1 / 19

Mitosis

Mitosis. Microtubules and Motors: MT polymer ratchets and motor proteins. F ~1-50pN. F ~ 1-10pN. Microtubule Polymer Dynamics. Dynamic Instability. (Mitchison and Kirschner, 1984). Teadmilling/Flux. (Margolis and Wilson, 1978; Mitchison, 1989). v g , v s , f res , f cat.

abby
Download Presentation

Mitosis

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Mitosis

  2. Microtubules and Motors: MT polymer ratchets and motor proteins. F ~1-50pN F ~ 1-10pN

  3. Microtubule Polymer Dynamics Dynamic Instability. (Mitchison and Kirschner, 1984). Teadmilling/Flux. (Margolis and Wilson, 1978; Mitchison, 1989). vg , vs, fres, fcat dn/dt = Kon[C] - Koff

  4. 1953: Shinya Inoue uses polarizing light microscopy

  5. Dynamic Equilibrium (Inoue, 1967).Poleward Flux (Forer, 1965). Steady state fibers polymerize at equator; depolymerize at poles. Polymerize/push; depolymerize/pull.

  6. The Spindle Machine: Drosophila spindle MTs display poleward flux AND dynamic instability. t1/2 = 5s (versus Ptk t1/2 = 400s). • How do microtubules and motors drive mitotic motility. • How are smooth, accurate movements produced if the microtubule tracks are constantly growing and shrinking.

  7. E.M. analysis by McIntosh et al, 1969-80: Sliding Filaments

  8. Polarity of MTs in the Spindle Interzone.

  9. Force Generation by Spindle Fibers. Ostegren, 1951; Force balance. Nicklas, 1983; 1 nN stall force. • Antagonistic poleward forces. • Force proportional to distance • from pole. • Forces balance at metaphase. • Poleward forces drive anaphase A

  10. Mitotic Force Generators. b. MT depolymerizing motors. a. MT polymer Ratchets. c. MT crosslinking and sliding motors.

  11. Metaphase Anaphase A Anaphase B Mechanism of Anaphase A and B

  12. Model for Anaphase B • Kinesin-5-dependent ipMT slidingpushes poles apart • Poleward Flux is an “on-off” Switch (Brust-Mascher et al, 2004, PNAS,101, 15938; Cheerambathur et al, 2007, JCB, 177, 995)

  13. f3 S(t) f2 f2 v1 v2 v3 f1 v4 L12 vpoly contains vgrow ,vshrink , fcat , fres Anaphase B Model Equations 1. dS/dt = 2 (vsliding- vdep) 2. dL/dt = 2 (vpoly - vsliding) 3. μ·(dS/dt) / 2 = k·N·L·Fm(1 - vsliding / Vm) (Gul Civelekoglu-Scholey)

  14. Model Results Conclude: Anaphase B – kinesin-5 motors drive ipMT sliding and flux = on/off switch

  15. Sharp et al. Nature Cell Biol, 2000 • Brust-Mascher & Scholey. MBC, 2002 • Brust-Mascher et al. PNAS, 2004 • Rogers et al. Nature, 2004 Rapid MT turnover: FRAP t1/2 ~ 5 sec MT Flux, Sliding and Pacman sliding: KLP61F flux: KLP10A Metaphase: sliding: KLP61F flux: KLP10A pacman: KLP59C Dynein Anaphase A: sliding: KLP61F flux: turned off Anaphase B:

  16. Metaphase Anaphase A Anaphase B Mechanism of Anaphase A

  17. Mechanism of Anaphase A. Kinetochore motility - Pacman versus poleward flux.

  18. Coupled kinesin-13 dependent flux-pacman model for anaphase A. (Rogers et al, 2004, Nature; 427, 364.)

  19. Cytokinesis in Animal Cells.

More Related