The point made by Professor Cumpsty concerning the results related to the variation of the weighting coefficients shown in Fig. 7 is well taken. We found that the figure’s legend was misplaced in the pamphlet paper; we have redrawn Fig. 7. If the stagnation pressure is approximated by pt=ps+1/2ρu2, the objective functions searched by the three sets of weighting coefficients shown in Fig. 7 are 
fh=minΔps+Δpt=minΔps+Δps+Δ1/2ρu2=min2Δps+Δ1/2ρu2
for α=1 and β=1, and 
fh=minΔps+3Δpt=minΔps+3Δp...
You do not currently have access to this content.