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Introduction
- This website is a collection of the sounds, images, and movies I've
created during my semester working at CTX.
I have been working with
Ben
Levitt and Professor
Mauel to try to better illustrate the data
collected at CTX by
using Mathematica and IDL. Furthermore, there are some images and movies
created with a webcam which help to
show how we make plasma at CTX.
At CTX, we use a mechanically suspended dipole magnet to
create a hot electron, ECRH plasma. We generally make a hydrogen
plasma, although occasionally we use other gases. Microwaves
are used to produce these energetic deeply-trapped electrons.
We then use a variety of diagnostics to study the plasma.
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Images
- Here is a collection of images created using a simple webcam. We
mounted an Apple iSight to the exterior of the chamber looking in
through a port hole, and then recorded a variety of different kinds
of shots. These are the best frames extracted from those movies. These
pictures clearly show the geometry of the deeply trapped dipole plasma,
characteristic of CTX.
- The light that we see in these pictures is emitted from charged particles
colliding with neutral particles. When a collision occurs, these neutrals
become excited, and upon relaxation they emit photons. The number of
neutrals is proportional to the density of the plasma. Therefore, in
higher density shots we see more light emitted.
- Furthermore, it is interesting that the high density region appears
to be so well defined. Plasma density is inversely proportional
to the radius^4. However, we see a clearly defined boundary of light.
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- High Density
- In this picture one can clearly see the torus
of plasma surrounding the polar grid detector, and one of
the floating potential
probes inserted into the plasma.
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- Medium Density
- This view is more of a close-up of the polar grid
detector and the tungsten mesh surrounding it. We can also
see some microwave heating effects on the fringe of the tungsten
mesh.
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- High Density
- For many of the shots, we would get strange
color variations, usually blue and purple. However, we believe
that this effect had to do with the iSight trying to compensate
for the
quick flash of light and not because of the nature of the
plasma.
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Sounds
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These sounds were generated using Mathematica and
IDL to help illustrate the rotationally driven interchange instability.
Ben Levitt is using the tungsten mesh to induce an electric
field, which in turn, rotates the plasma, and drives this instability.
The data was taken from one of the fast floating potential probes
and
converted
into
a
data file using IDL. The data was then imported into Mathematica
and used to generate time frequency domain plots (TFDs) and sound
files of the frequency content embedded in the fast floating probe
data. Here is the IDL
script.
Here is the Mathematica
File.
Movies
-
These movies are the original footage that we took
with the iSight. They are in real time. During roughly the first
.6 seconds, microwaves are being used to heat the plasma. However,
afterwards there is an afterglow period when, although the heating
is off, the plasma persists. This period is the clearest part of
the shot because we believe that the microwaves interfere with
the
CCD in
the iSight.
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In order to try to reduce the microwave interference,
we built a Faraday cage. We used a fine wire mesh surrounding the iSight
to try to reduce the effects of the microwaves. This
did
allow
us
to
see
more
of the
shot
without
interference. However, the wire mesh was still substantial enough to
obscure the view.
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- High Density
- w/ Faraday cage
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These movies are created using the polar grid detector.
The data from the detectors are processed in IDL and combined into
movie files. The IDL code is adapted from Ben Levitt's original
code. It uses cubic spline interpolation to create a polar contour
surface from a set of irregular grid points. The orange and yellow
colors represent areas of positive charge, and the blue and purple
colors represent areas of negative charge. The black dots are the
locations of the polar grid detectors.
- With these movies, we are trying to observe drift waves rotating
at roughly 5 khz. In the future we would like to use this setup to
observe the rotation of the plasma when we induce an electric field
with the tungsten mesh. However, currently the polar grid detector
hardware isn't sensitive enough yet to be used in the lower density
regime in
which we currently use the meshes.
- In these movies we can see some subtle signs of rotation. Not all
the detectors are working, which can be clearly seen by some strange
effects in the upper right corner of the plot. However, some drift
waves are noticeable.
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- High Density
- Shot 3830
- .51 < time .512
- 1000 frames
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- Thanks so much to Professor Mauel for the opportunity to work
at CTX this semester, and Ben Levitt for teaching me so much
about how
CTX works.
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