Planar laser-induced fluorescence temperature measurements in free jet flows with vibrational nonequilibrium

Author(s):  
J. PALMER ◽  
R. HANSON
AIAA Journal ◽  
2000 ◽  
Vol 38 (9) ◽  
pp. 1769-1772 ◽  
Author(s):  
P. C. Palma ◽  
S. G. Mallinson ◽  
S. B. O’Byrne ◽  
P. M. Danehy ◽  
R. Hillier

Author(s):  
Sara Seitz ◽  
Lesley M. Wright

Abstract Two-color, toluene-based, planar laser-induced fluorescence (PLIF) is utilized to characterize the thermal structure of a turbulent, free jet. The PLIF technique has been used to measure concentration gradients for combustion applications, but its use to quantify thermal gradients is limited. To validate the method, compressed air is seeded with toluene particles. The seeded airflow is heated to temperatures varying from 300 to 375 K, and the heated jet exits a 1.27-cm diameter orifice into quiescent, room temperature air. The jet Reynolds number is varied from 5000 to 15,000. As the jet exits the orifice, the toluene particles fluorescence across a 266 nm laser light sheet which ultimately provides a two-dimensional temperature distribution of the free jet. The rigorous calibration procedure for the PLIF technique is described along with the seeding nuances needed to quantify the thermal structure of the jets. The PLIF technique has been demonstrated for this fundamental flow field, and it has proven to be applicable to more complex heat transfer and cooling applications. Furthermore, the time-averaged temperature distributions obtained in this investigation can be used in the validation of turbulent computational fluid dynamics (CFD) solvers.


Author(s):  
Sara Seitz ◽  
Lesley M. Wright

Abstract Two-color, toluene based, planar laser induced fluorescence (PLIF) is utilized to characterize the thermal structure of a turbulent, free jet. The PLIF technique has been used to measure concentration gradients for combustion applications, but its use to quantify thermal gradients is limited. To validate the method, compressed air is seeded with toluene particles. The seeded airflow is heated to temperatures varying from 300–375 K, and the heated jet exits a 1.27-cm diameter orifice into quiescent, room temperature air. The jet Reynolds number is varied from 5,000 to 15,000. As the jet exits the orifice, the toluene particles fluorescence across a 266 nm laser light sheet which ultimately provides a two-dimensional temperature distribution of the free jet. The rigorous calibration procedure for the PLIF technique is described along with the seeding nuisances needed to quantify the thermal structure of the jets. The PLIF technique has been demonstrated for this fundamental flow field, and it has proven to be applicable to more complex heat transfer and cooling applications. Furthermore, the time averaged temperature distributions obtained in this investigation can be used in the validation of turbulent CFD solvers.


AIAA Journal ◽  
2000 ◽  
Vol 38 ◽  
pp. 1769-1772
Author(s):  
P. C. Palma ◽  
S. G. Mallinson ◽  
S. B. O'Byrne ◽  
P. M. Danehy ◽  
R. Hiller

2004 ◽  
Vol 127 (4) ◽  
pp. 724-739 ◽  
Author(s):  
Paul O. Hedman ◽  
Thomas H. Fletcher ◽  
Daniel V. Flores ◽  
Stewart G. Graham ◽  
Jason K. Haslam ◽  
...  

Instantaneous planar laser induced fluorescence (PLIF) images of OH, simultaneous axial/radial and axial/tangential velocity measurements with an LDA (laser Doppler anemometer), and instantaneous gas temperature measurements using a coherent anti-Stokes Raman spectrometer (CARS) were obtained in a pre-mixed, swirl-stabilized laboratory-scale combustor, fired with natural gas. Four operating conditions were examined (two swirl conditions and equivalence ratios of 0.80 and 0.65). The instantaneous PLIF images of OH illustrate the chaotic nature of the turbulent flame eddies. Mean and standard deviations of each variable were measured at different locations in the flame, along with probability density functions. Stability of the flame at each condition is related to measurements in the central and side recirculation zones.


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