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Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

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Page 1: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Bridging Time and Length Scales in MaterialsScience and Bio-Physics

Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics

September 26-30, 2005

Page 2: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

The Enigma of Biological Fusion

A comparison of two routes

With

Kirill Katsov (MRL, UC Santa Barbara)

Marcus Mueller (Institute fur Theoretische Physik, Gottingen)

Page 3: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Why is Fusion Important?

Cell Trafficking

Excocytosis/Endocytosis

Viral Entry

Page 4: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Trafficking

Page 5: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Exocytosis

Page 6: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Viral Entry

Page 7: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

1. Stability: long-lived holes must be difficult to form

2. Fusion: long-lived holes must be easy to form

Why is Fusion Difficult to Understand?

Page 8: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

The Biologist’s View of Fusion

Page 9: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

The Physicist’s View

Kozlov and Markin 1983

Page 10: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

SIMULATING FUSION

Page 11: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Stalk Formation

Page 12: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Stalk Formation and Expansion

Page 13: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Stalks increase rate of hole formation

Page 14: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Why does rate of hole formation go up?

Presumably, due to reduced line tension

Page 15: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Why does rate of hole formation go up?

Presumably, due to reduced line tension

Page 16: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005
Page 17: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005
Page 18: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

The intermediate in this second scenario

Page 19: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Hole Formation and Fusion are Correlated

Page 20: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Consequence for Experiment: Leakage

Page 21: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

An experiment to measure leakageV.A. Frolov et al. 2003

Page 22: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005
Page 23: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Analytic Approach to FusionSelf-Consistent Field Theory

• Investigate many possible configurations• Calculate free energy barriers of each• Change architecture easily• Analogous to Hartree Theory• Highly Non-Linear Set of Equations

Page 24: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Results for the Standard Mechanism

Page 25: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Formation of fusion pore

Page 26: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

1. Main Barrier in Old Mechanism is Expansion

Two Consequences

Page 27: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

2. Regime of Successful Fusion is Limited

Page 28: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

SCF Calculation of New Mechanism

Line tension of extended stalk favors small R and

Page 29: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

SCF Calculation (cont)

Reduced line tension of hole favors large Membrane tension favors large R

Page 30: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Just before F1(R,) = FIMI(R) +FS

Page 31: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

IMI and its free eneregy

Page 32: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Just before F1(R,) = FIMI(R) +FS

Just after F2(R,) = FHI(R) +(1-FH(R-)+Fd

F1(R,) = F2(R,) defines a ridge (R)

Page 33: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Free energy landscape in and R

Page 34: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Free energy barriers in new and old mechanism

new old

barriers decrease with decreasing f and increasing

Page 35: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Difference in free energy barriers of new and old mechanism

Page 36: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Prediction for at barrier: leakageCircumference =2R

Page 37: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Resolving the enigma of fusion1. Membranes are stable because line tension of holes is large

Page 38: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Resolving the enigma of fusion1. Membranes are stable because line tension of holes is large

2. But if hole forms next to stalk, line tension is reduced

Page 39: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Line tension of holes far from, and near to, stalk

Page 40: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Dependence of free energy on line tension

Energy of hole 2R-R2

Energy of critical hole

Boltzmann factorPH= (AH /s2) exp(-

kT)

Page 41: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Boltzmann factor PH=(AH/s2) exp(- kT)

EXPONENTIAL DEPENDENCE ON SQUARE OF

LINE TENSION:

1. ENSURES STABILITY OF NORMAL MEMBRANES

Page 42: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Boltzmann factor PH=(AH/s2) exp(- kT)

EXPONENTIAL DEPENDENCE ON SQUARE OF

LINE TENSION:

1. ENSURES STABILITY OF NORMAL MEMBRANES

Example: In simulation

H2/kT = 8.76, AH/s2=39

PH~ 6x10-3

Page 43: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Boltzmann factor PH=(AH/s2) exp(- kT)

EXPONENTIAL DEPENDENCE ON SQUARE OF

LINE TENSION:

1. ENSURES STABILITY OF NORMAL MEMBRANES

2. ENABLES FUSION TO OCCUR BY REDUCING THAT LINE TENSION

Page 44: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Reducing the line tension from H to dr = sh+(1-H

PH-->Psh = (Nsas/s2) exp(-dr/kT)

so

Psh/PH = (Nsas/AH) exp(H/kT)(1-

dr/bare)

= (Nsas/AH) (AH/s2 PH)x

x= (1-dr/

bare)

Stability implies PH<<1

Therefore rate of hole formation near stalk

Psh/PH>>1

Page 45: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

P~ exp(-kT)

PH~ 6x10-3

dr=H/2, Nsas/AH~0.3 Pdressed/Pbare~ 14

EXAMPLE: IN SIMULATION

Page 46: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

In Biological Membranes, Effect is GreaterH~2.6x10-6 erg/cm

20 erg/cm2

PH~1.7 x 10-11(AH/s2) very stable

Page 47: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

In Biological Membranes, Effect is GreaterH~2.6x10-6 erg/cm

20 erg/cm2

PH~1.7 x 10-11(AH/s2) very stable

dr/ H= 0.5, Nsas/AH~0.3

Psh/PH=0.3(1/ 1.7 x 10-11)7/16

~1x104

four orders of magnitude

Page 48: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Conclusion: The Enigma’s Solution

Because

1. fusion is thermally excited and

2. excitation energy proportional to

Page 49: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Conclusion: The Enigma’s Solution

Because

1. fusion is thermally excited and

2. excitation energy proportional to

Membranes can both be stable and undergo fusion

Page 50: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Furthermore

Any process which affects the line tension slightly affects the rate of fusion greatly

i.e. exquisite control

Page 51: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

To Do

1. Effect of mixture of lipids

Page 52: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

To Do

1. Effect of mixture of lipids

2. Effect of different composition of leaves

Page 53: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

To Do

1. Effect of mixture of lipids

2. Effect of different composition of leaves

3. Effect of fusion proteins

Page 54: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Effect of Fusion Proteins?

Page 55: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

To Do

1. Effect of mixture of lipids

2. Effect of different composition of leaves

3. Effect of fusion proteins

4. Dynamics

Page 56: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

Thanks to

isha Kozlov, Joshua Zimmerberg,

Vadim Frolov, Leonid Chernomordik, David Siegel, Barry Lentz, Siewert Jan Marrink

ATIONAL SCIENCE FOUNDATION

Page 57: Bridging Time and Length Scales in Materials Science and Bio-Physics Workshop I: Multiscale Modelling in Soft Matter and Bio-Physics September 26-30, 2005

AND