Volume 1 - The Atmospheric Studies Group at TRC
Volume 1 - The Atmospheric Studies Group at TRC Volume 1 - The Atmospheric Studies Group at TRC
σ = .02 u ( z > z ) (3-44) ws 0 zi i The total turbulence velocity is obtained from the sum of these components: w 2 wb 2 ws σ = σ + σ (3-45) Minimum Turbulence Velocities CALPUFF accepts minimum lateral turbulence velocities σ v as a function of stability class (6 values). A minimum value establishes a floor, so that any computed lateral turbulence less than the minimum is replaced. The default value for each stability class had been set to 0.5m/s. An additional set of minimum values for overwater cells has been added, so now there are 12 values, two for each stability class. The original set of six is now used for overland cells, and the default of 0.5m/s is retained. The AERMOD minimum lateral variance, 0.25 m 2 /s 2 , is equivalent. The new set of six used for overwater cells is set to a default of 0.37 m/s, a value originally used in the OCD model for overwater dispersion, and one that performed well in the model evaluations with the offshore tracer data sets. Similarly, a set of overland and overwater minimum vertical turbulence velocities σ w are also accepted, two for each stability class (12 values). The default values for overwater cells are equal to those for overland cells. ---------- LAND ---------- --------- WATER ---------- Stability Class : A B C D E F A B C D E F --- --- --- --- --- --- --- --- --- --- --- --- Default SVMIN : .50, .50, .50, .50, .50, .50, .37, .37, .37, .37, .37, .37 Default SWMIN : .20, .12, .08, .06, .03, .016, .20, .12, .08, .06, .03, .016 Lateral Puff Timescale Diagnostic Option For steady homogeneous dispersion, Taylor’s (1921) original expression for lateral plume spread σ y as a function of time is: ( t −τ + τ exp( − τ )) σ 2 = 2σ 2 τ t / (3-46) y v where τ is the Lagrangian timescale and σ v is the lateral turbulence intensity. This is typically approximated as: ( 1 / τ ) σ y = σ vt / + t 2 (3-47) which has the same limits as Equation 3-46 for small and large t/τ. Lateral growth in CALPUFF uses Draxler’s (1976) expression, which is equal to Equation 3-47 when τ=617.3s. Final Report Vol.1 18
Two methods of supplying the timescale τ were implemented for testing: • direct numeric input as a constant, and • selection of a timescale that is proportional to a characteristic length scale in the boundary layer divided by the lateral turbulence velocity. For the second option, a timescale estimate based on that in SCIPUFF (EPRI, 2000) is used: Λ H τ = (3-48) 0.75q where q is the turbulence velocity scale and Λ H is approximately 0.3z i within much of the surface layer, and may be of order 1000m or larger outside the surface layer. In the CALPUFF implementation, testing will be limited to near-surface tracer releases so the mesoscale limit for Λ H is not included. SCIPUFF explicitly considers the effects of shear-driven eddies and buoyancy-driven eddies separately. Their length scales in the boundary layer (z
- Page 1 and 2: Development of the Next Generation
- Page 3 and 4: 1. INTRODUCTION The purpose of this
- Page 5 and 6: • Prognostic Meteorological Model
- Page 7 and 8: o 1: Maul (1980)-Carson (1973) o 2:
- Page 9 and 10: into 50 tiles (90 RUC grid-points/t
- Page 11 and 12: y H ( 1− 34.15z / L) 1/ 3 = (3-9)
- Page 13 and 14: During execution, the bulk algorith
- Page 15 and 16: Anemometer Height Adjustment for La
- Page 17 and 18: T (ºK) g (m/s 2 ) temperature grav
- Page 19: adjusted to account for the effect
- Page 23 and 24: cell is the cell that determines th
- Page 25 and 26: June 4 (1130-1230 CET) L. Turbulenc
- Page 27 and 28: 4. MODEL PERFORMANCE EVALUATION 4.1
- Page 29 and 30: The CALMET preprocessors TERREL, CT
- Page 31 and 32: All sampler locations are used as r
- Page 33 and 34: Table 4-2b Over-water Meteorologica
- Page 35 and 36: Meteorological data used in the OCD
- Page 37 and 38: . . CARPINTERIA, CA 3814 . UTM Nort
- Page 39 and 40: Year Month Day Table 4-4 Over-water
- Page 41 and 42: Datum: NAS-C (North American 1927)
- Page 43 and 44: Table 4-5 Source Characterization f
- Page 45 and 46: Table 4-6a Over-water Meteorologica
- Page 47 and 48: Geophysical Processing Gridded land
- Page 49 and 50: Table 4-7 Source Characterization f
- Page 51 and 52: tape format called GF-3. These data
- Page 53 and 54: . . Strait of Oresund 6230 6220 UTM
- Page 55 and 56: . . Strait of Oresund 6230 6220 UTM
- Page 57 and 58: Table 4-10 SEA.DAT Meteorological D
- Page 59 and 60: the numbers refer to ICOARE values,
- Page 61 and 62: that are simulated during the one-h
- Page 63 and 64: 4.3 Evaluation Results Cameron, Car
- Page 65 and 66: improve model performance relative
- Page 67 and 68: Figure 4-7. Graphical depiction of
- Page 69 and 70: Figure 4-8. Graphical depiction of
σ = .02 u ( z > z )<br />
(3-44)<br />
ws<br />
0<br />
zi<br />
i<br />
<strong>The</strong> total turbulence velocity is obtained from the sum of these components:<br />
w<br />
2<br />
wb<br />
2<br />
ws<br />
σ = σ + σ<br />
(3-45)<br />
Minimum Turbulence Velocities<br />
CALPUFF accepts minimum l<strong>at</strong>eral turbulence velocities σ v as a function of stability<br />
class (6 values). A minimum value establishes a floor, so th<strong>at</strong> any computed l<strong>at</strong>eral<br />
turbulence less than the minimum is replaced. <strong>The</strong> default value for each stability<br />
class had been set to 0.5m/s. An additional set of minimum values for overw<strong>at</strong>er<br />
cells has been added, so now there are 12 values, two for each stability class. <strong>The</strong><br />
original set of six is now used for overland cells, and the default of 0.5m/s is retained.<br />
<strong>The</strong> AERMOD minimum l<strong>at</strong>eral variance, 0.25 m 2 /s 2 , is equivalent. <strong>The</strong> new set of<br />
six used for overw<strong>at</strong>er cells is set to a default of 0.37 m/s, a value originally used in<br />
the OCD model for overw<strong>at</strong>er dispersion, and one th<strong>at</strong> performed well in the model<br />
evalu<strong>at</strong>ions with the offshore tracer d<strong>at</strong>a sets.<br />
Similarly, a set of overland and overw<strong>at</strong>er minimum vertical turbulence velocities σ w<br />
are also accepted, two for each stability class (12 values). <strong>The</strong> default values for<br />
overw<strong>at</strong>er cells are equal to those for overland cells.<br />
---------- LAND ---------- --------- WATER ----------<br />
Stability Class : A B C D E F A B C D E F<br />
--- --- --- --- --- --- --- --- --- --- --- ---<br />
Default SVMIN : .50, .50, .50, .50, .50, .50, .37, .37, .37, .37, .37, .37<br />
Default SWMIN : .20, .12, .08, .06, .03, .016, .20, .12, .08, .06, .03, .016<br />
L<strong>at</strong>eral Puff Timescale Diagnostic Option<br />
For steady homogeneous dispersion, Taylor’s (1921) original expression for l<strong>at</strong>eral<br />
plume spread σ y as a function of time is:<br />
( t −τ<br />
+ τ exp( − τ ))<br />
σ 2 = 2σ<br />
2 τ<br />
t /<br />
(3-46)<br />
y<br />
v<br />
where τ is the Lagrangian timescale and σ v is the l<strong>at</strong>eral turbulence intensity. This is<br />
typically approxim<strong>at</strong>ed as:<br />
( 1 / τ )<br />
σ<br />
y<br />
= σ vt / + t 2<br />
(3-47)<br />
which has the same limits as Equ<strong>at</strong>ion 3-46 for small and large t/τ. L<strong>at</strong>eral growth in<br />
CALPUFF uses Draxler’s (1976) expression, which is equal to Equ<strong>at</strong>ion 3-47 when<br />
τ=617.3s.<br />
Final Report Vol.1 18