9th Aerospace Sciences Meeting 1971
DOI: 10.2514/6.1971-123
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A model for nitric oxide emission from aircraft gas turbine engines

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Cited by 36 publications
(13 citation statements)
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“…Consequently, a partially-stirred reactor (PaSR) model was developed in such a way that variations in gas composition, temperature and residence time, which influence directly the rates of pollutant formation, in particular NOx formation, are described statistically; however, only gross flow features at the reactor exit are predicted. Following 10,16 , in the PaSR model it is assumed that mixing is complete to a scale which is small compared with the combustor dimensions, but not on a molecular scale. Hence, within the zone there exists a number of well stirred eddies or fluid elements which have different residence times.…”
Section: Partially-stirred Reactor (Pasr) Modelmentioning
confidence: 99%
“…Consequently, a partially-stirred reactor (PaSR) model was developed in such a way that variations in gas composition, temperature and residence time, which influence directly the rates of pollutant formation, in particular NOx formation, are described statistically; however, only gross flow features at the reactor exit are predicted. Following 10,16 , in the PaSR model it is assumed that mixing is complete to a scale which is small compared with the combustor dimensions, but not on a molecular scale. Hence, within the zone there exists a number of well stirred eddies or fluid elements which have different residence times.…”
Section: Partially-stirred Reactor (Pasr) Modelmentioning
confidence: 99%
“…The first of these zones is a recirculation zone, modelled as a macromixed partially stirred reactor, following Fletcher and Heywood (1971). In this zone exist discrete fluid readily be seen from Figure 1 that equilibrium levels of carbon monoxide, indicated by a low value of Z, will be approached quite rapidly at most values of equivalence ratio at full power conditions.…”
Section: Basic Flame Modelmentioning
confidence: 99%
“…As discussed in Barnes and Mellor (1997), if the main fuel and air mixture is not homogeneous, then a distribution of equivalence ratios exists in the LP flame. Following Mik-us and Heywood (1971) and Fletcher and Heywood (1971), it is assumed that this equivalence 'The data were collected from a gas-fired, can-type, LP gas turbine combustor, Combustor A, at constant inlet temperature and pressure. See Barnes et al (1996) (1) when s approaches zero.…”
Section: = Constant I (2) Tonmentioning
confidence: 99%