Table 6 Comparison of time-averaged mixing coefficients under stationary conditions

R-CFLF

\(\bar {v}^{1}=0.219662\)

\(\bar {v}^{2}=0.329039\)

\(\bar {v}^{3}=0.224948\)

\(\bar {v}^{4}=0.226642\)

D-CFLF

\(\bar {v}^{1}_{1}=0.250000\)

\(\bar {v}^{2}_{1}=0.250000\)

\(\bar {v}^{3}_{1}=0.250000\)

\(\bar {v}^{4}_{1}=0.250000\)

\(\bar {v}^{1}_{2}=0.260383\)

\(\bar {v}^{2}_{2}=0.245273\)

\(\bar {v}^{3}_{2}=0.243011\)

\(\bar {v}^{4}_{2}=0.248331\)

\(\bar {v}^{1}_{3}=0.260950\)

\(\bar {v}^{2}_{3}=0.238969\)

\(\bar {v}^{3}_{3}=0.240371\)

\(\bar {v}^{4}_{3}=0.256708\)

\(\bar {v}^{1}_{4}=0.259955\)

\(\bar {v}^{2}_{4}=0.238969\)

\(\bar {v}^{3}_{4}=0.240596\)

\(\bar {v}^{4}_{4}=0.259483\)

\(\bar {v}^{1}_{5}=0.259482\)

\(\bar {v}^{2}_{5}=0.235899\)

\(\bar {v}^{3}_{5}=0.240934\)

\(\bar {v}^{4}_{5}=0.260747\)

\(\bar {v}^{1}_{6}=0.258075\)

\(\bar {v}^{2}_{6}=0.235125\)

\(\bar {v}^{3}_{6}=0.241462\)

\(\bar {v}^{4}_{6}=0.262336\)

\(\bar {v}^{1}_{7}=0.256902\)

\(\bar {v}^{2}_{7}=0.234466\)

\(\bar {v}^{3}_{7}=0.242221\)

\(\bar {v}^{4}_{7}=0.263409\)

\(\bar {v}^{1}_{8}=0.307697\)

\(\bar {v}^{2}_{8}=0.137990\)

\(\bar {v}^{3}_{8}=0.267800\)

\(\bar {v}^{4}_{8}=0.283511\)

\(\bar {v}^{1}_{9}=0.300305\)

\(\bar {v}^{2}_{9}=0.146743\)

\(\bar {v}^{3}_{9}=0.267666\)

\(\bar {v}^{4}_{9}=0.282285\)

\(\bar {v}^{1}_{10}=0.294155\)

\(\bar {v}^{2}_{10}=0.155295\)

\(\bar {v}^{3}_{10}=0.267576\)

\(\bar {v}^{4}_{10}=0.279972\)

\(\bar {v}^{1}_{11}=0.287647\)

\(\bar {v}^{2}_{11}=0.167800\)

\(\bar {v}^{3}_{11}=0.266095\)

\(\bar {v}^{4}_{11}=0.275457\)

\(\bar {v}^{1}_{12}=0.283007\)

\(\bar {v}^{2}_{12}=0.180514\)

\(\bar {v}^{3}_{12}=0.263361\)

\(\bar {v}^{4}_{12}=0.270116\)

M-CLMS

\(\bar {v}^{1}=0.194679\)

\(\bar {v}^{2}=0.430737\)

\(\bar {v}^{3}=0.185233\)

\(\bar {v}^{4}=0.186599\)

D-CLMS

\(\bar {v}^{1}_{1}=0.439073\)

\(\bar {v}^{2}_{1}=0.560926\)

\(\bar {v}^{1}_{2}=0.439087\)

\(\bar {v}^{2}_{2}=0.560991\)

\(\bar {v}^{1}_{3}=0.438953\)

\(\bar {v}^{2}_{3}=0.561046\)

\(\bar {v}^{1}_{4}=0.438959\)

\(\bar {v}^{2}_{4}=0.560403\)

\(\bar {v}^{1}_{5}=0.438893\)

\(\bar {v}^{2}_{5}=0.561116\)

\(\bar {v}^{1}_{6}=0.439248\)

\(\bar {v}^{2}_{6}=0.560751\)

\(\bar {v}^{1}_{7}=0.437971\)

\(\bar {v}^{2}_{7}=0.562028\)

\(\bar {v}^{1}_{8}=0.436686\)

\(\bar {v}^{2}_{6}=0.563313\)

\(\bar {v}^{1}_{9}=0.437216\)

\(\bar {v}^{2}_{9}=0.562783\)

\(\bar {v}^{1}_{10}=0.436428\)

\(\bar {v}^{2}_{10}=0.563471\)

\(\bar {v}^{1}_{11}=0.437432\)

\(\bar {v}^{2}_{11}=0.562567\)

\(\bar {v}^{1}_{12}=0.436643\)

\(\bar {v}^{2}_{12}=0.563356\)