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MD-PNP simulations of Alpha-Hemolysin open channel ion currents

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MD-PNP simulations of Alpha-Hemolysin open channel ion currents. Ioana Cozmuta**, J. T. O’Keeffe*, D. Bose** and V. Stolc* *NASA Ames Research Center, **Eloret Corp. The alpha hemolysin ion channel. ‘Natural’ function *. Alpha hemolysin is a toxin produced by Staphylococcus aureus bacteria - PowerPoint PPT Presentation

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Page 1: MD-PNP simulations of Alpha-Hemolysin open channel ion currents
Page 2: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

The alpha hemolysin ion channel

Page 3: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

‘Natural’ function*

Alpha hemolysin is a toxin produced by Staphylococcus aureus bacteria

It spontaneously self-assembles into a water soluble ionic channel with a molecular weight of 33.2 k-Dalton and a length of ~ 10nm

The channel contains 2051 AA residues organized in 7 sequence-identical chains (symmetry group C121)

The channel is strongly surface active and it inserts into pre-formed lipid membranes, damaging the membrane properties

Extra cellular Ca2+ or other divalent cations prevent cell damage by closing the channel

* Menestrina, G, The Journal of Membrane Biology, 90, 177-190, 1986

Page 4: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Experiments

Over-linear

Conductance*

* Biophysical Journal, 79, 4, 1967-1975, 2001

measured in voltage-clamp experiments

Asymmetric I-V characteristic: over linear increase in the first quadrant and sub linear in the third.

Linear relationship between the channel conductance and the conductivity (molarity) of the electrolyte solution at a constant clamp voltage.

The channel is slightly anion- selective at pH 7.0

Page 5: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

polymer speed inhibition

poly [rU] ~1 s/nucl 85-100%

poly [rA] ~20 s/nucl 85%

poly [rC] ~3 s/nucl 95%ELECTRIC FIELD- +

CIS TRANS

A bio-engineering application Alpha hemolysin channel in 1.0 M KCl

solution with an external applied voltage of 125 mV leads to an ionic current of 120 pA (channel conductance ~1nS)

ss-DNA or RNA molecules driven by an electric field through the ion channel generate a transient decrease of ionic current

Page 6: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

An atomistic view of the channel

Page 7: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

*Song, L., Hobaugh, M. R., Shustak, C., Cheley, S., Bayley, H., Gouaux, J. E., Structure of staphylococcal alpha-hemolysin, a heptameric transmembrane pore, Science 274 pp. 1859 (1996)

**Force field: Cornell et al, 1995 –AMBER, http://www.scripps.edu/

Coordinate MIN MAX Length

X -5.13 103.9 109

Y -17.27 84.93 102.2

Z -13.66 96.18 109.8

-sheet

Right handed -helix

Left handed -helix

Atomistic model• pdb file from the protein data bank:

http://www.rcsb.org/pdb/http://www.rcsb.org/pdb/

• Structure resolved via X-ray diffraction ~1.6 Å at 287K and a pH of 6*

• Ramachandran plot: backbone phi, – psi, angles (-180 to 180 deg)

• Topology file generated in Amber using the parm94 force field**

Page 8: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Geometry

C1 C2

C1: GLU(111) z=-11Å, R=7.4 Å acid

turn LYS(147) z=-11Å, R=6.1 Å basic

MET(113) z=-19Å, R=6.4 Å hydrophobic

turn THR(145) z=-19Å, R=8.2 Å hydrophilic

C2: LEU(135) z=-47Å, R=6.3 Å hydrophobic

C1

Page 9: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Amino Acids sequence

Page 10: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Charged residues on the inner pore

Page 11: MD-PNP simulations of Alpha-Hemolysin open channel ion currents
Page 12: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

The MD-PNP model

Page 13: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Multi-scale modeling*

distance Å nm micron mm cm meters

hours

seconds

nanosec

picosec

femtosec

time

MESO

QM

MD

ELECTRONS ATOMS GRAINS GRIDS

Continuum(macroscopic

equations, PNP)

)(

..

iri

iii

rVf

frm

i

ppppp CeDVCeJ

AJpJnI )(

* Goddard group, http://wag.caltech.edu/

Page 14: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

MD-PNP hybrid model

Poisson V(z,r,0))(0

Fnpr CCq

• Diffusion coefficients Dp,Dn of the ions• Fixed pore charges f

MolecularDynamics

• At steady state, the current gradients are zero

AJpJnI )( Open ChannelIon Current

0

0

p

n

J

JNerst-Plank

V(z,r,t)Cn(z,r,t)Cp(z,r,t)

ppppp CeDVCeJ

)(; rVffrmiriiii

slowifastiii ffrmMTS __:

Page 15: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

MD simulations

Page 16: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Benchmarking for NAMD

Machine CPU's Time (day/ns) Speedup/system MFLOPS(average/process) EfficiencyO3K (R12k/400MHz) 32 17.28 1 169.3 -O3K 64 8.89 1.94(of2) 165.1 0.97O3K 128 5.06 3.42(of 4) 153.2 0.86O3K (R14k/600MHz) 32 11.78 1 254.8 -O3K 64 6.13 1.92 255.8 0.96O3K 128 3.52 3.35 222.4 0.84

Machine CPU's Time (days/ns) Speedup/system MFLOPS(average/process) EfficiencyO2K (R10k/250MHz) 32 11.44 1 116 -O2K 64 5.92 1.93 110 0.965O3K (R12k/400MHz) 32 8.24 1 165.8 -O3K 64 4.22 1.95 157.4 0.975O3K 128 2.27 3.64 140.5 0.91O3K 256 1.22 6.5 120.5 0.813O3K (R14k/600MHz) 32 5.63 1 239.4 -O3K 64 2.93 1.92 233.2 0.96O3K 128 1.61 3.5 202.2 0.875O3K 256 0.86 6.55 155.9 0.819O3K 512 0.65 8.66 100.1 0.542

Solvated protein: 175,364 atoms, cutoff 20Å, UC~130Å, t=2fs: 3.52days/ns 128 CPU

Benchmark system: 92,000 atoms, cutoff 12Å, UC~109Å, t= 1fs: 1.61days/ns 128 CPU

Actual system: 120,000 atoms, cutoff 20Å, t=2fs (MTS): 1.29 days/ns for 200 CPU

http://www.ks.uiuc.edu/Research/namd/

Page 17: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

SPC/E water model

• SPC/E model: q(O)=-0.8476e, q(H)=0.4238e

Water RDF

g(OO)

RDF

Peak(Å)Ep

kcal/mol

D

10-9 m2/s

g/cc

SPM model 3 3 -9.89 2.8 0.998

experiments 2.5 3 -9.9 2.4 0.995

Page 18: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Ionic solution, 1MKCl• crystal structure arrangement of atoms (NaCl)

• selected number to correspond to 1M solution (1KCl pair for ~55 water molecules)

•box with 400 KCl pairs

KCl DSPM

10-9 m2/s

DK+

10-9 m2/s

DCl-

10-9 m2/s

400 pairs 2.7 1.8 1.5

experiments 2.5 1.83±0.05 1.8-2.9

K+ Van der Waals parameters (Aquist):

R* = 2.658Å; = 0.000328

G = -80.9kcal/mol;

Cl- Van der Waals parameters (Smith&Dang):

R* = 2.47Å; =0.01;

D(mutual) = 2.9*10-9m2/s

D( dilution) = 1.8*10-9m2/s

Page 19: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

MD procedure

• minimization for 5000 steps

• heating to 300K in steps of 50K

• NPT equilibration of solution for 400ps (time step 2fs)

• dynamics for ~1ns using MTS-NVE

• Pure diffusion

• External applied electric field

Page 20: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Checking the energy and density

Page 21: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Diffusion coefficients

Page 22: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

V=125 mV; Lz = 100 Å; 1 e-=1.6·10-19 C; 1Å = 10-10 m;

E = 0.0288 kcal/mol/Å /e-;

KCl solution inside the pore

Page 23: MD-PNP simulations of Alpha-Hemolysin open channel ion currents
Page 24: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

1K at z = 60Å (center)

ELECTRIC FIELD

- +

DIFFUSION

EEL ~ 40 kcal/mol

VdW ~ -0.03 kcal/mol

EEL~ 15 kcal/mol;

VdW ~ -0.02 kcal/mol

EEL ~ -2 kcal/mol

VdW ~ -0.01 kcal/mol

Page 25: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

K+ selection D (10-9 m2/s)

Cap 0.43

Stem 0.22

Pore 0.38

All K+ 1.95

All K+ no pore 2.01

K+ diffusion coefficients

Page 26: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Cl- selection D (10-9 m2/s)

Cap 0.45

Stem 0.18

Pore 0.31

All Cl- 1.75

All Cl- no pore 1.81

Cl- diffusion coefficients

Page 27: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

CONNOLYCONNOLY CALCULATIONS

PORE:

Rp=1Å V1 = 97199.9 ± 1186.3 Å3

Rp =1.4Å V1.4 = 98508.6 ± 738.7 Å3

Rp =25Å V25 = 212437.4 ± 2466.8 Å3

Vpore= 114583 ± 2835 Å3

n~69 ions

1M = N moles solute/1L solution

=NA molecules/1027 Å3 =6.023E-4 molec/ Å3

Pore volume

Page 28: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Binding energies

Page 29: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Binding energies in the poreK –40<E<-12 kcal/mol

K –40<E<-6 kcal/mol

water –15<E<-5 kcal/mol

water –15<E<-2.5 kcal/mol Cl –9<E<-2.5 kcal/mol

Cl –9<E<-1.5 kcal/mol

Pore E_best (kcal/mol)

+water -15.7

+Cl- -9.0

+ K+ -39.4

Page 30: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

PNP simulations

Page 31: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

z

r

Schematic representation of -hemolysin channel. In the PNP model a 2D grid (represented as concentric rings) corresponding to a cylindrical polar coordinate system (radial and axial) is applied over the pore stem.

2-D Poisson Nerst Plank (PNP)

Page 32: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Pore constrictions and transmembrane voltage(no fixed charges)

VOLTAGE+ 0

0.120 (V)0.120 (V)=20 =80=80

Pore constrictions, transmembrane voltage and fixed charges

Electrostatic potential maps

=80 =80=20

Page 33: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Study at 120mVCase D

(10-9 m2/s)

I

(pA)

Flux

(108 ions/s)

V=120mV, R_cylinder = 8.75Å

K+ Cl- total K+ Cl- K+ Cl-

Pore geometry 0.38 0.31 132.9 73.2 59.7 4.57 3.73

Pore geometry +

2 constrictions

R_min = 5.75 Å

0.38 0.31 95.2 52.4 42.8 3.27 2.67

Pore geometry + 2 constrictions + fixed charges

0.38 0.31 115.5 55.8 59.8 3.48 3.73

V=-120mV (reverse)

Pore geometry + 2 constrictions + fixed charges

0.38 0.31 -72 -38.6 -44.4 2.41 2.77

Page 34: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

V (mV) I (pA) G (nS) Cl-/K+-240 -119.47 0.50 1.18-180 -95.88 0.53 1.20-150 -83.87 0.56 1.15-120 -71.99 0.60 1.15-90 -56.38 0.63 1.14-60 -39.94 0.67 1.10-30 -21.47 0.72 1.1030 24.69 0.82 1.0960 52.68 0.88 1.1290 82.41 0.92 1.11

120* 115.54 0.96 1.07180 186.22 1.03 1.02240 264.16 1.10 0.98

Channel selectivity

* Menestrina, G, The Journal of Membrane Biology, 90, 177-190, 1986

Experimental values:

1M KCl, 120mV G~1nS;

0.5M t(K+)/t(Cl-) ~ 1.5

Anion selective

Page 35: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Open Channel Ion Current

-300

-200

-100

0

100

200

300

-300 -200 -100 0 100 200 300

Voltage (mV)

Ion

Cu

rren

t (p

A)

Geometry

Geometry with FixedCharge Potential

MD-PNP calculations

* Menestrina, G, The Journal of Membrane Biology, 90, 177-190, 1986

Page 36: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

CONCLUSIONS The MD calculations show that both K+ and Cl- ions are transported through the -

hemolysin channel The ions diffusion coefficient inside the pore is reduced by a factor of ~5 for K+ and

~6 for Cl- compared to pure solution. Overall (in solution and in the pore) D(K+) > D(Cl-) while in the pore-cap D(K+) <

D(Cl-) Binding sites for K+ occur at the two ends of the pore (cis and trans) while for Cl- the

best binding sites are located at the stem-cap connecting region There is a greater binding potential and also more binding sites for K+ than Cl-

2D-PNP model prediction show that I-V behavior is consistent with observed experimental profiles: over-linear for

positive voltages and sub-linear for negative voltages A smooth cylinder would have a larger conductance that is reduced by the presence of

the two constrictions The polar walls of the pore increase the current Channel is slightly anion (Cl-) selective

Page 37: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

ACKNOWLEDGEMENTS

• MD simulations with NAMD (http://www.ks.uiuc.edu/Research/namd*)

• Movies and analysis generated with VMD (http://www.ks.uiuc.edu/Research/vmd*)

• Amber, VMD, NAMD lists, GRID (Molecular Inc)

• NAS support group (http://www.nas.nasa.gov)

• System administrators of the Nanotechnology Division: Aldo Foot, Marcy Shull

*VMD/NAMD - developed by the Theoretical and Computational Biophysics Group in the Beckman Institute for Advanced Science and Technology at the University of Illinois at Urbana-Champaign.

Page 38: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

The temperature factor(B- or Debye-Waller factor)

• the molecular motions in the simulation (thermal vibrations) can be related to crystallographic Bi factors (calculated from X-ray scattering)

• Bi is the temperature factor of atom i• Ui is the mean square displacement of atom i• The pore stem and the pore inside are the

“dynamically active” parts

228 ii UB B(eq) = 8pi**2{1/3[U(1,1) + U(2,2) + U(3,3)]}

Page 39: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Hydrophobicity map

• Alternating layers with high (blue) and respectively low (red) hydrophobicity

• Hydrophobicity influences the ongoing dynamics: hydrophylic residues will form

more HB with water thus the local friction coefficient will be larger

Page 40: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

‘Ingredients’ for the MD modeling

ELECTRIC FIELD- +

Force field: Cornell et al, 1995 –AMBER, http://www.scripps.edu/

Multi-CPU scalable MD software: NAMD*, NAMD*, http://www.ks.uiuc.edu/

1M KClThe -hemolysin

pore

Page 41: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

1K at z=35Å (trans) DIFFUSION

ELECTRIC FIELD

- +Interaction energy K+-protein

Electrostatic ~ 15 kcal/mol

VdWaals ~ -0.02 kcal/mol

Page 42: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

1K at z=90Å (cis) DIFFUSION

ELECTRIC FIELD

- +Interaction energy K+-protein

Electrostatic ~ -2 kcal/mol

VdWaals ~ -0.01 kcal/mol

Page 43: MD-PNP simulations of Alpha-Hemolysin open channel ion currents

Diffusion ELECTRIC FIELD- +

1K along channel axis25 15105 354560 55758090 25 15105 354560 55758090