E. J. Skudrzyk 205 
The simple form of the Kolmogorov law applies for the equilibrium range 
of the phenomenon, which, by definition, is unaffected by the mechanism of the 
redistribution and the energy dissipation [4]. If the fluid is not infinitely ex- 
tended—if, for instance, the receiver is at a finite distance from the water 
surface—an additional parameter is available to describe the phenomenon. In 
altering the Kolmogorov law for this case, let us be guided by the experimental 
results. 
10°9 
25 FTX DepTH 
-10 
10 9 FT 
170 FT (B) 
120 FT 
170 FT (A) 
iol! 
= 
Co, 
Ss 
oO 
iy 
= la 
2 10 
's 
tad 
LP) 
oS 
oa 
= 
5 COMPUTED FOR A KOLMOGOROV-TYPE 
S193 POWER LAW ASSUMED AS 2 FOR A 
50 FT SPECTRUM CUT OFF AT THE LOWER 
WAVE -NUMBER END 
10° “0,001 001 Ol l 10 100 
PATCH DIAMETER X + 
Fig. 12.7. Curves of Fig. 12.6 represented to a normalized scale. 
