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Volume 1 - The Atmospheric Studies Group at TRC

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the numbers refer to ICOARE values, and the “d” and “s” refer to the deep-w<strong>at</strong>er and<br />

shallow-w<strong>at</strong>er Charnock parameter limits.<br />

CALMET must be started no l<strong>at</strong>er than the hour th<strong>at</strong> ends <strong>at</strong> 0500 in the base time<br />

zone (typically LST) and it does not need to cre<strong>at</strong>e meteorological fields for hours<br />

after the end of sampling, since no CALPUFF simul<strong>at</strong>ions are made after the<br />

sampling termin<strong>at</strong>es. <strong>The</strong>refore each experiment-day is simul<strong>at</strong>ed in a separ<strong>at</strong>e<br />

CALMET applic<strong>at</strong>ion.<br />

<strong>The</strong> fumig<strong>at</strong>ion study <strong>at</strong> Carpinteria is made up of several ½-hour periods instead of<br />

the one-hour periods used in the other d<strong>at</strong>asets. <strong>The</strong>se are simul<strong>at</strong>ed as one-hour<br />

experiments. On 10/4/1985 and 10/5/1985, three contiguous ½-hour sampling and<br />

meteorological averaging periods must be addressed (10:00, 10:30, 11:00). This is<br />

done by making two simul<strong>at</strong>ions of each day, with Hour 11 set to the 10:30 period in<br />

one, and 11:00 in the other. Hour 10 is period 10:00 in both runs.<br />

Oresund<br />

Emphasis is given to using all available measured winds and temper<strong>at</strong>ures <strong>at</strong> sites<br />

upwind of, across, and downwind of the strait of Oresund. Unlike most regular<br />

CALMET applic<strong>at</strong>ions, there is a wealth of d<strong>at</strong>a on the vertical structure. <strong>The</strong>refore,<br />

CALMET is configured to NOT extrapol<strong>at</strong>e the surface observ<strong>at</strong>ions. Winds in the<br />

UP.DAT files are given primary influence on the tracer transport and dispersion of<br />

these elev<strong>at</strong>ed releases.<br />

Over the Oresund itself, the boundary layer structure is characterized by the wind<br />

speed, air-sea temper<strong>at</strong>ure difference, rel<strong>at</strong>ive humidity and vertical temper<strong>at</strong>ure<br />

gradient listed in the SEA.DAT file. <strong>The</strong> overw<strong>at</strong>er mixing height is taken directly<br />

from the SEA.DAT file and tre<strong>at</strong>ed as an observ<strong>at</strong>ion when it is provided, or it is<br />

computed when it is not provided. CALMET is run both with and without estim<strong>at</strong>ed<br />

overw<strong>at</strong>er mixing heights. Over land, the boundary layer structure is characterized<br />

by the wind speed and cloud cover listed in the SURF.DAT file, along with the<br />

gridded surface characteristics contained in the geophysical d<strong>at</strong>a file th<strong>at</strong> account for<br />

land use vari<strong>at</strong>ions. <strong>The</strong> daytime mixing height over land includes the history of the<br />

computed surface fluxes and accounts for the modific<strong>at</strong>ion of the temper<strong>at</strong>ure<br />

structure aloft provided in the UP.DAT files. Note th<strong>at</strong> all mixing heights (over land<br />

and over w<strong>at</strong>er, whether computed or provided in the SEA.DAT file) are modified for<br />

advection affects which includes both off-shore and on-shore flow in this study.<br />

Altern<strong>at</strong>e methods for computing mixing heights are selected to explore the<br />

sensitivity of model performance to these choices. Overw<strong>at</strong>er mixing heights are<br />

either provided in the SEA.DAT file (these heights are listed in Table 4-10), or<br />

computed internally. Whenever the mixing height is computed (land or w<strong>at</strong>er) and<br />

the surface he<strong>at</strong> flux is positive, either the modified Maul-Carson model is used<br />

Final Report Vol.1 57

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