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Chapter 5<br />

Fluctuating<br />

vel f (u or v)<br />

U=lm/s mean (f 2)<br />

U=0.64 mean (f2 )<br />

max E (X/H=1.25)<br />

mean (f2 )<br />

max (f2 )<br />

max (f)<br />

u-Johns<br />

-1991<br />

E<br />

0.642 E<br />

0.018<br />

0.007<br />

0.010<br />

0.102<br />

v-Johns<br />

-1991<br />

0.35E<br />

0.35(0.642 )E<br />

0.018<br />

0.003<br />

0.004<br />

0.063<br />

u,v-Nak.<br />

-1987<br />

{ mean u,v }<br />

{(0. 18*0. 64)=0. 115}<br />

0.013<br />

0.019<br />

0.137<br />

Figure 18. Table <strong>of</strong> maximum fluctuating velocities u,v=f. Johns<br />

(1991) prescribes u=E and v=0.35E where E is the turbulence energy<br />

density in (m/s) 2 which has a peak value 0.018. We then assume a<br />

sinusoidal distribution for the fluctuating parameters which classically<br />

gives (f 2)max = l^H^mean. Data from Nakagawa & Nezu (1987)<br />

gives u,v directly.

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