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>

<ol>
	<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. E. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=The+effects+of+shear+flow+on+protein+structure+and+function.">The effects of shear flow on protein structure and function.</a> Biopolymers. 95 (11), 733-745 (2011).</li><li>Chistiakov, D. A., Orekhov, A. N., Bobryshev, Y. 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><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&amp;nbsp;</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 ...

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Bioengineering

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

Demonstrating the Uses of the Novel Gravitational Force Spectrometer to Stretch and Measure Fibrous Proteins

The study of macromolecular structure has become critical to the elucidation of molecular mechanisms and function. There are several limited, but important bioinstruments capable of testing the force dependence of structural features in proteins. Scale has been a limiting parameter on how accurately researchers can peer into the nanomechanical world of molecules, such as nucleic acids, enzymes, and motor proteins that perform life-sustaining work. Atomic force microscopy (AFM) is well tuned to determine native structures of fibrous proteins with a distance resolution on par with electron microscopy. However, in AFM force studies, the forces are typically much higher than a single molecule might experience 1, 2. Optical traps (OT) are very good at determining the relative distance between the trapped beads and they can impart very small forces 3. However, they do not yield accurate absolute lengths of the molecules under study. Molecular simulations provide supportive information to such experiments, but are limited in the ability to handle the same large molecular sizes, long time frames, and convince some researchers in the absence of other supporting evidence2, 4.
The gravitational force spectrometer (GFS) fills a critical niche in the arsenal of an investigator by providing a unique combination of abilities. This instrument is capable of generating forces typically with 98% or better accuracy from the femtonewton range to the nanonewton range. The distance measurements currently are capable of resolving the absolute molecular length down to five nanometers, and relative bead pair separation distances with a precision similar to an optical trap. Also, the GFS can determine stretching or uncoiling where the force is near equilibrium, or provide a graded force to juxtapose against any measured structural changes. It is even possible to determine how many amino acid residues are involved in uncoiling events under physiological force loads 2. Unlike in other methods where there is extensive force calibration that must precede any assay, the GFS requires no such force calibration 5. By complementing the strengths of other methods, the GFS will bridge gaps in understanding the nanomechanics of vital proteins and other macromolecules.

This is a step-by step guide showing the purpose, operation, and representative results from the novel gravitational force spectrometer.

The study of macromolecular structure has become critical to the elucidation of molecular mechanisms and function. There are several limited, but ...

Force Spectroscopy of Single Protein Molecules Using an Atomic Force Microscope

The determination of the folding process of proteins from their amino acid sequence to their native 3D structure is an important problem in biology. Atomic force microscopy (AFM) can address this problem by enabling stretching and relaxation of single protein molecules, which gives direct evidence of specific unfolding and refolding characteristics. AFM-based single-molecule force-spectroscopy (AFM-SMFS) provides a means to consistently measure high-energy conformations in proteins that are not possible in traditional bulk (biochemical) measurements. Although numerous papers were published to show principles of AFM-SMFS, it is not easy to conduct SMFS experiments due to a lack of an exhaustively complete protocol. In this study, we briefly illustrate the principles of AFM and extensively detail the protocols, procedures, and data analysis as a guideline to achieve good results from SMFS experiments. We demonstrate representative SMFS results of single protein mechanical unfolding measurements and we provide troubleshooting strategies for some commonly encountered problems.

We describe the detailed procedures and strategies to measure the mechanical properties and mechanical unfolding pathways of single protein molecules using an atomic force microscope. We also show representative results as a reference for selection and justification of good single protein molecule recordings.

The determination of the folding process of proteins from their amino acid sequence to their native 3D structure is an important problem in biology. ...

Biochemistry

Investigating Single Molecule Adhesion by Atomic Force Spectroscopy

Atomic force spectroscopy is an ideal tool to study molecules at surfaces and interfaces. An experimental protocol to couple a large variety of single molecules covalently onto an AFM tip is presented. At the same time the AFM tip is passivated to prevent unspecific interactions between the tip and the substrate, which is a prerequisite to study single molecules attached to the AFM tip. Analyses to determine the adhesion force, the adhesion length, and the free energy of these molecules on solid surfaces and bio-interfaces are shortly presented and external references for further reading are provided. Example molecules are the poly(amino acid) polytyrosine, the graft polymer PI-g-PS and the phospholipid POPE (1-palmitoyl-2-oleoyl-sn-glycero-3-phosphoethanolamine). These molecules are desorbed from different surfaces like CH3-SAMs, hydrogen terminated diamond and supported lipid bilayers under various solvent conditions. Finally, the advantages of force spectroscopic single molecule experiments are discussed including means to decide if truly a single molecule has been studied in the experiment.

A protocol to couple a large variety of single molecules covalently onto an AFM tip is presented. Procedures and examples to determine the adhesion force and free energy of these molecules on solid supports and bio-interfaces are provided.

Atomic force spectroscopy is an ideal tool to study molecules at surfaces and interfaces. An experimental protocol to couple a large variety of single ...

Engineering

Covalent Immobilization of Proteins for the Single Molecule Force Spectroscopy

In recent years, atomic force microscopy (AFM) based single molecule force spectroscopy (SMFS) extended our understanding of molecular properties and functions. It gave us the opportunity to explore a multiplicity of biophysical mechanisms, e.g., how bacterial adhesins bind to host surface receptors in more detail. Among other factors, the success of SMFS experiments depends on the functional and native immobilization of the biomolecules of interest on solid surfaces and AFM tips. Here, we describe a straightforward protocol for the covalent coupling of proteins to silicon surfaces using silane-PEG-carboxyls and the well-established N-hydroxysuccinimid/1-ethyl-3-(3-dimethyl-aminopropyl)carbodiimid (EDC/NHS) chemistry in order to explore the interaction of pilus-1 adhesin RrgA from the Gram-positive bacterium Streptococcus pneumoniae (S. pneumoniae) with the extracellular matrix protein fibronectin (Fn). Our results show that the surface functionalization leads to a homogenous distribution of Fn on the glass surface and to an appropriate concentration of RrgA on the AFM cantilever tip, apparent by the target value of up to 20% of interaction events during SMFS measurements and revealed that RrgA binds to Fn with a mean force of 52 pN. The protocol can be adjusted to couple via site specific free thiol groups. This results in a predefined protein or molecule orientation and is suitable for other biophysical applications besides the SMFS.

This protocol describes the covalent immobilization of proteins with a heterobifunctional silane coupling agent to silicon-oxide surfaces designed for the atomic force microscopy based single molecule force spectroscopy which is exemplified by the interaction of RrgA (pilus-1 tip adhesin of S. pneumoniae) with fibronectin.

In recent years, atomic force microscopy (AFM) based single molecule force spectroscopy (SMFS) extended our understanding of molecular properties and ...

Insights into the Interactions of Amino Acids and Peptides with Inorganic Materials Using Single-Molecule Force Spectroscopy

The interactions between proteins or peptides and inorganic materials lead to several interesting processes. For example, combining proteins with minerals leads to the formation of composite materials with unique properties. In addition, the undesirable process of biofouling is initiated by the adsorption of biomolecules, mainly proteins, on surfaces. This organic layer is an adhesion layer for bacteria and allows them to interact with the surface. Understanding the fundamental forces that govern the interactions at the organic-inorganic interface is therefore important for many areas of research and could lead to the design of new materials for optical, mechanical and biomedical applications. This paper demonstrates a single-molecule force spectroscopy technique that utilizes an AFM to measure the adhesion force between either peptides or amino acids and well-defined inorganic surfaces. This technique involves a protocol for attaching the biomolecule to the AFM tip through a covalent flexible linker and single-molecule force spectroscopy measurements by atomic force microscope. In addition, an analysis of these measurements is included.

Here we present a protocol to measure the force of interactions between a well-defined inorganic surface and either peptides or amino acids by single-molecule force spectroscopy measurements using an atomic force microscope (AFM). The information obtained from the measurement is important to better understand the peptide-inorganic material interphase.

The interactions between proteins or peptides and inorganic materials lead to several interesting processes. For example, combining proteins with minerals ...

Chemistry

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 ...

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 ...

Studying Large Amplitude Oscillatory Shear Response of Soft Materials

We investigate the sequence of physical processes exhibited during large amplitude oscillatory shearing (LAOS) of polyethylene oxide (PEO) in dimethyl sulfoxide (DMSO) and xanthan gum in water &#8212; two concentrated polymer solutions used as viscosifiers in foods, enhanced oil recovery, and soil remediation. Understanding the nonlinear rheological behavior of soft materials is important in the design and controlled manufacturing of many consumer products. It is shown how the response to LAOS of these polymer solutions can be interpreted in terms of a clear transition from linear viscoelasticity to viscoplastic deformation and back again during a period. The LAOS results are analyzed via the fully quantitative Sequence of Physical Processes (SPP) technique, using free MATLAB-based software. A detailed protocol of performing a LAOS measurement with a commercial rheometer, analyzing nonlinear stress responses with the freeware, and interpreting physical processes under LAOS is presented. It is further shown that, within the SPP framework, a LAOS response contains information regarding the linear viscoelasticity, the transient flow curves, and the critical strain responsible for the onset of nonlinearity.

We present a detailed protocol outlining how to perform nonlinear oscillatory shear rheology on soft materials, and how to run the SPP-LAOS analysis to understand the responses as a sequence of physical processes.

We investigate the sequence of physical processes exhibited during large amplitude oscillatory shearing (LAOS) of polyethylene oxide (PEO) in dimethyl ...

Covalent Attachment of Single Molecules for AFM-based Force Spectroscopy

Atomic force microscopy (AFM)-based single molecule force spectroscopy is an ideal tool for investigating the interactions between a single polymer and surfaces. For a true single molecule experiment, covalent attachment of the probe molecule is essential because only then can hundreds of force-extension traces with one and the same single molecule be obtained. Many traces are in turn necessary to prove that a single molecule alone is probed. Additionally, passivation is crucial for preventing unwanted interactions between the single probe molecule and the AFM cantilever tip as well as between the AFM cantilever tip and the underlying surface. The functionalization protocol presented here is reliable and can easily be applied to a variety of polymers. Characteristic single molecule events (i.e., stretches and plateaus) are detected in the force-extension traces. From these events, physical parameters such as stretching force, desorption force and desorption length can be obtained. This is particularly important for the precise investigation of stimuli-responsive systems at the single molecule level. As exemplary systems poly(ethylene glycol) (PEG), poly(N-isopropylacrylamide) (PNiPAM) and polystyrene (PS) are stretched and desorbed from SiOx (for PEG and PNiPAM) and from hydrophobic self-assembled monolayer surfaces (for PS) in aqueous environment.

Covalent attachment of probe molecules to atomic force microscopy (AFM) cantilever tips is an essential technique for the investigation of their physical properties. This allows us to determine the stretching force, desorption force and length of polymers via AFM-based single molecule force spectroscopy with high reproducibility.

Atomic force microscopy (AFM)-based single molecule force spectroscopy is an ideal tool for investigating the interactions between a single polymer and ...

Visualizing Solution Structure at Solid-Liquid Interfaces using Three-Dimensional Fast Force Mapping

Amongst the challenges for a variety of research fields are the visualization of solid-liquid interfaces and understanding how they are affected by the solution conditions such as ion concentrations, pH, ligands, and trace additives, as well as the underlying crystallography and chemistry. In this context, three-dimensional fast force mapping (3D FFM) has emerged as a promising tool for investigating solution structure at interfaces. This capability is based on atomic force microscopy (AFM) and allows the direct visualization of interfacial regions in three spatial dimensions with sub-nanometer resolution. Here we provide a detailed description of the experimental protocol for acquiring 3D FFM data. The main considerations for optimizing the operating parameters depending on the sample and application are discussed. Moreover, the basic methods for data processing and analysis are discussed, including the transformation of the measured instrument observables into tip-sample force maps that can be linked to the local solution structure. Finally, we shed light on some of the outstanding questions related to 3D FFM data interpretation and how this technique can become a central tool in the repertoire of surface science.

Here, we present a protocol for using three-dimensional fast force mapping - an atomic force microscopy technique - for visualizing solution structure at solid-liquid interfaces with the subnanometer resolution by mapping the tip-sample interactions within the interfacial region.

Amongst the challenges for a variety of research fields are the visualization of solid-liquid interfaces and understanding how they are affected by the ...