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Employing Microsecond-Level Simulations of Membrane Proteins to Capture Their Millisecond- Level Behaviors Using Blue Waters Mahmoud Moradi Department of Chemistry and Biochemistry University of Arkansas biosimlab.uark.edu Blue Waters


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SLIDE 1

Employing Microsecond-Level Simulations of Membrane Proteins to Capture Their Millisecond- Level Behaviors Using Blue Waters

Mahmoud Moradi

Department of Chemistry and Biochemistry University of Arkansas Blue Waters Symposium 2019 Sunriver, OR June 3, 2018

biosimlab.uark.edu

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SLIDE 2

Outline

  • Using molecular dynamics (MD) to study protein

large-scale conformational changes

  • Is the so-called unbiased MD reliable?
  • How can we use biased MD to study large-scale

conformational changes?

  • Developing loosely-coupled multiple-copy (LCMC)

MD algorithms within NAMD

  • Applications to proton-coupled oligopeptide

transporter GkPOT and mechanosensitive channel

  • f large conductance MscL
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SLIDE 3

Large-Scale Conformational Changes in Membrane Transport Proteins

  • Membrane transporters rely on

large-scale conformational changes between inward-facing (IF) and

  • utward-facing

(OF) states (alternating access mechanism).

  • Channels may require large-scale

conformational changes between their

  • pen/active

and closed/inactive states.

IF apo IF bound in

  • ut

in

  • ut

OF apo

  • ut

in

  • ut

in OF bound

  • pen/active

closed/inactive

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SLIDE 4

Large-Scale Conformational Changes in Membrane Transport Proteins

  • Membrane transporters rely on

large-scale conformational changes between inward-facing (IF) and

  • utward-facing

(OF) states (alternating access mechanism).

  • Channels may require large-scale

conformational changes between their

  • pen/active

and closed/inactive states.

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SLIDE 5

Large-Scale Conformational Changes in Membrane Transport Proteins

  • Large-scale conformational changes

require concerted motions

  • f

thousands of atoms whose motions are coupled by direct

  • r

indirect/allosteric interactions.

  • It

typically takes several to thousands of microseconds for a process like those described above to take place.

  • These conformational changes are

typically triggered by certain chemical/mechanical changes in the protein/environment.

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SLIDE 6
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SLIDE 7
  • ut

in in

  • ut

OF apo IF apo

+ + + +

× ×

×

OF,H+ IF,H+ OF,H+,S IF,H+,S S: Substrate

Is the so-called unbiased MD reliable? A Case Study: Proton-coupled Oligopeptide Transporters (POTs)

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SLIDE 8

A Case Study: Proton-coupled Oligopeptide Transporters (POTs)

GkPOT (PDB:4IKV, 1.9 Å) ~100,000 atoms Conventional unbiased MD simulations performed: 8 conditions (different protonation states, substrates) × 400 ns × 2 repeats

K Immadisetty, J Hettige, and M Moradi, What Can and Cannot Be Learned from What Can and Cannot Be Learned from Molecular Dynamics Simulations of Bacterial Proton Molecular Dynamics Simulations of Bacterial Proton-Coupled Coupled Oligopeptide Oligopeptide Transporter ransporter GkPOT GkPOT? J. Phys. Chem. B, 121:3644-3656, 2017.

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SLIDE 9

N-Bundle C

  • B

u n d l e

N-,C-Bundle Interdomain Angle L4,5-L10,11 Distance

Monitoring Global Conformational Changes

10 15 20 25 30 35 40 45 50

C−,N−Bundle Interdomain Angle(°)

UP:apo (Set−1) P:AA (Set−1) (Set−2) P:AA (Set−2) 10 13 16 19 22 25 28 100 200 300 400

L4,10−L5,11 Distance(Å) Time (ns)

UP:apo (Set−1) P:AA (Set−1)

Time (ns)

(Set−2) P:AA (Set−2) Condition 1 Condition 2 Condition 1 Condition 2

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SLIDE 10

10 15 20 25 30 35 40 45 50

C−,N−Bundle Interdomain Angle(°)

UP:apo (Set−1) P:AA (Set−1) UP:apo (Set−2) P:AA (Set−2) 10 13 16 19 22 25 28 100 200 300 400

L4,10−L5,11 Distance(Å) Time (ns)

UP:apo (Set−1) P:AA (Set−1) 100 200 300 400

Time (ns)

UP:apo (Set−2) P:AA (Set−2)

Reproducibility Check

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SLIDE 11

“Structural basis for dynamic mechanism of proton-coupled symport by the peptide transporter POT.” PNAS 2013 | vol. 110 | no. 28 | 11343–11348.

Although a common practice, statements made about millisecond-level biomolecular events based on unbiased sub-microsecond level simulations may not be reliable. Reproducibility Check

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SLIDE 12

How can we use biased MD to study large-scale conformational changes?

Inward-Facing Outward-Facing

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SLIDE 13

How can we use biased MD to study large-scale conformational changes?

Nonequilibrium Work

Empirical Protocol Optimization

Stage1: Path Generation

Conformational Transition Free Energy Reaction Coordinate

Stage 2: Path OptIimization Stage 3: Path Characterization

Simulation Time Collective Variable Collective Variable

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SLIDE 14
  • Path-finding algorithms:

e.g., string method (SM or SMwST)

– Start from an initial string of N images (𝜼$) – Restrain M copies of each image for time ∆𝑢

𝑉$ 𝝄 = *

+ 𝑙 𝝄 − 𝜼$ 2

– Release the restraints and run for time ∆𝑢′ – New string (𝜼$) is determined from 𝝄 𝑗’s – Iterate until converged

  • Free energy calculations:

e.g., umbrella sampling (US or BEUS):

– Bias one or more (e.g., M) copies: – Use a reweighting scheme to unbias the data:

𝑉$ 𝝄 = 1 2 𝑙 𝝄 − 𝜼$ 2

Path-Finding Algorithms and Free Energy Calculations Based on Loosely-Coupled Multiple-Copy (LCMC) MD

Shirts, Chodera, JCP, 129, 124105 (2008)

e−βF

i =

e−βUi (ξ t ) nje

−β(U j (ξ t )−Fj ) j

all samples

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SLIDE 15

Riemannian Reformulation

Fakharzadeh & Moradi, Effective Riemannian diffusion model for conformational dynamics of biomolecular systems. J Phys Chem Lett. 2016;7(24):4980-4987.

  • Riemannian reformulation of path-finding algorithms and free

energy calculations methods such as SMwST/BEUS provides solutions for the minimum free energy path and its free energy that are invariant under coordinate transformation.

  • The Riemannian formulation allows for developing more

robust free energy calculation methods and path-finding algorithms (due to the “invariance” feature).

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SLIDE 16

Multiple concurrent NAMD instances are launched with internal partitions of Charm++ and located continuously within a single communication

  • world. Messages between NAMD

instances are passed by low-level point-to-point communication functions, which are accessible through NAMD's TCL scripting interface.

LCMC MD with NAMD

  • W. Jiang, J. Phillips, et al. Computer Physics

Communications , 185, 908, 2014.

Within the LCMC MD scheme, we have developed various improved variations of SMwST/BEUS

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SLIDE 17

Free Energy (kcal/mol) Reaction Coordinate

Free Energy along the GKPOT IF-OF Transition Path

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SLIDE 18

Closed Open

TM Helices PDB: 2OAR MD Model

H+ H+

Tension Induced Opening Charge Induced Opening pH-Dependent Drug Release Proteoliposome Engineered MscL Wild-Type MscL

1 2 3

pH-induced Activation of an Engineered Mechanosensitive Channel of Large Conductance (MscL)

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SLIDE 19

Dylan Ogden Vivek Govind Kumar Adithya Polasa Curtis Goolsby Ugochi Isu Hamid Tabari