Origin of the surprising mechanical stability of kinesin’s neck coiled coil
description
Transcript of Origin of the surprising mechanical stability of kinesin’s neck coiled coil
Origin of the surprising mechanical stability of kinesin’s neck coiled coil
JI Qing
河北工业大学 生物物理研究所
June 2014, Beijing
Institute of Biophysics
Hebei University of Technology
1. Macromolecular dynamics: structure, function and life
R.Vale & R.Milligan, Science, 2000.
ATP hydrolysis:
55 /G kJ mol
5 8
24 /
W pN nm
kJ mol
Work in one step:
molecular motor
ATPase
Kinesin
One motor head:350 amino acids
Driving motility in life.
Tight coupling
2. Neck coiled coil: FunctionKinesin’s mechanochemical cycling needs exquisite inter-head communication and cooperation and gating between the mechanical steps and chemical steps.
Inter-head tension is crucial.
8 nm
Neck linker (4 nm)
The neck coiled coil should keep zippered under inter-head tension.
High efficiency — Tight coupling — No futile hydrolysis.
Experimantal facts: (1) Tomishige & Vale (JCB, 2000)Cross-linking coiled coil had relatively little effect on motor activity.
(3) Bornschlögl, Woehlke and Rief (PNAS, 2009)
The unconventional N-terminal parts of the neck coiled coil exhibit a surprising mechanical stability.The opening of only 2 N-terminal coiled-coil turns will destabilize the complete neck and lead to unfolding.
Substitution of Trp 340, the first hydrophobic core d position residue of the coiled-coil, with an Ala residue resulted in a greater than expected decrease in stability and helicity of the coiled-coil structure.
(2) Tripet and Hodges (JSB, 2002)
3. Neck coiled coil: Structure
Heptad :
The first two turns
The first heptad
abcdefg
A E E W K K K Y E K E K E K ----- W339 346 370
a b c d e f g a b c d e f g d
The neck domain (residues 339–370, 2KIN)
A B
A
B
Structure of conventional coiled coilCohen and Parry (Proteins, 1990)
The key features of coiled coil are as follows:
Fig. 2
Fig. 1
Thormählen, Marx, Sack, and Mandelkow (JSC,1998)Fig. 3
The sequence of neck coiled coil
4. Neck coiled coil: Structure-function relationship
0 5000 10000 15000 20000 25000 30000 350000
2
4
6
8
10
12
14
16
18
20
Dis
tanc
e (Å
)
Time (ps)
ALA339:CA-ALA114:CA TRP342:CA-TRP117:CA TYR346:CA-TYR121:CA
50pN
0 5000 10000 15000 20000 25000 30000 350000
2
4
6
8
10
12
14
16
18
20
Dis
tanc
e (Å
)
Time (ps)
ALA339:CA-ALA114:CA TRP342:CA-TRP117:CA TYR346:CA-TYR121:CA
150pN
0 5000 10000 15000 20000 25000 30000 350000
2
4
6
8
10
12
14
16
18
20
Dis
tanc
e (Å
)
Time (ps)
ALA339:CA-ALA114:CA TRP342:CA-TRP117:CA TYR346:CA-TRY121:CA
100pN
0 1000 2000 3000 4000 5000 6000 70000
5
10
15
20
25
30
35
40
45
50
55
Dis
tanc
e (Å
)
Time (ps)
ALA339:CA-ALA114:CA TRP342:CA-TRP117:CA TYR346:CA-TYR121:CA
170pN
4.1 Mechanical response to stretching forces
50 pN:
150 pN:
Partially open and then stable
Stable
100 pN:
Partially open and then stable
170 pN:
Totally open
4.2 Details of the opening process
第一个台阶: Fig. 3
4 ns 5.5 ns 7.5 ns
0 1000 2000 3000 4000 5000 6000 7000 8000 9000100002
4
6
8
10
12
14
16
d 339-3
39 (Å)
Time (ps)
100pN
4 ns
5.5 ns
7.5 nsThe first platform:
Backbone hydrogen bonds breaking
The second platform:
Peptide planes rotation
The unzippering process is stopped at Y346.
Y346
Y346
4.3 Tyrosine buckle and its mechanical function
The buckle structure
O’Shea et al. (Science,1991)
Fig 7. Schematic drawing (not to scale) showing differences betweenpositions a and d.
vdW Radii
H 1.2 Å
O 1.52 Å
N 1.55 Å
C 1.7 Å
Bondi (JPC,1964)
aa’
d’d
4.4 The buckle mechanics
In equilibrium:
0 c sF F
0c x F N
(A + B)
(A)
? 0y N
Constraint force Stretching force
Contact force
Ny is balanced by the special hydrophobic pressure.
A E E W K K K Y E K E K E K 339 342 346
a b c d e f g a b c d e f g
The first two heptads in the neck domain
Lyotropic liquid crystal
N
N’
Nx
Ny
N’x
N’y
Nx = Fc = Fs
y
x
N
N
y x sN N F N’y = N’x = F’s
Micelle
Hydrophobic pressure
phph Forces in equilibrium
0y N P
For (A), define
hdP p
In equilibrium:
P must have an upper limit and so does Fs.
Conclusion
The surprising mechanical stability of the neck coiled coil arises from the cooperation between the special hydrophobic pressure and the steric hindrance of the tyrosine buckle.
5. Special hydrophobic pressure?
The average distance between the Cs of the two Y346s is 4.678Å (the shortest).
0 2000 4000 6000 8000 100003
4
5
6
7
8
9
10
11
12
13
14
15
Dis
tanc
e (Å
)
Time (ps)
ALA339:CA-ALA114:CA TRP342:CA-TRP117:CA TYR346:CA-TYR121:CA GLU349:CA-GLU124:CA ASN353:CA-ASN128:CA LEU356:CA-LEU131:CA ILE360:CA-ILE135:CA
100pN
Average
The mechanical function of the Y-buckle is sensitive to the C-C distance.
'y yN N
'x xN N
The special arrangement of the neck residues results in the special hydrophobic pressure.
0 2000 4000 6000 8000 10000 12000 140000
2
4
6
8
10
12
14
16
r 3 (Å)
Time (ps)
TRP342:CE2-LYS118:HD1100 pN
r3 3.777 Å
0 2000 4000 6000 8000 10000 12000 14000
4
6
8
10
12
14
16
Dis
tance
(Å)
Time (ps)
LYS348:NZ-LYS345:NZ LYS344:NZ-LYS348:NZ LYS343:NZ-LYS344:NZ
100 pN
l1 (blue) 10.382 Å
l2 (red) 11.264 Å
l3 (black) 10.379 Å
Average
Average
A E E W K K K Y E K E K E K 339 342 346
a b c d e f g a b c d e f g
(1) W342(A) vs K343(B)
(2) KKK
(3) ……
Conclusion
Each detail has a reason.
My students in this work
Acknowledgement
刘书霞 (Shu-Xia Liu)
吕 刚 (Gang Lü)
柳睿殊 (Rui-Shu Liu)
耿轶钊 (Yi-Zhao Geng)
张 辉 (Hui Zhang)
The National Natural Science Foundation of China , No. 90403007
The National Natural Science Foundation of China , No. 10975044
卓益忠( Yin-Zhong Zhuo)
包景东( Jing-Dong Bao)
张红雨( Hong-Yu Zhang)
郝柏林( Bo-Lin Hao)
欧阳钟灿( Zhong-Can Ouyang)
陈润生( Run-Sheng Chen)