Name: Probing Myosin Ensemble Mechanics in Actin Filament Bundles Using Optical Tweezers (Video) | JoVE Journal
Uploaded: 2022-05-04T14:00:00.000+00:00
Duration: 6 min 53 s
Description: Learn to measure myosin ensemble mechanics in actin filament bundles using optical tweezers. This modular protocol enables precise investigation of motor protein dynamics within hierarchical cytoskeletal structures.

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5 minutes

This work is supported in part by the University of Mississippi Graduate Student Council Research Fellowship (OA), University of Mississippi Sally McDonnell-Barksdale Honors College (JCW, JER), the Mississippi Space Grant Consortium under grant number NNX15AH78H (JCW, DNR), and the American Heart Association under grant number 848586 (DNR).

1. Etching coverslips
<ol>
	<li>Dissolve 100 g of KOH in 300 mL of 100% ethanol in a 1,000 mL beaker. Stir with a stir bar until the majority of the KOH has dissolved. 
	CAUTION: Concentrated KOH solution can cause burns and damage to clothing. Wear gloves, eye protection, and a lab coat.</li>
	<li>Place coverslips individually in coverslip cleaning racks. 
	NOTE: Racks are designed with slits that hold single coverslips spaced apart to allow for etching and rinsing on each face of the coverslip, drain holes in the bottom, and made of material that can withstand the harsh etching conditions. They can be custom-made or purchased commercially.</li>
	<li>Prepare and label three 1,000 mL beakers: one with 300 mL of ethanol and two beakers with 300 mL of reverse osmosis (RO) water. 
	NOTE: Here, RO water was sourced from a lab water purifier, but it could also be purchased commercially if a local purifier is not available.</li>
	<li>Place each of the four beakers in a bath sonicator to degas for 5 min.</li>
	<li>Submerge a rack of coverslips in the beaker of KOH and ethanol and sonicate for 5 min.</li>
	<li>Transfer the rack of coverslips from the KOH/ethanol beaker to the ethanol-only beaker. Dip rack up and down in the beaker until there is no beading. 
	NOTE: Take care to not disturb the coverslips or forcefully drop the rack into the beaker. This will cause the coverslips to come out of the rack or cause chemical splashing.</li>
	<li>Carefully transfer the rack of coverslips from the ethanol beaker to a beaker of water, dipping up and down until there is no beading.</li>
	<li>Submerge the rack of coverslips in the beaker of water that has not been used yet and sonicate again for 5 min.</li>
	<li>Use a bottle to spray the rack of coverslips with water until it runs off the coverslips smoothly. Repeat with the ethanol.</li>
	<li>Place the racks to dry in an oven at 90 &#176;C for 20 min. Store the racks of etched coverslips at room temperature in closed containers to prevent contamination before use.</li>
</ol>
2. Actin filament polymerization
<ol>
	<li>Make Solution T
	<ol>
		<li>In a 50 mL conical tube, add 3.94 g of Tris-HCl and 0.147 g of CaCl2. Add RO water to make a total volume of 50 mL and mix well. 
		NOTE: The final concentrations of Solution T are 500 mM Tris-HCl and 20 mM CaCl2, respectively.</li>
		<li>Label the tube Solution T and store it at 4 &#176;C.</li>
	</ol>
	</li>
	<li>Make TC Buffer
	<ol>
		<li>Mix 40 mL of RO water and 1.5 mL of Solution T in a 50 mL conical tube. Change the pH to 8.0 by adding small amounts of concentrated KOH. Add water to make 50 mL of the solution, and verify the pH. Adjust the pH if needed. 
		NOTE: The final TC buffer contains 5 mM Tris-HCl and 0.2 mM CaCl2 at pH 8.</li>
		<li>Label the tube TC and store it at 4 &#176;C.</li>
	</ol>
	</li>
	<li>Make FC Buffer
	<ol>
		<li>Add 85 mL of RO water, 10 mL of Solution T, 3.73 g of KCl, and 0.041 g of MgCl2 to a 100 mL buffer bottle. Modify the pH to 7.5 by adding small volumes of concentrated KOH. Add water to make a final volume of 100 mL and verify the pH. 
		NOTE: The final FC buffer contains 500 mM Tris-HCl, 500 mM KCl, 2 mM MgCl2, and 2 mM CaCl2 at pH 7.5.</li>
		<li>Label the tube FC and store it at 4 &#176;C.</li>
	</ol>
	</li>
	<li>Prepare General Actin Buffer (GAB).
	<ol>
		<li>Mix 485 &#956;L of TC buffer, 10 &#956;L of 10 mM ATP, and 5 &#956;L of 50 mM DTT in a microcentrifuge tube. 
		NOTE: Final buffer conditions are 5 mM Tris-HCl, 0.2 mM CaCl2, 0.5 mM DTT, and 0.2 mM ATP.</li>
		<li>Label it as GAB and store it at 4 &#176;C.</li>
	</ol>
	</li>
	<li>Prepare Actin Polymerization Buffer (APB).
	<ol>
		<li>Mix 455 &#956;L of FC buffer, 25 &#956;L of 100 mM ATP, and 20 &#956;L of 50 mM DTT in a microcentrifuge tube. 
		NOTE: The final buffer conditions are 50 mM Tris-HCl, 500 mM KCl, 2 mM MgCl2, 2 mM CaCl2 2 mM DTT, and 5 mM ATP.</li>
		<li>Label the tube as APB and store it at 4 &#176;C.</li>
	</ol>
	</li>
	<li>Reconstitute actin
	<ol>
		<li>Reconstitute rabbit skeletal muscle actin by adding 100 &#956;L of deionized water to a 1 mg vial of lyophilized actin. Mix well by gently pipetting up and down. Aliquot into 5 &#956;L samples, snap-freeze, and store the 10 mg/mL actin aliquots at -80 &#176;C.</li>
		<li>Reconstitute biotinylated rabbit skeletal muscle actin by adding 20 &#956;L of RO water. Aliquot into 5 &#956;L samples, snap-freeze, and store the 1 mg/mL biotinylated actin aliquots at -80 &#176;C.</li>
	</ol>
	</li>
	<li>Non-labeled actin polymerization with rhodamine phalloidin stabilization
	<ol>
		<li>Thaw one vial of 10 mg/mL actin and keep it on ice.</li>
		<li>Prepare fresh GAB buffer, add 100 &#956;L of GAB to the actin aliquot, and mix by gently pipetting up and down. Incubate the solution on ice for 1 h.</li>
		<li>Prepare fresh APB during the incubation. After incubation, polymerize the actin into filaments by adding 11 &#956;L of APB to the actin solution. Mix well by gently pipetting up and down. Place on ice for 20 min.</li>
		<li>Add 5 &#956;L of rhodamine-labeled phalloidin to the freshly polymerized actin filament solution. Leave on ice in the dark for 1 h.</li>
		<li>Store the rhodamine actin vial wrapped in aluminum foil in the dark at 4 &#176;C. 
		NOTE: It is suggested to use these filaments for a maximum period of 1 week. AF quality can be confirmed each day through a quick imaging of a flow cell containing only AFs and viewing consistent filaments day to day.</li>
	</ol>
	</li>
	<li>Biotinylated actin polymerization with Alexa Fluor 488 phalloidin stabilization
	<ol>
		<li>Thaw one vial of 10 mg/mL actin and 1 vial of 1 mg/mL biotinylated actin and keep them on ice.</li>
		<li>Make fresh GAB buffer.</li>
		<li>Combine the two vials (step 2.8.1) in a 10:1 actin:biotinylated actin ratio. Add 100 &#956;L of GAB to the actin mixture and mix well by gently pipetting up and down. Incubate on ice for 1 h.</li>
		<li>Make fresh APB during the incubation.</li>
		<li>After the incubation step, polymerize the actin by adding 11 &#956;L of APB to the actin solution. Mix well by pipetting up and down gently. Incubate on ice for 20 min.</li>
		<li>Add 5 &#956;L of Alexa Fluor 488-labeled phalloidin and incubate on ice in the dark for 1 h.</li>
		<li>Store the biotinylated actin vial wrapped in aluminum foil in the dark at 4 &#176;C. 
		&#8203;NOTE: These filaments can be used for a maximum period of 1 week.</li>
	</ol>
	</li>
</ol>
3. Myosin and bead preparation
<ol>
	<li>Reconstitute Myosin II
	<ol>
		<li>Briefly spin down (~5 s) lyophilized skeletal myosin II to collect it at the bottom of the tube using a standard minicentrifuge.</li>
		<li>Reconstitute the myosin to 10 mg/mL by adding 100 &#956;L of 1 mM DTT prepared in RO water.</li>
		<li>Dilute the stock myosin solution 10x by adding 10 &#956;L of 10 mg/mL myosin to 90 &#956;L of 1 mM DTT in RO water. Make small-volume (1-5 &#956;L) aliquots, snap-freeze, and store at -80 &#176;C. 
		NOTE: Myosin activity can be confirmed by performing a standard gliding filament assay as published previously46,47. See the discussion for a brief description.</li>
	</ol>
	</li>
	<li>Cleaning streptavidin-coated beads
	<ol>
		<li>Dilute 20 &#956;L of 1 &#956;m streptavidin beads into 80 &#956;L of RO water. Wash four times by spinning down at 9,600 &#215; g and reconstituting in 100 &#956;L of RO water.</li>
		<li>Sonicate for 2 min at 40% amplitude and store the washed beads on a rotator at 4 &#176;C.</li>
	</ol>
	</li>
</ol>
4. Flow cell preparation
<ol>
	<li>Prepare a poly-l-lysine solution (PLL) by adding 30 mL of 100% ethanol to a 50 mL tube and adding 200 &#956;L of 0.1% w/v poly-l-lysine in water and mix well.</li>
	<li>Add an etched coverslip to the PLL solution and allow it to soak for 15 min. Remove the coverslip with tweezers, taking care to only touch the edge of the coverslip as it is pulled up from the tube (see Figure 1A-C). Grab the coverslips by their edges with a gloved hand.</li>
	<li>Dry the coverslip with a filtered airline until there is no ethanol left and no residue on the coverslip.</li>
	<li>Apply two pieces of double-sided sticky tape to the middle of a microscope slide, 3-4 mm apart from each other. Tear or cut off the excess tape that hangs off the edge of the slide.</li>
	<li>Add the PLL-coated coverslip on top of the tape perpendicular to the long axis of the microscope slide (forming a T) to form a channel.</li>
	<li>Use a small tube to compress the coverslip onto the tape and microscope slide thoroughly until the tape is transparent (Figure 1A). Ensure there are no bubbles in the tape as this can cause leakage from the flow channel. 
	&#8203;NOTE: The flow cell can hold a volume of 10-15 &#956;L.</li>
</ol>
5. Actomyosin bundle preparation
<ol>
	<li>In separate tubes, dilute each type of actin filament (rhodamine- and biotinylated 488-labeled) 600x by mixing 0.5 &#956;L of the respective, labeled actin with 300 &#956;L of APB. Add an additional 5 &#956;L of the correspondingly labeled phalloidin to each tube and incubate on ice in the dark for 15 min.</li>
	<li>To the biotinylated actin solution, add an oxygen scavenging system of 1 &#956;L of beta-D-glucose at 500 mg/mL, 1 &#956;L of glucose oxidase at 25 mg/mL, and 1 &#956;L of catalase at 500 units/mL. Add 1 &#956;L of 100 mM ATP and 1 &#956;L of 100x diluted, cleaned streptavidin beads. Gently stir with a pipette tip. Put the suspension on a rotator at 4 &#176;C while the rest of the actomyosin bundle is being assembled.</li>
	<li>Add 15 &#956;L of the diluted rhodamine actin to the PLL flow cell (Figure 1D). Wick the excess solution through the flow cell but do not allow the flow channel to become dry. Incubate for 10 min in a humidity chamber. 
	NOTE: Humidity chambers can be made from empty pipette tip boxes with water added to the bottom and the lid covered in aluminum foil to block light.</li>
	<li>Prepare a 1 mg/mL casein solution in APB.</li>
	<li>Add 15 &#956;L of 1 mg/mL casein to prevent non-specific binding of the subsequent components (Figure 1E). Incubate for 5 min in a humidity chamber.</li>
	<li>Add the desired concentration of myosin to the biotinylated actin and bead suspension from step 5.2. Gently stir with the pipette tip, and then immediately add 15 &#956;L of the step 5.2 suspension + the desired myosin concentration to the flow cell (Figure 1F,G). Incubate for 20 min. Seal the open ends of the flow cell with nail polish to prevent evaporation during imaging and optical trapping experiments. 
	NOTE: A myosin solution concentration of 1 &#956;M yields robust bundling and can be used as a starting point for the desired customization of the assay (see Figure 2).</li>
</ol>
6. Force measurements using Optical Trap (NT2 Nanotracker2)
NOTE: While the protocol below is specifically for the NT2 system, this assay can be used with other optical trapping systems, including those that are custom-built, that also have fluorescence capabilities. The general workflow remains the same of getting the surface of the slide in focus, performing bead calibrations, and acquiring data by finding fluorescent actin bundles. For the NT2 system, Supplemental Figure S1, Supplemental Figure S2, Supplemental Figure S3, Supplemental Figure S4, Supplemental Figure S5, Supplemental Figure S6, and Supplemental Figure S7 provide details of the optical trapping system and the software interface.
<ol>
	<li>Turn on the control box and laser (Supplemental Figure S1).</li>
	<li>Start the optical trap computer software by clicking on the JPK Nanotracker icon on the desktop.</li>
	<li>Wake up the remote controller by clicking on the Logitech button at the center (Supplemental Figure S2).</li>
	<li>Turn on the fluorescence module by toggling the on/off switch (Supplemental Figure S3).</li>
	<li>Turn the filter cube turret for brightfield imaging (Supplemental Figure S4).</li>
	<li>Once the system is ready, turn on the laser using the Laser Power button at the left-bottom corner of the screen to 50 mW and let it stabilize for 30 min (Supplemental Figure S5).</li>
	<li>Sequentially click on the Illumination, Camera, Objective, and Stage Movement buttons within the software to bring up those windows for viewing and manipulation during the experiment. Turn the microscope illumination on by clicking on the On/Off button and setting it to maximum power by clicking and dragging the bar all the way to the right (Supplemental Figure S5).</li>
	<li>Open the sample area and remove the sample holder from the microscope stage. Add the flow cell, secure it with the metal sample holders, and make sure that the slide with the coverslip is on the bottom.</li>
	<li>Add 30 &#956;L of RO water to the center of the bottom objective. Do not let the pipette tip touch the lens. Reinsert the sample stage. 
	NOTE: As the NT2 system uses a water immersion objective as the trapping objective, the immersion media may be different depending on the trapping objective in the user&#39;s setup.</li>
	<li>Raise the lower objective using the on-screen control arrows or L2 on the remote controller until the bead of water touches the coverslip (Supplemental Figure S5).</li>
	<li>Lower the top objective until about half the distance to the flow cell is reached using the on-screen arrows or R2 on the remote controller. Add 170 &#956;L of RO water to the top of the flow cell directly under the top objective. Lower the top objective until it breaks the surface tension of the water and forms a meniscus.</li>
	<li>Move the microscope stage using the arrow pad on the remote controller until the edge of the tape adjacent to the flow channel is reached. Close the sample door. 
	NOTE: A &#34;click&#34; upon closing the sample door indicates that the laser shutter is now open. This is a safety feature that only allows the shutter to open if the door is closed.</li>
	<li>Using the Objective window in the screen, bring the edge of the tape in focus by bringing the bottom objective named Laser Objective up by clicking on the upper arrow using the on-screen controls. Do the same for the top objective by clicking bottom arrow (Supplemental Figure S5). 
	NOTE: The double arrows move the objective or stage faster. The edge of the tape is used for focusing because it is a large, easy-to-find object that is close to the coverslip surface. Air bubbles within the tape are another option. However, this is not required if the user has an automated routine to find the surface focus or a preferred in-house method.</li>
	<li>Once the tape is in focus, partially close the iris at the top of the optical trap. Bring the top objective down until the polygon shape of the iris is visible. Bring those edges in focus, reopen the iris, and then couple the objectives using by clicking on the Padlock icon (Supplemental Figure S5).</li>
	<li>Find a floating bead and trap it by clicking on the Trap Shutter button, which will open the shutter and allow the trapping laser to hit the sample. Click on the Trap cursor on the screen and drag it to move the location of the trapping laser. Once trapped, calibrate the bead to correlate voltage measurements to force and displacement.</li>
	<li>Click on the Calibration button. Adjust the calibration routine based on power spectra analysis and fit the corner frequency within the software for the X, Y, and Z directions (Supplementary Figure S6).</li>
	<li>Click on Settings. Type in the diameter of the bead (1,000 nm), and type in the temperature of the stage found in the bottom left of the software window. (see Supplemental Figure S6).</li>
	<li>Click on Trap 1. Click on X Signal. Click on Run to perform the corner frequency fit. Click and drag within the window to optimize the function fit. Click on Use It for sensitivity and stiffness values. Click on Accept Values. Repeat for the Y and Z signals. Close the window. (see Supplemental Figure S6). 
	NOTE: Bead calibration routines on other optical trapping systems or custom-built systems that have been robustly tested by the user, such as the equipartition method or drag force method, are also acceptable57,58.</li>
	<li>Find an actomyosin bundle by searching for beads bound to AFs on the surface of the coverslip.</li>
	<li>When a bead uncrowded by other floating beads is detected, observe the AFs around it by fluorescence imaging to verify the presence of a bundle.</li>
	<li>Verify that a bundle is present by looking for both fluorescent AFs colocalized. Turn on the white light source and use the appropriate filter cube to image each actin filament by turning the turret (488 nm and 532 nm excitation filter cubes for Alexa Fluor 488 and rhodamine excitation, respectively). See Supplemental Figure S4. 
	NOTE: A control experiment to verify the fluorescence intensity of single AFs can be useful in identifying bundles that are composed of a single 488- and single rhodamine-labeled filaments, or applicable to whichever set of fluorophores the user chooses to use.</li>
	<li>Once verified, trap the bead attached to the top filament of the bundle by clicking on the Trap Shutter button.</li>
	<li>Use the on-screen controls to record the data by clicking on the Oscilloscope button (Supplemental Figure S7). To visualize measurements without recording the data, click on Start. To save all data, click on Autosave. To record measurements, click on Start Record. Choose which data are to be visualized in real-time (position, force, x-direction, y-direction) by choosing from the drop down menu X signal or Y signal. Remember that xdirection is left to right, and y-direction is up and down on the screen. See Supplemental Figure S7. 
	NOTE: Data will be saved as .out files and includes time, voltage, displacement, and force for each direction. These files can be exported into other software for visualization and analysis.</li>
</ol>

The authors have no conflicts of interest to declare.

An in vitro study using optical tweezers combined with fluorescence imaging was performed to investigate the dynamics of myosin ensembles interacting with actin filaments. Actin-myosin-actin bundles were assembled using muscle myosin II, rhodamine actin at the bottom of the bundle and on the coverslip surface, and 488-labeled, biotinylated actin filaments on the top of the bundle. Actin protein from rabbit muscle was polymerized and stabilized using general actin buffers (GAB) and actin polymerizing buffers (APB...

Motor proteins are essential to life, converting chemical energy into mechanical work1,2,3. Myosin motors interact with actin filaments by taking steps along the filaments similar to a track, and the dynamics of actin-myosin networks carry out muscle contraction, cell motility, the contractile ring during cytokinesis, and movement of cargo inside the cell, among other essential tasks3,4,5,6,7,8. Since myosins have so many essential roles, failure in the functionality of the myosin-actin network can lead to disease development, such as mutations in the myosin heavy chain that cause heart hypercontractility in hypertrophic cardiomyopathy (HCM)9,10,11,12,13,14. In muscle contraction, individual myosin motors cooperate with each other by working as an ensemble to provide the required mechanical energy that carries out the relative sliding of AFs4,15,16,17,18. Myosin motors form crossbridges between AFs and use conformational changes due to its mechanochemical cycle to collectively move toward the barbed end of the aligned filaments17,18,19,20,21.
Development of quantitative in vitro motility assays at the SM level using techniques such as optical trapping has facilitated gathering unprecedented detail of how individual myosin motors function, including measuring SM force generation and step sizes22,23,24,25,26,27,28,29,30. Finer et al. developed the &#34;three-bead&#34; or &#34;dumbbell&#34; optical trapping assay to probe the force-generation mechanics of single myosin II motors23,31. As muscle myosin II works in teams to contract AFs but is non-processive at the SM level, the optical trapping assay orientation had to be rearranged from the classic motor-bound bead approach32. To form the dumbbell assay, two optical traps were used to hold an AF over a myosin motor bound to a coverslip-attached bead, and force output by the single motor was measured through movements of the AF within the trap23.
However, SM forces and using a single motor/single filament assay orientation do not give a full image about system-level force generation since many motor proteins, including myosin II, do not work in isolation and often do not function as a sum of their parts15,16,17,32,33,34,35,36. More complex structures that include more than one motor interacting with more than one filament are necessary to better understand the synergy of myosin and actin filaments&#39; networks15,32. The dumbbell assay orientation has been exploited to investigate small ensemble force generation by having multiple myosins attached to a bead or using a myosin-thick filament attached to a surface and allowing the motors to interact with the suspended AF4,23,34,37,38,39,40.
Other small ensemble assays include an in vitro filament gliding assay wherein myosin motors are coated onto a coverslip surface, and a bead bound to an AF is used to probe the force generated by the team of motors4,35,36,38,39,40,41,42,43. In both these cases, the myosins are bound to a rigid surface &#8211; bead or coverslip &#8211; and utilize one AF. In these cases, the motors are not able to move freely or communicate with each other, nor does having myosins rigidly bound reflect the compliant, hierarchical environment in which the motors would work together in the sarcomere32. Previous studies have suggested that myosin II can sense its environment and adapt accordingly to changing viscoelastic or motor concentration conditions by altering characteristics such as force generation and duty ratio41,44,45. Thus, there is a need to develop an optical trapping assay that fosters and captures motor communication and system compliancy to paint a more realistic picture of the mechanistic underpinnings of myosin II ensemble force generation.
Here, we developed a method to couple hierarchical structure in vitro with optical trapping by forming actomyosin bundles or sandwiches consisting of multiple myosin motors interacting between two actin filaments. This modular assay geometry has the ability to directly probe how molecular and environmental factors influence ensemble myosin force generation. Further, investigating force generation mechanisms through these actin-myosin ensembles have the potential to aid in modeling and understanding how large-scale cellular tasks, such as muscle contraction, propagate up from the molecular level9,10,13.

<table><tbody><tr><td>Actin protein (biotin): skeletal muscle</td><td>Cytoskeleton</td><td>AB07-A</td><td>Biotinylated actin protein</td></tr><tr><td>Actin protein, rabbit skeletal muscle</td><td>Cytoskeleton</td><td>AKL99-A</td><td>Actin protein</td></tr><tr><td>Alexa Fluor 488 Phalloidin</td><td>Invitrogen</td><td>A12379</td><td>Actin stabilizer and Alexa Fluor 488 stain</td></tr><tr><td>ATP</td><td>Fisher scientific</td><td>BP413-25</td><td>Required for actin assembly and myosin motility</td></tr><tr><td>Beta-D-glucose</td><td>Fisher scientific</td><td>MP218069110</td><td>Part of oxygen scavenging system used to reduce photobleaching during fluorescence imaging</td></tr><tr><td>Blotting Grade Blocker (casein)</td><td>Biorad</td><td>1706404</td><td>Used to block surface from non-specific binding</td></tr><tr><td>CaCl&lt;sub&gt;2&lt;/sub&gt;</td><td>Fisher scientific</td><td>C79500</td><td>Calcium chloride, provides the necessary control over the dynamics of actin myosin network</td></tr><tr><td>Catalase</td><td>Fisher scientific</td><td>ICN10040280</td><td>Part of oxygen scavenging system used to reduce photobleaching during fluorescence imaging</td></tr><tr><td>Coverslips</td><td>Fisher scientific</td><td>12544C</td><td>Used to make flow cells</td></tr><tr><td>DTT</td><td>Fisher scientific</td><td>AC327190010</td><td>Used for buffer preparation</td></tr><tr><td>Ethanol</td><td>Fisher scientific</td><td>A4094</td><td>Regent used for cleaning coverslips</td></tr><tr><td>Glucose oxidase</td><td>Fisher scientific</td><td>34-538-610KU</td><td>Part of oxygen scavenging system used to reduce photobleaching during fluorescence imaging</td></tr><tr><td>KCl</td><td>Fisher scientific</td><td>P217-500</td><td>Used for buffer preparation</td></tr><tr><td>KOH</td><td>Fisher scientific</td><td>P250-1</td><td>Used to etch coverslips and adjust buffer pH</td></tr><tr><td>MgCl&lt;sub&gt;2&lt;/sub&gt;</td><td>Fisher scientific</td><td>M33-500</td><td>Used for buffer preparation</td></tr><tr><td>Microscope slides</td><td>Fisher scientific</td><td>12-544-2</td><td>Used to make flow cells</td></tr><tr><td>Myosin II protein: rabbit skeletal muscle</td><td>Cytoskeleton</td><td>MY02</td><td>Full length myosin motor protein isolated from rabbit skeletal muscle</td></tr><tr><td>Nanotracker2</td><td>Bruker/JPK</td><td>NT2</td><td>Optical trapping instrument</td></tr><tr><td>Poly-l-lysine</td><td>Sigma-Aldrich</td><td>P8920</td><td>Facilities adhesion of actin filaments onto glass surface of the coverslip</td></tr><tr><td>Rhodamine Phalloidin</td><td>Cytoskeleton</td><td>PHDR1</td><td>Actin stabilizer and rhodamine fluorescent stain</td></tr><tr><td>Streptavidin beads, 1 &amp;mu;m</td><td>Spherotech</td><td>SVP-10-5</td><td>Optical trapping handle</td></tr><tr><td>Tris-HCl</td><td>Fisher scientific</td><td>PR H5121</td><td>Used for buffer preparation</td></tr></tbody></table>

probing myosin ensemble mechanics in actin filament bundles using optical tweezers

Probing Myosin Ensemble Mechanics in Actin Filament Bundles Using Optical Tweezers

Myosins are motor proteins that hydrolyze ATP to step along actin filament (AF) tracks and are essential in cellular processes such as motility and muscle contraction. To understand their force-generating mechanisms, myosin II has been investigated both at the single-molecule (SM) level and as teams of motors in vitro using biophysical methods such as optical trapping.
These studies showed that myosin force-generating behavior can differ greatly when moving from the single-molecule level in a three-bead arrangement to groups of motors working together on a rigid bead or coverslip surface in a gliding arrangement. However, these assay constructions do not permit evaluating the group dynamics of myosin within viscoelastic structural hierarchy as they would within a cell. We have developed a method using optical tweezers to investigate the mechanics of force generation by myosin ensembles interacting with multiple actin filaments.
These actomyosin bundles facilitate investigation in a hierarchical and compliant environment that captures motor communication and ensemble force output. The customizable nature of the assay allows for altering experimental conditions to understand how modifications to the myosin ensemble, actin filament bundle, or the surrounding environment result in differing force outputs.

Flow cells containing the actomyosin bundle systems are of a standard design, consisting of a microscope slide and an etched coverslip separated by a channel made from double-sided sticky tape (Figure 1). The assay is then built from the coverslip up using staged introductions as described in the protocol. The final assay consists of template rhodamine-labeled actin filaments; the desired myosin concentration (1 μM was used for the representative results in Figure 2</str...

Formation of actomyosin bundles in vitro and measuring myosin ensemble force generation using optical tweezers is presented and discussed.

Myosins are motor proteins that hydrolyze ATP to step along actin filament (AF) tracks and are essential in cellular processes such as motility and muscle ...

probing-myosin-ensemble-mechanics-actin-filament-bundles-using

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Optical Tweezers to Study RNA-Protein Interactions in Translation Regulation

Here, we present a protocol to investigate the intracellular mechanical properties of isolated embryonic zebrafish cells in three-dimensional confinement with direct force measurement by an optical trap.

Direct Force Measurements of Subcellular Mechanics in Confinement using Optical Tweezers

Here, we present a protocol for reconstituting microtubule bundles in vitro and directly quantifying the forces exerted within them using simultaneous optical trapping and total internal reflection fluorescence microscopy. This assay allows for nanoscale-level measurement of the forces and displacements generated by protein ensembles within active microtubule networks.

Directly Measuring Forces Within Reconstituted Active Microtubule Bundles

We present protocols for simple actin filament microfluidic assays, in combination with fluorescence microscopy, that allow one to accurately monitor individual actin filaments in real-time while sequentially exposing them to different protein solutions.

Using Microfluidics and Fluorescence Microscopy to Study the Assembly Dynamics of Single Actin Filaments and Bundles

This paper presents protocols for engineering and characterizing tunable three-dimensional composite networks of co-entangled actin filaments and microtubules. Composites undergo active restructuring and ballistic motion, driven by myosin II and kinesin motors, and are tuned by the relative concentrations of actin, microtubules, motor proteins, and passive crosslinkers.

Reconstituting and Characterizing Actin-Microtubule Composites with Tunable Motor-Driven Dynamics and Mechanics

In this work, an in vitro reconstitution approach is employed to study the poroelasticity of actomyosin gels under controlled conditions. The dynamics of the actomyosin gel and the embedded solvent are quantified, through which the network poroelasticity is demonstrated. We also discuss the experimental challenges, common pitfalls, and relevance to cell cytoskeleton mechanics.

The Mechanics of (Poro-)Elastic Contractile Actomyosin Networks As a Model System of the Cell Cytoskeleton

Here, we present methods for preparing quasi-two-dimensional (2D) entangled, cross-linked, and liquid crystal actin assemblies from purified proteins.

Tuning the Contractility and Deformation Modes of Active Actin-Based Assemblies In Vitro: From Two-Dimensional Active Networks to Liquid Crystal Drops

Learn to measure myosin ensemble mechanics in actin filament bundles using optical tweezers. This modular protocol enables precise investigation of motor protein dynamics within hierarchical cytoskeletal structures.

Probing Myosin Ensemble Mechanics in Actin Filament Bundles Using Optical Tweezers

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