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Over the past few decades, the importance of the mechanical properties of a cellās environment has garnered increasing recognition in cell biology. Different tissues and extracellular matrices have different relative stiffnesses and, as cells migrate throughout the body, they navigate these changes, using these mechanical properties to guide them1,2,3,4,5,6,7. Cells use the stiffness of a given tissue to inform their motile behavior during processes such as development, wound healing, and cancer metastasis. However, the molecular mechanisms that allow sensation of and response to these mechanical inputs remain largely unknown1,2,3,4,5,6,7.
In order to study the mechanisms through which cells respond to physical environmental cues, the rigidity or stiffness of the substrate underlying adherent cells must be manipulated. In 2000, Chun-Min Lo, Yu-Li Wang and colleagues developed an assay8 whereby an individual cellās motile response to changing mechanical cues could be directly tested by stretching deformable extracellular matrix (ECM)-coated polyacrylamide hydrogels on which the cells were plated. Cells exhibits a significant preference for migrating towards stiffer substrates, a phenomenon they dubbed ādurotaxis.ā
Since the original report in 2000, many other techniques have been employed for the study of durotaxis. Steep stiffness gradients have been fabricated by casting gels over rigid features such as polystyrene beads9 or stiff polymer posts10 or by polymerizing the substrate around the edges of a glass coverslips11 to create mechanical āstep-boundariesā. Alternatively, hydrogels with shallower but fixed stiffness gradients have been fabricated by a variety of methods such as gradients of crosslinker created by microfluidic devices12,13 or side-by-side hydrogel solution droplets of differing stiffness8, or hydrogels with photoreactive crosslinker treated with graded UV light exposure to create a linear stiffness gradient14,15. These techniques have been used to great effect to investigate durotactic cellular movement en masse over time. However, typically these features are fabricated in advance of cell plating and their properties remain consistent over the course of the experiment, relying on random cell movement for sampling of mechanical gradients. None of these techniques are amenable to observation of rapid changes in cellular behavior in response to acute mechanical stimulus.
In order to observe cellular responses to acute changes in the mechanical environment, single cell durotaxis assays offer several advantages. In these assays, individual cells are given an acute, mechanical stimulus by pulling the underlying substrate away from the cell with a glass micropipette, thereby introducing a directional gradient of cell-matrix tension. Changes in the motile behavior, such as speed or direction of migration, are then observed by live-cell phase contrast microscopy. This approach facilitates direct observation of cause and effect relationships between mechanical stimuli and cell migration, as it allows rapid, iterative manipulation of the direction and magnitude of the tension gradient and assessment of consequent cellular responses in real time. Further, this method can also be used to mechanically stimulate cells expressing fluorescent fusion proteins or biosensors to visualize changes in the amount, activity, or subcellular localization of proteins suspected to be involved in mechanosensing and durotaxis.
This technique has been employed by groups who study durotaxis8,16 and is described here as it has been adapted by the Howe Laboratory to study the durotactic behavior of SKOV-3 ovarian cancer cells and the molecular mechanisms that underly durotaxis17. Additionally, a modified method is described for fabrication of hydrogels with a single, even layer of fluorescent microspheres near the cell culture surface; this facilitates visualization and optimization of micropipette-generated strain gradients and may allow assessment of cell contractility by traction force microscopy.