results from a field-theoretic approach to membrane fusion

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Results from a field- theoretic approach to membrane fusion Michael Schick Department of Physics University of Washington

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Results from a field-theoretic approach to membrane fusion. Michael Schick Department of Physics University of Washington. à mon cher maître. à mon cher maître. à mon cher maître. Maurice Ravel. Synaptic Vesicles. They are small R~15-25 nm cf bilayer thickness t~4nm - PowerPoint PPT Presentation

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Page 1: Results from a field-theoretic approach to membrane fusion

Results from a field-theoreticapproach to membrane fusion

Michael Schick

Department of Physics

University of Washington

Page 2: Results from a field-theoretic approach to membrane fusion

à mon cher maître

Page 3: Results from a field-theoretic approach to membrane fusion

à mon cher maître

Page 4: Results from a field-theoretic approach to membrane fusion

à mon cher maître

Maurice Ravel

Page 5: Results from a field-theoretic approach to membrane fusion
Page 6: Results from a field-theoretic approach to membrane fusion

Synaptic Vesicles

They are small R~15-25 nm

cf bilayer thickness t~4nm

They dock: nothing happens

They are triggered: fuse rapidly

Fusion on demand

Page 7: Results from a field-theoretic approach to membrane fusion

Synaptic vesicles in C. Elegans

J.L. Bessereau: www.biologie.ens.fr

Page 8: Results from a field-theoretic approach to membrane fusion

Questions

• Why does fusion occur and how?

• What are free energy barriers to fusion?

• What factors promote fusion?

Page 9: Results from a field-theoretic approach to membrane fusion

Theoretical Procedure

Consider fusion of vesicles of block copolymer: universality

Page 10: Results from a field-theoretic approach to membrane fusion

Theoretical Procedure

Consider fusion of vesicles of block copolymer: universality

Polymers->Random walk->Diffusion Eq.-> Quantum Mech.

Page 11: Results from a field-theoretic approach to membrane fusion

Theoretical Procedure

Consider fusion of vesicles of block copolymer: universality

Polymers->Random walk->Diffusion Eq.-> Quantum Mech.

SCFT of interacting polymers-> Hartree Theory

Advantages: microscopic model->architecture

calculation of free energies

Page 12: Results from a field-theoretic approach to membrane fusion

Bringing bilayers together removes water->

free energy per area increases-> bilayers are under tension

WHY DOES FUSION OCCUR?

Page 13: Results from a field-theoretic approach to membrane fusion

Bringing bilayers together removes water->

free energy per area increases-> bilayers are under tension

Fusion eliminates area -> reduces the free energy

Fusion is one possible response to induced tension

Lysis (rupture) is another

WHY DOES FUSION OCCUR?

Page 14: Results from a field-theoretic approach to membrane fusion

HOW DOES FUSION OCCUR?

one commonly accepted mechanism

Page 15: Results from a field-theoretic approach to membrane fusion

Kozlov and Markin 1983

Profiles obtained by the theory

Page 16: Results from a field-theoretic approach to membrane fusion

WHAT ARE THE FREE ENERGY BARRIERS TO FUSION?

Page 17: Results from a field-theoretic approach to membrane fusion

WHAT ARE THE FREE ENERGY BARRIERS TO FUSION?

Consider the fusion of two bilayers

One component only

A lamellar former

Page 18: Results from a field-theoretic approach to membrane fusion

Kozlov and Markin 1983

Profiles obtained by the theory

Page 19: Results from a field-theoretic approach to membrane fusion

One component, f = 0.4 (DOPC), /0 = 0.2, equilibrium H, stalk

1 bilayer =4.3 Rg

Page 20: Results from a field-theoretic approach to membrane fusion

One component, f = 0.4, /0 = 0.2, equilibrium H, stalk

Page 21: Results from a field-theoretic approach to membrane fusion

One component, f = 0.4, /0 = 0.2, equilibrium H, stalk

Page 22: Results from a field-theoretic approach to membrane fusion

One component, f = 0.4, /0 = 0.2, equilibrium H, stalk

Page 23: Results from a field-theoretic approach to membrane fusion

One component, f = 0.4, /0 = 0.2, equilibrium H, pore

Page 24: Results from a field-theoretic approach to membrane fusion

One component, f = 0.4, /0 = 0.2, equilibrium H, stalk & pore

Page 25: Results from a field-theoretic approach to membrane fusion

One component, f = 0.4, /0 = 0.2, equilibrium H, stalk & pore

In lipids, barrier would be 50 kT !

Page 26: Results from a field-theoretic approach to membrane fusion

WHAT FACTORS AFFECT FUSION?

Page 27: Results from a field-theoretic approach to membrane fusion

Effect of Tension

Page 28: Results from a field-theoretic approach to membrane fusion

Effect of Two Components and Asymmetry in Leaves

SMALL HEADS, LARGE TAILS FAVORED HERE IN PROXIMAL LEAF

Page 29: Results from a field-theoretic approach to membrane fusion

Effect of Two Components and Asymmetry in Leaves

Average concentration of hex-former is 0.35

0.35 in cis

0.40 in cis

0.43 in cis

F/kbT

f=0.4 (DOPC) and f=0.294 (DOPE)

Page 30: Results from a field-theoretic approach to membrane fusion

Effect of Two Components and Asymmetry in Leaves

Average concentration of hex-former is 0.35

0.35 in cis

0.40 in cis

0.43 in cis

F/kbT

Note that stalk becomes metastable. Its formation is now largest barrier

Page 31: Results from a field-theoretic approach to membrane fusion

Effect of curvatureFusion of Bilayer and Vesicle:

1 bilayer =4.3 Rg60:40 mixture J Y Lee & M.S. BJ 2008

Page 32: Results from a field-theoretic approach to membrane fusion

What should we expect the effect of curvature to be?

Page 33: Results from a field-theoretic approach to membrane fusion

As vesicle radius decreases, effective tension increases, which decreases barrier

Page 34: Results from a field-theoretic approach to membrane fusion

Fusion of two identical vesicles

60:40 mixture

Page 35: Results from a field-theoretic approach to membrane fusion

H = 2.2 R_g, zero tension, 60:40 mixture

Control Fusion by Controlling the Interbilayer Spacing

Page 36: Results from a field-theoretic approach to membrane fusion

H = 2.2, 2.7 R_g, zero tension

Page 37: Results from a field-theoretic approach to membrane fusion

H = 2.2, 2.7, 3.2 R_g, zero tension

Page 38: Results from a field-theoretic approach to membrane fusion

H = 2.2, 2.7, 3.2, 3.7 R_g, zero tension

Page 39: Results from a field-theoretic approach to membrane fusion

H = 2.2, 2.7, 3.2, 3.7, 4.0 R_g, zero tension

Page 40: Results from a field-theoretic approach to membrane fusion

Conclusions• Two barriers to fusion

Page 41: Results from a field-theoretic approach to membrane fusion

Conclusions• Two barriers to fusion• Barrier to stalk formation linear in distance

->easy to prevent fusion

Page 42: Results from a field-theoretic approach to membrane fusion

Conclusions• Two barriers to fusion• Barrier to stalk formation linear in distance

->easy to prevent fusion• Second barrier reduced by composition and

curvature

Page 43: Results from a field-theoretic approach to membrane fusion

Conclusions• Two barriers to fusion• Barrier to stalk formation linear in distance

->easy to prevent fusion• Second barrier reduced by composition and

curvature• Consequently, when brought close, stalk

barrier is small, ~13kT, and fusion is quick• Fusion on demand!

Page 44: Results from a field-theoretic approach to membrane fusion

Acknowledgements

Marcus MuellerKirill KatsovJae-Youn Lee

NSF Grant DMR 0503752