31
Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Embed Size (px)

Citation preview

Page 1: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Detecting small charge movements in biological

membrane systems

Benoit RouxUniversity of Chicago

March 2015

Page 2: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Sliding helix

Paddle

Transporter-like

Large movement

Small movement

Long, Campbell & Mackinnon. Crystal structure of a mammalian voltage-dependent Shaker family K+ channel.Science. 309(5736):897-903, 2005.

?

Page 3: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Voltage Gating 101…

OC

side II

side I

Vmp

++

+ ---

side II

side I

Vmp

++

+

---

Page 4: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

F. Khalili, V. Jogini, V. Yarov, E. Tajkhorshid, B. Roux, K. Schulten

MD of Full-length Kv1.2 in bilayer in open and closed state

Open Closed

Page 5: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

V=0

V

+

Page 6: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Define the excess free energy (or PMF) for the system at X arising from the applied membrane voltage V and averaged over all solvent degrees of freedom Y

Page 7: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

The constant field in PBC

Displacement charge

There are 3 routes that can be exploited:

• “W” PMF with & without voltage

• “Qd” Average displacement charge (with or without voltage)

• “G” Free energy of charging with & without voltage

Page 8: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Application of the Q-route to the VSD of Kv1.2

Correlation time is about 10 ns

RMS fluctuations are related to capacitance

Page 9: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Application of the Q-route to the VSD of Kv1.2

F. Khalili, V. Jogini, E. Tajkhorshid, K. Schulten, B. Roux

VSD

Page 10: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Application of the Q-route to the Kv1.2 channel

Khalili-Araghi et al. Calculation of the gating charge for the Kv1.2 voltage-activated potassium channel. Biophys J. 98(10):2189-98, 2010.

Page 11: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Application of the G-route to the Kv1.2 channel

Khalili-Araghi et al. Calculation of the gating charge for the Kv1.2 voltage-activated potassium channel. Biophys J. 98(10):2189-98, 2010.

Page 12: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015
Page 13: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Na+/K+-pump overview

K+

K+

Na+

Na+

ADP + Pi

ATP

Extracellularmatrix

Cytoplasm

• Membrane transporter

• P-type ATPase

• Actively export 3Na+ and import 2K+ per pump cycle.

• Maintain healthy ion concentration gradients across cell membrane.

• Indispensible for excitable cells such as neurons.

Skou, J. C., Biochim. Biophys. Acta. (1957) 23:394

Page 14: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

ForwardPump cycle

E1

E2

Na+/K+-pump overview

Extracellularmatrix

Cytoplasm

• “Alternating-access” pump cycle

Post, R. L. et al, J. Gen. Physiol. (1969) 54:306Gadsby, D. C. et al, Nat. Commun. (2012) 3:669

Page 15: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

ForwardPump cycle

Na+/K+-pump overview• Crystal structures available

PDBID: 2ZXE2.4 Å

PDBID: 3WGV2.8 Å

Shinoda, T. et al, Nature (2009) 459:446Kanai, R. et al, Nature (2013) 502:201

Page 16: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Na+/K+-pump overview

Extracellular matrix

Cytoplasm

β

α

β

α

A P

N

A P

N

PDBID: 3WGVNa3

.E1.(ADP.Pi)

PDBID: 2ZXEE2(K2)

• Crystal structures available

Page 17: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

ForwardPump cycle

??

Extracellular ion binding• Limited structural information on the P-E2 state

Page 18: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

(Ca2) E1~P:ADP

Ca2 E2P:ATP

Ca2 E1:ATP

E2P

Hn E2P:ATP

(Hn) E2 ~P:ATP

Hn E2:ATP

• Modeling the P-E2 state based on Ca2+ SERCA pump

PDBID1VFP

PDBID1WPG

PDBID3B9B

Ca2+ SERCAPump cycle

Extracellular ion binding

Page 19: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Ca2 E1:ATP

E2P

(Hn) E2 ~P:ATP

• Modeling the P-E2 state based on Ca2+ SERCA pump

PDBID1VFP

PDBID1WPG

PDBID3B9B

Ca2+ SERCAPump cycle

Extracellular ion binding

Page 20: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

• Models for outward facing, ion loaded Na+/K+ pump

P-E2.Na3 P-E2.K2

Extracellularmatrix

Cytoplasm

Extracellular ion binding

Water filled pathway leading to the binding site

Page 21: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

• Simultaneous rebinding of ions from the extracellular side

Extracellular ion binding

Na+ rebinding happens at 30-ns time mark in a 120-ns MD simulation.

Page 22: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Gating charge upon ion binding

Instantaneous displacement charge:

Average displacement charge of a trajectory:

Gating charge:

• Estimating gating charge (ΔQD) from MD trajectories

A 82 Å

B 107 Å

C 155 Å

nAtom ~150K

nPOPC 213

nWater 32K

System information

Page 23: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015
Page 24: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Gating charge upon ion binding

Triple occupancy Double occupancy Single occupancy Empty sites

• MD systems involved in Na+ release

1/3

1/3

1/3

1/3

1/3

1/3

1 1

Page 25: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Gating charge upon ion binding

Empty sites Single occupancy Double occupancy

• MD systems involved in K+ binding

1/2

1/2

11

Page 26: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Na+ release from P-E2.Na3 K+ binding in P-E2.K2

Calc. 0.56 ± 0.10 0.39 ± 0.07 0.01 ± 0.1 0.49 ± 0.12 0.37 ± 0.20

Exp. 0.61-0.71* ~0.3* 0.46** 0.27**

• Models for outward facing, ion loaded Na+/K+ pumpModelP-E2.Na3

ModelP-E2.K2

Table. Gating charge of ion binding/release from P-E2.

Gating charge upon ion binding

* Holmgren, M. et al, Nature (2000) 403:898**Castillo, J. P. et al, Nat. Commun. (under review)

Page 27: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

• Titratable residues at crystal structure ion binding sites

αM4αM5

αM8αM6

αM9

αM4αM5

αM8αM6

αM9

IIIIII

III

PDBID: 3WGVNa3

.E1.(ADP.Pi)

PDBID: 2ZXEE2(K2)

RMSDsiteHA = 3.0 Å

Ion binding site protonation state

Page 28: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

exp −ΔGab kT[ ] = dX exp[−Ub /kT]∫dX exp[−Ua /kT]∫

= dX exp[− Ub −Ua( ) /kT] exp[−Ua /kT]∫

dX exp[−Ua /kT]∫

= exp[− Ub −Ua( ) /kT](a)

Gb - Ga = − kT ln exp[− Ub −Ua( ) /kT](a)

⎛ ⎝ ⎜

⎞ ⎠ ⎟

Free Energy Perturbation

Page 29: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Difference in Hydration Free Energy

GNa −GK = - kT ln exp[−UNa −UK( ) / kT ](K)

⎛ ⎝ ⎜

⎞ ⎠ ⎟

-17.2 kcal/mol

K+ Na+

FEP/MD simulations

Page 30: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Selectivity of the Na+/K+ Pump in state E2P

System Setup Site I Site II

2ZXE: 334,786,811,815 -2.5 -2.7

3B8E: 327,779,804,808 -1.7 -4.5

The sites are selective for Na+ over K+ ?????!!!!!!!

Yu H, Ratheal IM, Artigas P, Roux B. Protonation of key acidic residues is critical for the K⁺-selectivity of the Na/K pump. Nat Struct Mol Biol. 18(10):1159-63, 2011.

Page 31: Detecting small charge movements in biological membrane systems Benoit Roux University of Chicago March 2015

Selectivity of the Na+/K+ Pump in the state E2P

System Setup Site I Site II

2ZXE: 334+,786+,811,815+ +4.0 +4.6

3B8E: 327+,779+,804,808+ +3.0 +1.7

2ZXE: 334+,786+,811,815 -0.4 +3.5

2ZXE: 334,786+,811,815+ -0.8 -7.7

2ZXE: 334,786,811,815 -2.5 -2.7

3B8E: 327,779,804,808 -1.7 -4.5

Na+/K+ pump can modulate the local electrostatic environmentof the binding sites to shift the pKa values of the residuesso that it can achieve K+ selectivity at the E2P state.