{"title":"有丝分裂纺锤体动力学模型中的弛豫和噪声驱动振荡","authors":"Dionn Hargreaves, Sarah Woolner, Oliver E. Jensen","doi":"arxiv-2402.10638","DOIUrl":null,"url":null,"abstract":"During cell division, the mitotic spindle moves dynamically through the cell\nto position the chromosomes and determine the ultimate spatial position of the\ntwo daughter cells. These movements have been attributed to the action of\ncortical force generators which pull on the astral microtubules to position the\nspindle, as well as pushing events by these same microtubules against the cell\ncortex and membrane. Attachment and detachment of cortical force generators\nworking antagonistically against centring forces of microtubules have been\nmodelled previously (Grill et al. 2005, Phys. Rev. Lett. 94:108104) via\nstochastic simulations and Fokker-Planck equations to predict oscillations of a\nspindle pole in one spatial dimension. Using systematic asymptotic methods, we\nreduce the Fokker-Planck system to a set of ordinary differential equations\n(ODEs), consistent with a set proposed by Grill et al., which provide accurate\npredictions of the conditions for the Fokker-Planck system to exhibit\noscillations. In the limit of small restoring forces, we derive an algebraic\nprediction of the amplitude of spindle-pole oscillations and demonstrate the\nrelaxation structure of nonlinear oscillations. We also show how noise-induced\noscillations can arise in stochastic simulations for conditions in which the\nFokker-Planck system predicts stability, but for which the period can be\nestimated directly by the ODE model.","PeriodicalId":501170,"journal":{"name":"arXiv - QuanBio - Subcellular Processes","volume":"9 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-02-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Relaxation and noise-driven oscillations in a model of mitotic spindle dynamics\",\"authors\":\"Dionn Hargreaves, Sarah Woolner, Oliver E. Jensen\",\"doi\":\"arxiv-2402.10638\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"During cell division, the mitotic spindle moves dynamically through the cell\\nto position the chromosomes and determine the ultimate spatial position of the\\ntwo daughter cells. These movements have been attributed to the action of\\ncortical force generators which pull on the astral microtubules to position the\\nspindle, as well as pushing events by these same microtubules against the cell\\ncortex and membrane. Attachment and detachment of cortical force generators\\nworking antagonistically against centring forces of microtubules have been\\nmodelled previously (Grill et al. 2005, Phys. Rev. Lett. 94:108104) via\\nstochastic simulations and Fokker-Planck equations to predict oscillations of a\\nspindle pole in one spatial dimension. Using systematic asymptotic methods, we\\nreduce the Fokker-Planck system to a set of ordinary differential equations\\n(ODEs), consistent with a set proposed by Grill et al., which provide accurate\\npredictions of the conditions for the Fokker-Planck system to exhibit\\noscillations. In the limit of small restoring forces, we derive an algebraic\\nprediction of the amplitude of spindle-pole oscillations and demonstrate the\\nrelaxation structure of nonlinear oscillations. We also show how noise-induced\\noscillations can arise in stochastic simulations for conditions in which the\\nFokker-Planck system predicts stability, but for which the period can be\\nestimated directly by the ODE model.\",\"PeriodicalId\":501170,\"journal\":{\"name\":\"arXiv - QuanBio - Subcellular Processes\",\"volume\":\"9 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-02-16\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - QuanBio - Subcellular Processes\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2402.10638\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - QuanBio - Subcellular Processes","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2402.10638","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Relaxation and noise-driven oscillations in a model of mitotic spindle dynamics
During cell division, the mitotic spindle moves dynamically through the cell
to position the chromosomes and determine the ultimate spatial position of the
two daughter cells. These movements have been attributed to the action of
cortical force generators which pull on the astral microtubules to position the
spindle, as well as pushing events by these same microtubules against the cell
cortex and membrane. Attachment and detachment of cortical force generators
working antagonistically against centring forces of microtubules have been
modelled previously (Grill et al. 2005, Phys. Rev. Lett. 94:108104) via
stochastic simulations and Fokker-Planck equations to predict oscillations of a
spindle pole in one spatial dimension. Using systematic asymptotic methods, we
reduce the Fokker-Planck system to a set of ordinary differential equations
(ODEs), consistent with a set proposed by Grill et al., which provide accurate
predictions of the conditions for the Fokker-Planck system to exhibit
oscillations. In the limit of small restoring forces, we derive an algebraic
prediction of the amplitude of spindle-pole oscillations and demonstrate the
relaxation structure of nonlinear oscillations. We also show how noise-induced
oscillations can arise in stochastic simulations for conditions in which the
Fokker-Planck system predicts stability, but for which the period can be
estimated directly by the ODE model.