2015
DOI: 10.1103/physreve.92.042714
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Intercentrosomal angular separation during mitosis plays a crucial role for maintaining spindle stability

Abstract: Cell division through proper spindle formation is one of the key puzzles in cell biology. In most mammalian cells, chromosomes spontaneously arrange to achieve a stable bipolar spindle during metaphase which eventually ensures proper segregation of the DNA into the daughter cells. In this paper, we present a robust three-dimensional mechanistic model to investigate the formation and maintenance of a bipolar mitotic spindle in mammalian cells under different physiological constraints. Using realistic parameters… Show more

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Cited by 8 publications
(35 citation statements)
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“…Further, we find that for sufficiently small kinetochore-MT interaction strength, both bipolar spindle structure and monopolar structure (with zero separation distance between centrosomes) are stable as has been observed in numerical studies of Ref. [3,4]. We also find a regime of bistability of spindle assembly for certain parameter range wherein the spindle can be stable for two different finite separation distance between centrosomes.…”
supporting
confidence: 78%
See 1 more Smart Citation
“…Further, we find that for sufficiently small kinetochore-MT interaction strength, both bipolar spindle structure and monopolar structure (with zero separation distance between centrosomes) are stable as has been observed in numerical studies of Ref. [3,4]. We also find a regime of bistability of spindle assembly for certain parameter range wherein the spindle can be stable for two different finite separation distance between centrosomes.…”
supporting
confidence: 78%
“…During mitotic cell division, the two centrosomes within the cell serves as the poles and nucleating sites for microtubules (MTs). The polymerizing MTs from the opposite centrosomes overlap, leading to the formation of spindle structure during metaphase [1][2][3][4] (see Fig. 1).…”
mentioning
confidence: 99%
“…1). Using conventional assumptions of a large number of isotropically distributed MTs (19,(41)(42)(43), we introduce the expressions for f CS−CS , and for respective potential energy of moving one CS from distance r 1 to r 2 away from another CS: Here f (0) CS−CS is the force between a pair of proximal CSs, r is the distance between CSs and L 1 is the spatial range of the force. Here we utilize one of the most simple and frequently used exponentially decreasing spatial dependence of the force; in the Supporting Information we explore other spatial dependencies.…”
Section: Methodsmentioning
confidence: 99%
“…1). Using conventional assumptions of a large number of isotropically distributed MTs (19,(41)(42)(43), we introduce the expressions for f CS−CS , and for respective potential energy of moving one CS from distance r 1 to r 2 away from another CS: In confinement of the cell volume, but without active interaction with the cortex, multipolar spindle emerges when CSs repel each other. (C) CSs aggregate into two clusters at the opposite cell poles, which chromosomes gather at the equator, creating bipolar spindle, when CSs are mutually attractive and also are attracted to the cell cortex ( f CS−C RT X ).…”
Section: Interactions Between Pairs Of Cssmentioning
confidence: 99%