Non-Universal Turbulence in Planetary Boundary Layers

Slides:



Advertisements
Similar presentations
AIR POLLUTION AND METEOROLOGY
Advertisements

Introduction Irina Surface layer and surface fluxes Anton
LARGE EDDY SIMULATION Chin-Hoh Moeng NCAR.
Section 2: The Planetary Boundary Layer
Training course: boundary layer IV Parametrization above the surface layer (layout) Overview of models Slab (integral) models K-closure model K-profile.
Boundary Layer Flow Describes the transport phenomena near the surface for the case of fluid flowing past a solid object.
Hurricanes Innovative Grid-Enable Multiple-scale Hurricane modeling system Konstantinos Menelaou International Hurricane Research Center Department of.
Session 2, Unit 3 Atmospheric Thermodynamics
Reading: Text, (p40-42, p49-60) Foken 2006 Key questions:
Direct numerical simulation study of a turbulent stably stratified air flow above the wavy water surface. O. A. Druzhinin, Y. I. Troitskaya Institute of.
Convection Convection Matt Penrice Astronomy 501 University of Victoria.
Atmospheric Analysis Lecture 3.
Sensible heat flux Latent heat flux Radiation Ground heat flux Surface Energy Budget The exchanges of heat, moisture and momentum between the air and the.
0.1m 10 m 1 km Roughness Layer Surface Layer Planetary Boundary Layer Troposphere Stratosphere height The Atmospheric (or Planetary) Boundary Layer is.
Internal Gravity Waves and Turbulence Closure Model for SBL Sergej Zilitinkevich Division of Atmospheric Sciences, Department of Physical Sciences University.
Linear Wave Theory fundamental description: L - wave length H - wave height T - period d - water depth Shore Protection Manual, 1984 Overview of Waves.
Earth Rotation Earth’s rotation gives rise to a fictitious force called the Coriolis force It accounts for the apparent deflection of motions viewed in.
Baroclinic Instability in the Denmark Strait Overflow and how it applies the material learned in this GFD course Emily Harrison James Mueller December.
Momentum flux across the sea surface
Temperature Lapse rate- decrease of temperature with height:  = - dT/dz Environmental lapse rate (  ) order 6C/km in free atmosphere  d - dry adiabatic.
Ang Atmospheric Boundary Layer and Turbulence Zong-Liang Yang Department of Geological Sciences.
Training course: boundary layer II Similarity theory: Outline Goals, Buckingham Pi Theorem and examples Surface layer (Monin Obukhov) similarity Asymptotic.
Atmospheric Analysis Lecture 2.
Boundary Layer Meteorology
KIT – University of the State of Baden-Wuerttemberg and National Research Center of the Helmholtz Association INSTITUTE OF METEOROLOGY AND CLIMATE RESEARCH,
Review of the Boundary Layer
Wind Driven Circulation I: Planetary boundary Layer near the sea surface.
微氣象學 ( 全英文 ) 授課老師 : 游政谷 Instructor: Cheng-Ku Yu ( Micrometeorology ) Micrometeorology(1)
Observations and Models of Boundary-Layer Processes Over Complex Terrain What is the planetary boundary layer (PBL)? What are the effects of irregular.
Monin-Obukhoff Similarity Theory
Evaporation Slides prepared by Daene C. McKinney and Venkatesh Merwade
1 Introduction to Isentropic Coordinates: a new view of mean meridional & eddy circulations Cristiana Stan School and Conference on “the General Circulation.
Effects of different surface types and human activities.
Xin Xi. 1946: Obukhov Length, as a universal length scale for exchange processes in surface layer. 1954: Monin-Obukhov Similarity Theory, as a starting.
Convective Feedback: Its Role in Climate Formation and Climate Change Igor N. Esau.
STRATIFICATION EFFECT ON THE ROUGHNESS LENGTH
Reynolds-Averaged Navier-Stokes Equations -- RANS
Turbulent properties: - vary chaotically in time around a mean value - exhibit a wide, continuous range of scale variations - cascade energy from large.
Xin Xi Feb. 28. Basics  Convective entrainment : The buoyant thermals from the surface layer rise through the mixed layer, and penetrate (with enough.
A canopy model of mean winds through urban areas O. COCEAL and S. E. BELCHER University of Reading, UK.
USE THESE VALUES. e(T) = e s (T Dew ) PRACTICE WITH STABILITY.
LES of Turbulent Flows: Lecture 2 (ME EN )
1 Equations of Motion Buoyancy Ekman and Inertial Motion September 17.
Large Eddy Simulation of PBL turbulence and clouds Chin-Hoh Moeng National Center for Atmospheric Research.
Analysis of Turbulence Development in the Morning
R. A. Brown 2003 U. Concepci Ó n. High Winds Study - Motivation UW PBL Model says U 10 > 35 m/s Composite Storms show high winds Buoy limits:
Evaluating forecasts of the evolution of the cloudy boundary layer using radar and lidar observations Andrew Barrett, Robin Hogan and Ewan O’Connor Submitted.
Next The evening boundary layer: turbulence or no turbulence? Bas van de Wiel, Ivo van Hooijdonk & Judith Donda in collaboration with: Fred Bosveld, Peter.
Chapter 5 - PBL MT 454 Material Based on Chapter 5 The Planetary Boundary Layer.
INTRODUCTION TO CONVECTION
Observed Structure of the Atmospheric Boundary Layer
Processes in the Planetary Boundary Layer
Numerical experiments with the COSMO Model boundary layer scheme based on a parcel displacement scheme for a turbulent length scale Veniamin Perov and.
Climate Change in the Arctic Ocean NABOS 2013 Atmospheric Boundary Layer (ABL) and Turbulence Tobias Wolf, Nansen Environmental and Remote Sensing Center.
What is the Planetary Boundary Layer? The PBL is defined by the presence of turbulent mixing that couples the air to the underlying surface on a time scale.
Atm S 547 Lecture 1, Slide 1 The Atmospheric Boundary Layer (ABL or PBL) The layer of fluid directly above the Earth’s surface in which significant fluxes.
Relaminarisation of turbulent stratified flow Bas van de Wiel Moene, Steeneveld, Holtslag.
Introduction to the Turbulence Models
TERRAINS Terrain, or land relief, is the vertical and horizontal dimension of land surface. Terrain is used as a general term in physical geography, referring.
Development of the two-equation second-order turbulence-convection model (dry version): analytical formulation, single-column numerical results, and.
Hodograph Analysis Thermal Advection Stability
Coastal Ocean Dynamics Baltic Sea Research Warnemünde
Reynolds-Averaged Navier-Stokes Equations -- RANS
Monin-Obukhoff Similarity Theory
The β-spiral Determining absolute velocity from density field
Hurricane Vortex X L Converging Spin up Diverging Spin down Ekman
anelastic: Boussinesque: Homework 1.1 …eliminates sound waves
New insights into turbulence dynamics under stabilizing
Turbulent Kinetic Energy (TKE)
Turbulent properties:
Presentation transcript:

Non-Universal Turbulence in Planetary Boundary Layers Igor N. Esau (igore@nersc.no) Nansen Environmental and Remote Sensing Centre Bergen, Norway

Classical View Turbulent boundary layers consist of random eddies (Kolmogorov 1941) Small eddies produce the shear stress and transport heat, scalars and momentum, therefore - “active” (Townsend 1961) Large eddies do not produce the shear stress and do not transport heat, scalar and momentum, therefore - “inactive” (Townsand 1961)

Universal Properties of Small Eddies Universal motions After Chapman, 1979, AIAA papers After Larson, 1986, RISOE report

Universal Properties of Small Eddies Kolmogorov's law for the energy spectrum: Structure function for the turbulent stress: Smagorinsky-Lilly eddy-viscosity relation for the turbulent stress:

Small eddies exert stress and carry momentum in classical boundary layers How do large eddies look like?

Classical Large Eddies Horseshoe vortices Top view Side view Ejections of low speed fluid carry stress

Turbulence in PBLs Real world turbulence is different: Rough surface Large scales Stratification Rotation

New View Internal wave radiation from PBL top (Zilitinkevich, 2000) Eddy blocking and distruction in surface layer (Hunt, 2000)

Fluxes of Turbulent Kinetic Energy Classical view New view Turbulence Free Atmosphere P=e=0 P=0 e>0 PBL Core P<e P<e P=e P>e Surface Layer P>e Roughness Layer P<e

Profiles of the Energy Flux Surface layer Roughness layer

Maximum of Non-dimensional TKE Measurements in shallow near-neutral PBLs (Hogstrom, 1990) Small stress Large stress LES data Measurements in deep near-neutral PBLs (Pennel, LeMone, 74) Small eddies Large eddies

Turbulent Stress Turbulent stress Turbulent stress decreases with the eddy size Turbulent stress does not change with the eddy size Critical eddy size

What determines the size of large eddies?

Coherent Structures in Sheared Flow Typical size of the first characteristic eddy is close to the critical eddy size for the stress fall-off. Lc~ 600 meters in atmospheric boundary layer

PBL Depth Imposed stability parameter accounts for the size of large eddies (Zilitinkevich, 2000)

Instant View

Why do we need this knowledge? Anthropogenic hazards Weather forecast Climate research Why do we need this knowledge? Air pollution management Understanding of cloud structures

Geostrophic Drag and Geostrophic Angle Larger eddies Smaller eddies Larger eddies Smaller eddies

A and B Functions

Conclusions Turbulent planetary boundary layer consists of large eddies Small eddies produce little shear stress and relate to large eddies Large eddies exert the most of the shear stress and transport the most of heat, scalar and momentum Large eddies are limited by (I) the PBL depth, which is the most important factor in real PBLs and (II) the characteristic size of coherent eddies

Thank you for your attention Bergen, Norway Thank you for your attention