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<br />-22- <br /> <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />II <br /> <br />8PECTEAL CHARACTERISTICS OF RELEASE SITE WINDS <br /> <br />The release-site winds during diffusion test periods were read <br />every five seconds and analyzed by the power spectrum method. For <br />each te st, the mean wind direction and speed, the total spectral energy <br />of. the wind direction and of the wind speed, the normalized spectral <br />density at selected frequencies (to depict the shape of the curves), and <br />the maximum coherence between speed and direction and the frequency <br />at which this occurs were computed. The total spectral energy and the <br />spectral densitie s at various frequencie s were then examined for re- <br />lationships to wind speed and wind direction. If mechanical turbulence <br />is a major contributor to the observed spectral energy, it should be <br />related to wind speed and possibly wind direction, because surface <br />roughness and topography vary with direction. <br /> <br />The total spectral energy of both wind direction and wind speed <br />were not significantly related to mean wind speed or mean wind direc- <br />tion, The spectral density at a high and a low frequency (0,05 and. 01 <br />cps) were then examined for a relationship to wind speed. The most <br />significant relationship found was between the wind direction and wind <br />speed spectral content at .05 cycles per second, and this is shown <br />in Figure 8. The result agrees with the findings of others, that the <br />high frequency end of the spectra for lateral and longitudinal velocity <br />components is controlled by wind speed (Lumley and Panofsky, 1964). <br /> <br /> <br />Mechanical turbulenc e should have an effect on the low frequency <br /> <br /> <br />part of the longitudinal velocity spectrum, but not on the lateral velocity <br /> <br /> <br />spectrum. The major effect on the lateral velocity spectrum should be <br /> <br /> <br />produced by stability. The computed spectra were ranked by stability <br /> <br /> <br />and examined for differences in shape. In general, the unstable cases <br /> <br /> <br />had proportionally more energy in the lower frequencies, and the coher- <br /> <br /> <br />ence between the wind direction and the wind speed was higher at all <br /> <br /> <br />frequencie s for the unstable case s. <br />