Handout (907.7 kB)
Most operational dispersion models being applied to the JR II chorine releases require, as a minimum, inputs of wind speed and direction, temperature, and stability class near the source location. The surface roughness length, zo, is also needed. Some models also desire to have inputs of friction velocity u*, Monin-Obukhov length L, convective velocity scale w*, and perhaps turbulence components σu, σv, and σw. Some models allow input of vertical profiles of these variables. A few models that make use of a diagnostic mass-consistent wind model can use the wind fields from the mesoscale networks.
We present the rationale for selecting JR II meteorological observations from a subgroup of wind, turbulence, and energy flux instruments near the source, and recommending meteorological inputs, separated into surface and upper air. Several difficulties are discussed. One is related to the fact that all releases were in early morning, during a period of boundary layer transition from stable to unstable. This time variability also affects the cloud as it traverses to 11 km across the sampling network. Another difficulty is related to the fact that the chlorine release took place in an environment that could be classified as a “drainage wind”, with large wind direction shears above 100 or 200 m. Another problem is caused by the mesoscale meandering or sloshing that is taking place across the sampling domain.