SUBJECT INDEX
461
Transport mechanism, inhomogcneity and
Transport model
nonstationarity of, 32 33
for gradient modeling of turbulent
transport. 43-47
inhomogeneity and nonstationarity of
transport mechanism in. 32-33
transition probability and diffusion
equation in. 33-34
Transport terms, in turbulent transport.
1 8 0 181
Turbidity, diffusion of by shear ,-ffect.
3 3 1 ~
337
Turbulence
Burgers' model of, 447--450
diffusive character of, 141
energy loss in largoscale type. 241-246
experimental data on, 4-5
fluid dynamic. 141
generation of by ocean surface waves.
gradient transport model limitations in,
high Reynolds number in, 401- 402
within internal boundary layer, 263 ~ 2 8 4
L;igr:ingian quantities in. 141- 162
mathematicid analysis of. 4
"noise" as, 367
phenomenological studies of, 289
scale of, 4
second-order. I70
stratification effects in. 400
theory of. 2- 3
vertical component of, in convective
conditions, 125 - 130
wall. .we Wall turbulence
36X- 369
25 54
Turbulence distributions, in atmospheric
Turbulence field, diffusion in. 327--328
Turhulcnce intensity. (is pure Eulerian
Turbulence model. Eulerian-Lagrangian
Turbulencc signals, electronic circuits for.
Turbulent atmospheric diffusion, I 21
boundary layer. 199--203
quantity, 166
relationship in, 165- 168
3sn- ~4
see ulso Diffusion; Turbulence; Turbuleni
diffusion
cause of, 7-X
generalized harmonic analysis in. 17
Turbulent boundary layer
hursts in. 306-313
bursts near wall in, 295-297, .W 305
low-momentum fluid from wall in, 3 I 1
*sweep" in, 287.295-297, 304-3 I3
Turbulent density interrace, molecular
Turbuleni diffusion, 31 5-329
diffusion eficct in, 433-443
see ulra Diffusion
beach pollution and. 371 -38 I
from continuous source at sea, 3 15- 329
dclincd. 2
cqulrtion for. 61
Euler-Lagrangian problem of, 62. 63
or passive scalar, 246
simulation of from two-dimensional flow,
"wavelike," 37-38
142-152
Turbulent diffusion coefficient. 12
Turbulent diflurivity tensor, 47 -53
Turbuknt flows
s w also Turbulent shear flow
"Burgerkncc" in, 244
energy cascade in large-cddy simulations
energy loss in large-scale turbulence.
filtered momentum and continuity
equations in. 238--241
largeeddy simulations of. 237.-247
linear homogeneous. 16
turbulent diffusion of passive scalar in. 246
d, 327--347
241-.246
Turbulent kinematic viscosity, 48 11.
Turbulent mixing luym
self-pr&erving region and virtual origin
temperature field characteristics in, 103
temperature fluctuations in. 103- 106
transport of heat across. 93- 108
in, 96--97
/Turbulent motion. continuous interaction in,
turbulent Prandtl number, 93
1 angular vclocity in. 218 220
equations of motion in. 226-228
free-slip boundaries in. 228-230
instantaneous velocity and length scales
initial conditions in, 231-232
mamentumless wake in. 232- 234
54
Turbulent shear flow
in, 213-223
461
Transport mechanism, inhomogcneity and
Transport model
nonstationarity of, 32 33
for gradient modeling of turbulent
transport. 43-47
inhomogeneity and nonstationarity of
transport mechanism in. 32-33
transition probability and diffusion
equation in. 33-34
Transport terms, in turbulent transport.
1 8 0 181
Turbidity, diffusion of by shear ,-ffect.
3 3 1 ~
337
Turbulence
Burgers' model of, 447--450
diffusive character of, 141
energy loss in largoscale type. 241-246
experimental data on, 4-5
fluid dynamic. 141
generation of by ocean surface waves.
gradient transport model limitations in,
high Reynolds number in, 401- 402
within internal boundary layer, 263 ~ 2 8 4
L;igr:ingian quantities in. 141- 162
mathematicid analysis of. 4
"noise" as, 367
phenomenological studies of, 289
scale of, 4
second-order. I70
stratification effects in. 400
theory of. 2- 3
vertical component of, in convective
conditions, 125 - 130
wall. .we Wall turbulence
36X- 369
25 54
Turbulence distributions, in atmospheric
Turbulence field, diffusion in. 327--328
Turhulcnce intensity. (is pure Eulerian
Turbulence model. Eulerian-Lagrangian
Turbulencc signals, electronic circuits for.
Turbulent atmospheric diffusion, I 21
boundary layer. 199--203
quantity, 166
relationship in, 165- 168
3sn- ~4
see ulso Diffusion; Turbulence; Turbuleni
diffusion
cause of, 7-X
generalized harmonic analysis in. 17
Turbulent boundary layer
hursts in. 306-313
bursts near wall in, 295-297, .W 305
low-momentum fluid from wall in, 3 I 1
*sweep" in, 287.295-297, 304-3 I3
Turbulent density interrace, molecular
Turbuleni diffusion, 31 5-329
diffusion eficct in, 433-443
see ulra Diffusion
beach pollution and. 371 -38 I
from continuous source at sea, 3 15- 329
dclincd. 2
cqulrtion for. 61
Euler-Lagrangian problem of, 62. 63
or passive scalar, 246
simulation of from two-dimensional flow,
"wavelike," 37-38
142-152
Turbulent diffusion coefficient. 12
Turbulent diflurivity tensor, 47 -53
Turbuknt flows
s w also Turbulent shear flow
"Burgerkncc" in, 244
energy cascade in large-cddy simulations
energy loss in large-scale turbulence.
filtered momentum and continuity
equations in. 238--241
largeeddy simulations of. 237.-247
linear homogeneous. 16
turbulent diffusion of passive scalar in. 246
d, 327--347
241-.246
Turbulent kinematic viscosity, 48 11.
Turbulent mixing luym
self-pr&erving region and virtual origin
temperature field characteristics in, 103
temperature fluctuations in. 103- 106
transport of heat across. 93- 108
in, 96--97
/Turbulent motion. continuous interaction in,
turbulent Prandtl number, 93
1 angular vclocity in. 218 220
equations of motion in. 226-228
free-slip boundaries in. 228-230
instantaneous velocity and length scales
initial conditions in, 231-232
mamentumless wake in. 232- 234
54
Turbulent shear flow
in, 213-223