This lecture covers two major structural biology techniques:
1️⃣ Small-Angle X-ray Scattering (SAXS) – low-resolution structural analysis in solution 2️⃣ Cryo-Electron Microscopy (Cryo-EM) – high-resolution imaging of macromolecules
Both techniques help scientists determine the structure of proteins and complexes without crystallizing them.
SAXS measures how X-rays scatter when they hit molecules in solution.
It provides information about overall size and shape of particles.
Typical structural scale:
So SAXS gives low-resolution structural information.
Think of it as:
👉 seeing the silhouette of a protein
not the individual atoms.
The SAXS experiment consists of several components.
1️⃣ X-ray source
Produces X-ray beam.
2️⃣ Monochromator
Ensures only one wavelength is used.
3️⃣ Sample
Usually dilute protein solution (~1% or ~10 mg/mL).
4️⃣ Detector
Measures scattered X-rays.
The scattering vector is defined as:
q = rac{4pi sin heta}{lambda}
Where:
The detector records the scattering intensity I(q).
| Feature | Crystallography | SAXS |
|---|---|---|
| Sample | Crystal | Solution |
| Structure | Atomic resolution | Low resolution |
| State | Sometimes non-native | Native conditions |
| Data richness | High | Low |
Key takeaway:
SAXS studies proteins in their natural environment.
But you lose detailed atomic information.
The raw SAXS data must be processed before interpretation.
Typical workflow:
1️⃣ Collect scattering intensity 2️⃣ Convert 2D detector image → 1D scattering curve 3️⃣ Perform background subtraction 4️⃣ Normalize data 5️⃣ Analyze curves
This produces the function:
I(q)
which describes how the sample scatters X-rays at different angles.
One of the most important SAXS analyses.
It describes the distribution of distances between atoms inside the particle.
Think of it as:
👉 a histogram of all distances inside the protein
From the scattering curve we can calculate:
p(r)
This solves the inverse scattering problem.
Why inverse?
Because:
So we mathematically convert I(q) → p(r).
Three key plots appear in almost every SAXS analysis.
Plot:
ln I(q) ext{ vs } q
This is the raw scattering data.
It shows how intensity decreases as scattering angle increases.
Plot:
ln I(q) ext{ vs } q^2
Used to determine:
Important concept:
The Guinier region corresponds to very small angles.
From the slope:
R_g^2 = -3 imes slope
This tells you how large the particle is.
Plot:
p(r) ext{ vs } r
Shows internal distance distribution.
From this we obtain:
Examples of shapes from p(r):
| Shape | p(r) pattern |
|---|---|
| Sphere | symmetric curve |
| Rod | long tail |
| Disk | skewed distribution |
The Kratky plot evaluates protein flexibility.
Plot:
q^2 I(q) ext{ vs } q
Interpretation:
| Shape | Meaning |
|---|---|
| Bell-shaped peak | Folded protein |
| Flat/continuous increase | Unfolded protein |
| Broad peak | Flexible protein |
This is a quick test of protein disorder.
At high scattering angles:
I(q) propto q^{-4}
This law indicates sharp particle boundaries.
Porod analysis helps determine:
Even though SAXS gives low-resolution data, we can reconstruct approximate shapes.
This uses:
The protein is represented by many small spheres.
Optimization algorithms (e.g., simulated annealing) adjust these spheres until the calculated scattering fits the data.
Example used in slides:
🧬 Lysozyme shape reconstruction.
If we already know the atomic structure (from crystallography), we can:
1️⃣ Compute theoretical SAXS scattering 2️⃣ Compare it with experimental SAXS data
This checks if the solution structure matches the crystal structure.
Advantages:
✔ native conditions ✔ no crystallization required ✔ small sample volume ✔ works at low concentration
SAXS is often used for:
The second part of the lecture introduces Cryo-EM.
This technique is currently revolutionizing structural biology.
Cryo-EM used to give low resolution.
But new technologies improved it dramatically:
Result:
Structures reaching ~1.8 Å resolution.
Because of this breakthrough:
🏆 2017 Nobel Prize in Chemistry
awarded to:
Cryo-EM commonly uses Single Particle Analysis.
Instead of crystallizing proteins, we image thousands of individual molecules.
Then computationally combine them.
The workflow is:
1️⃣ Protein purification 2️⃣ Apply sample to EM grid 3️⃣ Plunge freeze in liquid ethane (vitrification) 4️⃣ Image with electron microscope 5️⃣ Collect movies 6️⃣ Particle picking 7️⃣ 2D classification 8️⃣ 3D reconstruction 9️⃣ Build atomic model
Samples are frozen extremely fast.
This produces vitreous ice, which:
✔ preserves native structure ✔ avoids crystal formation
Procedure:
Protein grid → plunge into liquid ethane.
Temperature ≈ −180°C.
Two EM sample preparation methods.
Uses heavy metal salts (e.g., uranyl acetate).
Advantages:
Disadvantages:
Flash-frozen samples.
Advantages:
✔ native environment ✔ atomic resolution possible
Disadvantages:
TEM works similarly to a light microscope but uses electrons instead of light.
Main components:
Electrons have extremely small wavelengths.
This gives very high resolution.
Compared with light:
| Radiation | Wavelength | Resolution |
|---|---|---|
| Visible light | ~400 nm | limited |
| X-rays | Å scale | good |
| Electrons | picometers | extremely high |
Shorter wavelength → higher resolution.
Images rely on contrast.
Two types:
Occurs when electrons are absorbed or scattered away.
Heavier atoms scatter more electrons.
This reduces intensity reaching the detector.
Result:
dark regions in image.
Electrons behave like waves.
When passing through atoms:
The interference creates the image.
Cryo-EM mostly relies on phase contrast.
Three main events occur:
1️⃣ No scattering
Electron passes straight through.
2️⃣ Elastic scattering
Electron deflects but loses no energy.
Important for image formation.
3️⃣ Inelastic scattering
Electron loses energy.
Causes:
Biological samples are mostly:
💧 water + light atoms
Therefore:
This causes low signal-to-noise ratio.
To solve this:
➡ average many particles.
Images are analyzed in Fourier space.
Why?
Because it simplifies image processing.
Fourier transforms help with:
| Frequency | Meaning |
|---|---|
| Low frequency | overall shape |
| High frequency | fine details |
Noise often occurs in high frequencies.
Common filters:
| Filter | Function |
|---|---|
| Low-pass | removes high frequency noise |
| High-pass | removes background |
| Band-pass | selects specific frequencies |
These improve image quality.
Important imaging principle.
To resolve a structure of size d, pixel size must be:
pixel ≤ d/2
Otherwise:
⚠ aliasing occurs (loss of information).
Modern Cryo-EM uses DDD cameras.
Advantages:
✔ electron counting ✔ better sensitivity ✔ reduced blurring ✔ motion correction
This technology enabled the resolution revolution.
Detector records individual electron hits.
Instead of measuring intensity, it counts electrons.
Benefits:
Direct detectors can locate electrons with sub-pixel precision.
This increases effective resolution beyond pixel size.
After particle alignment:
Using back-projection algorithms we reconstruct a 3D density map.
Resolution is measured with:
Procedure:
1️⃣ Split dataset into two halves 2️⃣ Build two independent models 3️⃣ Compare similarity
This avoids overfitting.
Called the Gold-standard FSC.
Not all particles are good.
During 2D classification:
Particles are grouped into classes.
Then:
✔ good classes kept ❌ bad particles rejected
Only the best particles are used for final reconstruction.
Cryo-EM can be used for:
Examples:
✔ solution scattering ✔ low-resolution shape ✔ Guinier → Rg ✔ p(r) → particle size ✔ Kratky → folding state
✔ single particle analysis ✔ vitrified samples ✔ phase contrast imaging ✔ Fourier reconstruction ✔ atomic resolution possible
| Technique | Think of it like |
|---|---|
| SAXS | shadow of a protein |
| Cryo-EM | photograph of a frozen molecule |
| X-ray crystallography | atomic blueprint |