F
fddy diRiwion. 5
n i d e l ot, 1x1
Entrainmcnt equation. 123
1ntr:iinnictit prmxhc. in un+tutok 1ocoand;irj
luyur. 115 121
Environmental conditions, dilliiliion and.
322 321
Culerian field
gcwriiiinn of. IS3 1%
rrhiilth of. I44 145
Fuleri;in tloa lield Eulcri:in-L,ieri~iiPiBii rclotionrhip. ti1
!urbukncc nicxicl. IhS IhX
Eulcrun-Lagrangitin turbulent ddfiiwn
probkiii. h2. (60 Ihl
C: u ler ian-l.sgwnylon 1 crt tw I-velwiiy
lulsrian +puLr-tiinc ct)rrclaticni, (or two\pOctr*. 422 423
d itncnsionul iiumcrmtliy gcncrated tlow.
I 5 0
IG
(iiadicnt transport. directicond con*trilint
in. 47 52
(iradenl transport upprinimattons. niathenwtical rntnctions leading to, 27-2Y
Ciradient transport models. limitationr of.
25 ..(4
W k ' a/so Transport mudel
doposition in. 377 379
Great Laltes, 4losa p.wdoharungu.r
t i
liitrmnnk uiialysis, in turbulent atmospheric
Heat. turbulcnt dilbion of in mean.
diffusion. 17
353 .%9
E h t twnsfer
equalinns and definitions in. 94
exprimental urranwinentr in. Y5 97
mean velocity und tcnipcraturc distribiimcawcmcnt of fluc~utltnig qcfriiititier in.
tion in. 97 9U
9Y 102
hyur. Y. ? 108
Hc;it transport. a c r m turhulrnt mixing
1
I.M.S.T. (Inbtitut de Meaniquc Strtistique
dc la Turhulcnce). 391 404
Inslitntancour wlocitq and length scales. in
turhulcnt shear tlow. 213 -223
lntcrmediary dihlrihllli~n. in turbulent
regime. 103
lntrrnul boundary layer
experimental conditions in. 264 265
propgation velocities und hpectra of it
skewness and Hntness factors in, 265 271
turhuknrx: within. 263 2x4
und I V in. 272 283
lrich Sea. dilTu4on ctpcrimcnts in. 3lX
K
Kinctic theory model. simplcui, 29 31
Kinctic theory ritndoni walk niodcl. 29- 31
tiinc rcstrwtiun in. 31