Abstract

Flagella of eukaryotic cells are transient long cylindrical protrusions. The proteins needed to form and maintain flagella are synthesized in the cell body and transported to the distal tips. What ‘rulers’ or ‘timers’ a specific type of cells use to strike a balance between the outward and inward transport of materials so as to maintain a particular length of its flagella in the steady state is one of the open questions in cellular self-organization. Even more curious is how the two flagella of biflagellates, like Chlamydomonas reinhardtii, communicate through their base to coordinate their lengths. In this paper we develop a stochastic model for flagellar length control based on a time-of-flight (ToF) mechanism. This ToF mechanism decides whether or not structural proteins are to be loaded onto an intraflagellar transport (IFT) train just before it begins its motorized journey from the base to the tip of the flagellum. Because of the ongoing turnover, the structural proteins released from the flagellar tip are transported back to the cell body also by IFT trains. We represent the traffic of IFT trains as a totally asymmetric simple exclusion process (TASEP). The ToF mechanism for each flagellum, together with the TASEP-based description of the IFT trains, combined with a scenario of sharing of a common pool of flagellar structural proteins in biflagellates, can account for all key features of experimentally known phenomena. These include ciliogenesis, resorption, deflagellation as well as regeneration after selective amputation of one of the two flagella. We also show that the experimental observations of Ishikawa and Marshall are consistent with the ToF mechanism of length control if the effects of the mutual exclusion of the IFT trains captured by the TASEP are taken into account. Moreover, we make new predictions on the flagellar length fluctuations and the role of the common pool.

Highlights

  • In a classic article, titled “on being the right size”, J.B.S

  • We show that the experimental observations of Ishikawa and Marshall are consistent with the ToF mechanism of length control if the effects of the mutual exclusion of the intraflagellar transport (IFT) trains captured by the totally asymmetric simple exclusion process (TASEP) are taken into account

  • We begin with a model for length control of a single flagellum that incorporates all the following key features: (i) a ToF mechanism for length sensing [36], (ii) a mechanism of differential-loading of flagellar structural proteins as cargo on the IFT trains [37, 38], (iii) a TASEP-based representation of the collective traffic-like movement of IFT trains [31], (iv) a flagellar elongation rate that is proportional to anterograde flux of the flagellar structural proteins at the flagellar tip, (v) a flagellar shortening rate that is independent of the flagellar length, but dependent on the extent of IFT density at the flagellar tip, and (vi) synthesis and degradation of flagellar structural proteins in the cell body

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Summary

INTRODUCTION

In a classic article, titled “on being the right size”, J.B.S. Haldane [1] first analyzed the physical reasons that explain why “for every type of animal there is a convenient size”. We begin with a model for length control of a single flagellum that incorporates all the following key features: (i) a ToF mechanism for length sensing [36], (ii) a mechanism of differential-loading of flagellar structural proteins as cargo on the IFT trains [37, 38], (iii) a TASEP-based representation of the collective traffic-like movement of IFT trains [31], (iv) a flagellar elongation rate that is proportional to anterograde flux of the flagellar structural proteins at the flagellar tip, (v) a flagellar shortening rate that is independent of the flagellar length, but dependent on the extent of IFT density at the flagellar tip, and (vi) synthesis and degradation of flagellar structural proteins in the cell body.

Structures of Flagella
TIME OF FLIGHT FOR MEASURING LENGTH: ‘RULER’ IS A ‘TIMER’
STOCHASTIC MODEL FOR LENGTH CONTROL OF A SINGLE FLAGELLUM
Fokker-Planck Equation for a single flagellum
Rate Equations for a single flagellum
Steady-state of a flagellum: a “balance point”
Ciliogenesis: controlled assembly of a single flagellum
Effects of precursor pool on length of a flagellum
EXPERIMENTAL SUPPORTS FOR THE MODEL
Experimental test for the validities of ToF mechanism and TASEP for IFT
Role of depolymerases in the ‘balance-point’ scenario
STOCHASTIC MODEL FOR LENGTH CONTROL IN BIFLAGELLATES
Master equations for a biflagellate
VIII. RESULTS
Resorption in our model: a plausible scenario
An alternative scenario of resorption in our model
Flagellar dynamics after deflagellation and subsequent regeneration
Flagellar dynamics after selective amputation and subsequent regeneration
Beyond mean: fluctuations and correlation
COMPARISON WITH OTHER MODELS
SUMMARY AND CONCLUSIONS
33 Appendix E
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