Attachment conditions control actin filament buckling and the production of forces

被引:37
作者
Berro, Julien
Michelot, Alphee
Blanchoin, Laurent
Kovar, David R.
Martiel, Jean-Louis [1 ]
机构
[1] Inst Natl Sante & Rech Med, Lab Tech Imagerie, F-38706 La Tronche, France
[2] Univ Grenoble 1, F-38706 La Tronche, France
[3] INRA, Ctr Natl Rech Sci, Lab Physiol Cellulaire Veg, Inst Rech & Technol & Sci Vivant, F-38054 Grenoble, France
[4] Univ Chicago, Dept Mol Genet & Cell Biol, Chicago, IL 60637 USA
[5] Univ Chicago, Dept Biochem, Chicago, IL 60637 USA
[6] Univ Chicago, Dept Mol Biol, Chicago, IL 60637 USA
关键词
D O I
10.1529/biophysj.106.094672
中图分类号
Q6 [生物物理学];
学科分类号
071011 ;
摘要
Actin polymerization is the driving force for a large number of cellular processes. Formation of lamellipodia and fllopodia at the leading edge of motile cells requires actin polymerization induced mechanical deformation of the plasma membrane. To generate different types of membrane protrusions, the mechanical properties of actin. laments can be constrained by interacting proteins. A striking example of such constraint is the buckling of actin. laments generated in vitro by the cooperative effect of a processive actin nucleating factor (formin) and a molecular motor (myosin II). We developed a physical model based on equations for an elastic rod that accounts for actin. lament buckling. Both ends of the rod were maintained in a fixed position in space and we considered three sets of boundary conditions. The model qualitatively and quantitatively reproduces the shape distribution of actin. laments. We found that actin polymerization counterpoises a force in the range 0.4-1.6 pN for moderate end-to-end distance (similar to 1 mu m) and could be as large as 10 pN for shorter distances. If the actin rod attachment includes a spring, we discovered that the stiffness must be in the range 0.1-1.2 pN/nm to account for the observed buckling.
引用
收藏
页码:2546 / 2558
页数:13
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