SAXS and SANS facilities and experimental practice Clement Blanchet - - PowerPoint PPT Presentation
SAXS and SANS facilities and experimental practice Clement Blanchet - - PowerPoint PPT Presentation
SAXS and SANS facilities and experimental practice Clement Blanchet EMBL Hamburg Small Angle Scattering experiment Detector Sample X-ray or neutron 2 2 Beam s Buffer The beam hits the sample, X-rays/neutrons interact with the
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Small Angle Scattering experiment
2θ 2θ
s
X-ray or neutron Beam
Sample Buffer Detector
The beam hits the sample, X-rays/neutrons interact with the sample and are scattered, providing structural information on the sample. Same formalism but different scattered particles Different instrument.
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Outline
- X-rays / neutrons
- SAS instruments
- Sample environment
- Sample requirements and collection strategy
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X-rays and neutrons
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X-rays
Roengten, 1895
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Electromagnetic wave
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How are X-ray produced?
- Brehmstrahlung
– When a charge is accelerated charge, electromagnetic radiation is produced (from Maxwell equation)
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X-ray sources - Synchrotron
- Synchrotrons
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X-ray sources - synchrotron
- Synchrotron radiation – Insertion devices
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Insertion devices
Dipole bending magnet (APS) Undulator (PetraIII)
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Synchrotrons around the world
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X-ray sources - FEL
- Free electron laser
– Electrons are accelerated and send to a long undulator (several 100s meters) – Self amplified spontaneous emission: electrons group themselves into small bunches. – Production of very short and intense X-ray pulses
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X-ray sources - FEL
- Free electron laser
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Lab sources
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Lab sources
- Principle : electrons, produced by heating a
cathode are accelerated in an electric field and projected on a metallic anode. – Brehmstrahlung – Fluorescence
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X-ray sources
- Lab source (rotating anode, liquid jet)
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Neutron
λ=h/mv
James Chadwick
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Neutron production
- Nuclear reaction
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Neutron production
- Spallation source
– Accelerated protons hit a heavy metal target.
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Neutrons Facilities
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SAXS and SANS Instruments
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Optics
Polychromatic divergent beam from the source Monochromatic focused (parallel) beam for SAS
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Monochromatic X-ray
- Bragg diffraction on a crystal
nλ = 2dsinθ
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Monochromator
- Before
- Polychromatic
- After
- One wavelength + harmonics
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Focusing/low divergence
- Small beam at the detector position
- Small beam at the sample position
2θ 2θ
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Focusing X-ray
- Compound refractive lenses
- X-ray mirrors
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Focusing X-ray
- Focussing mirror
- Reflectivity
Energy [eV]
10000
Transmission
0,0 0,2 0,4 0,6 0,8 1,0
0.15 Degree 0.25 Degree 1 Degree
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Focussing mirror – harmonics filter
Monochromatic, focused x-ray beam
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Monochromatic neutrons
- De Broglie equation: λ=h/mv
The wavelength of a neutron is related to its velocity.
- Velocity selector
∆λ/λ=5-10%
- For pulsed source, TOF
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Collimation neutrons
- The collimator is used to obtain a parallel
beam
Get rid of parasitic scattering: slits
Beam defining slits Guard or anti-scatter slits
Hybrid slits
- Idea: use a crystal for the tip of the blade:
no scattering but diffraction
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Hybrid slits
- On the P12 beamline
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Sample environment
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Flight tube
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Beamstop
- Prevent the direct beam from hitting the
detector
– Big enough to stop the direct beam – Small enough to collect the small angle
- Measure transmitted beam
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Active Beamstop
- SAXS images needs to be accurately
scaled to allow for proper buffer subtraction and extraction of the solute SAXS pattern
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Detectors
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CCD detector
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Single photon counting detector principle
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Single photon counting detector Pilatus
– High dynamic range – No background noise – (relatively) Fast framing
Ideal for SAXS
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Neutron detection
- He3 detector:
n + 3He → 3H + 1H + 0.764 MeV
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Sample environment
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Samples
Metal alloys Nanomagnetic materials Sufactants Polymers Tissues Bio-macromolecules in solution
SAS applicable to many type of samples.
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Sample environment
Example ID02 (ESRF) multipurpose beamline
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Sample environment
- Bio-macromolecules in solution are weakly
scattering sample.
- For biological macromolecules in solution:
– fragile – Preferably in vacuum – Thermostated
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Sample cell
- Cell material: low absorption and scattering
– Mica, quartz, polycarbonate
- Sample thickness (t): compromise between
scattering and absorption
– Scattering α t – absorption α exp(-ut)
- For neutron, cell are rather thin (<1mm to avoid
multiple scattering
Solution SAXS
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10 years ago: Manual sample loading
- Buffer and sample should be
measured in the same cell
- Difficult to implement in vacuum
- 10-15 minutes per measurement
- High sample consumption
- Non-optimized cleaning procedure
- Tedious, energy and attention
consuming
SAXS sample changer @EMBL Hamburg
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SAXS sample changer
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Sample changer performances
- Large storage capacity
- Full cycle time (loading, exposure,
flushing, cleaning, drying) ≈ 1 min
- Volume 5-20 microliter
- Very efficient cleaning
- Flow measurement
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Online size exclusion column
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SEC + SAXS
Defined buffer region
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Experimental practice
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Buffer subtraction
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Buffer subtraction
- Biological sample scatters very weakly,
SAXS curves collected on the buffer should be carefully subtracted
– Exactly matching buffer (dialysis, elution buffer) – Sample and buffer measured in the same cell
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Monodispersity
- SAS is very sensible to aggregation, the
sample should be monodisperse
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Monodispersity
- Check the monodispersity of your sample
before coming to the beamline.
(native gel, dynamic light scattering, ultracentrifugation,…)
- Use online chromatography
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Inter-particle interactions
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Inter-particle interactions
- Change solution (pH, salt concentration) to
limit interactions
- Measure different concentrations and
extrapolate
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Measure also water and/or standard protein…
- … to estimate the molecular mass of your
sample using the forward scattering
– For data on an absolute scale (water measurement)
- M=I(0)*NA/(C*ν∗∆ρ)
– Using a protein standard
- M=MBSA*I(0)/IBSA(0)
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X-rays - Radiation damage!!!
- With intense synchrotron beam: radiation
damage:
- Monitor radiation damage: collect several
frames and compare them.
- Limit the radiation damage
H2O OH· Free radicals: oxidize proteins which leads to their aggregation H ·
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X-rays - Radiation damage!!!
Flow measurement Beam attenuation Use of additives Rnase – Static measurement
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Contrast in neutron
- Neutrons interact with the nucleus of
atoms
- Each atoms has its own scattering length:
H D C N O P S
- .3742
0.6671 0.6651 0.940 0.5804 0.517 0.2847
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Labeling
- Protein and nucleic acids have different
scattering length densities and the different components can readily be studied by SANS
- To study protein-protein complex, one of the
components needs to be deuterated (hydrogen exchanged with deuterium) to changed its scattering length density
- A deuterated protein is obtained by producing
the protein in a deuterated medium.
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Neutrong collection strategy
- Solvent matching
– Find the solvent composition that match the contrast of the component you want to hide – Measure the sample in this solvent
- Contrast variation
– Measure the sample in solvent with different D/H ratio, different scattering length. – Using Stuhrmann analysis you can access the curves of the different components.
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Summary: SAS sample
- Protein concentration: 0.1-10 mg/ml
- Volume: 5-50 microliter (SAXS), 200-300
microliter (SANS)
- Time:
- lab source: 5-60 min
- Synchrotron: seconds
- Neutrons: 30 minutes - hours
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Summary: SAS sample
- Pure and monodisperse sample
- Exactly matching buffer
- Measure concentration series
- For SAXS:
– Be aware of radiation damage
- For SANS:
– Carefully design your experiment, think of your collection strategy.
Conclusion
- To optimally use your beamtime: carefully plan your
experiment, prepare your sample and characterize them before coming to the beamline
- SAXS is now widely used. Dedicated instruments with
low background and high level of automation, high quality lab instruments.
- SANS more difficult: consume more time and sample,
requires good planning of your experiments and collection strategy, but can provides unique information.
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