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    <title>DSpace Collection: Theses--ERC</title>
    <link>http://digital.library.wisc.edu/1793/6478</link>
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      <link>http://minds.wisconsin.edu/simple-search</link>
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      <title>Wavelength-Agile Rayleigh Scattering by use of an Atomic Vapor Cell</title>
      <link>http://digital.library.wisc.edu/1793/6520</link>
      <description>Title: Wavelength-Agile Rayleigh Scattering by use of an Atomic Vapor Cell
&lt;br/&gt;
&lt;br/&gt;Authors: Pertzborn, Amanda Jo
&lt;br/&gt;
&lt;br/&gt;Abstract: A wavelength-agile technique using an atomic vapor cell is developed and applied &#xD;
to the measurement of Rayleigh scattering.  The atomic vapor cell displays a steep &#xD;
change in refractive index as a function of wavelength, thereby creating a wavelength &#xD;
scan over a narrow spectral range.  This scan can be utilized for high resolution spectral &#xD;
measurements.  For example, a short pulse duration laser was input into the cell and the &#xD;
resulting wavelength-agile scan was used to resolve a single iodine absorption feature.  &#xD;
These measurements revealed that the atomic vapor cell distorts the input pulse shape and &#xD;
therefore this technique must be used with care.  A wavelength-agile scan of the Rayleigh &#xD;
scattering spectrum was created using the atomic vapor cell; the resolved Rayleigh &#xD;
scattering spectrum can be compared to theory to obtain the temperature, pressure, and &#xD;
velocity of the scattering medium.  &#xD;
The overall goal of this research was to direct light scattered by the gas in a vortex &#xD;
tube into the atomic vapor cell in order to create a wavelength-agile Rayleigh scattering &#xD;
spectrum.  The temperature, pressure, and velocity at the scattering location would be &#xD;
resolved from the results of this time-of-flight technique.  In this research only the &#xD;
scattering in a fiber was measured due to experimental difficulties.  The results of this &#xD;
measurement indicate that this wavelength-agile Rayleigh scattering technique is &#xD;
difficult.  Rayleigh scattering is extremely weak and therefore difficult to measure while &#xD;
the atomic vapor cell distorts the light passing through it.
&lt;br/&gt;
&lt;br/&gt;Description: Pages: 198</description>
      <pubDate>Fri, 29 Oct 2004 22:58:59 GMT</pubDate>
    </item>
    <item>
      <title>High Spectral Resolution Emission Thermometry for Combustion Applications</title>
      <link>http://digital.library.wisc.edu/1793/6518</link>
      <description>Title: High Spectral Resolution Emission Thermometry for Combustion Applications
&lt;br/&gt;
&lt;br/&gt;Authors: Myers, Adam M.
&lt;br/&gt;
&lt;br/&gt;Abstract: Several spectroscopic emission methods were investigated for the determination of &#xD;
combustion gas temperature.  Spectroscopic simulations based on the HITRAN database &#xD;
were performed to aid in sensor design and data reduction.  Four sensors were created, &#xD;
and limited testing was performed on three of the sensors. &#xD;
 &#xD;
The first sensor was based on a tunable spectroscopic filter being used to resolve the &#xD;
spectrum of the water emission band near 2.6 μm.  The measured water spectrum was &#xD;
compared to simulations to determine the temperature in a gas turbine combustor at &#xD;
Wright-Patterson Air Force Base.   &#xD;
 &#xD;
The second sensor is based on H2O emission in the ν1 + ν3 bands.  Two emission lines &#xD;
located at 1404 nm and 1405 nm were used in a ratiometric manner to determine gas &#xD;
temperature.  A third channel near these lines was used to subtract background emission.   &#xD;
Testing of this sensor was delayed due to lower than expected light detection levels. &#xD;
 &#xD;
The third sensor is based on CO2 emission from 4.2 μm to 4.4 μm.  This region of the &#xD;
CO2 spectrum possesses the unique property of being optically dense over the engine operating range.  The emissivity of this feature is unity, thus the slope of the feature can &#xD;
be compared to the Planck curve to determine temperature.  This sensor was tested using &#xD;
an optically accessible engine based on the GM Triptane block.   &#xD;
 &#xD;
The fourth sensor is based on a commercial optical spectrum analyzer (OSA).  An OSA &#xD;
uses a scanning grating to direct light onto a detector.  It is able to accurately resolve the &#xD;
wavelength and power of incoming light.  The measured data is compared to simulations &#xD;
to determine gas temperature.  Testing of the OSA sensor was performed on a hydrogen- &#xD;
oxygen flame and on a high-pressure, high-temperature test cell.   &#xD;
 &#xD;
A high-pressure, high-temperature (HPHT) test cell was investigated and built to test a &#xD;
variety of sensors.   The HPHT test cell consists of a heated, sealed quartz cell with a &#xD;
known quantity of the species under investigation inside of it.  The cell is located in a &#xD;
pressurized vessel to keep the quartz cell from breaking.  Windows on both ends of the &#xD;
pressure vessel allow for the testing of both emissions and laser-based sensors.  The &#xD;
HTHP cell was tested with a commercial optical spectrum analyzer.
&lt;br/&gt;
&lt;br/&gt;Description: Under the supervision of Assistant Professor Scott T. Sanders, Pages: 104</description>
      <pubDate>Fri, 29 Oct 2004 22:58:59 GMT</pubDate>
    </item>
    <item>
      <title>Application of Supercontinuum Generation to Practical Absorption Spectroscopy</title>
      <link>http://digital.library.wisc.edu/1793/6516</link>
      <description>Title: Application of Supercontinuum Generation to Practical Absorption Spectroscopy
&lt;br/&gt;
&lt;br/&gt;Authors: Filipa, Jonathan A.
&lt;br/&gt;
&lt;br/&gt;Abstract: Supercontinuum light generation was used as a means to generate broadband light &#xD;
for spectroscopic measurements.  The generated broadband light was used to &#xD;
measure carbon monoxide (CO) absorption in a sealed laboratory test cell.  This &#xD;
investigation served as a proof of concept for optical system development that in the &#xD;
future can be applied towards making combustion measurements.   &#xD;
 &#xD;
Some of the basic concepts underlying supercontinuum generation are reviewed &#xD;
and the advantages and disadvantages of this broadband light generation technique &#xD;
are discussed.  Particularly, interference brought on by the propagation of &#xD;
broadband light is reviewed and methods to deal with it are discussed.  The &#xD;
distinction between high and low quality light for making spectroscopic &#xD;
measurements is detailed and CO absorption measurements were made using both &#xD;
types of light.  From reviewing the results, it was found that high quality light is &#xD;
superior to low quality light for making high-speed spectroscopic measurements.
&lt;br/&gt;
&lt;br/&gt;Description: Under the supervision of Assistant Professor Scott T. Sanders, Pages: 92</description>
      <pubDate>Fri, 29 Oct 2004 22:58:59 GMT</pubDate>
    </item>
    <item>
      <title>Development of a Spatially Resolved Optical Technique to Measure Temperature using Two-Photon Absorption of Xenon</title>
      <link>http://digital.library.wisc.edu/1793/6514</link>
      <description>Title: Development of a Spatially Resolved Optical Technique to Measure Temperature using Two-Photon Absorption of Xenon
&lt;br/&gt;
&lt;br/&gt;Authors: Bednar, Natalie J.
&lt;br/&gt;
&lt;br/&gt;Abstract: A new spatially resolved optical technique to measure temperature was developed using &#xD;
two-photon absorption of xenon.  This experiment excited the 256 nm two-photon &#xD;
transition of xenon by focusing the excitation source into a test cell at room temperature.  &#xD;
Two-photon absorption only occurs at the focus of a laser beam; therefore a point &#xD;
measurement technique was possible.  The spatial resolution for this experiment was &#xD;
approximately 0.6 mm; however, this technique enables higher resolution depending on &#xD;
the focus of the laser beam.  Two-photon absorbance versus xenon number density was &#xD;
determined experimentally and used to validate a theoretical model created in MATLAB.  &#xD;
This technique was designed primarily for two non-reacting flows:  the vortex tube and &#xD;
the pulse tube.  A case study for measurement in a vortex tube was presented; however, &#xD;
applying this technique to a pulse tube will be similar.
&lt;br/&gt;
&lt;br/&gt;Description: Under the supervision of Assistant Professor Scott T. Sanders, Pages: 95</description>
      <pubDate>Fri, 29 Oct 2004 22:58:59 GMT</pubDate>
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