We acknowledge Master Machinist Al Lance of the University of Delaware for machining the shear cell and Mr. Cedric Gagnon for design and drafting. This manuscript was prepared under cooperative agreement 70NANB7H6178 from NIST, U.S. Department of Commerce. This work utilized facilities supported in part by the National Science Foundation under Agreement No. DMR-0944772. The statements, findings, conclusions and recommendations are those of the author(s) and do not necessarily reflect the view of NIST or the U.S. Department of Commerce.&#160;

Figure 2 shows an assembled shear cell attached to the baseplate, which is mounted to the breadboard on the sample environment stage and aligned in the neutron beam for a SANS experiment. The stepper motor, gear box and belt drive, slit motor stage, shear cell and direction of the neutron beam are labeled in Figure 2. The present protocol provides directions for assembling the shear cell (section 1), mounting the shear cell onto the sample environment stage (section 2), calibrating the geometry for a SANS experiment (section 3), loading a sample (section 4), running an experiment and data collection (section 5) and ending an experiment (section 6). For reference, Figure 3 is a schematic of the assembled cell and Figure 4 shows the disassembled shear cell parts laid out from front plate to back plate, left to right, and the necessary tools for assembly (1/16 in&#160;and 3/16 in&#160;Allen wrenches and a 3/8 in&#160;open end wrench). From left to right in Figure 4 are the front plate, bearing, spring-loaded bushing, O-rings, quartz window, middle plate with O-rings, sample access ports and syringe connectors, set-screws, mandrel, and the parts for the back plate (quartz window, O-rings, spring-loaded bushing, bearing), back plate, four socket head cap screws and quick connect cooling hose with quick-connectors attached.
1. Assemble the Shear Cell (Inset to the Right in Figure 2)
<ol>
	<li>Prepare the middle plate for assembly.
	<ol>
		<li>Clean the middle plate including sample and set-screw pathways and identify the top of the plate by the score mark.</li>
		<li>Seal the sample loading pathways using the three set-screws. Wrap each set-screw in thread seal tape and use a 1/16 in&#160;Allen wrench to insert each screw into each hole at the &#8220;bottom&#8221; (2) and one set-screw into the hole on the &#8220;side&#8221;.</li>
		<li>Place the round white O-rings (2-14 in&#160;ID, Viton standard AS568 size 035) in the grooves on both sides of the middle plate.</li>
	</ol>
	</li>
	<li>Prepare the back and front plates for assembly (Figure 5).
	<ol>
		<li>Press fit the bearing into each of the front and back plates.</li>
		<li>Insert the spring-loaded bushing (which is a seal) with the spring-side open toward the sample into the front and back plates.</li>
		<li>Place the small (1-5/8 in&#160;ID) and large (2-1/4 in&#160;ID) Buna-N square double seal O-rings into the grooves in each of the front and back plates.</li>
		<li>Place the quartz windows on top of the square O-rings in each plate.</li>
	</ol>
	</li>
	<li>Assemble the front and middle plates together.
	<ol>
		<li>Place the front plate on a flat surface; align the score on the top of the middle and front plates and place the middle plate on the front plate. If necessary, apply a small amount of appropriate grease to the rounded O-rings in the middle plate to hold them in place during assembly.</li>
	</ol>
	</li>
	<li>Assemble the mandrel and back plate together.
	<ol>
		<li>Insert the short end of the mandrel shaft into the back plate. Use evenly applied force and the mandrel will &#8220;click&#8221; into place. Take note that the mandrel is now holding the quartz window and square O-rings in place on the back plate.</li>
	</ol>
	</li>
	<li>Assemble the front plate, middle plate, mandrel and back plate together.
	<ol>
		<li>Place the front and middle plate assembly on a raised platform with the middle plate facing up. This raised platform is to allow space for the mandrel shaft to extend below the assembly without hitting the table.</li>
		<li>Align the score on the top of the front plate assembly with the score on the back plate assembly.</li>
		<li>Insert the long part of the mandrel shaft into the front plate assembly. Make sure the rounded O-rings on the middle plate remain properly seated during assembly. The cell will slide together and again, &#8220;click&#8221; when properly assembled.</li>
		<li>Screw the assembly together using the four socket head cap screws and a 3/16 in&#160;Allen wrench. Tighten the screws in a cross-pattern so the cell maintains concentricity.</li>
	</ol>
	</li>
	<li>Wrap thread seal tape around the two access ports and screw them into the top of the middle plate. Tighten with a 3/8 in&#160;open-end wrench.</li>
	<li>Place the cadmium mask (Figure 6) into the receiving slot machined into the front of the front plate. Apply tape or tack to hold the mask in place if needed.</li>
	<li>Use the quick-connectors to cross-connect the coolant hose between the top ports on the front and back plates.</li>
</ol>
2. Mount the Shear Cell into the Beamline
<ol>
	<li>Cover the SANS detector window with the safety shield.</li>
	<li>Ask the responsible facility instrument scientist to align the sample environment stage with the neutron beam.</li>
	<li>Mount the breadboard to the sample environment stage using four &#188; in&#160;x 20 socket head Allen bolts and a 3/16 in&#160;Allen wrench.</li>
	<li>Attach the shear cell assembly to the cell-mounting bracket located on the baseplate (already attached to the breadboard (Figure 7)).
	<ol>
		<li>Identify the cell-mounting bracket and shaft coupler attached to the baseplate (Figure 8). Make sure the set-screws for the shaft coupler are loosened.</li>
		<li>Align the shaft coupler and the mandrel shaft such that the set-screws on the coupler will screw into the flat part of the mandrel shaft.</li>
		<li>Horizontally slide the shear cell into the cell-mounting bracket so that the assembly looks like that shown in Figure 8. This step should be performed with care as it is important not to bend the mandrel shaft or the shaft coupler.</li>
		<li>Attach the shear cell assembly to the cell-mounting bracket with two socket head cap-screws using a 3/16 in&#160;Allen wrench. Tighten securely always making sure the shear cell is flush against the cell-mounting bracket.</li>
		<li>Tighten the two set-screws on the shaft connector using a 1/16 in&#160;Allen wrench to connect the shear cell mandrel shaft to the drive assembly.</li>
	</ol>
	</li>
	<li>Align the shear cell geometry with the neutron beam.
	<ol>
		<li>Use the laser to adjust the SANS sample environment stage such that the height of the mandrel shaft is the same as the neutron beam. Align the center of the gap in the shear cell to the center of the neutron beamline path.</li>
	</ol>
	</li>
	<li>Insert the appropriate cadmium slit into the slit motor stage assembly that is mounted on the breadboard (Figure 8). Secure the slit with tack if necessary. 
	Note: The slit should be flush with the front plate and approximately placed within the gap of the shear cell. Choose the slit accordingly for the desired experiment. For gap resolution experiments 0.1 mm and 0.2 mm curved slits are available. Whereas for measurements that do not require spatial resolution a 0.8 mm rectangular slit is advisable.</li>
	<li>Move the motor position using the crank to adjust the tension of the drive belt so that there is approximately &#188; in&#160;deflection in the belt. When tensioned properly, lock the motor location by tightening the set-screw located below the wheel using a 7/64 in&#160;Allen wrench. 
	Note: An optional gear reducer may be added to the motor assembly. This option may be necessary based upon the required shear rates required for a specific experiment.</li>
	<li>Connect the two coolant bath hoses to the shear cell using the quick-connectors.</li>
	<li>Adjust any observation cameras or other auxiliary equipment specific to observing the experiment.</li>
	<li>Remove the safety shield protecting the SANS detector window.</li>
</ol>
3. SANS Setup and Calibration
<ol>
	<li>Attach a 0.5 in&#160;aperture to the end of the snout on the incident neutron beam.</li>
	<li>Set the desired SANS detector position (q-range), neutron wavelength, and wavelength spread following standard SANS protocols and optimized for the experimental conditions. 
	Note: The calculation for the sample-to-detector distance is based on the sample environment stage located on the &#8220;Huber table&#8221;.</li>
	<li>Align the slit position with the gap of the shear cell.
	<ol>
		<li>Use the slit motor stage (Figure 8) to align the slit position with the gap of the shear cell. Use a laser to emulate the neutron beam and a mirror to detect the laser once it passes through the quartz windows within the gap of the shear cell assembly.</li>
		<li>Fine-tune the position of the slit using SANS transmission measurements. Systematically vary the slit motor position from the inner wall of the shear cell gap to the outer wall of the shear cell gap using 0.1 mm motor slit translation steps. Observe the transmission (typically 2 sec) using SANS and record the slit motor position for each transmission measurement (Figure 9). 
		Note: If spatial resolution is desired, identify the motor positions necessary for the SANS experiments. If spatial resolution is not necessary identify the single motor position that aligns the slit with the middle of the shear cell gap. Aligning the slit with the gap in the shear cell is crucial for completing a good experiment. It is also possible (and recommended) to use water to align the position of the slit using SANS transmission measurements. Using water reduces the transmission and provides contrast with the shear cell housing (Figure 9). 
		Note: Load the water into the cell by following the sample loading protocol (section 4). Using water will generally require the shear cell to be removed from the baseplate, disassembled, dried, reassembled and remounted to the baseplate prior to loading the sample for the experiment. As long as the baseplate IS NOT removed from the sample environment stage this should not be a problem, but it is always important to verify the slit alignment with the gap.</li>
	</ol>
	</li>
	<li>Calibrate the sample geometry
	<ol>
		<li>Perform a blocked beam dark count and an empty cell measurement according to standardized SANS procedures. Note that the empty cell measurements should be performed at each spatial location as determined by the slit calibration performed in section 3.3.</li>
	</ol>
	</li>
</ol>
4. Sample Loading Protocol
<ol>
	<li>Place the safety shield on the SANS detector window.</li>
	<li>Mount the two syringe connectors (Nylon) and threaded syringe fixtures (blue and yellow) to the steel pipes at the top of the sample cell. Make sure the stopcocks are in the closed position.</li>
	<li>Preload the sample into a 10 ml threaded syringe (minimum sample volume is 6 ml). Make sure the sample is free of bubbles.
	<ol>
		<li>Eliminate bubbles by either centrifuging lightly or heating the sample to reduce the viscosity of the sample while loading the syringe. If the sample is heated, it is strongly recommended that the temperature of the shear cell is also increased to aid in loading the sample.</li>
	</ol>
	</li>
	<li>Place an empty syringe without the plunger on the connector in the middle of the shear cell to receive excess sample (Figure 8).</li>
	<li>Place the sample syringe on the other connector (Figure 8).</li>
	<li>Open both stopcocks.</li>
	<li>Inject the sample slowly until the sample begins to enter into the empty syringe.</li>
	<li>Remove any air bubbles from the gap of the shear cell.
	<ol>
		<li>Turn the motor control off to release the motor and allow the belt to be manually moved.</li>
		<li>Shear the sample by hand to help move the bubbles to the top of the shear cell, whereby additional sample injection will typically push the bubble into the outlet and out of the shear cell gap.</li>
	</ol>
	</li>
	<li>Close the stopcocks to lock the sample in the cell.</li>
	<li>Change the temperature of the water bath to the required experimental temperature, and precondition the sample&#8217;s shear history as appropriate.</li>
	<li>Check for any bubbles (and do so regularly during the course of the experiment). If bubbles are observed; open the stopcocks, use rotation to move the bubbles to the top of the shear zone, and inject additional sample to push the bubbles out of the shear zone of the cell.</li>
	<li>Remove the safety shield and any extraneous tools and supplies from the beam area.</li>
</ol>
5. Running the Shear Experiment and Collecting SANS Data
<ol>
	<li>For simple steady shear experiments:
	<ol>
		<li>Set the shear rate in the steady shear control file associated with the motor control software (see associated documentation for motor control software operation).</li>
		<li>Identify the shear direction of the sample during the experiment.</li>
		<li>Set up the desired SANS experiments according to the standardized SANS procedures.</li>
		<li>Start the shear cell motor.</li>
		<li>Start the SANS experiment. Check the detector counts and observe the SANS 2D pattern to insure SANS results are being properly recorded during shearing. An example of a typical pattern observed for the surfactant solutions discussed in the section on representative results is shown in Figure 10.</li>
		<li>Repeat the procedure (section 5.1) for each desired shear rate.</li>
	</ol>
	</li>
	<li>For time-resolved oscillatory shear experiments:
	<ol>
		<li>Verify the trigger position for the oscillatory shear experiment. For oscillatory shear, this is at the point of maximum strain and minimum (zero) strain rate.</li>
		<li>Set the oscillation frequency and strain amplitude in the time-resolved control file associated with the motor control software (see associated documentation for motor control software operation). Note that the strain amplitude is defined according to the amplitude of the applied strain centered at zero and is the rheologically defined strain amplitude.</li>
		<li>Start the shear cell motor for the oscillatory shear experiment.</li>
		<li>Start the SANS experiment. Check detector counts and observe the 2D pattern to insure SANS is properly being recorded during oscillatory shearing.</li>
		<li>Copy the time-stamped neutron detector log file from NISTO to Charlotte and preprocess the data using software provided by the NCNR.</li>
		<li>Reduce the preprocessed data set with the reduction software package in IGOR.</li>
		<li>Repeat the procedure (section 5.2) for each, desired oscillation frequency and strain amplitude condition.</li>
	</ol>
	</li>
</ol>
6. End of Experiment
<ol>
	<li>Turn off the neutron beam and motor control.</li>
	<li>Place the safety shield on the SANS detector window.</li>
	<li>Let the sample and apparatus stand in the closed beam for 5 min. Perform a standard radiation check before removing the shear cell from the baseplate.</li>
	<li>Open the stopcocks on the sample ports and withdraw or push out the sample using the sample syringes. Recover the sample, close the stopcocks, and remove the syringes.</li>
	<li>Turn off the temperature bath. Uncouple the fluid bath cooling hoses from the shear cell quick connect ports.</li>
	<li>Loosen the Allen screws on the shaft coupler between the mandrel and the drive shaft using a 1/16 in&#160;Allen wrench. Use a 3/16 in&#160;Allen wrench to unscrew the two socket head cap screws that attach the shear cell to the cell-mounting bracket. Slide the shear cell out of the cell mounting bracket.</li>
	<li>Disassemble the shear cell by reversing the assembly protocol (section 1 of the protocol).</li>
	<li>Clean the shear cell using soapy water. Rinse and dry thoroughly.</li>
</ol>

<ol>
	<li>Larson, R. G. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=.">.</a> The Structure and Rheology of Complex Fluids. , (1999).</li><li>Wagner, N. J., Brady, J. F. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Shear+thickening+in+colloidal+dispersions.">Shear thickening in colloidal dispersions.</a> Phys.Today. 62, 27-32 (2009).</li><li>Fardin, M. A., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Potential+&amp;#34;ways+of+thinking&amp;#34;+about+the+shear-banding+phenomenon.">Potential &amp;#34;ways of thinking&amp;#34; about the shear-banding phenomenon.</a> Soft Matter. 8, 910-922 (2012).</li><li>Eberle, A. P. R., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Shear-induced+anisotropy+in+nanoparticle+gels+with+short-ranged+interactions.">Shear-induced anisotropy in nanoparticle gels with short-ranged interactions.</a> Phys. Rev. Lett. , (2013).</li><li>Zaccarelli, E. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Colloidal+gels:+equilibrium+and+non-equilibrium+routes.">Colloidal gels: equilibrium and non-equilibrium routes.</a> J. Phys. Cond. Matter. 19, (2007).</li><li>Hsiao, L. C., Newman, R. S., Glotzer, S. C., Solomon, M. J. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Role+of+isostaticity+and+load-bearing+microstructure+in+the+elasticity+of+yielded+colloidal+gels.">Role of isostaticity and load-bearing microstructure in the elasticity of yielded colloidal gels.</a> Proc. Natl. Acad. Sci. U.S.A. 109, 16029-16034 (2012).</li><li>Zemb, T., Linder, P. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Neutron,+X-rays,+and+Light.+Scattering+Methods+Applied+to+Soft+Condensed+Matter.">Neutron, X-rays, and Light. Scattering Methods Applied to Soft Condensed Matter.</a> Elsevier Science. 552, (2002).</li><li>Eberle, A. P. R., Porcar, L. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Flow-SANS+and+Rheo-SANS+applied+to+soft+matter.">Flow-SANS and Rheo-SANS applied to soft matter.</a> Curr. Opin. Coll. Inter. Sci. 17, 33-43 (2012).</li><li>Liberatore, M. W., Nettesheim, F., Wagner, N. J., Porcar, L. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Spatially+resolved+small-angle+neutron+scattering+in+the+1-2+plane:+A+study+of+shear-induced+phase-separating+wormlike+micelles.">Spatially resolved small-angle neutron scattering in the 1-2 plane: A study of shear-induced phase-separating wormlike micelles.</a> Phys. Rev. E. 73, (2006).</li><li>Porcar, L., Pozzo, D., Langenbucher, G., Moyer, J., Butler, P. D. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Rheo-small-angle+neutron+scattering+at+the+National+Institute+of+Standards+and+Technology+Center+for+Neutron+Research.">Rheo-small-angle neutron scattering at the National Institute of Standards and Technology Center for Neutron Research.</a> Rev. Sci. Instr. 82, (2011).</li><li>Lopez-Barron, C. R., Porcar, L., Eberle, A. P. R., Wagner, N. J. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Dynamics+of+Melting+and+Recrystallization+in+a+Polymeric+Micellar+Crystal+Subjected+to+Large+Amplitude+Oscillatory+Shear+Flow.">Dynamics of Melting and Recrystallization in a Polymeric Micellar Crystal Subjected to Large Amplitude Oscillatory Shear Flow.</a> Phys. Rev. Lett. 108, 258301-2510 (2012).</li><li>Rogers, S., Kohlbrecher, J., Lettinga, M. P. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=The+molecular+origin+of+stress+generation+in+worm-like+micelles,+using+a+rheo-SANS+LAOS+approach.">The molecular origin of stress generation in worm-like micelles, using a rheo-SANS LAOS approach.</a> Soft Matter. 8, 3831-3839 (2012).</li><li>Helgeson, M. E., Porcar, L., Lopez-Barron, C., Wagner, N. J. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Direct+Observation+of+Flow-Concentration+Coupling+in+a+Shear-Banding+Fluid.">Direct Observation of Flow-Concentration Coupling in a Shear-Banding Fluid.</a> Phys. Rev. Lett. 105, (2010).</li><li>Helgeson, M. E., Reichert, M. D., Hu, Y. T., Wagner, N. J. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Relating+shear+banding,+structure,+and+phase+behavior+in+wormlike+micellar+solutions.">Relating shear banding, structure, and phase behavior in wormlike micellar solutions.</a> Soft Matter. 5, 3858-3869 (2009).</li><li>Helgeson, M. E., Vasquez, P. A., Kaler, E. W., Wagner, N. J. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Rheology+and+spatially+resolved+structure+of+cetyltrimethylammonium+bromide+wormlike+micelles+through+the+shear+banding+transition.">Rheology and spatially resolved structure of cetyltrimethylammonium bromide wormlike micelles through the shear banding transition.</a> J. Rheol. 53, 727-756 (2009).</li><li>Liberatore, M. W., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Microstructure+and+shear+rheology+of+entangled+wormlike+micelles+in+solution.">Microstructure and shear rheology of entangled wormlike micelles in solution.</a> J. Rheol. 53, 441-458 (2009).</li><li>Maranzano, B. J., Wagner, N. J. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Flow-small+angle+neutron+scattering+measurements+of+colloidal+dispersion+microstructure+evolution+through+the+shear+thickening+transition.">Flow-small angle neutron scattering measurements of colloidal dispersion microstructure evolution through the shear thickening transition.</a> J. Chem. Phys. 117, 10291-10302 (2002).</li><li>Wagner, N. J., Ackerson, B. J. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Analysis+of+nonequilibrium+structures+of+shearing+colloidal+suspensions.">Analysis of nonequilibrium structures of shearing colloidal suspensions.</a> J. Chem. Phys. 97, 1473-1483 (1992).</li><li>Zhou, L., Vasquez, P. A., Cook, L. P., McKinley, G. H. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Modeling+the+inhomogeneous+response+and+formation+of+shear+bands+in+steady+and+transient+flows+of+entangled+liquids.">Modeling the inhomogeneous response and formation of shear bands in steady and transient flows of entangled liquids.</a> J. Rheol. 52, 591-623 (2008).</li><li>Spenley, N. A., Cates, M. E., McLeish, T. C. B. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Nonlinear+rheology+of+wormlike+micelles+Phys.">Nonlinear rheology of wormlike micelles Phys.</a> Rev. Lett. 71, 939-942 (1993).</li><li>Lopez-Barron, C., Gurnon, A. K., Porcar, L., Wagner, N. J. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Structural+Evolution+of+a+Model,+Shear-Bading+Wormlike+Micellar+Soution+during+Shear+Start+Up+and+Cessation.">Structural Evolution of a Model, Shear-Bading Wormlike Micellar Soution during Shear Start Up and Cessation.</a> Phys. Rev. Lett.. , (2013).</li></ol>

The authors have nothing to disclose.

A new instrument capable of measuring the microstructure of shearing complex fluids in the velocity-velocity gradient plane of shear via small angle neutron scattering is developed and validated. The shear cell design complements other instruments using radiation sources, such as X-ray and light scattering, as well as rheo-SANS instruments capable of characterizing the microstructure in the two other planes of shear (velocity-vorticity and velocity gradient-vorticity)8,10. This instrument...

Developing a scientific understanding of a natural phenomenon requires accurate and precise measurements. Metrology is also the basis of successful engineering and design of new processes and materials. Rheology is the science of the deformation and flow of matter. Rheology is central in our ability to process a wide variety of materials and is also used by product formulators to target specific material properties. Typical examples of the former include molding polymers or forming composites, whereas the latter includes the development of everyday consumer products such as paints, shampoos, and foods. Whether the viscosity of a molten polymer is controlled so that it can be effectively injection molded or the viscoelasticity of a shampoo is changed so it has the correct consistency for the consumer, the rheological properties are controlled by changing the formulation of the material1. The rheology of materials and products also depends on the structure in the fluid state and this structure ranges from the microscale to the nanoscale. Furthermore, this structure changes with the processing parameters, such as flow rate and time of flow, which challenges rheologists to measure the structure during flow. It is this challenge that is met, in part, by the novel instrumentation described in this article.
Novel techniques capable of probing the microstructure of soft materials under shear flow can benefit soft material product engineering and processing condition optimization. Many intriguing and long-standing challenges for the application of soft materials in a variety of industries and in fundamental science involve unusual flow behavior, such as shear thickening in colloidal suspensions2, shear and vorticity banding in wormlike micelles3, and heterogeneities inherent in the flow of colloidal gels4-6. Rheologists are constantly challenged to elucidate the microstructural origins of the nonlinearities in the rheological responses and sometimes even in the velocity field of shearing viscoelastic materials. This challenge requires simultaneous acquisition of the microstructure as a function of both the spatial location in the flow field and the time dependent behaviors, which has proven a formidable task for experimentalists.&#160;
Small angle neutron scattering (SANS) is particularly well suited for measuring the structure of complex fluids as it can probe materials that are opaque to light. Also selective deuteration can be used to provide contrast between components that may appear similar under X-ray scattering7. Furthermore, neutrons have an advantage over X-rays as there is no radiation damage of biological or other soft-matter samples. In the experiments illustrated here, cold neutrons generated by a reactor or a spallation source are collimated and illuminated upon a sample. The scattering intensity yields information about the structure of the material on length scales from the atomic to hundreds of nanometers (and with ultra-small angle neutron scattering up to tens of microns), but in the form of a Fourier transform of the real space structure. Therefore, interpretation of the data can be challenging and involves an inverse transform or comparison to microstructural models or simulations. More about SANS instrumentation, experiments, and contrast matching can be found on the tutorials posted on the web site of the Center for Neutron Science, www.cns.che.udel.edu.
Here we describe a shear cell designed to extend the SANS method to examine materials under flow. A recent overview of the general methodology and instrumentation, as well as a substantial literature review of recent applications can be found in reference8 and the cited references therein.&#160;A convenient and nearly ideal environment to probe fluid structure under shear flow with SANS is a narrow gap Couette geometry, also known as concentric cylinders9. This geometry applies a simple (i.e.&#160;laminar) shear flow to the sample while maintaining a sufficient unobstructed volume for the incident neutron beam. The application of flow breaks the symmetry of the microstructure; as such a complete characterization of the material microstructure under simple shear flow requires microstructural measurements in all three planes of shear. Two planes of shear may be investigated using the standard Couette geometry configuration (Figure 1a): the neutron beam is configured to travel along the velocity gradient direction and probe the velocity-vorticity (1-3) plane of shear (&#8220;radial&#8221; configuration); alternatively, the beam is collimated by a thin slit and aligned parallel to the flow direction, thereby probing the velocity gradient-vorticity (2-3) plane (&#8220;tangential&#8221; configuration). This instrument is available commercially and has been recently documented for examining complex fluids under shear10. The aforementioned review describes its use and that of related devices for structure-property determination across a broad range of materials and applications8. Time-resolved experiments, such as for oscillatory shear flows have also been reported11,12.
Often the most interesting and most important plane of flow is the velocity-velocity gradient (1-2) plane (Figure 1b) but it is also the most difficult to investigate as it requires special instrumentation. A custom shear cell has been designed to enable direct investigation of the velocity-velocity gradient (1-2) plane by SANS such that the neutron beam travels parallel to the vorticity axis of shear13-16. Measurements in the 1-2 plane of flow are critical to gaining a quantitative understanding for the shear viscosity because they elucidate the orientation of the structure relative to the flow direction15,17,18. This is important for materials such as polymers, self-assembled surfactants, colloids, and other complex fluids. In addition, it is possible to investigate the materials&#8217; microstructure as a function of position across the gap in the gradient direction of shear flow. With the addition of spatial resolution, the method provides a means for studying materials that exhibit microstructural changes along the gradient direction of shear. An example for which investigating changes in microstructure and composition along the gradient direction of flow is shear-banding. Shear banding is a phenomenon caused by a coupling between the microstructure and flow direction that results in an inhomogeneous flow field13. In this article, we describe the instrument, its assembly and the flow-SANS measurement technique as implemented at the NIST Center for Neutron Research (NCNR) at the National Institute of Standards and Technology (NIST) in Gaithersburg, MD. This sample environment is the result of a collaboration between the University of Delaware, NIST and the Institut Laue-Langevin (ILL), and has been successfully implemented at both ILL and NIST. For purposes of this article, where the SANS specific portions of the protocol are concerned, the technique is described as implemented at NIST. However, modifying those instrument specific details should be straightforward and the overall technique can be implemented on any SANS instrument for steady flow (section 5.1). In addition, instruments equipped with time-resolved SANS capabilities may also perform oscillatory shear flow-SANS experiments (section 5.2). Technical drawings of the shear cell components are provided as Figures 12-23. &#160;

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			<td>Deuterated Water (99.9%)</td>
			<td>Cambridge Isotopes</td>
			<td>7789-20-0</td>
			<td>83.3 wt % in formulation 
			D2O</td>
		</tr>
		<tr>
			<td>CTAB- Cetyl Trimethyl Ammonium Bromide&#160;</td>
			<td>Sigma-Aldrich</td>
			<td>57-09-0&#160;</td>
			<td>16.7 wt % in formulation 
			CH3(CH2)15N(Br)(CH3)3</td>
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		<tr>
			<td>1/16&#34; Allen wrench</td>
			<td></td>
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			<td></td>
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			<td>3/16&#34; Allen wrench</td>
			<td></td>
			<td></td>
			<td></td>
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		<tr>
			<td>3/8&#34; open end wrench</td>
			<td></td>
			<td></td>
			<td></td>
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		<tr>
			<td>tape</td>
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			<td></td>
			<td></td>
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			<td>thread seal tape</td>
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			<td style="font-size: 13px; line-height: 1.6em;">syringes (2)</td>
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measuring material microstructure under flow using 1-2 plane flow-small angle neutron scattering

A new small-angle neutron scattering (SANS) sample environment optimized for studying the microstructure of complex fluids under simple shear flow is presented. The SANS shear cell consists of a concentric cylinder Couette geometry that is sealed and rotating about a horizontal axis so that the vorticity direction of the flow field is aligned with the neutron beam enabling scattering from the 1-2 plane of shear (velocity-velocity gradient, respectively). This approach is an advance over previous shear cell sample environments as there is a strong coupling between the bulk rheology and microstructural features in the 1-2 plane of shear. Flow-instabilities, such as shear banding, can also be studied by spatially resolved measurements. This is accomplished in this sample environment by using a narrow aperture for the neutron beam and scanning along the velocity gradient direction. Time resolved experiments, such as flow start-ups and large amplitude oscillatory shear flow are also possible by synchronization of the shear motion and time-resolved detection of scattered neutrons. Representative results using the methods outlined here demonstrate the useful nature of spatial resolution for measuring the microstructure of a wormlike micelle solution that exhibits shear banding, a phenomenon that can only be investigated by resolving the structure along the velocity gradient direction. Finally, potential improvements to the current design are discussed along with suggestions for supplementary experiments as motivation for future experiments on a broad range of complex fluids in a variety of shear motions.

Representative results of a successful flow-SANS experiment are given in Figures 9, 10, and 11. These examples are from investigations made on a wormlike micelle solution (WLM) (Table 1) known to exhibit shear banding during certain conditions of shear. A complete discussion of the scientific findings can be found in references15-17.
Figure 10 represents results of a scattering pattern obtained under shear flow usin...

Watch this Scientific Journal Video about Measuring Material Microstructure Under Flow Using 1-2 Plane Flow-Small Angle Neutron Scattering at JoVE.com

Measuring Material Microstructure Under Flow Using 1-2 Plane Flow-Small Angle Neutron Scattering

A shear cell is developed for small-angle neutron scattering measurements in the velocity-velocity gradient plane of shear and is used to characterize complex fluids. Spatially resolved measurements in the velocity gradient direction are possible for studying shear-banding materials. Applications include investigations of colloidal dispersions, polymer solutions, and self-assembled structures.

A new small-angle neutron scattering (SANS) sample environment optimized for studying the microstructure of complex fluids under simple shear flow is ...

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14.2K 조회수.  University of Delaware.  전단 셀은 전단 속도 - 속도 구배 평면에서 소각 중성자 산란 측정을 위해 개발되고 복잡한 유체를 특성화하기 위해 사용된다. 속도 구배 방향으로 공간 분해 측정 전단 밴딩 물질을 연구 할 수 있습니다. 응용 프로그램은 콜로이드 분산의 조사, 폴리머 솔루션, 자기 조립 구조를 포함한다. 

비디오: Measuring Material Microstructure Under Flow Using 1-2 Plane Flow-Small Angle Neutron Scattering

Measuring Spatially- and Directionally-varying Light Scattering from Biological Material

Light interacts with an organism's integument on a variety of spatial scales. For example in an iridescent bird: nano-scale structures produce color; the milli-scale structure of barbs and barbules largely determines the directional pattern of reflected light; and through the macro-scale spatial structure of overlapping, curved feathers, these directional effects create the visual texture. Milli-scale and macro-scale effects determine where on the organism's body, and from what viewpoints and under what illumination, the iridescent colors are seen. Thus, the highly directional flash of brilliant color from the iridescent throat of a hummingbird is inadequately explained by its nano-scale structure alone and questions remain. From a given observation point, which milli-scale elements of the feather are oriented to reflect strongly? Do some species produce broader "windows" for observation of iridescence than others? These and similar questions may be asked about any organisms that have evolved a particular surface appearance for signaling, camouflage, or other reasons.
In order to study the directional patterns of light scattering from feathers, and their relationship to the bird's milli-scale morphology, we developed a protocol for measuring light scattered from biological materials using many high-resolution photographs taken with varying illumination and viewing directions. Since we measure scattered light as a function of direction, we can observe the characteristic features in the directional distribution of light scattered from that particular feather, and because barbs and barbules are resolved in our images, we can clearly attribute the directional features to these different milli-scale structures. Keeping the specimen intact preserves the gross-scale scattering behavior seen in nature. The method described here presents a generalized protocol for analyzing spatially- and directionally-varying light scattering from complex biological materials at multiple structural scales.

We present a non-destructive method for sampling spatial variation in the direction of light scattered from structurally complex materials. By keeping the material intact, we preserve gross-scale scattering behavior, while concurrently capturing fine-scale directional contributions with high-resolution imaging. Results are visualized in software at biologically-relevant positions and scales.

Light interacts with an organism's integument on a variety of spatial scales. For example in an iridescent bird: nano-scale structures produce color; the ...

Atom Probe Tomography Studies on the Cu(In,Ga)Se2 Grain Boundaries

Compared with the existent techniques, atom probe tomography is a unique technique able to chemically characterize the internal interfaces at the nanoscale and in three dimensions. Indeed, APT possesses high sensitivity (in the order of ppm) and high spatial resolution (sub nm).
Considerable efforts were done here to prepare an APT tip which contains the desired grain boundary with a known structure. Indeed, site-specific sample preparation using combined focused-ion-beam, electron backscatter diffraction, and transmission electron microscopy is presented in this work. This method allows selected grain boundaries with a known structure and location in Cu(In,Ga)Se2 thin-films to be studied by atom probe tomography.
Finally, we discuss the advantages and drawbacks of using the atom probe tomography technique to study the grain boundaries in Cu(In,Ga)Se2 thin-film solar cells.

Atom Probe Tomography Studies on the CuIn,GaSe2 Grain Boundaries

In this work, we describe the use of the atom-probe tomography technique for studying the grain boundaries of the absorber layer in a CIGS solar cell. A novel approach to prepare the atom probe tips containing the desired grain boundary with a known structure is also presented here.

Compared with the existent techniques, atom probe tomography is a unique technique able to chemically characterize the internal interfaces at the ...

Using Neutron Spin Echo Resolved Grazing Incidence Scattering to Investigate Organic Solar Cell Materials

The spin echo resolved grazing incidence scattering (SERGIS) technique has been used to probe the length-scales associated with irregularly shaped crystallites. Neutrons are passed through two well defined regions of magnetic field; one before and one after the sample. The two magnetic field regions have opposite polarity and are tuned such that neutrons travelling through both regions, without being perturbed, will undergo the same number of precessions in opposing directions. In this case the neutron precession in the second arm is said to &#34;echo&#34; the first, and the original polarization of the beam is preserved. If the neutron interacts with a sample and scatters elastically the path through the second arm is not the same as the first and the original polarization is not recovered. Depolarization of the neutron beam is a highly sensitive probe at very small angles (&#60;50&#160;&#956;rad) but still allows a high intensity, divergent beam to be used. The decrease in polarization of the beam reflected from the sample as compared to that from the reference sample can be directly related to structure within the sample.
In comparison to scattering observed in neutron reflection measurements the SERGIS signals are often weak and are unlikely to be observed if the in-plane structures within the sample under investigation are dilute, disordered, small in size and polydisperse or the neutron scattering contrast is low. Therefore, good results will most likely be obtained using the SERGIS technique if the sample being measured consist of thin films on a flat substrate and contain scattering features that contains a high density of moderately sized features (30 nm to 5 &#181;m) which scatter neutrons strongly or the features are arranged on a lattice. An advantage of the SERGIS technique is that it can probe structures in the plane of the sample.

Progress has been made in utilizing spin echo resolved grazing incidence scattering (SERGIS) as a neutron scattering technique to probe the length-scales in irregular samples. Crystallites of [6,6]-phenyl-C61-butyric acid methyl ester have been probed using the SERGIS technique and the results confirmed by optical and atomic force microscopy.

The spin echo resolved grazing incidence scattering (SERGIS) technique has been used to probe the length-scales associated with irregularly shaped ...

In Situ Neutron Powder Diffraction Using Custom-made Lithium-ion Batteries

Li-ion batteries are widely used in portable electronic devices and are considered as promising candidates for higher-energy applications such as electric vehicles.1,2 However, many challenges, such as energy density and battery lifetimes, need to be overcome before this particular battery technology can be widely implemented in such applications.3 This research is challenging, and we outline a method to address these challenges using in situ NPD to probe the crystal structure of electrodes undergoing electrochemical cycling (charge/discharge) in a battery. NPD data help determine the underlying structural mechanism responsible for a range of electrode properties, and this information can direct the development of better electrodes and batteries.
We briefly review six types of battery designs custom-made for NPD experiments and detail the method to construct the &#8216;roll-over&#8217; cell that we have successfully used on the high-intensity NPD instrument, WOMBAT, at the Australian Nuclear Science and Technology Organisation (ANSTO). The design considerations and materials used for cell construction are discussed in conjunction with aspects of the actual in situ NPD experiment and initial directions are presented on how to analyze such complex in situ data.

In Situ Neutron Powder Diffraction Using Custom-made Lithium-ion Batteries

We describe the design and construction of an electrochemical cell for the examination of electrode materials using in situ neutron powder diffraction (NPD). We briefly comment on alternate in situ NPD cell designs and discuss methods for the analysis of the corresponding in situ NPD data produced using this cell.

Li-ion batteries are widely used in portable electronic devices and are considered as promising candidates for higher-energy applications such as electric ...

Characterization of Full Set Material Constants and Their Temperature Dependence for Piezoelectric Materials Using Resonant Ultrasound Spectroscopy

During the operation of high power electromechanical devices, a temperature rise is unavoidable due to mechanical and electrical losses, causing the degradation of device performance. In order to evaluate such degradations using computer simulations, full matrix material properties at elevated temperatures are needed as inputs. It is extremely difficult to measure such data for ferroelectric materials due to their strong anisotropic nature and property variation among samples of different geometries. Because the degree of depolarization is boundary condition dependent, data obtained by the IEEE (Institute of Electrical and Electronics Engineers) impedance resonance technique, which requires several samples with drastically different geometries, usually lack self-consistency. The resonant ultrasound spectroscopy (RUS) technique allows the full set material constants to be measured using only one sample, which can eliminate errors caused by sample to sample variation. A detailed RUS procedure is demonstrated here using a lead zirconate titanate (PZT-4) piezoceramic sample. In the example, the complete set of material constants was measured from room temperature to 120 &#176;C. Measured free dielectric constants <img alt="Equation 1" src="/files/ftp_upload/53461/image001.jpg" /> and&#160;<img alt="Equation 2" src="/files/ftp_upload/53461/image002.jpg" /> were compared with calculated ones based on the measured full set data, and piezoelectric constants d15 and d33 were also calculated using different formulas. Excellent agreement was found in the entire range of temperatures, which confirmed the self-consistency of the data set obtained by the RUS.

This protocol describes the procedure of measuring the temperature dependence of the full set material constants of piezoelectric materials using resonant ultrasound spectroscopy (RUS).

During the operation of high power electromechanical devices, a temperature rise is unavoidable due to mechanical and electrical losses, causing the ...

Experimental Methods for Investigation of Shape Memory Based Elastocaloric Cooling Processes and Model Validation

Shape Memory Alloys (SMA) using elastocaloric cooling processes have the potential to be an environmentally friendly alternative to the conventional vapor compression based cooling process. Nickel-Titanium (Ni-Ti) based alloy systems, especially, show large elastocaloric effects. Furthermore, exhibit large latent heats which is a necessary material property for the development of an efficient solid-state based cooling process. A scientific test rig has been designed to investigate these processes and the elastocaloric effects in SMAs. The realized test rig enables independent control of an SMA&#39;s mechanical loading and unloading cycles, as well as conductive heat transfer between SMA cooling elements and a heat source/sink. The test rig is equipped with a comprehensive monitoring system capable of synchronized measurements of mechanical and thermal parameters. In addition to determining the process-dependent mechanical work, the system also enables measurement of thermal caloric aspects of the elastocaloric cooling effect through use of a high-performance infrared camera. This combination is of particular interest, because it allows illustrations of localization and rate effects &#8212; both important for efficient heat transfer from the medium to be cooled.
The work presented describes an experimental method to identify elastocaloric material properties in different materials and sample geometries. Furthermore, the test rig is used to investigate different cooling process variations. The introduced analysis methods enable a differentiated consideration of material, process and related boundary condition influences on the process efficiency. The comparison of the experimental data with the simulation results (of a thermomechanically coupled finite element model) allows for better understanding of the underlying physics of the elastocaloric effect. In addition, the experimental results, as well as the findings based on the simulation results, are used to improve the material properties.

Experimental methods for investigation of solid state cooling processes and characterization of elastocaloric material properties of Shape Memory Alloys (SMA) are presented. A custom-built test rig has been designed for controlling and comprehensive monitoring of elastocaloric cooling processes. Furthermore, it provides a validation platform for thermomechanically coupled modeling approaches.

Shape Memory Alloys (SMA) using elastocaloric cooling processes have the potential to be an environmentally friendly alternative to the conventional vapor ...

Dielectric RheoSANS &#8212; Simultaneous Interrogation of Impedance, Rheology and Small Angle Neutron Scattering of Complex Fluids

A procedure for the operation of a new dielectric RheoSANS instrument capable of simultaneous interrogation of the electrical, mechanical and microstructural properties of complex fluids is presented. The instrument consists of a Couette geometry contained within a modified forced convection oven mounted on a commercial rheometer. This instrument is available for use on the small angle neutron scattering (SANS) beamlines at the National Institute of Standards and Technology (NIST) Center for Neutron Research (NCNR). The Couette geometry is machined to be transparent to neutrons and provides for measurement of the electrical properties and microstructural properties of a sample confined between titanium cylinders while the sample undergoes arbitrary deformation. Synchronization of these measurements is enabled through the use of a customizable program that monitors and controls the execution of predetermined experimental protocols. Described here is a protocol to perform a flow sweep experiment where the shear rate is logarithmically stepped from a maximum value to a minimum value holding at each step for a specified period of time while frequency dependent dielectric measurements are made. Representative results are shown from a sample consisting of a gel composed of carbon black aggregates dispersed in propylene carbonate. As the gel undergoes steady shear, the carbon black network is mechanically deformed, which causes an initial decrease in conductivity associated with the breaking of bonds comprising the carbon black network. However, at higher shear rates, the conductivity recovers associated with the onset of shear thickening. Overall, these results demonstrate the utility of the simultaneous measurement of the rheo-electro-microstructural properties of these suspensions using the dielectric RheoSANS geometry.

Dielectric RheoSANS &amp;#8212; Simultaneous Interrogation of Impedance, Rheology and Small Angle Neutron Scattering of Complex Fluids

Here, we present a procedure for the measurement of simultaneous impedance, rheology and neutron scattering from soft matter materials under shear flow.

A procedure for the operation of a new dielectric RheoSANS instrument capable of simultaneous interrogation of the electrical, mechanical and ...

Scanning Light Scattering Profiler (SLPS) Based Methodology to Quantitatively Evaluate Forward and Backward Light Scattering from Intraocular Lenses

The scanning light scattering profiler (SLSP) methodology has been developed for the full-angle quantitative evaluation of forward and backward light scattering from intraocular lenses (IOLs) using goniophotometer principles. This protocol describes the SLSP platform and how it employs a 360&#176; rotational photodetector sensor that is scanned around an IOL sample while recording the intensity and location of scattered light as it passes through the IOL medium. The SLSP platform can be used to predict, non-clinically, the propensity for current and novel IOL designs and materials to induce light scatter. Non-clinical evaluation of light scattering properties of IOLs can significantly reduce the number of patient complaints related to unwanted glare, glistening, optical defects, poor image quality, and other phenomena associated with the unintended light scattering. Future studies should be conducted to correlate SLSP data with clinical results to help identify which measured light scatter is most problematic for patients that have undergone cataract surgery subsequent to IOL implantation.

Scanning Light Scattering Profiler SLPS Based Methodology to Quantitatively Evaluate Forward and Backward Light Scattering from Intraocular Lenses

This protocol describes the scanning light scattering profiler (SLSP) that enables the full-angle quantitative evaluation of forward and backward scattering of light from intraocular lenses (IOLs) using goniophotometer principles.

The scanning light scattering profiler (SLSP) methodology has been developed for the full-angle quantitative evaluation of forward and backward light ...

High-speed Continuous-wave Stimulated Brillouin Scattering Spectrometer for Material Analysis

Recent years have witnessed a significant increase in the use of spontaneous Brillouin spectrometers for non-contact analysis of soft matter, such as aqueous solutions and biomaterials, with fast acquisition times. Here, we discuss the assembly and operation of a Brillouin spectrometer that uses stimulated Brillouin scattering (SBS) to measure stimulated Brillouin gain (SBG) spectra of water and lipid emulsion-based tissue-like samples in transmission mode with &lt;10 MHz spectral-resolution and &lt;35 MHz Brillouin-shift measurement precision at &lt;100 ms. The spectrometer consists of two nearly counter-propagating continuous-wave (CW) narrow-linewidth lasers at 780 nm whose frequency detuning is scanned through the material Brillouin shift. By using an ultra-narrowband hot rubidium-85 vapor notch filter and a phase-sensitive detector, the signal-to-noise-ratio of the SBG signal is significantly enhanced compared to that obtained with existing CW-SBS spectrometers. This improvement enables measurement of SBG spectra with up to 100-fold faster acquisition times, thereby facilitating high spectral-resolution and high-precision Brillouin analysis of soft materials at high speed.

We describe the construction of a rapid continuous-wave-stimulated-Brillouin-scattering (CW-SBS) spectrometer. The spectrometer employs single-frequency diode-lasers and an atomic vapor notch-filter to acquire transmission spectra of turbid/non-turbid samples with high spectral-resolution at speeds up to 100-fold faster than those of existing CW-SBS spectrometers. This improvement enables high-speed Brillouin material analysis.

Recent years have witnessed a significant increase in the use of spontaneous Brillouin spectrometers for non-contact analysis of soft matter, such as ...

Measurement of Dynamic Force Acted on Water Strider Leg Jumping Upward by the PVDF Film Sensor

This study aimed to make an explanation for the phenomenon in nature that water strider usually jumps or glides on the water surface easily but quickly, with its peak locomotion speed reaching 150 cm/s. First of all, we observed the microstructure and hierarchy of water strider legs using the scanning electron microscope. On the basis of the observed morphology of the legs, a theoretical model of the detachment from water surface was established, which explained water striders' capability to slide on water surface effortlessly in terms of energy reduction. Secondly, a dynamic force measurement system was devised using the PVDF film sensor with excellent sensitivity, which could detect the whole interaction process. Subsequently, a single leg in contact with water was pulled upward at different speeds, and the adhesion force was measured at the same time. The results of the departing experiment suggested a deep understanding of the fast jumping of water striders.

The protocol here is dedicated to investigating the free and quick maneuvering of water strider on water surface. The protocol includes observing the microstructure of legs and measuring the adhesion force when departing from water surface at different speeds.

This study aimed to make an explanation for the phenomenon in nature that water strider usually jumps or glides on the water surface easily but quickly, ...