title: Quantifying the contribution of actin networks to the elastic strength of fibroblasts.
abstract: The structural models created to understand the cytoskeletal mechanics of cells in suspension are described here. Suspended cells can be deformed by well-defined surface stresses in an Optical Stretcher [Guck, J., Ananthakrishnan, R., Mahmood, H., Moon, T.J., Cunningham, C.C., Käs, J., 2001. The optical stretcher: a novel laser tool to micromanipulate cells. Biophys. J. 81(2), 767-784], a two-beam optical trap designed for the contact-free deformation of cells. Suspended cells have a well-defined cytoskeleton, displaying a radially symmetric actin cortical network underlying the cell membrane with no actin stress fibers, and microtubules and intermediate filaments in the interior. Based on experimental data using suspended fibroblasts, we create two structural models: a thick shell actin cortex model that describes cell deformation for a localized stress distribution on these cells and a three-layered model that considers the entire cytoskeleton when a broad stress distribution is applied. Applying the models to data, we obtain a (actin) cortical shear moduli G of approximately 220 Pa for normal fibroblasts and approximately 185 Pa for malignantly transformed fibroblasts. Additionally, modeling the cortex as a transiently crosslinked isotropic actin network, we show that actin and its crosslinkers must be co-localized into a tight shell to achieve these cortical strengths. The similar moduli values and cortical actin and crosslinker densities but different deformabilities of the normal and cancerous cells suggest that a cell's structural strength is not solely determined by cytoskeletal composition but equally importantly by (actin) cytoskeletal architecture via differing cortical thicknesses. We also find that although the interior structural elements (microtubules, nucleus) contribute to the deformed cell's exact shape via their loose coupling to the cortex, it is the outer actin cortical shell (and its thickness) that mainly determines the cell's structural response.
authors.affiliation: Institute for Soft Matter Physics, University of Leipzig, 04103 Leipzig, Germany. revathi@ucdavis.edu <revathi@ucdavis.edu>
authors.forename: Revathi
authors.initials: R
authors.lastname: Ananthakrishnan
authors.forename: Jochen
authors.initials: J
authors.lastname: Guck
authors.forename: Falk
authors.initials: F
authors.lastname: Wottawah
authors.forename: Stefan
authors.initials: S
authors.lastname: Schinkinger
authors.forename: Bryan
authors.initials: B
authors.lastname: Lincoln
authors.forename: Maren
authors.initials: M
authors.lastname: Romeyke
authors.forename: Tess
authors.initials: T
authors.lastname: Moon
authors.forename: Josef
authors.initials: J
authors.lastname: Käs
mesh_terms: D000199:Actins / Q000502:physiology*; D000818:Animals; D002467:Cell Nucleus / Q000502:physiology; D048430:Cell Shape / Q000502:physiology; D003599:Cytoskeleton / Q000502:physiology; D004548:Elasticity; D005347:Fibroblasts / Q000502:physiology*; D020342:Finite Element Analysis; D008870:Microtubules / Q000502:physiology; D008954:Models, Biological; D013314:Stress, Mechanical
chemical_list: D000199:Actins