In cancer metastasis and other physiological processes, cells migrate through the three-dimensional (3D) extracellular matrix of connective tissue and must overcome the steric hindrance posed by pores that are smaller than the cells. It is currently assumed that low cell stiffness promotes cell migration through confined spaces, but other factors such as adhesion and traction forces may be equally important. To study 3D migration under confinement in a stiff (1.77 MPa) environment, we use soft lithography to fabricate polydimethylsiloxane (PDMS) devices consisting of linear channel segments with 20 μm length, 3.7 μm height, and a decreasing width from 11.2 to 1.7 μm. To study 3D migration in a soft (550 Pa) environment, we use self-assembled collagen networks with an average pore size of 3 μm. We then measure the ability of four different cancer cell lines to migrate through these 3D matrices, and correlate the results with cell physical properties including contractility, adhesiveness, cell stiffness, and nuclear volume. Furthermore, we alter cell adhesion by coating the channel walls with different amounts of adhesion proteins, and we increase cell stiffness by overexpression of the nuclear envelope protein lamin A. Although all cell lines are able to migrate through the smallest 1.7 μm channels, we find significant differences in the migration velocity. Cell migration is impeded in cell lines with larger nuclei, lower adhesiveness, and to a lesser degree also in cells with lower contractility and higher stiffness. Our data show that the ability to overcome the steric hindrance of the matrix cannot be attributed to a single cell property but instead arises from a combination of adhesiveness, nuclear volume, contractility, and cell stiffness.

We describe a method for quantifying the mechanical properties of cells in suspension with a microfluidic device consisting of a parallel array of micron-sized constrictions. Using a high-speed charge-coupled device camera, we measure the flow speed, cell deformation, and entry time into the constrictions of several hundred cells per minute during their passage through the device. From the flow speed and the occupation state of the microconstriction array with cells, the driving pressure across each constriction is continuously computed. Cell entry times into microconstrictions decrease with increased driving pressure and decreased cell size according to a power law. From this power-law relationship, the cell elasticity and fluidity can be estimated. When cells are treated with drugs that depolymerize or stabilize the cytoskeleton or the nucleus, elasticity and fluidity data from all treatments collapse onto a master curve. Power-law rheology and collapse onto a master curve are predicted by the theory of soft glassy materials and have been previously shown to describe the mechanical behavior of cells adhering to a substrate. Our finding that this theory also applies to cells in suspension provides the foundation for a quantitative high-throughput measurement of cell mechanical properties with microfluidic devices.

We have investigated and quantified the nuclear A-type lamin pool from human HeLa S3 suspension cells with respect to their distribution to detergent soluble and insoluble fractions. We devised a sequential extraction protocol and found that maximally 10% of A-type lamins are recovered in the soluble fraction. Notably, lamin C is enriched in low detergent fractions and only with 0.5% Nonidet P-40 lamin A and C are recovered in ratios nearly equivalent to those found in whole cell extracts and in the lamina fraction. Authentic nucleoplasmic proteins such as LAP2a, pRB and p53 are co-extracted to a large part together with the A-type lamins in these fractions. By sucrose density centrifugation we revealed that the majority of lamins co-sedimented with human IgG indicating they form rather small complexes in the range of dimers and slightly larger complexes. Some lamin A - but not lamin C - is obtained in addition in a much faster sedimenting fraction. Authentic nuclear proteins such as PCNA, p53 and LAP2a were found both in the light and the heavy sucrose fractions together with lamin A. Last but not least, immunoprecipitation experiments from both soluble fractions and from RIPA lysates of whole cells revealed that lamin A and lamin C do not form heterodimers but segregate practically completely. Correspondingly, immunofluorescence microscopy of formaldehyde-fixed cells clearly demonstrated that lamin A and C are localized at least in part to distinct patches within the lamina. Hence, the structural segregation of lamin A and C is indeed retained in the nuclear envelope to some extent too.