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Laboratory and Field Measurements of Environmental Stratified Flows Marko Princevac July 28, 2006 Stellar Hydro Days, 26-28 July, 2006 Los Alamos
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Outline Slope Flows Entrainment in Katabatic Current Eddy Diffusivity Waves vs. Turbulence Morning Inversion Break-up
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Slope Flows – Thermally Driven Phoenix Terrain induced flow Synoptic flow
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Upslope flow T U Q vs.
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Thermal blob Detachment occurs when
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Competing tendencies B
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Critical angle experiment Heating System Water-Glycerin solution 10 < Pr < 10000
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Critical angle vs. Pr
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Katabatic (Downslope, Drainage) Flow H
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Downslope flow - Idealized Topography
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ACS –VTMX ASU Site
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Slope Site - VTMX
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Downslope flow – Field Results
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Downslope flow - Pulsation T=55 min
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Downslope flow - Pulsation have oscillatory solution with the frequencyor period }, linearized
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Downslope flow - Pulsation T=55 min ACS =4 deg: T=20 – 50 min SS =1.8 deg: T=50 – 130 min
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Downslope flow - Entrainment Entrainment coefficientRichardson number
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Richardson Number Efficient Mixing -KH Regime Near Neutral Waves - very little turbulence Very stable Regime Non-turbulent
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Entrainment Entrainment velocities Entrainment coefficient Entrainment law
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Downslope flow – Laboratory Entrainment Turner (1986)
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Downslope flow - Entrainment
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Field data – 4 locations kilometer apart
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Downslope flow - Entrainment Turner (1986) - laboratory Field observations
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Downslope flow – Eddy diffusivities Eddy diffusivity of momentum Eddy diffusivity of heat High Re (10 7 – 10 8 ) Turbulent transport (u’w’, v’w’, w’ ’…) dominates molecular ( )
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ACS Tower
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Downslope flow – Eddy diffusivities Wave Dominated Transport ? Monti et al. 2002 Molecular ~ 10 -5 (m 2 s -1 )
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Waves vs. Turbulence
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Frequency, Wave Number EE
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Characteristics of Turbulent Flows - Irregularity, randomness Waves also - Diffusivity Waves also - Rotational Waves also – generally (exception example: surface waves) - Dissipative Waves are essentially nondissipative
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Data Filtering
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Filters – low-pass f E Low-pass filter pass bandtransition band stop band slope cut off frequency pass-band ripples stop-band ripples f E unfiltered signal
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Common Digital Filters Flattest Pass-band Frequency GainGain Butterworth Smoothest transition Frequency GainGain Bessel Steepest slope Frequency GainGain Elliptic
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Signal Spectra – where to cut? ? ?
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Shortest internalwave period Buoyancy frequency N corresponds to maximum possible wave frequency N= 0.05-0.1 rad/sec
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Cutting Frequency “waves”“turbulence” Period > 1 minPeriod < 1 min
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Filtering cut-off period of 1 minute 5 minute averaging 5 minute mean is subtracted before filtering Elliptical filter 1 min cut off
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K M from filtered and non-filtered data
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K H from filtered and non-filtered data
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TKE vs. “Wave” kinetic energy Non-filtered data Total KE (fluctuations) Filtered data “wave-less” KE (fluctuations) “Wave” KE = Total – Wave-less
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Rig=1
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Turbulent Prandtl Number (inversed)
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TKE from filtered and non-filtered data
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Nocturnal pooling
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Experimental setup
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Observed flow patterns Simple slope flow followed by recirculation Slope flow followed by recirculation plus layer “thickening” at the valley bottom Same as previous plus horizontal intrusions in stable core No large recirculation – all compensation of mass is via intrusions at different levels
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Governing Parameters Initial Stability (stratification) - N Slope Angle - Heat Flux (buoyancy flux) - q o Inversion Height - h Combination of dimensionless parameters: and
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Cold Pool Breakup Low B
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Cold Pool Breakup High B
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Flow dependence Low B regime High B regime B c =1000-2000 Lower values for smaller slope angles AngleB min B max 10 o 1072497 20 o 2128198 30 o 245564
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Inversion breakup in SLC valley Wheeler Farm cross-section (40 o 38’ N) Wheelers Farm 40 o 38’ N, 111 o 52’ W 1350 m MSL Wheeler Farm Site 2,410 m MSL 2,223 m MSL
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Expected Cold Pool Destruction for SLC
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Summary - Upslope flow - Downslope flow velocity
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Summary - Downslope flow periodicity - Entrainment
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Summary - Inversion breakup mechanisms - Eddy diffusivity
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Next Scale
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Filters – ideal f E unfiltered signal “Brick-wall” filter (hypothetical ideal filter) Low-pass example f E cut off frequency
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Filters – high-pass f E High-pass filter stop bandtransition band pass band slope cut off frequency stop-band ripples pass-band ripples f E unfiltered signal
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Filters – pass-band & stop-band Pass-band filter f E unfiltered signal f E pass- band width cut off frequency Stop-band filter f E stop- band width cut off frequency
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Friction velocity: filtered and non-filtered
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Normalized momentum flux
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Temperature scale
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Summary - Removing “waves” decreases momentum transport (K M ) for high Ri g - Removing “waves” does not affect heat transport (K H )
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Downslope flow – Normalized Eddy diffusivities
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