2008
DOI: 10.1016/j.jaridenv.2008.05.009
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Clearing enhances dust devil formation

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Cited by 22 publications
(23 citation statements)
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“…Rather than using a fixed annual occurrence time, they instead determined when and where dust devils should (or should not) occur based on the following constraints: locations with high convective buoyancy and low frictional dissipation, using a criterion suggested by Lyons et al (2008) and a high lapse rate criterion as suggested by Ryan (1972), Oke et al (2007b), and Ansmann et al (2009) (see Section 3.1 for more details). Jemmett- applied their criteria truly globally using high-resolution ECMWF operational analyses (see Section 3.1).…”
Section: Scaling Dust Fluxes Based On Field Measurements Of Individuamentioning
confidence: 99%
“…Rather than using a fixed annual occurrence time, they instead determined when and where dust devils should (or should not) occur based on the following constraints: locations with high convective buoyancy and low frictional dissipation, using a criterion suggested by Lyons et al (2008) and a high lapse rate criterion as suggested by Ryan (1972), Oke et al (2007b), and Ansmann et al (2009) (see Section 3.1 for more details). Jemmett- applied their criteria truly globally using high-resolution ECMWF operational analyses (see Section 3.1).…”
Section: Scaling Dust Fluxes Based On Field Measurements Of Individuamentioning
confidence: 99%
“…this model does not realistically represent the natural lower boundary and its possible effect on dust-devil activity (about this effect e.g. see Lyons et al 2008).…”
Section: Dust Devil Activitymentioning
confidence: 99%
“…Dust devils are typically observed between 10:00 and 17:30 local time (LT) [ Balme and Greeley , ], during clear to fair weather conditions [ Sinclair , ] and under relatively weak ambient winds [ Oke et al ., ]. Several observational studies show that dust devil and dusty plume (DDP) occurrence significantly depends on the local meteorology, defined using thresholds of near‐surface temperature lapse rate [ Ryan , ; Oke et al ., ; Ansmann et al ., ] and boundary layer scaling parameters [ Deardorff , ; Hess and Spillane , ; Lyons et al ., ; Kurgansky et al ., ].…”
Section: Introductionmentioning
confidence: 99%
“…Lyons et al [] suggest two key factors that govern the formation and development of dry convective vortices: the availability of convective buoyancy and the frictional dissipation, quantified using w * and u * , respectively. The significance of w * as a scaling parameter for convective boundary layers was first defined by Deardorff [] as w*=gtrueT¯h()ωTtrue¯013where gtrue/trueT¯ is the buoyancy parameter for an ideal gas, h is the boundary layer height (of the convective region), and trueωT¯0 is the kinematic heat flux near the surface.…”
Section: Introductionmentioning
confidence: 99%