SAXS and SANS facilities and experimental practice · PDF fileX-ray or neutron Beam Sample ......
Transcript of SAXS and SANS facilities and experimental practice · PDF fileX-ray or neutron Beam Sample ......
SAXS and SANS facilities and experimental practice
Clement Blanchet – EMBL Hamburg
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Small Angle Scattering experiment
2θ2θ sX-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-raysRoengten, 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
2θ2θ
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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
Tran
smis
sion
0,0
0,2
0,4
0,6
0,8
1,0
0.15 Degree0.25 Degree1 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/mvThe 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 detectorPilatus
– 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 PolymersTissues
Bio-macromolecules in solution
SAS applicable to many type of samples.
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Rapid mixing device
Heating stagesMagnetic field system
Sample changers
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
Definedbuffer 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 additivesRnase – 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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