A lab-scale cold flow model reactor to investigate near-wall particle segregation relevant to entrained-flow slagging coal gasifiers

作者：Troiano Maurizio; Carbone Ramona; Montagnaro Fabio; Salatino Piero^*; Solimene Roberto

来源：Fuel, 2014, 117: 1267-1273.

DOI：10.1016/j.fuel.2013.06.026

• Slagging gasifiers
• Particle-wall interaction
• Segregation
• Wax

This paper reports on preliminary results of an experimental investigation aimed at the development of a phenomenological model of the fate of coal/ash particles in entrained-flow slagging coal gasifiers. The study specifically addresses the interaction between the lean-dispersed particle phase and the reactor walls, and the establishment of a particle segregated phase in the near-wall region of the gasifier. Better mechanistic understanding of particle-wall interaction patterns in entrained-flow gasifiers is pursued using the tool of physical modeling. To this end a lab-scale cold flow reactor (0.04 m-ID) has been designed and set up, where molten wax is air-atomized (droplets of 50-100 mu m size) into a mainstream of air to simulate the near-wall fate of char/ash particles in a real hot environment. Preliminary characterization of the hydrodynamics of the lean-dispersed phase, of its interaction with the wall, of the buildup of the liquid wall layer has been accomplished with a focus on the "sticky wall-sticky particle'' sub-regime.
The particle deposition rate at the wall and the partitioning of wax droplets between the lean-dispersed phase and the wall liquid layer have been assessed under a range of operating conditions. Temperatures of the atomized wax, of the mainstream air and of the reactor wall have been set in a range of values (120-155 degrees C) at which the wax was fluid. Experiments with wax feeding rate of 0.2 g s(-1) and flow rate of atomizing air in the order of 0.30 m(3) h(-1) demonstrated that the fractional mass of wax in the dispersed phase decreased from 91% to 12% as the reactor length increased from 0.03 m to 0.27 m. The velocity of the descending wall liquid layer, whose thickness was in the order of 0.2 mm, ranged between 3 mm s(-1) and 6 mm s(-1). The effects of the flow rate of atomization air and of the nozzle temperature were limited.

• 出版日期2014-1