We found strong agreement between the lidar-derived and tower-derived σw2 and TKE over the entire diurnal cycle; the root-mean square error (RMSE) and best-fit slope (mb) between the lidar- and tower-derived values of σw2 were 0.18 m2 s-2 and 0.98, respectively. For TKE, RMSE and mb were 0.64 m2 s-2 and 1.02, respectively, and good agreement was found when distinguishing between daytime and nighttime. The good agreement between the sampling platforms provided us with confidence in using the tower datasets to distinguish and interpret turbulence characteristics across four distinct meteorological conditions: 1) clear and weak winds, 2) clear and strong winds, 3) cloudy and weak winds, and 4) cloudy and strong winds.
Throughout the study period, consistent with previous research at other ridgetop sites, mean winds were larger during the nighttime than during the daytime and the magnitude of this difference was largest at the uppermost sampling heights. Near-surface wind directions were typically from the northwest during the nighttime but were westerly during the daytime, whereas mean winds 300 m AGL were from the west and exhibited little time-of-day dependence. σw2 at 40 m AGL (300 m AGL) ranged from 0.25 m2 s-2 (0.50 m2 s-2) during the nighttime to a maximum of 0.75 m2 s-2 (1.25 m2 s-2) during the early afternoon, whereas TKE sampled 40 m AGL (300 m AGL) ranged from ~ 1.0 m2 s-2 (1.25 m2 s-2) to 2.5 m2 s-2 (3.0 m2 s-2). When evaluating different meteorological regimes, we observed that the greatest decrease in the diurnal wind speed occurred on clear, windy days. These days were also characterized by the largest σw2 and TKE, which reached peak values around 2 m2 s-2 and 5 m2 s-2, respectively, in the early afternoon. Larger S and K were observed during the nighttime than during the daytime, and the magnitude of the variability was quite similar across all sampling heights and meteorological regimes. The results from this work provide valuable insights into turbulence processes over forested, complex terrain and can contribute to refining turbulence parameterizations in NWP models.
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