Table 3: Results of the parameter study about the initial flame geometry. The last column states if the ignition conditions of a core detonation have been reached.
Model $t/{\rm s}$ $T_{\rm 9,~max}$ $\rho_{\rm 8,~max}$ Core ignition
s3.60A_2dq_256 0.627 9.09 6.14 yes
s4.10A_2dq_256 0.575 10.2 7.37 yes
s5.00A_2dq_256 0.609 12.1 9.05 yes
r4.24A_2dq_256 0.699 5.62 1.54 yes
r5.00A_2dq_256 0.718 6.00 1.69 yes
z4.24A_2dq_256 0.989 3.27 1.03 no
z5.00A_2dq_256 1.03 3.20 0.981 no
b1A_2dq_256 0.767 4.43 1.32 yes
b2A_2dq_256 0.678 8.61 4.85 yes
b3A_2dq_256 0.674 7.94 4.57 yes
b5iA_2dq_256 0.629 9.53 6.68 yes
b5iiA_2dq_256 0.648 9.00 6.13 yes
b5iiiA_2dq_256 0.648 9.03 6.37 yes
z4.24A_2d_256 1.08 8.53 4.52 yes
s4.30B_2dq_256 0.791 6.82 4.69 yes
s4.80B_2dq_256 0.745 8.17 5.99 yes
r4.50B_2dq_256 0.892 3.96 1.15 no
r5.00B_2dq_256 0.885 4.49 1.23 yes
z4.50B_2dq_256 1.21 2.42 0.808 no
z5.00B_2dq_256 1.24 2.39 0.768 no
b2B_2dq_256 0.855 6.72 4.34 yes
b5iB_2dq_256 0.806 7.63 5.47 yes
z4.50B_2d_256 1.31 6.50 3.38 yes

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