<p align="center"> <img src="https://raw.githubusercontent.com/MatthewFilipovich/pycharge/main/docs/source/_static/pycharge_logo.png" width="700px"> </p> <p align="center"> <em>Electromagnetics simulation library for moving point charges built on JAX</em> </p> <div align="center">

</div> <p align="center"> <img width="300" src="https://raw.githubusercontent.com/MatthewFilipovich/pycharge/main/docs/source/_static/oscillating_charge.gif"> </p>

[!IMPORTANT] Major update (v2): PyCharge has been rewritten in JAX with significant API changes. The legacy NumPy-based version remains available under the v1.1.0 tag.

Key Features

⚡️ Point Charge Electrodynamics: Compute relativistically-correct electromagnetic potentials and fields generated by moving point charges.
⚛️ Self-Consistent N-Body Electrodynamics: Simulate the dynamics of electromagnetic sources—such as free charges and dipoles—interacting through their self-generated fields.
🔥 Powered by JAX: Leverage JAX's just-in-time (XLA) compilation for GPU/TPU acceleration, vectorization, and scalable parallel execution.
🛠️ Fully Differentiable: End-to-end differentiability enables gradient-based optimization, control, and inverse design workflows.

Learn more about PyCharge in our research paper published in Computational Physics Communications and available on arXiv

Installation

PyCharge is available on PyPI and can be installed with:

pip install pycharge

Documentation

Read the full documentation at pycharge.readthedocs.io.

Usage

This example shows how to simulate an oscillating charge using PyCharge, computing and visualizing the scalar potential along the x-y axis at z=0 and t=0:

import jax
import jax.numpy as jnp
import matplotlib.pyplot as plt
from scipy.constants import e

from pycharge import Charge, potentials_and_fields

# Define an oscillating point charge with charge +e.
oscillating_charge = Charge(lambda t: [2e-9 * jnp.sin(7.5e16 * t), 0.0, 0.0], e)

# Define 1D axes for the observation points (x, y) and fix z, t.
lim, grid_size = 50e-9, 1000
x = jnp.linspace(-lim, lim, grid_size)
y = jnp.linspace(-lim, lim, grid_size)
z = jnp.array([0.0])
t = jnp.array([0.0])

# Form the full 4D spacetime grid (X, Y, Z, T).
X, Y, Z, T = jnp.meshgrid(x, y, z, t, indexing="ij")

# Build and JIT-compile a function that returns potentials and fields.
quantities_fn = potentials_and_fields([oscillating_charge])
jit_quantities_fn = jax.jit(quantities_fn)

# Evaluate all quantities on the grid (returns a `Quantities` object).
quantities = jit_quantities_fn(X, Y, Z, T)

# Extract and plot the scalar potential on the x–y plane at z=0, t=0.
scalar_2d = quantities.scalar[:, :, 0, 0]
plt.imshow(scalar_2d.T, vmax=0.2)
plt.colorbar(label="Scalar Potential (V)")

For more examples and detailed usage, please refer to the documentation.

Contributing

We welcome contributions! See our Contributing Guide for details.

Citing PyCharge

If you use PyCharge in your research, please cite our paper.

  @article{filipovich2022pycharge,
     title={PyCharge: An open-source Python package for self-consistent electrodynamics simulations of Lorentz oscillators and moving point charges},
     author={Matthew J. Filipovich and S. Hughes},
     year={2022},
     journaltitle = {Computer Physics Communications},
     volume = {274},
     pages = {108291},
     issn = {00104655},
     doi = {10.1016/j.cpc.2022.108291},
     url={https://doi.org/10.1016/j.cpc.2022.108291},
   }

License

PyCharge is distributed under the MIT License. See the LICENSE file for more details.

Pycharge

Install / Use

README