Toulouse IHOP meeting 15 June 2004 Water vapour variability within the growing convective boundary layer of 14 June 2002 with large eddy simulations and

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Toulouse IHOP meeting 15 June 2004 Water vapour variability within the growing convective boundary layer of 14 June 2002 with large eddy simulations and observations OUTLINE Methodology and Objectives Observational data: several scales of variability LES simulations: comparisons obs/model Conclusions & Perspectives Fleur Couvreux Franoise Guichard, Jean-Luc Redelsperger, Cyrille Flamant, Jean-Philippe Lafore, Valry Masson r v (g/kg) W (m/s) ENE WSW 6 4 2 0 -2 -4 11 10 8 9 7 12 Time (UTC) 12131415161718 Slide 2 Toulouse IHOP meeting 15 June 2004 Methodology & Objectives LES : Is such a high resolution model able to represent the observed water vapour variability ? first goal : from observations and simulations, to explain the mecanisms responsible for the water vapour variability second goal: to understand the role of such variability on cloud formation and maintenance IHOP observations: What are the fluctuations of water vapour mixing ratio observed within the growing convective boundary layer? 14 june 2002: BLE case What are the scales involved ? Is this day typical? Slide 3 Toulouse IHOP meeting 15 June 2004 Time 12h 13h 14h 15h 16h 17h 18h 19h (K) 306 294 1 0 Zi (km) Time 12h 13h 14h 15h 16h 17h 18h 19h 2 morning Early afternoon Boundary layer mean value of & r v Time in UTC=local time+5h 2 1 0 300 r v (g/kg) 7 1210 A classic convective BL growth but with large fluctuations of r v Zi (km) Slide 4 Toulouse IHOP meeting 15 June 2004 Main characteristics : Relatively simple case of a growing boundary layer: a well mixed boundary layer reaching 1.5 km High Pressure system, homogeneous temperature field Weak subsidence constant whole day Low shear and weak wind (< 5m/s) from N to NE Existence of thermals (cf Cloud radar) Small cumuli developed after 1500 UTC NE/SW moisture gradient Heavy precipitation the day before, coherent distribution with moisture gradient The 14 june 2002 case Data : Soundings (35) Lidars (DLR-DIAL, LEANDRE et SRL) In-situ aircraft data (NRL-P3 et UWKA) Surface flux measurements (ISSF) Slide 5 Toulouse IHOP meeting 15 June 2004 Different scales of variability: evidence in soundings 2 soundings separated from less than 10 km 1g.kg -1 1830 UTC Soundings : Different variability at different scales rvrv Soundings in a 200 km wide domain 1130 UTC 1700 UTC 3 g/kg 5 g/kg rvrv rvrv Slide 6 Toulouse IHOP meeting 15 June 2004 EW Different scales of variability : aircraft data and lidars + rvrv 3g.kg -1 rvrv 1.5 g.kg -1 Aircraft r v measurement 1710Time (UTC) 1710 12 8 7 8 +0.7 -0.7 Time (UTC) 1745 rvrv 1710 1745 r v measured by the DLR lidar 1500 1000 500 Height (m) 1500 1000 500 Height (m) WSW ENE 1500 1000 500 Height (m) Slide 7 Toulouse IHOP meeting 15 June 2004 Modelling: LES with Mso-NH (Lafore et al. 1998) Simulation : x= y=100m, z streched (< 50m in BL) 3D turbulence scheme (Cuxart et al. 2000) early morning to early afternoon (duration 7h) a realistic simulation: ISFF2 surface fluxes (prescribed) homogeneous initial sounding = composite of soundings at 1130 UTC large scale advection estimated from MM5 simulations and soundings Initial profile observations rvrv Slide 8 Toulouse IHOP meeting 15 June 2004 Mean profiles Temporal evolution of mean profiles rvrv Comparison obs/LES at 1800 UTC rvrv Slide 9 Toulouse IHOP meeting 15 June 2004 Time variations of boundary layer characteristics Sensitivity to surface fluxes : +Bo -> +z i Sensitivity to large- scale advection : +ADV -> +z i +Bo -> + m +Bo -> + qm Cf Bo ie SSH et SLH +ADV -> + m +ADV -> + qm Several factors : Ws -> z i -> , q Adv -> -> zi Adv q -> q Validated reference simulation, quantification of sensibility to different forcings rvrv zi Slide 10 Toulouse IHOP meeting 15 June 2004 Horizontal cross sections Z/zi=0.3 Z/zi=0.8 Z/zi=1. Z/zi=0.8 Z/zi=1. 11 10 9 8 7 6 5 11 10 9 8 7 6 5 11 10 9 8 7 6 5 305 304.5 304. 303.5 5 3 1 -3 5 3 1 -3 5 3 1 -3 W (m/s) v (K) 305 304.5 304. 303.5 306 304.5 304. 303.5 305.5 305 r v (g/kg) 10 km Slide 11 Toulouse IHOP meeting 15 June 2004 Characteristic length scale Los C( )= Reference simulation at 17h r v length scale is larger than length scale of v, , w from Lohou et al. (2002) (m) z/zi Rv v w Slide 12 Toulouse IHOP meeting 15 June 2004 LEANDRE and LES horizontal cross-sections Measurements from LEANDRE LES Simulations At 1600 UTC r v -r v rv ~10 km 1.2 3.5 1.2 3.5 Slide 13 Toulouse IHOP meeting 15 June 2004 Vertical cross sections Evidence of dry downdrafts Several thermals in one humid zone LES r v & w DLR-DIAL r v 6.5 5.5 6 7 7.5 8 8.5 9.5 10 9 10.5 6.5 5.5 6 7 7.5 8 8.5 9.5 10 9 10.5 Slide 14 Toulouse IHOP meeting 15 June 2004 Evaluation of histograms of , r v, w P3 aircraft KA aircraft Z=0.4z i model max --- min w rvrv Dry downdraft Overshooting updrafts zi Equivalent gaussian Slide 15 Toulouse IHOP meeting 15 June 2004 Boundary layer precipitable water Slide 16 Toulouse IHOP meeting 15 June 2004 Second order moments __ simulation __ lidar DIAL o P3 o KA Strong relation between The inversion strength and the variance Max( rv ) (g.kg -1 ) q z i (g.kg -1 ) 1.2 0.72 0.81 0.41 0.56 5.7 MNH 4.4 MNH 4.3 DIAL 3.9 DIAL 4.1 DIAL 3 lidar 10km-long Cross-section at 1730 UTC LES 1700 & 1800 UTC rvrv Slide 17 Toulouse IHOP meeting 15 June 2004 Joint probability distribution At z/zi=0.3 + z/z i + larger spectrum of w + and q - At z/zi=0.8 Slide 18 Toulouse IHOP meeting 15 June 2004 Conclusions: Evaluation of the LES Able to represent the variability observed at scales lower than 10 km (comparisons to soundings, lidars (DIAL et SRL), aircraft time-series) Quantification the impact of scales > 10 km on variability at scales < 10km At first order, the boundary layer dynamics explain the observed variability at scales lower than 10 km even without surface heterogeneities and variability in the initial atmospheric state Dry narrow downdrafts as a signature of the BL growth (via dynamics at the top) [Crum et al. (1987) and Weckwerth et al. (1996)] impact on length scale, skewness, vertical transport.. Negative skewness is common (cf other IHOP days) Observations from 14 juin 2002 during IHOP_2002 : Several scales of variability ( 10 km) Slide 19 Toulouse IHOP meeting 15 June 2004 Perspectives: Systematic analysis of IHOP data : - objective : to identify pertinent parameters controlling the water vapour variability in the boundary layer (such as strength of inversion ( ,q), fluxes) from more idealised simulations -> 1D parameterizations Understand the impact of such a variability on cloud formation and maintenance Quantify time scales concerned by mechanisms involved in the water vapour variability: dry intrusion life time, transient state Slide 20 Toulouse IHOP meeting 15 June 2004 F I N Slide 21 Toulouse IHOP meeting 15 June 2004 Development of the CBL ( courtesy of Bart Geerts) aspect ratio: 1:1 1330 UTC 1415 UTC 1530 UTC 1630 UTC 1730 UTC Slide 22 Toulouse IHOP meeting 15 June 2004 Surface fluxes Sensible heat flux Latent heat flux Bo~1. Bo~0.5 Slide 23 Toulouse IHOP meeting 15 June 2004 Large scale forcings (advection) Large-scale forcings Deduced from MM5 Horizontal advection of Horizontal advection of r v Subsiding w