File:Magnetic field of an idealized quadrupole with forces.svg
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Summary
DescriptionMagnetic field of an idealized quadrupole with forces.svg |
English: Magnetic field of an idealized quadrupole with forces
Русский: Магнитное поле и силы в квадрупольном магните |
Date | |
Source | python/matplotlib |
Author | Andre.holzner |
Other versions |
|
SVG development InfoField | This W3C-invalid vector image was created with an unknown SVG tool. |
Other information
xpoints = arange(-5,5,0.05)
ypoints = arange(-5,5,0.05)
X,Y = meshgrid(xpoints, ypoints)
circularMask = False
areaRadius = 4
# order of the magnet
n = 2
def func(x,y):
# the function to draw
return ((x + 1j * y)**(n)).real
func = vectorize(func)
V = func(X,Y)
# mask points which we don't want to draw
if circularMask:
# circular mask
distance = sqrt(X**2 + Y**2)
V = ma.masked_where(distance > areaRadius, V)
else:
# polygonal mask
# principal directions are at (i + 0.5) / (2n) * 2pi
#
for i in range(2*n):
angle = (i + 0.5) / float(2*n) * 2*pi
# define a straight angle perpendicular to angle
# mask all points on one side of this line
anchor_x = areaRadius * cos(angle)
anchor_y = areaRadius * sin(angle)
normal_x = cos(angle)
normal_y = sin(angle)
def acceptFunc(x,y):
value = (x - anchor_x) * normal_x + (y - anchor_y) * normal_y
return value > 0
acceptFunc = vectorize(acceptFunc)
V = ma.masked_where(acceptFunc(X,Y), V)
if True:
# levels equidistant in function value
vmax = V.max()
V /= vmax
levels = arange(-2,2,0.05)
else:
# levels equidistant on x and y axis
# determine the levels to draw from values on one of the axes
levels = [ float(func(x,0)) for x in arange(min(xpoints), max(xpoints),0.50) ] + \
[ float(func(0,y)) for y in arange(min(ypoints), max(ypoints),0.50) ]
levels = sorted(list(set(levels)))
vmax = 1
figure(figsize=(6,6));
Q = contour(X,Y, V, colors= 'black', linestyles = 'solid',
levels = levels
)
# axis([-5,5,-5,5])
xlabel("x coordinate")
ylabel("y coordinate")
# mask points which we don't want to draw
if not circularMask:
# polygonal mask
# principal directions are at (i + 0.5) / (2n) * 2pi
#
for i in range(2*n):
angle = (i + 0.5) / float(2*n) * 2*pi
if i % 2:
label = "N"
color = 'red'
else:
label = "S"
color = 'green'
anchor_x = 1.1 * areaRadius * cos(angle)
anchor_y = 1.1 * areaRadius * sin(angle)
text(anchor_x, anchor_y, label, size = 20, color = color,
horizontalalignment='center',
verticalalignment='center')
#----------------------------------------
if n == 2:
# quadrupole, draw some examples of force on charged particle
# find kth level line on axes (x = 0 and y = 0)
# the potential function is >= 0 on the x axis and <= 0 on the y axis
# for a quadrupole
lev = sorted(list(levels[levels >= 0]))[4]
# find distance of this level on axis from origin
# (exploit the 90 degree symmetry of the field)
dist = fsolve(lambda x: func(x,0) / vmax - lev,3)[0]
# rotation by +90 degrees
rotMatrix = array([[0,-1],[1,0]])
invRotMatrix = rotMatrix.T
arrowLength = 1.5
arrowStart = array([dist, 0])
origArrowDir = array([0, arrowLength])
bfieldLabelPosOffset = array([0.3, 0.5 * arrowLength])
forceLabelPosOffset = array([0.5 * arrowLength, -0.3])
for i in range(4):
arrowDir = origArrowDir[:]
for j in range(i):
arrowDir = rotMatrix.dot(arrowDir)
# take into account quadrupole structure
arrowDir *= (-1)**i
# draw arrow for the B field
arrow(arrowStart[0],arrowStart[1], arrowDir[0], arrowDir[1],head_width=0.3, head_length=0.3, color = 'red')
# add a label for the B field
textPos = arrowStart + (-1)**i * bfieldLabelPosOffset
text(textPos[0],
textPos[1], "B", size = 20, color = 'red',
horizontalalignment='center',
verticalalignment='center')
# draw the arrow for the force
arrowDir2 = invRotMatrix.dot(arrowDir)
arrow(arrowStart[0], arrowStart[1], arrowDir2[0], arrowDir2[1],head_width=0.3, head_length=0.3, color = 'blue')
# label for the force
textPos = arrowStart + (-1)**i * forceLabelPosOffset
text(textPos[0],
textPos[1], "F", size = 20, color = 'blue',
horizontalalignment='center',
verticalalignment='center')
#----------
# prepare next iteration
arrowStart = rotMatrix.dot(arrowStart)
bfieldLabelPosOffset = rotMatrix.dot(bfieldLabelPosOffset)
forceLabelPosOffset = rotMatrix.dot(forceLabelPosOffset)
Licensing
Andre.holzner, the copyright holder of this work, hereby publishes it under the following licenses:
Permission is granted to copy, distribute and/or modify this document under the terms of the GNU Free Documentation License, Version 1.2 or any later version published by the Free Software Foundation; with no Invariant Sections, no Front-Cover Texts, and no Back-Cover Texts. A copy of the license is included in the section entitled GNU Free Documentation License.http://www.gnu.org/copyleft/fdl.htmlGFDLGNU Free Documentation Licensetruetrue |
This file is licensed under the Creative Commons Attribution-Share Alike 3.0 Unported license.
Attribution: Andre.holzner
- You are free:
- to share – to copy, distribute and transmit the work
- to remix – to adapt the work
- Under the following conditions:
- attribution – You must give appropriate credit, provide a link to the license, and indicate if changes were made. You may do so in any reasonable manner, but not in any way that suggests the licensor endorses you or your use.
- share alike – If you remix, transform, or build upon the material, you must distribute your contributions under the same or compatible license as the original.
You may select the license of your choice.
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depicts
16 December 2012
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Date/Time | Thumbnail | Dimensions | User | Comment | |
---|---|---|---|---|---|
current | 21:12, 16 December 2012 | 540 × 540 (171 KB) | Andre.holzner | Uploading a self-made file using File Upload Wizard |
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Width | 432pt |
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Height | 432pt |