Title: The Conundrum of Biological Fusion
1Bridging Time and Length Scales in
Materials Science and Bio-Physics
Workshop I Multiscale Modelling in Soft Matter
and Bio-Physics
September 26-30, 2005
2The Enigma of Biological FusionA comparison of
two routes
- With
- Kirill Katsov (MRL, UC Santa Barbara)
- Marcus Mueller (Institute fur Theoretische
Physik, Gottingen)
3Why is Fusion Important?
Cell Trafficking Excocytosis/Endocytosis Viral
Entry
4Trafficking
5 Exocytosis
6Viral Entry
7Why is Fusion Difficult to Understand?
- Stability long-lived holes must be difficult to
form - Fusion long-lived holes must be easy to form
8The Biologists View of Fusion
9The Physicists View
Kozlov and Markin 1983
10SIMULATING FUSION
11Stalk Formation
12Stalk Formation and Expansion
13Stalks increase rate of hole formation
14Why does rate of hole formation go up?
Presumably, due to reduced line tension
15Why does rate of hole formation go up?
Presumably, due to reduced line tension
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18The intermediate in this second scenario
19 Hole Formation and Fusion are Correlated
20Consequence for Experiment Leakage
21An experiment to measure leakageV.A. Frolov et
al. 2003
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23Analytic 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
24Results for the Standard Mechanism
25Formation of fusion pore
26Two Consequences
1. Main Barrier in Old Mechanism is Expansion
272. Regime of Successful Fusion is Limited
28SCF Calculation of New Mechanism
Line tension of extended stalk favors small R and
a
29SCF Calculation (cont)
Reduced line tension of hole favors large
a Membrane tension favors large R
30IMI
Just before F1(R,a) aFIMI(R) FS
31IMI and its free eneregy
g/g00.0
g/g00.4
32IMI
Just before F1(R,a) aFIMI(R) FS
Just after F2(R,a) aFHI(R)
(1-a)FH(R-d)Fd
F1(R,a) F2(R,a) defines a ridge a(R)
33Free energy landscape in a and R
34Free energy barriers in new and old mechanism
new
old
barriers decrease with decreasing f and
increasing g
35Difference in free energy barriers of new and old
mechanism
36Prediction for a at barrier leakageCircumference
2pRa
37Resolving the enigma of fusion
- Membranes are stable because line tension of
holes is large
38Resolving the enigma of fusion
- Membranes are stable because line tension of
holes is large - But if hole forms next to stalk, line tension is
reduced
39Line tension of holes far from, and near to,
stalk
40Dependence of free energy on line tension
Energy of hole 2plHR-gpR2 Energy of critical
hole plH2/g Boltzmann factor PH (AH /s2) exp(-
plH2/gkT)
41- Boltzmann factor PH(AH/s2) exp(- plH2/gkT)
- EXPONENTIAL DEPENDENCE ON SQUARE OF
- LINE TENSION
- ENSURES STABILITY OF NORMAL MEMBRANES
42- Boltzmann factor PH(AH/s2) exp(- plH2/gkT)
- EXPONENTIAL DEPENDENCE ON SQUARE OF
- LINE TENSION
- ENSURES STABILITY OF NORMAL MEMBRANES
Example In simulation p lH2/gkT 8.76,
AH/s239 PH 6x10-3
43- Boltzmann factor PH(AH/s2) exp(- plH2/gkT)
- EXPONENTIAL DEPENDENCE ON SQUARE OF
- LINE TENSION
- ENSURES STABILITY OF NORMAL MEMBRANES
- ENABLES FUSION TO OCCUR BY REDUCING THAT LINE
TENSION
44Reducing the line tension from lH to ldr
alsh(1-a) lH
PH--gtPsh (Nsas/s2) exp(-pl2dr/gkT)
so Psh/PH (Nsas/AH)
exp(pl2H/gkT)(1-l2dr/l2bare)
(Nsas/AH) (AH/s2 PH)x
x (1-l2dr/l2bare) Stability implies
PHltlt1 Therefore rate of hole formation near stalk
Psh/PHgtgt1
45EXAMPLE IN SIMULATION
ldrlH/2, Nsas/AH0.3 Pdressed/Pbare 14
- P exp(-pl2/gkT)
- PH 6x10-3
46In Biological Membranes, Effect is Greater
lH2.6x10-6 erg/cm g 20 erg/cm2 PH1.7 x
10-11(AH/s2) very stable
47In Biological Membranes, Effect is Greater
lH2.6x10-6 erg/cm g 20 erg/cm2 PH1.7 x
10-11(AH/s2) very stable ldr/ lH 0.5,
Nsas/AH0.3 Psh/PH0.3(1/ 1.7 x 10-11)7/16
1x104 four orders of magnitude
48Conclusion The Enigmas Solution
- Because
- fusion is thermally excited and
- excitation energy proportional to l2
49Conclusion The Enigmas Solution
- Because
- fusion is thermally excited and
- excitation energy proportional to l2
Membranes can both be stable and undergo fusion
50Furthermore
Any process which affects the line tension
slightly affects the rate of fusion greatly
i.e. exquisite control
51To Do
- Effect of mixture of lipids
52To Do
- Effect of mixture of lipids
- Effect of different composition of leaves
53To Do
- Effect of mixture of lipids
- Effect of different composition of leaves
- Effect of fusion proteins
54Effect of Fusion Proteins?
55To Do
- Effect of mixture of lipids
- Effect of different composition of leaves
- Effect of fusion proteins
- Dynamics
56Thanks to
Misha Kozlov, Joshua Zimmerberg, Vadim Frolov,
Leonid Chernomordik, David Siegel, Barry Lentz,
Siewert Jan Marrink NATIONAL SCIENCE FOUNDATION
57AND