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author | Joshua Drake <Joshua.Ellis.Drake@gmail.com> | 2024-10-26 22:23:54 -0500 |
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committer | Joshua Drake <Joshua.Ellis.Drake@gmail.com> | 2024-10-26 22:23:54 -0500 |
commit | d21893d7b92a64b5b1f8f7ffe6fe3fffbc4ced66 (patch) | |
tree | ce921e2b164272bc7aa9fe3f561dc1bba158284a | |
parent | f97f266c8502a03b483b62ba1fea390923127133 (diff) |
Finished section on turbine engine description.
-rw-r--r-- | background.tex | 6 | ||||
-rw-r--r-- | dissertation_main.aux | 53 | ||||
-rw-r--r-- | dissertation_main.lof | 6 | ||||
-rw-r--r-- | dissertation_main.log | 55 | ||||
-rw-r--r-- | dissertation_main.pdf | bin | 2902921 -> 2905539 bytes | |||
-rw-r--r-- | dissertation_main.toc | 36 | ||||
-rw-r--r-- | missfont.log | 10 |
7 files changed, 94 insertions, 72 deletions
diff --git a/background.tex b/background.tex index 8c605df..dbba796 100644 --- a/background.tex +++ b/background.tex @@ -18,6 +18,12 @@ A cursory understanding of turbine engines is necessarry to contextualize this w The Inlet is the first section of the gas turbine engine, denoted by station numbers 0-2, and its operation and design are described in terms of the efficiency of the compression process, the external drag of the inlet, and the mass flow into the inlet. \cite{EoPGTR2} Inlet design is most heavily influenced by whether the air entering it is subsonic or supersonic. Subsonic inlet design is simple, and typically involves selecting an operating velocity at which air compression is most efficient at the expense of performance at other velocities. Supersonic inlets must take the shockwaves endemic to supersonic flow into account for optimal performace. This is accomplished by adjusting inlet geometry to reduce flow velocity while adding as little weight to the system as possible. Variable inlet geometry will allow for increased efficiency accross many velocities. \par Compressors, denoted by station numbers 2-3, increase the pressure of the flow obtained by the inlet such that the combustion and exhaust processes can be conducted more efficiently. Increasing the pressure of an initial volume of air results in the reduction of its volume, allowing for the combustion of the air/fuel mixture to occur within a smaller volume than it would otherwise. Turbine engines most commonly employ centrifugal or axial compressors. Figure \ref{EoPturbojet} appropriately depicts an axial compressor in the makeup of the common turbine engine by virtue of their superiority. However, centrifugal compressors find use in smaller, less expensive engines due to their simple design. Centrifugal compressors are comprised of an impeller, which serves to increase flow velocity through rotation; a diffuser, which decreases the velocity of the flow thereby increasing its pressure; and a manifold which directs the compressed air into the combustor. Axial compressors are made of a series of stator vanes and rotor blades that are concentric to the axis of rotation. Each set of these stators and rotors is referred to as a stage. ''The flow path in an axial compressor decreases in cross-sectional area in the direction of flow." \cite{EoPturbojet} Each stage of the compressor results in an increase in air density. Thus, multiple stages are used in the design of high compression ratio turbine engines. Many turbines, including that which is depicted in figure \ref{EoPturbojet}, are equiped with dual axial compressors. Dual axial compressors allow for a more uniform loading of compressor stages, as well as for improved flexibility in the balancing between the initial and later stages. +\par +The combustor, as illustrated in figure \ref{EoPturbojet} between station numbers 3 and 4, is responsible for burning a mixture of compressed air and fuel and delivering the resulting exhaust gases to the turbine stage at a consistent temperature. The air that enters the combustion chamber is characterized as either primary air, meaning that it mixes with fuel and burns, and secondary air, which cools the extremity of the combustion chamber as well as exhaust gases to ensure optimal temperature within the turbine. The air to fuel ratio varies from 30 to 60 parts of air to one part of fuel by weight, depending on the design and type of engine. \cite{EoPGTR2} The types of combustion chambers found within tubine engines are can, which consist of multiple circular chambers arranged in a similarly circular fashion; annular, a large single chamber design around a center casing; and can-annular, a combination of the previous architectures in which can chambers are organized within an annular cavity. +\par +The turbine section of the engine, denoted by station numbers 4 through 5, is responsible for taking the energy generated in the combustion chamber and turning it into shaft horsepower to drive the compressor stages and external loads. Almost 75 percent of the energy generated from the combustion process is required to drive the compressor alone.\cite{EoPGTR2}The axial-flow turbine is similar to the axial compressor, and is likewise comprised of a series of stages of rotors and stators. However, the turbine has the opposite effect of the compressor: it turns the energy contained within flow into shaft rotation. The stage quantity of the turbine section of a given turbine engine is typically lower than that of its compressor, as the flow is expanding rather than compressing. Axial turbines are either impulse design, which maintain flow velocity across their rotor and decrease pressure across their stator, whereas reaction stages increase pressure across their rotor blades and direct flow within their stator. Most turbines use a combination of these two stage designs, and must be dual or split commensurately with the design of the compressor. +\par +The final stage of the turbine engine, the exhaust nozzle, denoted by station numbers 5 through 9, is responsible for increasing the velocity of the exhaust gas before discharge such that ample thrust can be generated by the engine. Ideally, the exit pressure of the flow leaving the nozzle should equal ambient pressure, otherwise the engine will operate less efficiently than it is capable. Nozzles are typically either convergent, or convergent-divergent, meaning a convergent duct followed by a divergent duct. Simple convergent ducts are used in the case where the ratio of turbine exit pressure to nozzle exit pressure is less than 2. The convergent-divergent duct is employed in instances where this nozzle pressure ratio is in excess of 2. Such ducts incorporate more sophisticated aerodynamic features and variable geometry in certain applications.\cite{EoPGTR2} Gas turbine engines fall into four categories: turbofan, turboprop, and turboshaft, and turbojet. Turbojets make use of a propelling nozzle to create thrust by allowing the heated exhaust created by a gas turbine to expand. \cite{nasa_turbojet} diff --git a/dissertation_main.aux b/dissertation_main.aux index 078bca9..fdcf281 100644 --- a/dissertation_main.aux +++ b/dissertation_main.aux @@ -12,35 +12,38 @@ \@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces Ideal Turbojet with station numbering}}{2}{}\protected@file@percent } \newlabel{EoPturbojet}{{1}{2}{}{}{}} \citation{EoPturbojet} +\citation{EoPGTR2} +\citation{EoPGTR2} +\citation{EoPGTR2} \citation{nasa_turbojet} -\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces PBS TP100 Cutaway}}{4}{}\protected@file@percent } -\newlabel{tp100cutaway}{{2}{4}{}{}{}} -\@writefile{toc}{\contentsline {section}{\numberline {2.2}Generator Theory}{4}{}\protected@file@percent } -\@writefile{toc}{\contentsline {section}{\numberline {2.3}Battery Theory}{4}{}\protected@file@percent } -\@writefile{toc}{\contentsline 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7960b8e..c13dc68 100644 --- a/dissertation_main.lof +++ b/dissertation_main.lof @@ -1,9 +1,9 @@ \addvspace {10\p@ } \addvspace {10\p@ } \contentsline {figure}{\numberline {1}{\ignorespaces Ideal Turbojet with station numbering}}{2}{}% -\contentsline {figure}{\numberline {2}{\ignorespaces PBS TP100 Cutaway}}{4}{}% -\contentsline {figure}{\numberline {3}{\ignorespaces Turboelectric Architectures}}{4}{}% -\contentsline {figure}{\numberline {4}{\ignorespaces Parallel Turboelectric Design}}{5}{}% +\contentsline {figure}{\numberline {2}{\ignorespaces PBS TP100 Cutaway}}{5}{}% +\contentsline {figure}{\numberline {3}{\ignorespaces Turboelectric Architectures}}{6}{}% +\contentsline {figure}{\numberline {4}{\ignorespaces Parallel Turboelectric Design}}{6}{}% \addvspace {10\p@ } \addvspace {10\p@ } \addvspace {10\p@ } diff --git a/dissertation_main.log b/dissertation_main.log index f58473b..8f302ad 100644 --- a/dissertation_main.log +++ b/dissertation_main.log @@ -1,4 +1,4 @@ -This is pdfTeX, 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PDF statistics: - 86 PDF objects out of 1000 (max. 8388607) - 51 compressed objects within 1 object stream + 90 PDF objects out of 1000 (max. 8388607) + 54 compressed objects within 1 object stream 0 named destinations out of 1000 (max. 500000) 21 words of extra memory for PDF output out of 10000 (max. 10000000) diff --git a/dissertation_main.pdf b/dissertation_main.pdf Binary files differindex fc193fa..8549122 100644 --- a/dissertation_main.pdf +++ b/dissertation_main.pdf diff --git a/dissertation_main.toc b/dissertation_main.toc index 4b09922..e7650fa 100644 --- a/dissertation_main.toc +++ b/dissertation_main.toc @@ -2,21 +2,21 @@ \contentsline {chapter}{\numberline {I}INTRODUCTION}{1}{}% \contentsline {chapter}{\numberline {II}BACKGROUND}{2}{}% \contentsline {section}{\numberline {2.1}Turbine Engines}{2}{}% -\contentsline {section}{\numberline {2.2}Generator Theory}{4}{}% -\contentsline {section}{\numberline {2.3}Battery Theory}{4}{}% -\contentsline {section}{\numberline {2.4}Turboelectric Theory}{4}{}% -\contentsline {section}{\numberline {2.5}Previous Work}{4}{}% -\contentsline {chapter}{\numberline {III}METHODOLOGY}{6}{}% -\contentsline {section}{\numberline {3.1}General Aircraft System}{6}{}% -\contentsline {section}{\numberline {3.2}Configuration One}{6}{}% -\contentsline {subsection}{\numberline {3.2.1}Data Acquisition}{6}{}% -\contentsline {subsection}{\numberline {3.2.2}Experimental Procedure}{6}{}% -\contentsline {section}{\numberline {3.3}Configuration Two}{6}{}% -\contentsline {subsection}{\numberline {3.3.1}Data Acquisition}{6}{}% -\contentsline {subsection}{\numberline {3.3.2}Experimental Procedure}{6}{}% -\contentsline {chapter}{\numberline {IV}RESULTS}{7}{}% -\contentsline {section}{\numberline {4.1}Configuration One}{7}{}% -\contentsline {section}{\numberline {4.2}Configuration Two}{7}{}% -\contentsline {chapter}{\numberline {V}CONCLUSION, RECOMMENDATIONS, AND FUTURE WORK}{8}{}% -\contentsline {chapter}{REFERENCES}{9}{}% -\contentsline {chapter}{APPENDICES}{10}{}% +\contentsline {section}{\numberline {2.2}Generator Theory}{5}{}% +\contentsline {section}{\numberline {2.3}Battery Theory}{5}{}% +\contentsline {section}{\numberline {2.4}Turboelectric Theory}{5}{}% +\contentsline {section}{\numberline {2.5}Previous Work}{5}{}% +\contentsline {chapter}{\numberline {III}METHODOLOGY}{7}{}% +\contentsline {section}{\numberline {3.1}General Aircraft System}{7}{}% +\contentsline {section}{\numberline {3.2}Configuration One}{7}{}% +\contentsline {subsection}{\numberline {3.2.1}Data Acquisition}{7}{}% +\contentsline {subsection}{\numberline {3.2.2}Experimental Procedure}{7}{}% +\contentsline {section}{\numberline {3.3}Configuration Two}{7}{}% +\contentsline {subsection}{\numberline {3.3.1}Data Acquisition}{7}{}% +\contentsline {subsection}{\numberline {3.3.2}Experimental Procedure}{7}{}% +\contentsline {chapter}{\numberline {IV}RESULTS}{8}{}% +\contentsline {section}{\numberline {4.1}Configuration One}{8}{}% +\contentsline {section}{\numberline {4.2}Configuration Two}{8}{}% +\contentsline {chapter}{\numberline {V}CONCLUSION, RECOMMENDATIONS, AND FUTURE WORK}{9}{}% +\contentsline {chapter}{REFERENCES}{10}{}% +\contentsline {chapter}{APPENDICES}{11}{}% diff --git a/missfont.log b/missfont.log new file mode 100644 index 0000000..8cbaef8 --- /dev/null +++ b/missfont.log @@ -0,0 +1,10 @@ +mktextfm rsfs10 +mktextfm rsfs10 +mktextfm rsfs10 +mktextfm rsfs5 +mktextfm rsfs10 +mktextfm rsfs10 +mktextfm rsfs5 +mktextfm rsfs10 +mktextfm rsfs10 +mktextfm rsfs5 |