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Seeding particles, particle image velocimetry

Melling, A. (1997). Tracer particles and seeding for particle image velocimetry, Meas. Sci. and Technol. 8(12), 1406-1416. [Pg.254]

On comparing the two flames, it is evident that the flow structure of the lean limit methane flame fundamentally differs from that of the limit propane one. In the flame coordinate system, the velocity field shows a stagnation zone in the central region of the methane flame bubble, just behind the flame front. In this region, the combustion products move upward with the flame and are not replaced by the new ones produced in the reaction zone. For methane, at the lean limit an accumulation of particle image velocimetry (PIV) seeding particles can be seen within the stagnation core, in... [Pg.17]

See other pages where Seeding particles, particle image velocimetry is mentioned: [Pg.1172]    [Pg.145]    [Pg.292]    [Pg.3]    [Pg.131]    [Pg.319]    [Pg.916]    [Pg.57]    [Pg.28]    [Pg.98]    [Pg.17]    [Pg.422]    [Pg.38]    [Pg.96]    [Pg.123]    [Pg.1260]    [Pg.2133]    [Pg.765]    [Pg.1300]    [Pg.203]    [Pg.237]    [Pg.1331]   
See also in sourсe #XX -- [ Pg.243 ]



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