Conventions
Directory h3_sma contains 164 result files (2.81MB). The file names are hXXYYYYY.sma, where XX is x/D (x=distance from nozzle, D=inner diameter of nozzle, i.e. 8 mm; at x/D=2.5 XX is set to 02) and YYYYY is the radial distance from the flame axis in 100th mm. YYYYY can also be negative. For example, r20-0150.sma contains the results of the measuring location x/D=20 and r=-1.5 mm. The measuring location is also given in the file header. At the top of each file the ensemble mean values and the Favre mean values and their RMS fluctuations, respectively, are given, followed by a listing of all single pulse results.
Directory h5_sma contains 99 result files (1.99MB). The file names are h5XXYYYYY.sma, where x and Y are the same as h3_sma.
Directory m2_sma contains 83 result files (1.84MB). The file names are m2XXYYYY.sma, where XX is x/D and YYYY is the radial distance from the flame axis in 1/10 mm. YYYY can also be negative.
Directories ma_sma, mb_sma, mc_sma, and md_sma contain 17, 18, 18, and 20 files, respectively (1.47MB). The file names are mZXXYYYY.sma, where Z is either A,B,C, or D, XX is x/D and YYYY is the radial distance from the flame axis in 1/10 mm. YYYY can also be negative.
Directories c1_sma, c2_sma, and c3_sma contain 71, 38, and 39 files, respectively (2.53MB). The file names are cZXXYYYY.sma, where Z is either 1, 2, or 3, XX is x/D and YYYY is the radial distance from the flame axis in 1/100 mm. YYYY can also be negative.
Directory v1_sma contains 94 files (2.85MB). The file names are vXXXYYYY.sma, where XXX is x/D; at x/D=2.5 XXX is set to 002) and YYYY is the radial distance from the flame axis in 1/10 mm. YYYY can also be negative. For example, r0050075.sma contains the results of the measuring location x/D=5 and r=7.5 mm. The measuring location is also given in the file header. At the top of each file the ensemble mean values and the Favre mean values and their RMS fluctuations, respectively, are given, followed by a listing of all single pulse results. To calculate the Favre means, the density was determined by using the Rayleigh temperature.