Download e-book for iPad: Aerothermodynamics of Gas Turbine and Rocket Propulsion by G. Oates

By G. Oates

ISBN-10: 1563472414

ISBN-13: 9781563472411

ISBN-10: 1601192223

ISBN-13: 9781601192226

This publication on fuel turbine expertise has been a best-seller because it was once first released. It now contains a accomplished set of software program courses that supplement the textual content with difficulties and layout analyses. software program issues integrated are surroundings courses, quasi-one-dimensional stream courses (ideal constant-area warmth interplay, adiabatic constant-area stream with friction, rocket nozzle functionality, general surprise waves, indirect surprise waves), fuel turbine courses (engine cycle research and engine off-design performance), and rocket combustion courses (Tc and computer given, Hc and computer given, isentropic expansion).
- information and data showing during this publication are for informational reasons purely. AIAA and the writer aren't liable for any damage or harm due to use or reliance, nor do AIAA and the writer warrant that use or reliance might be loose from privately owned rights.

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Additional info for Aerothermodynamics of Gas Turbine and Rocket Propulsion

Example text

However, turbomachinery problems most often involve gases that may be considered perfect. 12 General Relationships between Properties An expression for a differential change in entropy, with the entropy considered to be a function of temperature and specific volume, is Y l d~ ds = (~-~)vdT+ (3v]T dT+,( idv 28 GAS TURBINE AND ROCKET PROPULSION which, with Eqs. 30) Similarly, the entropy is considered to be a function of temperature and pressure to give Os +l o, l ds=((-~p)rdp-(~_sh)" dT ,Op]r dp which, with Eqs.

41) It should be noted from Eq. 39) that when a gas is in a regime where dissociation is occurring, it is not, strictly speaking, a perfect gas. This is because dissociation changes the value of M and hence of R. However, if no dissociation occurs but substantial vibrational excitation occurs, then the gas would be perfect, but not calorically perfect. The behavior of a perfect gas may be illuminated by applying the relationships of Sec. 12. Thus, with Eq. 38) and Eqs. 43) hence, Cp is a function of temperature only.

Finally, modern compressors are equipped with "multiple spools" such that portions of the compressors are driven by their own separate portions of the turbine. ) tends to adjust its speed better to the then present axial velocity. Problems of scale are to be found when larger engines are scaled down for use in smaller aircraft. Tip clearance problems will obviously become greater, and the high-pressure blading can become extremely small. For this reason, it is often advantageous to employ a centrifugal compressor as a final stage, rather than the equivalent several stages of an axial compressor.

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Aerothermodynamics of Gas Turbine and Rocket Propulsion by G. Oates


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