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The Conundrum of Biological Fusion

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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 ... – PowerPoint PPT presentation

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Title: The Conundrum of Biological Fusion


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
2
The Enigma of Biological FusionA comparison of
two routes
  • With
  • Kirill Katsov (MRL, UC Santa Barbara)
  • Marcus Mueller (Institute fur Theoretische
    Physik, Gottingen)

3
Why is Fusion Important?

Cell Trafficking Excocytosis/Endocytosis Viral
Entry
4
Trafficking
5
Exocytosis
6
Viral Entry
7
Why is Fusion Difficult to Understand?
  • Stability long-lived holes must be difficult to
    form
  • Fusion long-lived holes must be easy to form

8
The Biologists View of Fusion
9
The Physicists View
Kozlov and Markin 1983
10
SIMULATING FUSION
11
Stalk Formation
12
Stalk Formation and Expansion

13
Stalks increase rate of hole formation
14
Why does rate of hole formation go up?
Presumably, due to reduced line tension
15
Why does rate of hole formation go up?
Presumably, due to reduced line tension
16
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17
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18
The intermediate in this second scenario
19

Hole Formation and Fusion are Correlated
20
Consequence for Experiment Leakage
21
An experiment to measure leakageV.A. Frolov et
al. 2003
22
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23
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

24
Results for the Standard Mechanism

25
Formation of fusion pore
26
Two Consequences
1. Main Barrier in Old Mechanism is Expansion
27
2. Regime of Successful Fusion is Limited
28
SCF Calculation of New Mechanism
Line tension of extended stalk favors small R and
a
29
SCF Calculation (cont)
Reduced line tension of hole favors large
a Membrane tension favors large R
30
IMI
Just before F1(R,a) aFIMI(R) FS
31
IMI and its free eneregy
g/g00.0
g/g00.4
32
IMI
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)
33
Free energy landscape in a and R
34
Free energy barriers in new and old mechanism
new
old
barriers decrease with decreasing f and
increasing g
35
Difference in free energy barriers of new and old
mechanism
36
Prediction for a at barrier leakageCircumference
2pRa

37
Resolving the enigma of fusion
  • Membranes are stable because line tension of
    holes is large

38
Resolving 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

39
Line tension of holes far from, and near to,
stalk
40
Dependence 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

44
Reducing 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
45
EXAMPLE IN SIMULATION
ldrlH/2, Nsas/AH0.3 Pdressed/Pbare 14
  • P exp(-pl2/gkT)
  • PH 6x10-3

46
In Biological Membranes, Effect is Greater
lH2.6x10-6 erg/cm g 20 erg/cm2 PH1.7 x
10-11(AH/s2) very stable
47
In 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
48
Conclusion The Enigmas Solution
  • Because
  • fusion is thermally excited and
  • excitation energy proportional to l2

49
Conclusion The Enigmas Solution
  • Because
  • fusion is thermally excited and
  • excitation energy proportional to l2

Membranes can both be stable and undergo fusion
50
Furthermore
Any process which affects the line tension
slightly affects the rate of fusion greatly
i.e. exquisite control
51
To Do
  • Effect of mixture of lipids

52
To Do
  • Effect of mixture of lipids
  • Effect of different composition of leaves

53
To Do
  • Effect of mixture of lipids
  • Effect of different composition of leaves
  • Effect of fusion proteins

54
Effect of Fusion Proteins?
55
To Do
  • Effect of mixture of lipids
  • Effect of different composition of leaves
  • Effect of fusion proteins
  • Dynamics

56
Thanks to
Misha Kozlov, Joshua Zimmerberg, Vadim Frolov,
Leonid Chernomordik, David Siegel, Barry Lentz,
Siewert Jan Marrink NATIONAL SCIENCE FOUNDATION
57
AND
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