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CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

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Page 1: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

CB201_12Tim Mitchison Lecture 3

Force generation by polymerization dynamics

Nucleation: controlling where and when polymers form

Page 2: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Force generation by the cytoskeleton

One of the main functions of the actin and microtubule cytoskeletons, and their prokaryotic counterparts, is to generate force for cell motility in a spatially and temporally controlled manner

Page 3: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Force generation by the cytoskeleton

One of the main functions of the actin and microtubule cytoskeletons, and their prokaryotic counterparts, is to generate force for cell motility in a spatially and temporally controlled manner

Force from polymerization dynamics

Eukaryotes and prokaryotes

Page 4: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Force generation by the cytoskeleton

One of the main functions of the actin and microtubule cytoskeletons, and their prokaryotic counterparts, is to generate force for cell motility in a spatially and temporally controlled manner

Force from polymerization dynamics

Eukaryotes and prokaryotes

ATPase motor proteins

Only Eukaryotes

Page 5: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Polymerization dynamics can perform mechanical work by pushing or pulling

Pushing by polymerizationLeading edge protrusion (actin)Listeria motility (actin)Plasmid separation in bacteria (ParM)

Pulling by depolymerizationChromosome movement in mitosis(microtubules)

Page 6: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Mechanical work requires enery dissipation

Mechanical work performed = force x distance

Total energy dissipated = G per elementary step x number of steps taken

Efficiency = work done/energy dissipated

In general, the efficiency of converting chemical energy into mechanical work must be less than 100% if the process that does the work is to proceed unidirectionally – ie some heat must be dissipated to make the process irreversible. This law of thermodynamics was developed for steam engines but applies equally to biology

The efficiency of biological motors can be quite high. Food human rowing Total efficiency = ~ 20%Food ATP efficiency = ~40%Therefore, effecience of ATP mechanical work in muscle = ~50%(Wikipedia)

Page 7: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Elementary steps

+

Actin filaments grow by ~2nm per subunit(Actin monomer is ~4nm long, filament has 2 strands)

Kinesin moves 8nm per step

Page 8: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Elementary steps

+

Actin filaments grow by ~2nm per subunit

Kinesin moves 8nm per step

Each step is coupled to hydrolysis of 1 molecule of ATP to ADP + Pi

This liberates ~8-12 kilocal per mol(= ~20kT per molecule)Bolzman constant

~4pN.nm

Page 9: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Elementary steps

Kinesin moves 8nm per step

Each step is coupled to hydrolysis of 1 molecule of ATP to ADP + Pi

This liberates ~8-12 kilocal per mol(= ~20kT per molecule)

Efficiency = 5pN.8nm/20kT = ~50%

Force distance Chemical energy dissipated

Page 10: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Elementary steps

+

Actin filaments grow by ~2nm per subunit(4nm subunit, 2 stranded polymer)

Kinesin moves 8nm per step

Each step is coupled to hydrolysis of 1 molecule of ATP to ADP + Pi

This liberates ~8-12 kilocal per mol(= ~20kT per molecule)

How do we think about force generation from polymerization or depolymerization?

Page 11: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Microtubule polymerizing in a microfabricated box. The force from polymerization causes the microtubule to buckle. Polymerization slows as the force on the ends increases. Eventually a catastrophe occurs.M. Dogterom and coworkers Science 278:856(1997), J Cell Biol 161:1029(2003)

Page 12: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Microtubule polymerizing in a microfabricated box. The force from polymerization causes the microtubule to buckle. Polymerization slows as the force on the ends increases. Eventually a catastrophe occurs.M. Dogterom and coworkers Science 278:856(1997), J Cell Biol 161:1029(2003)

How much force? Simple argument for maximum possible force:For every tubulin added, the microtubules grows 8/13nmSuppose the full energy of GTP hydrolysis is used to promote this reactionGTP -> GDP + G = ~ -50 kJ/mol = 5x10-4 /6x10-23 J/microtubule Force = work/distance = ~ 10-19/0.5x10-9 = ~2x10-10 N = ~200pN

Page 13: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Microtubule polymerizing in a microfabricated box. The force from polymerization causes the microtubule to buckle. Polymerization slows as the force on the ends increases. Eventually a catastrophe occurs.M. Dogterom and coworkers Science 278:856(1997), J Cell Biol 161:1029(2003)

How much force? Simple argument for maximum possible force:For every tubulin added, the microtubules grows 8/13nmSuppose the full energy of GTP hydrolysis is used to promote this reactionGTP -> GDP + G = ~ -50 kJ/mol = 5x10-4 /6x10-23 J/microtubule Force = work/distance = ~ 10-19/0.5x10-9 = ~2x10-10 N = ~200pN

Force can be estimated since we know the bending ridigity of the microtubule, and can thus estimate the force required to buckle it

Measured force ~5pN per microtubule (similar to the force exterted by a single motor molecule)

Not as efficient as a motor protein, but still substantial force on the molecular scale

Page 14: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Actin polymerization force pushes the front of motile cells forward

Page 15: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

How do cells control where and when cytoskeleton polymers accumulate?

Bacterium

Neutrophil

Chemotaxis

Phagocytosis

High density of actin filaments

Page 16: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Neutrophil chasing S aureus in a drop of bloodDavid Rogers 1950s

Page 17: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

How might cells control where and when cytoskeleton polymers accumulate?Neutrophil detects a bacterium

seconds

Signal (bacterial cell wall)

Receptor in plasma membrane

Signaling pathway

Cytoskeleton reorganization

Page 18: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

How might cells control where and when cytoskeleton polymers accumulate?Neutrophil detects a bacterium

seconds

Signal (bacterial cell wall)

Receptor in plasma membrane

Signaling pathway

Cytoskeleton reorganization

What kind of processes might work for this at the level of cytoskeleton filaments?

Page 19: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Many proteins binds to cytoskeleton filaments and control their behavior in cells

Bundling

Cross-linking

Capping

Gel-forming

Depolymerizing,Severing

Nucleating

Moving

Monomer binding, Monomer sequestering

Page 20: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Many proteins binds to cytoskeleton filaments and control their behavior in cells

Bundling

Cross-linking

Capping

Gel-forming

Depolymerizing,Severing

Nucleating

Moving

Monomer binding, Monomer sequestering

Page 21: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Nucleation is slow, elongation is fast

Nucleating a new filament is slow. Each incoming subunit makes only a subset of the favorable bonds

Elongating an existing filament is fast. Each incoming subunit makes all favorable bonds

The observation that elongating an existing filament is (much) faster than starting a new one is termed the kinetic barrier to nucleation.

The physical chemistry of polymer nucleation is similar to crystallization from a saturated solution or freezing of a supercooled liquid. In each case self-assembly can be nucleated by a pre-existing fragment of the polymer/crystal

Page 22: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Origin of the kinetic barrier to nucleation. 1) Condensation models (Oosawa-type models)

Break one bond. Fast

Break 2 bonds. Fast

Break 3 bonds. Slow

Diffusion controlled

Diffusion controlled

Diffusion controlled

Diffusion controlled

Break 3 bonds. Slow

“minimal seed”with n subunits

Page 23: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Origin of the kinetic barrier to nucleation. 1) Condensation models (Oosawa-type models)

- Requires multi-stranded polymer- Does not require conformational change of monomer (similar models work for crystallization)- Elongation rate is proportional to the concentration of the subunit.- Nucleation rate depends on concentration of subunit by a power law.

Break one bond. Fast

Break 2 bonds. Fast

Break 3 bonds. Slow

Diffusion controlled

Diffusion controlled

Diffusion controlled

Diffusion controlled

Break 3 bonds. Slow

“minimal seed”with n subunits

Page 24: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Origin of the kinetic barrier to nucleation. 1) Condensation models (Oosawa-type models)

Break one bond. Fast

Break 2 bonds. Fast

Break 3 bonds. Slow

Diffusion controlled

Diffusion controlled

Diffusion controlled

Diffusion controlled

“minimal seed”with n subunits

Break 3 bonds. Slow

Assume rapid equilibrium

Rate of formation of new filaments = concentration of ( n - 1)mers x rate that they turn into filaments

n-1 monomers ( n - 1)mer

Assume rapid equilibrium up until minimal seed. Then: [( n - 1)mer] ~ Kd[monomer]n-1;

nucleation rate ~ Kd[monomer]n-1 x k[monomer] ~ K’[monomer]n

N = 3-4 for actin Tobacman LS, Korn ED. J Biol Chem. 1983 258:3207-14.

Page 25: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Origin of the kinetic barrier to nucleation. 2) Conformational switch models

Non-polymerizing conformation (normal form of subunit after folding)

Polymerizing conformation (rare form of subunit)

Seed catalyzes conformational change

Slow, spontaneous conformational change + +

Page 26: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Origin of the kinetic barrier to nucleation. 2) Conformational switch models

- Does not requires multi-stranded polymer (in principle)- Requires conformational change of monomer that is catalyzed by polymer- Nucleation rate is independent of elongation rate and can be very slow.

Caspar DL, Namba K. (1990) Adv Biophys. 26:157-85; DePace et al 1998 Cell. 93:1241-52

More relevant to viral coat proteins and amyloid fibers

Non-polymerizing conformation (normal form of subunit after folding)

Polymerizing conformation (rare form of subunit)

Seed catalyzes conformational change

Slow, spontaneous conformational change + +

Page 27: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Nucleation factors in the cell

The kinetic barrier to nucleation prevents polymerization of cytoskeleton subunits at random in the cell. The cell controls where polymers form using nucleating factors.

Centrosome.Contains microtubule nucleating factor -tubulin ring complex

+

+

+

+

+

+ +

Page 28: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Nucleation factors in the cell

The kinetic barrier to nucleation prevents polymerization of cytoskeleton subunits at random in the cell. The cell controls where polymers form using nucleating factors.

Leading edge. Contains actin Nucleation + branching factor Arp2/3 complex

Centrosome.Contains microtubule nucleating factor -tubulin ring complex

+

+

+

+

+

+ +

These nucleating factors have the same fold as the filament subunit, suggesting a mechanism (templating) and an evolutionary origin. We now know other actin nucleating factors that are quite different in structure.

Page 29: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Evidence that centrosomes contain microtubule nucleating factors

(cells imaged by fixation and immunofluorescence)

Add nocodazole to depolymerize microtubules

Wash out drug

5 min

20 min

Brinkley BR.(1985). Annu Rev Cell Biol. 1:145-72.

Page 30: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Evidence that centrosomes contain microtubule nucleating factors

(cells imaged by fixation and immunofluorescence)

Add nocodazole to depolymerize microtubules

Wash out drug

5 min

20 min

Permeablize cells with non-ionic detergent

Add tubulin, GTP Incubate at 37o

Brinkley BR.(1985). Annu Rev Cell Biol. 1:145-72.

Page 31: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Microtubule Organizing Centers (MTOCs): Centrosomes, centrioles, basal bodies (animals) and spindle pole bodies

(fungi)

Centrosome = Centriole + Peri-centriolar material (PCM)

Centrioles

PCM (fibrous)

-tubulin ring complex(nucleates MTs)

Page 32: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Discovery of -tubulinAspergillus (a mycelium forming fungus)

-tubulin mutant

Select revertants

-tubulin, -tubulin double mutant

Defects in mitosis, nuclear transport

Oakley and Oakley 1989. Nature 338:662-4.

Page 33: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Discovery of -tubulinAspergillus (a mycelium forming fungus)

-tubulin mutant

Select revertants

-tubulin, -tubulin double mutant

-tubulin knockout: no microtubules

-tubulin localizes to spindle pole bodies by immunofluorescence

Defects in mitosis, nuclear transport

Oakley and Oakley 1989. Nature 338:662-4.

Page 34: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Centrosomes, centrioles, basal bodies and spindle pole bodies

Yeast spindle pole body forms on the nuclear envelope

Wigge et al 1998 J Cell Biol. 141:967-77

Centrosome = Centriole + Peri-centriolar material (PCM)

Animals Fungi

Page 35: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

-tubulin ring complex: the template model

Agard 2001 Curr Opin Struct Biol.11:174-81

Agard 2011 Nat Rev Cell Mol Biol.12:709

Note -tubulin has the same fold as tubulin, and the ring complex mimics a plus end

Page 36: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Actin nucleating complexes

Arp2/3 complexNucleates from the pointed (slow growing) endNucleates from the side of a pre-existing filamentGenerates brnached networksLammellipodia, Listeria comet tails, Endocytosis

ForminsNucleate from the barbed (fast growing) endRemain at the growing endGenerate long bundlesYeast actin cables, filopodia?

Formin dimer

Page 37: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

A pathogen provides a model for motility driven by actin polymerization

- Listeria monocytogenes is a gram positive bacterium that infects us from contaminated food- Enters the cytoplasm of many cell types by breaking out of phagosomes- Nucleates actin filaments and forms a comet tail that propels it through the cytoplasm and into neighboring cells- Other pathogens (Shigella, pox virus) also move using actin comet tails

“comet tail” of actin filaments Tilney and Portnoy (1989) J Cell Biol. 109:1597-608.

Page 38: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Listeria moving in cultured cell

Julie Theriot~1992Phase contrast

Page 39: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Listeria provides a system for dissecting the molecular mechanisms underlying leading edge motility

Identification of arp2/3 complex

Listeria moving in cell extract

fractionate cell extract by chromatography

Purify a protein complex that nucleates actin polymerization on the Listeria surface

Welch et al.(1997) Nature. 385:265-9

Page 40: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Listeria provides a system for dissecting the molecular mechanisms underlying leading edge motility

Identification of arp2/3 complex

Listeria moving in cell extract

fractionate cell extract by chromatography

Purify a protein complex that nucleates actin polymerization on the Listeria surface

Listeria movement was later reconstituted using 7 proteins:ActinArp2/3 complex (7 polypeptides)Profilin CofilinCapping proteinVASP+ActA on the bacterium surfaceLoisel et al.(1999). Nature. 401:613-6

Welch et al.(1997) Nature. 385:265-9

Page 41: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Arp2/3 structure

Arp2 and Arp3 subunits have the same fold as actin

Page 42: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Arp2/3 in action

Rhodamine actinTIRF microscopyPollard and Kovar

Page 43: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Arp2/3 mechanism

ActA, WASP etc.

To nucleate, Arp2/3 must:1)bind to the side of a pre-existing filament2)recruiting an activating protein. The activating protein brings in the first subunit of the new polymer

Arp2/3.

Page 44: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Arp2/3 mechanism

This mechanism generates dendritic actin assemblies, as seen in the leading edge of motile cells by EM

Pollard TD, Borisy GG. (2003) Cell. 112:453-65.

ActA, WASP etc.

To nucleate, Arp2/3 must:1)bind to the side of a pre-existing filament2)recruiting an activating protein. The activating protein brings in the first subunit of the new polymer

Arp2/3.

Page 45: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

How might cells control where and when cytoskeleton polymers accumulate?Neutrophil detects a bacterium

seconds

David Rogers 1950s

Page 46: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

Activating proteins make Arp2/3 activity dependent on multiple inputs

NWASP is activated by: Cdc42.GTPPhosphoinositol lipidsTyrosine phosphorylation

WAVE is activated by: Rac.GTPPhosphoinositol lipids

In both cases the WASP homolog acts as an AND gate for multiple biochemical signalsThese signals make Arp2/3 nucleation dependent on multiple signaling pathway inputs at the plasma membrane

Page 47: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

fMLP

GPCR G-protein coupled receptor

Different GPCRs for different signals

GDP

Heterotrimeric GTPase (inactive GDP bound state)

Leukocyte chemotactic signals are usually detected by GPCRs

GTP

G G

Signals to the actin cytoskeleton

Bacteria Human cells (eg leukocytes)

Leukotriene B4Chemokine – eg CCL2 etcEtc.

Page 48: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

fMLP

GDP

Chemotactic receptors send multiple signals to the actin cytoskeleton

GTP

G G

Actin polymerization at the leading edge

WAVEArp2/3

Myosin-II driven Contraction at the rear of the cell

Rac

Page 49: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

The actin cytoskeleton is polarized in motile cells

Actin Myosin-II in a fibroblast cell Actin RhoA in neutrophils

Page 50: CB201_12 Tim Mitchison Lecture 3 Force generation by polymerization dynamics Nucleation: controlling where and when polymers form

How does a neutrophil polarize?

How are the multiple signaling outputs from chemotactic receptors spatially organized to promote polarization?

Do different signals diffuse away from the receptor to different extents?

Does the front of the cell inhibit the back (or vice versa) – and if so by chemical signals, or physical signals such as membrane tension?

??