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Narayan Ganesan 1 , Sandeep Patel 2 , and Michela Taufer 1 Computer and Info. Sciences Dept. 1PowerPoint Presentation

Narayan Ganesan 1 , Sandeep Patel 2 , and Michela Taufer 1 Computer and Info. Sciences Dept. 1

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Narayan Ganesan 1 , Sandeep Patel 2 , and Michela Taufer 1 Computer and Info. Sciences Dept. 1

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CHARMM-G, a GPU based MD Simulation code with PME and Reaction Force field for Studying Large Membrane Regions

NarayanGanesan1, SandeepPatel2, and Michela Taufer1

Computer and Info. Sciences Dept.1

Chemistry and Biochemistry Dept.2

University of Delaware

- Overview of forces in molecular dynamics
- Data structures and methodology
- PME for long distance electrostatic interactions
- Steps involved in PME calculations
- Performance and profiling of large membranes
- Related work and conclusions

Classical Forces

Bonded

Non-Bonded

Bonds

Dihedrals

Van der Waals

Electrostatic

Angles

Reaction Field (RF)

PME

- Bond forces:acts only within pairs of molecules
- Angle forces: acts only within a triad of atoms
- Torsion or dihedral forces: acts only within quartet of atoms

- Van derWaals or Lennard-Jones potential: Decays rapidly with distance

- A cutoff of ~10A, accurately captures the effect of the Van der Waals potential

- Coulomb Potential: inverse square law

- Decays as 1/r with distance
- Since 1/r decays rather slowly, the potential can act over long distances

- Choosing a cutoff for electrostatic force/potential causes computational errors and inaccuracy
- Our solutions to sum long distance electrostatic forces:
- Reaction Force Field (RF)
- Ewald summation / Particle Mesh Ewald (PME)

- A single thread is assigned to each atom
- For each atom a set of lists is maintained:
- Bond list stores list of bonds the atom belongs to
- Angle list stores list of angles the atom belongs to
- Dihedral list stores list of dihedrals the atom belongs to
- Nonbond list stores non-bond interactions with atoms within cutoff

q1

q2

q3

q4

q6

q5

q7

q8

q9

q2, r2

q6, r6

q8, r8

q9, r9

Nonbond list for q5:

- MD simulations are iterative executions of MD steps
- Each iteration computes forces on each particle due to:
- Bonds – Bond List
- Angles – Angle List
- Dihedrals – Dihedral List
- Electrostatic
- Van der Waals

- If Ewald summation is used an additional component is added:
- Longdistance interaction using PME method

Bond, angle, anddihedral lists are unchanged for each atom throughout the simulation

Nonbondlist is updated based on acutoff buffer

- NonbondList

- Global neighbor list
- Each thread can iterate through the global list of atoms to build the nonbondlist

- Cell-based neighbor list
- Divide the domain into equal cells of size = cutoff
- Search only in current cell and adjacent cells for neighboring atoms
- There are 26 adjacent cells and 1 current cell in 3-dimensions

- Cell-based list is computationally very efficient but also needs regular cell updates

- Single thread manages a single or a set of cells
- Each cell is managed by a list of atoms in the cell called ‘CellList’
- When an atom ‘i’ moves from Cell A to Cell B, the thread responsible for Cell A updates the list of Cell B via thread safe integer atomic intrinsics
- Invalid atoms are removed from the cell lists by the ‘CellClean’kernel

Cell of interest of edge vectors ax, ay

q1

q1

q1

q1

q1

q1

q1

q1

q1

q2

q2

q2

q2

q2

q2

q2

q2

q2

q3

q3

q3

q3

q3

q3

q3

q3

q3

q6

q6

q6

q6

q6

q6

q6

q6

q6

q4

q4

q4

q4

q4

q4

q4

q4

q5

q5

q5

q5

q5

q5

q5

q5

q5

q4

q7

q7

q7

q7

q7

q7

q7

q7

q7

q8

q8

q8

q8

q8

q8

q8

q8

q8

q9

q9

q9

q9

q9

q9

q9

q9

q9

Region of influence

- Any molecule is surrounded by spherical cavity of finite radius
- Within the radius, electrostatic interactions are calculated explicitly
- Outside the cavity, the system is treaded as a dielectric continuum

- This model allows the replacement of the infinite Coulomb sum by a finite sum plus the reaction filed
where the second terms is the reaction filed correction and Rc is the radius of the cavity

Coulomb

potential

- Proposed by Paul Peter Ewald in 1921 for crystallographic systems
- Has found applications in molecular, astrophysical and crystallographic systems
- Used to sum inverse distance potential over long distance efficiently – e.g., Gravity and Coulomb Potential.
- Was started to be used in the late 70s for numerical simulations
- O(NlogN) instead of O(NxN)

- Three contributions to the total energy, depending on the distance of the interaction:
- Direct space (Edir)
- Reciprocal space (Erec)
- Self energy (Eself)

- Divide interactions into short range (Direct Space) and long range (Reciprocal Space)

Short Range

Direct space using NonbondList

Long Range

Fourier Space

V - Volume of the simulation region

S(m) – Structure parameters

Put charges on grids

1

3

2

4

Multiply with structure constants

FFT of charge grid

FFT back

Convolution yields potential at grid points

which have to be summed

5

Compute force on atom i by calculating

- Each charge is spread on a 4x4x4 = 64 grid points in 3-D
- Grid spacing 1 A by a cardinal B-Spline of order 4
- Create a 3 dimensional Charge Matrix “Q”.

- Mesh-based charge density
- Approximation by sum of charges at each grid point
- Multiple charges can influence a single lattice point

Essmanet al.,

J. Chem. Phys. 1995

Charges

xiyizi: position of the ith charge; k1k2k3: index of the lattice point

- B-Splinehas a region of influence of 4 units
- Each unit = 1A

- During charge spreadingB-Splinehas an impact on the neighboring 4x4x4 cells in 3 dimensions

- Charge Spreading by a cardinal B-Spline of order 4:
- CPU implementation is straightforward
- Time computation: Natomsx 4 x 4 x 4 time steps

- GPU implementation is hard to parallelize
- Can lead to racing conditions - need floating point atomic writes

- Current version of CUDA supports atomic writes for integers only
- Charges need to be converted to fixed point in order to utilize the functionality

Unitcell

charges

CPU spreading of charges:

GPU gathering of charges by a cardinal B-Spline of order 4:

Each thread is assigned

to a lattice point

- Charge spreading on GPU can be parallelized easily by the grid points instead of the atoms
- Each thread works on a single or a set of grid points
- Need O(ax*ay*az) threads, with each thread parsing through all the atoms within 4x4x4 neighborhood –> O(N)

- Each lattice point maintains a list of atoms within 4x4x4 neighborhood for charge gathering

1

2

Effect of charges 1, 2, 3 are gathered at the lattice point

3

q1, r1

q2, r2

q3, r3

Neighbor list of point:

- When a charge moves, several lattice points need to be updated
- The charge is added to the neighbor list of lattice points in dark gray
- The charge is removed from the neighbor list of lattice points in light gray
- Lattice points in white are not affected
- Since there are equal number of light gray and dark gray lattice points, a 1-to-1 mapping was devised

2’

2

The threads for lattice points in light gray update the list of lattice points in dark gray in a 1-to-1 fashion

1

2’

1’

2

- When a single lattice point is updated by multiple threads, thread safe integer atomic intrinsics are used to update the cell lists

- CUFFT provides library functions to compute FFT and inverse FFT
- 3D FFT implemented with series of 1D FFTs and transpositions

- CUFFTExeccan be optimized by choosing proper FFT dimensions
- Power of 2

- One-third of the human genome is composed of membrane-bound proteins
- Pharmaceuticals target membrane-bound protein receptors e.g., G-protein coupled receptors
- Importance of systems to human health and understanding of dysfunction

- State-of-the-art simulations only consider small regions (or patches) of physiological membranes
- Heterogeneity of the membrane spans length scales much larger than included in these smaller model systems.
- Our goal: apply large-scale GPU-enabled computations for the study of large membrane regions

- DiMyristoylPhosphatidylCholine(DMPC) lipid bilayers

- Small system: 17 004 atoms, 46. 8A x 46.8 A x 76.0 A
- Large system: 68 484 atoms, 93.6 A x 93.6 A x 152.0 A

92A

92A

Explicit solvent i.e., water

152A

Membrane

Small membrane (17 004 atoms)

- Largemembrane (68 484atoms)

Case studies: Global neighbor list and RF (I), with cell-based list and RF (II), with neighbor list

and PME (III), and with cell-based neighbor list and PME (IV)

- Large membrane – RF method

Global neighbor list

Cell-based neighbor list

- Large membrane – PME method

Global neighbor list

Cell-based neighbor list

- Other MD code including PME method:
M. J. Harvey and G. De. Fabritiis, J. Chem. Theory and Comp, 2009”

- Our implementation is different in terms of:
- Charge spreading algorithm
- Force field methods, including RF

- CHARMM-G is a flexible MD codebased on the CHARMM force field integrating
- Ewaldsummation
- Reaction force field

- The code supports explicit solvent representations and enables fast simulations of large membrane regions
- Improvements of the CUDA FFT will further improve the performance presented in the paper
- Future work include:
- Code optimizations and parallelization across multiple GPUs
- Scientific characterization of large membranes

GCL Members:

Trilce EstradaBoyu Zhang

Abel LiconNarayanGanesan

LifanXu Philip Saponaro

Maria Ruiz Michela Taufer

Collaborators:

Sandeep Patel, Brad A. Bauer, Joseph E. Davis (Dept. of Chemistry, UD)

Related work:

Bauer et al, JCC 2010 (In Press)

Davis et al., BICoB 2009

More questions: taufer@udel.edu

GCL members in Spring 2010

Sponsors: