This research work was supported by the National Science Foundation [CBET-1904921] and the National Institutes of Health [NIH R01CA236350] to H. M.

NOTE: All the buffers and the chemical reagents used in this protocol are listed in the Table Materials.
1. Preparation of the shear force microscope
NOTE: The shear force microscope contains two parts, a reaction unit (homogenizer) and a detection unit (fluorescence microscope). The magnification of the eyepiece is 10x, and the magnification of the objective lens (air) is 4x.
<ol>
	<li>Assemble the homogenizer and the microscope on a mounting table. Wear goggles and turn on the fluorescence microscope, and then adjust the homogenizer to make sure that the excitation light beam of an appropriate wavelength (here, 488 nm was used) passes through the center of the dispersing tip of the homogenizer.</li>
	<li>Prepare a flat-bottomed reaction chamber that is 5 cm in height and 1.5 cm2 x 1.5 cm2 in cross-section. To reduce the background, ensure that the selected chamber material does not fluoresce, such as glasses (some plastics have fluorescence).</li>
	<li>Choose an appropriate homogenizer dispersing tip that can provide the desired shear force. 
	NOTE: The shear rate is dependent on the distance between the rotor and stator at a fixed rotating speed11 according to the following equation: 
	<img alt="Equation 1" src="/files/ftp_upload/63741/63741eq01.jpg" style="margin: auto;" /> 
	where &#181; is the dynamic viscosity of water at 20 &#176;C; D is the inner diameter of the stator; d is the outer diameter of the rotor, and V is the shear speed (rpm/s).</li>
	<li>Clamp the reaction chamber on the sample stage of the fluorescence microscope, and then adjust the chamber to hold the dispersing tip of the homogenizer (Figure 1). Make sure the dispersing tip is slightly above (~1&#160;mm) the bottom surface of the reaction chamber.</li>
	<li>Adjust the vertical position of the homogenizer and the chamber together to ensure the focus of the microscope is on the surface of the dispersing tip. Then, adjust the horizontal position of the dispersing tip to ensure that the detection area (field of view) is set between the rotor and stator (Figure 1).</li>
	<li>Switch on the fluorescence channels according to the fluorescent dye used in the experiment.</li>
	<li>Before the high-speed shearing experiment, use deionized (DI) water to test the shearing with a low shearing speed (e.g., 2,000 rpm) to ensure the dispersing tip can work appropriately without touching the reaction chamber.</li>
</ol>
2. Unfolding i-motifs with and without ligands
<ol>
	<li>Prepare a human telomeric i-motif DNA (Table of Materials) labeled with a dye and a quencher at its two ends, respectively, in DI water, as described in Hu et al.11. 
	NOTE: i-motif containing sequence: 5&#39;-TAA CCC TAA CCC TAA CCC TAA CCC TAA.</li>
	<li>Dilute the DNA to 5 &#181;M in the 30 mM MES buffer at pH 5.5 or pH 7.4. To the DNA solution, add ligand L2H2-4OTD, which was synthesized according to Abraham Punnoose et al.13, in a concentration range of 0-60 &#181;M. Mix the solution gently for 10 min to fold the i-motif structures without light.</li>
	<li>Check and minimize the background fluorescence intensity of the reaction chamber that is filled with deionized DI water using the fluorescent microscope without shearing. An easy way to minimize the background fluorescence is to wash the reaction chamber with DI water. The background fluorescence value needs to be subtracted in the data analyses later. 
	NOTE: Stray light should be avoided from this step onwards.</li>
	<li>Set the parameters of the CCD camera using the software. The recommended parameters are as follows: exposure time = 0.5 s, CCD sensitivity = 1600, and recording time = 20 min.</li>
	<li>Using a long pipet, add the DNA solution into the empty and clean reaction chamber. Cover the reaction chamber with a black box. Then, start the homogenizer to perform shearing at a selected shear rate ranging from 9,724 s&#8722;1 to 97,245 s&#8722;1 (selected using the software associated with the homogenizer) for 20 min with the CCD camera turned on to record the data.</li>
	<li>After the experiment, remove the chamber and wash it with DI water.</li>
</ol>
3. Shear force-actuated click reaction
<ol>
	<li>Prepare i-motif DNA in DI water. Incubate 10 &#181;M i-motif DNA in 300 &#181;L of 30 mM Tris buffer (pH 7.4) supplemented with 150 &#181;M CuCl and 300 &#181;M ascorbic acid for 10 min to fold the i-motif structures (all concentrations are final concentrations in the solution). 
	NOTE: CuCl is the catalyst of the click reaction. Ascorbic acid will prevent copper (I) oxidization.</li>
	<li>Ultra-filtrate the solution with an ultrafiltration device at a centrifugal force of 14,300 x g. Replenish the solution to ~500 &#181;L with 30 mM Tris buffer (pH 7.4) supplemented with 300 &#181;M ascorbic acid after each filtration.</li>
	<li>Repeat the filtration 3x.</li>
	<li>Collect the residual solution and make a final volume of 300 &#181;L by adding 30 mM Tris (pH 7.4) supplemented with 300 &#181;M ascorbic acid along with 20 &#181;M Calfluor 488 azide, 20 &#181;M HPG, and 10 &#181;M TBTA. Once the reagents are added, move the solution to the darkroom. 
	NOTE: Light should be avoided after this step.</li>
	<li>Check and minimize the background fluorescence intensity of the reaction chamber filled with DI water using the microscope before the shearing experiments. An easy way to minimize the background fluorescence is to wash the reaction chamber with DI water.</li>
	<li>Add the DNA solution into the empty reaction chamber with a long pipet, and then start the homogenizer shearing at a shear rate of 63,209 s&#8722;1 for 20 min with the CCD camera turned on.</li>
	<li>After the experiment, remove the chamber and wash it with DI water.</li>
</ol>

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	<li>Neuman, K. C., Nagy, A. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Single-molecule+force+spectroscopy:+Optical+tweezers,+magnetic+tweezers+and+atomic+force+microscopy.">Single-molecule force spectroscopy: Optical tweezers, magnetic tweezers and atomic force microscopy.</a> Nature Methods. 5 (6), 491-505 (2008).</li><li>Woodside, M. T., 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=Nanomechanical+measurements+of+the+sequence-dependent+folding+landscapes+of+single+nucleic+acid+hairpins.">Nanomechanical measurements of the sequence-dependent folding landscapes of single nucleic acid hairpins.</a> Proceedings of the National Academy of Sciences of the United States of America. 103 (16), 6190-6195 (2006).</li><li>Grandbois, M., Beyer, M., Rief, M., Clausen-Schaumann, H., Gaub, H. E. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=How+strong+is+a+covalent+bond.">How strong is a covalent bond.</a> Science. 283 (5408), 1727-1730 (1999).</li><li>Strick, T. R., Allemand, J. F., Bensimon, D., Croquette, V. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Behavior+of+supercoiled+DNA.">Behavior of supercoiled DNA.</a> Biophysical Journal. 74 (4), 2016-2028 (1998).</li><li>Yang, D., Ward, A., Halvorsen, K., Wong, W. P. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Multiplexed+single-molecule+force+spectroscopy+using+a+centrifuge.">Multiplexed single-molecule force spectroscopy using a centrifuge.</a> Nature Communications. 7, 11026 (2016).</li><li>Su, H., 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=Light-responsive+polymer+particles+as+force+clamps+for+the+mechanical+unfolding+of+target+molecules.">Light-responsive polymer particles as force clamps for the mechanical unfolding of target molecules.</a> Nano Letters. 18 (4), 2630-2636 (2018).</li><li>Kirkness, M. W. H., Forde, N. R. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Single-molecule+assay+for+proteolytic+susceptibility:+Force-induced+collagen+destabilization.">Single-molecule assay for proteolytic susceptibility: Force-induced collagen destabilization.</a> Biophysical Journal. 114 (3), 570-576 (2018).</li><li>Astumian, R. D. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Thermodynamics+and+kinetics+of+molecular+motors.">Thermodynamics and kinetics of molecular motors.</a> Biophysical Journal. 98 (11), 2401-2409 (2010).</li><li>Bekard, I. B., Asimakis, P., Bertolini, J., Dunstan, D. 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V. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Effects+of+shear+stress+on+endothelial+cells:+go+with+the+flow.">Effects of shear stress on endothelial cells: go with the flow.</a> Acta Physiologica. 219 (2), 382-408 (2017).</li><li>Hu, C., Jonchhe, S., Pokhrel, P., Karna, D., Mao, H. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Mechanical+unfolding+of+ensemble+biomolecular+structures+by+shear+force.">Mechanical unfolding of ensemble biomolecular structures by shear force.</a> Chemical Science. 12 (30), 10159-10164 (2021).</li><li>Sedghi Masoud, S., 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=Analysis+of+interactions+between+telomeric+i-motif+DNA+and+a+cyclic+tetraoxazole+compound.">Analysis of interactions between telomeric i-motif DNA and a cyclic tetraoxazole compound.</a> ChemBioChem. 19 (21), 2268-2272 (2018).</li><li>Abraham Punnoose, J., 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=Adaptive+and+specific+recognition+of+telomeric+G-quadruplexes+via+polyvalency+induced+unstacking+of+binding+units.">Adaptive and specific recognition of telomeric G-quadruplexes via polyvalency induced unstacking of binding units.</a> Journal of the American Chemical Society. 139 (22), 7476-7484 (2017).</li><li>Dhakal, S., 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=Coexistence+of+an+ILPR+i-motif+and+a+partially+folded+structure+with+comparable+mechanical+stability+revealed+at+the+single-molecule+level.">Coexistence of an ILPR i-motif and a partially folded structure with comparable mechanical stability revealed at the single-molecule level.</a> Journal of the American Chemical Society. 132 (26), 8991-8997 (2010).</li><li>Hu, C., Tahir, R., Mao, H. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Single-molecule+mechanochemical+sensing.">Single-molecule mechanochemical sensing.</a> Accounts of Chemical Research. 55 (9), 1214-1225 (2022).</li></ol>

The authors have no conflicts of interest.

The protocol described in this manuscript allows real-time investigation of the unfolding of an ensemble set of biomolecular structures by shear force. The results presented here underscore that DNA i-motif structures can be unfolded by shear force. The unfolding of the ligand-bound i-motif and the shear force-actuated click reactions were proof-of-concept applications for this ensemble force spectroscopy method.
Figure 1 presents the instrument setup. The homogen...

In single-molecule force spectroscopy1 (SMFS), the mechanical properties of individual molecular structures have been studied by sophisticated instruments such as the atomic force microscope, optical tweezers, and magnetic tweezers2,3,4. Restricted by the same directionality requirement of the molecules in the force-generating/detecting setups or the small field of view in magnetic tweezers and the miniature centrifuge force microscope (MCF)5,6,7,8, only a limited number of molecules can be investigated simultaneously using SMFS. The low throughput of SMFS prevents its wide application in the molecular recognition field, which requires the involvement of a large set of molecules.
Shear flow provides a potential solution to apply forces to a massive set of molecules9. In a liquid flow inside a channel, the closer to the channel surface, the slower the flow rate10. Such a flow velocity gradient causes shear stress that is parallel to the boundary surface. When a molecule is placed in this shear flow, the molecule reorients itself so that its long axis aligns with the flow direction, as the shear force is applied to the long axis11. As a result of this reorientation, all the molecules of the same type (size and length of handles) are expected to align in the same direction while experiencing the same shear force.
This work describes a protocol to use such a shear flow to exert shear force on a massive set of molecular structures, as exemplified by the DNA i-motif. In this protocol, a shear flow is generated between the rotor and stator in a homogenizer tip. The present study found that the folded DNA i-motif structure could be unfolded by shear rates of 9724-97245 s&#8722;1. Besides, a dissociation constant of 36 &#181;M was found between the L2H2-4OTD ligand and the i-motif. This value is consistent with that of 31 &#181;M measured by the gel shift assay12. Further, the current technique is used to unfold the i-motif, which can expose the chelated copper (I) to catalyze a click reaction. This protocol thus allows one to unfold a large set of i-motif structures with low-cost instruments in a reasonable time (shorter than 30 min). Given that the shear force technique drastically increases the throughput of the force spectroscopy, we call this technique ensemble force spectroscopy (EFS). This protocol aims to provide experimental guidelines to facilitate the application of this shear force-based EFS.

<table border="1" fo:keep-together.within-page="1" fo:keep-with-next.within-page="always">
	<tbody>
		<tr>
			<td>3K MWCO Amicon</td>
			<td>Millipore Sigma</td>
			<td>ufc900324</td>
			<td></td>
		</tr>
		<tr>
			<td>Ascorbic acid</td>
			<td>VWR</td>
			<td>VWRC0143-100G</td>
			<td></td>
		</tr>
		<tr>
			<td>Calfluor 488 azide</td>
			<td>Click Chemistry Tools</td>
			<td>1369-1</td>
			<td></td>
		</tr>
		<tr>
			<td>CuCl</td>
			<td>Thermo&#160;</td>
			<td>ACRO270525000</td>
			<td></td>
		</tr>
		<tr>
			<td>Dispersion tip</td>
			<td>Switzerland</td>
			<td>PT-DA07/2EC-B101</td>
			<td></td>
		</tr>
		<tr>
			<td>DNA oligos</td>
			<td>IDT</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>Dye</td>
			<td>IDT</td>
			<td>/5Cy5/</td>
			<td></td>
		</tr>
		<tr>
			<td>Fluorescence microscope</td>
			<td>Janpan</td>
			<td>Nikon TE2000-U</td>
			<td></td>
		</tr>
		<tr>
			<td>Homogenizer</td>
			<td>Switzerland</td>
			<td>PT 3100D</td>
			<td></td>
		</tr>
		<tr>
			<td>HPG</td>
			<td>Santa Cruz Biotechnology</td>
			<td>cs-295271</td>
			<td></td>
		</tr>
		<tr>
			<td>KCl</td>
			<td>VWR</td>
			<td>VWRC26760.295</td>
			<td></td>
		</tr>
		<tr>
			<td>MES</td>
			<td>VWR</td>
			<td>VWRCE169-500G</td>
			<td></td>
		</tr>
		<tr>
			<td>Quencher</td>
			<td>IDT</td>
			<td>/3IAbRQSp/</td>
			<td></td>
		</tr>
		<tr>
			<td>TBTA</td>
			<td>Tokyo Chemical Industry</td>
			<td>T2993</td>
			<td></td>
		</tr>
		<tr>
			<td>Tris</td>
			<td>VWR</td>
			<td>VWRCE133-100G</td>
			<td></td>
		</tr>
	</tbody>
</table>

ensemble force spectroscopy by shear forces

Single-molecule techniques based on fluorescence and mechanochemical principles provide superior sensitivity in biological sensing. However, due to the lack of high throughput capabilities, the application of these techniques is limited in biophysics. Ensemble force spectroscopy (EFS) has demonstrated high throughput in the investigation of a massive set of molecular structures by converting mechanochemical studies of individual molecules into those of molecular ensembles. In this protocol, the DNA secondary structures (i-motifs) were unfolded in the shear flow between the rotor and stator of a homogenizer tip at shear rates up to 77796/s. The effects of flow rates and molecular sizes on the shear forces experienced by the i-motif were demonstrated. The EFS technique also revealed the binding affinity between DNA i-motifs and ligands. Furthermore, we have demonstrated a click chemistry reaction that can be actuated by shear force (i.e., mechano-click chemistry). These results establish the effectiveness of using shear force to control the conformation of molecular structures.

Figure 1 outlines the mechanical unfolding and real-time sensing of ensemble molecules in EFS. In Figure 1B, the fluorescence intensity of i-motif DNA was observed to increase with the shear rate ranging from 9,724 s&#8722;1 to 97,245 s&#8722;1 in a pH 5.5 MES buffer. As a control, fluorescence intensity was not increased when the same i-motif DNA was sheared at a rate of 63,209 s&#8722;1 in a pH 7.4 MES buffer. ...

Watch this Scientific Journal Video about Ensemble Force Spectroscopy by Shear Forces at JoVE.com

Ensemble Force Spectroscopy by Shear Forces

Ensemble force spectroscopy (EFS) is a robust technique for mechanical unfolding and real-time sensing of an ensemble set of biomolecular structures in biophysical and biosensing fields.

Single-molecule techniques based on fluorescence and mechanochemical principles provide superior sensitivity in biological sensing. However, due to the ...

ensemble-force-spectroscopy-by-shear-forces

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1.4K Views.  Kent State University. Ensemble force spectroscopy (EFS) is a robust technique for mechanical unfolding and real-time sensing of an ensemble set of biomolecular structures in biophysical and biosensing fields.

Video: Ensemble Force Spectroscopy by Shear Forces

Thermodynamics of Membrane Protein Folding Measured by Fluorescence Spectroscopy

Membrane protein folding is an emerging topic with both fundamental and health-related significance. The abundance of membrane proteins in cells underlies the need for comprehensive study of the folding of this ubiquitous family of proteins. Additionally, advances in our ability to characterize diseases associated with misfolded proteins have motivated significant experimental and theoretical efforts in the field of protein folding. Rapid progress in this important field is unfortunately hindered by the inherent challenges associated with membrane proteins and the complexity of the folding mechanism. Here, we outline an experimental procedure for measuring the thermodynamic property of the Gibbs free energy of unfolding in the absence of denaturant, &Delta;G&deg;H2O, for a representative integral membrane protein from E. coli. This protocol focuses on the application of fluorescence spectroscopy to determine equilibrium populations of folded and unfolded states as a function of denaturant concentration. Experimental considerations for the preparation of synthetic lipid vesicles as well as key steps in the data analysis procedure are highlighted. This technique is versatile and may be pursued with different types of denaturant, including temperature and pH, as well as in various folding environments of lipids and micelles. The current protocol is one that can be generalized to any membrane or soluble protein that meets the set of criteria discussed below.

This video article details the experimental procedure for obtaining the Gibbs free energy of membrane protein folding by tryptophan fluorescence.

Membrane protein folding is an emerging topic with both fundamental and health-related significance.  The abundance of membrane proteins in cells ...

Bacterial Immobilization for Imaging by Atomic Force Microscopy

AFM is a high-resolution (nm scale) imaging tool that mechanically probes a surface. It has the ability to image cells and biomolecules, in a liquid environment, without the need to chemically treat the sample. In order to accomplish this goal, the sample must sufficiently adhere to the mounting surface to prevent removal by forces exerted by the scanning AFM cantilever tip. In many instances, successful imaging depends on immobilization of the sample to the mounting surface. Optimally, immobilization should be minimally invasive to the sample such that metabolic processes and functional attributes are not compromised. By coating freshly cleaved mica surfaces with porcine (pig) gelatin, negatively charged bacteria can be immobilized on the surface and imaged in liquid by AFM. Immobilization of bacterial cells on gelatin-coated mica is most likely due to electrostatic interaction between the negatively charged bacteria and the positively charged gelatin. Several factors can interfere with bacterial immobilization, including chemical constituents of the liquid in which the bacteria are suspended, the incubation time of the bacteria on the gelatin coated mica, surface characteristics of the bacterial strain and the medium in which the bacteria are imaged. Overall, the use of gelatin-coated mica is found to be generally applicable for imaging microbial cells.

Live Gram-negative and Gram-positive bacteria can be immobilized on gelatin-coated mica and imaged in liquid using Atomic Force Microscopy (AFM).

AFM is a high-resolution (nm scale) imaging tool that mechanically probes a surface.  It has the ability to image cells and biomolecules, in a liquid ...

Investigating Receptor-ligand Systems of the Cellulosome with AFM-based Single-molecule Force Spectroscopy

Cellulosomes are discrete multienzyme complexes used by a subset of anaerobic bacteria and fungi to digest lignocellulosic substrates. Assembly of the enzymes onto the noncatalytic scaffold protein is directed by interactions among a family of related receptor-ligand pairs comprising interacting cohesin and dockerin modules. The extremely strong binding between cohesin and dockerin modules results in dissociation constants in the low picomolar to nanomolar range, which may hamper accurate off-rate measurements with conventional bulk methods. Single-molecule force spectroscopy (SMFS) with the atomic force microscope measures the response of individual biomolecules to force, and in contrast to other single-molecule manipulation methods (i.e.&#160;optical tweezers), is optimal for studying high-affinity receptor-ligand interactions because of its ability to probe the high-force regime (&#62;120 pN). Here we present our complete protocol for studying cellulosomal protein assemblies at the single-molecule level. Using a protein topology derived from the native cellulosome, we worked with enzyme-dockerin and carbohydrate binding module-cohesin (CBM-cohesin) fusion proteins, each with an accessible free thiol group at an engineered cysteine residue. We present our site-specific surface immobilization protocol, along with our measurement and data analysis procedure for obtaining detailed binding parameters for the high-affinity complex. We demonstrate how to quantify single subdomain unfolding forces, complex rupture forces, kinetic off-rates, and potential widths of the binding well. The successful application of these methods in characterizing the cohesin-dockerin interaction responsible for assembly of multidomain cellulolytic complexes is further described.

Cellulosomes are multienzyme complexes designed for digesting cellulose. AFM-based SMFS was used to study the mechanical properties and folding configuration of cellulosome-associated protein assemblies. We present a complete workflow for protein immobilization, data acquisition, and data analysis to study the interactions of individual receptor-ligand complexes involved in cellulosome assembly.

Cellulosomes are discrete multienzyme complexes used by a subset of anaerobic bacteria and fungi to digest lignocellulosic substrates. Assembly of the ...

Manufacture of Concentrated, Lipid-based Oxygen Microbubble Emulsions by High Shear Homogenization and Serial Concentration

Gas-filled microbubbles have been developed as ultrasound contrast and drug delivery agents. Microbubbles can be produced by processing surfactants using sonication, mechanical agitation, microfluidic devices, or homogenization. Recently, lipid-based oxygen microbubbles (LOMs) have been designed to deliver oxygen intravenously during medical emergencies, reversing life-threatening hypoxemia, and preventing subsequent organ injury, cardiac arrest, and death. We present methods for scaled-up production of highly oxygenated microbubbles using a closed-loop high-shear homogenizer. The process can produce 2 L of concentrated LOMs (90% by volume) in 90 min. Resulting bubbles have a mean diameter of ~2 &#956;m, and a rheologic profile consistent with that of blood when diluted to 60 volume %. This technique produces LOMs in high capacity and with high oxygen purity, suggesting that this technique may be useful for translational research labs.

We describe methods for the manufacture of large volumes of lipid-based oxygen microbubbles (LOMs) designed for intravenous oxygen delivery using high-shear homogenization and serial concentration.

Gas-filled microbubbles have been developed as ultrasound contrast and drug delivery agents. Microbubbles can be produced by processing surfactants using ...

Measurement of Maximum Isometric Force Generated by Permeabilized Skeletal Muscle Fibers

Analysis of the contractile properties of chemically skinned, or permeabilized, skeletal muscle fibers offers a powerful means by which to assess muscle function at the level of the single muscle cell. Single muscle fiber studies are useful in both basic science and clinical studies. For basic studies, single muscle fiber contractility measurements allow investigation of fundamental mechanisms of force production, and analysis of muscle function in the context of genetic manipulations. Clinically, single muscle fiber studies provide useful insight into the impact of injury and disease on muscle function, and may be used to guide the understanding of muscular pathologies. In this video article we outline the steps required to prepare and isolate an individual skeletal muscle fiber segment, attach it to force-measuring apparatus, activate it to produce maximum isometric force, and estimate its cross-sectional area for the purpose of normalizing the force produced.

Analysis of the contractile properties of chemically skinned, or permeabilized, skeletal muscle fibers offers a powerful means by which to assess muscle function at the level of the single muscle cell. In this article we outline a valid and reliable technique to prepare and test permeabilized skeletal muscle fibers in vitro.

Analysis of the contractile properties of chemically skinned, or permeabilized, skeletal muscle fibers offers a powerful means by which to assess muscle ...

Atomic Force Microscopy Imaging and Force Spectroscopy of Supported Lipid Bilayers

Atomic force microscopy (AFM) is a versatile, high-resolution imaging technique that allows visualization of biological membranes. It has sufficient magnification to examine membrane substructures and even individual molecules. AFM can act as a force probe to measure interactions and mechanical properties of membranes. Supported lipid bilayers are conventionally used as membrane models in AFM studies. In this protocol, we demonstrate how to prepare supported bilayers and characterize their structure and mechanical properties using AFM. These include bilayer thickness and breakthrough force. 
The information provided by AFM imaging and force spectroscopy help define mechanical and chemical properties of membranes. These properties play an important role in cellular processes such as maintaining cell hemostasis from environmental stress, bringing membrane proteins together, and stabilizing protein complexes.

We describe a protocol for preparation of supported lipid bilayers and its characterization using atomic force microscopy and force spectroscopy.

Atomic force microscopy (AFM) is a versatile, high-resolution imaging technique that allows visualization of biological membranes. It has sufficient ...

A Protocol for Using F&#246;rster Resonance Energy Transfer (FRET)-force Biosensors to Measure Mechanical Forces across the Nuclear LINC Complex

The LINC complex has been hypothesized to be the critical structure that mediates the transfer of mechanical forces from the cytoskeleton to the nucleus. Nesprin-2G is a key component of the LINC complex that connects the actin cytoskeleton to membrane proteins (SUN domain proteins) in the perinuclear space. These membrane proteins connect to lamins inside the nucleus. Recently, a F&#246;rster Resonance Energy Transfer (FRET)-force probe was cloned into mini-Nesprin-2G (Nesprin-TS (tension sensor)) and used to measure tension across Nesprin-2G in live NIH3T3 fibroblasts. This paper describes the process of using Nesprin-TS to measure LINC complex forces in NIH3T3 fibroblasts. To extract FRET information from Nesprin-TS, an outline of how to spectrally unmix raw spectral images into acceptor and donor fluorescent channels is also presented. Using open-source software (ImageJ), images are pre-processed and transformed into ratiometric images. Finally, FRET data of Nesprin-TS is presented, along with strategies for how to compare data across different experimental groups.

A Protocol for Using F&amp;#246;rster Resonance Energy Transfer (FRET)-force Biosensors to Measure Mechanical Forces across the Nuclear LINC Complex

A number of FRET-based force biosensors have recently been developed, enabling the protein-specific resolution of intracellular force. In this protocol, we demonstrate how one of these sensors, designed for the linker of the nucleoskeleton-cytoskeleton (LINC) complex protein Nesprin-2G can be used to measure actomyosin forces on the nuclear LINC complex.

The LINC complex has been hypothesized to be the critical structure that mediates the transfer of mechanical forces from the cytoskeleton to the nucleus. ...

Probing the Roles of Physical Forces in Early Chick Embryonic Morphogenesis

Embryonic development is traditionally studied from the perspective of biomolecular genetics, but the fundamental importance of mechanics in morphogenesis is becoming increasingly recognized. In particular, the embryonic chick heart and brain tube, which undergo drastic morphological changes as they develop, are among the prime candidates to study the role of physical forces in morphogenesis. Progressive ventral bending&#160;and rightward torsion of the tubular embryonic chick brain happen at the earliest stage of organ-level left-right asymmetry in chick embryonic development. The vitelline membrane (VM) constrains the dorsal side of the embryo and has been implicated in providing the force necessary to induce torsion of the developing brain. Here we present a combination of new ex-ovo experiments and physical modeling to identify the mechanics of brain torsion. At Hamburger-Hamilton stage 11, embryos are harvested and cultured ex ovo (in media). The VM is subsequently removed using a pulled capillary tube. By controlling the level of the fluid and subjecting the embryo to a fluid-air interface, the fluid surface tension of the media can be used to replace the mechanical role of the VM. Microsurgery experiments were also performed to alter the position of the heart to find the resultant change in the chirality of brain torsion. Results from this protocol illustrate the fundamental roles of mechanics in driving morphogenesis.

Here, we present a protocol introducing a set of new ex-ovo experiments and physical modeling approaches for studying the mechanics of morphogenesis during early chick embryonic brain torsion.

Embryonic development is traditionally studied from the perspective of biomolecular genetics, but the fundamental importance of mechanics in morphogenesis ...

Detection of Endotoxin in Nano-formulations Using Limulus Amoebocyte Lysate (LAL) Assays

When present in pharmaceutical products, a Gram-negative bacterial cell wall component endotoxin (often also called lipopolysaccharide) can cause inflammation, fever, hypo- or hypertension, and, in extreme cases, can lead to tissue and organ damage that may become fatal. The amounts of endotoxin in pharmaceutical products, therefore, are strictly regulated. Among the methods available for endotoxin detection and quantification, the Limulus Amoebocyte Lysate (LAL) assay is commonly used worldwide. While any pharmaceutical product can interfere with the LAL assay, nano-formulations represent a particular challenge due to their complexity. The purpose of this paper is to provide a practical guide to researchers inexperienced in estimating endotoxins in engineered nanomaterials and nanoparticle-formulated drugs. Herein, practical recommendations for performing three LAL formats including turbidity, chromogenic and gel-clot assays are discussed. These assays can be used to determine endotoxin contamination in nanotechnology-based drug products, vaccines, and adjuvants.

Detection of Endotoxin in Nano-formulations Using Limulus Amoebocyte Lysate LAL Assays

Detection of endotoxins in engineered nanomaterials represents one of the grand challenges in the field of nanomedicine. Here, we present a case study that describes the framework composed of three different LAL formats to estimate potential endotoxin contamination in nanoparticles.

When present in pharmaceutical products, a Gram-negative bacterial cell wall component endotoxin (often also called lipopolysaccharide) can cause ...

3D Printing of In Vitro Hydrogel Microcarriers by Alternating Viscous-Inertial Force Jetting

Microcarriers are beads with a diameter of 60-250 &#181;m and a large specific surface area, which are commonly used as carriers for large-scale cell cultures. Microcarrier culture technology has become one of the main techniques in cytological research and is commonly used in the field of large-scale cell expansion. Microcarriers have also been shown to play an increasingly important role in in vitro tissue engineering construction and clinical drug screening. Current methods for preparing microcarriers include microfluidic chips and inkjet printing, which often rely on complex flow channel design, an incompatible two-phase interface, and a fixed nozzle shape. These methods face the challenges of complex nozzle processing, inconvenient nozzle changes, and excessive extrusion forces when applied to multiple bioink. In this study, a 3D printing technique, called alternating viscous-inertial force jetting, was applied to enable the construction of hydrogel microcarriers with a diameter of 100-300 &#181;m. Cells were subsequently seeded on microcarriers to form tissue engineering modules. Compared to existing methods, this method offers a free nozzle tip diameter, flexible nozzle switching, free control of printing parameters, and mild printing conditions for a wide range of bioactive materials.

3D Printing of In Vitro Hydrogel Microcarriers by Alternating Viscous-Inertial Force Jetting

Presented here is a mild 3D printing technique driven by alternating viscous-inertial forces to enable the construction of hydrogel microcarriers. Homemade nozzles offer flexibility, allowing easy replacement for different materials and diameters. Cell binding microcarriers with a diameter of 50-500 &#181;m can be obtained and collected for further culturing.

Microcarriers are beads with a diameter of 60-250 &#181;m and a large specific surface area, which are commonly used as carriers for large-scale cell ...