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1. An introduction to Terra-Incognita 4. A potpourri of LES with complex boundaries 3. Large-eddy simulation (LES) A LARGE EDDY SIMULATION PERSPECTIVE OF TERRA-INCOGNITA 2. Rough wall SGS dynamics and Terra- Incognita

1. An introduction to Terra-Incognita

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A LARGE EDDY SIMULATION PERSPECTIVE OF TERRA-INCOGNITA. 1. An introduction to Terra-Incognita . 2. Rough wall SGS dynamics and Terra-Incognita. 3. Large-eddy simulation (LES). 4. A potpourri of LES with complex boundaries . Eric Terrill, Scripps Institute of Oceanography. Cathedral Rocks, AU. - PowerPoint PPT Presentation

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Page 1: 1. An introduction to Terra-Incognita

1. An introduction to Terra-Incognita

4. A potpourri of LES with complex boundaries

3. Large-eddy simulation (LES)

A LARGE EDDY SIMULATION PERSPECTIVE OF TERRA-INCOGNITA

2. Rough wall SGS dynamics and Terra-Incognita

Page 2: 1. An introduction to Terra-Incognita

Eric Terrill, Scripps Institute of Oceanography

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Cathedral Rocks, AU

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A MOTIVATION FOR OROGRAPHY AND TURBULENCE

$100M wind park, 33 turbinesExtensive downtime due to wind gusts (turbulence)Poor site

40 m

60 m~150 m

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Bolund is a combined measurement and modeling project related to wind energy in complex terrain. An isolated steep hill, Bolund, at Roskilde Fjord will be equipped with nine measurement masts with conventional meteorological instruments and remote sensing Lidars at several positions for obtaining detailed information of mean wind, wind shear, turbulence intensities etc.

METCRAX is investigating the structure and evolution of cold-air pools and stable BLs that form in basins and valleys.

LES OF ABLs WITH COMPLEX TERRAIN AND STABLE STRATIFICATION

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Physical space

Computational space

• 1-to-1 mapping

• is the Jacobian of the transformation

• Transform just the coordinates

• Fundamental unknowns are Cartesian velocity components ui

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u

w

p

x

z

Vertically staggered schemeCo-located scheme

w

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Momentum

Scalar

TKE

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Continuity

Momentum

Scalar (temperature)

SGS energy

Pressure equation

Plus rough wall zo boundary conditions

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Diagonal preconditioning matrix

Continuity

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Resolved turbulent stress

Form dragSubgrid (viscous) stress

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EXAMPLES

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PRESSURE FIELD IN TURBULENT FLOW OVER 2D BUMPS

RANS MODEL (Taylor etal, 1998)

?

LES

+-

U

+-

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Flow separation

PRESSURE CONTOURS AND FLOW VECTORS

smooth

rough

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TURBULENT FLOW OVER AND AROUND 3D OBSTACLES

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3D Hill

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150 s time averaged streamlines

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METCRAX is investigating the structure and evolution of cold-air pools and stable BLs that form in basins and valleys.

LES OF PBLs WITH COMPLEX TERRAIN AND STABLE STRATIFICATION

3D Crater

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FLOWFIELDS ON CRATER CENTERLINE XZ PLANE

150 s Time Average P’, Streamlines

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FLOWFIELDS ON CRATER CENTERLINE XZ PLANE

150 s Time Average P’, Streamlines

Snapshot of w

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MOVING WAVES

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HIGH RESOLUTION AIR-SEA INTERACTION: U ~ 15 m/s courtesy Eric Terrill

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Photograph from the research vessel Knorr in winds ranging from 60 to 100 knots and 30-40 foot tall waves on an expedition to the Irminger Sea in October 2007. (Photo by Kjetil Vage, Woods Hole Oceanographic Institution)

LANGMUIR CIRCULATIONS IN HIGH WINDS?

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GRID MOVEMENT IN THE LOWER BOUNDARY LAYER

Grid speed

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Continuity equation

Space conservation rule

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Continuity

Geometric conservation

Momentum

Scalar (temperature)

SGS energy

Pressure equation

Plus rough wall boundary conditions and matching to orbital velocity of wavefield

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Moving swell

Ug = 5 m/s, WAVE AGE = 4.8, PRESSURE CONTOURS AND VECTORS

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