This post demonstrates a simplified molecular dynamics (MD) simulation implemented in Python. We’ll explore the core components required to simulate particle motion under the influence of physical forces.
The simulation is governed by a few key physical parameters:
The positions and velocities of the particles are represented using NumPy arrays:
The calculate_forces function determines the interactions between particles. In this simplified model, we use a basic placeholder, but in a real simulation, this would involve potentials like the Lennard-Jones or harmonic oscillators.
The core loop follows the Velocity Verlet integration steps:
import numpy as np
# Simulation Constants
mass = 1.0
dt = 0.001
steps = 1000
# Initial State: Two particles in 3D space
positions = np.array([[0.0, 0.0, 0.0],
[1.0, 0.0, 0.0]])
velocities = np.array([[0.0, 0.0, 0.0],
[0.0, 1.0, 0.0]])
def calculate_forces(pos):
"""Placeholder for force calculation logic."""
forces = np.zeros_like(pos)
# Example: Simple attraction towards the origin
forces = -0.5 * pos
return forces
# Simulation Loop
print("Starting Simulation...")
for step in range(steps):
# Determine current forces
forces = calculate_forces(positions)
# Update state using Euler-Cromer integration
velocities += (forces / mass) * dt
positions += velocities * dt
# Optional: Log output periodically
if (step + 1) % 100 == 0:
print(f"Step {step+1}: Particle 1 Position -> {positions[0]}")
print("Simulation Complete.")
This code serves as a foundational demonstration of MD principles. For realistic biological simulations involving thousands of atoms, specialized high-performance software like GROMACS, NAMD, or LAMMPS is recommended.
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