6. Conclusions

  1. NO is formed rapidly from both fuels at all equivalence ratios in the first 150 mm from the atomiser nozzle by means of the fuel-NO mechanism. The amounts of fuel-N converted to NO were dependent on the stoichiometry and the furnace wall temperature. Although N2O was also observed, the role of the prompt-NO mechanism was deemed to be of minor relevance.

  2. As a result of the rapid formation of NO, significant amounts of NO2 are also formed at short distances in stoichiometric and fuel-rich conditions. NO2 is thought to be formed by means of the HO2 and RO2 mechanisms.

  3. The extent of NO formation at longer distances depends mainly on the stoichiometry of the combustion system and the furnace wall (flame) temperature. Large amounts of NO are formed in fuel-lean conditions. The conversion of fuel-N into NO is greatest under these conditions. The fuel with the larger fuel-N content yields greater concentrations of NO, whereas conversion is higher for the fuel with lower fuel-N content. Raising the furnace wall temperature increases the conversion of fuel-N into NO.

  4. Although significant amounts are formed, NO and NO2 are emitted in small amounts in stoichiometric conditions. The concentrations of both species are reduced at relatively long distances from the atomiser nozzle.

  5. Small amounts of NO are emitted at j = 1.200. NO2 constitutes the largest nitrogenous emission in these conditions. NO2 is thought to be formed by the reaction of NO with hydroperoxyl radicals (RO2) that stem from unburned hydrocarbons. Although further work is needed at 1,200 °C furnace wall temperature, the conversion of fuel-N into NO2 does not show a dependence on the furnace wall temperature nor the fuel-N content.

  6. No significant amounts of thermal-NO were found even in the most favourable conditions, ie 1,200 °C furnace wall temperature and j = 0.714.

  7. The measured concentrations of SO2 rise with the equivalence ratio due to the reduced volume of combustion gases associated with high equivalence ratios.

  8. In fuel-lean conditions the formation and emission of SO2 seems independent from the furnace wall temperature.

  9. In some cases the fuel-S conversion is slightly lower at j = 0.714 than at j = 0.833, which may indicate the formation of SO3.

  10. At stoichiometric and fuel-rich equivalence ratios the formation of SO2 reaches a maximum and decreases subsequently. Larger decreases were found at the higher furnace wall temperatures. SO2 is reduced into species such as COS, SO and H2S in low concentrations of oxygen.

Previous
Previous
Table of Contents
Table of Contents
Next
Next

Pollutant formation and interaction in the combustion of heavy liquid fuels
Luis Javier Molero de Blas, PhD thesis, University of London, 1998
© Luis Javier Molero de Blas