File:Mpl example Helmoltz coils.svg
Summary
| Description |
English: Cross section of B (magnetic field strength) magnitude in a Helmholtz coil (actually consisting of two coils: one at the top, one at the bottom in the plot). The eight contours are for field magnitudes of 0.5 {\displaystyle B_0}, 0.8 {\displaystyle B_0}, 0.9 {\displaystyle B_0}, 0.95 {\displaystyle B_0}, 0.99 {\displaystyle B_0}, 1.01 {\displaystyle B_0}, 1.05 {\displaystyle B_0}, and 1.1 {\displaystyle B_0}, where {\displaystyle B_0} is field strength at center. The large center area has almost uniform field strength. |
| Date | |
| Source | Own work |
| Author | Adrien F. Vincent |
| SVG development |
Rationale: this work aims at providing an up-to-date version of the similar work https://commons.wikimedia.org/wiki/File:Helmholtz_coil,_B_magnitude_cross_section.svg, done by Morn.
Source code has been modified into fully object-oriented matplotlib interface. It now uses the "viridis" colormap, instead of "jet" which produces perceptual glitches. Besides, some changes had to be done to work with versions of numpy more recent than the one originally used.
The matplotlib (mpl) version is 1.5.3, with Python 2.7 and numpy 1.10
Source code

This media was created with Matplotlib (comprehensive library for creating static, animated, and interactive visualizations in Python)Category:Images with Matplotlib source code and Python (general-purpose programming language)Category:Images with Python source code and NumPy (numerical programming package for the Python programming language)Category:Images with NumPy source code
Here is a listing of the source used to create this file.
Here is a listing of the source used to create this file.
##########
## Code for the figure
##########
# -*- coding: utf-8 -*-
from __future__ import division
import matplotlib.pyplot as plt
import numpy as np
from matplotlib.cm import viridis as colormap # future default colormap
"""
Setup
"""
r = 1.0
res = 200 # grid resolution. 100 may be enough, resulting in smaller SVG file)
def dist3(a, b, c, d, e, f):
"""Compute the Euclidian distance from (d, e, f) to (a, b, c),
raised to the 3rd power (and with lower boundary `r`).
"""
return np.maximum(r, np.sqrt((a - d)**2 + (b - e)**2 + (c - f)**2))
x = np.linspace(-150, 150, res)
y = np.linspace(-150, 150, res)
X, Y = np.meshgrid(x, y)
F = np.zeros((res, res, 3))
"""
Computing part
"""
# Loop over two coils
for coils in [1.0, -1.0]:
# Sum field contributions from coil in 10-degree steps
for p in np.arange(0, 360, 10):
xc = 100 * np.sin(np.pi * p / 180.0)
yc = 50 * coils
zc = 100 * np.cos(np.pi * p / 180.0)
MAG = 1.0 / ((r + dist3(X, Y, 0.0, xc, yc, zc))**3)
# (We leave out the necessary constants that would be required
# to get proper units because only scaling behavior will be shown
# in the plot. This is also why a sum instead of an integral
# can be used.)
#
# Due to more stringent casting rules in recent Numpy (>=1.10),
# one builds an explicit list of all the vectors (X - xc, Y - yc, -zc)
# instead of relying on broadcasting. One then reshapes the array Z
# (of the cross-product results) as previously expected.
vectors = np.array([[xval - xc, yval - yc, -zc] for (xval, yval)
in zip(X.reshape(-1), Y.reshape(-1))])
Z = np.cross(vectors, (-zc, 0.0, xc))
Z = Z.reshape(res, res, 3)
F += Z * MAG[:,:,np.newaxis]
# Compute the B-field
B = np.sqrt(F[..., 0]**2 + F[..., 1]**2 + F[..., 2]**2)
# Scale field strength by value at center
B = B / B[res // 2, res // 2]
"""
Plotting part
"""
fig_label = "helmoltz_coils"
plt.close(fig_label)
fig, ax = plt.subplots(figsize=(6, 6), num=fig_label, frameon=False)
levels = (0.5, 0.8, 0.9, 0.95, 0.99, 1.01, 1.05, 1.1)
cs = ax.contour(x, y, B, cmap=colormap, levels=levels)
# Add wire symbols
ax.scatter((100, 100, -100, -100), (50, -50, 50, -50), s=400, color="Black")
ax.axis((-130, 130, -130, 130))
ax.set_xticks([])
ax.set_yticks([])
plt.tight_layout()
plt.show()
fig.savefig("Helmholtz_coil,_B_magnitude_cross_section.svg")
##########
Licensing
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