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Remote Sensing

DYNAMICS OF THE ATMOSPHERIC BOUNDARY LAYER OVER A

PEATLAND WITH DOPPLER LIDAR

P. Ortiz-Amezcua*, A. Manninen, P. Pentikäinen, E.J. O’Connor, I.S.

Stachlewska, J.A. Casquero-Vera, J.A. Benavent-Oltra, J.L. Guerrero- Rascado, L. Alados-Arboledas, B.H. Chojnicki, D. Shüttemeyer

Contact: pablo.ortiz@fuw.edu.pl

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P. Ortiz-Amezcua Atmospheric Physics Seminar 2

CONTENTS

I NTRODUCTION AND MOTIVATION

I NSTRUMENTATION AND METHODOLOGY

E XPERIMENTAL SITE

R ESULTS

S UMMARY AND OUTLOOK

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I NTRODUCTION

AND MOTIVATION

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P. Ortiz-Amezcua Atmospheric Physics Seminar 4

MOTIVATION

Adapted from (Stull, 1988)

Atmospheric Boundary Layer: lowermost part of the atmosphere, directly influenced by the Earth’s surface

Importance:

-weather forecasting -climate studies

-pollutant dispersion

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MOTIVATION

Complex description:

interactions among multiple variables and processes

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P. Ortiz-Amezcua Atmospheric Physics Seminar 6

MOTIVATION

ABL height:

• Important for pollutant dispersion studies and meteorological modelling

• Strongly dependent on the tracer:

(Moreira et al., 2018)

-Air movement (dynamics)

-Aerosol concentration

-Temperature behaviour

(thermodynamics)

(7)

MOTIVATION

Adapted from (Emanuelson, 2013)

Dymanics of ABL: Turbulence

Turbulent eddies caused by mechanical and/or thermal processes

Statistical approach is

needed

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P. Ortiz-Amezcua Atmospheric Physics Seminar 8

I NSTRUMENTATION

AND METHODOLOGY

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INSTRUMENTATION

Lidar

(Light detection and ranging)

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P. Ortiz-Amezcua Atmospheric Physics Seminar 10

INSTRUMENTATION

Lidar

(Light detection and ranging)

Doppler Effect

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INSTRUMENTATION

Doppler Lidar technique:

retrieval of radial wind

with temporal and spatial resolution

1500

Detection type Heterodyne

Range resolution (m) 30

Usual integration time (s) ~2

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P. Ortiz-Amezcua Atmospheric Physics Seminar 12

METHODOLOGY

Wind vector field retrieval:

Velocity-Azimuth Display (VAD) scan

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METHODOLOGY

Wind vector field retrieval:

Velocity-Azimuth Display (VAD) scan

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P. Ortiz-Amezcua Atmospheric Physics Seminar 14

METHODOLOGY

Turbulence – vertical wind (w) statistical momenta

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METHODOLOGY

Turbulence – vertical wind (w) statistical momenta

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P. Ortiz-Amezcua Atmospheric Physics Seminar 16

METHODOLOGY

Turbulence – vertical wind (w) statistical momenta

Skewness:

Predominant direction of turbulent movements Variance:

Proportional to Turbulent Kinetic

Energy

(17)

METHODOLOGY

Derived products:

Wind shear

TKE dissipation rate:

Proxy for turbulence presence

O’Connor et al. (2010)

Boundary Layer Classification

Manninen et al. (2016)

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P. Ortiz-Amezcua Atmospheric Physics Seminar 18

E XPERIMENTAL

SITE

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EXPERIMENTAL SITE

PolWET site in Rzecin (PULS)

(20)

P. Ortiz-Amezcua Atmospheric Physics Seminar 20

EXPERIMENTAL SITE

PolWET site in Rzecin (PULS)

• Peatland environment with:

o 8,5 °C average T

o 526 mm annual precipitation o Prevailing W surface wind

• Strong interaction with climate system

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EXPERIMENTAL SITE

PolWET site in Rzecin (PULS)

• Peatland environment with:

o 8,5 °C average T

o 526 mm annual precipitation o Prevailing W surface wind

• Strong interaction with climate system

• ICOS site with instrumentation from

Poland AOD

(22)

P. Ortiz-Amezcua Atmospheric Physics Seminar 22

EXPERIMENTAL SITE

PolWET site in Rzecin (PULS)

• Peatland environment with:

o 8,5 °C average T

o 526 mm annual precipitation o Prevailing W surface wind

• Strong interaction with climate system

• ICOS site with instrumentation from Poland AOD

• POLIMOS campaign (ESA): 24 May – 24

September 2018

(23)

R ESULTS

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P. Ortiz-Amezcua Atmospheric Physics Seminar 24

SAMPLE CASES

θ θ

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BL-CLOUD FREQUENCY

Clouds mostly at central hours, with height increasing with time

10-20 % cloud occurrence:

➢ from 10-16 h UTC

➢ increasing heights from 1 – 3 km a.g.l.

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P. Ortiz-Amezcua Atmospheric Physics Seminar 26

HORIZONTAL WIND

Wind Speed:

• High average wind speeds

• Daytime: diurnal pattern strongly

influenced by the ABL development. Speeds increasing with height with minimum at noon

• Nighttime: strong winds, with maximum around 500 m a.g.l.

Wind Direction:

• Daytime: W-NW-N at all heights

• Nighttime: homogeneous distribution of winds.

• Strongest winds from NW

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TURBULENCE SOURCES

Convective mixing:

• Starts with sunrise in the lowest heights

• Gowing altitudes up to a maximum ~ 600 m a.g.l.

(70 % of cases)

Wind shear driven turbulence:

• Frequencies more than 40 % for some ranges and times

• Mostly detected < 100 m a.g.l.

Cloud driven turbulence:

• Mainly during central hours at heights of 600- 1000 m a.g.l.

• Frequencies around 5 %

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P. Ortiz-Amezcua Atmospheric Physics Seminar 28

S UMMARY

AND OUTLOOK

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SUMMARY

& OUTLOOK

• Most frequent horizontal wind from W with highest speeds during nighttime.

• Convective mixing: clear diurnal pattern up to 1 km a.g.l.

• Wind shear driven turbulence: important contribution below 100 m a.g.l.

• Cloud driven turbulence: non-negligible contribution during central hours.

(30)

P. Ortiz-Amezcua Atmospheric Physics Seminar 30

SUMMARY

& OUTLOOK

• Study of particular patterns with statistical techniques (e.g. PCA)

• Automatic detection of Low-level Jets

• Combination with Raman lidar: AEROSOL FLUXES

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THANK YOU FOR YOUR ATTENTION

This research has been done primarily in the frame of the Technical assistance for Polish Radar and Lidar Mobile Observation System (POLIMOS) funded by ESA-ESTEC Contract no. 4000119961/16/NL/FF/mg.

This research was funded by Spanish Ministerio de Educación, Cultura y Deporte, grant number FPU14/03684, by Spanish Ministerio de Economía y Competitividad, projects CGL2016-81092- R, CGL2017-83538-C3-1-R, and CGL2017- 90884-REDT, by Horizon 2020 Framework Programme of the European Union, grant number 654109.

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