Name: Dielectric RheoSANS — Simultaneous Interrogation of Impedance, Rheology and Small Angle Neutron Scattering of Complex Fluids (Video) | JoVE Journal
Uploaded: 2017-04-10T12:30:00.000+00:00
Duration: 7 min 51 s
Description: Learn simultaneous impedance, rheology, and neutron scattering for soft matter research using conductive carbon black suspensions. This technique reveals the intrinsic link between microstructure and macroscopic properties.

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5 minutes

The authors would like to acknowledge the NIST Center for Neutron Research CNS cooperative agreement number #70NANB12H239 grant for partial funding during this time period as well as the National Research Council for support. Certain commercial equipment, instruments, or materials are identified in this paper in order to specify the experimental procedure adequately. Such identification is not intended to imply recommendation or endorsement by the National Institute of Standards and Technology, nor is it intended to imply that the materials or equipment identified are necessarily the best available for the purpose.

1. Mounting the Rheometer onto the SANS Beamline
NOTE: See Figure 1 for definitions of named components.
<ol>
	<li>Ensure that the power to the rheometer is off, the transducer is locked and the motor air bearing protector is installed. Turn off the neutron beam, and close the oven door.</li>
	<li>Install the large base plate onto the table, remove the snout, install the window, and secure the 4 eyelets to the mounting brackets on the rheometer's crane adapter such that the cables do not tangle and are not twisted.</li>
	<li>Using the crane, lift the rheometer and maneuver it from the rheometer table to rest centered on the table with the LCD screen of the rheometer facing outward, taking care to guide the cables to minimize tangling.</li>
	<li>Using the SANS control software, send the table to the minimum Z position.</li>
	<li>Remove the rheometers' crane adapter and lift away from the platform using the crane.</li>
</ol>
2. Dielectric Cell Assembly
NOTE: See Figure 2 for definitions of named components.
<ol>
	<li>Ensure that the power to the rheometer is off, the transducer is locked and the motor air bearing protector is installed. Before use, clean the dielectric cup and bob assemblies using detergent solution followed by several deionized water rinses, and allow to fully dry.</li>
	<li>Open the oven door, unlock the transducer and remove the motor bearing lock. Mount the dielectric geometry and dielectric bob assembly onto the upper and lower tool mounts of the rheometer. Loosen both set screws on the dielectric geometry using a 2-mm Allen key and place the dielectric cup assembly so that it is mounted on the dielectric geometry.</li>
	<li>Using the rheometer control software, zero the gap from the sample geometry drop-down menu, and apply 10 N normal force using the axial force drop-down menu. Under compression, tighten screws using a 3-mm Allen key until the dielectric cup assembly is fully secured to the dielectric geometry.</li>
	<li>Set the gap to the measurement gap using the rheometer control software, and close the oven door. Ensure that the oven can fully enclose the dielectric cell with adequate vertical clearance on the top and bottom of the geometry. If a height adjustment is needed, adjust the set screw so that the oven enclosure fits with adequate tolerance around the dielectric cell. Adequate clearance is achieved when the dielectric geometry fits within the oven and can undergo a full revolution without touching the oven walls.</li>
	<li>Remove both the dielectric bob assembly and the dielectric cup assembly/dielectric geometry as one piece and replace with the rheometer alignment tool on the lower tool head.</li>
</ol>
3. Install the Slip Ring
NOTE: See Figure 3 for step-by-step pictorial summary.
<ol>
	<li>Install the wire baffle onto the shaft of the dielectric geometry and connect the dielectric cup connector to the slip ring connector.</li>
	<li>Hold the slip ring so that it is concentric with the shaft of the dielectric cup assembly/dielectric geometry but above the flange on the dielectric geometry. Place the slip ring adapters (x2) such that their nobs insert into the holes drilled into the dielectric geometry and their base rests on the dielectric geometry flange.</li>
	<li>Gently slide the slip ring over the slip ring adapters. The slip ring should slide effortlessly around the slip ring adapters holding them in place.</li>
</ol>
4. Alignment of the Rheometer
NOTE: See Figure 4 for schematic of beam path.
<ol>
	<li>Close the oven around the rheometer alignment tool. Install the truncated snout and the sample aperture (1 mm wide × 8 mm tall), and using rheometer control software, set the geometry displacement angle to 0.49 rad in the motor control drop-down menu.</li>
	<li>Using the SANS instrument control software, ensure that all the neutron guides are removed, and open the oven door so that the laser is visible. Perform a rough alignment of the rheometer by changing the height and angle of the table from the SANS instrument control software so that the beam passes through the oven and crosses through the slit in the center of the rheometer alignment tool.</li>
	<li>Using the SANS instrument control software, adjust the height of the table and its rotation to optimize laser alignment. Note the rheometer is aligned when the laser beam passes through the slit in the rheometer alignment tool with the geometry displacement set at 0.49 rad without impinging on its walls and the beam passes through the center line in the oven.</li>
</ol>
5. Calibration of the SANS Instrument
<ol>
	<li>Once the desired SANS instrument configuration is aligned by the instrument scientist, measure the open beam transmission, empty cell scattering, and dark current scattering measurements.
	<ol>
		<li>Perform the open beam transmission measurement by performing a beam transmission measurement at the desired detector position for 3 min.</li>
		<li>Perform the empty cell scattering measurement by installing the dielectric geometry and measuring a scattering measurement at the desired detector position.</li>
		<li>Perform the dark current scattering measurement using a 3-mm thick piece of cadmium that totally attenuates the main beam scattering signal.</li>
	</ol>
	</li>
</ol>
6. Connecting the Electric Components
<ol>
	<li>Set the gap using the LCD screen to 100 mm.</li>
	<li>Remove the rheometer alignment tool from the bottom tool flange. Reinstall the dielectric bob assembly on the upper tool head and the dielectric cup assembly/dielectric geometry/slip ring assembly onto the lower tool head as one piece and re-zero the gap.</li>
	<li>Ensure that the carbon brush assembly is secured to the carbon brush adapter using screws, and secure the carbon brush adapter and carbon brush assembly to the rheometer using screws. Ensure that the carbon brushes on the carbon brush assembly mate with the grooved metal rings of the slip ring. This ensures maintenance of the electrical contact.</li>
	<li>Connect the female pin connectors on the carbon brush assembly and the dielectric bob assembly to the male pin connectors of the top and bottom bus bars respectively. Ensure that the labeled shielded BNC cables connected to the bus bars and terminating at the LCR meter are installed in their corresponding BNC connectors.</li>
	<li>Connect the BNC cable labeled "TO SANS" to the BNC cable connected to the DAQ card labeled "AO0". Connect the BNC cable labeled "FROM SANS" to the BNC cable connected to the DAQ card labeled "AI0". Connect the BNC cable labeled "TRIGGER" to the BNC cable connected to the DAQ card labeled "AO1". Connect the BNC cable connected to the 15 pin connector on the back of the rheometer to the BNC cable labeled "AI3". Ensure that the LCR meter and rheometer are communicating with the control computer.</li>
</ol>
7. Preparing the Instrument for a Measurement
<ol>
	<li>Open the oven, set the gap to 100 mm, and load 4 mL of the carbon black dispersion in propylene carbonate into the temperature equilibrated dielectric cup assembly, taking care to minimize sample left on the cup wall.</li>
	<li>Lower the geometry to 40 mm using the front LCD screen. Set the velocity on the rheometer control software using the motor control settings to 1 rad/s. Using the slew option on the rheometer, lower the dielectric bob assembly until the gap distance is at 0.5 mm.</li>
	<li>Using the equipment software, go to dielectric geometry measurement gap, and set the motor velocity on rheometer control software using the motor control settings to 0 rad/s. At this stage, the sample is loaded. 
	Note: Check the sample fill level once more to ensure that the sample level fills all the way up the Couette wall without overfilling.</li>
	<li>Install the solvent trap by filling the inner dielectric bob assembly wall with the desired solvent and place the solvent trap on the rim of the dielectric cup assembly.</li>
</ol>
8. Running the Dielectric RheoSANS Experiment
<ol>
	<li>Configure code labeled "TA_ARES_FlowSweep.vi". A GUI will appear with modifiable fields that specify the experimental run conditions of the dielectric RheoSANS experiment. Set these fields in the following order.
	<ol>
		<li>Specify a path for the log file to and the base name of the log file. Run the code by pressing the "Run" arrow button on the menu bar.</li>
		<li>Select rheological parameters — the starting shear rate (25 rad/s), ending shear rate (1 rad/s), the number of shear rate points (6) and whether the points should be logarithmically or linear spaced (radio button). Select temperature to 25 °C for this experiment. Select preshear conditions (if desired, enable radio button to "ON") — in this experiment, use a 25 rad/s preshear for 600 s with a 300 s wait time after the preshear step.</li>
		<li>Specify time per shear rate and collection rate. Enable handshaking radio button. On test parameters tab select logarithmic or linear sweep — if radio button is green, a list of N number of points will be logarithmically spaced from min shear rate to max shear rate.</li>
		<li>Specify discrete shear rates and times via the "Discrete Values" tab if desired. Select the number of frequency points, the frequency minimum and the frequency maximum default. Set the time dependent frequency — specifies the desired time dependent frequency for all shear rates. Set the time for steady state — sets the amount of time that the code will measure dielectric parameters at a fixed frequency as a function of time for each shear rate.</li>
		<li>Specify the signal type and amplitude. Specify the number of cycles to average and the measurement time.</li>
	</ol>
	</li>
	<li>Turn on autoLogging on the SANS computer. Set the SANS configuration. Select the configuration and specify the run time to be at least 1 min longer than the total time contained within the shear rate list in the code. 
	Note: When the configuration is achieved VIPER should read "dio stat 16" which indicates that it will be waiting for the analogue signal from the data acquisition card to change.</li>
	<li>Configuring the rheometer control software. In the experiment tab, Press "Open Procedure File" in the "Procedure" drop down menu. Navigate to the procedure file labeled "Dielectric RheoSANS Script File". Ensure that rheometer is ready to execute experiment.</li>
	<li>When the SANS is ready, ensure control software is configured and rheometer control software script file is open, press "Parameters Set". This triggers execution of the specified experiment and all data should be logged throughout the preprogrammed sample run.</li>
</ol>
9. End of Experiment
<ol>
	<li>Turn off the neutron beam and disable auto-logging. Unload the sample and remove the dielectric cup and bob assemblies from the rheometer. Install the motor air bearing protector and lock the transducer.</li>
	<li>Power down the computer, LCR meter, and rheometer power supplies. Disconnect the air line. Disconnect all BNC cables and reinstall the crane lift onto the rheometer.</li>
	<li>Uninstall the truncated snout. Reinstall the rheometer's crane adapter. Lift the rheometer from the table and place onto the rheometer table ensuring that the cables remain untangled.</li>
</ol>
<img alt="Neutron scattering setup showing transducer lock, rheometer, detector tube in spectroscopy lab." src="/files/ftp_upload/55318/55318fig1.jpg" data-altupdatedat="1788250015000" data-alt="Figure 1"> 
Figure 1: a.)-e.) Pictures of Components of the SANS Beamline and the Rheometer necessary to Install Rheometer on the Beamline that are Labelled and Defined Below. <a href="http://cloudfront.jove.com/files/ftp_upload/55318/55318fig1large.jpg" target="_blank">Please click here to view a larger version of this figure.</a>
<img alt="High voltage capacitor components; dielectric assembly, carbon brush, slip ring; experiment setup." src="/files/ftp_upload/55318/55318fig2.jpg" data-altupdatedat="1788250015000" data-alt="Figure 2"> 
Figure 2: Pictures of Components Dielectric RheoSANS Geometry with Labels Defining Terms Below. <a href="http://cloudfront.jove.com/files/ftp_upload/55318/55318fig2large.jpg" target="_blank">Please click here to view a larger version of this figure.</a>
<img alt="Rheometer assembly diagram with torque, shear measurements; neutron scattering setup for LCR analysis." src="/files/ftp_upload/55318/55318fig3.jpg" data-altupdatedat="1788250015000" data-alt="Figure 3"> 
Figure 3: a.-d.) Pictures of Procedure for Installing the Slip-ring onto the Dielectric RheoSANS Geometry, and e.) Picture of Fully Assembled Dielectric RheoSANS Geometry. <a href="http://cloudfront.jove.com/files/ftp_upload/55318/55318fig3large.jpg" target="_blank">Please click here to view a larger version of this figure.</a>
<img alt="Neutron flight path diagram; beam entry/exit and geometry cross-section for scattering analysis." src="/files/ftp_upload/55318/55318fig4.jpg" data-altupdatedat="1788250015000" data-alt="Figure 4"> 
Figure 4: Schematic of Beam Path through Oven Geometry and Dielectric RheoSANS Geometry. <a href="http://cloudfront.jove.com/files/ftp_upload/55318/55318fig4large.jpg" target="_blank">Please click here to view a larger version of this figure.</a>

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The authors have nothing to disclose.

A dielectric RheoSANS experiment measures simultaneously the rheological, electrical and microstructural responses of a material as it undergoes a predefined deformation. The example shown here is an electrically conductive carbon black suspension that forms the conductive additive used in electrochemical flow cells. The dielectric RheoSANS instrument enables the interrogation of the radial plane of shear within a narrow gap Couette cell without compromising the fidelity of either the electrical or rheological measuremen...

Measurement of macroscopic properties are often used to gain fundamental insight into the nature of colloidal materials and self-assembled systems, usually with the goal of developing understanding in order to improve formulation performance. In particular, the field of rheology, which measures a fluid&#39;s dynamic response to an applied stress or deformation, provides valuable insight into colloidal behavior both under equilibrium conditions and also far from equilibrium, such as during processing1 Rheological tests of consumer and industrial fluids, gels, and glasses can also be used to measure rheological parameters, such as viscosity, that are targeted by formulators. While rheology is a powerful probe of material properties, it is an indirect measurement of colloidal information at the microscopic level, such that our understanding of fundamental colloidal behavior can be greatly enhanced by combining rheological measurements with complementary techniques.
One such orthogonal technique is impedance spectroscopy. Impedance spectroscopy is a bulk probe of dielectric relaxation behavior, which measures the response of a material to an applied oscillating electric field.2 The impedance spectrum results from electrical relaxation modes that are active within the material including charge transport and polarization.3,4 These measurements provide additional evidence for colloidal behavior particularly when combined with rheology.5 Therefore, the combination of these techniques is especially relevant when probing charged colloidal dispersions, proteins, ionic surfactants, nanocomposites, and other systems.6,7
A fundamental interest in investigations of colloidal behavior is the material&#39;s microstructure. The microstructure of a colloidal fluid is thought to encode all of the information necessary to reconstitute both its rheological and electrical behavior. Fundamentally, we seek to measure a snapshot of the nanoscale microstructural features that lead to a measured material response. Due to the complicated nature of many complex fluids&#39; dependence on their process history, much of the effort on microstructural characterization has focused on making in situ measurements of the material as it undergoes deformation. This has challenged experimentalists to devise methods to be able to make measurements of nano-sized particles under for example steady shear, where the velocities of the particles have made direct visualization intrinsically challenging. Direct measurement of material microstructure under flow has taken on many forms ranging from rheo-optics, rheo-microscopy and even rheo-NMR.8,9,10 Small angle scattering methods, and in particular small angle neutron scattering (SANS) techniques, have proven themselves effective at measuring the time-averaged microstructure of samples at steady state in a bulk shear field including all three planes of shear.11,12,13 However, new data acquisition techniques have allowed structural transients to be captured with time resolution as fine as 10 ms.14 Indeed combining rheology with various in situ scattering methods has proven invaluable in hundreds of recent studies.15
An emerging engineering challenge is the use of colloidal suspensions as conductive additives in semi-solid flow battery electrodes.16 In this application, conductive colloidal particles must maintain an electrically percolated network while the material is pumped through an electrochemical flow cell. The performance demands on these materials require that they maintain high conductivity without detrimental effect on the rheological performance over a wide range of shear rates.17 It is therefore highly desirable to be able to make measurements of the colloidal behavior under steady and time-dependent shear conditions in order to quantify and characterize the underlying rheological and electrical response of these materials far from their equilibrium state. A significant complicating factor that has hindered further theoretical development in this regard is the thixotropic nature of carbon black slurries.18 These history dependent rheological and electrical properties make experiments notoriously difficult to reproduce; thus, making it difficult to compare data sets measured using varying protocols. Furthermore, to date there is no single geometry capable of performing all three, dielectric, rheological, and microstructural characterizations, simultaneously. Simultaneous measurement is important as the flow can change the structure, such that rest measurements of processed materials may not provide accurate indications of the properties under flow, which are more relevant for their use. Additionally, as many of the measured properties of carbon black slurries are geometry dependent, there are complications with comparing data obtained from the same sample on different instruments.19
In order to meet this challenge in metrology, we have developed a new dielectric RheoSANS geometry at the NIST Center for Neutron Research and the University of Delaware capable of in situ impedance spectroscopy, rheology and SANS measurements of a material under arbitrary deformation on a commercial strain controlled rheometer. This is enabled by developing a Couette geometry capable of measuring the microstructural, electrical and rheological response of a material confined between the gap of two concentric cylinders. As the outer cylinder spins, torque imposed by the deformation of the sample is measured on the inner cylinder and the impedance measurement is made radially across the gap. The cylinders are machined from titanium so as to be transparent to neutrons and robust enough to withstand the shear stress experienced in the rheometer. We perform the SANS measurement through the radial position of the Couette, and have demonstrated that it is possible to measure high quality SANS patterns from the sample undergoing deformation. In this way, all three measurements are made on the same region of interest in the sample as it undergoes a well-defined deformation profile. The goal of this article is to describe the dielectric Couette geometry, its installation onto the RheoSANS instrument, and the successful execution of a simultaneous measurement. This rheometer is available at the NIST Center for Neutron Research at the National Institute of Standards and Technology. It has been designed to work on the NG-7 SANS beam line. We have provided drawings and a detailed description of the custom components that have been machined and assembled in order to enable this measurement.

<table><tbody><tr><td>ARES G2 Rheometer</td><td>TA Instruments</td><td>401000.501</td><td>Rheometer</td></tr><tr><td>ARES G2-DETA ACCY Kit</td><td>TA Instruments</td><td>402551.901</td><td>BNC Connectors</td></tr><tr><td>Geometry ARES 25 mm DETA</td><td>TA Instruments</td><td>402553.901</td><td>Dielectric Geometry</td></tr><tr><td>ARES G2 Forced Convection Oven</td><td>TA Instruments</td><td>401892.901</td><td>FCO</td></tr><tr><td>Agilent E4980A LCR Meter</td><td>TA Instruments</td><td>613.04946</td><td>LCR Meter</td></tr><tr><td>USB-6001</td><td>National Instruments</td><td>NI USB-6001</td><td>Data Acquisiton Card</td></tr><tr><td>Vulcan XC72R</td><td>Cabot</td><td>Vulcan XC72R</td><td></td></tr><tr><td>Propylene Carbonate</td><td>Aldrich</td><td>310328</td><td></td></tr><tr><td>LabVIEW&amp;nbsp; System Design Software</td><td>National Instruments</td><td>776671-35</td><td>Control Software&amp;nbsp;</td></tr></tbody></table>

dielectric rheosans &#8212; simultaneous interrogation of impedance, rheology and small angle neutron scattering of complex fluids

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.

Representative results from a dielectric RheoSANS experiment are shown in Figure 5 and 6. These data are taken on a suspension of conductive carbon black in propylene carbonate. These aggregates flocculate due to attractive interactions at relatively low solids loadings forming gels that are electrically conducting. The rheological and conductivity responses of such suspensions are an active area of research and current investigations seek to understand t...

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 ...

The overall goal of this procedure is to measure the simultaneous impedance, rheology and neutron scattering from a conductive carbon black suspension as it undergoes deformation in response to an applied shear field. This method can help answer key questions in the soft matter and applied materials fields about the intrinsic link between material microstructure and macroscopic properties such as conductivity and rheology. The main advantage of this technique is that the measurements are performed simultaneously, allowing the entire time evolution of mechanical, structural and electrical response to be reconstructed and compared.The implications of this technique extend to the development of advanced conductive materials for electrochemical and optoelectronic applications. Visual demonstration of this method is critical owing to the complex nature of the experimental protocol. NIST professionals will assist in some key aspects of the experiment.Before beginning the procedure, ensure that the neutron beam and the rheometer are both off, the transducer is locked and the motor bearing lock is installed. Clean the dielectric cup and bob assemblies with a detergent solution. Thoroughly rinse the assemblies with deionized water and allow the assembles to air dry.Unlock the transducer and remove the motor bearing lock. Then, turn on the rheometer and start the control software. Mount the dielectric geometry and bob assembly on the lower and upper tool mounts of the rheometer respectively.Use a three milometer allen key to loosen the dielectric geometry set screws. Mount the cup assembly on the dielectric geometry. Then, in the rheometer control software, zero the gap and apply 10 newtons of normal force.Under this axial compression, tighten the set screws to secure the cup assembly to the geometry. Then, set the gap to the measurement gap width. Close the oven door and verify that the oven fully encloses the dielectric cell assembly.With sufficient vertical clearance above and below the geometry to allow a full revolution without contacting the oven walls. Open the oven and remove the dielectric assemblies. Thread the geometry shaft through the slip ring and join the dielectric cup and slip ring connectors.While holding the slip ring, concentric with the shaft above the flange, secure the slip ring adapters on top of the flange. Gently slide the slip ring down to fit over the adapters. Next, mount the rheometer alignment tool on the lower tool head.Install the truncated snout and set the sample aperture to one millimeter by eight millimeters. In the rheometer control software, set the geometry displacement angle to 0.49 radians. Then in the SANS control software, verify that all neutron guides have been removed.Open the oven door to view the beam alignment laser. Use the SANS software to adjust the height and angle of the sample stage until the laser beam is directed along the oven center line and though the sample aperture without intersecting the aperture walls. After rheometer alignment, remove the alignment tool and perform a series of SANS measurements to calibrate the instrument.Then, use the rheometer LCD screen, to set the gap to 100 millimeters. Mount the dielectric cell with the bob assembly on the upper tool head and the cup geometry and slip ring assembly on the lower tool head. Use the instrument software to zero the gap.Next, mount the carbon brush assembly on the brush adapter. Line up the carbon brushes with the grooves on the slip ring and then secure the adapter to the rheometer with screws. Connect the carbon brush assembly to the top bus bar and the dielectric bob assembly to the bottom bus bar.Check the connections of the shielded BNC cables to the bus bars and the LCR meter. Connect the SANS and Trigger BNC cables to the DAQ card. Connect the rheometer to the DAQ card.Verify that the LCR meter and the rheometer are successfully communicating with the computer. Before loading the sample, verify that the gap is set to 100 millimeters. Then, load four millimeters of a carbon black dispersion in propylene carbonate into the dielectric cup assembly, minimizing the amount of sample left on the cup wall.Lower the geometry to 40 millimeter. Then in the rheometer control software, set the motor velocity to one radian per second. Lower the dielectric bob assembly to achieve a gap width of 0.1 millimeters and then set the motor velocity to zero radians per second.Check that the sample levels has reached the Couette wall but is not over filled. Fill the inner dielectric bob assembly with the chosen solvent for the experiment. Place the solvent trap on the rim of the dielectric cup assembly.Next, configure the virtual instrument file for the desired experimental conditions. Set the appropriate run times and procedures for the SANS instrument and the rheometer. Click parameters set to execute the experiment.A conductive carbon black suspension was evaluated by RheoSANS. Rheology, dielectric data and neutron scattering were measured continuously as the shear rate decreased logarithmically in steps, holding at each step for a specific time interval. The steady state, rheological dielectric and SANS data were processed and analyzed at each shear rate step.A period of decreasing conductivity and effective volume fraction with increasing shear rate was attributed to yielding of the microscopic gel. A subsequent period of increasing conductivity and decreasing effective volume fraction with increasing shear rate was attributed to shear thickening caused by hydrodynamic forces drawing aggregated particles together. Micro structural transitions at higher shear rates were represented with two dimensional plots.Dielectric RheoSANS provides a flexible platform capable of the interrogation of nonequilibrium behavior of soft matter systems. Using a wide variety of potential experimental protocols, this instrument is available for broad use by the scientific community at the NCNR.

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Research

JoVE Journal

Engineering

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Learn simultaneous impedance, rheology, and neutron scattering for soft matter research using conductive carbon black suspensions. This technique reveals the intrinsic link between microstructure and macroscopic properties.

Dielectric RheoSANS — Simultaneous Interrogation of Impedance, Rheology and Small Angle Neutron Scattering of Complex Fluids

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