本文へ移動
cccskills
無料GitHub で公開

physics-visualization

Publication-quality physics plots — vector fields, streamlines, contour maps, 3D surfaces, phase space, spectrograms, and animations. Optimized for journal submission with LaTeX labels, proper colormaps, and multi-panel layouts.

インストール方法を見る

含まれるファイル(1)

  • SKILL.md7.7 KB

SKILL.md(原文)

インストールする前に、エージェントに与えられる指示の中身を確認できます。

Physics Visualization

Overview

Generate publication-quality figures for physics: vector fields, streamlines, contour plots, 3D surfaces, phase diagrams, spectrograms, and animations. All plots use LaTeX rendering, proper colormaps, and journal-ready formatting.

When to Use

  • Any physics result that needs a figure
  • Vector fields (E&M, fluid flow, gravitational fields)
  • Contour/heatmap plots (potential fields, temperature distributions, wavefunctions)
  • Phase space plots (trajectories, Poincare sections)
  • 3D surface plots (energy landscapes, wavefunctions)
  • Animations (time-evolving systems)
  • Multi-panel comparison figures

Setup

import numpy as np
import matplotlib
matplotlib.use('Agg')  # non-interactive backend for scripts
import matplotlib.pyplot as plt
from matplotlib import cm
from mpl_toolkits.mplot3d import Axes3D

# Publication-quality defaults
plt.rcParams.update({
    'font.size': 12,
    'axes.labelsize': 14,
    'axes.titlesize': 15,
    'xtick.labelsize': 11,
    'ytick.labelsize': 11,
    'legend.fontsize': 11,
    'figure.dpi': 150,
    'savefig.dpi': 300,
    'savefig.bbox': 'tight',
    'axes.grid': True,
    'grid.alpha': 0.3,
    'lines.linewidth': 1.5,
})

# Enable LaTeX if available
try:
    plt.rcParams.update({
        'text.usetex': True,
        'font.family': 'serif',
    })
except:
    pass  # fallback to mathtext

Core Plot Types

1. Vector Field

def plot_vector_field(ax, X, Y, U, V, title='', normalize=True, cmap='viridis'):
    """Plot a 2D vector field with magnitude coloring."""
    magnitude = np.sqrt(U**2 + V**2)
    if normalize:
        U_n = U / (magnitude + 1e-10)
        V_n = V / (magnitude + 1e-10)
    else:
        U_n, V_n = U, V

    q = ax.quiver(X, Y, U_n, V_n, magnitude, cmap=cmap, alpha=0.8)
    plt.colorbar(q, ax=ax, label='|F|')
    ax.set_title(title)
    ax.set_aspect('equal')
    return q

# Example: Electric dipole field
x = np.linspace(-3, 3, 20)
y = np.linspace(-3, 3, 20)
X, Y = np.meshgrid(x, y)

# Dipole at (±0.5, 0)
def dipole_field(X, Y, d=0.5):
    r_plus = np.sqrt((X-d)**2 + Y**2)
    r_minus = np.sqrt((X+d)**2 + Y**2)
    Ex = (X-d)/r_plus**3 - (X+d)/r_minus**3
    Ey = Y/r_plus**3 - Y/r_minus**3
    return Ex, Ey

Ex, Ey = dipole_field(X, Y)
fig, ax = plt.subplots(figsize=(8, 8))
plot_vector_field(ax, X, Y, Ex, Ey, title='Electric Dipole Field')
ax.set_xlabel('x [m]')
ax.set_ylabel('y [m]')
plt.savefig('vector_field.png', dpi=150, bbox_inches='tight')

2. Streamlines

fig, ax = plt.subplots(figsize=(10, 8))
x_fine = np.linspace(-3, 3, 100)
y_fine = np.linspace(-3, 3, 100)
X_f, Y_f = np.meshgrid(x_fine, y_fine)
Ex_f, Ey_f = dipole_field(X_f, Y_f)
magnitude = np.sqrt(Ex_f**2 + Ey_f**2)

strm = ax.streamplot(X_f, Y_f, Ex_f, Ey_f, color=np.log10(magnitude+1e-3),
                      cmap='inferno', density=2, linewidth=1, arrowsize=1.5)
plt.colorbar(strm.lines, ax=ax, label=r'$\log_{10}|E|$')
ax.plot([-0.5, 0.5], [0, 0], 'ro', markersize=10, label='Charges')
ax.set_xlabel('x [m]')
ax.set_ylabel('y [m]')
ax.set_title('Electric Field Streamlines')
ax.legend()
plt.savefig('streamlines.png', dpi=150, bbox_inches='tight')

3. Contour / Heatmap

def plot_contour(ax, X, Y, Z, title='', levels=20, cmap='RdBu_r', symmetric=True):
    """Contour plot with optional symmetric colorbar (good for potentials)."""
    if symmetric:
        vmax = np.max(np.abs(Z))
        vmin = -vmax
    else:
        vmin, vmax = Z.min(), Z.max()

    cf = ax.contourf(X, Y, Z, levels=levels, cmap=cmap, vmin=vmin, vmax=vmax)
    cs = ax.contour(X, Y, Z, levels=levels, colors='k', linewidths=0.3, alpha=0.5)
    plt.colorbar(cf, ax=ax, label=title)
    ax.clabel(cs, inline=True, fontsize=8, fmt='%.1f')
    ax.set_aspect('equal')
    return cf

# Example: 2D wavefunction |ψ|²
r = np.linspace(-5, 5, 200)
X, Y = np.meshgrid(r, r)
R = np.sqrt(X**2 + Y**2)
# Hydrogen 2p orbital (simplified)
psi = R * np.exp(-R/2) * X / R  # p_x orbital
psi_sq = np.abs(psi)**2

fig, ax = plt.subplots(figsize=(8, 7))
plot_contour(ax, X, Y, psi_sq, title=r'$|\psi_{2p}|^2$', symmetric=False, cmap='hot')
ax.set_xlabel('x [a₀]')
ax.set_ylabel('y [a₀]')
ax.set_title(r'Hydrogen $2p_x$ Probability Density')
plt.savefig('wavefunction.png', dpi=150, bbox_inches='tight')

4. 3D Surface

fig = plt.figure(figsize=(10, 8))
ax = fig.add_subplot(111, projection='3d')

# Energy landscape
x = np.linspace(-2, 2, 100)
y = np.linspace(-2, 2, 100)
X, Y = np.meshgrid(x, y)
Z = (X**2 - 1)**2 + Y**2  # double-well potential

surf = ax.plot_surface(X, Y, Z, cmap='coolwarm', alpha=0.8,
                       linewidth=0, antialiased=True)
ax.set_xlabel('x')
ax.set_ylabel('y')
ax.set_zlabel('V(x,y)')
ax.set_title('Double-Well Potential')
fig.colorbar(surf, ax=ax, shrink=0.6, label='V')
plt.savefig('surface_3d.png', dpi=150, bbox_inches='tight')

5. Animation

from matplotlib.animation import FuncAnimation, PillowWriter

def create_animation(update_func, n_frames, fig, interval=50, filename='animation.gif'):
    """Create and save an animation."""
    anim = FuncAnimation(fig, update_func, frames=n_frames, interval=interval, blit=True)
    writer = PillowWriter(fps=1000/interval)
    anim.save(filename, writer=writer)
    print(f"Animation saved: {filename}")
    return anim

# Example: wave propagation
fig, ax = plt.subplots(figsize=(10, 4))
x = np.linspace(0, 10, 500)
line, = ax.plot(x, np.sin(x), 'b-', linewidth=2)
ax.set_ylim(-1.5, 1.5)
ax.set_xlabel('x')
ax.set_ylabel('u(x,t)')
time_text = ax.text(0.02, 0.95, '', transform=ax.transAxes)

def update(frame):
    t = frame * 0.05
    y = np.sin(2*np.pi*(x - t)) * np.exp(-0.1*t)
    line.set_ydata(y)
    time_text.set_text(f't = {t:.2f}')
    return line, time_text

create_animation(update, 200, fig, interval=33, filename='wave.gif')

6. Multi-Panel Figure

def multi_panel(n_rows, n_cols, figsize=None, sharex=False, sharey=False):
    """Create a multi-panel figure with consistent styling."""
    if figsize is None:
        figsize = (5*n_cols, 4*n_rows)
    fig, axes = plt.subplots(n_rows, n_cols, figsize=figsize,
                              sharex=sharex, sharey=sharey)
    # Add panel labels (a), (b), (c), ...
    if n_rows * n_cols > 1:
        for i, ax in enumerate(np.atleast_1d(axes).flat):
            label = chr(ord('a') + i)
            ax.text(-0.12, 1.05, f'({label})', transform=ax.transAxes,
                    fontsize=14, fontweight='bold', va='top')
    return fig, axes

Colormap Guide

Data TypeRecommended ColormapWhy
Sequential (magnitude, density)viridis, plasma, infernoPerceptually uniform, colorblind-safe
Diverging (potential, temperature anomaly)RdBu_r, coolwarmSymmetric around zero
Cyclic (phase, angle)twilight, hsvWraps around
Binary (positive/negative)bwrClear sign distinction

Never use jet or rainbow — they are not perceptually uniform and mislead.

Save Format Guide

FormatWhen to Use
PNG (300 dpi)General use, presentations
PDFJournal submission, vector graphics
SVGWeb, editable vector
EPSLegacy journals requiring EPS

Always save both PNG and PDF:

plt.savefig('figure.png', dpi=300, bbox_inches='tight')
plt.savefig('figure.pdf', bbox_inches='tight')

レビュー

まだレビューはありません。使ってみた感想をお寄せください。

同じリポジトリのスキル

概要と使いどころ

Simplest distributed training API. 4 lines to add distributed support to any PyTorch script. Unified API for DeepSpeed/FSDP/Megatron/DDP. Automatic device placement, mixed precision (FP16/BF16/FP8). Interactive config, single launch command. HuggingFace ecosystem standard.

日本語の概要は準備中です。原文の説明を表示しています。

huang-sh/DeepScience42026年7月15日 更新

ADMET property prediction for drug candidates. Full pharmacokinetic panel (Caco-2, PPB, clearance, CYP), toxicity (hERG, AMES, DILI), drug-likeness (Lipinski, QED), using RDKit descriptors and TDC models.

日本語の概要は準備中です。原文の説明を表示しています。

huang-sh/DeepScience42026年7月15日 更新

Interpretable ADMET analysis with mechanistic reasoning. Maps liabilities to structural causes and biological pathways. Based on CoTox (Park 2025) and DrugR (Liu 2026).

日本語の概要は準備中です。原文の説明を表示しています。

huang-sh/DeepScience42026年7月15日 更新

aeon

無料

This skill should be used for time series machine learning tasks including classification, regression, clustering, forecasting, anomaly detection, segmentation, and similarity search. Use when working with temporal data, sequential patterns, or time-indexed observations requiring specialized algorithms beyond standard ML approaches. Particularly suited for univariate and multivariate time series analysis with scikit-learn compatible APIs.

日本語の概要は準備中です。原文の説明を表示しています。

huang-sh/DeepScience42026年7月15日 更新

arboreto

無料

Infer gene regulatory networks (GRNs) from gene expression data using scalable algorithms (GRNBoost2, GENIE3). Use when analyzing transcriptomics data (bulk RNA-seq, single-cell RNA-seq) to identify transcription factor-target gene relationships and regulatory interactions. Supports distributed computation for large-scale datasets.

日本語の概要は準備中です。原文の説明を表示しています。

huang-sh/DeepScience42026年7月15日 更新

astropy

無料

Comprehensive Python library for astronomy and astrophysics. This skill should be used when working with astronomical data including celestial coordinates, physical units, FITS files, cosmological calculations, time systems, tables, world coordinate systems (WCS), and astronomical data analysis. Use when tasks involve coordinate transformations, unit conversions, FITS file manipulation, cosmological distance calculations, time scale conversions, or astronomical data processing.

日本語の概要は準備中です。原文の説明を表示しています。

huang-sh/DeepScience42026年7月15日 更新

huang-sh のスキルをすべて見る

このスキルの問題を報告する