This work was supported by NIH R01 EB014869.

1. Preparing Cells for Imaging
NOTE: The direct force probe (DFP) can be used for any adherent cell type. Here, NIH 3T3 mouse fibroblasts are used as the model cell line for this protocol.
<ol>
	<li>Culture NIH 3T3 fibroblast cells in Dulbecco&#39;s Modified Eagle&#39;s Medium (DMEM) supplemented with 10% donor bovine serum and 1% Penicillin-Streptomycin on a 35-mm glass bottom dish until desired confluency. Maintain cells at 37 &#176;C and 5% CO2.
	<ol>
		<li>Be sure to coat all 35-mm glass bottom dishes with 5 &#181;g/mL of fibronectin (or similar ECM protein), before seeding NIH 3T3 cells for imaging. 
		NOTE: The cells must be fully spread and adherent on the dish for the experiment. There are not any constraints in terms of confluency for the DFP method to work.</li>
	</ol>
	</li>
	<li>Immediately prior to the experiment, wash the cells twice with PBS followed by a single wash with complete growth medium.</li>
	<li>Add 3 mL of complete growth medium to the glass bottom dish.</li>
</ol>
2. Microscopy and Image Acquisition
Note: An inverted fluorescence microscope (or equivalent) with micromanipulator installed to the side arm, according to the manufacturer&#39;s recommendations. The microscope should also be outfitted with an environmental chamber to maintain the temperature at 37 &#176;C, and CO2 level at 5%. A micromanipulator and microinjector attached to the microscope is also required. An oil immersion 40x/1.3 NA or 60x/1.49 NA (or equivalent objectives) are recommended for the experiments. The microscope should be mounted on a vibration isolation table.
<img alt="Figure 1" class="xfigimg" src="/files/ftp_upload/58038/58038fig1.jpg" /> 
Figure 1. Nuclear Deformation and Microscope Focusing 
A.&#160;Maximum nuclear deformation and relaxation of nuclear deformation. Before calculating maximum nuclear deformation, the back edges of the nuclear shapes were first coincided to correct for the translation of deformed nucleus. The shape of the nucleus at the moment of micropipette tip detachment was overlaid on the initial nuclear shape before pulling. The difference in area between the two shapes was measured as &#916;A1. The maximum nuclear deformation was defined as &#916;A1&#160;divided by the original nuclear area. Similarly, a second parameter, &#916;A2, may be defined by overlaying the final steady state nuclear shape after micropipette detachment on the original nuclear shape. B. Focus the cell at plane A and then move the focal plane up to plane B to find the micropipette tip. During imaging, the micropipette was translated to the right (direction of orange arrow). This figure has been modified from Neelam et al.15. <a href="https://www.jove.com/files/ftp_upload/58038/58038fig1large.jpg" target="_blank">Please click here to view a larger version of this figure.</a>
<ol>
	<li>Turn on the microinjector per the manufacturer&#39;s protocol.</li>
	<li>Using an immersion oil dropper, apply a single drop of immersion oil on top of the objective lens.</li>
	<li>Clamp the dish tightly into the dish holder and load the dish holder onto the stage. 
	NOTE: The cells must be maintained at 37 &#176;C and 5% CO2 throughout the experiment.</li>
	<li>Adjust the height of the objective to bring the cells into focus (Plane A, Figure 1B).</li>
	<li>Move the microscope stage to find a cell of interest.</li>
	<li>Rotate the joystick on the micromanipulator to move the pipet holder to the top position. Load the 0.5 &#181;m diameter tip micropipette onto the pipet holder.
	<ol>
		<li>To avoid cell adhesion to the micropipette, pre-treat the micropipette tip with 0.3 mg/mL PLL-g-PEG solution for 1 h at room temperature. Test for adhesion by touching the micropipette to the nucleus without any suction pressure, and then translating the micropipette away from the nucleus. The absence of adhesion can be discerned from a complete lack of nuclear deformation and translation. 
		NOTE: Please follow manufacture suggestions to open the package.</li>
	</ol>
	</li>
	<li>Raise the objective focal plane above Plane A and the top of the cell to Plane B by adjusting the fine control (Figure 1B, see step 2.4).</li>
	<li>Set the micromanipulator to Coarse control. Slowly bring the micropipette down to Plane B by watching for the silhouette of the micropipette, until the micropipette comes fully into focus.</li>
	<li>Once the micropipette tip is in focus, set the micromanipulator to Fine control.</li>
	<li>Lower the objective to the equatorial plane of the cell (Plane A, Figure 1B) and lower the micropipette to around 15 &#181;m above Plane A (Figure 1B, dashed micropipette).</li>
	<li>Set the compensation pressure (Pc) on the microinjector to desired pressure; wait several seconds for the pressure to stabilize. 
	NOTE: The optimal pressure set point depends on both cell type and the specific goals of the experiment. For most cases, 300 hPa would be a good starting point.</li>
	<li>Ensure that the micropipette is not clogged by using the Clean setting on the micromanipulator panel and checking to make sure air bubbles emerge from the micropipette tip.</li>
	<li>Insert the tip into the cell by gradually lowering the micropipette until the tip is lightly touching the nuclear surface. 
	NOTE: When lowering the micropipette, the silhouette of the micropipette tip will become clear as it comes into focus. Before the micropipette touches the nucleus, raise the objective focus and align the micropipette tip with nucleus (same x-y coordinate, higher z-plane). Return the focus back to the equatorial plane of the nucleus (Plane A, Figure 1B) and gradually lower the micropipette tip.</li>
	<li>Create a seal between the micropipette tip and the nuclear membrane by disconnecting the pressure-supply tube from the microinjection system, thereby opening the end of the micropipette tube to the atmosphere. This step creates a negative pressure equal to&#160;Pc&#160;on the nuclear surface.</li>
	<li>Acquire images with the microscopes image collection software. Set up an avi-acquisition (video) or nd-acquisition (images) in the image collection software. 
	NOTE:&#160;For any imaging acquiring software, set up real-time video imaging or time-lapse image acquisitions with a short time interval.</li>
	<li>Toggle to the corresponding fluorescent imaging channel (i.e., GFP, RFP, etc.) and begin imaging.</li>
	<li>Translate the micropipette tip away from the body of the cell (to the right, Figure 1B) until the nucleus detaches from the micropipette. 
	NOTE: Pull the tip along the positive x-direction (to the right in the field of view). The pulling rate can be programmed and controlled by computer or the joystick can be moved manually. We have not found any correlation between the pulling rate and nuclear deformation15 suggesting a primarily elastic response to force.</li>
</ol>
3. Data Analysis
<ol>
	<li>Perform image analysis with any basic image-processing software available. The extent of nuclear deformation can be quantified by either the length strain (&#400;) or the area strain (Figure 1A). Quantify length strain using Equation 1, where L and L0 represent the lengths of the nucleus at maximum deformation and the initial position, respectively. 
	<img alt="Equation 1" src="/files/ftp_upload/58038/58038eq1.jpg" />&#160;(Equation 1)</li>
</ol>

<ol><li>Chow, K. H., Factor, R. E., Ullman, K. S. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((The+nuclear+envelope+environment+and+its+cancer+connections%5BTitle%5D)+AND+%22Nature+Reviews+Cancer%22%5BJournal%5D)">The nuclear envelope environment and its cancer connections.</a> Nature Reviews Cancer. 12 (3), 196-209 (2012).</li>
<li>Zink, D., Fischer, A. H., Nickerson, J. A. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((Nuclear+structure+in+cancer+cells%5BTitle%5D)+AND+%22Nature+Reviews+Cancer%22%5BJournal%5D)">Nuclear structure in cancer cells.</a> Nature Reviews Cancer. 4 (9), 677-687 (2004).</li>
<li>Bank, E. M., Gruenbaum, Y. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((The+nuclear+lamina+and+heterochromatin%3A+a+complex+relationship%5BTitle%5D)+AND+%22Biochemical+Society+Transactions%22%5BJournal%5D)">The nuclear lamina and heterochromatin: a complex relationship.</a> Biochemical Society Transactions. 39 (6), 1705-1709 (2011).</li>
<li>Lammerding, J., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((Lamins+A+and+C+but+not+lamin+B1+regulate+nuclear+mechanics%5BTitle%5D)+AND+%22Journal+of+Biological+Chemistry%22%5BJournal%5D)">Lamins A and C but not lamin B1 regulate nuclear mechanics.</a> Journal of Biological Chemistry. 281 (35), 25768-25780 (2006).</li>
<li>Dahl, K. N., Engler, A. J., Pajerowski, J. D., Discher, D. E. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((Power-law+rheology+of+isolated+nuclei+with+deformation+mapping+of+nuclear+substructures%5BTitle%5D)+AND+%22Biophysical+Journal%22%5BJournal%5D)">Power-law rheology of isolated nuclei with deformation mapping of nuclear substructures.</a> Biophysical Journal. 89 (4), 2855-2864 (2005).</li>
<li>Crisp, M., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((Coupling+of+the+nucleus+and+cytoplasm%3A+role+of+the+LINC+complex%5BTitle%5D)+AND+%22Journal+of+Cell+Biology%22%5BJournal%5D)">Coupling of the nucleus and cytoplasm: role of the LINC complex.</a> Journal of Cell Biology. 172 (1), 41-53 (2006).</li>
<li>Sosa, B. A., Rothballer, A., Kutay, U., Schwartz, T. U. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((LINC+complexes+form+by+binding+of+three+KASH+peptides+to+domain+interfaces+of+trimeric+SUN+proteins%5BTitle%5D)+AND+%22Cell%22%5BJournal%5D)">LINC complexes form by binding of three KASH peptides to domain interfaces of trimeric SUN proteins.</a> Cell. 149 (5), 1035-1047 (2012).</li>
<li>Tapley, E. C., Starr, D. A. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((Connecting+the+nucleus+to+the+cytoskeleton+by+SUN-KASH+bridges+across+the+nuclear+envelope%5BTitle%5D)+AND+%22Current+Opinion+in+Cell+Biology%22%5BJournal%5D)">Connecting the nucleus to the cytoskeleton by SUN-KASH bridges across the nuclear envelope.</a> Current Opinion in Cell Biology. 25 (1), 57-62 (2013).</li>
<li>Arsenovic, P. T., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((Nesprin-2G%2C+a+Component+of+the+Nuclear+LINC+Complex%2C+Is+Subject+to+Myosin-Dependent+Tension%5BTitle%5D)+AND+%22Biophysical+Journal%22%5BJournal%5D)">Nesprin-2G, a Component of the Nuclear LINC Complex, Is Subject to Myosin-Dependent Tension.</a> Biophysical Journal. 110 (1), 34-43 (2016).</li>
<li>Rowat, A. C., Lammerding, J., Ipsen, J. H. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((Mechanical+properties+of+the+cell+nucleus+and+the+effect+of+emerin+deficiency%5BTitle%5D)+AND+%22Biophysical+Journal%22%5BJournal%5D)">Mechanical properties of the cell nucleus and the effect of emerin deficiency.</a> Biophysical Journal. 91 (12), 4649-4664 (2006).</li>
<li>Rowat, A. C., Foster, L. J., Nielsen, M. M., Weiss, M., Ipsen, J. H. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((Characterization+of+the+elastic+properties+of+the+nuclear+envelope%5BTitle%5D)+AND+%22Journal+of+the+Royal+Society+Interface%22%5BJournal%5D)">Characterization of the elastic properties of the nuclear envelope.</a> Journal of the Royal Society Interface. 2 (2), 63-69 (2005).</li>
<li>Pagliara, S., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((Auxetic+nuclei+in+embryonic+stem+cells+exiting+pluripotency%5BTitle%5D)+AND+%22Nature+Materials%22%5BJournal%5D)">Auxetic nuclei in embryonic stem cells exiting pluripotency.</a> Nature Materials. 13 (6), 638-644 (2014).</li>
<li>Liu, H., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((In+situ+mechanical+characterization+of+the+cell+nucleus+by+atomic+force+microscopy%5BTitle%5D)+AND+%22ACS+Nanotechnology%22%5BJournal%5D)">In situ mechanical characterization of the cell nucleus by atomic force microscopy.</a> ACS Nanotechnology. 8 (4), 3821-3828 (2014).</li>
<li>Krause, M., Te Riet, J., Wolf, K. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((Probing+the+compressibility+of+tumor+cell+nuclei+by+combined+atomic+force-confocal+microscopy%5BTitle%5D)+AND+%22Physical+Biology%22%5BJournal%5D)">Probing the compressibility of tumor cell nuclei by combined atomic force-confocal microscopy.</a> Physical Biology. 10 (6), 065002(2013).</li>
<li>Neelam, S., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((Direct+force+probe+reveals+the+mechanics+of+nuclear+homeostasis+in+the+mammalian+cell%5BTitle%5D)+AND+%22Proceedings+of+the+National+Academy+of+Sciences+of+the+United+States+of+America%22%5BJournal%5D)">Direct force probe reveals the mechanics of nuclear homeostasis in the mammalian cell.</a> Proceedings of the National Academy of Sciences of the United States of America. 112 (18), 5720-5725 (2015).</li>
<li>Pajerowski, J. D., Dahl, K. N., Zhong, F. L., Sammak, P. J., Discher, D. E. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((Physical+plasticity+of+the+nucleus+in+stem+cell+differentiation%5BTitle%5D)+AND+%22Proceedings+of+the+National+Academy+of+Sciences+of+the+United+States+of+America%22%5BJournal%5D)">Physical plasticity of the nucleus in stem cell differentiation.</a> Proceedings of the National Academy of Sciences of the United States of America. 104 (40), 15619-15624 (2007).</li>
<li>Lammerding, J., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((Lamin+A%2FC+deficiency+causes+defective+nuclear+mechanics+and+mechanotransduction%5BTitle%5D)+AND+%22Journal+of+Clinical+Investigation%22%5BJournal%5D)">Lamin A/C deficiency causes defective nuclear mechanics and mechanotransduction.</a> Journal of Clinical Investigation. 113 (3), 370-378 (2004).</li>
<li>Chancellor, T. J., Lee, J., Thodeti, C. K., Lele, T. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((Actomyosin+tension+exerted+on+the+nucleus+through+nesprin-1+connections+influences+endothelial+cell+adhesion%2C+migration%2C+and+cyclic+strain-induced+reorientation%5BTitle%5D)+AND+%22Biophysical+Journal%22%5BJournal%5D)">Actomyosin tension exerted on the nucleus through nesprin-1 connections influences endothelial cell adhesion, migration, and cyclic strain-induced reorientation.</a> Biophysical Journal. 99 (1), 115-123 (2010).</li>
<li>Neelam, S., Dickinson, R. B., Lele, T. P. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/pubmed?term=((New+approaches+for+understanding+the+nuclear+force+balance+in+living%2C+adherent+cells%5BTitle%5D)+AND+%22Methods%22%5BJournal%5D)">New approaches for understanding the nuclear force balance in living, adherent cells.</a> Methods. 94, 27-32 (2016).</li>
</ol>

The authors have nothing to disclose.

Measuring the mechanical integration of the nucleus with the cytoskeleton is a challenge for most current methods, such as micropipette aspiration16, because they require either isolated nuclei (where the nucleus is decoupled from the cytoskeleton) or nuclei in suspended cells (where extracellular forces, such as traction forces, are absent). Force has been applied to the nucleus by applying biaxial strain to cells adherent to a membrane17,18</s...

Pathologies such as cancer involve alterations to nuclear shape and structure1,2, which are generally accompanied by a &#39;softening&#39; of the nucleus3,4. Nuclear resistance to mechanical deformation has been generally characterized by applying a force to isolated nuclei5.
The nucleus in cells is molecularly connected to the cytoskeleton by the Linker of Nucleoskeleton and Cytoskeleton (LINC) complex6,7,8,9. As a result, the nucleus is mechanically integrated with the cytoskeleton and, through cell-substratum adhesions, the extracellular matrix. Mechanically probing the nucleus inside adherent cells can provide insight into this mechanical integration. Methods to manipulate nuclei in living cells include micropipette aspiration10,11, and atomic force microscopy12,13,14. We recently described a direct force probe (DFP) that applies mechanical forces directly on the nucleus in a living adherent cell15.
Here, we outline the procedure for using a microinjection system that is commonly available in microscopy facilities to apply a known, nano-scale mechanical force directly to the nucleus in an adherent cell. A femtotip (0.5 &#181;m diameter micropipette tip) is mounted and connected to the microinjection system by a tube. The tip, positioned at a 45&#176; angle relative to the surface of the culture dish, is lowered until adjacent to the nuclear surface. The tube is then disconnected and opened to the atmosphere, which creates a negative suction pressure on the nuclear surface and seals the micropipette tip against the nuclear surface. Through translation of the micropipette tip, the nucleus is deformed and eventually (depending on the magnitude of force applied), detached from the micropipette. This detachment occurs when the restoring (resisting) forces, exerted by the nucleus and cell, equal the suction force applied by the micropipette. Analysis can be performed by measuring the displacement of the nucleus, the length strain (Equation 1), or the area strain (Figure 1A).

<table><tbody><tr><td>FluoroDish</td><td>WPI</td><td>FD35</td><td></td></tr><tr><td>SYTO 59</td><td>ThermoFisher Scientific</td><td>S11341</td><td></td></tr><tr><td>Femtotips&amp;nbsp;</td><td>Eppendorf</td><td>930000043</td><td></td></tr><tr><td>InjectMan NI2</td><td>Eppendorf</td><td>NA</td><td>discontinued, current equivalent model: InjectMan 4</td></tr><tr><td>FemtoJet</td><td>Eppendorf</td><td>NA</td><td>Current model FemtoJet 4i</td></tr><tr><td>Plan Fluor oil immersion 40x</td><td>Nikon</td><td>NA</td><td></td></tr><tr><td>Apo TIRF oil immersion 60x</td><td>Nikon</td><td>NA</td><td></td></tr><tr><td>Donor Bovine Serum (DBS)</td><td>ThermoFisher Scientific</td><td>16030074</td><td>NIH 3T3 serum</td></tr><tr><td>Dulbecco&#039;s Modification of Eagle&#039;s (DMEM)</td><td>Mediatech cellgro</td><td>MT10013CVRF</td><td>NIH 3T3 medium</td></tr><tr><td>Penicillin-Streptomycin&amp;nbsp;</td><td>Mediatech</td><td>MT30004CIRF</td><td>NIH 3T3 medium supplement</td></tr><tr><td>Immersion Oil Type LDF Non-Fluorescing</td><td>Nikon</td><td>77007</td><td>Immersion oil for objective lens&amp;nbsp;</td></tr></tbody></table>

a direct force probe for measuring mechanical integration between the nucleus and the cytoskeleton

The mechanical properties of the nucleus determine its response to mechanical forces generated in cells. Because the nucleus is molecularly continuous with the cytoskeleton, methods are needed to probe its mechanical behavior in adherent cells. Here, we discuss the direct force probe (DFP) as a tool to apply force directly to the nucleus in a living adherent cell. We attach a narrow micropipette to the nuclear surface with suction. The micropipette is translated away from the nucleus, which causes the nucleus to deform and translate. When the restoring force is equal to the suction force, the nucleus detaches and elastically relaxes. Because the suction pressure is precisely known, the force on the nuclear surface is known. This method has revealed that nano-scale forces are sufficient to deform and translate the nucleus in adherent cells, and identified cytoskeletal elements that enable the nucleus to resist forces. The DFP can be used to dissect the contributions of cellular and nuclear components to nuclear mechanical properties in living cells.

Figure 2A shows the forcing of an NIH 3T3 mouse fibroblast nucleus. As the micropipette tip is translated to the right, the nucleus deforms and eventually detaches from the micropipette tip. The length strain of the nucleus is seen to increase with increasing suction force (Figure 2B). The front edge of the nucleus (micropipette pulling edge) forms a nuclear protrusion and the trailing edge is displaced from its original position...

Watch this Scientific Journal Video about A Direct Force Probe for Measuring Mechanical Integration Between the Nucleus and the Cytoskeleton at JoVE.com

A Direct Force Probe for Measuring Mechanical Integration Between the Nucleus and the Cytoskeleton

In this protocol, we describe a micropipette method to directly apply a controlled force to the nucleus in a living cell. This assay allows interrogation of nuclear mechanical properties in the living, adherent cell.

The mechanical properties of the nucleus determine its response to mechanical forces generated in cells. Because the nucleus is molecularly continuous ...

a-direct-force-probe-for-measuring-mechanical-integration-between

Research

JoVE Journal

Biochemistry

15.3K Views.  University of Florida. In dit protocol beschrijven we een micropipet-methode om een gecontroleerde kracht direct toepassen in de kern in een levende cel. Deze bepaling laat ondervraging van nucleaire mechanische eigenschappen in de cel levend, aanhangend.

Video: A Direct Force Probe for Measuring Mechanical Integration Between the Nucleus and the Cytoskeleton

Fluorescence Biomembrane Force Probe: Concurrent Quantitation of Receptor-ligand Kinetics and Binding-induced Intracellular Signaling on a Single Cell

Membrane receptor-ligand interactions mediate many cellular functions. Binding kinetics and downstream signaling triggered by these molecular interactions are likely affected by the mechanical environment in which binding and signaling take place. A recent study demonstrated that mechanical force can regulate antigen recognition by and triggering of the T-cell receptor (TCR). This was made possible by a new technology we developed and termed fluorescence biomembrane force probe (fBFP), which combines single-molecule force spectroscopy with fluorescence microscopy. Using an ultra-soft human red blood cell as the sensitive force sensor, a high-speed camera and real-time imaging tracking techniques, the fBFP is of ~1 pN (10-12 N), ~3 nm and ~0.5 msec in force, spatial and temporal resolution. With the fBFP, one can precisely measure single receptor-ligand binding kinetics under force regulation and simultaneously image binding-triggered intracellular calcium signaling on a single live cell. This new technology can be used to study other membrane receptor-ligand interaction and signaling in other cells under mechanical regulation.

We describe a technique for concurrently measuring force-regulated single receptor-ligand binding kinetics and real-time imaging of calcium signaling in a single T lymphocyte.

Membrane receptor-ligand interactions mediate many cellular functions. Binding kinetics and downstream signaling triggered by these molecular interactions ...

Bioengineering

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 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. ...

Direct Force Measurements of Subcellular Mechanics in Confinement using Optical Tweezers

During the development of a multicellular organism, a single fertilized cell divides and gives rise to multiple tissues with diverse functions. Tissue morphogenesis goes in hand with molecular and structural changes at the single cell level that result in variations of subcellular mechanical properties. As a consequence, even within the same cell, different organelles and compartments resist differently to mechanical stresses; and mechanotransduction pathways can actively regulate their mechanical properties. The ability of a cell to adapt to the microenvironment of the tissue niche thus is in part due to the ability to sense and respond to mechanical stresses. We recently proposed a new mechanosensation paradigm in which nuclear deformation and positioning enables a cell to gauge the physical 3D environment and endows the cell with a sense of proprioception to decode changes in cell shape. In this article, we describe a new method to measure the forces and material properties that shape the cell nucleus inside living cells, exemplified on adherent cells and mechanically confined cells. The measurements can be performed non-invasively with optical traps inside cells, and the forces are directly accessible through calibration-free detection of light momentum. This allows measuring the mechanics of the nucleus independently from cell surface deformations and allowing dissection of exteroceptive and interoceptive mechanotransduction pathways. Importantly, the trapping experiment can be combined with optical microscopy to investigate the cellular response and subcellular dynamics using fluorescence imaging of the cytoskeleton, calcium ions, or nuclear morphology. The presented method is straightforward to apply, compatible with commercial solutions for force measurements, and can easily be extended to investigate the mechanics of other subcellular compartments, e.g., mitochondria, stress-fibers, and endosomes.

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.

During the development of a multicellular organism, a single fertilized cell divides and gives rise to multiple tissues with diverse functions. Tissue ...

Developmental Biology

Measurement of Force-Sensitive Protein Dynamics in Living Cells Using a Combination of Fluorescent Techniques

Cells sense and respond to physical cues in their environment by converting mechanical stimuli into biochemically-detectable signals in a process called mechanotransduction. A crucial step in mechanotransduction is the transmission of forces between the external and internal environments. To transmit forces, there must be a sustained, unbroken physical linkage created by a series of protein-protein interactions. For a given protein-protein interaction, mechanical load can either have no effect on the interaction, lead to faster disassociation of the interaction, or even stabilize the interaction. Understanding how molecular load dictates protein turnover in living cells can provide valuable information about the mechanical state of a protein, in turn elucidating its role in mechanotransduction. Existing techniques for measuring force-sensitive protein dynamics either lack direct measurements of protein load or rely on the measurements performed outside of the cellular context. Here, we describe a protocol for the F&#246;rster resonance energy transfer-fluorescence recovery after photobleaching (FRET-FRAP) technique, which enables the measurement of force-sensitive protein dynamics within living cells. This technique is potentially applicable to any FRET-based tension sensor, facilitating the study of force-sensitive protein dynamics in variety of subcellular structures and in different cell types.

Here, we present a protocol for the simultaneous use of F&#246;rster resonance energy transfer-based tension sensors to measure protein load and fluorescence recovery after photobleaching to measure protein dynamics enabling the measurement of force-sensitive protein dynamics within living cells.

Cells sense and respond to physical cues in their environment by converting mechanical stimuli into biochemically-detectable signals in a process called ...

Biophysical Assays to Probe the Mechanical Properties of the Interphase Cell Nucleus: Substrate Strain Application and Microneedle Manipulation

In most eukaryotic cells, the nucleus is the largest organelle and is typically 2 to 10 times stiffer than the surrounding cytoskeleton; consequently, the physical properties of the nucleus contribute significantly to the overall biomechanical behavior of cells under physiological and pathological conditions. For example, in migrating neutrophils and invading cancer cells, nuclear stiffness can pose a major obstacle during extravasation or passage through narrow spaces within tissues.1 On the other hand, the nucleus of cells in mechanically active tissue such as muscle requires sufficient structural support to withstand repetitive mechanical stress. Importantly, the nucleus is tightly integrated into the cellular architecture; it is physically connected to the surrounding cytoskeleton, which is a critical requirement for the intracellular movement and positioning of the nucleus, for example, in polarized cells, synaptic nuclei at neuromuscular junctions, or in migrating cells.2 Not surprisingly, mutations in nuclear envelope proteins such as lamins and nesprins, which play a critical role in determining nuclear stiffness and nucleo-cytoskeletal coupling, have been shown recently to result in a number of human diseases, including Emery-Dreifuss muscular dystrophy, limb-girdle muscular dystrophy, and dilated cardiomyopathy.3 To investigate the biophysical function of diverse nuclear envelope proteins and the effect of specific mutations, we have developed experimental methods to study the physical properties of the nucleus in single, living cells subjected to global or localized mechanical perturbation. Measuring induced nuclear deformations in response to precisely applied substrate strain application yields important information on the deformability of the nucleus and allows quantitative comparison between different mutations or cell lines deficient for specific nuclear envelope proteins. Localized cytoskeletal strain application with a microneedle is used to complement this assay and can yield additional information on intracellular force transmission between the nucleus and the cytoskeleton. Studying nuclear mechanics in intact living cells preserves the normal intracellular architecture and avoids potential artifacts that can arise when working with isolated nuclei. Furthermore, substrate strain application presents a good model for the physiological stress experienced by cells in muscle or other tissues (e.g., vascular smooth muscle cells exposed to vessel strain). Lastly, while these tools have been developed primarily to study nuclear mechanics, they can also be applied to investigate the function of cytoskeletal proteins and mechanotransduction signaling.

We present two independent, microscope-based tools to measure the induced nuclear and cytoskeletal deformations in single, living adherent cells in response to global or localized strain application. These techniques are used to determine nuclear stiffness (i.e., deformability) and to probe intracellular force transmission between the nucleus and the cytoskeleton.

In most eukaryotic cells, the nucleus is the largest organelle and is typically 2 to 10 times stiffer than the surrounding cytoskeleton; consequently, the ...

Biology

DNA Tension Probes to Map the Transient Piconewton Receptor Forces by Immune Cells

Mechanical forces transmitted at the junction between two neighboring cells and at the junction between cells and the extracellular matrix are critical for regulating many processes ranging from development to immunology. Therefore, developing the tools to study these forces at the molecular scale is critical. Our group developed a suite of molecular tension sensors to quantify and visualize the forces generated by cells and transmitted to specific ligands. The most sensitive class of molecular tension sensors are comprised of nucleic acid stem-loop hairpins. These sensors use fluorophore-quencher pairs to report on the mechanical extension and unfolding of DNA hairpins under force. One challenge with DNA hairpin tension sensors is that they are reversible with rapid hairpin refolding upon termination of the tension and thus transient forces are difficult to record. In this article, we describe the protocols for preparing DNA tension sensors that can be "locked" and prevented from refolding to enable "storing" of mechanical information. This allows for the recording of highly transient piconewton forces, which can be subsequently "erased" by the addition of complementary nucleic acids that remove the lock. This ability to toggle between real-time tension mapping and mechanical information storing reveals weak, short-lived, and less abundant forces, that are commonly employed by T cells as part of their immune functions.

This paper describes a detailed protocol for using DNA-based tension probes to image the receptor forces applied by immune cells. This approach can map receptor forces &gt;4.7pN in real-time and can integrate forces over time.

Mechanical forces transmitted at the junction between two neighboring cells and at the junction between cells and the extracellular matrix are critical ...

Protrusion Force Microscopy: A Method to Quantify Forces Developed by Cell Protrusions

In numerous biological contexts, animal cells need to interact physically with their environment by developing mechanical forces. Among these, traction forces have been well-characterized, but there is a lack of techniques allowing the measurement of the protrusion forces exerted by cells orthogonally to their substrate. We designed an experimental setup to measure the protrusion forces exerted by adherent cells on their substrate. Cells plated on a compliant Formvar sheet deform this substrate and the resulting topography is mapped by atomic force microscopy (AFM) at the nanometer scale. Force values are then extracted from an analysis of the deformation profile based on the geometry of the protrusive cellular structures. Hence, the forces exerted by the individual protruding units of a living cell can be measured over time. This technique will enable the study of force generation and its regulation in the many cellular processes involving protrusion. Here, we describe its application to measure the protrusive forces generated by podosomes formed by human macrophages.

Here, we detail the experimental techniques used to evaluate the protrusion forces that podosomes apply on a compliant film, from the preparation of the film to the automated analysis of topographical images.

In numerous biological contexts, animal cells need to interact physically with their environment by developing mechanical forces. Among these, traction ...

Isolating Myofibrils from Skeletal Muscle Biopsies and Determining Contractile Function with a Nano-Newton Resolution Force Transducer

Striated muscle cells are indispensable for the activity of humans and animals. Single muscle fibers are comprised of myofibrils, which consist of serially linked sarcomeres, the smallest contractile units in muscle. Sarcomeric dysfunction contributes to muscle weakness in patients with mutations in genes encoding for sarcomeric proteins. The study of myofibril mechanics allows for the assessment of actin-myosin interactions without potential confounding effects of damaged, adjacent myofibrils when measuring the contractility of single muscle fibers. Ultrastructural damage and misalignment of myofibrils might contribute to impaired contractility. If structural damage is present in the myofibrils, they likely break during the isolation procedure or during the experiment. Furthermore, studies in myofibrils provide the assessment of actin-myosin interactions in the presence of the geometrical constraints of the sarcomeres. For instance, measurements in myofibrils can elucidate whether myofibrillar dysfunction is the primary effect of a mutation in a sarcomeric protein. In addition, perfusion with calcium solutions or compounds is almost instant due to the small diameter of the myofibril. This makes myofibrils eminently suitable to measure the rates of activation and relaxation during force production. The protocol described in this paper employs an optical force probe based on the principle of a Fabry-P&#233;rot interferometer capable of measuring forces in the nano-Newton range, coupled to a piezo length motor and a fast-step perfusion system. This setup enables the study of myofibril mechanics with high resolution force measurements.

Presented here is a protocol to assess the contractile properties of striated muscle myofibrils with nano-Newton resolution. The protocol employs a setup with an interferometry-based, optical force probe. This setup generates data with a high signal-to-noise ratio and enables the assessment of the contractile kinetics of myofibrils.

Striated muscle cells are indispensable for the activity of humans and animals. Single muscle fibers are comprised of myofibrils, which consist of ...

Directly Measuring Forces Within Reconstituted Active Microtubule Bundles

Microtubule networks are employed in cells to accomplish a wide range of tasks, ranging from acting as tracks for vesicle transport to working as specialized arrays during mitosis to regulate chromosome segregation. Proteins that interact with microtubules include motors such as kinesins and dynein, which can generate active forces and directional motion, as well as non-motor proteins that crosslink filaments into higher-order networks or regulate filament dynamics. To date, biophysical studies of microtubule-associated proteins have overwhelmingly focused on the role of single motor proteins needed for vesicle transport, and significant progress has been made in elucidating the force-generating properties and mechanochemical regulation of kinesins and dyneins. However, for processes in which microtubules act both as cargo and track, such as during filament sliding within the mitotic spindle, much less is understood about the biophysical regulation of ensembles of the crosslinking proteins involved. Here, we detail our methodology for directly probing force generation and response within crosslinked microtubule minimal networks reconstituted from purified microtubules and mitotic proteins. Microtubule pairs are crosslinked by proteins of interest, one microtubule is immobilized to a microscope coverslip, and the second microtubule is manipulated by an optical trap. Simultaneous total internal reflection fluorescence microscopy allows for multichannel visualization of all the components of this microtubule network as the filaments slide apart to generate force. We also demonstrate how these techniques can be used to probe pushing forces exerted by kinesin-5 ensembles and how viscous braking forces arise between sliding microtubule pairs crosslinked by the mitotic MAP PRC1. These assays provide insights into the mechanisms of spindle assembly and function and can be more broadly adapted to study dense microtubule network mechanics in diverse contexts, such as the axon and dendrites of neurons and polar epithelial cells.

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.

Microtubule networks are employed in cells to accomplish a wide range of tasks, ranging from acting as tracks for vesicle transport to working as ...

Combining 3D Magnetic Force Actuator and Multi-Functional Fluorescence Imaging to Study Nucleus Mechanobiology

A fundamental question in mechanobiology is how living cells sense extracellular mechanical stimuli in the context of cell physiology and pathology. The cellular mechano-sensation of extracellular mechanical stimuli is believed to be through the membrane receptors, the associated protein complex, and the cytoskeleton. Recent advances in mechanobiology demonstrate that the cell nucleus in cytoplasm itself can independently sense mechanical stimuli simultaneously. However, a mechanistic understanding of how the cell nucleus senses, transduces, and responds to mechanical stimuli is lacking, mainly because of the technical challenges in accessing and quantifying the nucleus mechanics by conventional tools. This paper describes the design, fabrication, and implementation of a new magnetic force actuator that applies precise and non-invasive 3D mechanical stimuli to directly deform the cell nucleus. Using CRISPR/Cas9-engineered cells, this study demonstrates that this tool, combined with high-resolution confocal fluorescent imaging, enables the revelation of the real-time dynamics of a mechano-sensitive yes-associated protein (YAP) in single cells as a function of nucleus deformation. This simple method has the potential to bridge the current technology gap in the mechanobiology community and provide answers to the knowledge gap that exists in the relation between nucleus mechanotransduction and cell function.

This study presents a new protocol to directly apply mechanical force on the cell nucleus through magnetic microbeads delivered into the cytoplasm and to conduct simultaneous live-cell fluorescent imaging.

A fundamental question in mechanobiology is how living cells sense extracellular mechanical stimuli in the context of cell physiology and pathology. The ...

A Direct Force Probe for Measuring Mechanical Integration Between the Nucleus and the Cytoskeleton

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