1991
DOI: 10.1007/bf00120057
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The dependence of the bulk Richardson number on stability in the surface layer

Abstract: Relationships between the bulk Richardson number, B, and other stability parameters were derived for the atmospheric surface layer. Nomograms were constructed, relating the Monin-Obukhov stability parameter, z/L, to B. The nomograms and the graph of Golder (1972) were used to establish various schemes for classifying z/L, B and Ri, in terms of the Pasquill stability classes.

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Cited by 37 publications
(13 citation statements)
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“…4(b). As stability parameter, the Bulk-Richardson number (Zoumakis and Kelessis, 1991) was calculated from operational analysis data from the COSMO-DE numerical weather prediction (NWP) model (Doms and Schättler, 2002) as…”
Section: Measured Wake Effectsmentioning
confidence: 99%
“…4(b). As stability parameter, the Bulk-Richardson number (Zoumakis and Kelessis, 1991) was calculated from operational analysis data from the COSMO-DE numerical weather prediction (NWP) model (Doms and Schättler, 2002) as…”
Section: Measured Wake Effectsmentioning
confidence: 99%
“…The flow conditions expressed in terms of atmospheric stability classification has been established with reference to the Bulk Richardson approach. The Bulk Richardson number has been used as a stability parameters in many atmospheric studies (e.g., Hsu ; Zoumakis and Kelessis ). The Bulk Richardson number ( Ri b ) is based on a paper by Grachev and Fairall from a single wind speed observation ( U h ), measured at 15–20 m height ( h ) above mean sea level combined with the air and water temperature difference ( Δt) from [equation ] and the absolute temperature ( T ) measured 13–16 m above mean sea level.…”
Section: Wind Farm Layoutmentioning
confidence: 99%
“…The histogram (bar-graph in Figure 3) presents the diurnal variation of the percentage of central heating fuel consumed hourly in Thessaloniki during the cold part of the year. During the morning hours the increase of the SO 2 emission sources, in conjunction with the shallow mixing height and the stable stratification of the atmosphere result in higher SO 2 columnar values (12,28,29). During midday and until the early afternoon, columnar SO 2 is declining due to the decreasing of local sources and increasing of intensity of mixing and wind speed into the mixing layer (9,30).…”
Section: Instrumentationmentioning
confidence: 99%