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Rowan-Gollan-PhD-Thesis - Mechanical Engineering - University of ...

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Chapter 6<br />

Applications<br />

In Chapters 4 and 5 the development work on models for thermochemical nonequilibrium was<br />

presented; this chapter discusses the applications <strong>of</strong> that development work, that is, the range<br />

<strong>of</strong> calculations which make use <strong>of</strong> the models for thermochemical nonequilibrium. At the very<br />

beginning <strong>of</strong> the discussion (Section 1.4), it was stated that there were two direct benefits <strong>of</strong><br />

this thesis work: a longer term benefit, providing a foundation for modelling <strong>of</strong> radiating flow<br />

fields; and an immediate benefit, the simulation <strong>of</strong> flows in impulse facilities. That immediate<br />

benefit is the subject <strong>of</strong> this chapter: two “demonstration” calculations <strong>of</strong> expansion tube flows<br />

are presented as examples <strong>of</strong> application <strong>of</strong> this work.<br />

The work on modelling chemical nonequilibrium — the finite-rate chemistry model — has<br />

had considerable use during the course <strong>of</strong> this project. At the beginning <strong>of</strong> this work, gen-<br />

eral codes for computing the influence <strong>of</strong> chemistry in compressible flows were not widely<br />

available or easily obtainable. 1 There were implementations <strong>of</strong> specific models, such as mod-<br />

els for dissociating nitrogen or reacting air, but not generalised implementations to treat an<br />

arbitrary mixture <strong>of</strong> gases. Yet over the years, the interest in reacting gases in the hyper-<br />

sonic regime has continued to grow, now including mixtures containing carbon dioxide (the<br />

atmospheres <strong>of</strong> Mars and Venus); hydrogen and helium (the Jovian atmosphere); and methane<br />

and nitrogen (the Titan atmosphere). Thus a general chemistry code with easy user input was<br />

a desirable addition to the local modelling capabilities. The implementation <strong>of</strong> a finite-rate<br />

chemistry module as part <strong>of</strong> this work has been used in a number <strong>of</strong> calculations over the<br />

course <strong>of</strong> this project: one-dimensional simulations <strong>of</strong> expansion tube flows (Stewart [172] and<br />

Chiu [173]); two-dimensional (axisymmetric) simulations <strong>of</strong> expansion tube flows (Chiu [173],<br />

Jacobs et al. [174], Scott [175], Brandis et al. [176] and <strong>Gollan</strong> et al. [177]); in the analysis <strong>of</strong><br />

results for radiation measurements on blunt bodies (Capra [178]); and as part <strong>of</strong> studies on<br />

modelling turbulent boundary layers with heat release (Denman [179]).<br />

More recently, the general thermochemical nonequilibrium model (finite-rate chemistry<br />

with vibrational nonequilibrium) has been used in calculations <strong>of</strong> carbon dioxide flows in an<br />

expansion tube facility (Potter et al. (2007) [180] and Potter et al. (2008) [181]). These are the<br />

first CFD calculations to quantitatively assess the extent <strong>of</strong> vibrational nonequilibrium in the<br />

test gas <strong>of</strong> an expansion tube flow.<br />

1 This statement is still true at the time <strong>of</strong> writing.<br />

113

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