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Reactions of sulphur and acetylene on a palladium (III) surfacePatterson, C. H. January 1985 (has links)
No description available.
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Proportional integral derivative control of an oil-heated fractal-like branching microchannel desorber /Davis, Keith R. January 1900 (has links)
Thesis (M.S.)--Oregon State University, 2008. / Printout. Includes bibliographical references (leaves 90-92). Also available on the World Wide Web.
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Activated and nonactivated desorption from polymer surfacesIlie, Carolina Cristina. January 2008 (has links)
Thesis (Ph.D.)--University of Nebraska-Lincoln, 2008. / Title from title screen (site viewed Apr. 9, 2009). PDF text: xvii, 113 p. : ill. (some col.) ; 3 Mb. UMI publication number: AAT 3339351. Includes bibliographical references. Also available in microfilm and microfiche formats.
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SiCl4 desorption in chlorine etching of Si(100): a first principle study.January 1999 (has links)
Chan Siu-pang. / Thesis (M.Phil.)--Chinese University of Hong Kong, 1999. / Includes bibliographical references (leaves 45-47). / Abstract also in Chinese. / TITLE PAGE --- p.i / THESIS COMMUTE --- p.ii / ABSTRACT (English) --- p.iii / ABSTRACT (Chinese) --- p.iv / ACKNOWLEDGMENT --- p.v / TABLE OF CONTENTS --- p.vi / LIST OF FIGURES --- p.vii / LIST OF TABLES --- p.viii / Chapter CHAPTER 1. --- Introduction --- p.1 / Chapter Section 1.1. --- General Introduction --- p.1 / Chapter Section 1.2. --- Background Information --- p.2 / Chapter 1.2.1. --- Si(100) Surface --- p.2 / Chapter 1.2.2. --- Structure of Cl/Si(100) --- p.7 / Chapter Section 1.3. --- Etching of Si(100) by Chlorine --- p.9 / Chapter Section 1.4. --- Theory --- p.14 / Chapter Section 1.5. --- Computational Model --- p.17 / Chapter CHAPTER 2. --- Desorption Mechanism of SiCl4 --- p.19 / Chapter Section 2.1. --- Desorption Mechanism --- p.19 / Chapter 2.1.1. --- Trajectory1 --- p.20 / Chapter 2.1.2. --- Trajectory2 --- p.23 / Chapter 2.1.3. --- Trajectory3 --- p.26 / Chapter 2.1.4. --- Trajectory4 --- p.29 / Chapter 2.1.5. --- Trajectory5 --- p.32 / Chapter 2.1.6. --- Trajectory6 --- p.35 / Chapter Section 2.2. --- Discussion --- p.38 / Chapter Section 2.3. --- Conclusion --- p.44 / REFERENCES: --- p.45
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An experimental study of co-flow ammonia-water desorption in an oil-heated, microscale, fractal-like branching heat exchangerMouchka, Gregory A. 24 March 2006 (has links)
An experimental study was performed in which an ammonia-water solution
was desorbed within a branching fractal-like microchannel array. The solution entered
in the center of a disk, and flowed out radially until discharging in to a gravity-driven
separation chamber. Heat was added to the ammonia-water through a thin wall, above
which flowed heat transfer oil in a separate branching fractal-like microchannel array.
Such arrays have been shown to utilize the increased heat transfer coefficients seen in
parallel channel arrays; however, they do so with a lower pressure drop.
An experimental flow loop consisting of ammonia-water and heat transfer oil
sub-loops was instrumented along with a test manifold for global measurements to be
taken. Temperature, pressure, density and mass flow rate measurements permitted
calculation of desorption and heat transfer characteristics. Parameters included oil
mass flow rate, oil inlet temperature, and strong solution flow rate, while strong
solution concentration, temperature, and weak solution pressure were kept constant.
The desorber was assumed to achieve equilibrium conditions between the
vapor and weak solution in the separation chamber. The exit plenum was large and
acted as a flash chamber, making the assumption reasonable. The vapor mass fraction
was determined from knowledge of the weak solution saturation temperature.
Heat exchanger analyses (LMTD and ε-NTU) were done to determine the heat
transfer characteristics of the desorber. Calculated values of UA are shown to be as
high as 5.0 W/K, and desorber heat duties were measured as high as 334 W. Strong
solution, at 0.30 mass fraction, was desorbed into weak solution and vapor with
concentrations ranging from 0.734 to 0.964. Circulation ratios, defined as strong
solution mass flow rate per unit desorbed vapor mass flow rate, varied in this study
from 3.4 to 20.
A method for specifying desorber operating conditions is described, in which a
minimum desorber heat input per unit vapor flow rate is determined at an optimum
circulation ratio. A description of how the circulation ratio behaves as a function of
strong solution mass flow rate, oil flow rate, and the maximum temperature difference
between oil and ammonia-water solution is shown. / Graduation date: 2006
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Transport mechanisms in nanoscale amorphous solid water filmsMcClure, Sean Michael, January 1900 (has links) (PDF)
Thesis (Ph. D.)--University of Texas at Austin, 2006. / Vita. Includes bibliographical references.
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Design and testing of a laboratory apparatus for scaled experiments of in-situ thermal desorptionHartman, Meghan M. 04 June 2015 (has links)
There are 1,305 Superfund Sites on the United States Environmental Protection Agencies National Priorities List that may require remediation due to the environmental or human health risks associated with subsurface contamination. The contaminants present at these sites and others vary with respect to their physical and chemical properties which dictate the selection of appropriate remediation technologies. In-Situ Thermal Desorption (ISTD) has been studied as a remediation technique for removing many recalcitrant contaminants from soil. ISTD involves passing electrical current through heating elements in wells and removing contaminants through heater/vacuum wells. Heating occurs by heat conduction through the soil. At high temperatures, even relatively low volatility contaminants can be vaporized, removed by vacuum and treated with an on-site recovery system. The main objective of this research was to design and test a laboratory apparatus scaled to a typical ISTD field site and to use it to conduct experiments that could be used to aid in the validation of the STARS numerical simulator. A dimensional analysis was done on the governing energy balance equation to determine the most important scaling groups for the ISTD process so the laboratory experiments could be scaled up to the field. The laboratory apparatus was modeled after a symmetry element of the hexagonal field pattern and a triangular glass prism was constructed for heated sandpack experiments. Temperature data was measured in dry sand, sand partially saturated with water, and sand with both water and PCE added to it. The apparatus was made of glass so that the behavior of the PCE contaminant could be observed when the sand was heated. / text
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Transport mechanisms in nanoscale amorphous solid water filmsMcClure, Sean Michael 28 August 2008 (has links)
Not available / text
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Temperature programmed desorption of graphene oxide under ultra-high vacuum /Field, Daniel Alexander, January 1900 (has links)
Thesis (M.S.)--Texas State University--San Marcos, 2008. / Vita. Includes bibliographical references (leaves 61-63). Also available on microfilm.
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Temperature programmed desorption study of dodecanethiol self-assembled monolayers on Ag /Nava, Simona Rieman, January 1900 (has links)
Thesis (M.S.)--Texas State University--San Marcos, 2009. / Vita. Appendices: leaves 38-39. Includes bibliographical references (leaves 40-41). Also available on microfilm.
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