First observation of one noctilucent cloud by a twin lidar in two different directions
dc.bibliographicCitation.firstPage | 1863 | eng |
dc.bibliographicCitation.issue | 11 | eng |
dc.bibliographicCitation.journalTitle | Annales Geophysicae | eng |
dc.bibliographicCitation.lastPage | 1868 | eng |
dc.bibliographicCitation.volume | 20 | |
dc.contributor.author | Baumgarten, G. | |
dc.contributor.author | Lübken, F.-J. | |
dc.contributor.author | Fricke, K.-H. | |
dc.date.accessioned | 2018-03-09T10:43:59Z | |
dc.date.available | 2019-06-28T12:38:32Z | |
dc.date.issued | 2002 | |
dc.description.abstract | In the early morning hours of 14 July 1999, a noctilucent cloud (NLC) was observed simultaneously by the two branches of a twin lidar system located at the ALOMAR observatory in northern Norway (69° N). The telescopes of the two lidars were pointing vertical (L^) and off the zenith by 30° (L30°). The two lidars detected an enhancement in the altitude profile of backscattered light (relative to the molecular background) for more than 5 h, starting approximately at 01:00 UT. These measurements constitute the detection of one NLC by two lidars under different directions and allow for a detailed study of the morphology of the NLC layer. A cross-correlation analysis of the NLC signals demonstrates that the main structures seen by both lidars are practically identical. This implies that a temporal evolution of the microphysics within the NLC during its drift from one lidar beam to the other is negligible. From the time delay of the NLC structures, a drift velocity of 55–65 m/s is derived which agrees nicely with radar wind measurements. During the observation period, the mean NLC altitude decreases by ~0.5 km/h (=14 cm/s) at both observation volumes. Further-more, the NLC is consistently observed approximately 500 m lower in altitude at L30° compared to L^. Supplementing these data by observations from rocket-borne and ground-based instruments, we show that the general downward progression of the NLC layer through the night, as seen by both lidars, is caused by a combination of particle sedimentation by 4–5 cm/s and a downward directed vertical wind by 9–10 cm/s, whereas a tilt of the layer in drift direction can be excluded. | eng |
dc.description.version | publishedVersion | eng |
dc.format | application/pdf | |
dc.identifier.uri | https://doi.org/10.34657/1528 | |
dc.identifier.uri | https://oa.tib.eu/renate/handle/123456789/4073 | |
dc.language.iso | eng | eng |
dc.publisher | München : European Geopyhsical Union | eng |
dc.relation.doi | https://doi.org/10.5194/angeo-20-1863-2002 | |
dc.rights.license | CC BY 3.0 Unported | eng |
dc.rights.uri | https://creativecommons.org/licenses/by/3.0/ | eng |
dc.subject.ddc | 530 | eng |
dc.subject.other | Atmospheric composition and structure (cloud physics and chemistry | eng |
dc.subject.other | aerosols and particles) Meteorology and atmospheric dynamics (middle atmosphere dynamics) | eng |
dc.title | First observation of one noctilucent cloud by a twin lidar in two different directions | eng |
dc.type | Article | eng |
dc.type | Text | eng |
tib.accessRights | openAccess | eng |
wgl.contributor | IAP | eng |
wgl.subject | Physik | eng |
wgl.subject | Geowissenschaften | eng |
wgl.type | Zeitschriftenartikel | eng |
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