / insect / mammalian — driven by whether you need post-translational modification; cell-free systems for speed and difficult targets |
| Tags | His / Strep / GST for purification — but tags can perturb structure and crystallisation, so plan protease cleavage (TEV, thrombin, 3C) from the start |
| Codon optimisation | Each host has codon bias; rare codons silently cost you yield |
| Purification | Affinity → ion exchange (choose cation/anion from the pI) → size exclusion; a combination is normal for high purity |
| Verification | SDS-PAGE (purity), IEX (charge state), SEC (folding/aggregation), MS (identity and modifications), activity assay (function) |
| Vendor management | Multiple CROs by strength; synchronised tasks; regular reporting — the actual leadership work |
10 · Practice before the next lecture (18 Nov)
Four tasks, and they are the reason Part II will make sense.
- Install PyMOL (pymol.org) and work through the tutorial — it is used in class next week.
- Skim paper 1 for how the authors expressed and crystallised NDM-1.
- Read paper 2 for how the co-crystal structures of benzylpenicillin, oxacillin, methicillin and meropenem were obtained, then load them in PyMOL and look at the bound small molecules.
- Read one of the earliest reports of the SARS-CoV-2 spike cryo-EM structure.
Reference shelf from the deck: RCSB PDB (rcsb.org) · M-CSA enzyme mechanisms (EBI) · UniProt · Caltech cryo-EM course · cryoem101.org · SSRL SAXS workshop material.
11 · Two cases where structure changed the decision
| Case | What the structure showed | What it decided |
|---|---|---|
| Gleevec (imatinib) and c-Abl kinase | The drug binds a pocket next to the ATP site in the inactive conformation, locking the kinase “off” | Moved the logic from “inhibit activity” to “freeze a conformation” — the textbook case of structure producing a drug, and why mutations such as T315I break it |
| PD-1 in complex with an antibody | The antibody binds the ligand-binding face of PD-1, blocking the PD-L1 contact surface | Blocking does not require mimicking the ligand — occupying the same surface is enough; epitope choice matters more than raw affinity |
12 · Model validation: “it looks right” is not enough
After the electron density map, amino acids are built into the density (model building) and refined repeatedly. Validation asks a different question: how much should anyone trust this model?
| Metric | What it measures | Intuition |
|---|---|---|
| R-factor / R-free | Gap between predicted and observed diffraction; R-free uses data never fitted | Like a held-out exam score — a high R-free means the model memorised the training data |
| Ramachandran plot | Whether backbone dihedral angles fall in allowed regions | Checks the backbone is not bent into impossible angles |
| B-factor | Which regions are loose or disordered | Higher means “wobblier” — that part is genuinely flexible |
| Density fit | Whether side chains actually sit in the density | You cannot force the model in and call it “close enough” |
13 · PDB: publish it or nobody can use it
Models and structure factors are deposited in the Protein Data Bank and receive a four-character ID (for example 1IEP for the classic Gleevec–Abl structure). The PDB holds both coordinates and structure factors, so anyone can re-validate the model rather than trust a picture.