C C C BISSONNETTE-MELLOR HIGH REYNOLDS NUMBER TURBULENCE DATA C AT SEVERAL STATIONS (OMEGA=0) C C *THE TURBULENT VELOCITY MOMENTS ARE TABULATED IN FEET}/SEC}* R = 7.95E+04 OMEGA = .0 STATION NO1 STATION NO3 Y U2 W2 UW V2 UV VW U2 W2 UW V2 UV VW .015 NM NM NM NM NM NM NM NM NM NM NM NM .021 20.83 10.96 .45 NM NM NM NM NM NM NM NM NM .024 NM NM NM NM NM NM 26.46 12.17 .05 NM NM NM .025 NM NM NM NM NM NM NM NM NM NM NM NM 25 .040 NM NM NM 5.55 -5.44 .53 NM NM NM 8.04 -6.39 .69 .057 NM NM NM NM NM NM NM NM NM NM NM NM .063 18.74 10.16 .51 NM NM NM NM NM NM NM NM NM .066 NM NM NM NM NM NM 21.87 11.40 .47 NM NM NM .067 NM NM NM NM NM NM NM NM NM NM NM NM 22 .082 NM NM NM 5.56 -5.39 .17 NM NM NM 7.68 -5.99 .66 .098 NM NM NM NM NM NM NM NM NM NM NM NM .104 18.03 9.61 .33 NM NM NM NM NM NM NM NM NM .107 NM NM NM NM NM NM 19.93 10.21 .47 NM NM NM .108 NM NM NM NM NM NM NM NM NM NM NM NM 21 .123 NM NM NM 5.75 -4.98 .25 NM NM NM 6.92 -5.38 .29 .140 NM NM NM NM NM NM NM NM NM NM NM NM .146 16.88 9.24 .18 NM NM NM NM NM NM NM NM NM .149 NM NM NM NM NM NM 19.52 9.39 .74 NM NM NM .150 NM NM NM NM NM NM NM NM NM NM NM NM 20 .165 NM NM NM 6.05 -4.97 .29 NM NM NM 5.68 -4.91 .62 .182 NM NM NM NM NM NM NM NM NM NM NM NM .188 15.64 .955 .12 NM NM NM NM NM NM NM NM NM .191 NM NM NM NM NM NM 18.13 9.01 .61 NM NM NM .192 NM NM NM NM NM NM NM NM NM NM NM NM 18 .207 NM NM NM 5.47 -4.43 .05 NM NM NM 5.66 -4.13 .66 .223 NM NM NM NM NM NM NM NM NM NM NM NM .229 14.11 8.08 .30 NM NM NM NM NM NM NM NM NM .232 NM NM NM NM NM NM 16.45 7.64 .22 NM NM NM .233 NM NM NM NM NM NM NM NM NM NM NM NM 17 .248 NM NM NM 5.28 -4.05 -.19 NM NM NM 5.12 -4.09 .50 .249 NM NM NM NM NM NM NM NM NM NM NM NM .271 12.55 6.41 .31 NM NM NM NM NM NM NM NM NM .274 NM NM NM NM NM NM 14.87 7.24 .03 NM NM NM .275 NM NM NM NM NM NM NM NM NM NM NM NM 16 .290 NM NM NM 4.48 -3.62 .50 NM NM NM 5.04 -3.79 .35 .313 10.32 5.83 .09 NM NM NM NM NM NM NM NM NM .316 NM NM NM NM NM NM 12.94 6.08 .20 NM NM NM .332 NM NM NM 3.56 -2.56 .21 NM NM NM 4.28 -3.15 .13 .354 8.66 4.26 .03 NM NM NM NM NM NM NM NM NM .358 NM NM NM NM NM NM NM NM NM NM NM NM 12 .373 NM NM NM 3.19 -2.31 .11 NM NM NM 3.75 -2.85 .11 .399 NM NM NM NM NM NM 9.92 3.81 .12 NM NM NM .415 NM NM NM 1.99 -1.35 -.13 NM NM NM 3.06 -2.20 .41 .436 NM NM NM NM NM NM NM NM NM NM NM NM .437 4.75 2.37 .09 NM NM NM NM NM NM NM NM NM .442 NM NM NM NM NM NM NM NM NM NM NM NM 9 .457 NM NM NM 1.75 -1.30 .06 NM NM NM 2.63 -1.80 .00 .482 NM NM NM NM NM NM 6.11 2.75 .01 NM NM NM .498 NM NM NM 1.45 -.87 .03 NM NM NM NM NM NM .500 NM NM NM NM NM NM NM NM NM NM NM NM .521 2.29 1.22 .01 NM NM NM NM NM NM NM NM NM .525 NM NM NM NM NM NM NM NM NM NM NM NM 6 .540 NM NM NM 1.18 -.61 .07 NM NM NM 1.85 -1.11 .08 .566 NM NM NM NM NM NM 3.07 1.74 .05 NM NM NM .604 .99 .92 .01 NM NM NM NM NM NM NM NM NM .623 NM NM NM NM NM NM NM NM NM 1.10 -.59 .01 .649 NM NM NM NM NM NM 1.59 .88 .02 NM NM NM .650 NM NM NM NM NM NM NM NM NM NM NM NM 2 .665 NM NM NM NM NM NM NM NM NM NM NM NM .707 NM NM NM NM NM NM NM NM NM .66 -.25 .03 .729 .50 .53 .00 NM NM NM NM NM NM NM NM NM .744 NM NM NM NM NM NM .56 .62 .00 NM NM NM .748 NM NM NM NM NM NM NM NM NM NM NM NM .775 NM NM NM NM NM NM NM NM NM NM NM NM .790 NM NM NM NM NM NM NM NM NM NM NM NM .900 NM NM NM NM NM NM NM NM NM NM NM NM .915 NM NM NM NM NM NM NM NM NM NM NM NM .942 NM NM NM NM NM NM NM NM NM NM NM NM .957 NM NM NM NM NM NM NM NM NM NM NM NM