Evolution of Downslope Flow Under Strong Opposing Trade Winds and Frequent Trade-Wind Rainshowers Over the Island of Hawaii

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Evolution of Downslope Flow Under Strong Opposing Trade Winds and Frequent Trade-Wind Rainshowers Over the Island of Hawaii 956 MONTHLY WEATHER REVIEW VOLUME 129 Evolution of Downslope Flow under Strong Opposing Trade Winds and Frequent Trade-Wind Rainshowers over the Island of Hawaii JEFFREY L. FRYE* AND YI-LENG CHEN Department of Meteorology, School of Ocean and Earth Science and Technology, University of Hawaii at Manoa, Honolulu, Hawaii (Manuscript received 6 August 1999, in ®nal form 6 August 2000) ABSTRACT The evolution of downslope ¯ow on the windward side of the island of Hawaii during 7±8 August 1990 is investigated. This period is characterized by atypical strong (;11 m s21) upstream trade winds and frequent nocturnal rainshowers. In the late afternoon, the onset of downslope ¯ow ®rst occurs on the upper slope, which is frequently dominated by orographic clouds. With mean weak surface winds on the windward slopes because of island blocking, the downslope ¯ow onset occurs after the slope surface becomes negatively buoyant. Along the Hilo coastal areas that are well exposed to decelerating trade-wind ¯ow, the offshore ¯ow onset there occurs much later (;2 h) than the Hawaiian Rainband Project (HaRP) mean as the drainage front moves slowly from the windward lowlands toward the coast against the atypical strong incoming trade-wind ¯ow. The downslope ¯ow onset along the coast occurs after a band of trade-wind rainshowers has moved over the coast. These rainshowers produce evaporatively cooled air in the lowest levels and allow the westerly downslope ¯ow to extend offshore. Nevertheless, throughout the night, the horizontal extent of the offshore ¯ow is limited (,10 km) as the leading edge of the offshore ¯ow encounters increasing trade-wind ¯ow farther offshore. During 0300±0500 Hawaiian Standard Time (HST), a second group of rainshowers moves over the island. With a small horizontal extent and a weak density current structure, offshore ¯ow is temporarily destroyed by rainshowers as a result of vertical mixing. It retreats to windward lowlands as trade-wind rainshowers move onshore. Signi®cant enhancement and focusing of the scattered trade-wind rainshowers occur over the conver- gence zone inland. The surface rainfall forcing is also enhanced by orographic lifting aloft producing the wettest early morning 0300±0700 HST period observed during HaRP. During the early morning, the onset of onshore ¯ow along the coast occurs approximately 1±2 h earlier than the HaRP wet cases. Immediately before the onset of the onshore ¯ow, the surface air along the coast is still negatively buoyant. It appears that the onset of onshore ¯ow is caused by the retrograde motion of the leading edge of the offshore ¯ow. With decreasing buoyancy de®cit after sunrise, the gravity current retreats westward, allowing the warm, moist trade winds offshore to return. The retrograde motion of the density current is more likely to occur in the early morning after sunrise, if the opposing trade winds are stronger. 1. Introduction The Hawaiian Rainband Project (HaRP) was con- ducted during July±August 1990 over the island of Ha- The largest island in the Hawaiian chain, Hawaii is waii to better understand the interaction between steady dominated by two volcanic mountains exceeding 4 km trade-wind ¯ow and an island obstacle. It is the ®rst in elevation, well above the typical height of the trade- time that comprehensive datasets were collected by ad- wind inversion (;2.2 km). In the summer months, the vanced instruments over a subtropical island. During nearly continuous exposure to easterly trade winds HaRP, high-resolution datasets were collected from 50 makes the island ideal for studying air¯ow and precip- National Center for Atmospheric Research (NCAR) itation patterns due to the effects of orographic lifting, Portable Automated Mesonet (PAM) stations, research dynamic blocking, and thermally driven circulations. aircraft (NCAR Electra), tethersondes, rawinsondes, a National Oceanic and Atmospheric Administration (NOAA) boundary layer wind pro®ler, and a dual-Dopp- * Current af®liation: United States Transportation Command, Scott ler network (NCAR CP-3 and CP-4) (Fig. 1). One of Air Force Base, Illinois. the major goals of HaRP was to document the structure and evolution of rainbands frequently observed along the windward coast during the morning hours. Corresponding author address: Dr. Yi-Leng Chen, Department of Meteorology, SOEST, University of Hawaii at Manoa, Honolulu, HI Leopold (1949) described the trade-wind inversion as 96822. a ``lid'' forcing trade-wind ¯ow to move around the E-mail: [email protected] island. He suggested that the formation of band clouds q 2001 American Meteorological Society Unauthenticated | Downloaded 09/23/21 08:22 PM UTC MAY 2001 FRYE AND CHEN 957 and depth of the offshore ¯ow. They maintain, however, that the convergence line is primarily a result of dynamic forcing. Analyses of the HaRP data show the effects of thermal forcing on mesoscale circulations. In contrast to mod- eling studies, HaRP analyses show that the nighttime downslope ¯ow on the windward side is not pure dy- namically driven reversed ¯ow. Chen and Nash (1994) present a detailed analysis of the PAM data and show that in regions of weak mean surface winds caused by island blocking, the thermally driven winds become sig- ni®cant. They describe windward rainfall as a complex interaction of orographic lifting, thermal forcing, and dynamic blocking. Chen and Wang (1994) found that on the windward slopes and lowlands with weak mean surface winds, the onset of upslope (downslope) ¯ow is closely related to the thermal contrast between slope surface and upstream environment at the same altitude. Carbone et al. (1995) are in agreement with previous HaRP analyses that show that the westerly ¯ow on the FIG. 1. Windward Hawaii with PAM sites (solid circles with station windward side is primarily a thermally driven circula- number), the tethersonde site at Kaumana Elementary School (open tion. They compared the westerly ¯ow to a classic grav- circle), Doppler radar locations, and pro®ler location. Contour inter- val for elevation is 1000 m. ity current with a 1% density discontinuity across the ¯ow convergence line. Reisner and Smolarkiewicz (1994) studied low (,1) Fr ¯ow past a three-dimen- offshore of Hilo is caused by the interaction between sional obstacle with uniform heating at the surface and the land breeze and incoming trade-wind ¯ow. Garrett obtained a simple criterion for the transition from the (1980) conducted an observational study of the ¯ow blocked ¯ow to an unblocked ¯ow regime. Chen and pattern over the eastern slopes of Mauna Loa. He com- Wang (1994) show that variations in surface temperature bined previous work from other researchers (Leopold and dew point are related to orography, surface air¯ow, 1949; Eber 1957; Lavoie 1967; Mendonca 1969) with and distributions of cloudiness and rainfall. The am- his observations from a Hilo to Mauna Loa transect to plitudes of the diurnal surface air temperatures are not form a conceptual model of the island-induced circu- uniform over the island. Dry, barren lava soils on the lations. The daytime regime is triggered by differential upper slopes and on the lee sides of mountain ridges heating rates over land and sea, which result in a com- heat up more quickly than moist, well-vegetated sur- bined anabatic and sea breeze wind. At night, the sit- faces on the windward lowlands. After sunrise (before uation reverses, with a thermally forced westerly kat- sunset) the onset of upslope (downslope) ¯ow occurs abatic wind at peak strength just before sunrise. The on the windward slopes where the virtual temperature offshore ¯ow meets the incoming trade winds well off- ®rst becomes warmer (colder) than the upstream envi- shore, resulting in the development of cloud bands off- ronment at the same altitude. In addition, precipitation shore of Hilo. and cloud distributions also affect the air¯ow over the In contrast to early observational efforts, the mod- island. Chen and Wang (1995) found that rainshowers eling studies (Smolarkiewicz et al. 1988; Rasmussen et and clouds can affect the timing of the wind shifts from al. 1989; Smolarkiewicz and Rotunno 1990) describe downslope±offshore (upslope±onshore) to upslope±on- the development of westerly ¯ow as a result of a stably shore (downslope±offshore) ¯ow in the early morning strati®ed ¯ow moving over a mountain barrier for (late afternoon) by modifying the thermodynamic ®elds Froude number (Fr 5 U/Nh, where U is the upstream near the surface. wind speed, N is the Brunt±VaÈisaÈlaÈ frequency, and h is From the analysis of tethersonde and PAM data dur- the height of the barrier) less than unity. For typical ing HaRP, Wang and Chen (1995) take a detailed look trade-wind values (7.5 m s21) upstream of the island of at near-surface winds and thermal pro®les during the Hawaii, the Froude number is between 0.2 and 0.5. On transition periods between katabatic and anabatic ¯ow. the upwind side of the island, the low-level winds are They suggest that the katabatic ¯ow just before sunrise predicted to reverse direction as a result of island block- is characterized by a 50±150-m nocturnal inversion of ing. A convergence line is created where the reverse about a 1±4 K strength. A nocturnal wind maximum is ¯ow encounters the trade winds, resulting in the for- also observed just below the inversion. Wang and Chen mation of Hilo cloud bands. More recent studies by (1995) also note that during rain cases the nocturnal Rasmussen and Smolarkiewicz (1993) suggest the im- inversion and nocturnal wind maximum are weaker than portance of nocturnal cooling in modulating the strength for dry cases owing to cloudiness and vertical mixing. Unauthenticated | Downloaded 09/23/21 08:22 PM UTC 958 MONTHLY WEATHER REVIEW VOLUME 129 The depth of the downslope ¯ow, however, is deeper Chen and Nash (1994, p.
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